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	<title>Particles, Vol. 9, Pages 49: Beaming of Polarized Radiation in Subcritical X-Ray Pulsars</title>
	<link>https://www.mdpi.com/2571-712X/9/2/49</link>
	<description>Radiation of X-ray pulsars is powered by accretion on the neutron star surface from a binary companion under the influence of a strong magnetic field. We study the beaming of this radiation in the case of subcritical X-ray pulsars, where it is formed in the accretion channel close to the neutron star surface. We solve equations of the hydrodynamics and radiative transfer of two coupled polarization modes in the accretion channel numerically, taking into account resonant Compton scattering and vacuum polarization. The beaming patterns are obtained for different accretion rates, photon energies, and polarizations, as well as for different models of the neutron star surface radiation. The calculated beaming patterns are converted into light curves for both the intensity and polarization, taking into account the effects of General Relativity. These beaming patterns and light curves are found to be strongly affected by the resonant Compton scattering for photon energies comparable with the electron cyclotron energy. In particular, the angular redistribution of radiation near the cyclotron resonance may reduce the light-curve modulation amplitude, which is consistent with observational indications of a suppressed pulsed fraction at these energies.</description>
	<pubDate>2026-05-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 49: Beaming of Polarized Radiation in Subcritical X-Ray Pulsars</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/49">doi: 10.3390/particles9020049</a></p>
	<p>Authors:
		Ivan D. Markozov
		Alexander Y. Potekhin
		Alexander D. Kaminker
		Alexander A. Mushtukov
		</p>
	<p>Radiation of X-ray pulsars is powered by accretion on the neutron star surface from a binary companion under the influence of a strong magnetic field. We study the beaming of this radiation in the case of subcritical X-ray pulsars, where it is formed in the accretion channel close to the neutron star surface. We solve equations of the hydrodynamics and radiative transfer of two coupled polarization modes in the accretion channel numerically, taking into account resonant Compton scattering and vacuum polarization. The beaming patterns are obtained for different accretion rates, photon energies, and polarizations, as well as for different models of the neutron star surface radiation. The calculated beaming patterns are converted into light curves for both the intensity and polarization, taking into account the effects of General Relativity. These beaming patterns and light curves are found to be strongly affected by the resonant Compton scattering for photon energies comparable with the electron cyclotron energy. In particular, the angular redistribution of radiation near the cyclotron resonance may reduce the light-curve modulation amplitude, which is consistent with observational indications of a suppressed pulsed fraction at these energies.</p>
	]]></content:encoded>

	<dc:title>Beaming of Polarized Radiation in Subcritical X-Ray Pulsars</dc:title>
			<dc:creator>Ivan D. Markozov</dc:creator>
			<dc:creator>Alexander Y. Potekhin</dc:creator>
			<dc:creator>Alexander D. Kaminker</dc:creator>
			<dc:creator>Alexander A. Mushtukov</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020049</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-05-05</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-05-05</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>49</prism:startingPage>
		<prism:doi>10.3390/particles9020049</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/49</prism:url>
	
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        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/48">

	<title>Particles, Vol. 9, Pages 48: Nuclear Exotic Structures, Exotic Decays and Near-Barrier Reactions</title>
	<link>https://www.mdpi.com/2571-712X/9/2/48</link>
	<description>The reaction dynamics of weakly-bound nuclear systems at near-barrier energies is a compelling topic in nuclear physics. This review summarizes decades of experimental work by the Nuclear Reaction Group at the China Institute of Atomic Energy. Using transfer reactions with the distorted wave born approximation and asymptotic normalization coefficient analyses, we confirm the first excited neutron halo (13C) on the &amp;amp;beta;-stability line and identified new halo states in 12B. Total reaction cross-section measurements revealed proton halo nuclei 27P and 29S, with core enlargement observed in 27P and 28P. We established conditions for halo formation and delineated the proton halo existence region. In two-proton emission studies, we observed 2He cluster emission from highly excited 17,18Ne and 28,29S, with 29S being the second such case internationally. In &amp;amp;beta;-delayed decay, we discovered &amp;amp;beta;2p emission in 22Si and determined its mass, observing isospin-symmetry breaking in 20Mg, 22Si, and 27S. Decay schemes for 27S and 26P addressed the 26Al abundance problem. For nuclear interactions, we investigated the 6He optical potential, finding the dispersion relation inapplicable for 6He + 209Bi, and developed notch and Bayesian methods to constrain uncertainties. For unstable nuclei, the proton drip-line systems 8B and 17F have been intensively studied via complete kinematics measurements of the 8B + 120Sn and 17F + 58Ni reactions, respectively. The results show that elastic breakup dominates for proton-halo 8B, while inelastic breakup prevails for 17F, with proton-rich nuclei exhibiting lower breakup probabilities than neutron-halo nuclei due to Coulomb effects. Fusion studies revealed sub-barrier enhancement in 17F + 58Ni from continuum couplings. We propose direct fusion&amp;amp;ndash;evaporation measurements with deflection systems integrated with breakup detection to disentangle complete and incomplete fusion channels.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 48: Nuclear Exotic Structures, Exotic Decays and Near-Barrier Reactions</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/48">doi: 10.3390/particles9020048</a></p>
	<p>Authors:
		Cheng Yin
		Chengjian Lin
		Lei Yang
		Feng Yang
		Huiming Jia
		Nanru Ma
		Peiwei Wen
		Tianpeng Luo
		</p>
	<p>The reaction dynamics of weakly-bound nuclear systems at near-barrier energies is a compelling topic in nuclear physics. This review summarizes decades of experimental work by the Nuclear Reaction Group at the China Institute of Atomic Energy. Using transfer reactions with the distorted wave born approximation and asymptotic normalization coefficient analyses, we confirm the first excited neutron halo (13C) on the &amp;amp;beta;-stability line and identified new halo states in 12B. Total reaction cross-section measurements revealed proton halo nuclei 27P and 29S, with core enlargement observed in 27P and 28P. We established conditions for halo formation and delineated the proton halo existence region. In two-proton emission studies, we observed 2He cluster emission from highly excited 17,18Ne and 28,29S, with 29S being the second such case internationally. In &amp;amp;beta;-delayed decay, we discovered &amp;amp;beta;2p emission in 22Si and determined its mass, observing isospin-symmetry breaking in 20Mg, 22Si, and 27S. Decay schemes for 27S and 26P addressed the 26Al abundance problem. For nuclear interactions, we investigated the 6He optical potential, finding the dispersion relation inapplicable for 6He + 209Bi, and developed notch and Bayesian methods to constrain uncertainties. For unstable nuclei, the proton drip-line systems 8B and 17F have been intensively studied via complete kinematics measurements of the 8B + 120Sn and 17F + 58Ni reactions, respectively. The results show that elastic breakup dominates for proton-halo 8B, while inelastic breakup prevails for 17F, with proton-rich nuclei exhibiting lower breakup probabilities than neutron-halo nuclei due to Coulomb effects. Fusion studies revealed sub-barrier enhancement in 17F + 58Ni from continuum couplings. We propose direct fusion&amp;amp;ndash;evaporation measurements with deflection systems integrated with breakup detection to disentangle complete and incomplete fusion channels.</p>
	]]></content:encoded>

	<dc:title>Nuclear Exotic Structures, Exotic Decays and Near-Barrier Reactions</dc:title>
			<dc:creator>Cheng Yin</dc:creator>
			<dc:creator>Chengjian Lin</dc:creator>
			<dc:creator>Lei Yang</dc:creator>
			<dc:creator>Feng Yang</dc:creator>
			<dc:creator>Huiming Jia</dc:creator>
			<dc:creator>Nanru Ma</dc:creator>
			<dc:creator>Peiwei Wen</dc:creator>
			<dc:creator>Tianpeng Luo</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020048</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>48</prism:startingPage>
		<prism:doi>10.3390/particles9020048</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/48</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/47">

	<title>Particles, Vol. 9, Pages 47: Lifetime Measurements&amp;mdash;A Powerful Tool to Study Nuclear Structure</title>
	<link>https://www.mdpi.com/2571-712X/9/2/47</link>
	<description>Advanced Doppler-shift methods for the calculation of the &amp;amp;gamma;-ray lineshape registered in recoil-distance Doppler-shift and Doppler-shift attenuation methods are presented, emphasizing the case using a gate set on the shifted part of a direct feeding transition. For the precise description of the &amp;amp;gamma;-ray lineshape, the process of evaporation of light particles from the compound nucleus has to be taken into account in the case of heavy ion-induced fusion-evaporation reactions. In addition, the impact of different approaches for calculating stopping powers is investigated in the process of the lifetime determinations. In the RDDS experiments, the &amp;amp;gamma;-emission during the slowing down in the stopper is discussed in detail. Applications of the new procedures are demonstrated in two experiments: the first one is a plunger experiment performed in order to check for chirality in the 134Pr nucleus and the second one is a DSAM experiment conducted to test the isospin symmetry in 31P and 31S mirror nuclei.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 47: Lifetime Measurements&amp;mdash;A Powerful Tool to Study Nuclear Structure</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/47">doi: 10.3390/particles9020047</a></p>
	<p>Authors:
		Dimitar Tonev
		Galina D. Dimitrova
		Anguel Demerdjiev
		Giovanni De Gregorio
		Giacomo de Angelis
		Elena Geleva
		Nikolay Goutev
		Nikolay N. Petrov
		Ivaylo Pantaleev
		Lilianna Panteleev-Simeonova
		</p>
	<p>Advanced Doppler-shift methods for the calculation of the &amp;amp;gamma;-ray lineshape registered in recoil-distance Doppler-shift and Doppler-shift attenuation methods are presented, emphasizing the case using a gate set on the shifted part of a direct feeding transition. For the precise description of the &amp;amp;gamma;-ray lineshape, the process of evaporation of light particles from the compound nucleus has to be taken into account in the case of heavy ion-induced fusion-evaporation reactions. In addition, the impact of different approaches for calculating stopping powers is investigated in the process of the lifetime determinations. In the RDDS experiments, the &amp;amp;gamma;-emission during the slowing down in the stopper is discussed in detail. Applications of the new procedures are demonstrated in two experiments: the first one is a plunger experiment performed in order to check for chirality in the 134Pr nucleus and the second one is a DSAM experiment conducted to test the isospin symmetry in 31P and 31S mirror nuclei.</p>
	]]></content:encoded>

	<dc:title>Lifetime Measurements&amp;amp;mdash;A Powerful Tool to Study Nuclear Structure</dc:title>
			<dc:creator>Dimitar Tonev</dc:creator>
			<dc:creator>Galina D. Dimitrova</dc:creator>
			<dc:creator>Anguel Demerdjiev</dc:creator>
			<dc:creator>Giovanni De Gregorio</dc:creator>
			<dc:creator>Giacomo de Angelis</dc:creator>
			<dc:creator>Elena Geleva</dc:creator>
			<dc:creator>Nikolay Goutev</dc:creator>
			<dc:creator>Nikolay N. Petrov</dc:creator>
			<dc:creator>Ivaylo Pantaleev</dc:creator>
			<dc:creator>Lilianna Panteleev-Simeonova</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020047</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>47</prism:startingPage>
		<prism:doi>10.3390/particles9020047</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/47</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/46">

	<title>Particles, Vol. 9, Pages 46: Radiative Decays of Hadronic Molecules: From Confusion to Inspiration</title>
	<link>https://www.mdpi.com/2571-712X/9/2/46</link>
	<description>Radiative decays of hadronic states provide an essential source of information that can facilitate deciphering their nature and properties. However, a lot of confusion concerning radiative decays of hadronic molecules and their interpretation can be found in the literature. In this paper, we briefly review several types of such decays and pinpoint similarities and essential differences between them. In particular, we emphasise the crucial role played by the hierarchy of the scales relevant to the studied system and the resulting necessity of employing an approach that considers them appropriately. We illustrate the situation with several instructive examples.</description>
	<pubDate>2026-04-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 46: Radiative Decays of Hadronic Molecules: From Confusion to Inspiration</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/46">doi: 10.3390/particles9020046</a></p>
	<p>Authors:
		Feng-Kun Guo
		Christoph Hanhart
		Alexey Nefediev
		</p>
	<p>Radiative decays of hadronic states provide an essential source of information that can facilitate deciphering their nature and properties. However, a lot of confusion concerning radiative decays of hadronic molecules and their interpretation can be found in the literature. In this paper, we briefly review several types of such decays and pinpoint similarities and essential differences between them. In particular, we emphasise the crucial role played by the hierarchy of the scales relevant to the studied system and the resulting necessity of employing an approach that considers them appropriately. We illustrate the situation with several instructive examples.</p>
	]]></content:encoded>

	<dc:title>Radiative Decays of Hadronic Molecules: From Confusion to Inspiration</dc:title>
			<dc:creator>Feng-Kun Guo</dc:creator>
			<dc:creator>Christoph Hanhart</dc:creator>
			<dc:creator>Alexey Nefediev</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020046</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-28</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-28</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>46</prism:startingPage>
		<prism:doi>10.3390/particles9020046</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/46</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/45">

	<title>Particles, Vol. 9, Pages 45: Symmetry- Preserving Contact Interaction Approaches: An Overview of Meson and Diquark Form Factors</title>
	<link>https://www.mdpi.com/2571-712X/9/2/45</link>
	<description>We present an updated overview of the symmetry-preserving contact interaction model in hadronic physics, which was developed a little over a decade ago to describe the mass spectrum and internal structure of mesons and diquarks composed of light and heavy quarks. Over the years, the contact interaction model has evolved into a framework capable of treating both ground and excited states, providing a simple yet consistent approach to nonperturbative QCD. In this review, we examine the mass spectrum and elastic form factors of forty mesons with different spins and parities, together with their corresponding diquark partners. Importantly, we update the comparison of contact interaction predictions using recent results from the literature, offering a fresh perspective on the model&amp;amp;rsquo;s performance, strengths, and limitations. The analysis presented here refines previous conclusions and supports the contact interaction model as a practical tool for hadron structure studies, with potential applications to baryons and multiquark states. We also present comparisons with other theoretical models and approaches, including lattice quantum chromodynamics, and comment on future prospects in view of ongoing and planned experimental programs regarding hadron structure. In particular, forthcoming measurements at FAIR together with future studies at Jefferson Lab and the Electron Ion Collider are expected to provide key insights into hadron structure, with FAIR offering indirect constraints via hadron spectroscopy, hadronic interactions, and in-medium properties; high-precision data on meson structure and form factors from Jefferson Lab and the Electron Ion Collider will provide valuable benchmarks with which to confront predictions based on the contact interaction model.</description>
	<pubDate>2026-04-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 45: Symmetry- Preserving Contact Interaction Approaches: An Overview of Meson and Diquark Form Factors</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/45">doi: 10.3390/particles9020045</a></p>
	<p>Authors:
		Laura Xiomara Gutiérrez-Guerrero
		Roger José Hernández-Pinto
		</p>
	<p>We present an updated overview of the symmetry-preserving contact interaction model in hadronic physics, which was developed a little over a decade ago to describe the mass spectrum and internal structure of mesons and diquarks composed of light and heavy quarks. Over the years, the contact interaction model has evolved into a framework capable of treating both ground and excited states, providing a simple yet consistent approach to nonperturbative QCD. In this review, we examine the mass spectrum and elastic form factors of forty mesons with different spins and parities, together with their corresponding diquark partners. Importantly, we update the comparison of contact interaction predictions using recent results from the literature, offering a fresh perspective on the model&amp;amp;rsquo;s performance, strengths, and limitations. The analysis presented here refines previous conclusions and supports the contact interaction model as a practical tool for hadron structure studies, with potential applications to baryons and multiquark states. We also present comparisons with other theoretical models and approaches, including lattice quantum chromodynamics, and comment on future prospects in view of ongoing and planned experimental programs regarding hadron structure. In particular, forthcoming measurements at FAIR together with future studies at Jefferson Lab and the Electron Ion Collider are expected to provide key insights into hadron structure, with FAIR offering indirect constraints via hadron spectroscopy, hadronic interactions, and in-medium properties; high-precision data on meson structure and form factors from Jefferson Lab and the Electron Ion Collider will provide valuable benchmarks with which to confront predictions based on the contact interaction model.</p>
	]]></content:encoded>

	<dc:title>Symmetry- Preserving Contact Interaction Approaches: An Overview of Meson and Diquark Form Factors</dc:title>
			<dc:creator>Laura Xiomara Gutiérrez-Guerrero</dc:creator>
			<dc:creator>Roger José Hernández-Pinto</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020045</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-24</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-24</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>45</prism:startingPage>
		<prism:doi>10.3390/particles9020045</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/45</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/44">

	<title>Particles, Vol. 9, Pages 44: A Solution of the Scalar Nonet Mass Puzzle</title>
	<link>https://www.mdpi.com/2571-712X/9/2/44</link>
	<description>We present a short review dedicated to low-lying meson states. We present all meson nonets, which consist from up, down and strange light quarks. We consider the scalar nonet as a basic nonet. We work in the framework of the massless Nambu&amp;amp;ndash;Jona-Lasinio UR(3)&amp;amp;times;UL(3) quark model. The collective meson states are described through initially bare quark&amp;amp;ndash;antiquark pairs, whose condensates lead simultaneously to spontaneous breaking of the chiral and the flavour symmetry. After quantisation and the spontaneous breaking of the chiral symmetry, when quarks obtain constituent nonzero masses, they become dressed. We present an explanation of the inverse mass hierarchy of the low-lying nonet of the scalar mesons. The proposed explanation is based on symmetry principles. It is shown that, due to the flavour symmetry breaking, two isodoublets of K0*(700) mesons play the role of Goldstone bosons. It is also proven that there exists a solution with almost degenerate masses of the a0(980) and f0(980) mesons and a zero mass of the f0(500) meson. Short description of the physical properties of other meson nonets is provided. In particular unique mass relations among the different nonets, which are experimentally confirmed, are presented.</description>
	<pubDate>2026-04-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 44: A Solution of the Scalar Nonet Mass Puzzle</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/44">doi: 10.3390/particles9020044</a></p>
	<p>Authors:
		Mihail Chizhov
		Emanuil Chizhov
		Daniela Kirilova
		Momchil Naydenov
		</p>
	<p>We present a short review dedicated to low-lying meson states. We present all meson nonets, which consist from up, down and strange light quarks. We consider the scalar nonet as a basic nonet. We work in the framework of the massless Nambu&amp;amp;ndash;Jona-Lasinio UR(3)&amp;amp;times;UL(3) quark model. The collective meson states are described through initially bare quark&amp;amp;ndash;antiquark pairs, whose condensates lead simultaneously to spontaneous breaking of the chiral and the flavour symmetry. After quantisation and the spontaneous breaking of the chiral symmetry, when quarks obtain constituent nonzero masses, they become dressed. We present an explanation of the inverse mass hierarchy of the low-lying nonet of the scalar mesons. The proposed explanation is based on symmetry principles. It is shown that, due to the flavour symmetry breaking, two isodoublets of K0*(700) mesons play the role of Goldstone bosons. It is also proven that there exists a solution with almost degenerate masses of the a0(980) and f0(980) mesons and a zero mass of the f0(500) meson. Short description of the physical properties of other meson nonets is provided. In particular unique mass relations among the different nonets, which are experimentally confirmed, are presented.</p>
	]]></content:encoded>

	<dc:title>A Solution of the Scalar Nonet Mass Puzzle</dc:title>
			<dc:creator>Mihail Chizhov</dc:creator>
			<dc:creator>Emanuil Chizhov</dc:creator>
			<dc:creator>Daniela Kirilova</dc:creator>
			<dc:creator>Momchil Naydenov</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020044</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-23</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-23</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>44</prism:startingPage>
		<prism:doi>10.3390/particles9020044</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/44</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/43">

	<title>Particles, Vol. 9, Pages 43: Nuclear Binding Energies from Composite-Knot Ropelength: A Topological Model That Mirrors Quantum-Mechanical Phenomenology</title>
	<link>https://www.mdpi.com/2571-712X/9/2/43</link>
	<description>We report a curious numerical observation: If atomic nuclei are modelled as connect-sums of threefoil knots with alternating chirality, the ropelength of the composite knot&amp;amp;mdash;a purely geometric quantity requiring no quantum mechanics&amp;amp;mdash;tracks the experimental binding-energy curve from hydrogen to uranium. A two-parameter fit to 50 nuclei gives R2=0.9998 (coefficient of determination; 1 = perfect fit) and RMS=6.9MeV (root-mean-square deviation between model and experiment), comparable to the five-parameter Bethe&amp;amp;ndash;Weizs&amp;amp;auml;cker formula (RMS=8.3MeV) at less than half the parameter count. Out-of-sample predictions for Pu244 and Cf252, not used in the fit, are accurate to 0.4MeV and 8.4MeV, respectively. What makes the observation worth reporting is not the fit itself, but the range of nuclear phenomenology that emerges uninstructed from the topology: saturation, surface energy, isospin pairing, odd-even staggering, and geometric analogues of nuclear isomers all appear as consequences of the connect-sum construction, without additional assumptions. We catalogue these correspondences, assess which are structural and which may be coincidental, and identify concrete numerical tests that would distinguish the two possibilities.</description>
	<pubDate>2026-04-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 43: Nuclear Binding Energies from Composite-Knot Ropelength: A Topological Model That Mirrors Quantum-Mechanical Phenomenology</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/43">doi: 10.3390/particles9020043</a></p>
	<p>Authors:
		Thomas Riedel
		</p>
	<p>We report a curious numerical observation: If atomic nuclei are modelled as connect-sums of threefoil knots with alternating chirality, the ropelength of the composite knot&amp;amp;mdash;a purely geometric quantity requiring no quantum mechanics&amp;amp;mdash;tracks the experimental binding-energy curve from hydrogen to uranium. A two-parameter fit to 50 nuclei gives R2=0.9998 (coefficient of determination; 1 = perfect fit) and RMS=6.9MeV (root-mean-square deviation between model and experiment), comparable to the five-parameter Bethe&amp;amp;ndash;Weizs&amp;amp;auml;cker formula (RMS=8.3MeV) at less than half the parameter count. Out-of-sample predictions for Pu244 and Cf252, not used in the fit, are accurate to 0.4MeV and 8.4MeV, respectively. What makes the observation worth reporting is not the fit itself, but the range of nuclear phenomenology that emerges uninstructed from the topology: saturation, surface energy, isospin pairing, odd-even staggering, and geometric analogues of nuclear isomers all appear as consequences of the connect-sum construction, without additional assumptions. We catalogue these correspondences, assess which are structural and which may be coincidental, and identify concrete numerical tests that would distinguish the two possibilities.</p>
	]]></content:encoded>

	<dc:title>Nuclear Binding Energies from Composite-Knot Ropelength: A Topological Model That Mirrors Quantum-Mechanical Phenomenology</dc:title>
			<dc:creator>Thomas Riedel</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020043</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-22</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-22</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>43</prism:startingPage>
		<prism:doi>10.3390/particles9020043</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/43</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/42">

	<title>Particles, Vol. 9, Pages 42: Poincar&amp;eacute; Invariance and the Unruh Effect</title>
	<link>https://www.mdpi.com/2571-712X/9/2/42</link>
	<description>In quantum field theory, the vacuum is popularly considered to be a complex medium populated with virtual particle + antiparticle pairs. To an observer experiencing uniform acceleration, it is generally held that these virtual particles become real, appearing as a gas at a temperature that grows with the acceleration. This is the Unruh effect. However, it has been shown that vacuum complexity is an artifact produced by treating quantum field theory in a manner that does not manifestly enforce causality. Choosing a quantization approach that patently enforces causality, the quantum field theory vacuum is barren, bereft even of virtual particles. We show that acceleration has no effect on a trivial vacuum; hence, there is no Unruh effect in such a treatment of quantum field theory. Since the standard calculations suggesting an Unruh effect are formally consistent, insofar as they have been completed, there must be a canceling contribution that is omitted in the usual analyses. We argue that it is the dynamical action of conventional Lorentz transformations on the structure of an Unruh detector.</description>
	<pubDate>2026-04-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 42: Poincar&amp;eacute; Invariance and the Unruh Effect</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/42">doi: 10.3390/particles9020042</a></p>
	<p>Authors:
		Alexandre Deur
		Stanley J. Brodsky
		Craig D. Roberts
		Balša Terzić
		</p>
	<p>In quantum field theory, the vacuum is popularly considered to be a complex medium populated with virtual particle + antiparticle pairs. To an observer experiencing uniform acceleration, it is generally held that these virtual particles become real, appearing as a gas at a temperature that grows with the acceleration. This is the Unruh effect. However, it has been shown that vacuum complexity is an artifact produced by treating quantum field theory in a manner that does not manifestly enforce causality. Choosing a quantization approach that patently enforces causality, the quantum field theory vacuum is barren, bereft even of virtual particles. We show that acceleration has no effect on a trivial vacuum; hence, there is no Unruh effect in such a treatment of quantum field theory. Since the standard calculations suggesting an Unruh effect are formally consistent, insofar as they have been completed, there must be a canceling contribution that is omitted in the usual analyses. We argue that it is the dynamical action of conventional Lorentz transformations on the structure of an Unruh detector.</p>
	]]></content:encoded>

	<dc:title>Poincar&amp;amp;eacute; Invariance and the Unruh Effect</dc:title>
			<dc:creator>Alexandre Deur</dc:creator>
			<dc:creator>Stanley J. Brodsky</dc:creator>
			<dc:creator>Craig D. Roberts</dc:creator>
			<dc:creator>Balša Terzić</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020042</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-22</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-22</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>42</prism:startingPage>
		<prism:doi>10.3390/particles9020042</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/42</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/41">

	<title>Particles, Vol. 9, Pages 41: Observational Diagnostics of a Parametrized Deceleration Parameter in FLRW Cosmology</title>
	<link>https://www.mdpi.com/2571-712X/9/2/41</link>
	<description>The evolution of the deceleration parameter q(z) plays a crucial role in understanding the dynamics of dark energy within the framework of modern cosmology. In this study, we perform a parametric reconstruction of q(z) in a spatially flat Friedmann&amp;amp;ndash;Robertson&amp;amp;ndash;Walker (FLRW) Universe composed of radiation, pressureless dark matter, and dark energy. We consider a physically motivated form of q(z) that effectively describes the transition of the Universe from a decelerating to an accelerating expansion phase. This parametrization is incorporated into the Friedmann equations to derive the corresponding Hubble parameter, which is then confronted with a comprehensive set of observational data, including Hubble parameter measurements H(z), Type Ia supernovae (SNIa), and Baryon Acoustic Oscillations (BAO) data. Employing the Markov Chain Monte Carlo (MCMC) approach, we constrain the model parameters using the combined H(z)+SNIa+BAO dataset. The best-fit parameters are subsequently used to reconstruct the cosmographic quantities, such as the deceleration, jerk, and snap parameters, which provide deeper insight into the expansion history of the Universe. Finally, a comparative analysis with the standard &amp;amp;Lambda;CDM model is carried out to assess the compatibility and effectiveness of the proposed parametrization.</description>
	<pubDate>2026-04-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 41: Observational Diagnostics of a Parametrized Deceleration Parameter in FLRW Cosmology</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/41">doi: 10.3390/particles9020041</a></p>
	<p>Authors:
		Bhupendra Kumar Shukla
		Deger Sofuoğlu
		Aroonkumar Beesham
		Rishi Kumar Tiwari
		Mfanafuthi Siyabonga Msweli
		</p>
	<p>The evolution of the deceleration parameter q(z) plays a crucial role in understanding the dynamics of dark energy within the framework of modern cosmology. In this study, we perform a parametric reconstruction of q(z) in a spatially flat Friedmann&amp;amp;ndash;Robertson&amp;amp;ndash;Walker (FLRW) Universe composed of radiation, pressureless dark matter, and dark energy. We consider a physically motivated form of q(z) that effectively describes the transition of the Universe from a decelerating to an accelerating expansion phase. This parametrization is incorporated into the Friedmann equations to derive the corresponding Hubble parameter, which is then confronted with a comprehensive set of observational data, including Hubble parameter measurements H(z), Type Ia supernovae (SNIa), and Baryon Acoustic Oscillations (BAO) data. Employing the Markov Chain Monte Carlo (MCMC) approach, we constrain the model parameters using the combined H(z)+SNIa+BAO dataset. The best-fit parameters are subsequently used to reconstruct the cosmographic quantities, such as the deceleration, jerk, and snap parameters, which provide deeper insight into the expansion history of the Universe. Finally, a comparative analysis with the standard &amp;amp;Lambda;CDM model is carried out to assess the compatibility and effectiveness of the proposed parametrization.</p>
	]]></content:encoded>

	<dc:title>Observational Diagnostics of a Parametrized Deceleration Parameter in FLRW Cosmology</dc:title>
			<dc:creator>Bhupendra Kumar Shukla</dc:creator>
			<dc:creator>Deger Sofuoğlu</dc:creator>
			<dc:creator>Aroonkumar Beesham</dc:creator>
			<dc:creator>Rishi Kumar Tiwari</dc:creator>
			<dc:creator>Mfanafuthi Siyabonga Msweli</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020041</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-20</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-20</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>41</prism:startingPage>
		<prism:doi>10.3390/particles9020041</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/41</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/40">

	<title>Particles, Vol. 9, Pages 40: &amp;beta; Decay of 20Na</title>
	<link>https://www.mdpi.com/2571-712X/9/2/40</link>
	<description>20Na is a well-known &amp;amp;beta;-delayed &amp;amp;alpha; emitter, owing to the large decay energy of 20Na above the &amp;amp;alpha; + 16O threshold in the A=5&amp;amp;alpha; daughter nucleus 20Ne. In this work, the decay property of 20Na is investigated in detail via the &amp;amp;beta;-&amp;amp;gamma; &amp;amp;beta;-&amp;amp;alpha; and &amp;amp;beta;-&amp;amp;gamma;-&amp;amp;alpha; coincidence spectroscopy. As the day-one experiment of the Beijing Rare Isotope Facility (BRIF), the intense 20Na beam was produced using the Isotope Separator On Line (ISOL) technique through the 100 MeV proton bombarding a stack of MgO as a thick target. Specific interest was focused on the exotic decay mode of 20Na; the previously reported low-energy &amp;amp;alpha; lines at 713 and 846 keV were confirmed, and several weak &amp;amp;beta;-&amp;amp;gamma;-&amp;amp;alpha; decay sequences were clearly identified for the first time, thanks to the strong resolving power of &amp;amp;alpha;-&amp;amp;gamma; coincidence spectroscopy. The decay properties of 20Na are compared to the shell model calculation, which agree reasonably well with the allowed &amp;amp;beta; transition strengths and subsequent electro-magnetic transitions with the use of the sd shell-model space with the USDB interaction.</description>
	<pubDate>2026-04-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 40: &amp;beta; Decay of 20Na</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/40">doi: 10.3390/particles9020040</a></p>
	<p>Authors:
		Qiang Wang
		You-Bao Wang
		Jun Su
		Zhi-Yu Han
		B. Alex Brown
		Li-Hua Chen
		Zi-Qiang Chen
		Bao-Qun Cui
		Bo Dai
		Tao Ge
		Xin-Yue Li
		Yun-Ju Li
		Zhi-Hong Li
		Gang Lian
		Yin-Long Lyu
		Rui-Gang Ma
		Tian-Li Ma
		Xie Ma
		Ying-Jun Ma
		Yi Su
		Bing Tang
		Chun-Guang Wang
		Hong-Yi Wu
		Fu-Rong Xu
		Sheng-Quan Yan
		Sheng Zeng
		Hao Zhang
		Yun Zheng
		Chao Zhou
		Yang-Ping Shen
		Bing Guo
		Tian-Jue Zhang
		Wei-Ping Liu
		</p>
	<p>20Na is a well-known &amp;amp;beta;-delayed &amp;amp;alpha; emitter, owing to the large decay energy of 20Na above the &amp;amp;alpha; + 16O threshold in the A=5&amp;amp;alpha; daughter nucleus 20Ne. In this work, the decay property of 20Na is investigated in detail via the &amp;amp;beta;-&amp;amp;gamma; &amp;amp;beta;-&amp;amp;alpha; and &amp;amp;beta;-&amp;amp;gamma;-&amp;amp;alpha; coincidence spectroscopy. As the day-one experiment of the Beijing Rare Isotope Facility (BRIF), the intense 20Na beam was produced using the Isotope Separator On Line (ISOL) technique through the 100 MeV proton bombarding a stack of MgO as a thick target. Specific interest was focused on the exotic decay mode of 20Na; the previously reported low-energy &amp;amp;alpha; lines at 713 and 846 keV were confirmed, and several weak &amp;amp;beta;-&amp;amp;gamma;-&amp;amp;alpha; decay sequences were clearly identified for the first time, thanks to the strong resolving power of &amp;amp;alpha;-&amp;amp;gamma; coincidence spectroscopy. The decay properties of 20Na are compared to the shell model calculation, which agree reasonably well with the allowed &amp;amp;beta; transition strengths and subsequent electro-magnetic transitions with the use of the sd shell-model space with the USDB interaction.</p>
	]]></content:encoded>

	<dc:title>&amp;amp;beta; Decay of 20Na</dc:title>
			<dc:creator>Qiang Wang</dc:creator>
			<dc:creator>You-Bao Wang</dc:creator>
			<dc:creator>Jun Su</dc:creator>
			<dc:creator>Zhi-Yu Han</dc:creator>
			<dc:creator>B. Alex Brown</dc:creator>
			<dc:creator>Li-Hua Chen</dc:creator>
			<dc:creator>Zi-Qiang Chen</dc:creator>
			<dc:creator>Bao-Qun Cui</dc:creator>
			<dc:creator>Bo Dai</dc:creator>
			<dc:creator>Tao Ge</dc:creator>
			<dc:creator>Xin-Yue Li</dc:creator>
			<dc:creator>Yun-Ju Li</dc:creator>
			<dc:creator>Zhi-Hong Li</dc:creator>
			<dc:creator>Gang Lian</dc:creator>
			<dc:creator>Yin-Long Lyu</dc:creator>
			<dc:creator>Rui-Gang Ma</dc:creator>
			<dc:creator>Tian-Li Ma</dc:creator>
			<dc:creator>Xie Ma</dc:creator>
			<dc:creator>Ying-Jun Ma</dc:creator>
			<dc:creator>Yi Su</dc:creator>
			<dc:creator>Bing Tang</dc:creator>
			<dc:creator>Chun-Guang Wang</dc:creator>
			<dc:creator>Hong-Yi Wu</dc:creator>
			<dc:creator>Fu-Rong Xu</dc:creator>
			<dc:creator>Sheng-Quan Yan</dc:creator>
			<dc:creator>Sheng Zeng</dc:creator>
			<dc:creator>Hao Zhang</dc:creator>
			<dc:creator>Yun Zheng</dc:creator>
			<dc:creator>Chao Zhou</dc:creator>
			<dc:creator>Yang-Ping Shen</dc:creator>
			<dc:creator>Bing Guo</dc:creator>
			<dc:creator>Tian-Jue Zhang</dc:creator>
			<dc:creator>Wei-Ping Liu</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020040</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-17</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-17</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>40</prism:startingPage>
		<prism:doi>10.3390/particles9020040</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/40</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/39">

	<title>Particles, Vol. 9, Pages 39: Leading Low-Temperature Correction to the Heisenberg&amp;ndash;Euler Lagrangian</title>
	<link>https://www.mdpi.com/2571-712X/9/2/39</link>
	<description>In this article, we show that the well-known leading low-temperature correction to the Heisenberg&amp;amp;ndash;Euler Lagrangian in a constant electromagnetic field arising at two loops can be efficiently extracted from its one-loop zero-temperature analogue. Resorting to the real-time formalism of equilibrium quantum field theory that explicitly separates out the zero-temperature contribution from the finite-temperature corrections, the determination becomes essentially trivial. In essence, it only requires taking derivatives of the Heisenberg&amp;amp;ndash;Euler Lagrangian at one loop and zero temperature for the field strength. As a bonus, we then effectively dress the low-temperature contribution at two loops by one-particle reducible tadpole structures. This generates a subset of higher-loop contributions to the Heisenberg&amp;amp;ndash;Euler Lagrangian in the limit of low temperatures. We extract their leading strong-field behavior at a given loop order, and finally resum these to all loop orders.</description>
	<pubDate>2026-04-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 39: Leading Low-Temperature Correction to the Heisenberg&amp;ndash;Euler Lagrangian</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/39">doi: 10.3390/particles9020039</a></p>
	<p>Authors:
		Felix Karbstein
		</p>
	<p>In this article, we show that the well-known leading low-temperature correction to the Heisenberg&amp;amp;ndash;Euler Lagrangian in a constant electromagnetic field arising at two loops can be efficiently extracted from its one-loop zero-temperature analogue. Resorting to the real-time formalism of equilibrium quantum field theory that explicitly separates out the zero-temperature contribution from the finite-temperature corrections, the determination becomes essentially trivial. In essence, it only requires taking derivatives of the Heisenberg&amp;amp;ndash;Euler Lagrangian at one loop and zero temperature for the field strength. As a bonus, we then effectively dress the low-temperature contribution at two loops by one-particle reducible tadpole structures. This generates a subset of higher-loop contributions to the Heisenberg&amp;amp;ndash;Euler Lagrangian in the limit of low temperatures. We extract their leading strong-field behavior at a given loop order, and finally resum these to all loop orders.</p>
	]]></content:encoded>

	<dc:title>Leading Low-Temperature Correction to the Heisenberg&amp;amp;ndash;Euler Lagrangian</dc:title>
			<dc:creator>Felix Karbstein</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020039</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-15</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-15</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>39</prism:startingPage>
		<prism:doi>10.3390/particles9020039</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/39</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/38">

	<title>Particles, Vol. 9, Pages 38: Recent Developments in and Applications of the Relativistic Chiral Nuclear Force</title>
	<link>https://www.mdpi.com/2571-712X/9/2/38</link>
	<description>The nuclear force is central to our understanding of complex nuclear phenomena and to the applications of nuclear techniques. The non-perturbative nature of low-energy strong interaction and color confinement have provided an ab initio understanding of nuclear force, a challenge for almost a century, since the pioneering work of Yukawa. Since 1990, chiral effective field theory (ChEFT) has become the de facto standard for describing nuclear interactions; most prior studies employed heavy-baryon chiral perturbation theory. Only recently, there have been successful attempts to construct a chiral nuclear force employing covariant baryon chiral perturbation theory. In this work, we review recent developments and applications of relativistic chiral nuclear forces. We first elaborate on the necessity of relativistic/covariant theories, then present the construction of the first high-precision relativistic chiral nuclear force up to next-to-next-to-leading order (NNLO), and discuss the ongoing progress in higher-order nucleon&amp;amp;ndash;nucleon (NN) and n-d scattering, as well as their applications in nuclear matter, finite nuclei, and hypernuclear systems. Finally, we summarize the achievements and outline the future outlook of this research field.</description>
	<pubDate>2026-04-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 38: Recent Developments in and Applications of the Relativistic Chiral Nuclear Force</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/38">doi: 10.3390/particles9020038</a></p>
	<p>Authors:
		Li-Sheng Geng
		Jun-Xu Lu
		Qing-Yu Zhai
		Zhi-Wei Liu
		Shi-Hang Shen
		</p>
	<p>The nuclear force is central to our understanding of complex nuclear phenomena and to the applications of nuclear techniques. The non-perturbative nature of low-energy strong interaction and color confinement have provided an ab initio understanding of nuclear force, a challenge for almost a century, since the pioneering work of Yukawa. Since 1990, chiral effective field theory (ChEFT) has become the de facto standard for describing nuclear interactions; most prior studies employed heavy-baryon chiral perturbation theory. Only recently, there have been successful attempts to construct a chiral nuclear force employing covariant baryon chiral perturbation theory. In this work, we review recent developments and applications of relativistic chiral nuclear forces. We first elaborate on the necessity of relativistic/covariant theories, then present the construction of the first high-precision relativistic chiral nuclear force up to next-to-next-to-leading order (NNLO), and discuss the ongoing progress in higher-order nucleon&amp;amp;ndash;nucleon (NN) and n-d scattering, as well as their applications in nuclear matter, finite nuclei, and hypernuclear systems. Finally, we summarize the achievements and outline the future outlook of this research field.</p>
	]]></content:encoded>

	<dc:title>Recent Developments in and Applications of the Relativistic Chiral Nuclear Force</dc:title>
			<dc:creator>Li-Sheng Geng</dc:creator>
			<dc:creator>Jun-Xu Lu</dc:creator>
			<dc:creator>Qing-Yu Zhai</dc:creator>
			<dc:creator>Zhi-Wei Liu</dc:creator>
			<dc:creator>Shi-Hang Shen</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020038</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-04</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>38</prism:startingPage>
		<prism:doi>10.3390/particles9020038</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/38</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/37">

	<title>Particles, Vol. 9, Pages 37: Emergent Higgs Field and the Schwarzschild Black Hole</title>
	<link>https://www.mdpi.com/2571-712X/9/2/37</link>
	<description>The derivations presented in this paper suggest an intimate relationship between geometry and the electroweak sector at the Planck scale. A Lorentz-invariant maximally symmetric stochastically perturbed spacetime transformed to spherical coordinates reveals an emergent Schwarzschild metric, entirely a statistical structure of stochastic spacetime. Similarly, the transition from a maximally symmetric universe with a complex SU(2) scalar doublet &amp;amp;#981;, comprising four independent real scalar fields with a zero vacuum expectation value (VEV), to spherical coordinates at the Planck scale reveals the spontaneously broken electroweak (EW) sector. Working in the unitarity gauge, the resulting EW potential can be simultaneously mapped in space at the Planck scale and across the EW sector. In space, the resulting EW potential includes a deep well within the Schwarzschild sphere and a shallow well just outside corresponding to an accretion disk. The same potential mapped in the EW space provides an entire family of possible sombrero hat potentials with fourth-order coupling specific to a point in space. At the minimum points of the potential in space, inside the Schwarzschild sphere and at the accretion disk, the &amp;amp;lambda; corresponding to the Standard Model (SM) fourth-order coupling is instead derived as &amp;amp;lambda;5. The factor of 15 is a simple consequence of the conservation of the EW VEV and the fact that the SM formulation of the EW potential does not account for situations where the perturbations in &amp;amp;#981; dominate. A more general formulation of the EW potential restores the SM quartic coupling and preserves &amp;amp;lambda; in space. An emergent Higgs field inside the Schwarzschild black hole is found to directly relate to the stochastic spacetime fields normalized by the Schwarzschild radius. The corresponding Higgs vacuum has both a ground and excited state and the possibility of both positive and negative vacuum entropy. Finally, the scalar-field VEV degeneracy in EW space of the metastable Higgs vacuum appears instead differentiated in space with possible probability, tunneling, and entropy implications.</description>
	<pubDate>2026-04-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 37: Emergent Higgs Field and the Schwarzschild Black Hole</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/37">doi: 10.3390/particles9020037</a></p>
	<p>Authors:
		Dragana Pilipović
		</p>
	<p>The derivations presented in this paper suggest an intimate relationship between geometry and the electroweak sector at the Planck scale. A Lorentz-invariant maximally symmetric stochastically perturbed spacetime transformed to spherical coordinates reveals an emergent Schwarzschild metric, entirely a statistical structure of stochastic spacetime. Similarly, the transition from a maximally symmetric universe with a complex SU(2) scalar doublet &amp;amp;#981;, comprising four independent real scalar fields with a zero vacuum expectation value (VEV), to spherical coordinates at the Planck scale reveals the spontaneously broken electroweak (EW) sector. Working in the unitarity gauge, the resulting EW potential can be simultaneously mapped in space at the Planck scale and across the EW sector. In space, the resulting EW potential includes a deep well within the Schwarzschild sphere and a shallow well just outside corresponding to an accretion disk. The same potential mapped in the EW space provides an entire family of possible sombrero hat potentials with fourth-order coupling specific to a point in space. At the minimum points of the potential in space, inside the Schwarzschild sphere and at the accretion disk, the &amp;amp;lambda; corresponding to the Standard Model (SM) fourth-order coupling is instead derived as &amp;amp;lambda;5. The factor of 15 is a simple consequence of the conservation of the EW VEV and the fact that the SM formulation of the EW potential does not account for situations where the perturbations in &amp;amp;#981; dominate. A more general formulation of the EW potential restores the SM quartic coupling and preserves &amp;amp;lambda; in space. An emergent Higgs field inside the Schwarzschild black hole is found to directly relate to the stochastic spacetime fields normalized by the Schwarzschild radius. The corresponding Higgs vacuum has both a ground and excited state and the possibility of both positive and negative vacuum entropy. Finally, the scalar-field VEV degeneracy in EW space of the metastable Higgs vacuum appears instead differentiated in space with possible probability, tunneling, and entropy implications.</p>
	]]></content:encoded>

	<dc:title>Emergent Higgs Field and the Schwarzschild Black Hole</dc:title>
			<dc:creator>Dragana Pilipović</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020037</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-03</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-03</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>37</prism:startingPage>
		<prism:doi>10.3390/particles9020037</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/37</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/35">

	<title>Particles, Vol. 9, Pages 35: Searching for Stable States in the TDD1 Systems Based on a Chiral Quark Model</title>
	<link>https://www.mdpi.com/2571-712X/9/2/35</link>
	<description>Experimentally, the 1+ state X(3872) was first discovered, and subsequently, its partner state Y(4260), with the same quark content (cq&amp;amp;macr;qc&amp;amp;macr;) and quantum number 1&amp;amp;minus; was also observed. Inspired by this pattern, we systematically investigate the newly discovered 1+ state Tcc and its possible 1&amp;amp;minus; partner, the TDD1 system with the same quark content (cq&amp;amp;macr;cq&amp;amp;macr;). Within the framework of the chiral quark model, we perform a comprehensive study of the bound and resonance states of TDD1 using the Gaussian expansion method (GEM). Two quark configurations, the molecular structure and the diquark structure, are considered in our calculations. Our results indicate the existence of a shallow bound state dominated by the DD1* channel, which is analogous to the experimentally observed Tcc, as well as two compact resonant states with narrow widths around 4.5 GeV. To avoid the influence of model parameters on the results, we additionally fitted a new set of parameters and obtained consistent conclusions. According to our calculation results, although the color-octet and diquark configurations have relatively high energies, the channel-coupling effects induced by them play a crucial role in the formation of these stable states. We strongly encourage experimental efforts to search for the stable states predicted in the TDD1 system.</description>
	<pubDate>2026-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 35: Searching for Stable States in the TDD1 Systems Based on a Chiral Quark Model</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/35">doi: 10.3390/particles9020035</a></p>
	<p>Authors:
		Yuheng Wu
		Linkai Li
		Yuheng Xing
		Xinxing Wu
		Yue Tan
		</p>
	<p>Experimentally, the 1+ state X(3872) was first discovered, and subsequently, its partner state Y(4260), with the same quark content (cq&amp;amp;macr;qc&amp;amp;macr;) and quantum number 1&amp;amp;minus; was also observed. Inspired by this pattern, we systematically investigate the newly discovered 1+ state Tcc and its possible 1&amp;amp;minus; partner, the TDD1 system with the same quark content (cq&amp;amp;macr;cq&amp;amp;macr;). Within the framework of the chiral quark model, we perform a comprehensive study of the bound and resonance states of TDD1 using the Gaussian expansion method (GEM). Two quark configurations, the molecular structure and the diquark structure, are considered in our calculations. Our results indicate the existence of a shallow bound state dominated by the DD1* channel, which is analogous to the experimentally observed Tcc, as well as two compact resonant states with narrow widths around 4.5 GeV. To avoid the influence of model parameters on the results, we additionally fitted a new set of parameters and obtained consistent conclusions. According to our calculation results, although the color-octet and diquark configurations have relatively high energies, the channel-coupling effects induced by them play a crucial role in the formation of these stable states. We strongly encourage experimental efforts to search for the stable states predicted in the TDD1 system.</p>
	]]></content:encoded>

	<dc:title>Searching for Stable States in the TDD1 Systems Based on a Chiral Quark Model</dc:title>
			<dc:creator>Yuheng Wu</dc:creator>
			<dc:creator>Linkai Li</dc:creator>
			<dc:creator>Yuheng Xing</dc:creator>
			<dc:creator>Xinxing Wu</dc:creator>
			<dc:creator>Yue Tan</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020035</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>35</prism:startingPage>
		<prism:doi>10.3390/particles9020035</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/35</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/36">

	<title>Particles, Vol. 9, Pages 36: Description of 29F and 31F Within the Deformed Relativistic Hartree&amp;ndash;Bogoliubov Theory in Continuum</title>
	<link>https://www.mdpi.com/2571-712X/9/2/36</link>
	<description>The experimental exploration of halo nuclei over the past four decades has established ground-state halo phenomena in about twenty nuclei, providing important benchmarks for modern nuclear theories. The deformed relativistic Hartree&amp;amp;ndash;Bogoliubov theory in continuum (DRHBc) has been successfully applied to describe known halo nuclei and to predict new candidates during the last dozen years. In this work, the possible two-neutron halo nuclei F29 and F31 are investigated within the DRHBc framework. In the spherical limit, an inversion between the 2p3/2 and 1f7/2 orbitals is obtained relative to the conventional single-particle ordering, which plays a crucial role in the formation of deformed halos in these nuclei. Assuming a prolate deformation with &amp;amp;beta;2&amp;amp;asymp;0.4, as suggested in previous studies, a deformed two-neutron halo in F29 is reproduced. For F31, a well-deformed ground state with &amp;amp;beta;2&amp;amp;asymp;0.24 and a more pronounced two-neutron halo emerge self-consistently.</description>
	<pubDate>2026-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 36: Description of 29F and 31F Within the Deformed Relativistic Hartree&amp;ndash;Bogoliubov Theory in Continuum</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/36">doi: 10.3390/particles9020036</a></p>
	<p>Authors:
		Kaiyuan Zhang
		Ling Li
		Jie Yan
		Guixiang Ye
		Xinhui Wu
		Jia-Lin An
		Shi-Sheng Zhang
		Cong Pan
		Xiang-Xiang Sun
		</p>
	<p>The experimental exploration of halo nuclei over the past four decades has established ground-state halo phenomena in about twenty nuclei, providing important benchmarks for modern nuclear theories. The deformed relativistic Hartree&amp;amp;ndash;Bogoliubov theory in continuum (DRHBc) has been successfully applied to describe known halo nuclei and to predict new candidates during the last dozen years. In this work, the possible two-neutron halo nuclei F29 and F31 are investigated within the DRHBc framework. In the spherical limit, an inversion between the 2p3/2 and 1f7/2 orbitals is obtained relative to the conventional single-particle ordering, which plays a crucial role in the formation of deformed halos in these nuclei. Assuming a prolate deformation with &amp;amp;beta;2&amp;amp;asymp;0.4, as suggested in previous studies, a deformed two-neutron halo in F29 is reproduced. For F31, a well-deformed ground state with &amp;amp;beta;2&amp;amp;asymp;0.24 and a more pronounced two-neutron halo emerge self-consistently.</p>
	]]></content:encoded>

	<dc:title>Description of 29F and 31F Within the Deformed Relativistic Hartree&amp;amp;ndash;Bogoliubov Theory in Continuum</dc:title>
			<dc:creator>Kaiyuan Zhang</dc:creator>
			<dc:creator>Ling Li</dc:creator>
			<dc:creator>Jie Yan</dc:creator>
			<dc:creator>Guixiang Ye</dc:creator>
			<dc:creator>Xinhui Wu</dc:creator>
			<dc:creator>Jia-Lin An</dc:creator>
			<dc:creator>Shi-Sheng Zhang</dc:creator>
			<dc:creator>Cong Pan</dc:creator>
			<dc:creator>Xiang-Xiang Sun</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020036</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>36</prism:startingPage>
		<prism:doi>10.3390/particles9020036</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/36</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/34">

	<title>Particles, Vol. 9, Pages 34: Current Status and Future Prospects of the LHCf Experiment</title>
	<link>https://www.mdpi.com/2571-712X/9/2/34</link>
	<description>The Large Hadron Collider forward (LHCf) experiment studies the production of neutral particles in the very forward region of high-energy hadronic collisions at the LHC. These measurements provide essential calibration data for hadronic interaction models used in simulations of extensive air showers initiated by ultra-high-energy cosmic rays. The LHCf experiment measures forward-produced neutral particles, such as neutrons, photons, &amp;amp;pi;0, and &amp;amp;eta; mesons, which play a key role in the development of extensive air showers. Proton&amp;amp;ndash;proton collisions at the LHC reach center-of-mass energies up to 13.6 TeV, corresponding in the fixed-target frame to cosmic-ray interactions at energies close to 1017 eV in the Earth&amp;amp;rsquo;s atmosphere. LHCf has collected data in proton&amp;amp;ndash;proton collisions at several energies, as well as in proton&amp;amp;ndash;lead collisions, enabling detailed comparisons between experimental results and predictions of hadronic interaction models. This contribution reviews the most significant LHCf results, with emphasis on Run II proton&amp;amp;ndash;proton data at s=13TeV, including measurements of forward neutron, photon, and &amp;amp;eta; meson production. Finally, future prospects are discussed, focusing on ongoing analyses of Run III proton&amp;amp;ndash;proton data at s=13.6TeV and on the final LHCf operation in proton-oxygen collisions at sNN=9.6TeV, which best reproduces cosmic-ray interactions with nuclei of the Earth&amp;amp;rsquo;s atmosphere.</description>
	<pubDate>2026-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 34: Current Status and Future Prospects of the LHCf Experiment</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/34">doi: 10.3390/particles9020034</a></p>
	<p>Authors:
		Oscar Adriani
		Eugenio Berti
		Pietro Betti
		Lorenzo Bonechi
		Massimo Bongi
		Raffaello D’Alessandro
		Sebastiano Detti
		Elena Gensini
		Elena Geraci
		Maurice Haguenauer
		Vlera Hajdini
		Cigdem Issever
		Yoshitaka Itow
		Katsuaki Kasahara
		Haruka Kobayashi
		Clara Leitgeb
		Yutaka Matsubara
		Hiroaki Menjo
		Yasushi Muraki
		Andrea Paccagnella
		Paolo Papini
		Giuseppe Piparo
		Sergio Bruno Ricciarini
		Takashi Sako
		Nobuyuki Sakurai
		Monica Scaringella
		Yuki Shimizu
		Tadashi Tamura
		Alessio Tiberio
		Shoji Torii
		Alessia Tricomi
		Bill Turner
		Kenji Yoshida
		</p>
	<p>The Large Hadron Collider forward (LHCf) experiment studies the production of neutral particles in the very forward region of high-energy hadronic collisions at the LHC. These measurements provide essential calibration data for hadronic interaction models used in simulations of extensive air showers initiated by ultra-high-energy cosmic rays. The LHCf experiment measures forward-produced neutral particles, such as neutrons, photons, &amp;amp;pi;0, and &amp;amp;eta; mesons, which play a key role in the development of extensive air showers. Proton&amp;amp;ndash;proton collisions at the LHC reach center-of-mass energies up to 13.6 TeV, corresponding in the fixed-target frame to cosmic-ray interactions at energies close to 1017 eV in the Earth&amp;amp;rsquo;s atmosphere. LHCf has collected data in proton&amp;amp;ndash;proton collisions at several energies, as well as in proton&amp;amp;ndash;lead collisions, enabling detailed comparisons between experimental results and predictions of hadronic interaction models. This contribution reviews the most significant LHCf results, with emphasis on Run II proton&amp;amp;ndash;proton data at s=13TeV, including measurements of forward neutron, photon, and &amp;amp;eta; meson production. Finally, future prospects are discussed, focusing on ongoing analyses of Run III proton&amp;amp;ndash;proton data at s=13.6TeV and on the final LHCf operation in proton-oxygen collisions at sNN=9.6TeV, which best reproduces cosmic-ray interactions with nuclei of the Earth&amp;amp;rsquo;s atmosphere.</p>
	]]></content:encoded>

	<dc:title>Current Status and Future Prospects of the LHCf Experiment</dc:title>
			<dc:creator>Oscar Adriani</dc:creator>
			<dc:creator>Eugenio Berti</dc:creator>
			<dc:creator>Pietro Betti</dc:creator>
			<dc:creator>Lorenzo Bonechi</dc:creator>
			<dc:creator>Massimo Bongi</dc:creator>
			<dc:creator>Raffaello D’Alessandro</dc:creator>
			<dc:creator>Sebastiano Detti</dc:creator>
			<dc:creator>Elena Gensini</dc:creator>
			<dc:creator>Elena Geraci</dc:creator>
			<dc:creator>Maurice Haguenauer</dc:creator>
			<dc:creator>Vlera Hajdini</dc:creator>
			<dc:creator>Cigdem Issever</dc:creator>
			<dc:creator>Yoshitaka Itow</dc:creator>
			<dc:creator>Katsuaki Kasahara</dc:creator>
			<dc:creator>Haruka Kobayashi</dc:creator>
			<dc:creator>Clara Leitgeb</dc:creator>
			<dc:creator>Yutaka Matsubara</dc:creator>
			<dc:creator>Hiroaki Menjo</dc:creator>
			<dc:creator>Yasushi Muraki</dc:creator>
			<dc:creator>Andrea Paccagnella</dc:creator>
			<dc:creator>Paolo Papini</dc:creator>
			<dc:creator>Giuseppe Piparo</dc:creator>
			<dc:creator>Sergio Bruno Ricciarini</dc:creator>
			<dc:creator>Takashi Sako</dc:creator>
			<dc:creator>Nobuyuki Sakurai</dc:creator>
			<dc:creator>Monica Scaringella</dc:creator>
			<dc:creator>Yuki Shimizu</dc:creator>
			<dc:creator>Tadashi Tamura</dc:creator>
			<dc:creator>Alessio Tiberio</dc:creator>
			<dc:creator>Shoji Torii</dc:creator>
			<dc:creator>Alessia Tricomi</dc:creator>
			<dc:creator>Bill Turner</dc:creator>
			<dc:creator>Kenji Yoshida</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020034</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>34</prism:startingPage>
		<prism:doi>10.3390/particles9020034</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/34</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/33">

	<title>Particles, Vol. 9, Pages 33: Complexity: What Is It?</title>
	<link>https://www.mdpi.com/2571-712X/9/2/33</link>
	<description>On the basis of the correlations of distant&amp;amp;mdash;in time and/or in space&amp;amp;mdash;elements of a many-element system, we propose the hard core of a mathematical definition of what may be referred to as complexity. This definition consistently leads to the concept of degree of complexity.</description>
	<pubDate>2026-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 33: Complexity: What Is It?</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/33">doi: 10.3390/particles9020033</a></p>
	<p>Authors:
		Constantino Tsallis
		</p>
	<p>On the basis of the correlations of distant&amp;amp;mdash;in time and/or in space&amp;amp;mdash;elements of a many-element system, we propose the hard core of a mathematical definition of what may be referred to as complexity. This definition consistently leads to the concept of degree of complexity.</p>
	]]></content:encoded>

	<dc:title>Complexity: What Is It?</dc:title>
			<dc:creator>Constantino Tsallis</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020033</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Perspective</prism:section>
	<prism:startingPage>33</prism:startingPage>
		<prism:doi>10.3390/particles9020033</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/33</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/32">

	<title>Particles, Vol. 9, Pages 32: Progress on the Proton Decays of A &amp;sim; 20 Nuclei Around the Proton Drip Line</title>
	<link>https://www.mdpi.com/2571-712X/9/2/32</link>
	<description>Experimental studies on the spontaneous nucleon emission in nuclei around the drip line enable us to explore new isotopes or resonant states, and to reveal exotic structures and decay properties of nuclei located far from the &amp;amp;beta; stability line; consequently, they are of critical importance for probing limits of nuclear stability and understanding nucleon&amp;amp;ndash;nucleon interactions under extreme conditions of isospin asymmetry. With the radioactive isotope beam 20Mg provided by the National Superconducting Cyclotron Laboratory at Michigan State University, we studied the proton decays of nuclei around the proton drip line at A&amp;amp;sim;20 mass region. Complete-kinematics measurements were performed for proton decays of one-proton resonant states in 18Na, two-proton resonant states in 20Mg, three-proton resonant states in 21Al, and four-proton resonant states in 18Mg, yielding decay energy spectra for all four nuclei. With the invariant mass method, the ground state of 18Na was firmly identified, clarifying previous ambiguities of its position. The isotope 18Mg, which is located two neutrons beyond the proton drip line, was experimentally observed for the first time. Multi-body correlation analysis of emitted protons from 20Mg, 21Al, and 18Mg, combined with Monte Carlo simulations, reveals that the identified resonant states in 20Mg and 21Al predominantly decay via two and three sequential steps of 1p emission, respectively, whereas the 18Mg ground state decays mainly through a two-step cascade of prompt 2p emission.</description>
	<pubDate>2026-04-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 32: Progress on the Proton Decays of A &amp;sim; 20 Nuclei Around the Proton Drip Line</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/32">doi: 10.3390/particles9020032</a></p>
	<p>Authors:
		Lei Ni
		Yu Jin
		Hui Hua
		Zhihuan Li
		</p>
	<p>Experimental studies on the spontaneous nucleon emission in nuclei around the drip line enable us to explore new isotopes or resonant states, and to reveal exotic structures and decay properties of nuclei located far from the &amp;amp;beta; stability line; consequently, they are of critical importance for probing limits of nuclear stability and understanding nucleon&amp;amp;ndash;nucleon interactions under extreme conditions of isospin asymmetry. With the radioactive isotope beam 20Mg provided by the National Superconducting Cyclotron Laboratory at Michigan State University, we studied the proton decays of nuclei around the proton drip line at A&amp;amp;sim;20 mass region. Complete-kinematics measurements were performed for proton decays of one-proton resonant states in 18Na, two-proton resonant states in 20Mg, three-proton resonant states in 21Al, and four-proton resonant states in 18Mg, yielding decay energy spectra for all four nuclei. With the invariant mass method, the ground state of 18Na was firmly identified, clarifying previous ambiguities of its position. The isotope 18Mg, which is located two neutrons beyond the proton drip line, was experimentally observed for the first time. Multi-body correlation analysis of emitted protons from 20Mg, 21Al, and 18Mg, combined with Monte Carlo simulations, reveals that the identified resonant states in 20Mg and 21Al predominantly decay via two and three sequential steps of 1p emission, respectively, whereas the 18Mg ground state decays mainly through a two-step cascade of prompt 2p emission.</p>
	]]></content:encoded>

	<dc:title>Progress on the Proton Decays of A &amp;amp;sim; 20 Nuclei Around the Proton Drip Line</dc:title>
			<dc:creator>Lei Ni</dc:creator>
			<dc:creator>Yu Jin</dc:creator>
			<dc:creator>Hui Hua</dc:creator>
			<dc:creator>Zhihuan Li</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020032</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-04-01</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-04-01</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>32</prism:startingPage>
		<prism:doi>10.3390/particles9020032</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/32</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/31">

	<title>Particles, Vol. 9, Pages 31: Concept of Isomer Beam Production with Heavy-Ion Storage Rings</title>
	<link>https://www.mdpi.com/2571-712X/9/2/31</link>
	<description>Heavy radioactive ion beams produced by in-flight techniques often involve long-lived excited states (isomers). This presents a challenge for reaction studies because none of the existing fragment separators worldwide can resolve isomers in-flight. Here, we propose a novel scheme to produce tagged cocktail beams or pure isomer beams using an ion storage ring. The mass resolving powers of storage rings enable us to identify and separate ions of the isomeric state from the corresponding ground state in a secondary beam. For short-lived isomers, the Rare-RI Ring (R3) facility at the RI Beam Factory (RIBF) will be available, while for long-lived isomers the Experimental Storage Ring (ESR) at the GSI/FAIR facility will be utilized. Isomers often have spins and deformations significantly different from the ground states. Studying isomer structures will provide unique insight into their specific interactions, opening a new frontier in reaction studies with radioactive ion beams in the coming years.</description>
	<pubDate>2026-03-29</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 31: Concept of Isomer Beam Production with Heavy-Ion Storage Rings</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/31">doi: 10.3390/particles9020031</a></p>
	<p>Authors:
		Takayuki Yamaguchi
		Yoshitaka Yamaguchi
		Tetsuya Ohnishi
		Daisuke Nagae
		Yury A. Litvinov
		</p>
	<p>Heavy radioactive ion beams produced by in-flight techniques often involve long-lived excited states (isomers). This presents a challenge for reaction studies because none of the existing fragment separators worldwide can resolve isomers in-flight. Here, we propose a novel scheme to produce tagged cocktail beams or pure isomer beams using an ion storage ring. The mass resolving powers of storage rings enable us to identify and separate ions of the isomeric state from the corresponding ground state in a secondary beam. For short-lived isomers, the Rare-RI Ring (R3) facility at the RI Beam Factory (RIBF) will be available, while for long-lived isomers the Experimental Storage Ring (ESR) at the GSI/FAIR facility will be utilized. Isomers often have spins and deformations significantly different from the ground states. Studying isomer structures will provide unique insight into their specific interactions, opening a new frontier in reaction studies with radioactive ion beams in the coming years.</p>
	]]></content:encoded>

	<dc:title>Concept of Isomer Beam Production with Heavy-Ion Storage Rings</dc:title>
			<dc:creator>Takayuki Yamaguchi</dc:creator>
			<dc:creator>Yoshitaka Yamaguchi</dc:creator>
			<dc:creator>Tetsuya Ohnishi</dc:creator>
			<dc:creator>Daisuke Nagae</dc:creator>
			<dc:creator>Yury A. Litvinov</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020031</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-29</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-29</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>31</prism:startingPage>
		<prism:doi>10.3390/particles9020031</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/31</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/2/30">

	<title>Particles, Vol. 9, Pages 30: Instruments for Focal Plane X-Ray Polarimetry in the Next Decade</title>
	<link>https://www.mdpi.com/2571-712X/9/2/30</link>
	<description>The successful detection of X-ray polarization from many celestial sources belonging to different classes by the IXPE mission has opened a new window in X-ray astronomy. While an impressive number of scientific topics have already been addressed by IXPE, many of them would benefit from a new class of instrumentation that could be launched on a relatively short time scale. In this contribution, we present the development activities of a focal-plane polarimeter whose goal is to extend the energy range of IXPE up to tens of keV, with better sensitivity and lower background. Our design is based on the use of multilayer mirrors and stacked instrumentation, comprising either a low- or medium-energy imaging photoelectric polarimeter and an active Compton polarimeter. Such an approach relies on hardware with flight heritage and&amp;amp;mdash;although still under development for the specific application in X-ray polarimetry&amp;amp;mdash;it has the potential to answer compelling scientific questions and to soon become competitive from the point of view of feasibility for space applications.</description>
	<pubDate>2026-03-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 30: Instruments for Focal Plane X-Ray Polarimetry in the Next Decade</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/2/30">doi: 10.3390/particles9020030</a></p>
	<p>Authors:
		Fabio Muleri
		Stefano Cesare
		Enrico Costa
		Walter Cugno
		Klaus Desch
		Alessandro Di Marco
		Sergio Fabiani
		Riccardo Ferrazzoli
		Markus Gruber
		Daniel Heuchel
		Saba Imtiaz
		Jochen Kaminski
		Dawoon Edwin Kim
		Alessandro Lacerenza
		Carlo Lefevre
		Hemanth Manikantan
		Vladislavs Plesanovs
		John Rankin
		Ajay Ratheesh
		Alda Rubini
		Paolo Soffitta
		</p>
	<p>The successful detection of X-ray polarization from many celestial sources belonging to different classes by the IXPE mission has opened a new window in X-ray astronomy. While an impressive number of scientific topics have already been addressed by IXPE, many of them would benefit from a new class of instrumentation that could be launched on a relatively short time scale. In this contribution, we present the development activities of a focal-plane polarimeter whose goal is to extend the energy range of IXPE up to tens of keV, with better sensitivity and lower background. Our design is based on the use of multilayer mirrors and stacked instrumentation, comprising either a low- or medium-energy imaging photoelectric polarimeter and an active Compton polarimeter. Such an approach relies on hardware with flight heritage and&amp;amp;mdash;although still under development for the specific application in X-ray polarimetry&amp;amp;mdash;it has the potential to answer compelling scientific questions and to soon become competitive from the point of view of feasibility for space applications.</p>
	]]></content:encoded>

	<dc:title>Instruments for Focal Plane X-Ray Polarimetry in the Next Decade</dc:title>
			<dc:creator>Fabio Muleri</dc:creator>
			<dc:creator>Stefano Cesare</dc:creator>
			<dc:creator>Enrico Costa</dc:creator>
			<dc:creator>Walter Cugno</dc:creator>
			<dc:creator>Klaus Desch</dc:creator>
			<dc:creator>Alessandro Di Marco</dc:creator>
			<dc:creator>Sergio Fabiani</dc:creator>
			<dc:creator>Riccardo Ferrazzoli</dc:creator>
			<dc:creator>Markus Gruber</dc:creator>
			<dc:creator>Daniel Heuchel</dc:creator>
			<dc:creator>Saba Imtiaz</dc:creator>
			<dc:creator>Jochen Kaminski</dc:creator>
			<dc:creator>Dawoon Edwin Kim</dc:creator>
			<dc:creator>Alessandro Lacerenza</dc:creator>
			<dc:creator>Carlo Lefevre</dc:creator>
			<dc:creator>Hemanth Manikantan</dc:creator>
			<dc:creator>Vladislavs Plesanovs</dc:creator>
			<dc:creator>John Rankin</dc:creator>
			<dc:creator>Ajay Ratheesh</dc:creator>
			<dc:creator>Alda Rubini</dc:creator>
			<dc:creator>Paolo Soffitta</dc:creator>
		<dc:identifier>doi: 10.3390/particles9020030</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-24</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-24</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>30</prism:startingPage>
		<prism:doi>10.3390/particles9020030</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/2/30</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/29">

	<title>Particles, Vol. 9, Pages 29: Magnetodynamic Characteristics of QGP Energy Dissipation in RMHD Framework with Relativistic Heavy-Ion Collisions</title>
	<link>https://www.mdpi.com/2571-712X/9/1/29</link>
	<description>Relativistic heavy-ion collisions generate ultra-strong magnetic fields that interact with the quark&amp;amp;ndash;gluon plasma (QGP), a key focus of high-energy physics research. This study investigates QGP energy density evolution under time-dependent magnetic fields within a (1 + 1)D relativistic magnetohydrodynamic (RMHD) framework integrated with Bjorken flow. Three magnetic field temporal evolution models (Type-1, Type-2, Type-3) are analyzed for two different equations of state: (1) p=cs2e (simplified ultra-relativistic), and (2) p=cs2e&amp;amp;minus;2MB (magnetized conformal), incorporating a temperature-dependent magnetic susceptibility derived from lattice QCD. Results show that stronger magnetic fields consistently suppress QGP energy density decay, with suppression magnitude dependent on the magnetic field&amp;amp;rsquo;s temporal profile. Ultra-relativistic fluids exhibit slowed energy decay due to magnetic pressure counteracting hydrodynamic expansion. In contrast, magnetized conformal fluids display faster energy dissipation under identical conditions, arising from the synergistic effect of enhanced magnetic fluid coupling, increased energy dissipation during interaction, and QGP&amp;amp;rsquo;s perfect fluid expansion at elevated temperatures. Temperature-dependent magnetic susceptibility reveals a transition from diamagnetic (confined phase) to paramagnetic (deconfined QGP phase) behavior, introducing a feedback mechanism that strengthens energy retention at higher temperatures. This work clarifies the interplay between magnetic field dynamics, QCD phase structure, and hydrodynamic expansion, providing key observational signatures for distinguishing fluid types in heavy-ion collisions and advancing realistic modeling of magnetized QGP.</description>
	<pubDate>2026-03-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 29: Magnetodynamic Characteristics of QGP Energy Dissipation in RMHD Framework with Relativistic Heavy-Ion Collisions</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/29">doi: 10.3390/particles9010029</a></p>
	<p>Authors:
		Huang-Jing Zheng
		Sheng-Qin Feng
		</p>
	<p>Relativistic heavy-ion collisions generate ultra-strong magnetic fields that interact with the quark&amp;amp;ndash;gluon plasma (QGP), a key focus of high-energy physics research. This study investigates QGP energy density evolution under time-dependent magnetic fields within a (1 + 1)D relativistic magnetohydrodynamic (RMHD) framework integrated with Bjorken flow. Three magnetic field temporal evolution models (Type-1, Type-2, Type-3) are analyzed for two different equations of state: (1) p=cs2e (simplified ultra-relativistic), and (2) p=cs2e&amp;amp;minus;2MB (magnetized conformal), incorporating a temperature-dependent magnetic susceptibility derived from lattice QCD. Results show that stronger magnetic fields consistently suppress QGP energy density decay, with suppression magnitude dependent on the magnetic field&amp;amp;rsquo;s temporal profile. Ultra-relativistic fluids exhibit slowed energy decay due to magnetic pressure counteracting hydrodynamic expansion. In contrast, magnetized conformal fluids display faster energy dissipation under identical conditions, arising from the synergistic effect of enhanced magnetic fluid coupling, increased energy dissipation during interaction, and QGP&amp;amp;rsquo;s perfect fluid expansion at elevated temperatures. Temperature-dependent magnetic susceptibility reveals a transition from diamagnetic (confined phase) to paramagnetic (deconfined QGP phase) behavior, introducing a feedback mechanism that strengthens energy retention at higher temperatures. This work clarifies the interplay between magnetic field dynamics, QCD phase structure, and hydrodynamic expansion, providing key observational signatures for distinguishing fluid types in heavy-ion collisions and advancing realistic modeling of magnetized QGP.</p>
	]]></content:encoded>

	<dc:title>Magnetodynamic Characteristics of QGP Energy Dissipation in RMHD Framework with Relativistic Heavy-Ion Collisions</dc:title>
			<dc:creator>Huang-Jing Zheng</dc:creator>
			<dc:creator>Sheng-Qin Feng</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010029</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-19</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-19</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>29</prism:startingPage>
		<prism:doi>10.3390/particles9010029</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/29</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/28">

	<title>Particles, Vol. 9, Pages 28: Nanofusion: Plasmons Help to Accelerate Protons</title>
	<link>https://www.mdpi.com/2571-712X/9/1/28</link>
	<description>We report on laser fusion research with nanotechnology-improved targets embedded in special polymers. The results of the last three years are reviewed here, including laser matter interaction craters, laser infrared breakdown spectroscopy, and Raman spectroscopy results, as well as a selected Thomson parabola image showing protons accelerated up to 300 keV. In this paper, we focus on proton acceleration and plasmonic enhancement mechanisms rather than on the direct demonstration of sustained fusion reactions.</description>
	<pubDate>2026-03-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 28: Nanofusion: Plasmons Help to Accelerate Protons</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/28">doi: 10.3390/particles9010028</a></p>
	<p>Authors:
		Tamás Biró
		</p>
	<p>We report on laser fusion research with nanotechnology-improved targets embedded in special polymers. The results of the last three years are reviewed here, including laser matter interaction craters, laser infrared breakdown spectroscopy, and Raman spectroscopy results, as well as a selected Thomson parabola image showing protons accelerated up to 300 keV. In this paper, we focus on proton acceleration and plasmonic enhancement mechanisms rather than on the direct demonstration of sustained fusion reactions.</p>
	]]></content:encoded>

	<dc:title>Nanofusion: Plasmons Help to Accelerate Protons</dc:title>
			<dc:creator>Tamás Biró</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010028</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-19</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-19</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>28</prism:startingPage>
		<prism:doi>10.3390/particles9010028</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/28</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/27">

	<title>Particles, Vol. 9, Pages 27: Halos and Multineutron Correlations in Light Neutron-Rich Nuclei</title>
	<link>https://www.mdpi.com/2571-712X/9/1/27</link>
	<description>This review summarizes recent experimental progress in the structure and correlations of light neutron-rich nuclei. We first highlight achievements based on quasi-free scattering reactions in inverse kinematics at the Radioactive Isotope Beam Factory (RIBF), including investigations of the single-particle composition of halo systems&amp;amp;mdash;for example, revealing the minimal s-wave component in the &amp;amp;ldquo;weak-halo&amp;amp;rdquo; nucleus 17B&amp;amp;mdash;and the mapping of universal, surface-localized dineutron correlations in Borromean nuclei such as 11Li, 14Be and 17B. We then discuss recent advances in the study of multineutron correlations and cluster states, addressing both experimental challenges and major breakthroughs. These include the observation of a candidate 4n resonance, the absence of a resonant state in the 3n system, the characterization of direct two-neutron decay in 16Be, and evidence for a condensate-like &amp;amp;alpha;+n2+n2 cluster structure in the He8(02+) state. Finally, we discuss prospects for extending such investigations to heavier halo candidates and more complex multineutron systems, and outline the development of next-generation neutron detector arrays that will drive future progress in this field.</description>
	<pubDate>2026-03-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 27: Halos and Multineutron Correlations in Light Neutron-Rich Nuclei</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/27">doi: 10.3390/particles9010027</a></p>
	<p>Authors:
		Zheyang Lin
		Zaihong Yang
		</p>
	<p>This review summarizes recent experimental progress in the structure and correlations of light neutron-rich nuclei. We first highlight achievements based on quasi-free scattering reactions in inverse kinematics at the Radioactive Isotope Beam Factory (RIBF), including investigations of the single-particle composition of halo systems&amp;amp;mdash;for example, revealing the minimal s-wave component in the &amp;amp;ldquo;weak-halo&amp;amp;rdquo; nucleus 17B&amp;amp;mdash;and the mapping of universal, surface-localized dineutron correlations in Borromean nuclei such as 11Li, 14Be and 17B. We then discuss recent advances in the study of multineutron correlations and cluster states, addressing both experimental challenges and major breakthroughs. These include the observation of a candidate 4n resonance, the absence of a resonant state in the 3n system, the characterization of direct two-neutron decay in 16Be, and evidence for a condensate-like &amp;amp;alpha;+n2+n2 cluster structure in the He8(02+) state. Finally, we discuss prospects for extending such investigations to heavier halo candidates and more complex multineutron systems, and outline the development of next-generation neutron detector arrays that will drive future progress in this field.</p>
	]]></content:encoded>

	<dc:title>Halos and Multineutron Correlations in Light Neutron-Rich Nuclei</dc:title>
			<dc:creator>Zheyang Lin</dc:creator>
			<dc:creator>Zaihong Yang</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010027</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-16</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-16</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>27</prism:startingPage>
		<prism:doi>10.3390/particles9010027</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/27</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/26">

	<title>Particles, Vol. 9, Pages 26: Measurement of Elastic Scattering Angular Distributions for Proton-Rich Nuclei 21,22Na on Double-Magic Nucleus 40Ca</title>
	<link>https://www.mdpi.com/2571-712X/9/1/26</link>
	<description>Present and future rare isotope accelerator facilities provide new opportunities to explore the structure of unstable nuclei. We report the measurements of the elastic scattering angular distributions of 21Na and 22Na on the doubly magic 40Ca above the Coulomb barrier energies, using high-purity post-accelerated ISOL beams from Beijing Radioactive Ion Beam Facility (BRIF). Angular distributions were measured with a silicon detector telescope array, and relative cross sections were determined with a CaF2 target on Au backing. The data were well reproduced by optical model calculations with Woods&amp;amp;ndash;Saxon and USNP potentials, the latter giving better agreement. These results confirm the stable operation and performance of the BRIF ISOL production and post-acceleration system, demonstrate its capability to provide radioactive beams of useful intensity and purity for future investigations of reaction dynamics and astrophysically relevant processes involving proton-rich nuclei, and simultaneously extend proton-rich elastic scattering studies to heavier systems.</description>
	<pubDate>2026-03-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 26: Measurement of Elastic Scattering Angular Distributions for Proton-Rich Nuclei 21,22Na on Double-Magic Nucleus 40Ca</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/26">doi: 10.3390/particles9010026</a></p>
	<p>Authors:
		Yuwen Chen
		Wei Nan
		Bing Guo
		Chengjian Lin
		Bing Tang
		Danyang Pang
		Lei Yang
		Dongxi Wang
		Guo Yang
		Yangping Shen
		Qiwen Fan
		Yiwen Bao
		Lei Cao
		Lihua Chen
		Baoqun Cui
		Yueming Hu
		Qinghua Huang
		Huiming Jia
		Chaoxin Kan
		Kangning Li
		Yaoqian Li
		Yunju Li
		Zhihong Li
		Gang Lian
		Junhui Liao
		Zhenwei Liu
		Tianpeng Luo
		Nanru Ma
		Ruigang Ma
		Xie Ma
		Yingjun Ma
		Guofang Song
		Lei Wang
		Xiaofei Wang
		Youbao Wang
		Yuheng Wang
		Peiwei Wen
		Shengquan Yan
		Feng Yang
		Sheng Zeng
		Yifan Zhang
		Tianjue Zhang
		Weiping Liu
		</p>
	<p>Present and future rare isotope accelerator facilities provide new opportunities to explore the structure of unstable nuclei. We report the measurements of the elastic scattering angular distributions of 21Na and 22Na on the doubly magic 40Ca above the Coulomb barrier energies, using high-purity post-accelerated ISOL beams from Beijing Radioactive Ion Beam Facility (BRIF). Angular distributions were measured with a silicon detector telescope array, and relative cross sections were determined with a CaF2 target on Au backing. The data were well reproduced by optical model calculations with Woods&amp;amp;ndash;Saxon and USNP potentials, the latter giving better agreement. These results confirm the stable operation and performance of the BRIF ISOL production and post-acceleration system, demonstrate its capability to provide radioactive beams of useful intensity and purity for future investigations of reaction dynamics and astrophysically relevant processes involving proton-rich nuclei, and simultaneously extend proton-rich elastic scattering studies to heavier systems.</p>
	]]></content:encoded>

	<dc:title>Measurement of Elastic Scattering Angular Distributions for Proton-Rich Nuclei 21,22Na on Double-Magic Nucleus 40Ca</dc:title>
			<dc:creator>Yuwen Chen</dc:creator>
			<dc:creator>Wei Nan</dc:creator>
			<dc:creator>Bing Guo</dc:creator>
			<dc:creator>Chengjian Lin</dc:creator>
			<dc:creator>Bing Tang</dc:creator>
			<dc:creator>Danyang Pang</dc:creator>
			<dc:creator>Lei Yang</dc:creator>
			<dc:creator>Dongxi Wang</dc:creator>
			<dc:creator>Guo Yang</dc:creator>
			<dc:creator>Yangping Shen</dc:creator>
			<dc:creator>Qiwen Fan</dc:creator>
			<dc:creator>Yiwen Bao</dc:creator>
			<dc:creator>Lei Cao</dc:creator>
			<dc:creator>Lihua Chen</dc:creator>
			<dc:creator>Baoqun Cui</dc:creator>
			<dc:creator>Yueming Hu</dc:creator>
			<dc:creator>Qinghua Huang</dc:creator>
			<dc:creator>Huiming Jia</dc:creator>
			<dc:creator>Chaoxin Kan</dc:creator>
			<dc:creator>Kangning Li</dc:creator>
			<dc:creator>Yaoqian Li</dc:creator>
			<dc:creator>Yunju Li</dc:creator>
			<dc:creator>Zhihong Li</dc:creator>
			<dc:creator>Gang Lian</dc:creator>
			<dc:creator>Junhui Liao</dc:creator>
			<dc:creator>Zhenwei Liu</dc:creator>
			<dc:creator>Tianpeng Luo</dc:creator>
			<dc:creator>Nanru Ma</dc:creator>
			<dc:creator>Ruigang Ma</dc:creator>
			<dc:creator>Xie Ma</dc:creator>
			<dc:creator>Yingjun Ma</dc:creator>
			<dc:creator>Guofang Song</dc:creator>
			<dc:creator>Lei Wang</dc:creator>
			<dc:creator>Xiaofei Wang</dc:creator>
			<dc:creator>Youbao Wang</dc:creator>
			<dc:creator>Yuheng Wang</dc:creator>
			<dc:creator>Peiwei Wen</dc:creator>
			<dc:creator>Shengquan Yan</dc:creator>
			<dc:creator>Feng Yang</dc:creator>
			<dc:creator>Sheng Zeng</dc:creator>
			<dc:creator>Yifan Zhang</dc:creator>
			<dc:creator>Tianjue Zhang</dc:creator>
			<dc:creator>Weiping Liu</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010026</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-13</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-13</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>26</prism:startingPage>
		<prism:doi>10.3390/particles9010026</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/26</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/25">

	<title>Particles, Vol. 9, Pages 25: Ab Initio Study on the Halo Structure in 11Be</title>
	<link>https://www.mdpi.com/2571-712X/9/1/25</link>
	<description>We present an ab initio study on the one-neutron halo nucleus 11Be using nuclear lattice effective field theory with high-fidelity chiral interactions at N3LO. By employing the wavefunction matching method to mitigate the sign problem and the pinhole algorithm to sample many-body correlations, we successfully reproduce the ground-state parity inversion and the extended matter radius characteristic of the halo structure. We analyze the intrinsic density distributions and geometric shapes of 11Be in comparison with the core nucleus 10Be. Our results reveal a prominent two-cluster structure in both nuclei and the occupation of the &amp;amp;sigma; molecular orbital by the valence neutron in 11Be. It enhances the prolate deformation as well as the diffuse neutron tail, distinct from the &amp;amp;pi;-orbital occupation observed in the 10Be ground state.</description>
	<pubDate>2026-03-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 25: Ab Initio Study on the Halo Structure in 11Be</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/25">doi: 10.3390/particles9010025</a></p>
	<p>Authors:
		Shihang Shen
		Serdar Elhatisari
		Dean Lee
		Ulf-G. Meißner
		Zhengxue Ren
		</p>
	<p>We present an ab initio study on the one-neutron halo nucleus 11Be using nuclear lattice effective field theory with high-fidelity chiral interactions at N3LO. By employing the wavefunction matching method to mitigate the sign problem and the pinhole algorithm to sample many-body correlations, we successfully reproduce the ground-state parity inversion and the extended matter radius characteristic of the halo structure. We analyze the intrinsic density distributions and geometric shapes of 11Be in comparison with the core nucleus 10Be. Our results reveal a prominent two-cluster structure in both nuclei and the occupation of the &amp;amp;sigma; molecular orbital by the valence neutron in 11Be. It enhances the prolate deformation as well as the diffuse neutron tail, distinct from the &amp;amp;pi;-orbital occupation observed in the 10Be ground state.</p>
	]]></content:encoded>

	<dc:title>Ab Initio Study on the Halo Structure in 11Be</dc:title>
			<dc:creator>Shihang Shen</dc:creator>
			<dc:creator>Serdar Elhatisari</dc:creator>
			<dc:creator>Dean Lee</dc:creator>
			<dc:creator>Ulf-G. Meißner</dc:creator>
			<dc:creator>Zhengxue Ren</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010025</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-10</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-10</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>25</prism:startingPage>
		<prism:doi>10.3390/particles9010025</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/25</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/24">

	<title>Particles, Vol. 9, Pages 24: Performance of the ATLAS Muon Spectrometer Detectors During Run 3 Data-Taking</title>
	<link>https://www.mdpi.com/2571-712X/9/1/24</link>
	<description>With the conclusion of proton&amp;amp;ndash;proton collision data-taking in 2025, the ATLAS experiment has now integrated a luminosity exceeding 300 fb&amp;amp;minus;1 during the Run 3 period, which began in July 2022 following Long Shutdown 2 (LS2). During LS2, a series of detector upgrades were implemented, including the installation of the New Small Wheel (NSW) in the innermost stations of the Muon Spectrometer end-caps. The ATLAS Muon Spectrometer, the largest muon system ever built at a collider, now comprises both established gaseous detectors&amp;amp;mdash;Monitored Drift Tubes, Thin Gap Chambers, and Resistive Plate Chambers&amp;amp;mdash;and newer detectors like Micromegas and small-strip TGCs in the NSW. These new systems are now in stable operation following an extensive phase of construction and commissioning, providing enhanced muon tracking and trigger capabilities. This presentation covers the performance of the muon system, focusing on the stability of the established detectors over time, their ability to handle increasing luminosity and associated irradiation levels, and studies on detector aging. Emphasis will be placed on the NSW upgrade, including the strategies adopted for alignment, track reconstruction, and trigger. The performance results presented in this contribution are based on Run 3 data collected up to 2024.</description>
	<pubDate>2026-03-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 24: Performance of the ATLAS Muon Spectrometer Detectors During Run 3 Data-Taking</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/24">doi: 10.3390/particles9010024</a></p>
	<p>Authors:
		Arisa Wada
		</p>
	<p>With the conclusion of proton&amp;amp;ndash;proton collision data-taking in 2025, the ATLAS experiment has now integrated a luminosity exceeding 300 fb&amp;amp;minus;1 during the Run 3 period, which began in July 2022 following Long Shutdown 2 (LS2). During LS2, a series of detector upgrades were implemented, including the installation of the New Small Wheel (NSW) in the innermost stations of the Muon Spectrometer end-caps. The ATLAS Muon Spectrometer, the largest muon system ever built at a collider, now comprises both established gaseous detectors&amp;amp;mdash;Monitored Drift Tubes, Thin Gap Chambers, and Resistive Plate Chambers&amp;amp;mdash;and newer detectors like Micromegas and small-strip TGCs in the NSW. These new systems are now in stable operation following an extensive phase of construction and commissioning, providing enhanced muon tracking and trigger capabilities. This presentation covers the performance of the muon system, focusing on the stability of the established detectors over time, their ability to handle increasing luminosity and associated irradiation levels, and studies on detector aging. Emphasis will be placed on the NSW upgrade, including the strategies adopted for alignment, track reconstruction, and trigger. The performance results presented in this contribution are based on Run 3 data collected up to 2024.</p>
	]]></content:encoded>

	<dc:title>Performance of the ATLAS Muon Spectrometer Detectors During Run 3 Data-Taking</dc:title>
			<dc:creator>Arisa Wada</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010024</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-10</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-10</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>24</prism:startingPage>
		<prism:doi>10.3390/particles9010024</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/24</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/23">

	<title>Particles, Vol. 9, Pages 23: Fully Heavy Pentaquarks with Jethad: A High-Energy Viewpoint</title>
	<link>https://www.mdpi.com/2571-712X/9/1/23</link>
	<description>We examine the leading-power fragmentation of fully heavy pentaquarks in high-energy hadronic collisions. To this end, we complete the release of the hadron structure-oriented PQ5Q1.0 fragmentation functions by discussing the P5c set and delivering the P5b one. These functions incorporate an improved computation of the initial-scale input for the constituent heavy-quark fragmentation channel, making them particularly suitable for describing both the direct formation of a compact multicharm state and the hadronization from a diquark&amp;amp;ndash;antiquark&amp;amp;ndash;diquark configuration. For phenomenological applications, we employ the data-validated (sym)Jethad framework to compute and analyze NLL/NLO+ semi-inclusive production rates of pentaquark-plus-jet systems at the upcoming HL-LHC and the future FCC. This study marks a further step toward connecting hadronic structure, precision QCD, and the emerging physics of exotic matter.</description>
	<pubDate>2026-03-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 23: Fully Heavy Pentaquarks with Jethad: A High-Energy Viewpoint</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/23">doi: 10.3390/particles9010023</a></p>
	<p>Authors:
		Francesco Giovanni Celiberto
		</p>
	<p>We examine the leading-power fragmentation of fully heavy pentaquarks in high-energy hadronic collisions. To this end, we complete the release of the hadron structure-oriented PQ5Q1.0 fragmentation functions by discussing the P5c set and delivering the P5b one. These functions incorporate an improved computation of the initial-scale input for the constituent heavy-quark fragmentation channel, making them particularly suitable for describing both the direct formation of a compact multicharm state and the hadronization from a diquark&amp;amp;ndash;antiquark&amp;amp;ndash;diquark configuration. For phenomenological applications, we employ the data-validated (sym)Jethad framework to compute and analyze NLL/NLO+ semi-inclusive production rates of pentaquark-plus-jet systems at the upcoming HL-LHC and the future FCC. This study marks a further step toward connecting hadronic structure, precision QCD, and the emerging physics of exotic matter.</p>
	]]></content:encoded>

	<dc:title>Fully Heavy Pentaquarks with Jethad: A High-Energy Viewpoint</dc:title>
			<dc:creator>Francesco Giovanni Celiberto</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010023</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-03</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-03</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>23</prism:startingPage>
		<prism:doi>10.3390/particles9010023</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/23</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/22">

	<title>Particles, Vol. 9, Pages 22: Emergence of the Geometric Contribution to the Superfluid Density in the Inner Crust of Neutron Stars</title>
	<link>https://www.mdpi.com/2571-712X/9/1/22</link>
	<description>The geometric contribution to superfluid density has been found to be of great importance in the inner crust of neutron stars. In this work we clarify how this contribution arises in the context of a band theory for neutrons. Specifically, we derive the dependence of the superfluid density on the magnitude of the pairing gap when the system has many bands cutting the Fermi energy, as is the case for neutrons in the inner crust. Also, in the perturbation theory framework, we find that it is essential to account for corrections to (Bogoliubov) quasi-particle states in order to obtain the geometric contribution. Accounting only for the corrections to (Hartree&amp;amp;ndash;Fock) single-particle states leads to the conventional contribution only.</description>
	<pubDate>2026-03-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 22: Emergence of the Geometric Contribution to the Superfluid Density in the Inner Crust of Neutron Stars</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/22">doi: 10.3390/particles9010022</a></p>
	<p>Authors:
		Giorgio Almirante
		</p>
	<p>The geometric contribution to superfluid density has been found to be of great importance in the inner crust of neutron stars. In this work we clarify how this contribution arises in the context of a band theory for neutrons. Specifically, we derive the dependence of the superfluid density on the magnitude of the pairing gap when the system has many bands cutting the Fermi energy, as is the case for neutrons in the inner crust. Also, in the perturbation theory framework, we find that it is essential to account for corrections to (Bogoliubov) quasi-particle states in order to obtain the geometric contribution. Accounting only for the corrections to (Hartree&amp;amp;ndash;Fock) single-particle states leads to the conventional contribution only.</p>
	]]></content:encoded>

	<dc:title>Emergence of the Geometric Contribution to the Superfluid Density in the Inner Crust of Neutron Stars</dc:title>
			<dc:creator>Giorgio Almirante</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010022</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>22</prism:startingPage>
		<prism:doi>10.3390/particles9010022</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/22</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/21">

	<title>Particles, Vol. 9, Pages 21: Halo Phenomena in Light- to Medium-Mass Nuclei with Three-Body Models</title>
	<link>https://www.mdpi.com/2571-712X/9/1/21</link>
	<description>Short-lived nuclear systems with light to medium masses are showing halo phenomena in regions of the nuclear chart that were still unexplored when halo nuclei were discovered 40 years ago. We study these exotic systems with three-body models, including nucleon&amp;amp;ndash;nucleon correlations, with the aim of reproducing measurable properties like radii and electromagnetic transition strengths. On the nucleon-rich side, drip-line fluorine isotopes are showing clear signs of a halo structure. Recently, we proposed that F29 is a moderate two-neutron halo nucleus with a large radius and a strong B(E1) response to the continuum. The three-body model places it at the borders of the island of inversion, which is corroborated by new data. According to our models, the next interesting isotope, F31, also has large spatial extension due to p-wave components and enhanced B(E1) response, pointing to a speculative halo structure. On the proton-rich side, we have studied the Sb102 system, composed of a Sn100 core plus a proton&amp;amp;ndash;neutron-correlated subsystem. We find that the weakening of the proton&amp;amp;ndash;neutron correlations with respect to the bare deuteron indicates that this is a one-proton emitter. We propose that the presence of a resonant state and its decay might provide a crucial benchmark for this system.</description>
	<pubDate>2026-03-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 21: Halo Phenomena in Light- to Medium-Mass Nuclei with Three-Body Models</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/21">doi: 10.3390/particles9010021</a></p>
	<p>Authors:
		Lorenzo Fortunato
		</p>
	<p>Short-lived nuclear systems with light to medium masses are showing halo phenomena in regions of the nuclear chart that were still unexplored when halo nuclei were discovered 40 years ago. We study these exotic systems with three-body models, including nucleon&amp;amp;ndash;nucleon correlations, with the aim of reproducing measurable properties like radii and electromagnetic transition strengths. On the nucleon-rich side, drip-line fluorine isotopes are showing clear signs of a halo structure. Recently, we proposed that F29 is a moderate two-neutron halo nucleus with a large radius and a strong B(E1) response to the continuum. The three-body model places it at the borders of the island of inversion, which is corroborated by new data. According to our models, the next interesting isotope, F31, also has large spatial extension due to p-wave components and enhanced B(E1) response, pointing to a speculative halo structure. On the proton-rich side, we have studied the Sb102 system, composed of a Sn100 core plus a proton&amp;amp;ndash;neutron-correlated subsystem. We find that the weakening of the proton&amp;amp;ndash;neutron correlations with respect to the bare deuteron indicates that this is a one-proton emitter. We propose that the presence of a resonant state and its decay might provide a crucial benchmark for this system.</p>
	]]></content:encoded>

	<dc:title>Halo Phenomena in Light- to Medium-Mass Nuclei with Three-Body Models</dc:title>
			<dc:creator>Lorenzo Fortunato</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010021</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-03-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-03-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Brief Report</prism:section>
	<prism:startingPage>21</prism:startingPage>
		<prism:doi>10.3390/particles9010021</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/21</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/20">

	<title>Particles, Vol. 9, Pages 20: Detection of Shielded Nuclear Materials Using Superheated Liquid Detectors</title>
	<link>https://www.mdpi.com/2571-712X/9/1/20</link>
	<description>Superheated liquid detectors (SLDs) exhibit strong sensitivity to fast neutrons and intrinsic insensitivity to gamma radiation, making them promising candidates for detecting shielded nuclear materials in security and non-proliferation applications. This work evaluates the feasibility of octafluoropropane-based superheated droplet detectors (SDDs) for identifying neutron-emitting materials concealed behind common attenuators. A combined acoustic and optical readout system was implemented, including a validated pulse-shape analysis method and a machine-learning-based bubble detection algorithm using YOLOv5. The optical system achieved a detection precision of approximately 80% within the defined region of interest. While the acoustic system remains the primary and more mature detection channel, the optical approach demonstrates feasibility but is not yet operationally ready for field deployment. Experiments with an AmBe neutron source and various shielding materials demonstrate that SDDs reliably detect fast neutrons under realistic inspection conditions while remaining insensitive to gamma radiation. These results support the feasibility of SLD-based systems as low-cost, passive tools for detecting shielded nuclear materials in field environments.</description>
	<pubDate>2026-02-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 20: Detection of Shielded Nuclear Materials Using Superheated Liquid Detectors</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/20">doi: 10.3390/particles9010020</a></p>
	<p>Authors:
		Leonardo Rodrigues
		Miguel Felizardo
		</p>
	<p>Superheated liquid detectors (SLDs) exhibit strong sensitivity to fast neutrons and intrinsic insensitivity to gamma radiation, making them promising candidates for detecting shielded nuclear materials in security and non-proliferation applications. This work evaluates the feasibility of octafluoropropane-based superheated droplet detectors (SDDs) for identifying neutron-emitting materials concealed behind common attenuators. A combined acoustic and optical readout system was implemented, including a validated pulse-shape analysis method and a machine-learning-based bubble detection algorithm using YOLOv5. The optical system achieved a detection precision of approximately 80% within the defined region of interest. While the acoustic system remains the primary and more mature detection channel, the optical approach demonstrates feasibility but is not yet operationally ready for field deployment. Experiments with an AmBe neutron source and various shielding materials demonstrate that SDDs reliably detect fast neutrons under realistic inspection conditions while remaining insensitive to gamma radiation. These results support the feasibility of SLD-based systems as low-cost, passive tools for detecting shielded nuclear materials in field environments.</p>
	]]></content:encoded>

	<dc:title>Detection of Shielded Nuclear Materials Using Superheated Liquid Detectors</dc:title>
			<dc:creator>Leonardo Rodrigues</dc:creator>
			<dc:creator>Miguel Felizardo</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010020</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-18</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-18</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>20</prism:startingPage>
		<prism:doi>10.3390/particles9010020</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/19">

	<title>Particles, Vol. 9, Pages 19: POEMMA&amp;ndash;Balloon with Radio: A Balloon-Borne Multi- Messenger Multi-Detector Observatory</title>
	<link>https://www.mdpi.com/2571-712X/9/1/19</link>
	<description>The Probe Of Extreme Multi-Messenger Astrophysics (POEMMA) is a proposed dual-satellite mission to observe Ultra-High-Energy Cosmic Rays (UHECRs), increase the statistics at the highest energies, and observe Very-High-Energy Neutrinos (VHENs) following multi-messenger alerts of astrophysical transient events, such as gamma-ray bursts and gravitational wave events, throughout the universe. POEMMA&amp;amp;ndash;Balloon with radio (PBR) is a small-scale version of the POEMMA design, adapted to be flown as a payload on one of NASA&amp;amp;rsquo;s suborbital Super Pressure Balloons (SPBs) circling over the Southern Ocean for more than 20 days after a launch from Wanaka, New Zealand. The main science objectives of PBR are: (1) to observe UHECRs via the fluorescence technique from suborbital space; (2) to observe horizontal high-altitude air showers (HAHAs) with energies above the cosmic ray knee (E &amp;amp;gt; 3PeV) using optical and radio detection for the first time; and (3) to follow astrophysical event alerts in the search of VHENs. The PBR instrument consists of a 1.1 m aperture Schmidt telescope similar to the POEMMA design, with two cameras on its focal surface: a Fluorescence Camera (FC) and a Cherenkov Camera (CC). In addition, PBR has a Radio Instrument (RI) optimized for detecting EASs (covering the 60&amp;amp;ndash;660 Mhz range). The FC observes UHECR-induced EASs in the ultraviolet (UV) spectrum using an array of 9216-pixel Multi-Anode Photo-Multiplier Tubes (MAPMTs) imaged every 1 &amp;amp;mu;s. The CC uses a 2048-pixel Silicon Photo-Multiplier (SiPM) imager to observe cosmic-ray-induced HAHAs and search for neutrino-induced upward-going EASs. The CC covers a spectral range of 320&amp;amp;ndash;900 nm, with an integration time of 10 ns. This contribution provides an overview of PBR instruments and their current status.</description>
	<pubDate>2026-02-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 19: POEMMA&amp;ndash;Balloon with Radio: A Balloon-Borne Multi- Messenger Multi-Detector Observatory</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/19">doi: 10.3390/particles9010019</a></p>
	<p>Authors:
		Giuseppe Osteria
		Johannes Eser
		Angela Olinto
		</p>
	<p>The Probe Of Extreme Multi-Messenger Astrophysics (POEMMA) is a proposed dual-satellite mission to observe Ultra-High-Energy Cosmic Rays (UHECRs), increase the statistics at the highest energies, and observe Very-High-Energy Neutrinos (VHENs) following multi-messenger alerts of astrophysical transient events, such as gamma-ray bursts and gravitational wave events, throughout the universe. POEMMA&amp;amp;ndash;Balloon with radio (PBR) is a small-scale version of the POEMMA design, adapted to be flown as a payload on one of NASA&amp;amp;rsquo;s suborbital Super Pressure Balloons (SPBs) circling over the Southern Ocean for more than 20 days after a launch from Wanaka, New Zealand. The main science objectives of PBR are: (1) to observe UHECRs via the fluorescence technique from suborbital space; (2) to observe horizontal high-altitude air showers (HAHAs) with energies above the cosmic ray knee (E &amp;amp;gt; 3PeV) using optical and radio detection for the first time; and (3) to follow astrophysical event alerts in the search of VHENs. The PBR instrument consists of a 1.1 m aperture Schmidt telescope similar to the POEMMA design, with two cameras on its focal surface: a Fluorescence Camera (FC) and a Cherenkov Camera (CC). In addition, PBR has a Radio Instrument (RI) optimized for detecting EASs (covering the 60&amp;amp;ndash;660 Mhz range). The FC observes UHECR-induced EASs in the ultraviolet (UV) spectrum using an array of 9216-pixel Multi-Anode Photo-Multiplier Tubes (MAPMTs) imaged every 1 &amp;amp;mu;s. The CC uses a 2048-pixel Silicon Photo-Multiplier (SiPM) imager to observe cosmic-ray-induced HAHAs and search for neutrino-induced upward-going EASs. The CC covers a spectral range of 320&amp;amp;ndash;900 nm, with an integration time of 10 ns. This contribution provides an overview of PBR instruments and their current status.</p>
	]]></content:encoded>

	<dc:title>POEMMA&amp;amp;ndash;Balloon with Radio: A Balloon-Borne Multi- Messenger Multi-Detector Observatory</dc:title>
			<dc:creator>Giuseppe Osteria</dc:creator>
			<dc:creator>Johannes Eser</dc:creator>
			<dc:creator>Angela Olinto</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010019</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-16</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-16</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>19</prism:startingPage>
		<prism:doi>10.3390/particles9010019</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/18">

	<title>Particles, Vol. 9, Pages 18: Massive Black Hole Formation in Proto-Stellar Clusters via Early Gas Accretion</title>
	<link>https://www.mdpi.com/2571-712X/9/1/18</link>
	<description>In this paper, we review our semi-analytic model of stellar black hole (BH) mass growth via gas accretion in gas-rich stellar clusters during their birthstage within the first &amp;amp;sim;10Myr after the first stellar formation event. Such proto-stellar clusters are massive and compact, with typical masses &amp;amp;sim;106M&amp;amp;#8857; and sizes &amp;amp;sim;1pc, as suggested by recent James Webb Space Telescope (JWST) observations. We find that by the end of the gas depletion process, BH masses are shifted to values within and above the BH mass gap, well within the range of components of the recent gravitational-wave (GW) signal GW231123, and up to masses &amp;amp;sim;103M&amp;amp;#8857;.</description>
	<pubDate>2026-02-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 18: Massive Black Hole Formation in Proto-Stellar Clusters via Early Gas Accretion</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/18">doi: 10.3390/particles9010018</a></p>
	<p>Authors:
		Zacharias Roupas
		</p>
	<p>In this paper, we review our semi-analytic model of stellar black hole (BH) mass growth via gas accretion in gas-rich stellar clusters during their birthstage within the first &amp;amp;sim;10Myr after the first stellar formation event. Such proto-stellar clusters are massive and compact, with typical masses &amp;amp;sim;106M&amp;amp;#8857; and sizes &amp;amp;sim;1pc, as suggested by recent James Webb Space Telescope (JWST) observations. We find that by the end of the gas depletion process, BH masses are shifted to values within and above the BH mass gap, well within the range of components of the recent gravitational-wave (GW) signal GW231123, and up to masses &amp;amp;sim;103M&amp;amp;#8857;.</p>
	]]></content:encoded>

	<dc:title>Massive Black Hole Formation in Proto-Stellar Clusters via Early Gas Accretion</dc:title>
			<dc:creator>Zacharias Roupas</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010018</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-15</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-15</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>18</prism:startingPage>
		<prism:doi>10.3390/particles9010018</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/17">

	<title>Particles, Vol. 9, Pages 17: Specular Reflectivity and Diffuse Scattering of Plasma Mirror as a Function of Laser Intensity in Polymer Target</title>
	<link>https://www.mdpi.com/2571-712X/9/1/17</link>
	<description>We present a systematic study on the optical response of plasma mirrors generated in polymer foils under ultrashort laser pulse irradiation within the non-relativistic intensity regime, reaching up to 2&amp;amp;times;1017 W/cm2. Using a Ti:sapphire system that delivers 50 fs pulses, we simultaneously measured reflection, transmission, and diffuse scattering with three energy meters for single-shot laser energies of 5, 10, 15, and 20 mJ as a function of the laser spot size on the target. The results reveal intensity-dependent variations in reflectivity, accompanied by simultaneous changes in transmission and scattering, allowing to estimate laser energy absorption by the polymer. Morphological analysis of the plasma surface suggests a significant role in modifying energy absorption, with implications for the efficiency of processes such as laser particle acceleration, nuclear fusion, and attosecond pulse generation. These findings provide critical insights into plasma mirror formation, absorption dynamics in polymers, and the potential of nanostructured polymer targets in high-intensity laser&amp;amp;ndash;matter interaction applications.</description>
	<pubDate>2026-02-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 17: Specular Reflectivity and Diffuse Scattering of Plasma Mirror as a Function of Laser Intensity in Polymer Target</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/17">doi: 10.3390/particles9010017</a></p>
	<p>Authors:
		Imene Benabdelghani
		Miklós Ákos Kedves
		Ádám Inger
		Márk Aladi
		</p>
	<p>We present a systematic study on the optical response of plasma mirrors generated in polymer foils under ultrashort laser pulse irradiation within the non-relativistic intensity regime, reaching up to 2&amp;amp;times;1017 W/cm2. Using a Ti:sapphire system that delivers 50 fs pulses, we simultaneously measured reflection, transmission, and diffuse scattering with three energy meters for single-shot laser energies of 5, 10, 15, and 20 mJ as a function of the laser spot size on the target. The results reveal intensity-dependent variations in reflectivity, accompanied by simultaneous changes in transmission and scattering, allowing to estimate laser energy absorption by the polymer. Morphological analysis of the plasma surface suggests a significant role in modifying energy absorption, with implications for the efficiency of processes such as laser particle acceleration, nuclear fusion, and attosecond pulse generation. These findings provide critical insights into plasma mirror formation, absorption dynamics in polymers, and the potential of nanostructured polymer targets in high-intensity laser&amp;amp;ndash;matter interaction applications.</p>
	]]></content:encoded>

	<dc:title>Specular Reflectivity and Diffuse Scattering of Plasma Mirror as a Function of Laser Intensity in Polymer Target</dc:title>
			<dc:creator>Imene Benabdelghani</dc:creator>
			<dc:creator>Miklós Ákos Kedves</dc:creator>
			<dc:creator>Ádám Inger</dc:creator>
			<dc:creator>Márk Aladi</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010017</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-14</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-14</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>17</prism:startingPage>
		<prism:doi>10.3390/particles9010017</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/16">

	<title>Particles, Vol. 9, Pages 16: Preliminary Results of the 64-Channel SiPM Readout MIZAR ASIC</title>
	<link>https://www.mdpi.com/2571-712X/9/1/16</link>
	<description>This work describes the development of the Multi-channel Integrated Zone-sampling Analogue-memory based Readout (MIZAR) ASIC. This 64-channel chip was designed as part of NASA&amp;amp;rsquo;s POEMMA Balloon with RADIO (PBR) mission, which aims to detect Ultra-High-Energy Cosmic Rays (UHECRs) and &amp;amp;tau; showers produced by the interaction of Cosmic Neutrinos (CNs) in the crust. The ASIC was implemented to read out a tile of 8 &amp;amp;times; 8 Silicon Photomultipliers (SiPMs) used to acquire the optical Cherenkov signals generated by Extensive Air Showers (EASs). A channel is partitioned into 256 cells where each one integrates an analogue memory, a Wilkinson Analog-to-Digital Converter (ADC) and a digital memory operating at the nominal sampling rate of 200 MS/s (with a 5 ns integration time). The signal is digitized on-chip, then the converted data is read out by an FPGA. The MIZAR also provides a 64-bit hitmap as a first-level trigger which can be elaborated by an external firmware. This ASIC can also be configured to further segment the channels into units of 32 or 64 cells each and the ADC resolution can be set to a range between 8 and 12 bits. The chip was designed in a commercial 65 nm CMOS technology node and it was submitted for production in December 2024. The ASICs were delivered in March 2025.</description>
	<pubDate>2026-02-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 16: Preliminary Results of the 64-Channel SiPM Readout MIZAR ASIC</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/16">doi: 10.3390/particles9010016</a></p>
	<p>Authors:
		Andrea Di Salvo
		Emanuele Trossarello
		Micol Maria Bargelli
		Federico Reynaud
		Matteo Abrate
		Richard Wheadon
		Marco Mignone
		Angelo Rivetti
		Sara Garbolino
		Mario Edoardo Bertaina
		</p>
	<p>This work describes the development of the Multi-channel Integrated Zone-sampling Analogue-memory based Readout (MIZAR) ASIC. This 64-channel chip was designed as part of NASA&amp;amp;rsquo;s POEMMA Balloon with RADIO (PBR) mission, which aims to detect Ultra-High-Energy Cosmic Rays (UHECRs) and &amp;amp;tau; showers produced by the interaction of Cosmic Neutrinos (CNs) in the crust. The ASIC was implemented to read out a tile of 8 &amp;amp;times; 8 Silicon Photomultipliers (SiPMs) used to acquire the optical Cherenkov signals generated by Extensive Air Showers (EASs). A channel is partitioned into 256 cells where each one integrates an analogue memory, a Wilkinson Analog-to-Digital Converter (ADC) and a digital memory operating at the nominal sampling rate of 200 MS/s (with a 5 ns integration time). The signal is digitized on-chip, then the converted data is read out by an FPGA. The MIZAR also provides a 64-bit hitmap as a first-level trigger which can be elaborated by an external firmware. This ASIC can also be configured to further segment the channels into units of 32 or 64 cells each and the ADC resolution can be set to a range between 8 and 12 bits. The chip was designed in a commercial 65 nm CMOS technology node and it was submitted for production in December 2024. The ASICs were delivered in March 2025.</p>
	]]></content:encoded>

	<dc:title>Preliminary Results of the 64-Channel SiPM Readout MIZAR ASIC</dc:title>
			<dc:creator>Andrea Di Salvo</dc:creator>
			<dc:creator>Emanuele Trossarello</dc:creator>
			<dc:creator>Micol Maria Bargelli</dc:creator>
			<dc:creator>Federico Reynaud</dc:creator>
			<dc:creator>Matteo Abrate</dc:creator>
			<dc:creator>Richard Wheadon</dc:creator>
			<dc:creator>Marco Mignone</dc:creator>
			<dc:creator>Angelo Rivetti</dc:creator>
			<dc:creator>Sara Garbolino</dc:creator>
			<dc:creator>Mario Edoardo Bertaina</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010016</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-13</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-13</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>16</prism:startingPage>
		<prism:doi>10.3390/particles9010016</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/15">

	<title>Particles, Vol. 9, Pages 15: Baryon-like Space Distribution of Dark Matter from Point of View of Explanation of Positron Anomaly</title>
	<link>https://www.mdpi.com/2571-712X/9/1/15</link>
	<description>In this work we test the possibility of accounting for the positron anomaly with annihilating dark matter particles without contradicting the gamma-ray constraints due to their unconventional space distribution. To achieve that, we consider two-component dark matter, whose major constituent is inert and forms the halo of the Galaxy, while the second, minor, component consists of annihilating particles that could form some different structure. This work is the next logical step after our previous &amp;amp;ldquo;dark disk model&amp;amp;rdquo; where an active DM component was considered to form a disk, allowing good suppression of accompanying gamma-radiation. Nowadays that model is not enough to avoid the contradiction, so we are testing a new, more complex one with a spiral spatial distribution like the one of baryons. We have previously tested two simplified toy models of ring-like density profiles and one simple spiral density profile that have shown good improvement compared to the disk case. In this work, we take things further and consider a more physically grounded density profile constructed on the base of a modern model of the baryon density of our Galaxy. Contrary to our expectations, this advanced model shows much worse agreement with the data than previous toy models.</description>
	<pubDate>2026-02-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 15: Baryon-like Space Distribution of Dark Matter from Point of View of Explanation of Positron Anomaly</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/15">doi: 10.3390/particles9010015</a></p>
	<p>Authors:
		Konstantin M. Belotsky
		Maksim L. Solovev
		</p>
	<p>In this work we test the possibility of accounting for the positron anomaly with annihilating dark matter particles without contradicting the gamma-ray constraints due to their unconventional space distribution. To achieve that, we consider two-component dark matter, whose major constituent is inert and forms the halo of the Galaxy, while the second, minor, component consists of annihilating particles that could form some different structure. This work is the next logical step after our previous &amp;amp;ldquo;dark disk model&amp;amp;rdquo; where an active DM component was considered to form a disk, allowing good suppression of accompanying gamma-radiation. Nowadays that model is not enough to avoid the contradiction, so we are testing a new, more complex one with a spiral spatial distribution like the one of baryons. We have previously tested two simplified toy models of ring-like density profiles and one simple spiral density profile that have shown good improvement compared to the disk case. In this work, we take things further and consider a more physically grounded density profile constructed on the base of a modern model of the baryon density of our Galaxy. Contrary to our expectations, this advanced model shows much worse agreement with the data than previous toy models.</p>
	]]></content:encoded>

	<dc:title>Baryon-like Space Distribution of Dark Matter from Point of View of Explanation of Positron Anomaly</dc:title>
			<dc:creator>Konstantin M. Belotsky</dc:creator>
			<dc:creator>Maksim L. Solovev</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010015</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-13</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-13</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/particles9010015</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/14">

	<title>Particles, Vol. 9, Pages 14: Performance Evaluation of the Readout Electronics Board Based on the Smart Asic for the Adapt Instrument</title>
	<link>https://www.mdpi.com/2571-712X/9/1/14</link>
	<description>The Advanced Particle&amp;amp;ndash;astrophysics Telescope (APT) is a mission concept for a future space-based MeV-TeV observatory, designed to combine a Compton and e+e&amp;amp;minus; pair telescope, aiming to improve the sensitivity of the instruments to &amp;amp;gamma; rays in the MeV-GeV range by at least one order of magnitude. To validate and study the technologies that will be employed on the observatory, a small-scale prototype, the Antarctic Demonstrator for APT (ADAPT), is currently being developed to fly on a balloon in Antarctica during the local 2026&amp;amp;ndash;2027 flight season. Among its subdetectors there is an Imaging CsI calorimeter (ICC), consisting of 4 layers of CsI(Na) crystals with crossed WLS fibers, coupled to Silicon Photomultipliers (SiPMs). A key element of the design is the multichannel front-end electronics, based on the SMART (SiPM Multichannel ASIC for high-Resolution Cherenkov Telescopes) ASIC, which combines compactness, cost-effectiveness, and a high level of integration. This work reports the results of quality-control tests performed on the custom readout boards for the ICC, and provides an overview of the present status of the mission.</description>
	<pubDate>2026-02-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 14: Performance Evaluation of the Readout Electronics Board Based on the Smart Asic for the Adapt Instrument</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/14">doi: 10.3390/particles9010014</a></p>
	<p>Authors:
		Gaia De Palma
		Marco Cecca
		Leonardo Di Venere
		Francesco Licciulli
		Mario Nicola Mazziotta
		Elisabetta Bissaldi
		James Buckley
		Blake Bal
		Richard Bose
		Adrian Zink
		</p>
	<p>The Advanced Particle&amp;amp;ndash;astrophysics Telescope (APT) is a mission concept for a future space-based MeV-TeV observatory, designed to combine a Compton and e+e&amp;amp;minus; pair telescope, aiming to improve the sensitivity of the instruments to &amp;amp;gamma; rays in the MeV-GeV range by at least one order of magnitude. To validate and study the technologies that will be employed on the observatory, a small-scale prototype, the Antarctic Demonstrator for APT (ADAPT), is currently being developed to fly on a balloon in Antarctica during the local 2026&amp;amp;ndash;2027 flight season. Among its subdetectors there is an Imaging CsI calorimeter (ICC), consisting of 4 layers of CsI(Na) crystals with crossed WLS fibers, coupled to Silicon Photomultipliers (SiPMs). A key element of the design is the multichannel front-end electronics, based on the SMART (SiPM Multichannel ASIC for high-Resolution Cherenkov Telescopes) ASIC, which combines compactness, cost-effectiveness, and a high level of integration. This work reports the results of quality-control tests performed on the custom readout boards for the ICC, and provides an overview of the present status of the mission.</p>
	]]></content:encoded>

	<dc:title>Performance Evaluation of the Readout Electronics Board Based on the Smart Asic for the Adapt Instrument</dc:title>
			<dc:creator>Gaia De Palma</dc:creator>
			<dc:creator>Marco Cecca</dc:creator>
			<dc:creator>Leonardo Di Venere</dc:creator>
			<dc:creator>Francesco Licciulli</dc:creator>
			<dc:creator>Mario Nicola Mazziotta</dc:creator>
			<dc:creator>Elisabetta Bissaldi</dc:creator>
			<dc:creator>James Buckley</dc:creator>
			<dc:creator>Blake Bal</dc:creator>
			<dc:creator>Richard Bose</dc:creator>
			<dc:creator>Adrian Zink</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010014</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-10</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-10</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/particles9010014</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/13">

	<title>Particles, Vol. 9, Pages 13: Gamma-RayBurst Polarimetry with the COMCUBE-S CubeSat Swarm&amp;mdash;Design and Performance Simulations</title>
	<link>https://www.mdpi.com/2571-712X/9/1/13</link>
	<description>COMCUBE-S (Compton Telescope CubeSat Swarm) is a proposed mission aimed at understanding the radiation mechanisms of ultra-relativistic jets from Gamma-Ray Bursts (GRBs). It consists of a swarm of 16U CubeSats carrying a state-of-the-art Compton polarimeter and a bismuth germanium oxide (BGO) spectrometer to perform timing, spectroscopic and polarimetric measurements of the prompt emission from GRBs. The mission is currently in a feasibility study phase (Phase A) with the European Space Agency to prepare an in-orbit demonstration. Here, we present the simulation work used to optimise the design and operational concept of the microsatellite constellation, as well as estimate the mission performance in terms of GRB detection rate and polarimetry. We used the MEGAlib software to simulate the response function of the gamma-ray instruments, together with a detailed model for the background particle and radiation fluxes in low-Earth orbit. We also developed a synthetic GRB population model to best estimate the detection rate. These simulations show that COMCUBE-S will detect about 2 GRBs per day, which is significantly higher than that of all past and current GRB missions. Furthermore, simulated performance for linear polarisation measurements shows that COMCUBE-S will be able to uniquely distinguish between competing models of the GRB prompt emission, thereby shedding new light on some of the most fundamental aspects of GRB physics.</description>
	<pubDate>2026-02-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 13: Gamma-RayBurst Polarimetry with the COMCUBE-S CubeSat Swarm&amp;mdash;Design and Performance Simulations</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/13">doi: 10.3390/particles9010013</a></p>
	<p>Authors:
		Nathan Franel
		Vincent Tatischeff
		David Murphy
		Alexey Ulyanov
		Caimin McKenna
		Lorraine Hanlon
		Prerna Baranwal
		Christophe Beigbeder
		Arnaud Claret
		Ion Cojocari
		Nicolas de Séréville
		Nicolas Dosme
		Eric Doumayrou
		Mariya Georgieva
		Clarisse Hamadache
		Sally Hankache
		Jimmy Jeglot
		Mózsi Kiss
		Beng-Yun Ky
		Vincent Lafage
		Philippe Laurent
		Christine Le Galliard
		Joseph Mangan
		Aline Meuris
		Mark Pearce
		Jean Peyré
		Arjun Poitaya
		Diana Renaud
		Arnaud Saussac
		Varun Varun
		Matias Vecchio
		Colin Wade
		</p>
	<p>COMCUBE-S (Compton Telescope CubeSat Swarm) is a proposed mission aimed at understanding the radiation mechanisms of ultra-relativistic jets from Gamma-Ray Bursts (GRBs). It consists of a swarm of 16U CubeSats carrying a state-of-the-art Compton polarimeter and a bismuth germanium oxide (BGO) spectrometer to perform timing, spectroscopic and polarimetric measurements of the prompt emission from GRBs. The mission is currently in a feasibility study phase (Phase A) with the European Space Agency to prepare an in-orbit demonstration. Here, we present the simulation work used to optimise the design and operational concept of the microsatellite constellation, as well as estimate the mission performance in terms of GRB detection rate and polarimetry. We used the MEGAlib software to simulate the response function of the gamma-ray instruments, together with a detailed model for the background particle and radiation fluxes in low-Earth orbit. We also developed a synthetic GRB population model to best estimate the detection rate. These simulations show that COMCUBE-S will detect about 2 GRBs per day, which is significantly higher than that of all past and current GRB missions. Furthermore, simulated performance for linear polarisation measurements shows that COMCUBE-S will be able to uniquely distinguish between competing models of the GRB prompt emission, thereby shedding new light on some of the most fundamental aspects of GRB physics.</p>
	]]></content:encoded>

	<dc:title>Gamma-RayBurst Polarimetry with the COMCUBE-S CubeSat Swarm&amp;amp;mdash;Design and Performance Simulations</dc:title>
			<dc:creator>Nathan Franel</dc:creator>
			<dc:creator>Vincent Tatischeff</dc:creator>
			<dc:creator>David Murphy</dc:creator>
			<dc:creator>Alexey Ulyanov</dc:creator>
			<dc:creator>Caimin McKenna</dc:creator>
			<dc:creator>Lorraine Hanlon</dc:creator>
			<dc:creator>Prerna Baranwal</dc:creator>
			<dc:creator>Christophe Beigbeder</dc:creator>
			<dc:creator>Arnaud Claret</dc:creator>
			<dc:creator>Ion Cojocari</dc:creator>
			<dc:creator>Nicolas de Séréville</dc:creator>
			<dc:creator>Nicolas Dosme</dc:creator>
			<dc:creator>Eric Doumayrou</dc:creator>
			<dc:creator>Mariya Georgieva</dc:creator>
			<dc:creator>Clarisse Hamadache</dc:creator>
			<dc:creator>Sally Hankache</dc:creator>
			<dc:creator>Jimmy Jeglot</dc:creator>
			<dc:creator>Mózsi Kiss</dc:creator>
			<dc:creator>Beng-Yun Ky</dc:creator>
			<dc:creator>Vincent Lafage</dc:creator>
			<dc:creator>Philippe Laurent</dc:creator>
			<dc:creator>Christine Le Galliard</dc:creator>
			<dc:creator>Joseph Mangan</dc:creator>
			<dc:creator>Aline Meuris</dc:creator>
			<dc:creator>Mark Pearce</dc:creator>
			<dc:creator>Jean Peyré</dc:creator>
			<dc:creator>Arjun Poitaya</dc:creator>
			<dc:creator>Diana Renaud</dc:creator>
			<dc:creator>Arnaud Saussac</dc:creator>
			<dc:creator>Varun Varun</dc:creator>
			<dc:creator>Matias Vecchio</dc:creator>
			<dc:creator>Colin Wade</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010013</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-06</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-06</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>13</prism:startingPage>
		<prism:doi>10.3390/particles9010013</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/12">

	<title>Particles, Vol. 9, Pages 12: Clusters of PBHs in a Framework of Multidimensional f(R)-Gravity</title>
	<link>https://www.mdpi.com/2571-712X/9/1/12</link>
	<description>We investigate primordial black hole (PBH) production via the collapse of supercritical domain walls in a quadratic f(R)-gravity model with tensor extensions. The effective field theory for an extra space&amp;amp;rsquo;s scalar curvature provides a foundation for the formation of these dense walls. In our work, domain walls are found to be supercritical. Their properties were extensively studied in the literature, where it was demonstrated that they create wormholes and escape into baby universes through them. Closure of the wormhole leads to black hole creation, providing a mechanism for the production of primordial black holes in our model. We calculate the mass spectrum of such black holes and mass distribution within clusters of them. When accretion is accounted for, the black holes produced under this mechanism present viable dark matter candidates.</description>
	<pubDate>2026-02-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 12: Clusters of PBHs in a Framework of Multidimensional f(R)-Gravity</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/12">doi: 10.3390/particles9010012</a></p>
	<p>Authors:
		Maxim Krasnov
		Valery Nikulin
		</p>
	<p>We investigate primordial black hole (PBH) production via the collapse of supercritical domain walls in a quadratic f(R)-gravity model with tensor extensions. The effective field theory for an extra space&amp;amp;rsquo;s scalar curvature provides a foundation for the formation of these dense walls. In our work, domain walls are found to be supercritical. Their properties were extensively studied in the literature, where it was demonstrated that they create wormholes and escape into baby universes through them. Closure of the wormhole leads to black hole creation, providing a mechanism for the production of primordial black holes in our model. We calculate the mass spectrum of such black holes and mass distribution within clusters of them. When accretion is accounted for, the black holes produced under this mechanism present viable dark matter candidates.</p>
	]]></content:encoded>

	<dc:title>Clusters of PBHs in a Framework of Multidimensional f(R)-Gravity</dc:title>
			<dc:creator>Maxim Krasnov</dc:creator>
			<dc:creator>Valery Nikulin</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010012</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-03</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-03</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>12</prism:startingPage>
		<prism:doi>10.3390/particles9010012</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/11">

	<title>Particles, Vol. 9, Pages 11: Holographic Naturalness and Information See-Saw Mechanism for Neutrinos</title>
	<link>https://www.mdpi.com/2571-712X/9/1/11</link>
	<description>The microscopic origin of the de Sitter entropy remains a central puzzle in quantum gravity that is related to the cosmological constant problem. Within the paradigm of Holographic Naturalness, we propose that this entropy is carried by a vast number of light, coherent degrees of freedom&amp;amp;mdash;called &amp;amp;ldquo;hairons&amp;amp;rdquo;&amp;amp;mdash;which emerge as the moduli of gravitational instantons on orbifolds. Starting from the Euclidean de Sitter instanton (S4), we construct a new class of orbifold gravitational instantons, S4/ZN, where N corresponds to the de Sitter entropy. We demonstrate that the dimension of the moduli space of these instantons scales linearly with N, and we identify these moduli with the hairon fields. A ZN symmetry, derived from Wilson loops in the instanton background, ensures the distinguishability of these modes, leading to the correct entropy count. The hairons acquire a mass of the order of the Hubble scale and exhibit negligible mutual interactions, suggesting that the de Sitter vacuum is a coherent state, or Bose&amp;amp;ndash;Einstein condensate, of these fundamental excitations. Then, we present a novel framework which unifies neutrino mass generation with the cosmological constant through gravitational topology and holography. The small neutrino mass scale emerges naturally from first principles, without requiring new physics beyond the Standard Model and Gravity. The gravitational Chern&amp;amp;ndash;Simons structure and its anomaly with neutrinos force a topological Higgs mechanism, leading to neutrino condensation via S4/ZN gravitational instantons. The number of topological degrees of freedom N&amp;amp;sim;MP2/&amp;amp;Lambda;&amp;amp;sim;10120 provides both the holographic counting of the de Sitter entropy and a 1/Ninformation see-saw mechanism for neutrino masses. Our framework makes the following predictions: (i) a neutrino superfluid condensation forming Cooper pairs below meV energies, as a viable candidate for cold dark matter; (ii) a possible resolution of the strong CP problem through a QCD composite axion state; (iii) time-varying neutrino masses which track the evolution of dark energy; and (iv) several distinctive signatures in astroparticle physics, ultra-high-energy cosmic rays and high magnetic field experiments.</description>
	<pubDate>2026-02-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 11: Holographic Naturalness and Information See-Saw Mechanism for Neutrinos</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/11">doi: 10.3390/particles9010011</a></p>
	<p>Authors:
		Andrea Addazi
		Giuseppe Meluccio
		</p>
	<p>The microscopic origin of the de Sitter entropy remains a central puzzle in quantum gravity that is related to the cosmological constant problem. Within the paradigm of Holographic Naturalness, we propose that this entropy is carried by a vast number of light, coherent degrees of freedom&amp;amp;mdash;called &amp;amp;ldquo;hairons&amp;amp;rdquo;&amp;amp;mdash;which emerge as the moduli of gravitational instantons on orbifolds. Starting from the Euclidean de Sitter instanton (S4), we construct a new class of orbifold gravitational instantons, S4/ZN, where N corresponds to the de Sitter entropy. We demonstrate that the dimension of the moduli space of these instantons scales linearly with N, and we identify these moduli with the hairon fields. A ZN symmetry, derived from Wilson loops in the instanton background, ensures the distinguishability of these modes, leading to the correct entropy count. The hairons acquire a mass of the order of the Hubble scale and exhibit negligible mutual interactions, suggesting that the de Sitter vacuum is a coherent state, or Bose&amp;amp;ndash;Einstein condensate, of these fundamental excitations. Then, we present a novel framework which unifies neutrino mass generation with the cosmological constant through gravitational topology and holography. The small neutrino mass scale emerges naturally from first principles, without requiring new physics beyond the Standard Model and Gravity. The gravitational Chern&amp;amp;ndash;Simons structure and its anomaly with neutrinos force a topological Higgs mechanism, leading to neutrino condensation via S4/ZN gravitational instantons. The number of topological degrees of freedom N&amp;amp;sim;MP2/&amp;amp;Lambda;&amp;amp;sim;10120 provides both the holographic counting of the de Sitter entropy and a 1/Ninformation see-saw mechanism for neutrino masses. Our framework makes the following predictions: (i) a neutrino superfluid condensation forming Cooper pairs below meV energies, as a viable candidate for cold dark matter; (ii) a possible resolution of the strong CP problem through a QCD composite axion state; (iii) time-varying neutrino masses which track the evolution of dark energy; and (iv) several distinctive signatures in astroparticle physics, ultra-high-energy cosmic rays and high magnetic field experiments.</p>
	]]></content:encoded>

	<dc:title>Holographic Naturalness and Information See-Saw Mechanism for Neutrinos</dc:title>
			<dc:creator>Andrea Addazi</dc:creator>
			<dc:creator>Giuseppe Meluccio</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010011</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>11</prism:startingPage>
		<prism:doi>10.3390/particles9010011</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/10">

	<title>Particles, Vol. 9, Pages 10: Evaluation of a Timepix3 Telescope for Applications as a Compton Scatter Polarimeter for Hard X- and Soft &amp;gamma;-Rays</title>
	<link>https://www.mdpi.com/2571-712X/9/1/10</link>
	<description>This work presents a simulation study of a Timepix3 telescope composed of nine detectors for use as a Compton scatter polarimeter in the energy range of 35&amp;amp;ndash;100 keV. Four detectors carry 1 mm thick silicon (Si) sensors and five detectors carry 1 mm thick cadmium telluride (CdTe) sensors. The modulation factor for 100% linearly polarized X-ray beams was found to be &amp;amp;mu;100&amp;amp;gt;70% in the energy range of 55&amp;amp;ndash;80 keV. The quality factor of the polarimeter has its maximum 12.8% at the energy 75 keV. The comparison of quality factors and the calculations of a hypothetical observation of the Crab nebula show that this multilayer Timepix3 approach is competitive with contemporary X-ray polarimeters.</description>
	<pubDate>2026-02-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 10: Evaluation of a Timepix3 Telescope for Applications as a Compton Scatter Polarimeter for Hard X- and Soft &amp;gamma;-Rays</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/10">doi: 10.3390/particles9010010</a></p>
	<p>Authors:
		Jindrich Jelinek
		Benedikt Bergmann
		Petr Smolyanskiy
		</p>
	<p>This work presents a simulation study of a Timepix3 telescope composed of nine detectors for use as a Compton scatter polarimeter in the energy range of 35&amp;amp;ndash;100 keV. Four detectors carry 1 mm thick silicon (Si) sensors and five detectors carry 1 mm thick cadmium telluride (CdTe) sensors. The modulation factor for 100% linearly polarized X-ray beams was found to be &amp;amp;mu;100&amp;amp;gt;70% in the energy range of 55&amp;amp;ndash;80 keV. The quality factor of the polarimeter has its maximum 12.8% at the energy 75 keV. The comparison of quality factors and the calculations of a hypothetical observation of the Crab nebula show that this multilayer Timepix3 approach is competitive with contemporary X-ray polarimeters.</p>
	]]></content:encoded>

	<dc:title>Evaluation of a Timepix3 Telescope for Applications as a Compton Scatter Polarimeter for Hard X- and Soft &amp;amp;gamma;-Rays</dc:title>
			<dc:creator>Jindrich Jelinek</dc:creator>
			<dc:creator>Benedikt Bergmann</dc:creator>
			<dc:creator>Petr Smolyanskiy</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010010</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-02-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-02-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>10</prism:startingPage>
		<prism:doi>10.3390/particles9010010</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/9">

	<title>Particles, Vol. 9, Pages 9: High-Precision Cross-Sections for Galactic Cosmic Rays: Highlights from XSCRC2024 and Follow-Up Actions</title>
	<link>https://www.mdpi.com/2571-712X/9/1/9</link>
	<description>The interpretation of high-precision Galactic cosmic-ray data from AMS-02, CALET, DAMPE, etc., is fundamentally limited by nuclear cross-sections uncertainties. This proceeding highlights the results presented at the XSCRC2024 workshop, which aims at bringing together the cosmic-ray, nuclear, and particle physics communities, with the goal of improving cross-section measurements across various domains, from nuclei production for constraining cosmic-ray transport parameters, to antiproton and anti-deuteron production for dark matter searches. This workshop lead to a comprehensive roadmap for new cross-section measurements in the next decade, as well as other outcomes.</description>
	<pubDate>2026-01-26</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 9: High-Precision Cross-Sections for Galactic Cosmic Rays: Highlights from XSCRC2024 and Follow-Up Actions</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/9">doi: 10.3390/particles9010009</a></p>
	<p>Authors:
		David Maurin
		Fiorenza Donato
		Saverio Mariani
		</p>
	<p>The interpretation of high-precision Galactic cosmic-ray data from AMS-02, CALET, DAMPE, etc., is fundamentally limited by nuclear cross-sections uncertainties. This proceeding highlights the results presented at the XSCRC2024 workshop, which aims at bringing together the cosmic-ray, nuclear, and particle physics communities, with the goal of improving cross-section measurements across various domains, from nuclei production for constraining cosmic-ray transport parameters, to antiproton and anti-deuteron production for dark matter searches. This workshop lead to a comprehensive roadmap for new cross-section measurements in the next decade, as well as other outcomes.</p>
	]]></content:encoded>

	<dc:title>High-Precision Cross-Sections for Galactic Cosmic Rays: Highlights from XSCRC2024 and Follow-Up Actions</dc:title>
			<dc:creator>David Maurin</dc:creator>
			<dc:creator>Fiorenza Donato</dc:creator>
			<dc:creator>Saverio Mariani</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010009</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-26</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-26</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Conference Report</prism:section>
	<prism:startingPage>9</prism:startingPage>
		<prism:doi>10.3390/particles9010009</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/8">

	<title>Particles, Vol. 9, Pages 8: Identified-Hadron Spectra in &amp;pi;+ + Be at 60 GeV/c with Channel-Wise Subcollision Acceptance in PYTHIA 8 Angantyr</title>
	<link>https://www.mdpi.com/2571-712X/9/1/8</link>
	<description>Identified-hadron production (p, &amp;amp;pi;&amp;amp;plusmn;, K&amp;amp;plusmn;) in &amp;amp;pi;++Be at plab=60GeV/c (s&amp;amp;#8771;10.6GeV) is investigated using Pythia 8.315 (Monash tune) with the Angantyr extension. Differential multiplicities d2n/(dpd&amp;amp;theta;) are confronted with NA61/SHINE measurements across standard &amp;amp;theta; bins. Within the fluctuating-radii Double-Strikman (DS) scheme, two unsuppressed opacity mappings are compared to quantify systematics. In addition, a minimal extension is introduced: a flat, post-classification, channel-wise acceptance applied after ND/SD/DD/EL tagging. It acts on primary and secondary &amp;amp;pi;N pairs, keeps hadronization fixed (Lund string), and leaves the internal event generation of each admitted subcollision unchanged. Opacity-mapping variations alone induce only percent-level differences and do not resolve the soft/forward tensions. By contrast, the flat acceptance&amp;amp;mdash;interpretable as a reduced effective ND weight&amp;amp;mdash;improves agreement across species and angles. It hardens the forward &amp;amp;pi;+ spectra and lowers large-&amp;amp;theta; yields, produces milder charge-asymmetric changes for &amp;amp;pi;&amp;amp;minus; consistent with the weaker leading feed, suppresses proton yields at all angles (with a residual &amp;amp;sim;30% forward high-p deficit), and improves K&amp;amp;plusmn;, with a stronger effect for K+ than K&amp;amp;minus;. These results show that a geometry-blind reweighting of the subcollision mixture suffices to capture the main NA61/SHINE trends for &amp;amp;pi;++Be at SPS energies without modifying hadronization. The approach provides a controlled baseline for subsequent, channel-balanced refinements and broader &amp;amp;pi;+A tuning.</description>
	<pubDate>2026-01-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 8: Identified-Hadron Spectra in &amp;pi;+ + Be at 60 GeV/c with Channel-Wise Subcollision Acceptance in PYTHIA 8 Angantyr</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/8">doi: 10.3390/particles9010008</a></p>
	<p>Authors:
		Nuha Felemban
		</p>
	<p>Identified-hadron production (p, &amp;amp;pi;&amp;amp;plusmn;, K&amp;amp;plusmn;) in &amp;amp;pi;++Be at plab=60GeV/c (s&amp;amp;#8771;10.6GeV) is investigated using Pythia 8.315 (Monash tune) with the Angantyr extension. Differential multiplicities d2n/(dpd&amp;amp;theta;) are confronted with NA61/SHINE measurements across standard &amp;amp;theta; bins. Within the fluctuating-radii Double-Strikman (DS) scheme, two unsuppressed opacity mappings are compared to quantify systematics. In addition, a minimal extension is introduced: a flat, post-classification, channel-wise acceptance applied after ND/SD/DD/EL tagging. It acts on primary and secondary &amp;amp;pi;N pairs, keeps hadronization fixed (Lund string), and leaves the internal event generation of each admitted subcollision unchanged. Opacity-mapping variations alone induce only percent-level differences and do not resolve the soft/forward tensions. By contrast, the flat acceptance&amp;amp;mdash;interpretable as a reduced effective ND weight&amp;amp;mdash;improves agreement across species and angles. It hardens the forward &amp;amp;pi;+ spectra and lowers large-&amp;amp;theta; yields, produces milder charge-asymmetric changes for &amp;amp;pi;&amp;amp;minus; consistent with the weaker leading feed, suppresses proton yields at all angles (with a residual &amp;amp;sim;30% forward high-p deficit), and improves K&amp;amp;plusmn;, with a stronger effect for K+ than K&amp;amp;minus;. These results show that a geometry-blind reweighting of the subcollision mixture suffices to capture the main NA61/SHINE trends for &amp;amp;pi;++Be at SPS energies without modifying hadronization. The approach provides a controlled baseline for subsequent, channel-balanced refinements and broader &amp;amp;pi;+A tuning.</p>
	]]></content:encoded>

	<dc:title>Identified-Hadron Spectra in &amp;amp;pi;+ + Be at 60 GeV/c with Channel-Wise Subcollision Acceptance in PYTHIA 8 Angantyr</dc:title>
			<dc:creator>Nuha Felemban</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010008</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-19</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-19</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>8</prism:startingPage>
		<prism:doi>10.3390/particles9010008</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/7">

	<title>Particles, Vol. 9, Pages 7: Testing and Characterization of Detection Plane Elements of the XGIS Instrument on Board the THESEUS Mission</title>
	<link>https://www.mdpi.com/2571-712X/9/1/7</link>
	<description>This paper presents the procedures employed for experimental functional and performance characterization of a 2 &amp;amp;times; 2 pixel prototype detection system tailored specifically for the X and Gamma-ray Imaging Spectrometer (XGIS) instrument onboard the THESEUS mission. The XGIS system comprises of two coded masked wide field cameras integrated with monolithic SDDs (Silicon Drift Detectors) and CsI:Tl (Thallium doped-Cesium Iodide) scintillators, contributing to its broad X and &amp;amp;gamma;-ray detection range. Given the space instrumentation complexity, thorough requirement qualification and testing procedures are essential. This work focuses on working principle, the testing setup utilized, and observed performance for the small scale four-pixel XGIS prototype. Furthermore, the alignment of light output performance of the four-pixel SDD and scintillator prototype detection system with the XGIS instrument requirements is emphasized.</description>
	<pubDate>2026-01-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 7: Testing and Characterization of Detection Plane Elements of the XGIS Instrument on Board the THESEUS Mission</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/7">doi: 10.3390/particles9010007</a></p>
	<p>Authors:
		Smiriti Srivastava
		Evgeny Demenev
		Claudio Labanti
		Lorenzo Amati
		Riccardo Campana
		Giuseppe Baldazzi
		Edoardo Borciani
		Paolo Calabretto
		Francesco Ficorella
		Ezequiel J. Marchesini
		Giulia Mattioli
		Ajay Sharma
		David Novel
		Giancarlo Pepponi
		Enrico Virgilli
		</p>
	<p>This paper presents the procedures employed for experimental functional and performance characterization of a 2 &amp;amp;times; 2 pixel prototype detection system tailored specifically for the X and Gamma-ray Imaging Spectrometer (XGIS) instrument onboard the THESEUS mission. The XGIS system comprises of two coded masked wide field cameras integrated with monolithic SDDs (Silicon Drift Detectors) and CsI:Tl (Thallium doped-Cesium Iodide) scintillators, contributing to its broad X and &amp;amp;gamma;-ray detection range. Given the space instrumentation complexity, thorough requirement qualification and testing procedures are essential. This work focuses on working principle, the testing setup utilized, and observed performance for the small scale four-pixel XGIS prototype. Furthermore, the alignment of light output performance of the four-pixel SDD and scintillator prototype detection system with the XGIS instrument requirements is emphasized.</p>
	]]></content:encoded>

	<dc:title>Testing and Characterization of Detection Plane Elements of the XGIS Instrument on Board the THESEUS Mission</dc:title>
			<dc:creator>Smiriti Srivastava</dc:creator>
			<dc:creator>Evgeny Demenev</dc:creator>
			<dc:creator>Claudio Labanti</dc:creator>
			<dc:creator>Lorenzo Amati</dc:creator>
			<dc:creator>Riccardo Campana</dc:creator>
			<dc:creator>Giuseppe Baldazzi</dc:creator>
			<dc:creator>Edoardo Borciani</dc:creator>
			<dc:creator>Paolo Calabretto</dc:creator>
			<dc:creator>Francesco Ficorella</dc:creator>
			<dc:creator>Ezequiel J. Marchesini</dc:creator>
			<dc:creator>Giulia Mattioli</dc:creator>
			<dc:creator>Ajay Sharma</dc:creator>
			<dc:creator>David Novel</dc:creator>
			<dc:creator>Giancarlo Pepponi</dc:creator>
			<dc:creator>Enrico Virgilli</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010007</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-18</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-18</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>7</prism:startingPage>
		<prism:doi>10.3390/particles9010007</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/6">

	<title>Particles, Vol. 9, Pages 6: Critical Aspects in the Modeling of Sub-GeV Calorimetric Particle Detectors: The Case Study of the High-Energy Particle Detector (HEPD-02) on Board the CSES-02 Satellite</title>
	<link>https://www.mdpi.com/2571-712X/9/1/6</link>
	<description>The accurate simulation of sub-GeV particle detectors is essential for interpreting experimental data and optimizing detector design. This work identifies and addresses several critical aspects in modeling such detectors, taking as a case study the High-Energy Particle Detector (HEPD-02), a space-borne instrument developed within the CSES-02 mission to measure electrons in the &amp;amp;sim;3&amp;amp;ndash;100 MeV range, protons and light nuclei in the &amp;amp;sim;30&amp;amp;ndash;200 MeV/n. The HEPD-02 instrument consists of a silicon tracker, plastic and LYSO scintillator calorimeters, and anticoincidence systems, making it a representative example of a complex low-energy particle detector operating in Low Earth Orbit. Key challenges arise from replicating intricate detector geometries derived from CAD models, selecting appropriate hadronic physics lists for low-energy interactions, and accurately describing the detector response&amp;amp;mdash;particularly quenching effects in scintillators and digitization in solid-state tracking planes. Particular attention is given to three critical aspects: the precise CAD-level geometry implementation, the impact of hadronic physics models on the detector response, and the parameterization of scintillation quenching. In this study, we present original solutions to these challenges and provide data&amp;amp;ndash;MC comparisons using data from HEPD-02 beam tests.</description>
	<pubDate>2026-01-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 6: Critical Aspects in the Modeling of Sub-GeV Calorimetric Particle Detectors: The Case Study of the High-Energy Particle Detector (HEPD-02) on Board the CSES-02 Satellite</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/6">doi: 10.3390/particles9010006</a></p>
	<p>Authors:
		Simona Bartocci
		Roberto Battiston
		Stefania Beolè
		Franco Benotto
		Piero Cipollone
		Silvia Coli
		Andrea Contin
		Marco Cristoforetti
		Cinzia De Donato
		Cristian De Santis
		Andrea Di Luca
		Floarea Dumitrache
		Francesco Maria Follega
		Simone Garrafa Botta
		Giuseppe Gebbia
		Roberto Iuppa
		Alessandro Lega
		Mauro Lolli
		Giuseppe Masciantonio
		Matteo Mergè
		Marco Mese
		Riccardo Nicolaidis
		Francesco Nozzoli
		Alberto Oliva
		Giuseppe Osteria
		Francesco Palma
		Federico Palmonari
		Beatrice Panico
		Stefania Perciballi
		Francesco Perfetto
		Piergiorgio Picozza
		Michele Pozzato
		Marco Ricci
		Ester Ricci
		Sergio Bruno Ricciarini
		Zouleikha Sahnoun
		Umberto Savino
		Valentina Scotti
		Enrico Serra
		Alessandro Sotgiu
		Roberta Sparvoli
		Pietro Ubertini
		Veronica Vilona
		Simona Zoffoli
		Paolo Zuccon
		</p>
	<p>The accurate simulation of sub-GeV particle detectors is essential for interpreting experimental data and optimizing detector design. This work identifies and addresses several critical aspects in modeling such detectors, taking as a case study the High-Energy Particle Detector (HEPD-02), a space-borne instrument developed within the CSES-02 mission to measure electrons in the &amp;amp;sim;3&amp;amp;ndash;100 MeV range, protons and light nuclei in the &amp;amp;sim;30&amp;amp;ndash;200 MeV/n. The HEPD-02 instrument consists of a silicon tracker, plastic and LYSO scintillator calorimeters, and anticoincidence systems, making it a representative example of a complex low-energy particle detector operating in Low Earth Orbit. Key challenges arise from replicating intricate detector geometries derived from CAD models, selecting appropriate hadronic physics lists for low-energy interactions, and accurately describing the detector response&amp;amp;mdash;particularly quenching effects in scintillators and digitization in solid-state tracking planes. Particular attention is given to three critical aspects: the precise CAD-level geometry implementation, the impact of hadronic physics models on the detector response, and the parameterization of scintillation quenching. In this study, we present original solutions to these challenges and provide data&amp;amp;ndash;MC comparisons using data from HEPD-02 beam tests.</p>
	]]></content:encoded>

	<dc:title>Critical Aspects in the Modeling of Sub-GeV Calorimetric Particle Detectors: The Case Study of the High-Energy Particle Detector (HEPD-02) on Board the CSES-02 Satellite</dc:title>
			<dc:creator>Simona Bartocci</dc:creator>
			<dc:creator>Roberto Battiston</dc:creator>
			<dc:creator>Stefania Beolè</dc:creator>
			<dc:creator>Franco Benotto</dc:creator>
			<dc:creator>Piero Cipollone</dc:creator>
			<dc:creator>Silvia Coli</dc:creator>
			<dc:creator>Andrea Contin</dc:creator>
			<dc:creator>Marco Cristoforetti</dc:creator>
			<dc:creator>Cinzia De Donato</dc:creator>
			<dc:creator>Cristian De Santis</dc:creator>
			<dc:creator>Andrea Di Luca</dc:creator>
			<dc:creator>Floarea Dumitrache</dc:creator>
			<dc:creator>Francesco Maria Follega</dc:creator>
			<dc:creator>Simone Garrafa Botta</dc:creator>
			<dc:creator>Giuseppe Gebbia</dc:creator>
			<dc:creator>Roberto Iuppa</dc:creator>
			<dc:creator>Alessandro Lega</dc:creator>
			<dc:creator>Mauro Lolli</dc:creator>
			<dc:creator>Giuseppe Masciantonio</dc:creator>
			<dc:creator>Matteo Mergè</dc:creator>
			<dc:creator>Marco Mese</dc:creator>
			<dc:creator>Riccardo Nicolaidis</dc:creator>
			<dc:creator>Francesco Nozzoli</dc:creator>
			<dc:creator>Alberto Oliva</dc:creator>
			<dc:creator>Giuseppe Osteria</dc:creator>
			<dc:creator>Francesco Palma</dc:creator>
			<dc:creator>Federico Palmonari</dc:creator>
			<dc:creator>Beatrice Panico</dc:creator>
			<dc:creator>Stefania Perciballi</dc:creator>
			<dc:creator>Francesco Perfetto</dc:creator>
			<dc:creator>Piergiorgio Picozza</dc:creator>
			<dc:creator>Michele Pozzato</dc:creator>
			<dc:creator>Marco Ricci</dc:creator>
			<dc:creator>Ester Ricci</dc:creator>
			<dc:creator>Sergio Bruno Ricciarini</dc:creator>
			<dc:creator>Zouleikha Sahnoun</dc:creator>
			<dc:creator>Umberto Savino</dc:creator>
			<dc:creator>Valentina Scotti</dc:creator>
			<dc:creator>Enrico Serra</dc:creator>
			<dc:creator>Alessandro Sotgiu</dc:creator>
			<dc:creator>Roberta Sparvoli</dc:creator>
			<dc:creator>Pietro Ubertini</dc:creator>
			<dc:creator>Veronica Vilona</dc:creator>
			<dc:creator>Simona Zoffoli</dc:creator>
			<dc:creator>Paolo Zuccon</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010006</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-15</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-15</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>6</prism:startingPage>
		<prism:doi>10.3390/particles9010006</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/5">

	<title>Particles, Vol. 9, Pages 5: Coherent State Description of Astrophysical Gamma-Ray Amplification from a Para-Positronium Condensate</title>
	<link>https://www.mdpi.com/2571-712X/9/1/5</link>
	<description>The para-positronium system S01Ps is described by means of specially constructed coherent states (CSs) in the Klauder&amp;amp;ndash;Perelomov sense. It is analyzed from the physical point of view and from the geometry underlying the relevant symmetry group establishing the dynamics of the processes. In this new theoretical context, the possibility of a gamma-ray laser emission is investigated within a QFT context, showing explicitly that, in addition to the oscillator solution based only on a Bogoliubov approximation for the condensate, there is a second phase or &amp;amp;ldquo;squeezed&amp;amp;rdquo; stage by which physical features beyond the classical ones appear. Explicitly, while the generated photons are in the active medium (e.g., Ps-BEC), the evolution is described by a Heisenberg&amp;amp;ndash;Weyl coherent state with displacement operators dependent on the interaction time, which is related to the condensate shape. After the interaction time has elapsed, we explicitly demonstrate that the displacement operator of the S01Ps is transformed into a squeezed operator of the photonic fields modulated by the matrix element of the Positronium decay MS01Ps&amp;amp;rarr;2&amp;amp;gamma;. We also show that this squeezed operator (belonging to the Metaplectic group) generates a non-classical radiation state spanning only even (s = 1/4) levels in the number of photons. The implications in astrophysical systems of interest, considering gamma-ray coherent emission and the possibility of an S01Ps&amp;amp;minus;BEC in the context of pulsars, blazars, and quasars, are briefly discussed.</description>
	<pubDate>2026-01-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 5: Coherent State Description of Astrophysical Gamma-Ray Amplification from a Para-Positronium Condensate</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/5">doi: 10.3390/particles9010005</a></p>
	<p>Authors:
		Diego Julio Cirilo-Lombardo
		</p>
	<p>The para-positronium system S01Ps is described by means of specially constructed coherent states (CSs) in the Klauder&amp;amp;ndash;Perelomov sense. It is analyzed from the physical point of view and from the geometry underlying the relevant symmetry group establishing the dynamics of the processes. In this new theoretical context, the possibility of a gamma-ray laser emission is investigated within a QFT context, showing explicitly that, in addition to the oscillator solution based only on a Bogoliubov approximation for the condensate, there is a second phase or &amp;amp;ldquo;squeezed&amp;amp;rdquo; stage by which physical features beyond the classical ones appear. Explicitly, while the generated photons are in the active medium (e.g., Ps-BEC), the evolution is described by a Heisenberg&amp;amp;ndash;Weyl coherent state with displacement operators dependent on the interaction time, which is related to the condensate shape. After the interaction time has elapsed, we explicitly demonstrate that the displacement operator of the S01Ps is transformed into a squeezed operator of the photonic fields modulated by the matrix element of the Positronium decay MS01Ps&amp;amp;rarr;2&amp;amp;gamma;. We also show that this squeezed operator (belonging to the Metaplectic group) generates a non-classical radiation state spanning only even (s = 1/4) levels in the number of photons. The implications in astrophysical systems of interest, considering gamma-ray coherent emission and the possibility of an S01Ps&amp;amp;minus;BEC in the context of pulsars, blazars, and quasars, are briefly discussed.</p>
	]]></content:encoded>

	<dc:title>Coherent State Description of Astrophysical Gamma-Ray Amplification from a Para-Positronium Condensate</dc:title>
			<dc:creator>Diego Julio Cirilo-Lombardo</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010005</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-14</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-14</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>5</prism:startingPage>
		<prism:doi>10.3390/particles9010005</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/4">

	<title>Particles, Vol. 9, Pages 4: Spectral Performance of Single-Channel Plastic and GAGG Scintillator Bars of the CUbesat Solar Polarimeter (CUSP)</title>
	<link>https://www.mdpi.com/2571-712X/9/1/4</link>
	<description>Our Sun is the closest X-ray astrophysical source to Earth. As such, it makes for a strong case study to better understand astrophysical processes. Solar flares are particularly interesting as they are linked to coronal mass ejections as well as magnetic field reconnection sites in the solar atmosphere. Flares can therefore provide insightful information on the physical processes at play on their production sites but also on the emission and acceleration of energetic charged particles towards our planet, making it an excellent forecasting tool for space weather. While solar flares are critical to understanding magnetic reconnection and particle acceleration, their hard X-ray polarization&amp;amp;mdash;key to distinguishing between competing theoretical models&amp;amp;mdash;remains poorly constrained by existing observations. To address this, we present the CUbesat Solar Polarimeter (CUSP), a mission under development to perform solar flare polarimetry in the 25&amp;amp;ndash;100 keV energy range. CUSP consists of a 6U-XL platform hosting a dual-phase Compton polarimeter. The polarimeter is made of a central assembly of four 4 &amp;amp;times; 4 arrays of plastic scintillators, each coupled to multi-anode photomultiplier tubes, surrounded by four strips of eight elongated GAGG scintillator bars coupled to avalanche photodiodes. Both types of sensors from Hamamatsu are, respectively, read out by the MAROC-3A and SKIROC-2A ASICs from Weeroc. In this manuscript, we present the preliminary spectral performances of single plastic and GAGG channels measured in a laboratory using development boards of the ASICs foreseen for the flight model.</description>
	<pubDate>2026-01-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 4: Spectral Performance of Single-Channel Plastic and GAGG Scintillator Bars of the CUbesat Solar Polarimeter (CUSP)</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/4">doi: 10.3390/particles9010004</a></p>
	<p>Authors:
		Nicolas De Angelis
		Abhay Kumar
		Sergio Fabiani
		Ettore Del Monte
		Enrico Costa
		Giovanni Lombardi
		Alda Rubini
		Paolo Soffitta
		Andrea Alimenti
		Riccardo Campana
		Mauro Centrone
		Giovanni De Cesare
		Sergio Di Cosimo
		Giuseppe Di Persio
		Alessandro Lacerenza
		Pasqualino Loffredo
		Gabriele Minervini
		Fabio Muleri
		Paolo Romano
		Emanuele Scalise
		Enrico Silva
		Davide Albanesi
		Ilaria Baffo
		Daniele Brienza
		Valerio Campomaggiore
		Giovanni Cucinella
		Andrea Curatolo
		Giulia de Iulis
		Andrea Del Re
		Vito Di Bari
		Simone Di Filippo
		Immacolata Donnarumma
		Pierluigi Fanelli
		Nicolas Gagliardi
		Paolo Leonetti
		Matteo Mergè
		Dario Modenini
		Andrea Negri
		Daniele Pecorella
		Massimo Perelli
		Alice Ponti
		Francesca Sbop
		Paolo Tortora
		Alessandro Turchi
		Valerio Vagelli
		Emanuele Zaccagnino
		Alessandro Zambardi
		Costantino Zazza
		</p>
	<p>Our Sun is the closest X-ray astrophysical source to Earth. As such, it makes for a strong case study to better understand astrophysical processes. Solar flares are particularly interesting as they are linked to coronal mass ejections as well as magnetic field reconnection sites in the solar atmosphere. Flares can therefore provide insightful information on the physical processes at play on their production sites but also on the emission and acceleration of energetic charged particles towards our planet, making it an excellent forecasting tool for space weather. While solar flares are critical to understanding magnetic reconnection and particle acceleration, their hard X-ray polarization&amp;amp;mdash;key to distinguishing between competing theoretical models&amp;amp;mdash;remains poorly constrained by existing observations. To address this, we present the CUbesat Solar Polarimeter (CUSP), a mission under development to perform solar flare polarimetry in the 25&amp;amp;ndash;100 keV energy range. CUSP consists of a 6U-XL platform hosting a dual-phase Compton polarimeter. The polarimeter is made of a central assembly of four 4 &amp;amp;times; 4 arrays of plastic scintillators, each coupled to multi-anode photomultiplier tubes, surrounded by four strips of eight elongated GAGG scintillator bars coupled to avalanche photodiodes. Both types of sensors from Hamamatsu are, respectively, read out by the MAROC-3A and SKIROC-2A ASICs from Weeroc. In this manuscript, we present the preliminary spectral performances of single plastic and GAGG channels measured in a laboratory using development boards of the ASICs foreseen for the flight model.</p>
	]]></content:encoded>

	<dc:title>Spectral Performance of Single-Channel Plastic and GAGG Scintillator Bars of the CUbesat Solar Polarimeter (CUSP)</dc:title>
			<dc:creator>Nicolas De Angelis</dc:creator>
			<dc:creator>Abhay Kumar</dc:creator>
			<dc:creator>Sergio Fabiani</dc:creator>
			<dc:creator>Ettore Del Monte</dc:creator>
			<dc:creator>Enrico Costa</dc:creator>
			<dc:creator>Giovanni Lombardi</dc:creator>
			<dc:creator>Alda Rubini</dc:creator>
			<dc:creator>Paolo Soffitta</dc:creator>
			<dc:creator>Andrea Alimenti</dc:creator>
			<dc:creator>Riccardo Campana</dc:creator>
			<dc:creator>Mauro Centrone</dc:creator>
			<dc:creator>Giovanni De Cesare</dc:creator>
			<dc:creator>Sergio Di Cosimo</dc:creator>
			<dc:creator>Giuseppe Di Persio</dc:creator>
			<dc:creator>Alessandro Lacerenza</dc:creator>
			<dc:creator>Pasqualino Loffredo</dc:creator>
			<dc:creator>Gabriele Minervini</dc:creator>
			<dc:creator>Fabio Muleri</dc:creator>
			<dc:creator>Paolo Romano</dc:creator>
			<dc:creator>Emanuele Scalise</dc:creator>
			<dc:creator>Enrico Silva</dc:creator>
			<dc:creator>Davide Albanesi</dc:creator>
			<dc:creator>Ilaria Baffo</dc:creator>
			<dc:creator>Daniele Brienza</dc:creator>
			<dc:creator>Valerio Campomaggiore</dc:creator>
			<dc:creator>Giovanni Cucinella</dc:creator>
			<dc:creator>Andrea Curatolo</dc:creator>
			<dc:creator>Giulia de Iulis</dc:creator>
			<dc:creator>Andrea Del Re</dc:creator>
			<dc:creator>Vito Di Bari</dc:creator>
			<dc:creator>Simone Di Filippo</dc:creator>
			<dc:creator>Immacolata Donnarumma</dc:creator>
			<dc:creator>Pierluigi Fanelli</dc:creator>
			<dc:creator>Nicolas Gagliardi</dc:creator>
			<dc:creator>Paolo Leonetti</dc:creator>
			<dc:creator>Matteo Mergè</dc:creator>
			<dc:creator>Dario Modenini</dc:creator>
			<dc:creator>Andrea Negri</dc:creator>
			<dc:creator>Daniele Pecorella</dc:creator>
			<dc:creator>Massimo Perelli</dc:creator>
			<dc:creator>Alice Ponti</dc:creator>
			<dc:creator>Francesca Sbop</dc:creator>
			<dc:creator>Paolo Tortora</dc:creator>
			<dc:creator>Alessandro Turchi</dc:creator>
			<dc:creator>Valerio Vagelli</dc:creator>
			<dc:creator>Emanuele Zaccagnino</dc:creator>
			<dc:creator>Alessandro Zambardi</dc:creator>
			<dc:creator>Costantino Zazza</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010004</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-13</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-13</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/particles9010004</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/3">

	<title>Particles, Vol. 9, Pages 3: The X and Gamma-Ray Imager and Spectrometer Onboard THESEUS&amp;mdash;Status and Technological Progresses</title>
	<link>https://www.mdpi.com/2571-712X/9/1/3</link>
	<description>Gamma-Ray Bursts (GRBs) are intense bursts of high-energy photons which, in just a few seconds, outshine all other &amp;amp;gamma;-ray emitters in the sky. Due to their extreme luminosity, GRBs are not only important as high-energy astrophysical phenomena but also serve as valuable probe models of the far, high-redshift Universe. The importance of these events has pushed the High-Energy Astrophysics community to propose new mission concepts over the past decade, prompting dedicated research and development efforts to achieve the required technological readiness levels. The X and Gamma-Ray Imager and Spectrometer (XGIS) is one of the two GRB monitors onboard the proposed, upcoming THESEUS space mission. Building on strong heritage from previous studies, ongoing developments and optimizations are focused on enhancing the instrument&amp;amp;rsquo;s capabilities and increasing its technological maturity. This work presents the current status of the XGIS instrument and the latest technological advancements achieved in preparation for its deployment on THESEUS.</description>
	<pubDate>2026-01-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 3: The X and Gamma-Ray Imager and Spectrometer Onboard THESEUS&amp;mdash;Status and Technological Progresses</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/3">doi: 10.3390/particles9010003</a></p>
	<p>Authors:
		Giulia Mattioli
		Claudio Labanti
		Enrico Virgilli
		Lorenzo Amati
		Riccardo Campana
		Giuseppe Baldazzi
		Smiriti Srivastava
		Edoardo Borciani
		Paolo Calabretto
		Ezequiel J. Marchesini
		Ajay Sharma
		Evgeny Demenev
		Francesco Ficorella
		David Novel
		Giancarlo Pepponi
		Giovanni La Rosa
		Paolo Nogara
		Giuseppe Sottile
		</p>
	<p>Gamma-Ray Bursts (GRBs) are intense bursts of high-energy photons which, in just a few seconds, outshine all other &amp;amp;gamma;-ray emitters in the sky. Due to their extreme luminosity, GRBs are not only important as high-energy astrophysical phenomena but also serve as valuable probe models of the far, high-redshift Universe. The importance of these events has pushed the High-Energy Astrophysics community to propose new mission concepts over the past decade, prompting dedicated research and development efforts to achieve the required technological readiness levels. The X and Gamma-Ray Imager and Spectrometer (XGIS) is one of the two GRB monitors onboard the proposed, upcoming THESEUS space mission. Building on strong heritage from previous studies, ongoing developments and optimizations are focused on enhancing the instrument&amp;amp;rsquo;s capabilities and increasing its technological maturity. This work presents the current status of the XGIS instrument and the latest technological advancements achieved in preparation for its deployment on THESEUS.</p>
	]]></content:encoded>

	<dc:title>The X and Gamma-Ray Imager and Spectrometer Onboard THESEUS&amp;amp;mdash;Status and Technological Progresses</dc:title>
			<dc:creator>Giulia Mattioli</dc:creator>
			<dc:creator>Claudio Labanti</dc:creator>
			<dc:creator>Enrico Virgilli</dc:creator>
			<dc:creator>Lorenzo Amati</dc:creator>
			<dc:creator>Riccardo Campana</dc:creator>
			<dc:creator>Giuseppe Baldazzi</dc:creator>
			<dc:creator>Smiriti Srivastava</dc:creator>
			<dc:creator>Edoardo Borciani</dc:creator>
			<dc:creator>Paolo Calabretto</dc:creator>
			<dc:creator>Ezequiel J. Marchesini</dc:creator>
			<dc:creator>Ajay Sharma</dc:creator>
			<dc:creator>Evgeny Demenev</dc:creator>
			<dc:creator>Francesco Ficorella</dc:creator>
			<dc:creator>David Novel</dc:creator>
			<dc:creator>Giancarlo Pepponi</dc:creator>
			<dc:creator>Giovanni La Rosa</dc:creator>
			<dc:creator>Paolo Nogara</dc:creator>
			<dc:creator>Giuseppe Sottile</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010003</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-08</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-08</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Technical Note</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/particles9010003</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/2">

	<title>Particles, Vol. 9, Pages 2: Unlocking the Future of X-Ray Polarimetry with IXPE: Lessons Learned and Next Steps</title>
	<link>https://www.mdpi.com/2571-712X/9/1/2</link>
	<description>This paper discusses issues encountered during the early development of the instrument on the Imaging X-ray Polarimetry Explorer (IXPE), a NASA&amp;amp;ndash;ASI Small Explorer mission launched on 9 December 2021. IXPE has observed about 100 sources, yielding meaningful polarimetry for most of them. An on-board calibration system mitigated most non-ideal detector behaviors during operations. Data from the on-board polarized and unpolarized X-ray sources are routinely ingested by the flight pipeline to correct the instrument response in a manner transparent to users. Based on its scientific return and payload health, the IXPE mission has been extended through 2028. The lessons learned are informing the design of next-generation X-ray polarimetry missions, as discussed elsewhere in these conferences.</description>
	<pubDate>2026-01-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 2: Unlocking the Future of X-Ray Polarimetry with IXPE: Lessons Learned and Next Steps</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/2">doi: 10.3390/particles9010002</a></p>
	<p>Authors:
		Paolo Soffitta
		Enrico Costa
		Ettore Del Monte
		Alessandro Di Marco
		Sergio Fabiani
		Riccardo Ferrazzoli
		Fabio La Monaca
		Fabio Muleri
		Alda Rubini
		Alessio Trois
		</p>
	<p>This paper discusses issues encountered during the early development of the instrument on the Imaging X-ray Polarimetry Explorer (IXPE), a NASA&amp;amp;ndash;ASI Small Explorer mission launched on 9 December 2021. IXPE has observed about 100 sources, yielding meaningful polarimetry for most of them. An on-board calibration system mitigated most non-ideal detector behaviors during operations. Data from the on-board polarized and unpolarized X-ray sources are routinely ingested by the flight pipeline to correct the instrument response in a manner transparent to users. Based on its scientific return and payload health, the IXPE mission has been extended through 2028. The lessons learned are informing the design of next-generation X-ray polarimetry missions, as discussed elsewhere in these conferences.</p>
	]]></content:encoded>

	<dc:title>Unlocking the Future of X-Ray Polarimetry with IXPE: Lessons Learned and Next Steps</dc:title>
			<dc:creator>Paolo Soffitta</dc:creator>
			<dc:creator>Enrico Costa</dc:creator>
			<dc:creator>Ettore Del Monte</dc:creator>
			<dc:creator>Alessandro Di Marco</dc:creator>
			<dc:creator>Sergio Fabiani</dc:creator>
			<dc:creator>Riccardo Ferrazzoli</dc:creator>
			<dc:creator>Fabio La Monaca</dc:creator>
			<dc:creator>Fabio Muleri</dc:creator>
			<dc:creator>Alda Rubini</dc:creator>
			<dc:creator>Alessio Trois</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010002</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-06</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-06</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/particles9010002</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/9/1/1">

	<title>Particles, Vol. 9, Pages 1: Review of the Performance of the CMS Hadron Calorimeter</title>
	<link>https://www.mdpi.com/2571-712X/9/1/1</link>
	<description>The hadron calorimeter is a central component of the CMS detector, vital for measuring hadron energies and reconstructing missing transverse momentum. This paper reviews its performance before and after the Phase 1 upgrade (completed in 2019), which upgraded both back-end and front-end electronics, including photodetectors and charge-integrating ADC with precise-timing TDC, as well as its depth segmentation in the barrel and endcaps. This paper describes energy reconstruction algorithms that suppress out-of-time signals, along with high-precision timing alignment and multi-step energy calibration procedures to mitigate radiation damage and improve energy resolution Performance evaluations using proton&amp;amp;ndash;proton collision data demonstrate that the upgraded detector and reconstruction techniques achieve good resolution and robust operation under high-luminosity conditions.</description>
	<pubDate>2026-01-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 9, Pages 1: Review of the Performance of the CMS Hadron Calorimeter</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/9/1/1">doi: 10.3390/particles9010001</a></p>
	<p>Authors:
		Yide Wei
		Hui Wang
		</p>
	<p>The hadron calorimeter is a central component of the CMS detector, vital for measuring hadron energies and reconstructing missing transverse momentum. This paper reviews its performance before and after the Phase 1 upgrade (completed in 2019), which upgraded both back-end and front-end electronics, including photodetectors and charge-integrating ADC with precise-timing TDC, as well as its depth segmentation in the barrel and endcaps. This paper describes energy reconstruction algorithms that suppress out-of-time signals, along with high-precision timing alignment and multi-step energy calibration procedures to mitigate radiation damage and improve energy resolution Performance evaluations using proton&amp;amp;ndash;proton collision data demonstrate that the upgraded detector and reconstruction techniques achieve good resolution and robust operation under high-luminosity conditions.</p>
	]]></content:encoded>

	<dc:title>Review of the Performance of the CMS Hadron Calorimeter</dc:title>
			<dc:creator>Yide Wei</dc:creator>
			<dc:creator>Hui Wang</dc:creator>
		<dc:identifier>doi: 10.3390/particles9010001</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2026-01-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2026-01-02</prism:publicationDate>
	<prism:volume>9</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/particles9010001</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/9/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/104">

	<title>Particles, Vol. 8, Pages 104: Enhanced Energy Transfer in Resonating Gold Doped Matter Irradiated by Infrared Laser</title>
	<link>https://www.mdpi.com/2571-712X/8/4/104</link>
	<description>Laser-driven ion acceleration in dense, hydrogen-rich media can be significantly enhanced by embedding metallic nanoantennas that support localized surface plasmon (LSP) resonances. Using large-scale particle-in-cell (PIC) simulations with the EPOCH code, we investigate how nanoantenna geometry and laser pulse parameters influence proton acceleration in gold-doped polymer targets. The study covers dipole, crossed, and advanced 3D-cross antenna configurations under laser intensities of 1017&amp;amp;ndash;1019 W/cm2 and pulse durations from 2.5 to 500 fs, corresponding to experimental conditions at the ELI laser facility. Results show that the dipole antennas exhibit resonance-limited proton energies of ~0.12 MeV, with optimal acceleration at the intensities 4 &amp;amp;times; 1017&amp;amp;ndash;1 &amp;amp;times; 1018 W/cm2 and pulse durations around 100&amp;amp;ndash;150 fs. This energy is higher by roughly three orders of magnitude than the proton energy for the same field and same polymer without dopes: ~1&amp;amp;ndash;2 &amp;amp;times; 10&amp;amp;minus;4 MeV. Crossed antennas achieve higher energies (~0.2 MeV) due to dual-mode plasmonic coupling that sustains local fields longer. Advanced 3D and Yagi-like geometries further enhance field localization, yielding proton energies up to 0.4 MeV and larger high-energy proton populations. For dipole antennas, experimental data from ELI exists and our results agree with it. We find that moderate pulses preserve plasmonic resonance for longer and improve energy transfer efficiency, while overly intense pulses disrupt the resonance early. These findings reveal that plasmonic field enhancement and its lifetime govern energy transfer efficiency in laser&amp;amp;ndash;matter interaction. Crossed and 3D geometries with optimized spacing enable multimode resonance and sequential proton acceleration, overcoming the saturation limitations of simple dipoles. The results establish clear design principles for tailoring nanoantenna geometry and pulse characteristics to optimize compact, high-energy proton sources for inertial confinement fusion and high-energy-density applications.</description>
	<pubDate>2025-12-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 104: Enhanced Energy Transfer in Resonating Gold Doped Matter Irradiated by Infrared Laser</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/104">doi: 10.3390/particles8040104</a></p>
	<p>Authors:
		Konstantin Zsukovszki
		Istvan Papp
		</p>
	<p>Laser-driven ion acceleration in dense, hydrogen-rich media can be significantly enhanced by embedding metallic nanoantennas that support localized surface plasmon (LSP) resonances. Using large-scale particle-in-cell (PIC) simulations with the EPOCH code, we investigate how nanoantenna geometry and laser pulse parameters influence proton acceleration in gold-doped polymer targets. The study covers dipole, crossed, and advanced 3D-cross antenna configurations under laser intensities of 1017&amp;amp;ndash;1019 W/cm2 and pulse durations from 2.5 to 500 fs, corresponding to experimental conditions at the ELI laser facility. Results show that the dipole antennas exhibit resonance-limited proton energies of ~0.12 MeV, with optimal acceleration at the intensities 4 &amp;amp;times; 1017&amp;amp;ndash;1 &amp;amp;times; 1018 W/cm2 and pulse durations around 100&amp;amp;ndash;150 fs. This energy is higher by roughly three orders of magnitude than the proton energy for the same field and same polymer without dopes: ~1&amp;amp;ndash;2 &amp;amp;times; 10&amp;amp;minus;4 MeV. Crossed antennas achieve higher energies (~0.2 MeV) due to dual-mode plasmonic coupling that sustains local fields longer. Advanced 3D and Yagi-like geometries further enhance field localization, yielding proton energies up to 0.4 MeV and larger high-energy proton populations. For dipole antennas, experimental data from ELI exists and our results agree with it. We find that moderate pulses preserve plasmonic resonance for longer and improve energy transfer efficiency, while overly intense pulses disrupt the resonance early. These findings reveal that plasmonic field enhancement and its lifetime govern energy transfer efficiency in laser&amp;amp;ndash;matter interaction. Crossed and 3D geometries with optimized spacing enable multimode resonance and sequential proton acceleration, overcoming the saturation limitations of simple dipoles. The results establish clear design principles for tailoring nanoantenna geometry and pulse characteristics to optimize compact, high-energy proton sources for inertial confinement fusion and high-energy-density applications.</p>
	]]></content:encoded>

	<dc:title>Enhanced Energy Transfer in Resonating Gold Doped Matter Irradiated by Infrared Laser</dc:title>
			<dc:creator>Konstantin Zsukovszki</dc:creator>
			<dc:creator>Istvan Papp</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040104</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-18</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-18</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>104</prism:startingPage>
		<prism:doi>10.3390/particles8040104</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/104</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/103">

	<title>Particles, Vol. 8, Pages 103: Insights into the Temperature Parameters from K*0 Spectrum in Nuclear Particle Collisions at the Relativistic High-Energy Collider Beam Energies</title>
	<link>https://www.mdpi.com/2571-712X/8/4/103</link>
	<description>The blast-wave model with Boltzmann&amp;amp;ndash;Gibbs statistics is used to examine the transverse momentum spectra of K&amp;amp;lowast;0 mesons generated at the Relativistic High-Energy Collider (RHIC) Beam Energies with mid-rapidity (|y|&amp;amp;lt;1) in symmetric Au&amp;amp;minus;Au collisions. There is a clear correlation between the extracted kinetic freeze-out temperature (T0) and transverse flow velocity (&amp;amp;beta;T) in various collision centralities and center-of-mass energies (sNN). Since a larger initial energy density delays freeze-out and a shorter system lifetime limits cooling, T0 is directly proportional to both sNN and peripheral collisions. On the other hand, &amp;amp;beta;T drops in peripheral symmetric collisions due to weaker collective expansion, while it rises with sNN because of larger pressure gradients. The concurrence between the thermal and collective energy components in the expanding fireball is reflected in the obvious anti-correlation between T0 and &amp;amp;beta;T. These findings support hydrodynamic predictions and offer important new information about QGP&amp;amp;rsquo;s freeze-out behavior.</description>
	<pubDate>2025-12-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 103: Insights into the Temperature Parameters from K*0 Spectrum in Nuclear Particle Collisions at the Relativistic High-Energy Collider Beam Energies</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/103">doi: 10.3390/particles8040103</a></p>
	<p>Authors:
		Pei-Pin Yang
		Abd Haj Ismail
		</p>
	<p>The blast-wave model with Boltzmann&amp;amp;ndash;Gibbs statistics is used to examine the transverse momentum spectra of K&amp;amp;lowast;0 mesons generated at the Relativistic High-Energy Collider (RHIC) Beam Energies with mid-rapidity (|y|&amp;amp;lt;1) in symmetric Au&amp;amp;minus;Au collisions. There is a clear correlation between the extracted kinetic freeze-out temperature (T0) and transverse flow velocity (&amp;amp;beta;T) in various collision centralities and center-of-mass energies (sNN). Since a larger initial energy density delays freeze-out and a shorter system lifetime limits cooling, T0 is directly proportional to both sNN and peripheral collisions. On the other hand, &amp;amp;beta;T drops in peripheral symmetric collisions due to weaker collective expansion, while it rises with sNN because of larger pressure gradients. The concurrence between the thermal and collective energy components in the expanding fireball is reflected in the obvious anti-correlation between T0 and &amp;amp;beta;T. These findings support hydrodynamic predictions and offer important new information about QGP&amp;amp;rsquo;s freeze-out behavior.</p>
	]]></content:encoded>

	<dc:title>Insights into the Temperature Parameters from K*0 Spectrum in Nuclear Particle Collisions at the Relativistic High-Energy Collider Beam Energies</dc:title>
			<dc:creator>Pei-Pin Yang</dc:creator>
			<dc:creator>Abd Haj Ismail</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040103</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-15</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-15</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>103</prism:startingPage>
		<prism:doi>10.3390/particles8040103</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/103</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/102">

	<title>Particles, Vol. 8, Pages 102: Onboard Machine Learning for High-Energy Observatories for Spacecraft Autonomy and Ground Segment Operations</title>
	<link>https://www.mdpi.com/2571-712X/8/4/102</link>
	<description>Next-generation space observatories for high-energy gamma-ray astrophysics will increase scientific return using onboard machine learning (ML). This is now possible thanks to today&amp;amp;rsquo;s low-power, radiation-tolerant processors and artificial intelligence accelerators. This paper provides an overview of current and future ML applications in gamma-ray space missions focused on high-energy transient phenomena. We discuss onboard ML use cases that will be implemented in the future, including real-time event detection and classification (e.g., gamma-ray bursts), and autonomous decision-making, such as rapid repointing to transient events or optimising instrument configuration based on the scientific target or environmental conditions.</description>
	<pubDate>2025-12-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 102: Onboard Machine Learning for High-Energy Observatories for Spacecraft Autonomy and Ground Segment Operations</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/102">doi: 10.3390/particles8040102</a></p>
	<p>Authors:
		Andrea Bulgarelli
		Luca Castaldini
		Nicolò Parmiggiani
		Ambra Di Piano
		Riccardo Falco
		Alessio Aboudan
		Lorenzo Amati
		Andrea Argan
		Paolo Calabretto
		Mauro Dadina
		Adriano De Rosa
		Valentina Fioretti
		Claudio Labanti
		Giulia Mattioli
		Gabriele Panebianco
		Carlotta Pittori
		Alessandro Rizzo
		Smiriti Srivastava
		Enrico Virgilli
		</p>
	<p>Next-generation space observatories for high-energy gamma-ray astrophysics will increase scientific return using onboard machine learning (ML). This is now possible thanks to today&amp;amp;rsquo;s low-power, radiation-tolerant processors and artificial intelligence accelerators. This paper provides an overview of current and future ML applications in gamma-ray space missions focused on high-energy transient phenomena. We discuss onboard ML use cases that will be implemented in the future, including real-time event detection and classification (e.g., gamma-ray bursts), and autonomous decision-making, such as rapid repointing to transient events or optimising instrument configuration based on the scientific target or environmental conditions.</p>
	]]></content:encoded>

	<dc:title>Onboard Machine Learning for High-Energy Observatories for Spacecraft Autonomy and Ground Segment Operations</dc:title>
			<dc:creator>Andrea Bulgarelli</dc:creator>
			<dc:creator>Luca Castaldini</dc:creator>
			<dc:creator>Nicolò Parmiggiani</dc:creator>
			<dc:creator>Ambra Di Piano</dc:creator>
			<dc:creator>Riccardo Falco</dc:creator>
			<dc:creator>Alessio Aboudan</dc:creator>
			<dc:creator>Lorenzo Amati</dc:creator>
			<dc:creator>Andrea Argan</dc:creator>
			<dc:creator>Paolo Calabretto</dc:creator>
			<dc:creator>Mauro Dadina</dc:creator>
			<dc:creator>Adriano De Rosa</dc:creator>
			<dc:creator>Valentina Fioretti</dc:creator>
			<dc:creator>Claudio Labanti</dc:creator>
			<dc:creator>Giulia Mattioli</dc:creator>
			<dc:creator>Gabriele Panebianco</dc:creator>
			<dc:creator>Carlotta Pittori</dc:creator>
			<dc:creator>Alessandro Rizzo</dc:creator>
			<dc:creator>Smiriti Srivastava</dc:creator>
			<dc:creator>Enrico Virgilli</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040102</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-12</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Perspective</prism:section>
	<prism:startingPage>102</prism:startingPage>
		<prism:doi>10.3390/particles8040102</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/102</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/101">

	<title>Particles, Vol. 8, Pages 101: The EPSI R&amp;amp;D: Development of an Innovative Electron&amp;ndash;Positron Discrimination Technique for Space Applications</title>
	<link>https://www.mdpi.com/2571-712X/8/4/101</link>
	<description>The study of the antimatter component in cosmic rays is essential for the understanding of their acceleration and propagation mechanisms, and is one of the most powerful tools for the indirect search of dark matter. Current methods rely on magnetic spectrometers for charge-sign discrimination, but these are not suitable for extending measurements to the TeV region within a short timeframe of a few decades. Since most of present and upcoming high-energy space experiments use large calorimeters, it is crucial to develop an alternative charge-sign discrimination technique that can be integrated with them. The Electron/Positron Space Instrument (EPSI) project, a two-year R&amp;amp;amp;D initiative launched in 2023 with EU recovery funds, aims to address this challenge. The basic idea is to exploit the synchrotron radiation emitted by charged particles moving through Earth&amp;amp;rsquo;s magnetic field. The simultaneous detection of an electron/positron with an electromagnetic calorimeter and synchrotron photons with an X-ray detector is enough to discriminate between the two particles at the event level. The main challenge is to develop an X-ray detector with a very large active area, high X-ray detection efficiency, and a low-energy detection threshold, compliant with space applications. In this paper, we give an overview of the EPSI project, with a focus on the general idea of the detection principle, the concept of the space instrument, and the design of the X-ray detector.</description>
	<pubDate>2025-12-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 101: The EPSI R&amp;amp;D: Development of an Innovative Electron&amp;ndash;Positron Discrimination Technique for Space Applications</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/101">doi: 10.3390/particles8040101</a></p>
	<p>Authors:
		Oscar Adriani
		Lucia Baldesi
		Eugenio Berti
		Pietro Betti
		Massimo Bongi
		Alberto Camaiani
		Massimo Chiari
		Raffaello D’Alessandro
		Giacomo De Giorgi
		Noemi Finetti
		Leonardo Forcieri
		Elena Gensini
		Andrea Paccagnella
		Lorenzo Pacini
		Paolo Papini
		Oleksandr Starodubtsev
		Anna Vinattieri
		Chiara Volpato
		</p>
	<p>The study of the antimatter component in cosmic rays is essential for the understanding of their acceleration and propagation mechanisms, and is one of the most powerful tools for the indirect search of dark matter. Current methods rely on magnetic spectrometers for charge-sign discrimination, but these are not suitable for extending measurements to the TeV region within a short timeframe of a few decades. Since most of present and upcoming high-energy space experiments use large calorimeters, it is crucial to develop an alternative charge-sign discrimination technique that can be integrated with them. The Electron/Positron Space Instrument (EPSI) project, a two-year R&amp;amp;amp;D initiative launched in 2023 with EU recovery funds, aims to address this challenge. The basic idea is to exploit the synchrotron radiation emitted by charged particles moving through Earth&amp;amp;rsquo;s magnetic field. The simultaneous detection of an electron/positron with an electromagnetic calorimeter and synchrotron photons with an X-ray detector is enough to discriminate between the two particles at the event level. The main challenge is to develop an X-ray detector with a very large active area, high X-ray detection efficiency, and a low-energy detection threshold, compliant with space applications. In this paper, we give an overview of the EPSI project, with a focus on the general idea of the detection principle, the concept of the space instrument, and the design of the X-ray detector.</p>
	]]></content:encoded>

	<dc:title>The EPSI R&amp;amp;amp;D: Development of an Innovative Electron&amp;amp;ndash;Positron Discrimination Technique for Space Applications</dc:title>
			<dc:creator>Oscar Adriani</dc:creator>
			<dc:creator>Lucia Baldesi</dc:creator>
			<dc:creator>Eugenio Berti</dc:creator>
			<dc:creator>Pietro Betti</dc:creator>
			<dc:creator>Massimo Bongi</dc:creator>
			<dc:creator>Alberto Camaiani</dc:creator>
			<dc:creator>Massimo Chiari</dc:creator>
			<dc:creator>Raffaello D’Alessandro</dc:creator>
			<dc:creator>Giacomo De Giorgi</dc:creator>
			<dc:creator>Noemi Finetti</dc:creator>
			<dc:creator>Leonardo Forcieri</dc:creator>
			<dc:creator>Elena Gensini</dc:creator>
			<dc:creator>Andrea Paccagnella</dc:creator>
			<dc:creator>Lorenzo Pacini</dc:creator>
			<dc:creator>Paolo Papini</dc:creator>
			<dc:creator>Oleksandr Starodubtsev</dc:creator>
			<dc:creator>Anna Vinattieri</dc:creator>
			<dc:creator>Chiara Volpato</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040101</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-12</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>101</prism:startingPage>
		<prism:doi>10.3390/particles8040101</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/101</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/100">

	<title>Particles, Vol. 8, Pages 100: Neutrino-Pair Bremsstrahlung Due to Electromagnetic Collisions in Neutron Star Cores Revisited</title>
	<link>https://www.mdpi.com/2571-712X/8/4/100</link>
	<description>We reconsider the problem of neutrino-pair bremsstrahlung emission originating from the electromagnetic collisions of charged particles in nucleonic (npe&amp;amp;mu;) neutron star cores. Two limiting cases are considered: (i) protons in the normal state and (ii) protons in the superconducting state. In both cases, the dominant contribution to the bremsstrahlung emissivity QBrem comes from the transverse part of in-medium electromagnetic interactions. For non-superconducting matter, we obtain an unusual QBrem&amp;amp;prop;T23/3 temperature dependence due to the dynamical character of plasma screening in the transverse channel, but these are considerably smaller values of QBrem than in previous studies, rendering the considered process unimportant in practice. In contrast, for superconducting and superfluid matter, the neutrino emission processes involving nucleons are suppressed and QBrem due to lepton collisions provides the residual contribution to the neutrino emissivity of neutron star core matter. In the superconducting case, the plasma screening becomes static and the standard QBrem&amp;amp;prop;T8 temperature scaling is restored. Simple analytical expressions for QBrem in both limiting cases are provided.</description>
	<pubDate>2025-12-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 100: Neutrino-Pair Bremsstrahlung Due to Electromagnetic Collisions in Neutron Star Cores Revisited</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/100">doi: 10.3390/particles8040100</a></p>
	<p>Authors:
		Peter S. Shternin
		</p>
	<p>We reconsider the problem of neutrino-pair bremsstrahlung emission originating from the electromagnetic collisions of charged particles in nucleonic (npe&amp;amp;mu;) neutron star cores. Two limiting cases are considered: (i) protons in the normal state and (ii) protons in the superconducting state. In both cases, the dominant contribution to the bremsstrahlung emissivity QBrem comes from the transverse part of in-medium electromagnetic interactions. For non-superconducting matter, we obtain an unusual QBrem&amp;amp;prop;T23/3 temperature dependence due to the dynamical character of plasma screening in the transverse channel, but these are considerably smaller values of QBrem than in previous studies, rendering the considered process unimportant in practice. In contrast, for superconducting and superfluid matter, the neutrino emission processes involving nucleons are suppressed and QBrem due to lepton collisions provides the residual contribution to the neutrino emissivity of neutron star core matter. In the superconducting case, the plasma screening becomes static and the standard QBrem&amp;amp;prop;T8 temperature scaling is restored. Simple analytical expressions for QBrem in both limiting cases are provided.</p>
	]]></content:encoded>

	<dc:title>Neutrino-Pair Bremsstrahlung Due to Electromagnetic Collisions in Neutron Star Cores Revisited</dc:title>
			<dc:creator>Peter S. Shternin</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040100</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-11</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-11</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>100</prism:startingPage>
		<prism:doi>10.3390/particles8040100</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/100</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/99">

	<title>Particles, Vol. 8, Pages 99: Pattern Recognition with Artificial Intelligence in Space Experiments</title>
	<link>https://www.mdpi.com/2571-712X/8/4/99</link>
	<description>The application of advanced Artificial Intelligence (AI) techniques in astroparticle experiments represents a major advancement in both data analysis and experimental design. As space missions become increasingly complex, integrating AI tools is essential for optimizing system performance and maximizing scientific return. This study explores the use of Graph Neural Networks (GNNs) within the tracking systems of space-based experiments. A key challenge in track reconstruction is the high level of noise, primarily due to backscattering tracks, which can obscure the identification of primary particle trajectories. We propose a novel GNN-based approach for node-level classification tasks, specifically designed to distinguish primary tracks from backscattered ones within the tracker. In this framework, AI is employed as a powerful tool for pattern recognition, enabling the system to identify meaningful structures within complex tracking data and to discriminate signal from backscattering with higher precision. By addressing these challenges, our work aims to enhance the accuracy and reliability of data interpretation in astroparticle physics through the advanced deep learning techniques.</description>
	<pubDate>2025-12-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 99: Pattern Recognition with Artificial Intelligence in Space Experiments</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/99">doi: 10.3390/particles8040099</a></p>
	<p>Authors:
		Federica Cuna
		Maria Bossa
		Fabio Gargano
		Mario Nicola Mazziotta
		</p>
	<p>The application of advanced Artificial Intelligence (AI) techniques in astroparticle experiments represents a major advancement in both data analysis and experimental design. As space missions become increasingly complex, integrating AI tools is essential for optimizing system performance and maximizing scientific return. This study explores the use of Graph Neural Networks (GNNs) within the tracking systems of space-based experiments. A key challenge in track reconstruction is the high level of noise, primarily due to backscattering tracks, which can obscure the identification of primary particle trajectories. We propose a novel GNN-based approach for node-level classification tasks, specifically designed to distinguish primary tracks from backscattered ones within the tracker. In this framework, AI is employed as a powerful tool for pattern recognition, enabling the system to identify meaningful structures within complex tracking data and to discriminate signal from backscattering with higher precision. By addressing these challenges, our work aims to enhance the accuracy and reliability of data interpretation in astroparticle physics through the advanced deep learning techniques.</p>
	]]></content:encoded>

	<dc:title>Pattern Recognition with Artificial Intelligence in Space Experiments</dc:title>
			<dc:creator>Federica Cuna</dc:creator>
			<dc:creator>Maria Bossa</dc:creator>
			<dc:creator>Fabio Gargano</dc:creator>
			<dc:creator>Mario Nicola Mazziotta</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040099</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-10</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-10</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>99</prism:startingPage>
		<prism:doi>10.3390/particles8040099</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/99</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/98">

	<title>Particles, Vol. 8, Pages 98: Magnetic Field Amplification and Reconstruction in Rotating Astrophysical Plasmas: Verifying the Roles of &amp;alpha; and &amp;beta; in Dynamo Action</title>
	<link>https://www.mdpi.com/2571-712X/8/4/98</link>
	<description>We investigate the &amp;amp;alpha; and &amp;amp;beta; effects in a rotating spherical plasma system relevant to astrophysical contexts. In particular, we focus on how kinetic and magnetic (current) helicities influence the magnetic diffusivity &amp;amp;beta;. These coefficients were modeled using three complementary theoretical approaches. Direct numerical simulation (DNS) data (large-scale magnetic field B&amp;amp;macr;, turbulent velocity u, and turbulent magnetic field b) were then used to obtain the actual values of &amp;amp;alpha;EM&amp;amp;minus;HM, &amp;amp;beta;EM&amp;amp;minus;HM, &amp;amp;beta;vv&amp;amp;minus;vw, and &amp;amp;beta;bb+jb. Using these coefficients, we reconstructed B&amp;amp;macr; and compared it with the DNS results. In the kinematic regime, where B&amp;amp;macr; remains weak, all models agree well with DNS. In the nonlinear regime, however, the field reconstructed with &amp;amp;beta;vv&amp;amp;minus;vw alone deviates from DNS and grows without bound. Incorporating the turbulent magnetic diffusion term &amp;amp;beta;bb+jb suppresses this unphysical growth and restores consistency. Specifically, B&amp;amp;macr;DNS saturates at approximately 0.23 in the nonlinear regime. The reconstructed B&amp;amp;macr; using &amp;amp;beta;EM&amp;amp;minus;HM saturates at B&amp;amp;macr;&amp;amp;sim;0.3. When &amp;amp;beta;vv&amp;amp;minus;vw+bb+jb(=&amp;amp;beta;vv&amp;amp;minus;vw+&amp;amp;beta;bb+jb) is used, B&amp;amp;macr; varies from about 0.3 to 0.23. These results indicate that kinetic helicity reduces &amp;amp;beta; (or provides a negative contribution), thereby amplifying B&amp;amp;macr;, whereas turbulent current helicity, together with turbulent magnetic and kinetic energies, enhances &amp;amp;beta;, thus suppressing B&amp;amp;macr; in the nonlinear regime. In this respect, the new form of &amp;amp;beta; differs from the conventional one, which acts solely to diffuse the magnetic field.</description>
	<pubDate>2025-12-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 98: Magnetic Field Amplification and Reconstruction in Rotating Astrophysical Plasmas: Verifying the Roles of &amp;alpha; and &amp;beta; in Dynamo Action</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/98">doi: 10.3390/particles8040098</a></p>
	<p>Authors:
		Kiwan Park
		</p>
	<p>We investigate the &amp;amp;alpha; and &amp;amp;beta; effects in a rotating spherical plasma system relevant to astrophysical contexts. In particular, we focus on how kinetic and magnetic (current) helicities influence the magnetic diffusivity &amp;amp;beta;. These coefficients were modeled using three complementary theoretical approaches. Direct numerical simulation (DNS) data (large-scale magnetic field B&amp;amp;macr;, turbulent velocity u, and turbulent magnetic field b) were then used to obtain the actual values of &amp;amp;alpha;EM&amp;amp;minus;HM, &amp;amp;beta;EM&amp;amp;minus;HM, &amp;amp;beta;vv&amp;amp;minus;vw, and &amp;amp;beta;bb+jb. Using these coefficients, we reconstructed B&amp;amp;macr; and compared it with the DNS results. In the kinematic regime, where B&amp;amp;macr; remains weak, all models agree well with DNS. In the nonlinear regime, however, the field reconstructed with &amp;amp;beta;vv&amp;amp;minus;vw alone deviates from DNS and grows without bound. Incorporating the turbulent magnetic diffusion term &amp;amp;beta;bb+jb suppresses this unphysical growth and restores consistency. Specifically, B&amp;amp;macr;DNS saturates at approximately 0.23 in the nonlinear regime. The reconstructed B&amp;amp;macr; using &amp;amp;beta;EM&amp;amp;minus;HM saturates at B&amp;amp;macr;&amp;amp;sim;0.3. When &amp;amp;beta;vv&amp;amp;minus;vw+bb+jb(=&amp;amp;beta;vv&amp;amp;minus;vw+&amp;amp;beta;bb+jb) is used, B&amp;amp;macr; varies from about 0.3 to 0.23. These results indicate that kinetic helicity reduces &amp;amp;beta; (or provides a negative contribution), thereby amplifying B&amp;amp;macr;, whereas turbulent current helicity, together with turbulent magnetic and kinetic energies, enhances &amp;amp;beta;, thus suppressing B&amp;amp;macr; in the nonlinear regime. In this respect, the new form of &amp;amp;beta; differs from the conventional one, which acts solely to diffuse the magnetic field.</p>
	]]></content:encoded>

	<dc:title>Magnetic Field Amplification and Reconstruction in Rotating Astrophysical Plasmas: Verifying the Roles of &amp;amp;alpha; and &amp;amp;beta; in Dynamo Action</dc:title>
			<dc:creator>Kiwan Park</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040098</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-04</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>98</prism:startingPage>
		<prism:doi>10.3390/particles8040098</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/98</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/97">

	<title>Particles, Vol. 8, Pages 97: A Nanosatellite-Sized Detector for Sub-MeV Charged Cosmic Ray Fluxes in Low Earth Orbit: The Low-Energy Module (LEM) Onboard the NUSES Space Mission</title>
	<link>https://www.mdpi.com/2571-712X/8/4/97</link>
	<description>NUSES is a planned space mission aiming to test new observational and technological approaches related to the study of low-energy cosmic rays, gamma rays, and high-energy astrophysical neutrinos. Two scientific payloads will be hosted onboard the NUSES space mission: Terzina and Zir&amp;amp;egrave;. Terzina will be an optical telescope readout by SiPM arrays for the detection and study of Cerenkov light emitted by Extensive Air Showers (EASs) generated by high-energy cosmic rays and neutrinos in the atmosphere. Zir&amp;amp;egrave; will focus on the detection of protons and electrons up to a few hundred MeV and 0.1&amp;amp;ndash;30 MeV photons and will include the Low-Energy Module (LEM). The LEM will be a particle spectrometer devoted to the observation of fluxes of low-energy electrons in the 0.1&amp;amp;ndash;7-MeV range and protons in the 3&amp;amp;ndash;50 MeV range in low Earth orbit (LEO) followed by the hosting platform. The detection of Particle Bursts (PBs) in this physics channel of interest could provide insights into understanding complex phenomena such as possible correlations between seismic events or volcanic activity with the collective motion of particles in the plasma populating Van Allen belts. With its compact size and limited acceptance, the LEM will allow the exploration of hostile environments such as the South Atlantic Anomaly (SAA) and the inner Van Allen belt, in which the anticipated electron fluxes are on the order of 106 to 107 electrons per square centimeter per steradian per second. Concerning the vast literature on space-based particle spectrometers, the innovative aspect of the LEM resides in its compactness, within 10&amp;amp;times;10&amp;amp;times;10 cm3, and in its &amp;amp;ldquo;active collimation&amp;amp;rdquo; approach to dealing with the problem of multiple scattering at these low energies. In this work, the geometry of the detector, its detection concept, its operation modes, and the hardware adopted will be presented. Some preliminary results from a Monte Carlo simulation (Geant4) will be shown.</description>
	<pubDate>2025-12-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 97: A Nanosatellite-Sized Detector for Sub-MeV Charged Cosmic Ray Fluxes in Low Earth Orbit: The Low-Energy Module (LEM) Onboard the NUSES Space Mission</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/97">doi: 10.3390/particles8040097</a></p>
	<p>Authors:
		Riccardo Nicolaidis
		Andrea Abba
		Domenico Borrelli
		Adriano Di Giovanni
		Luigi Ferrentino
		Giovanni Franchi
		Francesco Nozzoli
		Giancarlo Pepponi
		Lorenzo Perillo
		David Schledewitz
		Enrico Verroi
		</p>
	<p>NUSES is a planned space mission aiming to test new observational and technological approaches related to the study of low-energy cosmic rays, gamma rays, and high-energy astrophysical neutrinos. Two scientific payloads will be hosted onboard the NUSES space mission: Terzina and Zir&amp;amp;egrave;. Terzina will be an optical telescope readout by SiPM arrays for the detection and study of Cerenkov light emitted by Extensive Air Showers (EASs) generated by high-energy cosmic rays and neutrinos in the atmosphere. Zir&amp;amp;egrave; will focus on the detection of protons and electrons up to a few hundred MeV and 0.1&amp;amp;ndash;30 MeV photons and will include the Low-Energy Module (LEM). The LEM will be a particle spectrometer devoted to the observation of fluxes of low-energy electrons in the 0.1&amp;amp;ndash;7-MeV range and protons in the 3&amp;amp;ndash;50 MeV range in low Earth orbit (LEO) followed by the hosting platform. The detection of Particle Bursts (PBs) in this physics channel of interest could provide insights into understanding complex phenomena such as possible correlations between seismic events or volcanic activity with the collective motion of particles in the plasma populating Van Allen belts. With its compact size and limited acceptance, the LEM will allow the exploration of hostile environments such as the South Atlantic Anomaly (SAA) and the inner Van Allen belt, in which the anticipated electron fluxes are on the order of 106 to 107 electrons per square centimeter per steradian per second. Concerning the vast literature on space-based particle spectrometers, the innovative aspect of the LEM resides in its compactness, within 10&amp;amp;times;10&amp;amp;times;10 cm3, and in its &amp;amp;ldquo;active collimation&amp;amp;rdquo; approach to dealing with the problem of multiple scattering at these low energies. In this work, the geometry of the detector, its detection concept, its operation modes, and the hardware adopted will be presented. Some preliminary results from a Monte Carlo simulation (Geant4) will be shown.</p>
	]]></content:encoded>

	<dc:title>A Nanosatellite-Sized Detector for Sub-MeV Charged Cosmic Ray Fluxes in Low Earth Orbit: The Low-Energy Module (LEM) Onboard the NUSES Space Mission</dc:title>
			<dc:creator>Riccardo Nicolaidis</dc:creator>
			<dc:creator>Andrea Abba</dc:creator>
			<dc:creator>Domenico Borrelli</dc:creator>
			<dc:creator>Adriano Di Giovanni</dc:creator>
			<dc:creator>Luigi Ferrentino</dc:creator>
			<dc:creator>Giovanni Franchi</dc:creator>
			<dc:creator>Francesco Nozzoli</dc:creator>
			<dc:creator>Giancarlo Pepponi</dc:creator>
			<dc:creator>Lorenzo Perillo</dc:creator>
			<dc:creator>David Schledewitz</dc:creator>
			<dc:creator>Enrico Verroi</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040097</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-04</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>97</prism:startingPage>
		<prism:doi>10.3390/particles8040097</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/97</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/96">

	<title>Particles, Vol. 8, Pages 96: Simulation of a SiPM-Based Cherenkov Camera</title>
	<link>https://www.mdpi.com/2571-712X/8/4/96</link>
	<description>Future space detectors for Ultra High Energy neutrinos and cosmic rays will utilize Cherenkov telescopes to detect forward-beamed Cherenkov light produced by charged particles in Extensive Air Showers (EASs). A Cherenkov detector can be equipped with an array of Silicon Photo-Multiplier (SiPM) pixels, which offer several advantages over traditional Photo-Multiplier Tubes (PMTs). SiPMs are compact and lightweight and operate at lower voltages, making them well-suited for space-based experiments. The SiSMUV (SiPM-based Space Monitor for UV-light) is developing a SiPM-based Cherenkov camera for PBR (POEMMA Baloon with Radio) at INFN Napoli. To understand the response of such an instrument, a comprehensive simulation of the response of individual SiPM pixels to incident light is needed. For the accurate simulation of a threshold trigger, this simulation must reproduce the current produced by a SiPM pixel as a function of time. Since a SiPM pixel is made of many individual Avalanche Photo-Diodes (APDs), saturation and pileup in APDs must also be simulated. A Gaussian mixture fit to ADC count spectrum of a SiPM pixel exposed to low levels of laser light at INFN Napoli shows a significant amount of samples between the expected PE (Photo Electron) peaks. Thus, noise sources such as dark counts and afterpulses, which result in partially integrated APD pulses, must be accounted for. With static, reasonable values for noise rates, the simulation chain presented in this work uses the characteristics of individual APDs to produce the aggregate current produced by a SiPM pixel. When many such pulses are simulated and integrated, the ADC spectra generated by low levels of laser light at the INFN Napoli SiSMUV test setup can be accurately reproduced.</description>
	<pubDate>2025-12-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 96: Simulation of a SiPM-Based Cherenkov Camera</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/96">doi: 10.3390/particles8040096</a></p>
	<p>Authors:
		Isaac Buckland
		Riccardo Munini
		Valentina Scotti
		</p>
	<p>Future space detectors for Ultra High Energy neutrinos and cosmic rays will utilize Cherenkov telescopes to detect forward-beamed Cherenkov light produced by charged particles in Extensive Air Showers (EASs). A Cherenkov detector can be equipped with an array of Silicon Photo-Multiplier (SiPM) pixels, which offer several advantages over traditional Photo-Multiplier Tubes (PMTs). SiPMs are compact and lightweight and operate at lower voltages, making them well-suited for space-based experiments. The SiSMUV (SiPM-based Space Monitor for UV-light) is developing a SiPM-based Cherenkov camera for PBR (POEMMA Baloon with Radio) at INFN Napoli. To understand the response of such an instrument, a comprehensive simulation of the response of individual SiPM pixels to incident light is needed. For the accurate simulation of a threshold trigger, this simulation must reproduce the current produced by a SiPM pixel as a function of time. Since a SiPM pixel is made of many individual Avalanche Photo-Diodes (APDs), saturation and pileup in APDs must also be simulated. A Gaussian mixture fit to ADC count spectrum of a SiPM pixel exposed to low levels of laser light at INFN Napoli shows a significant amount of samples between the expected PE (Photo Electron) peaks. Thus, noise sources such as dark counts and afterpulses, which result in partially integrated APD pulses, must be accounted for. With static, reasonable values for noise rates, the simulation chain presented in this work uses the characteristics of individual APDs to produce the aggregate current produced by a SiPM pixel. When many such pulses are simulated and integrated, the ADC spectra generated by low levels of laser light at the INFN Napoli SiSMUV test setup can be accurately reproduced.</p>
	]]></content:encoded>

	<dc:title>Simulation of a SiPM-Based Cherenkov Camera</dc:title>
			<dc:creator>Isaac Buckland</dc:creator>
			<dc:creator>Riccardo Munini</dc:creator>
			<dc:creator>Valentina Scotti</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040096</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-12-03</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-12-03</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>96</prism:startingPage>
		<prism:doi>10.3390/particles8040096</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/96</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/95">

	<title>Particles, Vol. 8, Pages 95: Discovering the Underlying Analytic Structure Within Standard Model Constants Using Artificial Intelligence</title>
	<link>https://www.mdpi.com/2571-712X/8/4/95</link>
	<description>This paper presents a method for uncovering hidden analytic relationships among the fundamental parameters of the Standard Model (SM), a foundational theory in physics that describes the fundamental particles and their interactions, using symbolic regression and genetic programming. Using this approach, we identify the simplest analytic relationships connecting pairs of these constants and report several notable expressions obtained with relative precision better than 1%. These results may serve as valuable inputs for model builders and artificial intelligence methods aimed at uncovering hidden patterns among the SM constants, or potentially used as building blocks for a deeper underlying law that connects all parameters of the SM through a small set of fundamental constants.</description>
	<pubDate>2025-11-29</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 95: Discovering the Underlying Analytic Structure Within Standard Model Constants Using Artificial Intelligence</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/95">doi: 10.3390/particles8040095</a></p>
	<p>Authors:
		Sergei V. Chekanov
		Håkan Kjellerstrand
		</p>
	<p>This paper presents a method for uncovering hidden analytic relationships among the fundamental parameters of the Standard Model (SM), a foundational theory in physics that describes the fundamental particles and their interactions, using symbolic regression and genetic programming. Using this approach, we identify the simplest analytic relationships connecting pairs of these constants and report several notable expressions obtained with relative precision better than 1%. These results may serve as valuable inputs for model builders and artificial intelligence methods aimed at uncovering hidden patterns among the SM constants, or potentially used as building blocks for a deeper underlying law that connects all parameters of the SM through a small set of fundamental constants.</p>
	]]></content:encoded>

	<dc:title>Discovering the Underlying Analytic Structure Within Standard Model Constants Using Artificial Intelligence</dc:title>
			<dc:creator>Sergei V. Chekanov</dc:creator>
			<dc:creator>Håkan Kjellerstrand</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040095</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-29</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-29</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>95</prism:startingPage>
		<prism:doi>10.3390/particles8040095</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/95</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/94">

	<title>Particles, Vol. 8, Pages 94: A SiPM-Based RICH Detector with Timing Capabilities for Isotope Identification</title>
	<link>https://www.mdpi.com/2571-712X/8/4/94</link>
	<description>In this work, we present a novel compact particle identification (PID) detector concept based on Silicon Photomultipliers (SiPMs) optimized to perform combined Ring-Imaging Cherenkov (RICH) and Time-of-Flight (TOF) measurements using a common photodetector layer. The system consists of a Cherenkov radiator layer separated from a photosensitive surface equipped with SiPMs by an expansion gap. A thin glass slab, acting as a second Cherenkov radiator, is coupled to the SiPMs to perform Cherenkov-based charged particle timing measurements. We assembled a small-scale prototype instrumented with various Hamamatsu SiPM array sensors with pixel pitches ranging from 2 to 3 mm and coupled with 1 mm thick fused silica window. The RICH radiator consisted of a 2 cm thick aerogel tile with a refractive index of 1.03 at 400 nm. The prototype was successfully tested in beam test campaigns at the CERN PS T10 beam line with pions and protons. We measured a single-hit angular resolution of about 4 mrad at the Cherenkov angle saturation value and a time resolution better than 50 ps RMS for charged particles with Z = 1. The present technology makes the proposed SiPM-based PID system particularly attractive for space applications due to the limited detector volumes available. In this work, we present beam test results obtained with the detector prototype and we discuss possible configurations optimized for the identification of ions in space applications.</description>
	<pubDate>2025-11-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 94: A SiPM-Based RICH Detector with Timing Capabilities for Isotope Identification</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/94">doi: 10.3390/particles8040094</a></p>
	<p>Authors:
		Mario Nicola Mazziotta
		Liliana Congedo
		Giuseppe De Robertis
		Mario Giliberti
		Francesco Licciulli
		Antonio Liguori
		Leonarda Lorusso
		Nicola Nicassio
		Giuliana Panzarini
		Roberta Pillera
		</p>
	<p>In this work, we present a novel compact particle identification (PID) detector concept based on Silicon Photomultipliers (SiPMs) optimized to perform combined Ring-Imaging Cherenkov (RICH) and Time-of-Flight (TOF) measurements using a common photodetector layer. The system consists of a Cherenkov radiator layer separated from a photosensitive surface equipped with SiPMs by an expansion gap. A thin glass slab, acting as a second Cherenkov radiator, is coupled to the SiPMs to perform Cherenkov-based charged particle timing measurements. We assembled a small-scale prototype instrumented with various Hamamatsu SiPM array sensors with pixel pitches ranging from 2 to 3 mm and coupled with 1 mm thick fused silica window. The RICH radiator consisted of a 2 cm thick aerogel tile with a refractive index of 1.03 at 400 nm. The prototype was successfully tested in beam test campaigns at the CERN PS T10 beam line with pions and protons. We measured a single-hit angular resolution of about 4 mrad at the Cherenkov angle saturation value and a time resolution better than 50 ps RMS for charged particles with Z = 1. The present technology makes the proposed SiPM-based PID system particularly attractive for space applications due to the limited detector volumes available. In this work, we present beam test results obtained with the detector prototype and we discuss possible configurations optimized for the identification of ions in space applications.</p>
	]]></content:encoded>

	<dc:title>A SiPM-Based RICH Detector with Timing Capabilities for Isotope Identification</dc:title>
			<dc:creator>Mario Nicola Mazziotta</dc:creator>
			<dc:creator>Liliana Congedo</dc:creator>
			<dc:creator>Giuseppe De Robertis</dc:creator>
			<dc:creator>Mario Giliberti</dc:creator>
			<dc:creator>Francesco Licciulli</dc:creator>
			<dc:creator>Antonio Liguori</dc:creator>
			<dc:creator>Leonarda Lorusso</dc:creator>
			<dc:creator>Nicola Nicassio</dc:creator>
			<dc:creator>Giuliana Panzarini</dc:creator>
			<dc:creator>Roberta Pillera</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040094</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-28</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-28</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>94</prism:startingPage>
		<prism:doi>10.3390/particles8040094</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/94</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/93">

	<title>Particles, Vol. 8, Pages 93: The Scintillating Fiber Tracker of the Zir&amp;eacute; Detector Onboard the NUSES Space Mission</title>
	<link>https://www.mdpi.com/2571-712X/8/4/93</link>
	<description>NUSES is a pathfinder satellite that will be deployed in a low Earth orbit, designed with new technologies for space-based detectors. Zir&amp;amp;eacute; is one of the payloads of NUSES and aims to measure the spectra of electrons, protons, and light nuclei in a kinetic energy range spanning from a few MeVs to several hundred MeVs, as well as photons in the energy range from 0.1 MeV to 30 MeV. Zir&amp;amp;eacute; consists of a Fiber TracKer (FTK), a Plastic Scintillator Tower (PST), a calorimeter (CALOg), an AntiCoincidence System (ACS) and a Low Energy Module (LEM). The FTK is based on thin scintillating fibers read out by Silicon Photomultiplier (SiPM) arrays. We assembled a prototype of Zir&amp;amp;eacute; (Zirettino) equipped with a single FTK layer, a reduced number of PST layers and a partially instrumented CALOg. A preliminary version of the Zir&amp;amp;eacute; custom Front-End Board (FEB) featuring the on-the-shelf ASIC CITIROC by OMEGA/Weeroc was used for the readout. We carried out several beam test campaigns at CERN&amp;amp;rsquo;s PS facility and a dynamic qualification test. The performance of FTK will be presented and discussed.</description>
	<pubDate>2025-11-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 93: The Scintillating Fiber Tracker of the Zir&amp;eacute; Detector Onboard the NUSES Space Mission</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/93">doi: 10.3390/particles8040093</a></p>
	<p>Authors:
		Felicia Carla Tiziana Barbato
		Ivan De Mitri
		Giuseppe De Robertis
		Adriano Di Giovanni
		Leonardo Di Venere
		Giulio Fontanella
		Fabio Gargano
		Mario Giliberti
		Francesco Licciulli
		Antonio Liguori
		Francesco Loparco
		Leonarda Lorusso
		Mario Nicola Mazziotta
		Giuliana Panzarini
		Roberta Pillera
		Pierpaolo Savina
		Aleksei Smirnov
		</p>
	<p>NUSES is a pathfinder satellite that will be deployed in a low Earth orbit, designed with new technologies for space-based detectors. Zir&amp;amp;eacute; is one of the payloads of NUSES and aims to measure the spectra of electrons, protons, and light nuclei in a kinetic energy range spanning from a few MeVs to several hundred MeVs, as well as photons in the energy range from 0.1 MeV to 30 MeV. Zir&amp;amp;eacute; consists of a Fiber TracKer (FTK), a Plastic Scintillator Tower (PST), a calorimeter (CALOg), an AntiCoincidence System (ACS) and a Low Energy Module (LEM). The FTK is based on thin scintillating fibers read out by Silicon Photomultiplier (SiPM) arrays. We assembled a prototype of Zir&amp;amp;eacute; (Zirettino) equipped with a single FTK layer, a reduced number of PST layers and a partially instrumented CALOg. A preliminary version of the Zir&amp;amp;eacute; custom Front-End Board (FEB) featuring the on-the-shelf ASIC CITIROC by OMEGA/Weeroc was used for the readout. We carried out several beam test campaigns at CERN&amp;amp;rsquo;s PS facility and a dynamic qualification test. The performance of FTK will be presented and discussed.</p>
	]]></content:encoded>

	<dc:title>The Scintillating Fiber Tracker of the Zir&amp;amp;eacute; Detector Onboard the NUSES Space Mission</dc:title>
			<dc:creator>Felicia Carla Tiziana Barbato</dc:creator>
			<dc:creator>Ivan De Mitri</dc:creator>
			<dc:creator>Giuseppe De Robertis</dc:creator>
			<dc:creator>Adriano Di Giovanni</dc:creator>
			<dc:creator>Leonardo Di Venere</dc:creator>
			<dc:creator>Giulio Fontanella</dc:creator>
			<dc:creator>Fabio Gargano</dc:creator>
			<dc:creator>Mario Giliberti</dc:creator>
			<dc:creator>Francesco Licciulli</dc:creator>
			<dc:creator>Antonio Liguori</dc:creator>
			<dc:creator>Francesco Loparco</dc:creator>
			<dc:creator>Leonarda Lorusso</dc:creator>
			<dc:creator>Mario Nicola Mazziotta</dc:creator>
			<dc:creator>Giuliana Panzarini</dc:creator>
			<dc:creator>Roberta Pillera</dc:creator>
			<dc:creator>Pierpaolo Savina</dc:creator>
			<dc:creator>Aleksei Smirnov</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040093</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-28</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-28</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>93</prism:startingPage>
		<prism:doi>10.3390/particles8040093</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/93</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/92">

	<title>Particles, Vol. 8, Pages 92: The SiSMUV Project: Development and Characterization of SiPM-Based UV-Light Detectors for Space Telescope Applications</title>
	<link>https://www.mdpi.com/2571-712X/8/4/92</link>
	<description>The study of Ultra-High-Energy Cosmic Rays is made possible by space telescopes that allow for the recording of signals generated by Extensive Air Showers (EAS) on the night side of the Earth&amp;amp;rsquo;s atmosphere. One of the requirements for these telescopes is the detection of very low photon fluxes, achievable using the latest generation SiPMs characterized by high intrinsic gains, low power consumption, low weight, and robustness against accidental exposure to light. Despite these advantages, some technological issues still need to be addressed, such as the radiation hardness for operation in space. Therefore, the design of a SiPM-based focal surface for UHECR detection must consider the space qualification of SiPM arrays, with the development of compact arrays optimized for low dead-area focal surfaces. SiSMUV (SiPM-based Space Monitor for UV light) is a project dedicated to developing a compact and modular UV detector for use in space telescopes designed to study the fluorescence and Cherenkov signals produced by Ultra-High-Energy Cosmic Rays (UHECRs). Each SiSMUV module incorporates a matrix of SiPMs, a readout ASIC (Radioroc by Weeroc), and an FPGA into a monolithic block. This design enables the acquisition and processing of signals from the sensors. The system can connect to a PC for standalone operation or with back-end electronics for integration into more complex systems. In this paper, we will describe the prototype electronics, the experimental setup and the measurements performed to obtain parameters such as the gain of the SiPMs, and their photon detection efficiency (PDE). We will also present the firmware developed to interface with the readout ASIC and to transmit data to other peripherals.</description>
	<pubDate>2025-11-27</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 92: The SiSMUV Project: Development and Characterization of SiPM-Based UV-Light Detectors for Space Telescope Applications</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/92">doi: 10.3390/particles8040092</a></p>
	<p>Authors:
		Valentina Scotti
		Giuseppe Osteria
		Marco Mese
		Antonio Anastasio
		Alfonso Boiano
		Isaac Buckland
		Vincenzo Masone
		Riccardo Munini
		Beatrice Panico
		Haroon Akhtar Qureshi
		</p>
	<p>The study of Ultra-High-Energy Cosmic Rays is made possible by space telescopes that allow for the recording of signals generated by Extensive Air Showers (EAS) on the night side of the Earth&amp;amp;rsquo;s atmosphere. One of the requirements for these telescopes is the detection of very low photon fluxes, achievable using the latest generation SiPMs characterized by high intrinsic gains, low power consumption, low weight, and robustness against accidental exposure to light. Despite these advantages, some technological issues still need to be addressed, such as the radiation hardness for operation in space. Therefore, the design of a SiPM-based focal surface for UHECR detection must consider the space qualification of SiPM arrays, with the development of compact arrays optimized for low dead-area focal surfaces. SiSMUV (SiPM-based Space Monitor for UV light) is a project dedicated to developing a compact and modular UV detector for use in space telescopes designed to study the fluorescence and Cherenkov signals produced by Ultra-High-Energy Cosmic Rays (UHECRs). Each SiSMUV module incorporates a matrix of SiPMs, a readout ASIC (Radioroc by Weeroc), and an FPGA into a monolithic block. This design enables the acquisition and processing of signals from the sensors. The system can connect to a PC for standalone operation or with back-end electronics for integration into more complex systems. In this paper, we will describe the prototype electronics, the experimental setup and the measurements performed to obtain parameters such as the gain of the SiPMs, and their photon detection efficiency (PDE). We will also present the firmware developed to interface with the readout ASIC and to transmit data to other peripherals.</p>
	]]></content:encoded>

	<dc:title>The SiSMUV Project: Development and Characterization of SiPM-Based UV-Light Detectors for Space Telescope Applications</dc:title>
			<dc:creator>Valentina Scotti</dc:creator>
			<dc:creator>Giuseppe Osteria</dc:creator>
			<dc:creator>Marco Mese</dc:creator>
			<dc:creator>Antonio Anastasio</dc:creator>
			<dc:creator>Alfonso Boiano</dc:creator>
			<dc:creator>Isaac Buckland</dc:creator>
			<dc:creator>Vincenzo Masone</dc:creator>
			<dc:creator>Riccardo Munini</dc:creator>
			<dc:creator>Beatrice Panico</dc:creator>
			<dc:creator>Haroon Akhtar Qureshi</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040092</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-27</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-27</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>92</prism:startingPage>
		<prism:doi>10.3390/particles8040092</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/92</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/91">

	<title>Particles, Vol. 8, Pages 91: Advanced Readout Logic for the XGIS Instrument: Discriminating X-Ray and Gamma-Ray Photons from the Background and Particles</title>
	<link>https://www.mdpi.com/2571-712X/8/4/91</link>
	<description>The X and Gamma Imager and Spectrometer (XGIS) on board THESEUS is a finely pixelized and modular instrument designed for broadband high-energy transient detection. XGIS consists of two cameras, each composed of 10 supermodules, with each supermodule further divided into 10 modules and each module made with 64 independent readout pixels based on Silicon Drift Detectors coupled with 5 &amp;amp;times; 5 &amp;amp;times; 30 mm3 CsI scintillator bars. An algorithm to quickly read out the signals from the 64 pixels and send them in chronological order through the module and supermodule logic up to the camera logic is under development. Furthermore, a challenge for space-based high-energy instruments is distinguishing X-/gamma-ray photons while effectively rejecting background photons and particles, including electrons, protons, and heavier cosmic rays. Unlike traditional systems that rely on anticoincidence systems, XGIS aims to achieve background rejection through an innovative readout logic that analyzes the spatial and temporal properties of energy deposits in the detector. By leveraging the finely pixelized structure, the readout system can differentiate single-photon events from charged-particle tracks based on energy deposition patterns and event topology.</description>
	<pubDate>2025-11-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 91: Advanced Readout Logic for the XGIS Instrument: Discriminating X-Ray and Gamma-Ray Photons from the Background and Particles</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/91">doi: 10.3390/particles8040091</a></p>
	<p>Authors:
		Paolo Calabretto
		Claudio Labanti
		Enrico Virgilli
		Lorenzo Amati
		Riccardo Campana
		Giulia Mattioli
		Smiriti Srivastava
		Ezequiel J. Marchesini
		Edoardo Borciani
		Ajay Sharma
		Giovanni La Rosa
		Paolo Nogara
		Giuseppe Sottile
		Alfonso Pisapia
		</p>
	<p>The X and Gamma Imager and Spectrometer (XGIS) on board THESEUS is a finely pixelized and modular instrument designed for broadband high-energy transient detection. XGIS consists of two cameras, each composed of 10 supermodules, with each supermodule further divided into 10 modules and each module made with 64 independent readout pixels based on Silicon Drift Detectors coupled with 5 &amp;amp;times; 5 &amp;amp;times; 30 mm3 CsI scintillator bars. An algorithm to quickly read out the signals from the 64 pixels and send them in chronological order through the module and supermodule logic up to the camera logic is under development. Furthermore, a challenge for space-based high-energy instruments is distinguishing X-/gamma-ray photons while effectively rejecting background photons and particles, including electrons, protons, and heavier cosmic rays. Unlike traditional systems that rely on anticoincidence systems, XGIS aims to achieve background rejection through an innovative readout logic that analyzes the spatial and temporal properties of energy deposits in the detector. By leveraging the finely pixelized structure, the readout system can differentiate single-photon events from charged-particle tracks based on energy deposition patterns and event topology.</p>
	]]></content:encoded>

	<dc:title>Advanced Readout Logic for the XGIS Instrument: Discriminating X-Ray and Gamma-Ray Photons from the Background and Particles</dc:title>
			<dc:creator>Paolo Calabretto</dc:creator>
			<dc:creator>Claudio Labanti</dc:creator>
			<dc:creator>Enrico Virgilli</dc:creator>
			<dc:creator>Lorenzo Amati</dc:creator>
			<dc:creator>Riccardo Campana</dc:creator>
			<dc:creator>Giulia Mattioli</dc:creator>
			<dc:creator>Smiriti Srivastava</dc:creator>
			<dc:creator>Ezequiel J. Marchesini</dc:creator>
			<dc:creator>Edoardo Borciani</dc:creator>
			<dc:creator>Ajay Sharma</dc:creator>
			<dc:creator>Giovanni La Rosa</dc:creator>
			<dc:creator>Paolo Nogara</dc:creator>
			<dc:creator>Giuseppe Sottile</dc:creator>
			<dc:creator>Alfonso Pisapia</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040091</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-22</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>91</prism:startingPage>
		<prism:doi>10.3390/particles8040091</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/91</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/90">

	<title>Particles, Vol. 8, Pages 90: The Cherenkov Camera for the PBR Mission</title>
	<link>https://www.mdpi.com/2571-712X/8/4/90</link>
	<description>POEMMA-Balloon with Radio (PBR) is designed as a payload for a NASA suborbital Super Pressure Balloon that will circle over the Southern Ocean and a mission duration as long as 50 days. The PBR instrument consists of a 1.1 m aperture Schmidt telescope similar to the POEMMA design with two cameras in its focal surface: a Fluorescence Camera (FC) and a Cherenkov Camera (CC). The CC camera is mainly devoted to the observation of cosmic-ray-induced high-altitude horizontal air showers (HAHAs) and search for neutrino-induced upward-going EAS. It will be made of 2048 SiPMs with a surface of 3 &amp;amp;times; 3 mm2 and a FoV of 12&amp;amp;deg; by 6&amp;amp;deg;, covering a spectral range of 320&amp;amp;ndash;900 nm. The CC camera is an innovative detector currently under construction. In this paper, information about its current status will be given.</description>
	<pubDate>2025-11-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 90: The Cherenkov Camera for the PBR Mission</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/90">doi: 10.3390/particles8040090</a></p>
	<p>Authors:
		Beatrice Panico
		Roberto Ammendola
		Antonio Anastasio
		Davide Badoni
		Mario Bertaina
		Francesco Cafagna
		Donatella Campana
		Marco Casolino
		Cristian De Santis
		Andrea Di Salvo
		Raffaele Gargiulo
		Alessandro Marcelli
		Laura Marcelli
		Vincenzo Masone
		Marco Mese
		Marco Mignone
		Giuseppe Osteria
		Giuseppe Passeggio
		Francesco Perfetto
		Haroon Akhtar Qureshi
		Enzo Reali
		Ester Ricci
		Valentina Scotti
		</p>
	<p>POEMMA-Balloon with Radio (PBR) is designed as a payload for a NASA suborbital Super Pressure Balloon that will circle over the Southern Ocean and a mission duration as long as 50 days. The PBR instrument consists of a 1.1 m aperture Schmidt telescope similar to the POEMMA design with two cameras in its focal surface: a Fluorescence Camera (FC) and a Cherenkov Camera (CC). The CC camera is mainly devoted to the observation of cosmic-ray-induced high-altitude horizontal air showers (HAHAs) and search for neutrino-induced upward-going EAS. It will be made of 2048 SiPMs with a surface of 3 &amp;amp;times; 3 mm2 and a FoV of 12&amp;amp;deg; by 6&amp;amp;deg;, covering a spectral range of 320&amp;amp;ndash;900 nm. The CC camera is an innovative detector currently under construction. In this paper, information about its current status will be given.</p>
	]]></content:encoded>

	<dc:title>The Cherenkov Camera for the PBR Mission</dc:title>
			<dc:creator>Beatrice Panico</dc:creator>
			<dc:creator>Roberto Ammendola</dc:creator>
			<dc:creator>Antonio Anastasio</dc:creator>
			<dc:creator>Davide Badoni</dc:creator>
			<dc:creator>Mario Bertaina</dc:creator>
			<dc:creator>Francesco Cafagna</dc:creator>
			<dc:creator>Donatella Campana</dc:creator>
			<dc:creator>Marco Casolino</dc:creator>
			<dc:creator>Cristian De Santis</dc:creator>
			<dc:creator>Andrea Di Salvo</dc:creator>
			<dc:creator>Raffaele Gargiulo</dc:creator>
			<dc:creator>Alessandro Marcelli</dc:creator>
			<dc:creator>Laura Marcelli</dc:creator>
			<dc:creator>Vincenzo Masone</dc:creator>
			<dc:creator>Marco Mese</dc:creator>
			<dc:creator>Marco Mignone</dc:creator>
			<dc:creator>Giuseppe Osteria</dc:creator>
			<dc:creator>Giuseppe Passeggio</dc:creator>
			<dc:creator>Francesco Perfetto</dc:creator>
			<dc:creator>Haroon Akhtar Qureshi</dc:creator>
			<dc:creator>Enzo Reali</dc:creator>
			<dc:creator>Ester Ricci</dc:creator>
			<dc:creator>Valentina Scotti</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040090</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-21</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-21</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>90</prism:startingPage>
		<prism:doi>10.3390/particles8040090</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/90</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/89">

	<title>Particles, Vol. 8, Pages 89: Design of the ANTARES4 Readout ASIC for the Second Flight of the GAPS Experiment: Motivations and Requirements</title>
	<link>https://www.mdpi.com/2571-712X/8/4/89</link>
	<description>The General AntiParticle Spectrometer is a balloon-borne experiment designed to search for low-energy cosmic-ray antinuclei as a potential indirect signature of dark matter. Over the course of at least three long-duration flights over Antarctica, it will explore the sub-250&amp;amp;nbsp;MeV/n energy range with sensitivity to antideuterons and antihelium, while also extending antiproton measurements below 100 MeV. The instrument features a tracker built from more than one thousand lithium-drifted silicon detectors, each read out by a dedicated custom integrated circuit. With the first flight scheduled for the austral summer of 2025, a new prototype chip, ANTARES4, has been developed using a commercial 65 nm complementary metal-oxide semiconductor process for use in the second flight. It integrates eight independent analog channels, each incorporating a low-noise charge-sensitive amplifier with dynamic signal compression, a CR&amp;amp;ndash;RC shaping stage with eight selectable peaking times, and on-chip calibration circuitry. The charge-sensitive amplifier uses metal-oxide semiconductor feedback elements with voltage-dependent capacitance to support the wide input energy range from 10 keV to 100 MeV. Four alternative feedback implementations are included to compare performance and design trade-offs. Leakage current compensation up to 200 nA per detector strip is provided by a Krummenacher current&amp;amp;ndash;feedback network. This paper presents the design and architecture of ANTARES4, highlighting the motivations, design drivers, and performance requirements that guided its development.</description>
	<pubDate>2025-11-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 89: Design of the ANTARES4 Readout ASIC for the Second Flight of the GAPS Experiment: Motivations and Requirements</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/89">doi: 10.3390/particles8040089</a></p>
	<p>Authors:
		Luca Ghislotti
		Paolo Lazzaroni
		Massimo Manghisoni
		Elisa Riceputi
		</p>
	<p>The General AntiParticle Spectrometer is a balloon-borne experiment designed to search for low-energy cosmic-ray antinuclei as a potential indirect signature of dark matter. Over the course of at least three long-duration flights over Antarctica, it will explore the sub-250&amp;amp;nbsp;MeV/n energy range with sensitivity to antideuterons and antihelium, while also extending antiproton measurements below 100 MeV. The instrument features a tracker built from more than one thousand lithium-drifted silicon detectors, each read out by a dedicated custom integrated circuit. With the first flight scheduled for the austral summer of 2025, a new prototype chip, ANTARES4, has been developed using a commercial 65 nm complementary metal-oxide semiconductor process for use in the second flight. It integrates eight independent analog channels, each incorporating a low-noise charge-sensitive amplifier with dynamic signal compression, a CR&amp;amp;ndash;RC shaping stage with eight selectable peaking times, and on-chip calibration circuitry. The charge-sensitive amplifier uses metal-oxide semiconductor feedback elements with voltage-dependent capacitance to support the wide input energy range from 10 keV to 100 MeV. Four alternative feedback implementations are included to compare performance and design trade-offs. Leakage current compensation up to 200 nA per detector strip is provided by a Krummenacher current&amp;amp;ndash;feedback network. This paper presents the design and architecture of ANTARES4, highlighting the motivations, design drivers, and performance requirements that guided its development.</p>
	]]></content:encoded>

	<dc:title>Design of the ANTARES4 Readout ASIC for the Second Flight of the GAPS Experiment: Motivations and Requirements</dc:title>
			<dc:creator>Luca Ghislotti</dc:creator>
			<dc:creator>Paolo Lazzaroni</dc:creator>
			<dc:creator>Massimo Manghisoni</dc:creator>
			<dc:creator>Elisa Riceputi</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040089</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-15</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-15</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>89</prism:startingPage>
		<prism:doi>10.3390/particles8040089</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/89</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/88">

	<title>Particles, Vol. 8, Pages 88: Study of the &amp;rho;0 Decay into &amp;pi;0&amp;pi;0&amp;gamma; Within Framework of Chiral Perturbation Theory with Resonances</title>
	<link>https://www.mdpi.com/2571-712X/8/4/88</link>
	<description>In this work, we calculate the Branching Ratio (BR) of the process &amp;amp;rho;0&amp;amp;rarr;&amp;amp;pi;0&amp;amp;pi;0&amp;amp;gamma; at tree level within the theoretical framework of with resonances, including the odd intrinsic parity sector. Owing to the nature of an effective field theory, the BR depends on three unknown couplings of the model: d4 and the combination c57=c5+c7. To constrain these unknown couplings, we use the experimental BR of this decay and explore the possibility of reducing the number of unknown couplings through the on-shell condition at one vertex. Our result suggests that off-shell conditions must be applied to both vertices, leading to a space parameter for the pair (c57,d4).</description>
	<pubDate>2025-11-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 88: Study of the &amp;rho;0 Decay into &amp;pi;0&amp;pi;0&amp;gamma; Within Framework of Chiral Perturbation Theory with Resonances</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/88">doi: 10.3390/particles8040088</a></p>
	<p>Authors:
		José A. Barajas-Aguilar
		Francisco V. Flores-Baez
		José R. Morones-Ibarra
		</p>
	<p>In this work, we calculate the Branching Ratio (BR) of the process &amp;amp;rho;0&amp;amp;rarr;&amp;amp;pi;0&amp;amp;pi;0&amp;amp;gamma; at tree level within the theoretical framework of with resonances, including the odd intrinsic parity sector. Owing to the nature of an effective field theory, the BR depends on three unknown couplings of the model: d4 and the combination c57=c5+c7. To constrain these unknown couplings, we use the experimental BR of this decay and explore the possibility of reducing the number of unknown couplings through the on-shell condition at one vertex. Our result suggests that off-shell conditions must be applied to both vertices, leading to a space parameter for the pair (c57,d4).</p>
	]]></content:encoded>

	<dc:title>Study of the &amp;amp;rho;0 Decay into &amp;amp;pi;0&amp;amp;pi;0&amp;amp;gamma; Within Framework of Chiral Perturbation Theory with Resonances</dc:title>
			<dc:creator>José A. Barajas-Aguilar</dc:creator>
			<dc:creator>Francisco V. Flores-Baez</dc:creator>
			<dc:creator>José R. Morones-Ibarra</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040088</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-11</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-11</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>88</prism:startingPage>
		<prism:doi>10.3390/particles8040088</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/88</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/87">

	<title>Particles, Vol. 8, Pages 87: Advanced Particle Classification in Space Calorimetry Using Transformer-Based and Gradient Boosting Models</title>
	<link>https://www.mdpi.com/2571-712X/8/4/87</link>
	<description>Artificial intelligence has made remarkable progress across numerous domains, including physics, where machine learning and deep learning methods have become increasingly common. In high-energy physics, these approaches have significantly advanced tasks like event reconstruction, pattern recognition, and large-scale data analysis. The present study explores the application of machine learning techniques to the classification of electromagnetic and hadronic showers in space calorimeter experiments. Leveraging Monte Carlo simulations and a dedicated feature engineering, the findings demonstrate the strong potential of AI to improve classification performance in space calorimetry.</description>
	<pubDate>2025-11-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 87: Advanced Particle Classification in Space Calorimetry Using Transformer-Based and Gradient Boosting Models</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/87">doi: 10.3390/particles8040087</a></p>
	<p>Authors:
		Maria Bossa
		Federica Cuna
		Fabio Gargano
		</p>
	<p>Artificial intelligence has made remarkable progress across numerous domains, including physics, where machine learning and deep learning methods have become increasingly common. In high-energy physics, these approaches have significantly advanced tasks like event reconstruction, pattern recognition, and large-scale data analysis. The present study explores the application of machine learning techniques to the classification of electromagnetic and hadronic showers in space calorimeter experiments. Leveraging Monte Carlo simulations and a dedicated feature engineering, the findings demonstrate the strong potential of AI to improve classification performance in space calorimetry.</p>
	]]></content:encoded>

	<dc:title>Advanced Particle Classification in Space Calorimetry Using Transformer-Based and Gradient Boosting Models</dc:title>
			<dc:creator>Maria Bossa</dc:creator>
			<dc:creator>Federica Cuna</dc:creator>
			<dc:creator>Fabio Gargano</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040087</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-11-05</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-11-05</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>87</prism:startingPage>
		<prism:doi>10.3390/particles8040087</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/87</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/86">

	<title>Particles, Vol. 8, Pages 86: A Cosmic Radiation Modular Telescope on the Moon: The MoonRay Concept</title>
	<link>https://www.mdpi.com/2571-712X/8/4/86</link>
	<description>The MoonRay project is carrying out a concept study of a permanent lunar cosmic-ray (CR) and gamma-ray observatory, in view of the implementation of habitats on our satellite. The idea is to build a modular telescope that will be able to overcome the limitations, in available power and weight, of the present generation of CR instruments in Low Earth Orbit, while carrying out high-energy gamma-ray observations from a vantage point at the South Pole of the Moon. An array of fully independent modules (towers), with limited individual size and mass, can provide an acceptance more than one order of magnitude larger than instruments in flight at present. The modular telescope is designed to be deployed progressively, during a series of lunar missions, while collecting meaningful scientific data at the intermediate stages of its implementation. The operational power will be made available by the facilities maintaining the lunar habitats. With a geometric factor close to 15 m2sr and about 8 times larger sensitive area than FERMI-LAT, MoonRay will be able to carry out a very rich observational program over a time span of a few decades with an energy reach of 10 PeV allowing the exploration of the CR &amp;amp;ldquo;knee&amp;amp;rdquo; and the observation of the Southern Sky with gamma rays well into the TeV scale. Each tower (of approximate size 20 cm &amp;amp;times; 20 cm &amp;amp;times;100 cm) is equipped with three instruments. A combined Charge and Time-of-Flight detector (CD-ToF) can identify individual cosmic elements, leveraging on an innovative two-layered array of pixelated Low-Gain Avalanche Diode (LGAD) sensors, with sub-ns time resolution. The latter can achieve an unprecedented rejection power against backscattered radiation from the calorimeter. It is followed by a tracker, providing also photon conversion, and by a thick crystal calorimeter (55 radiation lengths, 3 proton interaction lengths at normal incidence) with an energy resolution of 30&amp;amp;ndash;40% (1&amp;amp;ndash;2%) for protons (electrons) and a proton/electron rejection in excess of 105. A time resolution close to 100 ps has been obtained, with prototypal arrays of 3 mm &amp;amp;times; 3 mm LGAD pixels, in a recent test campaign carried out at CERN with Pb beam fragments.</description>
	<pubDate>2025-10-27</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 86: A Cosmic Radiation Modular Telescope on the Moon: The MoonRay Concept</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/86">doi: 10.3390/particles8040086</a></p>
	<p>Authors:
		Pier Simone Marrocchesi
		</p>
	<p>The MoonRay project is carrying out a concept study of a permanent lunar cosmic-ray (CR) and gamma-ray observatory, in view of the implementation of habitats on our satellite. The idea is to build a modular telescope that will be able to overcome the limitations, in available power and weight, of the present generation of CR instruments in Low Earth Orbit, while carrying out high-energy gamma-ray observations from a vantage point at the South Pole of the Moon. An array of fully independent modules (towers), with limited individual size and mass, can provide an acceptance more than one order of magnitude larger than instruments in flight at present. The modular telescope is designed to be deployed progressively, during a series of lunar missions, while collecting meaningful scientific data at the intermediate stages of its implementation. The operational power will be made available by the facilities maintaining the lunar habitats. With a geometric factor close to 15 m2sr and about 8 times larger sensitive area than FERMI-LAT, MoonRay will be able to carry out a very rich observational program over a time span of a few decades with an energy reach of 10 PeV allowing the exploration of the CR &amp;amp;ldquo;knee&amp;amp;rdquo; and the observation of the Southern Sky with gamma rays well into the TeV scale. Each tower (of approximate size 20 cm &amp;amp;times; 20 cm &amp;amp;times;100 cm) is equipped with three instruments. A combined Charge and Time-of-Flight detector (CD-ToF) can identify individual cosmic elements, leveraging on an innovative two-layered array of pixelated Low-Gain Avalanche Diode (LGAD) sensors, with sub-ns time resolution. The latter can achieve an unprecedented rejection power against backscattered radiation from the calorimeter. It is followed by a tracker, providing also photon conversion, and by a thick crystal calorimeter (55 radiation lengths, 3 proton interaction lengths at normal incidence) with an energy resolution of 30&amp;amp;ndash;40% (1&amp;amp;ndash;2%) for protons (electrons) and a proton/electron rejection in excess of 105. A time resolution close to 100 ps has been obtained, with prototypal arrays of 3 mm &amp;amp;times; 3 mm LGAD pixels, in a recent test campaign carried out at CERN with Pb beam fragments.</p>
	]]></content:encoded>

	<dc:title>A Cosmic Radiation Modular Telescope on the Moon: The MoonRay Concept</dc:title>
			<dc:creator>Pier Simone Marrocchesi</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040086</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-10-27</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-10-27</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>86</prism:startingPage>
		<prism:doi>10.3390/particles8040086</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/86</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/85">

	<title>Particles, Vol. 8, Pages 85: The Kaon Off-Shell Generalized Parton Distributions and Transverse Momentum Dependent Parton Distributions</title>
	<link>https://www.mdpi.com/2571-712X/8/4/85</link>
	<description>We investigate the off-shell generalized parton distributions (GPDs) and transverse momentum dependent parton distributions (TMDs) of kaons within the framework of the Nambu&amp;amp;ndash;Jona-Lasinio model, employing proper time regularization. Compared to the pion case, the off-shell effects in kaons are of similar magnitude, modifying the GPDs by about 10&amp;amp;ndash;25%, which is notable. The absence of crossing symmetry leads to odd powers in the x-moments of the off-shell GPDs, giving rise to new off-shell form factors. We analyze the relations among these kaon off-shell form factors by analogy with electromagnetic form factors. Our results extend the off-shell GPDs from pions to kaons and simultaneously address the associated off-shell form factors. We also compare the off-shell and on-shell gravitational form factors of the kaon. In addition, the off-shell kaon TMD shows a stronger dependence on the momentum fraction x than its on-shell counterpart.</description>
	<pubDate>2025-10-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 85: The Kaon Off-Shell Generalized Parton Distributions and Transverse Momentum Dependent Parton Distributions</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/85">doi: 10.3390/particles8040085</a></p>
	<p>Authors:
		Jin-Li Zhang
		</p>
	<p>We investigate the off-shell generalized parton distributions (GPDs) and transverse momentum dependent parton distributions (TMDs) of kaons within the framework of the Nambu&amp;amp;ndash;Jona-Lasinio model, employing proper time regularization. Compared to the pion case, the off-shell effects in kaons are of similar magnitude, modifying the GPDs by about 10&amp;amp;ndash;25%, which is notable. The absence of crossing symmetry leads to odd powers in the x-moments of the off-shell GPDs, giving rise to new off-shell form factors. We analyze the relations among these kaon off-shell form factors by analogy with electromagnetic form factors. Our results extend the off-shell GPDs from pions to kaons and simultaneously address the associated off-shell form factors. We also compare the off-shell and on-shell gravitational form factors of the kaon. In addition, the off-shell kaon TMD shows a stronger dependence on the momentum fraction x than its on-shell counterpart.</p>
	]]></content:encoded>

	<dc:title>The Kaon Off-Shell Generalized Parton Distributions and Transverse Momentum Dependent Parton Distributions</dc:title>
			<dc:creator>Jin-Li Zhang</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040085</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-10-25</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-10-25</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>85</prism:startingPage>
		<prism:doi>10.3390/particles8040085</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/85</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/84">

	<title>Particles, Vol. 8, Pages 84: Pre-Supernova (Anti)Neutrino Emission Due to Weak-Interaction Reactions with Hot Nuclei</title>
	<link>https://www.mdpi.com/2571-712X/8/4/84</link>
	<description>Reliable predictions of (anti)neutrino spectra and luminosities are essential for assessing the feasibility of detecting pre-supernova neutrinos. Using the stellar evolution code MESA, we calculate the (anti)neutrino spectra and luminosities under realistic conditions of temperature, density, and electron fraction. Our study includes (anti)neutrinos produced by both thermal processes and nuclear weak-interaction reactions. By comparing the results of the thermal quasiparticle random-phase approximation with the standard technique based on the effective Q-value method, we investigate how thermal effects influence the spectra and luminosities of emitted (anti)neutrinos. Our findings show that a thermodynamically consistent treatment of Gamow&amp;amp;ndash;Teller transitions in hot nuclei enhances both the energy luminosity and the average energies of the emitted (anti)neutrinos.</description>
	<pubDate>2025-10-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 84: Pre-Supernova (Anti)Neutrino Emission Due to Weak-Interaction Reactions with Hot Nuclei</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/84">doi: 10.3390/particles8040084</a></p>
	<p>Authors:
		Alan A. Dzhioev
		Andrey V. Yudin
		Natalia V. Dunina-Barkovskaya
		Andrey I. Vdovin
		</p>
	<p>Reliable predictions of (anti)neutrino spectra and luminosities are essential for assessing the feasibility of detecting pre-supernova neutrinos. Using the stellar evolution code MESA, we calculate the (anti)neutrino spectra and luminosities under realistic conditions of temperature, density, and electron fraction. Our study includes (anti)neutrinos produced by both thermal processes and nuclear weak-interaction reactions. By comparing the results of the thermal quasiparticle random-phase approximation with the standard technique based on the effective Q-value method, we investigate how thermal effects influence the spectra and luminosities of emitted (anti)neutrinos. Our findings show that a thermodynamically consistent treatment of Gamow&amp;amp;ndash;Teller transitions in hot nuclei enhances both the energy luminosity and the average energies of the emitted (anti)neutrinos.</p>
	]]></content:encoded>

	<dc:title>Pre-Supernova (Anti)Neutrino Emission Due to Weak-Interaction Reactions with Hot Nuclei</dc:title>
			<dc:creator>Alan A. Dzhioev</dc:creator>
			<dc:creator>Andrey V. Yudin</dc:creator>
			<dc:creator>Natalia V. Dunina-Barkovskaya</dc:creator>
			<dc:creator>Andrey I. Vdovin</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040084</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-10-12</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-10-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>84</prism:startingPage>
		<prism:doi>10.3390/particles8040084</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/84</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/83">

	<title>Particles, Vol. 8, Pages 83: Diquark Study in Quark Model</title>
	<link>https://www.mdpi.com/2571-712X/8/4/83</link>
	<description>To investigate diquark correlation in baryons, the baryon spectra with different light&amp;amp;ndash;heavy quark combinations are calculated using Gaussian expansion method within both the naive quark model and the chiral quark model. By computing the diquark energies and separations between any two quarks in baryons, we analyze the diquark effect in the ud-q/Q, us-Q, ss-q/Q, and QQ-q/Q systems (where q=u,d, or s; Q=c,b). The results show that diquark correlations exist in baryons. In particular, for qq-Q and QQ-q systems, the same type of diquark exhibits nearly identical energy and size across different baryons. In the orbital ground states of baryons, scalar&amp;amp;ndash;isoscalar diquarks have lower energy and a smaller size compared to vector&amp;amp;ndash;isovector diquark, which qualifies them as &amp;amp;ldquo;good diquarks&amp;amp;rdquo;. In QQ-q systems, a larger mass of Q leads to a smaller diquark separation and a more pronounced diquark effect. In qq-Q systems, the separation between the two light quarks remains larger than that between a light and a heavy quark, indicating that the internal structure of such diquarks must be taken into account. A comparison between the naive quark model and the chiral quark model reveals that the introduction of meson exchange slightly increases the diquark size in most systems.</description>
	<pubDate>2025-10-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 83: Diquark Study in Quark Model</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/83">doi: 10.3390/particles8040083</a></p>
	<p>Authors:
		Xinmei Zhu
		Hongxia Huang
		Jialun Ping
		</p>
	<p>To investigate diquark correlation in baryons, the baryon spectra with different light&amp;amp;ndash;heavy quark combinations are calculated using Gaussian expansion method within both the naive quark model and the chiral quark model. By computing the diquark energies and separations between any two quarks in baryons, we analyze the diquark effect in the ud-q/Q, us-Q, ss-q/Q, and QQ-q/Q systems (where q=u,d, or s; Q=c,b). The results show that diquark correlations exist in baryons. In particular, for qq-Q and QQ-q systems, the same type of diquark exhibits nearly identical energy and size across different baryons. In the orbital ground states of baryons, scalar&amp;amp;ndash;isoscalar diquarks have lower energy and a smaller size compared to vector&amp;amp;ndash;isovector diquark, which qualifies them as &amp;amp;ldquo;good diquarks&amp;amp;rdquo;. In QQ-q systems, a larger mass of Q leads to a smaller diquark separation and a more pronounced diquark effect. In qq-Q systems, the separation between the two light quarks remains larger than that between a light and a heavy quark, indicating that the internal structure of such diquarks must be taken into account. A comparison between the naive quark model and the chiral quark model reveals that the introduction of meson exchange slightly increases the diquark size in most systems.</p>
	]]></content:encoded>

	<dc:title>Diquark Study in Quark Model</dc:title>
			<dc:creator>Xinmei Zhu</dc:creator>
			<dc:creator>Hongxia Huang</dc:creator>
			<dc:creator>Jialun Ping</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040083</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-10-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-10-02</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>83</prism:startingPage>
		<prism:doi>10.3390/particles8040083</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/83</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/4/82">

	<title>Particles, Vol. 8, Pages 82: A New Measurement of Light Yield Quenching in EJ-200 and LYSO Scintillators</title>
	<link>https://www.mdpi.com/2571-712X/8/4/82</link>
	<description>Lutetium&amp;amp;ndash;Yttrium Oxyorthosilicate (LYSO) crystals and EJ-200 plastic scintillators are widely recognized fast scintillating materials, valued for their high light yield and mechanical robustness, which make them well suited for demanding applications in high-energy physics and space research. Their non-proportional light response, along with their non-linear behavior at low-energy X-rays, has been extensively investigated in previous studies, revealing potential systematic effects in existing measurements. In this work, light quenching in both scintillators is measured under charged-particle excitation. The results are interpreted using the modified Birks&amp;amp;ndash;Onsager model, which provides a theoretical framework for understanding the underlying quenching mechanisms, as well as a generalized logistic parametrization, offering experimentalists a useful tool to characterize the detector&amp;amp;rsquo;s light yield and associated uncertainties.</description>
	<pubDate>2025-09-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 82: A New Measurement of Light Yield Quenching in EJ-200 and LYSO Scintillators</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/4/82">doi: 10.3390/particles8040082</a></p>
	<p>Authors:
		Francesco Dimiccoli
		Francesco Maria Follega
		Luigi Ernesto Ghezzer
		Roberto Iuppa
		Alessandro Lega
		Riccardo Nicolaidis
		Francesco Nozzoli
		Ester Ricci
		Enrico Verroi
		Paolo Zuccon
		</p>
	<p>Lutetium&amp;amp;ndash;Yttrium Oxyorthosilicate (LYSO) crystals and EJ-200 plastic scintillators are widely recognized fast scintillating materials, valued for their high light yield and mechanical robustness, which make them well suited for demanding applications in high-energy physics and space research. Their non-proportional light response, along with their non-linear behavior at low-energy X-rays, has been extensively investigated in previous studies, revealing potential systematic effects in existing measurements. In this work, light quenching in both scintillators is measured under charged-particle excitation. The results are interpreted using the modified Birks&amp;amp;ndash;Onsager model, which provides a theoretical framework for understanding the underlying quenching mechanisms, as well as a generalized logistic parametrization, offering experimentalists a useful tool to characterize the detector&amp;amp;rsquo;s light yield and associated uncertainties.</p>
	]]></content:encoded>

	<dc:title>A New Measurement of Light Yield Quenching in EJ-200 and LYSO Scintillators</dc:title>
			<dc:creator>Francesco Dimiccoli</dc:creator>
			<dc:creator>Francesco Maria Follega</dc:creator>
			<dc:creator>Luigi Ernesto Ghezzer</dc:creator>
			<dc:creator>Roberto Iuppa</dc:creator>
			<dc:creator>Alessandro Lega</dc:creator>
			<dc:creator>Riccardo Nicolaidis</dc:creator>
			<dc:creator>Francesco Nozzoli</dc:creator>
			<dc:creator>Ester Ricci</dc:creator>
			<dc:creator>Enrico Verroi</dc:creator>
			<dc:creator>Paolo Zuccon</dc:creator>
		<dc:identifier>doi: 10.3390/particles8040082</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-09-30</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-09-30</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>82</prism:startingPage>
		<prism:doi>10.3390/particles8040082</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/4/82</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/81">

	<title>Particles, Vol. 8, Pages 81: Development of Array-Type Secondary Electron Emission Monitor Toward Single-Shot Measurement of Extraction Efficiency of FEL Oscillators</title>
	<link>https://www.mdpi.com/2571-712X/8/3/81</link>
	<description>To enable the single-shot measurement of extraction efficiency, a key parameter of an FEL oscillator, we developed an array-type secondary electron emission monitor capable of measuring the temporal evolution of the electron beam energy distribution in a macro-pulse at KU-FEL. The monitor consists of 24 ribbon-shaped electrodes and 2 shielding electrodes, and it is positioned after the energy analyzer magnet and just before a beam dump. The beam energy evolutions in a macro-pulse with and without FEL lasing were measured in a single shot with approximately 100 ns temporal resolution. From the results obtained, the extraction efficiency of FEL oscillators can be evaluated.</description>
	<pubDate>2025-09-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 81: Development of Array-Type Secondary Electron Emission Monitor Toward Single-Shot Measurement of Extraction Efficiency of FEL Oscillators</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/81">doi: 10.3390/particles8030081</a></p>
	<p>Authors:
		Zhuang Bi
		Kotaro Tanaka
		Heishun Zen
		Hideaki Ohgaki
		</p>
	<p>To enable the single-shot measurement of extraction efficiency, a key parameter of an FEL oscillator, we developed an array-type secondary electron emission monitor capable of measuring the temporal evolution of the electron beam energy distribution in a macro-pulse at KU-FEL. The monitor consists of 24 ribbon-shaped electrodes and 2 shielding electrodes, and it is positioned after the energy analyzer magnet and just before a beam dump. The beam energy evolutions in a macro-pulse with and without FEL lasing were measured in a single shot with approximately 100 ns temporal resolution. From the results obtained, the extraction efficiency of FEL oscillators can be evaluated.</p>
	]]></content:encoded>

	<dc:title>Development of Array-Type Secondary Electron Emission Monitor Toward Single-Shot Measurement of Extraction Efficiency of FEL Oscillators</dc:title>
			<dc:creator>Zhuang Bi</dc:creator>
			<dc:creator>Kotaro Tanaka</dc:creator>
			<dc:creator>Heishun Zen</dc:creator>
			<dc:creator>Hideaki Ohgaki</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030081</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-09-19</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-09-19</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>81</prism:startingPage>
		<prism:doi>10.3390/particles8030081</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/81</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/80">

	<title>Particles, Vol. 8, Pages 80: Crosstalk Simulation of Magnets for Siam Photon Source II Storage Ring</title>
	<link>https://www.mdpi.com/2571-712X/8/3/80</link>
	<description>During the detailed design of magnets for the storage ring of Siam Photon Source II (SPS-II), the influence of magnetic crosstalk between adjacent magnets in the compact Double Triple Bend Achromat (DTBA) lattice was investigated. Using Opera-3D magnetostatic simulation, six magnet pairs were analyzed to investigate the changes in magnetic field distribution along the electron trajectory and integrated magnetic field within each magnet aperture. The study employed polynomial and Fourier analyses to calculate multipole field components. Results indicate that magnetic crosstalk affects the field distribution in the region between magnets, particularly for the defocusing quadrupole and dipole magnets (QD2-D01) and the focusing quadrupole and octupole magnets (QF42-OF1) pairs, which have the pole-to-pole distances of 153.37 mm and 116.45 mm, respectively. Although these separations exceed the estimated fringe field regions, deviations of up to 1% in the main field components were observed. Notably, even an unpowered neighboring magnet contributes to magnetic field distortion due to the modified magnetic flux distribution. Crosstalk effects on the higher-order multipole fields are mostly within the acceptable limit, except for the extra quadrupole field from QD2 found in the dipole D01 magnet. This study highlights the effects of magnetic interference in tightly packed lattice and underscores the need to include a complete multipole field data with crosstalk consideration in the SPS-II lattice model in order to ensure an accurate beam dynamics simulation and predict the operating current adjustments for machine commissioning.</description>
	<pubDate>2025-09-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 80: Crosstalk Simulation of Magnets for Siam Photon Source II Storage Ring</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/80">doi: 10.3390/particles8030080</a></p>
	<p>Authors:
		Warissara Tangyotkhajorn
		Thongchai Leetha
		Supachai Prawanta
		Prapaiwan Sunwong
		</p>
	<p>During the detailed design of magnets for the storage ring of Siam Photon Source II (SPS-II), the influence of magnetic crosstalk between adjacent magnets in the compact Double Triple Bend Achromat (DTBA) lattice was investigated. Using Opera-3D magnetostatic simulation, six magnet pairs were analyzed to investigate the changes in magnetic field distribution along the electron trajectory and integrated magnetic field within each magnet aperture. The study employed polynomial and Fourier analyses to calculate multipole field components. Results indicate that magnetic crosstalk affects the field distribution in the region between magnets, particularly for the defocusing quadrupole and dipole magnets (QD2-D01) and the focusing quadrupole and octupole magnets (QF42-OF1) pairs, which have the pole-to-pole distances of 153.37 mm and 116.45 mm, respectively. Although these separations exceed the estimated fringe field regions, deviations of up to 1% in the main field components were observed. Notably, even an unpowered neighboring magnet contributes to magnetic field distortion due to the modified magnetic flux distribution. Crosstalk effects on the higher-order multipole fields are mostly within the acceptable limit, except for the extra quadrupole field from QD2 found in the dipole D01 magnet. This study highlights the effects of magnetic interference in tightly packed lattice and underscores the need to include a complete multipole field data with crosstalk consideration in the SPS-II lattice model in order to ensure an accurate beam dynamics simulation and predict the operating current adjustments for machine commissioning.</p>
	]]></content:encoded>

	<dc:title>Crosstalk Simulation of Magnets for Siam Photon Source II Storage Ring</dc:title>
			<dc:creator>Warissara Tangyotkhajorn</dc:creator>
			<dc:creator>Thongchai Leetha</dc:creator>
			<dc:creator>Supachai Prawanta</dc:creator>
			<dc:creator>Prapaiwan Sunwong</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030080</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-09-13</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-09-13</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>80</prism:startingPage>
		<prism:doi>10.3390/particles8030080</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/80</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/79">

	<title>Particles, Vol. 8, Pages 79: High-Efficiency WLS Plastic for a Compact Cherenkov Detector</title>
	<link>https://www.mdpi.com/2571-712X/8/3/79</link>
	<description>The Cherenkov effect, whereby a charged particle emits light when traveling faster than the phase velocity of light in a dielectric medium, is widely employed in particle identification techniques. However, Cherenkov light yield is relatively low, typically amounting to only 100&amp;amp;ndash;200 visible photons per centimeter of path length in materials like water, plastic, or glass. In this study, we investigate the optical response of FB118, a wavelength-shifting (WLS) plastic developed by Glass to Power, under exposure to ionizing particles. Our measurements confirm the absence of residual scintillation in FB118, allowing for a clean separation of Cherenkov signals. Moreover, the intrinsic WLS properties of the material enable a significant enhancement of light detection in the visible range. These features make FB118 a promising candidate for use in compact Cherenkov detectors, particularly in astroparticle physics experiments where space and power constraints demand efficient, compact solutions.</description>
	<pubDate>2025-09-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 79: High-Efficiency WLS Plastic for a Compact Cherenkov Detector</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/79">doi: 10.3390/particles8030079</a></p>
	<p>Authors:
		Francesco Nozzoli
		Luigi Ernesto Ghezzer
		Francesco Bruni
		Daniele Corti
		Francesco Meinardi
		Riccardo Nicolaidis
		Leonardo Ricci
		Piero Spinnato
		Enrico Verroi
		Paolo Zuccon
		</p>
	<p>The Cherenkov effect, whereby a charged particle emits light when traveling faster than the phase velocity of light in a dielectric medium, is widely employed in particle identification techniques. However, Cherenkov light yield is relatively low, typically amounting to only 100&amp;amp;ndash;200 visible photons per centimeter of path length in materials like water, plastic, or glass. In this study, we investigate the optical response of FB118, a wavelength-shifting (WLS) plastic developed by Glass to Power, under exposure to ionizing particles. Our measurements confirm the absence of residual scintillation in FB118, allowing for a clean separation of Cherenkov signals. Moreover, the intrinsic WLS properties of the material enable a significant enhancement of light detection in the visible range. These features make FB118 a promising candidate for use in compact Cherenkov detectors, particularly in astroparticle physics experiments where space and power constraints demand efficient, compact solutions.</p>
	]]></content:encoded>

	<dc:title>High-Efficiency WLS Plastic for a Compact Cherenkov Detector</dc:title>
			<dc:creator>Francesco Nozzoli</dc:creator>
			<dc:creator>Luigi Ernesto Ghezzer</dc:creator>
			<dc:creator>Francesco Bruni</dc:creator>
			<dc:creator>Daniele Corti</dc:creator>
			<dc:creator>Francesco Meinardi</dc:creator>
			<dc:creator>Riccardo Nicolaidis</dc:creator>
			<dc:creator>Leonardo Ricci</dc:creator>
			<dc:creator>Piero Spinnato</dc:creator>
			<dc:creator>Enrico Verroi</dc:creator>
			<dc:creator>Paolo Zuccon</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030079</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-09-12</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-09-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>79</prism:startingPage>
		<prism:doi>10.3390/particles8030079</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/79</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/78">

	<title>Particles, Vol. 8, Pages 78: Design and Optimization of a Broadband Stripline Kicker for Low Beam Emittance Ring Accelerators</title>
	<link>https://www.mdpi.com/2571-712X/8/3/78</link>
	<description>The performance and beam quality of the new fourth-generation synchrotron light source with ultra-low emittance are highly susceptible to coupled-bunch instabilities. These instabilities arise from the interaction between the bunched electron beam and the surrounding vacuum chamber installations. To mitigate these effects, the installation of a transverse bunch-by-bunch feedback system is planned. This system will comprise a button-type beam position monitor (BPM) for beam signal detection, a digital feedback controller, a broadband power amplifier, and a broadband stripline kicker as the primary actuator. One of the critical challenges lies in the development of the stripline kicker, which must be optimized for high shunt impedance and wide bandwidth while minimizing beam-coupling impedance. This work focuses on the comprehensive design of the stripline kicker intended for transverse (horizontal and vertical) bunch-by-bunch feedback in the Siam Photon Source II (SPS-II) storage ring. The stripline kicker design also incorporates features to enable its use for beam excitation in the SPS-II tune measurement system. The optimization process involves analytical approximations and detailed numerical electromagnetic field analysis of the stripline&amp;amp;rsquo;s 3D geometry, focusing on impedance matching, field homogeneity, power transmission, and beam-coupling impedance. The details of engineering design are discussed to ensure that it meets the fabrication possibilities and stringent requirements of the SPS-II accelerator.</description>
	<pubDate>2025-08-29</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 78: Design and Optimization of a Broadband Stripline Kicker for Low Beam Emittance Ring Accelerators</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/78">doi: 10.3390/particles8030078</a></p>
	<p>Authors:
		Sakdinan Naeosuphap
		Sarunyu Chaichuay
		Siriwan Jummunt
		Porntip Sudmuang
		</p>
	<p>The performance and beam quality of the new fourth-generation synchrotron light source with ultra-low emittance are highly susceptible to coupled-bunch instabilities. These instabilities arise from the interaction between the bunched electron beam and the surrounding vacuum chamber installations. To mitigate these effects, the installation of a transverse bunch-by-bunch feedback system is planned. This system will comprise a button-type beam position monitor (BPM) for beam signal detection, a digital feedback controller, a broadband power amplifier, and a broadband stripline kicker as the primary actuator. One of the critical challenges lies in the development of the stripline kicker, which must be optimized for high shunt impedance and wide bandwidth while minimizing beam-coupling impedance. This work focuses on the comprehensive design of the stripline kicker intended for transverse (horizontal and vertical) bunch-by-bunch feedback in the Siam Photon Source II (SPS-II) storage ring. The stripline kicker design also incorporates features to enable its use for beam excitation in the SPS-II tune measurement system. The optimization process involves analytical approximations and detailed numerical electromagnetic field analysis of the stripline&amp;amp;rsquo;s 3D geometry, focusing on impedance matching, field homogeneity, power transmission, and beam-coupling impedance. The details of engineering design are discussed to ensure that it meets the fabrication possibilities and stringent requirements of the SPS-II accelerator.</p>
	]]></content:encoded>

	<dc:title>Design and Optimization of a Broadband Stripline Kicker for Low Beam Emittance Ring Accelerators</dc:title>
			<dc:creator>Sakdinan Naeosuphap</dc:creator>
			<dc:creator>Sarunyu Chaichuay</dc:creator>
			<dc:creator>Siriwan Jummunt</dc:creator>
			<dc:creator>Porntip Sudmuang</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030078</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-29</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-29</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>78</prism:startingPage>
		<prism:doi>10.3390/particles8030078</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/78</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/77">

	<title>Particles, Vol. 8, Pages 77: Design and Prototype Development of a Combined-Function Quadrupole-Sextupole Magnet for the SPS-II Booster Synchrotron</title>
	<link>https://www.mdpi.com/2571-712X/8/3/77</link>
	<description>The development of a prototype booster magnet for the Siam Photon Source II (SPS-II) was launched in 2023 as a milestone in advancing accelerator technology through domestic manufacturing capabilities in Thailand. In the SPS-II booster lattice, the magnet integrates focusing quadrupole and sextupole functions into a combined-function quadrupole-sextupole magnet, enabling a more compact lattice and reducing the total number of magnets required. To meet the required magnet specifications, the design was carefully optimized using Opera-3D software (version 2021) to achieve a quadrupole gradient of 19.395 T/m and a sextupole gradient of 22.327 T/m2 over an effective magnetic length of 0.25 m, while maintaining a magnetic field homogeneity better than 1 &amp;amp;times; 10&amp;amp;minus;3. A key manufacturing challenge involved fabricating laminated magnet cores and establishing precise production processes. Magnetic field measurements performed on the prototype using the Hall-probe technique validated the magnet&amp;amp;rsquo;s quality and accuracy. This paper presents the overall development process, including the magnet design, details of the magnetic field simulation methodology, prototype fabrication, and initial magnetic field measurements.</description>
	<pubDate>2025-08-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 77: Design and Prototype Development of a Combined-Function Quadrupole-Sextupole Magnet for the SPS-II Booster Synchrotron</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/77">doi: 10.3390/particles8030077</a></p>
	<p>Authors:
		Siriwan Jummunt
		Prapaiwan Sunwong
		Supachai Prawanta
		Thongchai Leetha
		Pajeeraporn Numanoy
		Netchanok Thiabsi
		Porntip Sudmuang
		</p>
	<p>The development of a prototype booster magnet for the Siam Photon Source II (SPS-II) was launched in 2023 as a milestone in advancing accelerator technology through domestic manufacturing capabilities in Thailand. In the SPS-II booster lattice, the magnet integrates focusing quadrupole and sextupole functions into a combined-function quadrupole-sextupole magnet, enabling a more compact lattice and reducing the total number of magnets required. To meet the required magnet specifications, the design was carefully optimized using Opera-3D software (version 2021) to achieve a quadrupole gradient of 19.395 T/m and a sextupole gradient of 22.327 T/m2 over an effective magnetic length of 0.25 m, while maintaining a magnetic field homogeneity better than 1 &amp;amp;times; 10&amp;amp;minus;3. A key manufacturing challenge involved fabricating laminated magnet cores and establishing precise production processes. Magnetic field measurements performed on the prototype using the Hall-probe technique validated the magnet&amp;amp;rsquo;s quality and accuracy. This paper presents the overall development process, including the magnet design, details of the magnetic field simulation methodology, prototype fabrication, and initial magnetic field measurements.</p>
	]]></content:encoded>

	<dc:title>Design and Prototype Development of a Combined-Function Quadrupole-Sextupole Magnet for the SPS-II Booster Synchrotron</dc:title>
			<dc:creator>Siriwan Jummunt</dc:creator>
			<dc:creator>Prapaiwan Sunwong</dc:creator>
			<dc:creator>Supachai Prawanta</dc:creator>
			<dc:creator>Thongchai Leetha</dc:creator>
			<dc:creator>Pajeeraporn Numanoy</dc:creator>
			<dc:creator>Netchanok Thiabsi</dc:creator>
			<dc:creator>Porntip Sudmuang</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030077</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-28</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-28</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>77</prism:startingPage>
		<prism:doi>10.3390/particles8030077</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/77</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/76">

	<title>Particles, Vol. 8, Pages 76: The Study and Development of BPM Noise Monitoring at the Siam Photon Source</title>
	<link>https://www.mdpi.com/2571-712X/8/3/76</link>
	<description>This study presents the development of a noise-monitoring system for the storage ring at the Siam Photon Source, designed to detect and classify noise patterns in real time using beam position monitor (BPM) data. Noise patterns were categorized into four classes: broad peak, multipeak, normal peak, and no beam. Two BPMs located at the multipole wiggler section, BPM-MPW1 and BPM-MPW2, were selected for detailed monitoring based on consistent noise trends observed across the ring. The dataset was organized in two complementary formats: two-dimensional (2D) images used for training and validating the models and one-dimensional (1D) CSV files containing the corresponding raw numerical signal data. Pre-trained deep learning and 1D convolutional neural network (CNN) models were employed to classify these patterns, achieving an overall classification accuracy of up to 99.83%. The system integrates with the EPICS control framework and archiver log data, enabling continuous data acquisition and long-term analyses. Visualization and monitoring features were developed using CS-Studio/Phoebus, providing both operators and beamline scientists with intuitive tools to track beam quality and investigate noise-related anomalies. This approach highlights the potential of combining beam diagnostics with machine learning to enhance operational stability and optimize the synchrotron radiation performance for user experiments.</description>
	<pubDate>2025-08-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 76: The Study and Development of BPM Noise Monitoring at the Siam Photon Source</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/76">doi: 10.3390/particles8030076</a></p>
	<p>Authors:
		Wanisa Promdee
		Sukho Kongtawong
		Surakawin Suebka
		Thapakron Pulampong
		Natthawut Suradet
		Roengrut Rujanakraikarn
		Puttimate Hirunuran
		Siriwan Jummunt
		</p>
	<p>This study presents the development of a noise-monitoring system for the storage ring at the Siam Photon Source, designed to detect and classify noise patterns in real time using beam position monitor (BPM) data. Noise patterns were categorized into four classes: broad peak, multipeak, normal peak, and no beam. Two BPMs located at the multipole wiggler section, BPM-MPW1 and BPM-MPW2, were selected for detailed monitoring based on consistent noise trends observed across the ring. The dataset was organized in two complementary formats: two-dimensional (2D) images used for training and validating the models and one-dimensional (1D) CSV files containing the corresponding raw numerical signal data. Pre-trained deep learning and 1D convolutional neural network (CNN) models were employed to classify these patterns, achieving an overall classification accuracy of up to 99.83%. The system integrates with the EPICS control framework and archiver log data, enabling continuous data acquisition and long-term analyses. Visualization and monitoring features were developed using CS-Studio/Phoebus, providing both operators and beamline scientists with intuitive tools to track beam quality and investigate noise-related anomalies. This approach highlights the potential of combining beam diagnostics with machine learning to enhance operational stability and optimize the synchrotron radiation performance for user experiments.</p>
	]]></content:encoded>

	<dc:title>The Study and Development of BPM Noise Monitoring at the Siam Photon Source</dc:title>
			<dc:creator>Wanisa Promdee</dc:creator>
			<dc:creator>Sukho Kongtawong</dc:creator>
			<dc:creator>Surakawin Suebka</dc:creator>
			<dc:creator>Thapakron Pulampong</dc:creator>
			<dc:creator>Natthawut Suradet</dc:creator>
			<dc:creator>Roengrut Rujanakraikarn</dc:creator>
			<dc:creator>Puttimate Hirunuran</dc:creator>
			<dc:creator>Siriwan Jummunt</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030076</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-25</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-25</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>76</prism:startingPage>
		<prism:doi>10.3390/particles8030076</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/76</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/75">

	<title>Particles, Vol. 8, Pages 75: Test of Diamond sCVD Detectors at High Flux of Fast Neutrons</title>
	<link>https://www.mdpi.com/2571-712X/8/3/75</link>
	<description>We have tested the performance of spectroscopic single-crystal Chemical Vapor-Deposited (sCVD) diamond detectors with radioactive sources and with a pulsed deuterium-tritium neutron generator. The tests demonstrate that the detectors could provide good timing and spectroscopic information at high neutron fluxes. The spectroscopic information can be obtained at a 14 MeV neutron rate as high as 1010 n/cm2/s, despite some limitations associated with pulse character of the used neutron generator. Monte-Carlo simulations were performed in order to achieve better understanding of neutron interaction with the detector material. Possible applications for the use of the detectors at Soreq Applied Research Accelerator Facility (SARAF) are considered. The detectors could be used as reliable neutron rate monitors in the vicinity of a strong accelerator-based source of energetic neutrons. The detectors could also be utilized as time-of-flight tagging counters in nuclear physics experiments under condition of high neutron fluxes during short beam pulses. In particular, measurement of the 12C(n,n&amp;amp;prime;)3&amp;amp;alpha; cross-section is discussed.</description>
	<pubDate>2025-08-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 75: Test of Diamond sCVD Detectors at High Flux of Fast Neutrons</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/75">doi: 10.3390/particles8030075</a></p>
	<p>Authors:
		Leo Weissman
		Asher Shor
		Sergey Vaintraub
		</p>
	<p>We have tested the performance of spectroscopic single-crystal Chemical Vapor-Deposited (sCVD) diamond detectors with radioactive sources and with a pulsed deuterium-tritium neutron generator. The tests demonstrate that the detectors could provide good timing and spectroscopic information at high neutron fluxes. The spectroscopic information can be obtained at a 14 MeV neutron rate as high as 1010 n/cm2/s, despite some limitations associated with pulse character of the used neutron generator. Monte-Carlo simulations were performed in order to achieve better understanding of neutron interaction with the detector material. Possible applications for the use of the detectors at Soreq Applied Research Accelerator Facility (SARAF) are considered. The detectors could be used as reliable neutron rate monitors in the vicinity of a strong accelerator-based source of energetic neutrons. The detectors could also be utilized as time-of-flight tagging counters in nuclear physics experiments under condition of high neutron fluxes during short beam pulses. In particular, measurement of the 12C(n,n&amp;amp;prime;)3&amp;amp;alpha; cross-section is discussed.</p>
	]]></content:encoded>

	<dc:title>Test of Diamond sCVD Detectors at High Flux of Fast Neutrons</dc:title>
			<dc:creator>Leo Weissman</dc:creator>
			<dc:creator>Asher Shor</dc:creator>
			<dc:creator>Sergey Vaintraub</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030075</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-07</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-07</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>75</prism:startingPage>
		<prism:doi>10.3390/particles8030075</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/75</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/74">

	<title>Particles, Vol. 8, Pages 74: Study of High-Altitude Coplanarity Phenomena in Super-High-Energy EAS Cores with a Thick Calorimeter</title>
	<link>https://www.mdpi.com/2571-712X/8/3/74</link>
	<description>A number of phenomena were observed in experiments on the study of cosmic rays at mountain altitudes and in the stratosphere at ultra-high energies; in particular, the coplanarity of the most energetic particles and local subcascades in the so-called families of &amp;amp;gamma;-rays and hadrons in the cores of extensive air showers at E0 &amp;amp;#8819; 2&amp;amp;middot;1015 eV (&amp;amp;radic;s &amp;amp;#8819; 2 TeV). These effects are not described by theoretical models. To explain this phenomenon, it may be necessary to introduce a new process of generating the most energetic particles in the interactions of hadrons with the nuclei of atmospheric atoms. A new experimental array of cosmic ray detectors, including the ADRON-55 ionization calorimeter, has been created to study processes in EAS cores at ultra-high energies. The possibility of using it to study the coplanarity effect is being considered.</description>
	<pubDate>2025-08-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 74: Study of High-Altitude Coplanarity Phenomena in Super-High-Energy EAS Cores with a Thick Calorimeter</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/74">doi: 10.3390/particles8030074</a></p>
	<p>Authors:
		Rauf Mukhamedshin
		Turlan Sadykov
		Vladimir Galkin
		Alia Argynova
		Aidana Almenova
		Dauren Muratov
		Khanshaiym Makhmet
		Valery Zhukov
		Vladimir Ryabov
		Vyacheslav Piscal
		Yernar Tautayev
		Zhakypbek Sadykov
		</p>
	<p>A number of phenomena were observed in experiments on the study of cosmic rays at mountain altitudes and in the stratosphere at ultra-high energies; in particular, the coplanarity of the most energetic particles and local subcascades in the so-called families of &amp;amp;gamma;-rays and hadrons in the cores of extensive air showers at E0 &amp;amp;#8819; 2&amp;amp;middot;1015 eV (&amp;amp;radic;s &amp;amp;#8819; 2 TeV). These effects are not described by theoretical models. To explain this phenomenon, it may be necessary to introduce a new process of generating the most energetic particles in the interactions of hadrons with the nuclei of atmospheric atoms. A new experimental array of cosmic ray detectors, including the ADRON-55 ionization calorimeter, has been created to study processes in EAS cores at ultra-high energies. The possibility of using it to study the coplanarity effect is being considered.</p>
	]]></content:encoded>

	<dc:title>Study of High-Altitude Coplanarity Phenomena in Super-High-Energy EAS Cores with a Thick Calorimeter</dc:title>
			<dc:creator>Rauf Mukhamedshin</dc:creator>
			<dc:creator>Turlan Sadykov</dc:creator>
			<dc:creator>Vladimir Galkin</dc:creator>
			<dc:creator>Alia Argynova</dc:creator>
			<dc:creator>Aidana Almenova</dc:creator>
			<dc:creator>Dauren Muratov</dc:creator>
			<dc:creator>Khanshaiym Makhmet</dc:creator>
			<dc:creator>Valery Zhukov</dc:creator>
			<dc:creator>Vladimir Ryabov</dc:creator>
			<dc:creator>Vyacheslav Piscal</dc:creator>
			<dc:creator>Yernar Tautayev</dc:creator>
			<dc:creator>Zhakypbek Sadykov</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030074</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-04</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>74</prism:startingPage>
		<prism:doi>10.3390/particles8030074</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/74</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/73">

	<title>Particles, Vol. 8, Pages 73: A Scintillation Hodoscope for Measuring the Flux of Cosmic Ray Muons at the Tien Shan High Mountain Station</title>
	<link>https://www.mdpi.com/2571-712X/8/3/73</link>
	<description>For further investigation of the properties of the muon component in the core regions of extensive air showers (EASs), a new underground hodoscopic set-up with a total sensitive area of 22 m2 was built at the Tien Shan High Mountain Cosmic Ray Station. The hodoscope is based on a set of large-sized scintillation charged particle detectors with an output signal of analog type. The installation ensures a (5–8) GeV energy threshold of muon registration and a ∼104 dynamic range for the measurement of the density of muon flux. A program facility was designed that uses modern machine learning techniques for automated search for the typical scintillation pulse pattern in an oscillogram of a noisy analog signal at the output of the hodoscope detector. The program provides a ∼99% detection probability of useful signals, with a relative share of false positives below 1%, and has a sufficient operation speed for real-time analysis of incoming data. Complete verification of the hardware and software tools was performed under realistic operation conditions, and the results obtained demonstrate the correctness of the proposed method and its practical applicability to the investigation of the muon flux in EASs. In the course of the installation testing, a preliminary physical result was obtained concerning the rise of the multiplicity of muon particles around an EAS core in dependence on the primary EAS energy.</description>
	<pubDate>2025-08-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 73: A Scintillation Hodoscope for Measuring the Flux of Cosmic Ray Muons at the Tien Shan High Mountain Station</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/73">doi: 10.3390/particles8030073</a></p>
	<p>Authors:
		Alexander Shepetov
		Aliya Baktoraz
		Orazaly Kalikulov
		Svetlana Mamina
		Yerzhan Mukhamejanov
		Kanat Mukashev
		Vladimir Ryabov
		Nurzhan Saduyev
		Turlan Sadykov
		Saken Shinbulatov
		Tairzhan Skokbayev
		Ivan Sopko
		Shynbolat Utey
		Ludmila Vildanova
		Nurzhan Yerezhep
		Valery Zhukov
		</p>
	<p>For further investigation of the properties of the muon component in the core regions of extensive air showers (EASs), a new underground hodoscopic set-up with a total sensitive area of 22 m2 was built at the Tien Shan High Mountain Cosmic Ray Station. The hodoscope is based on a set of large-sized scintillation charged particle detectors with an output signal of analog type. The installation ensures a (5–8) GeV energy threshold of muon registration and a ∼104 dynamic range for the measurement of the density of muon flux. A program facility was designed that uses modern machine learning techniques for automated search for the typical scintillation pulse pattern in an oscillogram of a noisy analog signal at the output of the hodoscope detector. The program provides a ∼99% detection probability of useful signals, with a relative share of false positives below 1%, and has a sufficient operation speed for real-time analysis of incoming data. Complete verification of the hardware and software tools was performed under realistic operation conditions, and the results obtained demonstrate the correctness of the proposed method and its practical applicability to the investigation of the muon flux in EASs. In the course of the installation testing, a preliminary physical result was obtained concerning the rise of the multiplicity of muon particles around an EAS core in dependence on the primary EAS energy.</p>
	]]></content:encoded>

	<dc:title>A Scintillation Hodoscope for Measuring the Flux of Cosmic Ray Muons at the Tien Shan High Mountain Station</dc:title>
			<dc:creator>Alexander Shepetov</dc:creator>
			<dc:creator>Aliya Baktoraz</dc:creator>
			<dc:creator>Orazaly Kalikulov</dc:creator>
			<dc:creator>Svetlana Mamina</dc:creator>
			<dc:creator>Yerzhan Mukhamejanov</dc:creator>
			<dc:creator>Kanat Mukashev</dc:creator>
			<dc:creator>Vladimir Ryabov</dc:creator>
			<dc:creator>Nurzhan Saduyev</dc:creator>
			<dc:creator>Turlan Sadykov</dc:creator>
			<dc:creator>Saken Shinbulatov</dc:creator>
			<dc:creator>Tairzhan Skokbayev</dc:creator>
			<dc:creator>Ivan Sopko</dc:creator>
			<dc:creator>Shynbolat Utey</dc:creator>
			<dc:creator>Ludmila Vildanova</dc:creator>
			<dc:creator>Nurzhan Yerezhep</dc:creator>
			<dc:creator>Valery Zhukov</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030073</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-08-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-08-04</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>73</prism:startingPage>
		<prism:doi>10.3390/particles8030073</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/73</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/72">

	<title>Particles, Vol. 8, Pages 72: Effect of the Coulomb Interaction on Nuclear Deformation and Drip Lines</title>
	<link>https://www.mdpi.com/2571-712X/8/3/72</link>
	<description>Nuclei are self-bound systems in which the strong interaction (nuclear force) plays a dominant role, and the isospin is approximately a good quantum number. The isospin symmetry is primarily violated by electromagnetic interactions, namely Coulomb interactions among protons, the effects of which need be studied to understand the importance of the isospin symmetry. We investigate the effect of the Coulomb interaction on nuclear properties, especially quadrupole deformation and neutron drip line, utilizing the density functional method, which provides a universal description of nuclear systems in the entire nuclear chart. We carry out calculations of even&amp;amp;ndash;even nuclei with a proton number of 2&amp;amp;le;Z&amp;amp;le;60. The results show that the Coulomb interaction plays a significant role in enhancing quadrupole deformation across a wide range of nuclei. We also find that, after including the Coulomb interaction, some nuclei near the neutron drip line become stable against two-neutron emissions, resulting in a shift in the drip line towards larger neutron numbers.</description>
	<pubDate>2025-07-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 72: Effect of the Coulomb Interaction on Nuclear Deformation and Drip Lines</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/72">doi: 10.3390/particles8030072</a></p>
	<p>Authors:
		Kenta Hagihara
		Takashi Nakatsukasa
		Nobuo Hinohara
		</p>
	<p>Nuclei are self-bound systems in which the strong interaction (nuclear force) plays a dominant role, and the isospin is approximately a good quantum number. The isospin symmetry is primarily violated by electromagnetic interactions, namely Coulomb interactions among protons, the effects of which need be studied to understand the importance of the isospin symmetry. We investigate the effect of the Coulomb interaction on nuclear properties, especially quadrupole deformation and neutron drip line, utilizing the density functional method, which provides a universal description of nuclear systems in the entire nuclear chart. We carry out calculations of even&amp;amp;ndash;even nuclei with a proton number of 2&amp;amp;le;Z&amp;amp;le;60. The results show that the Coulomb interaction plays a significant role in enhancing quadrupole deformation across a wide range of nuclei. We also find that, after including the Coulomb interaction, some nuclei near the neutron drip line become stable against two-neutron emissions, resulting in a shift in the drip line towards larger neutron numbers.</p>
	]]></content:encoded>

	<dc:title>Effect of the Coulomb Interaction on Nuclear Deformation and Drip Lines</dc:title>
			<dc:creator>Kenta Hagihara</dc:creator>
			<dc:creator>Takashi Nakatsukasa</dc:creator>
			<dc:creator>Nobuo Hinohara</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030072</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-24</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-24</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>72</prism:startingPage>
		<prism:doi>10.3390/particles8030072</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/72</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/71">

	<title>Particles, Vol. 8, Pages 71: Investigating Coherent Smith&amp;ndash;Purcell Radiation from Shallow Blazed Gratings: Shading Effect&amp;rsquo;s Influence on Surface Current Model</title>
	<link>https://www.mdpi.com/2571-712X/8/3/71</link>
	<description>To evaluate the characteristics of Smith&amp;amp;ndash;Purcell radiation, we modified a surface current model to consider the geometrical shading effect of a grating, which was ignored in the original one, and compared it with measurements for a grating with a shallow blaze angle. According to the numerical calculations based on the surface current model with and without the shading effect, it was found that the azimuthal angular distribution, polarization components and the variation in radiation intensity with the blaze angle of the grating are predicted to show significantly different behaviors under our experimental conditions. Generating the coherent Smith&amp;amp;ndash;Purcell radiation using the very short electron bunch in the test accelerator, t-ACTS at the Research Center for Accelerator and Radioisotope Science, Tohoku University, we measured polarization and the angular distribution of radiation for the gratings with different blaze angles. This study supports the validity of the modified surface current model with the shading effect and will provide new insights into the evaluation of the characteristics of Smith&amp;amp;ndash;Purcell radiation.</description>
	<pubDate>2025-07-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 71: Investigating Coherent Smith&amp;ndash;Purcell Radiation from Shallow Blazed Gratings: Shading Effect&amp;rsquo;s Influence on Surface Current Model</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/71">doi: 10.3390/particles8030071</a></p>
	<p>Authors:
		Hiroki Yamada
		Toshiya Muto
		Fujio Hinode
		Shigeru Kashiwagi
		Kenichi Nanbu
		Ikuro Nagasawa
		Kotaro Shibata
		Ken Takahashi
		Anjali Bhagwan Kavar
		Kodai Kudo
		Hayato Abiko
		Pitchayapak Kitisri
		Hiroyuki Hama
		</p>
	<p>To evaluate the characteristics of Smith&amp;amp;ndash;Purcell radiation, we modified a surface current model to consider the geometrical shading effect of a grating, which was ignored in the original one, and compared it with measurements for a grating with a shallow blaze angle. According to the numerical calculations based on the surface current model with and without the shading effect, it was found that the azimuthal angular distribution, polarization components and the variation in radiation intensity with the blaze angle of the grating are predicted to show significantly different behaviors under our experimental conditions. Generating the coherent Smith&amp;amp;ndash;Purcell radiation using the very short electron bunch in the test accelerator, t-ACTS at the Research Center for Accelerator and Radioisotope Science, Tohoku University, we measured polarization and the angular distribution of radiation for the gratings with different blaze angles. This study supports the validity of the modified surface current model with the shading effect and will provide new insights into the evaluation of the characteristics of Smith&amp;amp;ndash;Purcell radiation.</p>
	]]></content:encoded>

	<dc:title>Investigating Coherent Smith&amp;amp;ndash;Purcell Radiation from Shallow Blazed Gratings: Shading Effect&amp;amp;rsquo;s Influence on Surface Current Model</dc:title>
			<dc:creator>Hiroki Yamada</dc:creator>
			<dc:creator>Toshiya Muto</dc:creator>
			<dc:creator>Fujio Hinode</dc:creator>
			<dc:creator>Shigeru Kashiwagi</dc:creator>
			<dc:creator>Kenichi Nanbu</dc:creator>
			<dc:creator>Ikuro Nagasawa</dc:creator>
			<dc:creator>Kotaro Shibata</dc:creator>
			<dc:creator>Ken Takahashi</dc:creator>
			<dc:creator>Anjali Bhagwan Kavar</dc:creator>
			<dc:creator>Kodai Kudo</dc:creator>
			<dc:creator>Hayato Abiko</dc:creator>
			<dc:creator>Pitchayapak Kitisri</dc:creator>
			<dc:creator>Hiroyuki Hama</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030071</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-23</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-23</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>71</prism:startingPage>
		<prism:doi>10.3390/particles8030071</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/71</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/70">

	<title>Particles, Vol. 8, Pages 70: Intertwined Orders and the Physics of High Temperature Superconductors</title>
	<link>https://www.mdpi.com/2571-712X/8/3/70</link>
	<description>Complex phase diagrams are a generic feature of quantum materials that display high-temperature superconductivity. In addition to d-wave superconductivity (or other unconventional states), these phase diagrams typically include various forms of charge-ordered phases, including charge-density waves and/or spin-density waves, as well as electronic nematic states. In most cases, these phases have critical temperatures comparable in magnitude to that of the superconducting state and appear in a &amp;amp;ldquo;pseudo-gap&amp;amp;rdquo; regime. In these systems, the high temperature state does not produce a good metal with well-defined quasiparticles but a &amp;amp;rdquo;strange metal&amp;amp;rdquo;. These states typically arise from doping a strongly correlated Mott insulator. With my collaborators, I have identified these behaviors as a problem with &amp;amp;ldquo;Intertwined Orders&amp;amp;rdquo;. A pair-density wave is a type of superconducting state that embodies the physics of intertwined orders. Here, I discuss the phenomenology of intertwined orders and the quantum materials that are known to display these behaviors.</description>
	<pubDate>2025-07-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 70: Intertwined Orders and the Physics of High Temperature Superconductors</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/70">doi: 10.3390/particles8030070</a></p>
	<p>Authors:
		Eduardo Fradkin
		</p>
	<p>Complex phase diagrams are a generic feature of quantum materials that display high-temperature superconductivity. In addition to d-wave superconductivity (or other unconventional states), these phase diagrams typically include various forms of charge-ordered phases, including charge-density waves and/or spin-density waves, as well as electronic nematic states. In most cases, these phases have critical temperatures comparable in magnitude to that of the superconducting state and appear in a &amp;amp;ldquo;pseudo-gap&amp;amp;rdquo; regime. In these systems, the high temperature state does not produce a good metal with well-defined quasiparticles but a &amp;amp;rdquo;strange metal&amp;amp;rdquo;. These states typically arise from doping a strongly correlated Mott insulator. With my collaborators, I have identified these behaviors as a problem with &amp;amp;ldquo;Intertwined Orders&amp;amp;rdquo;. A pair-density wave is a type of superconducting state that embodies the physics of intertwined orders. Here, I discuss the phenomenology of intertwined orders and the quantum materials that are known to display these behaviors.</p>
	]]></content:encoded>

	<dc:title>Intertwined Orders and the Physics of High Temperature Superconductors</dc:title>
			<dc:creator>Eduardo Fradkin</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030070</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-23</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-23</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>70</prism:startingPage>
		<prism:doi>10.3390/particles8030070</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/70</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/69">

	<title>Particles, Vol. 8, Pages 69: Background Measurements and Simulations of the ComPair Balloon Flight</title>
	<link>https://www.mdpi.com/2571-712X/8/3/69</link>
	<description>ComPair, a prototype of the All-sky Medium Energy Gamma-ray Observatory (AMEGO), completed a short-duration high-altitude balloon campaign on 27 August 2023 from Fort Sumner, New Mexico, USA. The goal of the balloon flight was to demonstrate ComPair as both a Compton and Pair telescope in flight, reject the charged particle background, and measure the background &amp;amp;gamma;-ray spectrum. This analysis compares measurements from the balloon flight with Monte Carlo simulations to benchmark the instrument. The comparison finds good agreement between the measurements and simulations and supports the conclusion that ComPair accomplished its goals for the balloon campaign. Additionally, two charged particle background rejection schemes are discussed: a soft ACD veto that records a higher charged particle event rate but with less risk of event loss, and a hard ACD veto that limits the charged particle event rate on board. There was little difference in the measured spectra from the soft and hard ACD veto schemes, indicating that the hard ACD veto could be used for future flights. The successes of ComPair&amp;amp;rsquo;s engineering flight will inform the development of the next generation of ComPair with upgraded detector technology and larger active area.</description>
	<pubDate>2025-07-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 69: Background Measurements and Simulations of the ComPair Balloon Flight</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/69">doi: 10.3390/particles8030069</a></p>
	<p>Authors:
		Zachary Metzler
		Nicholas Kirschner
		Lucas Smith
		Nicholas Cannady
		Makoto Sasaki
		Daniel Shy
		Regina Caputo
		Carolyn Kierans
		Aleksey Bolotnikov
		Thomas J. Caligiure
		Gabriella A. Carini
		Alexander Wilder Crosier
		Jack Fried
		Priyarshini Ghosh
		Sean Griffin
		Jon Eric Grove
		Elizabeth Hays
		Sven Herrmann
		Emily Kong
		Iker Liceaga-Indart
		Julie McEnery
		John Mitchell
		Alexander A. Moiseev
		Lucas Parker
		Jeremy Perkins
		Bernard Phlips
		Adam J. Schoenwald
		Clio Sleator
		David J. Thompson
		Janeth Valverde
		Sambid Wasti
		Richard Woolf
		Eric Wulf
		Anna Zajczyk
		</p>
	<p>ComPair, a prototype of the All-sky Medium Energy Gamma-ray Observatory (AMEGO), completed a short-duration high-altitude balloon campaign on 27 August 2023 from Fort Sumner, New Mexico, USA. The goal of the balloon flight was to demonstrate ComPair as both a Compton and Pair telescope in flight, reject the charged particle background, and measure the background &amp;amp;gamma;-ray spectrum. This analysis compares measurements from the balloon flight with Monte Carlo simulations to benchmark the instrument. The comparison finds good agreement between the measurements and simulations and supports the conclusion that ComPair accomplished its goals for the balloon campaign. Additionally, two charged particle background rejection schemes are discussed: a soft ACD veto that records a higher charged particle event rate but with less risk of event loss, and a hard ACD veto that limits the charged particle event rate on board. There was little difference in the measured spectra from the soft and hard ACD veto schemes, indicating that the hard ACD veto could be used for future flights. The successes of ComPair&amp;amp;rsquo;s engineering flight will inform the development of the next generation of ComPair with upgraded detector technology and larger active area.</p>
	]]></content:encoded>

	<dc:title>Background Measurements and Simulations of the ComPair Balloon Flight</dc:title>
			<dc:creator>Zachary Metzler</dc:creator>
			<dc:creator>Nicholas Kirschner</dc:creator>
			<dc:creator>Lucas Smith</dc:creator>
			<dc:creator>Nicholas Cannady</dc:creator>
			<dc:creator>Makoto Sasaki</dc:creator>
			<dc:creator>Daniel Shy</dc:creator>
			<dc:creator>Regina Caputo</dc:creator>
			<dc:creator>Carolyn Kierans</dc:creator>
			<dc:creator>Aleksey Bolotnikov</dc:creator>
			<dc:creator>Thomas J. Caligiure</dc:creator>
			<dc:creator>Gabriella A. Carini</dc:creator>
			<dc:creator>Alexander Wilder Crosier</dc:creator>
			<dc:creator>Jack Fried</dc:creator>
			<dc:creator>Priyarshini Ghosh</dc:creator>
			<dc:creator>Sean Griffin</dc:creator>
			<dc:creator>Jon Eric Grove</dc:creator>
			<dc:creator>Elizabeth Hays</dc:creator>
			<dc:creator>Sven Herrmann</dc:creator>
			<dc:creator>Emily Kong</dc:creator>
			<dc:creator>Iker Liceaga-Indart</dc:creator>
			<dc:creator>Julie McEnery</dc:creator>
			<dc:creator>John Mitchell</dc:creator>
			<dc:creator>Alexander A. Moiseev</dc:creator>
			<dc:creator>Lucas Parker</dc:creator>
			<dc:creator>Jeremy Perkins</dc:creator>
			<dc:creator>Bernard Phlips</dc:creator>
			<dc:creator>Adam J. Schoenwald</dc:creator>
			<dc:creator>Clio Sleator</dc:creator>
			<dc:creator>David J. Thompson</dc:creator>
			<dc:creator>Janeth Valverde</dc:creator>
			<dc:creator>Sambid Wasti</dc:creator>
			<dc:creator>Richard Woolf</dc:creator>
			<dc:creator>Eric Wulf</dc:creator>
			<dc:creator>Anna Zajczyk</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030069</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-19</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-19</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>69</prism:startingPage>
		<prism:doi>10.3390/particles8030069</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/69</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/68">

	<title>Particles, Vol. 8, Pages 68: High Average Current Electron Beam Generation Using RF Gated Thermionic Electron Gun</title>
	<link>https://www.mdpi.com/2571-712X/8/3/68</link>
	<description>High-current electron beams can significantly enhance the productivity of variety of applications including medical radioisotope (RI) production and wastewater purification. High-power superconducting radio frequency (SRF) linacs are capable of producing such high-current electron beams due to the key advantage to operate in continuous wave (CW) mode. However, this requires an injector capable of generating electron bunches with high repetition rate and in CW mode, while minimizing beam losses to avoid damage to SRF cavities due to quenching. RF gating to the grid of a thermionic electron gun is a promising solution, as it ensures CW bunch generation at the repetition rate same as the fundamental or sub-harmonics of the accelerating RF frequency, with minimal beam loss. This paper presents detailed beam dynamics simulations demonstrating that an RF-gated gun operating at 1.3 GHz can generate bunches with 148 ps full width with 8.96 pC charge.</description>
	<pubDate>2025-07-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 68: High Average Current Electron Beam Generation Using RF Gated Thermionic Electron Gun</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/68">doi: 10.3390/particles8030068</a></p>
	<p>Authors:
		Anjali Bhagwan Kavar
		Shigeru Kashiwagi
		Kai Masuda
		Toshiya Muto
		Fujio Hinode
		Kenichi Nanbu
		Ikuro Nagasawa
		Kotaro Shibata
		Ken Takahashi
		Hiroki Yamada
		Kodai Kudo
		Hayato Abiko
		Pitchayapak Kitisri
		Hiroyuki Hama
		</p>
	<p>High-current electron beams can significantly enhance the productivity of variety of applications including medical radioisotope (RI) production and wastewater purification. High-power superconducting radio frequency (SRF) linacs are capable of producing such high-current electron beams due to the key advantage to operate in continuous wave (CW) mode. However, this requires an injector capable of generating electron bunches with high repetition rate and in CW mode, while minimizing beam losses to avoid damage to SRF cavities due to quenching. RF gating to the grid of a thermionic electron gun is a promising solution, as it ensures CW bunch generation at the repetition rate same as the fundamental or sub-harmonics of the accelerating RF frequency, with minimal beam loss. This paper presents detailed beam dynamics simulations demonstrating that an RF-gated gun operating at 1.3 GHz can generate bunches with 148 ps full width with 8.96 pC charge.</p>
	]]></content:encoded>

	<dc:title>High Average Current Electron Beam Generation Using RF Gated Thermionic Electron Gun</dc:title>
			<dc:creator>Anjali Bhagwan Kavar</dc:creator>
			<dc:creator>Shigeru Kashiwagi</dc:creator>
			<dc:creator>Kai Masuda</dc:creator>
			<dc:creator>Toshiya Muto</dc:creator>
			<dc:creator>Fujio Hinode</dc:creator>
			<dc:creator>Kenichi Nanbu</dc:creator>
			<dc:creator>Ikuro Nagasawa</dc:creator>
			<dc:creator>Kotaro Shibata</dc:creator>
			<dc:creator>Ken Takahashi</dc:creator>
			<dc:creator>Hiroki Yamada</dc:creator>
			<dc:creator>Kodai Kudo</dc:creator>
			<dc:creator>Hayato Abiko</dc:creator>
			<dc:creator>Pitchayapak Kitisri</dc:creator>
			<dc:creator>Hiroyuki Hama</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030068</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-08</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-08</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>68</prism:startingPage>
		<prism:doi>10.3390/particles8030068</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/68</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/67">

	<title>Particles, Vol. 8, Pages 67: EM Characterization of a Compact RFQ Cold Model Prototype Employing a New Power Injection Scheme</title>
	<link>https://www.mdpi.com/2571-712X/8/3/67</link>
	<description>The experimental and computational characterization of a cold model prototype designed to test the electromagnetic properties of a new RFQ (Radio-Frequency Quadrupole) cavity is reported. This cavity is intended to be an essential part of a compact, high-gradient proton accelerator for medical purposes. The RFQ&amp;amp;rsquo;s design employs a novel RF power-coupler injection solution. One common way to couple the RF power in proton RFQs has been the use of loop-couplers inserted into the mid-section of the RFQ&amp;amp;rsquo;s lobe sections. This technique has been demonstrated to be reliable and effective but introduces a significant perturbation into the lobe that can be more noticeable when dealing with compact structures. We propose a RF injection scheme that uses direct transition from a coaxial cable to the RFQ by connecting the inner coaxial conductor to the RFQ vane body. As a consequence, the lobe geometry is not perturbed, and the transversal electrical fields are directly excited through the vanes. Moreover, by using a pair of such couplers connected to opposite vanes at a given transversal plane of the RFQ, it is also possible to excite the desired quadrupolar TE210 modes while avoiding the excitation of dipolar TE110 modes. The resonances corresponding to different RFQ modes have been characterized, and the dependence of the amplitude of the modes on the relative phase of the field injected through the RF power ports has been demonstrated both by measurements and simulations.</description>
	<pubDate>2025-07-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 67: EM Characterization of a Compact RFQ Cold Model Prototype Employing a New Power Injection Scheme</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/67">doi: 10.3390/particles8030067</a></p>
	<p>Authors:
		Marco A. López
		Joaquín Portilla
		Victor Etxebarria
		Iñigo Arredondo
		Jorge Feuchtwanger
		</p>
	<p>The experimental and computational characterization of a cold model prototype designed to test the electromagnetic properties of a new RFQ (Radio-Frequency Quadrupole) cavity is reported. This cavity is intended to be an essential part of a compact, high-gradient proton accelerator for medical purposes. The RFQ&amp;amp;rsquo;s design employs a novel RF power-coupler injection solution. One common way to couple the RF power in proton RFQs has been the use of loop-couplers inserted into the mid-section of the RFQ&amp;amp;rsquo;s lobe sections. This technique has been demonstrated to be reliable and effective but introduces a significant perturbation into the lobe that can be more noticeable when dealing with compact structures. We propose a RF injection scheme that uses direct transition from a coaxial cable to the RFQ by connecting the inner coaxial conductor to the RFQ vane body. As a consequence, the lobe geometry is not perturbed, and the transversal electrical fields are directly excited through the vanes. Moreover, by using a pair of such couplers connected to opposite vanes at a given transversal plane of the RFQ, it is also possible to excite the desired quadrupolar TE210 modes while avoiding the excitation of dipolar TE110 modes. The resonances corresponding to different RFQ modes have been characterized, and the dependence of the amplitude of the modes on the relative phase of the field injected through the RF power ports has been demonstrated both by measurements and simulations.</p>
	]]></content:encoded>

	<dc:title>EM Characterization of a Compact RFQ Cold Model Prototype Employing a New Power Injection Scheme</dc:title>
			<dc:creator>Marco A. López</dc:creator>
			<dc:creator>Joaquín Portilla</dc:creator>
			<dc:creator>Victor Etxebarria</dc:creator>
			<dc:creator>Iñigo Arredondo</dc:creator>
			<dc:creator>Jorge Feuchtwanger</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030067</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-07-01</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-07-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>67</prism:startingPage>
		<prism:doi>10.3390/particles8030067</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/67</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/66">

	<title>Particles, Vol. 8, Pages 66: Design and Development of Dipole Magnet for MIR/THz Free Electron Laser Beam Dumps and Spectrometers</title>
	<link>https://www.mdpi.com/2571-712X/8/3/66</link>
	<description>This study presents the design and development of electromagnetic dipole magnets for use as beam dumps and spectrometers in the MIR and THz free-electron laser (FEL) beamlines at the PBP-CMU Electron Linac Laboratory (PCELL). The magnets were optimized to achieve a 60-degree bending angle for electron beams with energies up to 30 MeV, without requiring water cooling. Using CST EM Studio for 3D magnetic field simulations and ASTRA for particle tracking, the THz dipole (with 414 turns) and MIR dipole (with 600 turns) generated magnetic fields of 0.1739 T and 0.2588 T, respectively, while both operating at currents below 10 A. Performance analysis confirmed effective beam deflection, with the THz dipole showing that it was capable of handling beam energies up to 20 MeV and the MIR dipole could handle up to 30 MeV. The energy measurement at the spectrometer screen position was simulated, taking into account transverse beam size, fringe fields, and space charge effects, using ASTRA. The energy resolution, defined as the ratio of energy uncertainty to the mean energy, was evaluated for selected cases. For beam energies of 16 MeV and 25 MeV, resolutions of 0.2% and 0.5% were achieved with transverse beam sizes of 1 mm and 4 mm, respectively. All evaluated cases maintained energy resolutions below 1%, confirming the spectrometer&amp;amp;rsquo;s suitability for high-precision beam diagnostics. Furthermore, the relationship between the initial and measured energy spread errors, taking into account a camera resolution of 0.1 mm/pixel, was evaluated. Simulations across various beam energies (10&amp;amp;ndash;16 MeV for the THz dipole and 20&amp;amp;ndash;25 MeV for the MIR dipole) confirmed that the measurement error in energy spread decreases with smaller RMS transverse beam sizes. This trend was consistent across all tested energies and magnet configurations. To ensure accurate energy spread measurements, a small initial beam size is recommended. Specifically, for beams with a narrow initial energy spread, a transverse beam size below 1 mm is essential.</description>
	<pubDate>2025-06-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 66: Design and Development of Dipole Magnet for MIR/THz Free Electron Laser Beam Dumps and Spectrometers</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/66">doi: 10.3390/particles8030066</a></p>
	<p>Authors:
		Ekkachai Kongmon
		Kantaphon Damminsek
		Nopadon Khangrang
		Sakhorn Rimjaem
		Chitrlada Thongbai
		</p>
	<p>This study presents the design and development of electromagnetic dipole magnets for use as beam dumps and spectrometers in the MIR and THz free-electron laser (FEL) beamlines at the PBP-CMU Electron Linac Laboratory (PCELL). The magnets were optimized to achieve a 60-degree bending angle for electron beams with energies up to 30 MeV, without requiring water cooling. Using CST EM Studio for 3D magnetic field simulations and ASTRA for particle tracking, the THz dipole (with 414 turns) and MIR dipole (with 600 turns) generated magnetic fields of 0.1739 T and 0.2588 T, respectively, while both operating at currents below 10 A. Performance analysis confirmed effective beam deflection, with the THz dipole showing that it was capable of handling beam energies up to 20 MeV and the MIR dipole could handle up to 30 MeV. The energy measurement at the spectrometer screen position was simulated, taking into account transverse beam size, fringe fields, and space charge effects, using ASTRA. The energy resolution, defined as the ratio of energy uncertainty to the mean energy, was evaluated for selected cases. For beam energies of 16 MeV and 25 MeV, resolutions of 0.2% and 0.5% were achieved with transverse beam sizes of 1 mm and 4 mm, respectively. All evaluated cases maintained energy resolutions below 1%, confirming the spectrometer&amp;amp;rsquo;s suitability for high-precision beam diagnostics. Furthermore, the relationship between the initial and measured energy spread errors, taking into account a camera resolution of 0.1 mm/pixel, was evaluated. Simulations across various beam energies (10&amp;amp;ndash;16 MeV for the THz dipole and 20&amp;amp;ndash;25 MeV for the MIR dipole) confirmed that the measurement error in energy spread decreases with smaller RMS transverse beam sizes. This trend was consistent across all tested energies and magnet configurations. To ensure accurate energy spread measurements, a small initial beam size is recommended. Specifically, for beams with a narrow initial energy spread, a transverse beam size below 1 mm is essential.</p>
	]]></content:encoded>

	<dc:title>Design and Development of Dipole Magnet for MIR/THz Free Electron Laser Beam Dumps and Spectrometers</dc:title>
			<dc:creator>Ekkachai Kongmon</dc:creator>
			<dc:creator>Kantaphon Damminsek</dc:creator>
			<dc:creator>Nopadon Khangrang</dc:creator>
			<dc:creator>Sakhorn Rimjaem</dc:creator>
			<dc:creator>Chitrlada Thongbai</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030066</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-25</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-25</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>66</prism:startingPage>
		<prism:doi>10.3390/particles8030066</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/66</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/65">

	<title>Particles, Vol. 8, Pages 65: On the Evidence for the Violation of the Equivalence Principle in Disk Galaxies</title>
	<link>https://www.mdpi.com/2571-712X/8/3/65</link>
	<description>We examine the claimed observations of a gravitational external field effect (EFE) reported by Chae et al. We show that observations suggestive of the EFE can be interpreted without violating Einstein&amp;amp;rsquo;s equivalence principle, namely from known correlations between the morphology, the environment, and dynamics of galaxies. While Chae et al.&amp;amp;rsquo;s analysis provides a valuable attempt at a clear test of modified Newtonian dynamics, an evidently important topic, a re-analysis of the observational data does not permit us to confidently assess the presence of an EFE or to distinguish this interpretation from that proposed in this article.</description>
	<pubDate>2025-06-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 65: On the Evidence for the Violation of the Equivalence Principle in Disk Galaxies</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/65">doi: 10.3390/particles8030065</a></p>
	<p>Authors:
		Corey Sargent
		William Clark
		Antonia Seifert
		Alicia Mand
		Emerson Rogers
		Adam Lane
		Alexandre Deur
		Balša Terzić
		</p>
	<p>We examine the claimed observations of a gravitational external field effect (EFE) reported by Chae et al. We show that observations suggestive of the EFE can be interpreted without violating Einstein&amp;amp;rsquo;s equivalence principle, namely from known correlations between the morphology, the environment, and dynamics of galaxies. While Chae et al.&amp;amp;rsquo;s analysis provides a valuable attempt at a clear test of modified Newtonian dynamics, an evidently important topic, a re-analysis of the observational data does not permit us to confidently assess the presence of an EFE or to distinguish this interpretation from that proposed in this article.</p>
	]]></content:encoded>

	<dc:title>On the Evidence for the Violation of the Equivalence Principle in Disk Galaxies</dc:title>
			<dc:creator>Corey Sargent</dc:creator>
			<dc:creator>William Clark</dc:creator>
			<dc:creator>Antonia Seifert</dc:creator>
			<dc:creator>Alicia Mand</dc:creator>
			<dc:creator>Emerson Rogers</dc:creator>
			<dc:creator>Adam Lane</dc:creator>
			<dc:creator>Alexandre Deur</dc:creator>
			<dc:creator>Balša Terzić</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030065</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-22</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>65</prism:startingPage>
		<prism:doi>10.3390/particles8030065</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/65</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/64">

	<title>Particles, Vol. 8, Pages 64: Beam Emittance and Bunch Length Diagnostics for the MIR-FEL Beamline at Chiang Mai University</title>
	<link>https://www.mdpi.com/2571-712X/8/3/64</link>
	<description>The generation of high-quality mid-infrared free-electron laser (MIR-FEL) radiation depends critically on precise control of electron beam parameters, including energy, energy spread, transverse emittance, bunch charge, and bunch length. At the PBP-CMU Electron Linac Laboratory (PCELL), effective beam diagnostics are essential for optimizing FEL performance. However, dedicated systems for direct measurement of transverse emittance and bunch length at the undulator entrance have been lacking. This paper addresses this gap by presenting the design, simulation, and analysis of diagnostic stations for accurate characterization of these parameters. A two-quadrupole emittance measurement system was developed, enabling independent control of beam-focusing in both transverse planes. An analytical model was formulated specifically for this configuration to enhance emittance reconstruction accuracy. Systematic error analysis was conducted using ASTRA beam dynamics simulations, incorporating 3D field maps from CST Studio Suite and fully including space-charge effects. Results show that transverse emittance values as low as 0.15 mm&amp;amp;middot;mrad can be measured with less than 20% error when the initial RMS beam size is under 2 mm. Additionally, quadrupole misalignment effects were quantified, showing that alignment within &amp;amp;plusmn;0.95 mm limits systematic errors to below 33.3%. For bunch length measurements, a transition radiation (TR) station coupled with a Michelson interferometer was designed. Spectral and interferometric simulations reveal that transverse beam size and beam splitter properties significantly affect measurement accuracy. A 6% error due to transverse size was identified, while Kapton beam splitters introduced additional systematic distortions. In contrast, a 6 mm-thick silicon beam splitter enabled accurate, correction-free measurements. The finite size of the radiator was also found to suppress low-frequency components, resulting in up to 10.6% underestimation of bunch length. This work provides a practical and comprehensive diagnostic framework that accounts for multiple error sources in both transverse emittance and bunch length measurements. These findings contribute valuable insight for the beam diagnostics community and support improved control of beam quality in MIR FEL systems.</description>
	<pubDate>2025-06-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 64: Beam Emittance and Bunch Length Diagnostics for the MIR-FEL Beamline at Chiang Mai University</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/64">doi: 10.3390/particles8030064</a></p>
	<p>Authors:
		Kittipong Techakaew
		Kanlayaporn Kongmali
		Siriwan Pakluea
		Sakhorn Rimjaem
		</p>
	<p>The generation of high-quality mid-infrared free-electron laser (MIR-FEL) radiation depends critically on precise control of electron beam parameters, including energy, energy spread, transverse emittance, bunch charge, and bunch length. At the PBP-CMU Electron Linac Laboratory (PCELL), effective beam diagnostics are essential for optimizing FEL performance. However, dedicated systems for direct measurement of transverse emittance and bunch length at the undulator entrance have been lacking. This paper addresses this gap by presenting the design, simulation, and analysis of diagnostic stations for accurate characterization of these parameters. A two-quadrupole emittance measurement system was developed, enabling independent control of beam-focusing in both transverse planes. An analytical model was formulated specifically for this configuration to enhance emittance reconstruction accuracy. Systematic error analysis was conducted using ASTRA beam dynamics simulations, incorporating 3D field maps from CST Studio Suite and fully including space-charge effects. Results show that transverse emittance values as low as 0.15 mm&amp;amp;middot;mrad can be measured with less than 20% error when the initial RMS beam size is under 2 mm. Additionally, quadrupole misalignment effects were quantified, showing that alignment within &amp;amp;plusmn;0.95 mm limits systematic errors to below 33.3%. For bunch length measurements, a transition radiation (TR) station coupled with a Michelson interferometer was designed. Spectral and interferometric simulations reveal that transverse beam size and beam splitter properties significantly affect measurement accuracy. A 6% error due to transverse size was identified, while Kapton beam splitters introduced additional systematic distortions. In contrast, a 6 mm-thick silicon beam splitter enabled accurate, correction-free measurements. The finite size of the radiator was also found to suppress low-frequency components, resulting in up to 10.6% underestimation of bunch length. This work provides a practical and comprehensive diagnostic framework that accounts for multiple error sources in both transverse emittance and bunch length measurements. These findings contribute valuable insight for the beam diagnostics community and support improved control of beam quality in MIR FEL systems.</p>
	]]></content:encoded>

	<dc:title>Beam Emittance and Bunch Length Diagnostics for the MIR-FEL Beamline at Chiang Mai University</dc:title>
			<dc:creator>Kittipong Techakaew</dc:creator>
			<dc:creator>Kanlayaporn Kongmali</dc:creator>
			<dc:creator>Siriwan Pakluea</dc:creator>
			<dc:creator>Sakhorn Rimjaem</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030064</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-21</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-21</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>64</prism:startingPage>
		<prism:doi>10.3390/particles8030064</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/64</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/3/63">

	<title>Particles, Vol. 8, Pages 63: Porting MADGRAPH to FPGA Using High-Level Synthesis (HLS)</title>
	<link>https://www.mdpi.com/2571-712X/8/3/63</link>
	<description>The escalating demand for data processing in particle physics research has spurred the exploration of novel technologies to enhance the efficiency and speed of calculations. This study presents the development of an implementation of MADGRAPH, a widely used tool in particle collision simulations, to Field Programmable Gate Array (FPGA) using High-Level Synthesis (HLS). This research presents a proof of concept limited to a single, relatively simple process e+e&amp;amp;minus;&amp;amp;rarr;&amp;amp;mu;+&amp;amp;mu;&amp;amp;minus;. The experimental evaluation methodology is described, focusing on performance comparison between traditional CPU implementations, GPU acceleration, and the new FPGA approach. This study describes the complex process of adapting MADGRAPH to FPGA using HLS, focusing on optimizing algorithms for parallel processing. These advancements could enable faster execution of complex simulations, highlighting FPGA&amp;amp;rsquo;s crucial role in advancing particle physics research. The encouraging results obtained in this proof of concept prove potential interest in testing the performance of the FPGA implementation of more complex processes.</description>
	<pubDate>2025-06-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 63: Porting MADGRAPH to FPGA Using High-Level Synthesis (HLS)</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/3/63">doi: 10.3390/particles8030063</a></p>
	<p>Authors:
		Héctor Gutiérrez Arance
		Luca Fiorini
		Alberto Valero Biot
		Francisco Hervás Álvarez
		Santiago Folgueras
		Carlos Vico Villalba
		Pelayo Leguina López
		Arantza Oyanguren Campos
		Valerii Kholoimov
		Volodymyr Svintozelskyi
		Jiahui Zhuo
		</p>
	<p>The escalating demand for data processing in particle physics research has spurred the exploration of novel technologies to enhance the efficiency and speed of calculations. This study presents the development of an implementation of MADGRAPH, a widely used tool in particle collision simulations, to Field Programmable Gate Array (FPGA) using High-Level Synthesis (HLS). This research presents a proof of concept limited to a single, relatively simple process e+e&amp;amp;minus;&amp;amp;rarr;&amp;amp;mu;+&amp;amp;mu;&amp;amp;minus;. The experimental evaluation methodology is described, focusing on performance comparison between traditional CPU implementations, GPU acceleration, and the new FPGA approach. This study describes the complex process of adapting MADGRAPH to FPGA using HLS, focusing on optimizing algorithms for parallel processing. These advancements could enable faster execution of complex simulations, highlighting FPGA&amp;amp;rsquo;s crucial role in advancing particle physics research. The encouraging results obtained in this proof of concept prove potential interest in testing the performance of the FPGA implementation of more complex processes.</p>
	]]></content:encoded>

	<dc:title>Porting MADGRAPH to FPGA Using High-Level Synthesis (HLS)</dc:title>
			<dc:creator>Héctor Gutiérrez Arance</dc:creator>
			<dc:creator>Luca Fiorini</dc:creator>
			<dc:creator>Alberto Valero Biot</dc:creator>
			<dc:creator>Francisco Hervás Álvarez</dc:creator>
			<dc:creator>Santiago Folgueras</dc:creator>
			<dc:creator>Carlos Vico Villalba</dc:creator>
			<dc:creator>Pelayo Leguina López</dc:creator>
			<dc:creator>Arantza Oyanguren Campos</dc:creator>
			<dc:creator>Valerii Kholoimov</dc:creator>
			<dc:creator>Volodymyr Svintozelskyi</dc:creator>
			<dc:creator>Jiahui Zhuo</dc:creator>
		<dc:identifier>doi: 10.3390/particles8030063</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-20</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-20</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>63</prism:startingPage>
		<prism:doi>10.3390/particles8030063</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/3/63</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/62">

	<title>Particles, Vol. 8, Pages 62: Coherent Grating Transition Radiation of a Hollow Relativistic Electron Beam from a Flat 2D Photonic Crystal</title>
	<link>https://www.mdpi.com/2571-712X/8/2/62</link>
	<description>Hollow electron beams are a promising tool for generating coherent radiation in various frequency ranges. Hollow beams have unique properties, including increased stability and the ability to achieve high current densities without significant deterioration of beam quality. This paper presents the results of a theoretical study on coherent grating transition radiation arising during the interaction between a relativistic hollow electron beam and a flat two-dimensional photonic crystal. The radiation field is calculated using the dipole approximation. Theoretical analysis has shown that, under certain conditions, a high degree of radiation coherence can be achieved. The results open up new possibilities for the creation of new sources of coherent terahertz radiation.</description>
	<pubDate>2025-06-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 62: Coherent Grating Transition Radiation of a Hollow Relativistic Electron Beam from a Flat 2D Photonic Crystal</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/62">doi: 10.3390/particles8020062</a></p>
	<p>Authors:
		Daria Yu. Sergeeva
		Alexey A. Tishchenko
		</p>
	<p>Hollow electron beams are a promising tool for generating coherent radiation in various frequency ranges. Hollow beams have unique properties, including increased stability and the ability to achieve high current densities without significant deterioration of beam quality. This paper presents the results of a theoretical study on coherent grating transition radiation arising during the interaction between a relativistic hollow electron beam and a flat two-dimensional photonic crystal. The radiation field is calculated using the dipole approximation. Theoretical analysis has shown that, under certain conditions, a high degree of radiation coherence can be achieved. The results open up new possibilities for the creation of new sources of coherent terahertz radiation.</p>
	]]></content:encoded>

	<dc:title>Coherent Grating Transition Radiation of a Hollow Relativistic Electron Beam from a Flat 2D Photonic Crystal</dc:title>
			<dc:creator>Daria Yu. Sergeeva</dc:creator>
			<dc:creator>Alexey A. Tishchenko</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020062</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-12</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>62</prism:startingPage>
		<prism:doi>10.3390/particles8020062</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/62</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/61">

	<title>Particles, Vol. 8, Pages 61: Nuclear Structure Study Using a Hybrid Approach of Shell Model and Gogny-Type Density Functionals</title>
	<link>https://www.mdpi.com/2571-712X/8/2/61</link>
	<description>Nuclear density functional theory (DFT) is able to reproduce the saturation properties of nuclear matter, as well as properties of finite nuclei. Consequently, the DFT calculations are applicable to nuclei across a wide range of masses on the nuclear chart. The Gogny-type density functional, which is equivalent to the mean-field calculations with finite-range density-dependent effective interactions, is a successful example. In contrast, the shell model (configuration interaction) calculation is a powerful tool to describe nuclear structure, especially spectroscopic properties. The shell model is able to take into account correlations beyond mean-field in a truncated model space. In this work, we report an investigation on sd-shell nuclei and Ca isotopes using a hybrid approach of the shell model and Gogny-type DFT.</description>
	<pubDate>2025-06-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 61: Nuclear Structure Study Using a Hybrid Approach of Shell Model and Gogny-Type Density Functionals</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/61">doi: 10.3390/particles8020061</a></p>
	<p>Authors:
		Kota Yoshinaga
		Noritaka Shimizu
		Takashi Nakatsukasa
		</p>
	<p>Nuclear density functional theory (DFT) is able to reproduce the saturation properties of nuclear matter, as well as properties of finite nuclei. Consequently, the DFT calculations are applicable to nuclei across a wide range of masses on the nuclear chart. The Gogny-type density functional, which is equivalent to the mean-field calculations with finite-range density-dependent effective interactions, is a successful example. In contrast, the shell model (configuration interaction) calculation is a powerful tool to describe nuclear structure, especially spectroscopic properties. The shell model is able to take into account correlations beyond mean-field in a truncated model space. In this work, we report an investigation on sd-shell nuclei and Ca isotopes using a hybrid approach of the shell model and Gogny-type DFT.</p>
	]]></content:encoded>

	<dc:title>Nuclear Structure Study Using a Hybrid Approach of Shell Model and Gogny-Type Density Functionals</dc:title>
			<dc:creator>Kota Yoshinaga</dc:creator>
			<dc:creator>Noritaka Shimizu</dc:creator>
			<dc:creator>Takashi Nakatsukasa</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020061</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-11</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-11</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>61</prism:startingPage>
		<prism:doi>10.3390/particles8020061</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/61</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/60">

	<title>Particles, Vol. 8, Pages 60: Semileptonic and Missing Energy B Decays at Belle II</title>
	<link>https://www.mdpi.com/2571-712X/8/2/60</link>
	<description>The Belle II experiment has collected a 364 fb&amp;amp;minus;1 sample of collisions at the &amp;amp;Upsilon;(4S) resonance. This dataset, with its low particle multiplicity and well-constrained initial state, provides an ideal environment for studying semileptonic and missing energy B decays. In this paper, I will present recent results on these decays, emphasizing their impact on the determination of CKM matrix elements and potential new physics. I will also discuss the techniques used for missing energy reconstruction and the challenges of signal-background discrimination. Future analysis prospects with larger datasets will also be highlighted.</description>
	<pubDate>2025-06-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 60: Semileptonic and Missing Energy B Decays at Belle II</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/60">doi: 10.3390/particles8020060</a></p>
	<p>Authors:
		Giovanni Gaudino
		</p>
	<p>The Belle II experiment has collected a 364 fb&amp;amp;minus;1 sample of collisions at the &amp;amp;Upsilon;(4S) resonance. This dataset, with its low particle multiplicity and well-constrained initial state, provides an ideal environment for studying semileptonic and missing energy B decays. In this paper, I will present recent results on these decays, emphasizing their impact on the determination of CKM matrix elements and potential new physics. I will also discuss the techniques used for missing energy reconstruction and the challenges of signal-background discrimination. Future analysis prospects with larger datasets will also be highlighted.</p>
	]]></content:encoded>

	<dc:title>Semileptonic and Missing Energy B Decays at Belle II</dc:title>
			<dc:creator>Giovanni Gaudino</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020060</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-04</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-04</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>60</prism:startingPage>
		<prism:doi>10.3390/particles8020060</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/60</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/59">

	<title>Particles, Vol. 8, Pages 59: Investigating K/&amp;pi; Decay Muon Yields Using K/&amp;pi; Yields and a Fast Simulation Method</title>
	<link>https://www.mdpi.com/2571-712X/8/2/59</link>
	<description>In ultra-relativistic heavy-ion collisions, the study of muons from kaon (K) and pion (&amp;amp;pi;) decays provides insights into hadron production and propagation in the Quark&amp;amp;ndash;Gluon Plasma (QGP). This paper investigates muon yields from K and &amp;amp;pi; decays in Pb&amp;amp;ndash;Pb collisions at sNN=2.76 TeV using a fast simulation method. We employ a fast Monte Carlo procedure to estimate muon yields from charged kaons and pions. The simulation involves generating pions and kaons with uniform pT and y distributions, simulating their decay kinematics via PYTHIA, and reweighting to match the physical spectra. Our results show the transverse momentum distributions of muons from K and &amp;amp;pi; decays at forward rapidity (2.5&amp;amp;lt;y&amp;amp;lt;4.0) for different centrality classes. The systematic uncertainties are primarily from the mid-rapidity charged K/&amp;amp;pi; spectra and rapidity-dependent RAA uncertainties. The muon yields from pion and kaon decays exhibit consistency across centrality classes in the pT range of 3&amp;amp;ndash;10 GeV/c. This study contributes to understanding hadronic interactions and decay kinematics in heavy-ion collisions, offering references for investigating pion and kaon decay channels and hot medium effects.</description>
	<pubDate>2025-06-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 59: Investigating K/&amp;pi; Decay Muon Yields Using K/&amp;pi; Yields and a Fast Simulation Method</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/59">doi: 10.3390/particles8020059</a></p>
	<p>Authors:
		Zuman Zhang
		Sha Li
		Ning Yu
		Hongge Xu
		Yuanmeng Xiong
		Kun Liu
		</p>
	<p>In ultra-relativistic heavy-ion collisions, the study of muons from kaon (K) and pion (&amp;amp;pi;) decays provides insights into hadron production and propagation in the Quark&amp;amp;ndash;Gluon Plasma (QGP). This paper investigates muon yields from K and &amp;amp;pi; decays in Pb&amp;amp;ndash;Pb collisions at sNN=2.76 TeV using a fast simulation method. We employ a fast Monte Carlo procedure to estimate muon yields from charged kaons and pions. The simulation involves generating pions and kaons with uniform pT and y distributions, simulating their decay kinematics via PYTHIA, and reweighting to match the physical spectra. Our results show the transverse momentum distributions of muons from K and &amp;amp;pi; decays at forward rapidity (2.5&amp;amp;lt;y&amp;amp;lt;4.0) for different centrality classes. The systematic uncertainties are primarily from the mid-rapidity charged K/&amp;amp;pi; spectra and rapidity-dependent RAA uncertainties. The muon yields from pion and kaon decays exhibit consistency across centrality classes in the pT range of 3&amp;amp;ndash;10 GeV/c. This study contributes to understanding hadronic interactions and decay kinematics in heavy-ion collisions, offering references for investigating pion and kaon decay channels and hot medium effects.</p>
	]]></content:encoded>

	<dc:title>Investigating K/&amp;amp;pi; Decay Muon Yields Using K/&amp;amp;pi; Yields and a Fast Simulation Method</dc:title>
			<dc:creator>Zuman Zhang</dc:creator>
			<dc:creator>Sha Li</dc:creator>
			<dc:creator>Ning Yu</dc:creator>
			<dc:creator>Hongge Xu</dc:creator>
			<dc:creator>Yuanmeng Xiong</dc:creator>
			<dc:creator>Kun Liu</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020059</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-06-03</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-06-03</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>59</prism:startingPage>
		<prism:doi>10.3390/particles8020059</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/59</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/58">

	<title>Particles, Vol. 8, Pages 58: Hadron Identification Prospects with Granular Calorimeters</title>
	<link>https://www.mdpi.com/2571-712X/8/2/58</link>
	<description>In this work we consider the problem of determining the identity of hadrons at high energies based on the topology of their energy depositions in dense matter, along with the time of the interactions. Using GEANT4 simulations of a homogeneous lead tungstate calorimeter with high transverse and longitudinal segmentation, we investigated the discrimination of protons, positive pions, and positive kaons at 100 GeV. The analysis focuses on the impact of calorimeter granularity by progressively merging detector cells and extracting features like energy deposition patterns and timing information. Two machine learning approaches, XGBoost and fully connected deep neural networks, were employed to assess the classification performance across particle pairs. The results indicate that fine segmentation improves particle discrimination, with higher granularity yielding more detailed characterization of energy showers. Additionally, the results highlight the importance of shower radius, energy fractions, and timing variables in distinguishing particle types. The XGBoost model demonstrated computational efficiency and interpretability advantages over deep learning for tabular data structures, while achieving similar classification performance. This motivates further work required to combine high- and low-level feature analysis, e.g., using convolutional and graph-based neural networks, and extending the study to a broader range of particle energies and types.</description>
	<pubDate>2025-05-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 58: Hadron Identification Prospects with Granular Calorimeters</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/58">doi: 10.3390/particles8020058</a></p>
	<p>Authors:
		Andrea De Vita
		 Abhishek
		Max Aehle
		Muhammad Awais
		Alessandro Breccia
		Riccardo Carroccio
		Long Chen
		Tommaso Dorigo
		Nicolas R. Gauger
		Ralf Keidel
		Jan Kieseler
		Enrico Lupi
		Federico Nardi
		Xuan Tung Nguyen
		Fredrik Sandin
		Kylian Schmidt
		Pietro Vischia
		Joseph Willmore
		</p>
	<p>In this work we consider the problem of determining the identity of hadrons at high energies based on the topology of their energy depositions in dense matter, along with the time of the interactions. Using GEANT4 simulations of a homogeneous lead tungstate calorimeter with high transverse and longitudinal segmentation, we investigated the discrimination of protons, positive pions, and positive kaons at 100 GeV. The analysis focuses on the impact of calorimeter granularity by progressively merging detector cells and extracting features like energy deposition patterns and timing information. Two machine learning approaches, XGBoost and fully connected deep neural networks, were employed to assess the classification performance across particle pairs. The results indicate that fine segmentation improves particle discrimination, with higher granularity yielding more detailed characterization of energy showers. Additionally, the results highlight the importance of shower radius, energy fractions, and timing variables in distinguishing particle types. The XGBoost model demonstrated computational efficiency and interpretability advantages over deep learning for tabular data structures, while achieving similar classification performance. This motivates further work required to combine high- and low-level feature analysis, e.g., using convolutional and graph-based neural networks, and extending the study to a broader range of particle energies and types.</p>
	]]></content:encoded>

	<dc:title>Hadron Identification Prospects with Granular Calorimeters</dc:title>
			<dc:creator>Andrea De Vita</dc:creator>
			<dc:creator> Abhishek</dc:creator>
			<dc:creator>Max Aehle</dc:creator>
			<dc:creator>Muhammad Awais</dc:creator>
			<dc:creator>Alessandro Breccia</dc:creator>
			<dc:creator>Riccardo Carroccio</dc:creator>
			<dc:creator>Long Chen</dc:creator>
			<dc:creator>Tommaso Dorigo</dc:creator>
			<dc:creator>Nicolas R. Gauger</dc:creator>
			<dc:creator>Ralf Keidel</dc:creator>
			<dc:creator>Jan Kieseler</dc:creator>
			<dc:creator>Enrico Lupi</dc:creator>
			<dc:creator>Federico Nardi</dc:creator>
			<dc:creator>Xuan Tung Nguyen</dc:creator>
			<dc:creator>Fredrik Sandin</dc:creator>
			<dc:creator>Kylian Schmidt</dc:creator>
			<dc:creator>Pietro Vischia</dc:creator>
			<dc:creator>Joseph Willmore</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020058</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-05-16</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-05-16</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>58</prism:startingPage>
		<prism:doi>10.3390/particles8020058</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/58</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/57">

	<title>Particles, Vol. 8, Pages 57: Masses and Quadrupole Deformations of Even-Z Nuclei Within a Triaxial Relativistic Hartree&amp;ndash;Bogoliubov Model</title>
	<link>https://www.mdpi.com/2571-712X/8/2/57</link>
	<description>This study investigates the masses and quadrupole deformations of even-Z nuclei within the range 8&amp;amp;#10877;Z&amp;amp;#10877;104 using the triaxial relativistic Hartree&amp;amp;ndash;Bogoliubov model (TRHB) with the PC-PK1 density functional. For odd-mass nuclei, the global minima were determined using the automatic blocking method and their dynamical correlation energies (DCEs) were approximated using the average values of neighboring even&amp;amp;ndash;even nuclei calculated from a microscopic, five-dimensional, collective Hamiltonian (5DCH). The mean-field results underestimate the binding energies of most open-shell nuclei, with an initial root&amp;amp;ndash;mean&amp;amp;ndash;square (rms) deviation of 2.56 MeV for 1223 even-Z nuclei. Incorporating DCEs significantly reduces this deviation to 1.36 MeV. Additionally, the descriptions of two-neutron and one-neutron separation energies are improved, with rms deviations decreasing to 0.75 MeV and 0.65 MeV, respectively. Further refinement through accounting for odd&amp;amp;ndash;even differences in DCEs reduces the rms deviations for binding energies and one-neutron separation energies to 1.30 MeV and 0.63 MeV, respectively. Regarding the quadrupole deformations, TRHB calculations reveal spherical shapes near shell and subshell closures, well-deformed shapes at the mid-shell, and rapid shape transitions in medium- and heavy-mass regions. Oblate shapes dominate in regions (Z,N)&amp;amp;sim;(14,14),(34,36), and (40,60), and the neutron-deficient Pb region, with notable odd&amp;amp;ndash;even shape staggering attributed to the blocking effect of the odd nucleon. Triaxial shapes are favored in the mass regions (Z,N)&amp;amp;sim;(60,76) and (76,116).</description>
	<pubDate>2025-05-09</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 57: Masses and Quadrupole Deformations of Even-Z Nuclei Within a Triaxial Relativistic Hartree&amp;ndash;Bogoliubov Model</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/57">doi: 10.3390/particles8020057</a></p>
	<p>Authors:
		Qin Zhou
		Zhipan Li
		</p>
	<p>This study investigates the masses and quadrupole deformations of even-Z nuclei within the range 8&amp;amp;#10877;Z&amp;amp;#10877;104 using the triaxial relativistic Hartree&amp;amp;ndash;Bogoliubov model (TRHB) with the PC-PK1 density functional. For odd-mass nuclei, the global minima were determined using the automatic blocking method and their dynamical correlation energies (DCEs) were approximated using the average values of neighboring even&amp;amp;ndash;even nuclei calculated from a microscopic, five-dimensional, collective Hamiltonian (5DCH). The mean-field results underestimate the binding energies of most open-shell nuclei, with an initial root&amp;amp;ndash;mean&amp;amp;ndash;square (rms) deviation of 2.56 MeV for 1223 even-Z nuclei. Incorporating DCEs significantly reduces this deviation to 1.36 MeV. Additionally, the descriptions of two-neutron and one-neutron separation energies are improved, with rms deviations decreasing to 0.75 MeV and 0.65 MeV, respectively. Further refinement through accounting for odd&amp;amp;ndash;even differences in DCEs reduces the rms deviations for binding energies and one-neutron separation energies to 1.30 MeV and 0.63 MeV, respectively. Regarding the quadrupole deformations, TRHB calculations reveal spherical shapes near shell and subshell closures, well-deformed shapes at the mid-shell, and rapid shape transitions in medium- and heavy-mass regions. Oblate shapes dominate in regions (Z,N)&amp;amp;sim;(14,14),(34,36), and (40,60), and the neutron-deficient Pb region, with notable odd&amp;amp;ndash;even shape staggering attributed to the blocking effect of the odd nucleon. Triaxial shapes are favored in the mass regions (Z,N)&amp;amp;sim;(60,76) and (76,116).</p>
	]]></content:encoded>

	<dc:title>Masses and Quadrupole Deformations of Even-Z Nuclei Within a Triaxial Relativistic Hartree&amp;amp;ndash;Bogoliubov Model</dc:title>
			<dc:creator>Qin Zhou</dc:creator>
			<dc:creator>Zhipan Li</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020057</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-05-09</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-05-09</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>57</prism:startingPage>
		<prism:doi>10.3390/particles8020057</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/57</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/56">

	<title>Particles, Vol. 8, Pages 56: Beta Decay Properties of Waiting-Point N = 50 and 82 Isotopes</title>
	<link>https://www.mdpi.com/2571-712X/8/2/56</link>
	<description>We performed the microscopic calculation of &amp;amp;beta;-decay properties for waiting-point nuclei with neutron-closed magic shells. Allowed Gamow&amp;amp;ndash;Teller (GT) and first-forbidden (FF) transitions were simulated using a schematic model (SM) for waiting-point N = 50,82 isotopes in the framework of a proton&amp;amp;ndash;neutron quasiparticle random phase approximation (pn-QRPA). The Woods&amp;amp;ndash;Saxon (WS) potential basis was used in our calculations. The pn-QRPA equations of allowed (GT) and (FF) transitions were utilized in both the particle&amp;amp;ndash;hole (ph) and particle&amp;amp;ndash;particle (pp) channels in the SM. We solved the secular equations of the GT and FF transitions for eigenvalues and eigenfunctions of the corresponding Hamiltonians. A spherical shape was assigned to each waiting-point nucleus in all simulations. Significantly, this study marks the first time that &amp;amp;beta;-decay analysis has been applied to certain nuclei, including 82Ge50, 83As50, 84Se50, 85Br50 and 87Rb50 with N=50 isotones, and 132Sn82, 133Sb82, 134Te82, 135I82 and 137Cs82 with N=82 isotones. Since there is no prior theoretical research on these nuclei, this work is a unique addition to the field. We compared our results with the previous calculations and measured data, and our calculations agree with the experimental data and the other theoretical results.</description>
	<pubDate>2025-05-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 56: Beta Decay Properties of Waiting-Point N = 50 and 82 Isotopes</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/56">doi: 10.3390/particles8020056</a></p>
	<p>Authors:
		Necla Çakmak
		Najm Abdullah Saleh
		</p>
	<p>We performed the microscopic calculation of &amp;amp;beta;-decay properties for waiting-point nuclei with neutron-closed magic shells. Allowed Gamow&amp;amp;ndash;Teller (GT) and first-forbidden (FF) transitions were simulated using a schematic model (SM) for waiting-point N = 50,82 isotopes in the framework of a proton&amp;amp;ndash;neutron quasiparticle random phase approximation (pn-QRPA). The Woods&amp;amp;ndash;Saxon (WS) potential basis was used in our calculations. The pn-QRPA equations of allowed (GT) and (FF) transitions were utilized in both the particle&amp;amp;ndash;hole (ph) and particle&amp;amp;ndash;particle (pp) channels in the SM. We solved the secular equations of the GT and FF transitions for eigenvalues and eigenfunctions of the corresponding Hamiltonians. A spherical shape was assigned to each waiting-point nucleus in all simulations. Significantly, this study marks the first time that &amp;amp;beta;-decay analysis has been applied to certain nuclei, including 82Ge50, 83As50, 84Se50, 85Br50 and 87Rb50 with N=50 isotones, and 132Sn82, 133Sb82, 134Te82, 135I82 and 137Cs82 with N=82 isotones. Since there is no prior theoretical research on these nuclei, this work is a unique addition to the field. We compared our results with the previous calculations and measured data, and our calculations agree with the experimental data and the other theoretical results.</p>
	]]></content:encoded>

	<dc:title>Beta Decay Properties of Waiting-Point N = 50 and 82 Isotopes</dc:title>
			<dc:creator>Necla Çakmak</dc:creator>
			<dc:creator>Najm Abdullah Saleh</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020056</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-05-06</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-05-06</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>56</prism:startingPage>
		<prism:doi>10.3390/particles8020056</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/56</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/55">

	<title>Particles, Vol. 8, Pages 55: Chiral Effects in Hydrodynamics: New Trends</title>
	<link>https://www.mdpi.com/2571-712X/8/2/55</link>
	<description>By chiral effects, one understands the manifestations of chiral gauge anomaly and of gravitational chiral anomaly in hydrodynamics. In the last two to three years, our understanding of chiral effects has considerably changed. Here, we present a mini-review of two topics: first, a shift in understanding symmetry, which underlies the chiral magnetic effect and second, the interpretation of the chiral kinematical effect uncovered recently.</description>
	<pubDate>2025-05-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 55: Chiral Effects in Hydrodynamics: New Trends</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/55">doi: 10.3390/particles8020055</a></p>
	<p>Authors:
		Valentin Zakharov
		Oleg Teryaev
		Georgy Prokhorov
		</p>
	<p>By chiral effects, one understands the manifestations of chiral gauge anomaly and of gravitational chiral anomaly in hydrodynamics. In the last two to three years, our understanding of chiral effects has considerably changed. Here, we present a mini-review of two topics: first, a shift in understanding symmetry, which underlies the chiral magnetic effect and second, the interpretation of the chiral kinematical effect uncovered recently.</p>
	]]></content:encoded>

	<dc:title>Chiral Effects in Hydrodynamics: New Trends</dc:title>
			<dc:creator>Valentin Zakharov</dc:creator>
			<dc:creator>Oleg Teryaev</dc:creator>
			<dc:creator>Georgy Prokhorov</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020055</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-05-02</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-05-02</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>55</prism:startingPage>
		<prism:doi>10.3390/particles8020055</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/55</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2571-712X/8/2/54">

	<title>Particles, Vol. 8, Pages 54: Production Optimization of Exotic Hypernuclei via Heavy-Ion Beams at GSI-FAIR</title>
	<link>https://www.mdpi.com/2571-712X/8/2/54</link>
	<description>Building on the successful demonstration of hypernuclear spectroscopy using heavy-ion beams, the HypHI Collaboration is shifting its focus to investigating proton- and neutron-rich hypernuclei. A crucial component of this research is the implementation of a fragment separator, which facilitates the production and separation of rare isotope beams and is vital for accessing hypernuclei far from the stability line. High-precision spectroscopy of these exotic hypernuclei is planned to be conducted at GSI first, which will be followed by experiments at the FAIR facility utilizing the FRS and Super-FRS fragment separators. A thorough systematic investigation paired with an optimization analysis was employed to establish the most favorable experimental setup for producing high-isospin hypernuclei. Theoretical models describing heavy-ion-induced reactions and hypernuclear synthesis guided this process, which was complemented by Monte Carlo simulations to obtain experimental efficiencies for the production and transmission of the exotic secondary beams. The outlined methodology offers insights into the anticipated yields of He&amp;amp;Lambda;6, C&amp;amp;Lambda;9, and a range of both proton- and neutron-rich hypernuclei.</description>
	<pubDate>2025-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Particles, Vol. 8, Pages 54: Production Optimization of Exotic Hypernuclei via Heavy-Ion Beams at GSI-FAIR</b></p>
	<p>Particles <a href="https://www.mdpi.com/2571-712X/8/2/54">doi: 10.3390/particles8020054</a></p>
	<p>Authors:
		Samuel Escrig
		Christophe Rappold
		</p>
	<p>Building on the successful demonstration of hypernuclear spectroscopy using heavy-ion beams, the HypHI Collaboration is shifting its focus to investigating proton- and neutron-rich hypernuclei. A crucial component of this research is the implementation of a fragment separator, which facilitates the production and separation of rare isotope beams and is vital for accessing hypernuclei far from the stability line. High-precision spectroscopy of these exotic hypernuclei is planned to be conducted at GSI first, which will be followed by experiments at the FAIR facility utilizing the FRS and Super-FRS fragment separators. A thorough systematic investigation paired with an optimization analysis was employed to establish the most favorable experimental setup for producing high-isospin hypernuclei. Theoretical models describing heavy-ion-induced reactions and hypernuclear synthesis guided this process, which was complemented by Monte Carlo simulations to obtain experimental efficiencies for the production and transmission of the exotic secondary beams. The outlined methodology offers insights into the anticipated yields of He&amp;amp;Lambda;6, C&amp;amp;Lambda;9, and a range of both proton- and neutron-rich hypernuclei.</p>
	]]></content:encoded>

	<dc:title>Production Optimization of Exotic Hypernuclei via Heavy-Ion Beams at GSI-FAIR</dc:title>
			<dc:creator>Samuel Escrig</dc:creator>
			<dc:creator>Christophe Rappold</dc:creator>
		<dc:identifier>doi: 10.3390/particles8020054</dc:identifier>
	<dc:source>Particles</dc:source>
	<dc:date>2025-05-01</dc:date>

	<prism:publicationName>Particles</prism:publicationName>
	<prism:publicationDate>2025-05-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>54</prism:startingPage>
		<prism:doi>10.3390/particles8020054</prism:doi>
	<prism:url>https://www.mdpi.com/2571-712X/8/2/54</prism:url>
	
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</item>
    
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