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	<title>Quantum Reports, Vol. 8, Pages 46: A Hybrid Quantum-Classical Framework for Saliency-Aware Medical Image Encoding</title>
	<link>https://www.mdpi.com/2624-960X/8/2/46</link>
	<description>Quantum image processing provides significant storage benefits over classical methods. However, current quantum image representation techniques exhibit limitations regarding encoding efficiency, circuit complexity, and adaptability to image content. This paper proposes Saliency-Aware Hybrid Quantum Image Representation (SAHQR), utilizing saliency detection for content-adaptive representation. It selectively focuses on salient regions, allocating quantum resources proportionally to visual importance, whereas existing techniques represent all regions uniformly.The proposed approach is evaluated against ten state-of-the-art quantum image representation techniques using ten criteria: number of qubits, circuit depth, gate complexity, encoding time, scalability, information loss, compression ratio, memory overhead, and implementation complexity Experimental results on 6097 medical images from the MINC database demonstrate that this work should be interpreted as a proof of concept for saliency-aware quantum encoding, rather than as a universally optimal representation.The evaluation is extended to 2000 Synthetic Aperture Radar (SAR) tiles and 2298 Brain Tumor MRI scans to validate cross-domain generalization. Statistical significance tests (p &amp;amp;lt; 0.001) confirm SAHQR yields statistically significant improvements over existing techniques across all three domains.</description>
	<pubDate>2026-05-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 46: A Hybrid Quantum-Classical Framework for Saliency-Aware Medical Image Encoding</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/46">doi: 10.3390/quantum8020046</a></p>
	<p>Authors:
		Vrushali Nikam
		Trupti Atre
		Lavanya Santhosh
		Asha K N
		Praveena M V
		</p>
	<p>Quantum image processing provides significant storage benefits over classical methods. However, current quantum image representation techniques exhibit limitations regarding encoding efficiency, circuit complexity, and adaptability to image content. This paper proposes Saliency-Aware Hybrid Quantum Image Representation (SAHQR), utilizing saliency detection for content-adaptive representation. It selectively focuses on salient regions, allocating quantum resources proportionally to visual importance, whereas existing techniques represent all regions uniformly.The proposed approach is evaluated against ten state-of-the-art quantum image representation techniques using ten criteria: number of qubits, circuit depth, gate complexity, encoding time, scalability, information loss, compression ratio, memory overhead, and implementation complexity Experimental results on 6097 medical images from the MINC database demonstrate that this work should be interpreted as a proof of concept for saliency-aware quantum encoding, rather than as a universally optimal representation.The evaluation is extended to 2000 Synthetic Aperture Radar (SAR) tiles and 2298 Brain Tumor MRI scans to validate cross-domain generalization. Statistical significance tests (p &amp;amp;lt; 0.001) confirm SAHQR yields statistically significant improvements over existing techniques across all three domains.</p>
	]]></content:encoded>

	<dc:title>A Hybrid Quantum-Classical Framework for Saliency-Aware Medical Image Encoding</dc:title>
			<dc:creator>Vrushali Nikam</dc:creator>
			<dc:creator>Trupti Atre</dc:creator>
			<dc:creator>Lavanya Santhosh</dc:creator>
			<dc:creator>Asha K N</dc:creator>
			<dc:creator>Praveena M V</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020046</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-07</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-07</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>46</prism:startingPage>
		<prism:doi>10.3390/quantum8020046</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/46</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/45">

	<title>Quantum Reports, Vol. 8, Pages 45: A Two-Step Quantum Approximate Optimization Algorithm for Portfolio Optimization and Risk Assessment</title>
	<link>https://www.mdpi.com/2624-960X/8/2/45</link>
	<description>Quantum finance represents a pivotal and cutting-edge application domain within the burgeoning field of quantum computing. In this work, we propose a two-step quantum approximate optimization algorithm (two-step QAOA) for portfolio optimization and risk assessment. The algorithm initiates by formulating the stock selection problem as a quadratic unconstrained binary optimization (QUBO) problem and employs a classical-quantum hybrid method to find the ground state of the Hamiltonian. We then introduce an energy-based characteristic indicator U&amp;amp;isin;[0,1), which quantitatively evaluates portfolio performance under customizable investment preferences, effectively capturing the trade-off between expected return and risk. The number of qubits required scales with the number of stocks N in the pool, and the number of Hamiltonian terms is O(N2). Numerical simulations show that the algorithm provides consistent and reasonable assessment results on both training and test datasets under different investment preferences (aggressive or conservative), validating the capability of the characteristic indicator to extract intrinsic information from the portfolios. Additionally, by incorporating warm-starting and digitized counterdiabatic techniques, the algorithm achieves improved scalability and faster convergence. Our work presents a flexible and practical algorithmic framework for applying quantum computing in the financial domain.</description>
	<pubDate>2026-05-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 45: A Two-Step Quantum Approximate Optimization Algorithm for Portfolio Optimization and Risk Assessment</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/45">doi: 10.3390/quantum8020045</a></p>
	<p>Authors:
		Boxuan Wu
		Lei Wang
		</p>
	<p>Quantum finance represents a pivotal and cutting-edge application domain within the burgeoning field of quantum computing. In this work, we propose a two-step quantum approximate optimization algorithm (two-step QAOA) for portfolio optimization and risk assessment. The algorithm initiates by formulating the stock selection problem as a quadratic unconstrained binary optimization (QUBO) problem and employs a classical-quantum hybrid method to find the ground state of the Hamiltonian. We then introduce an energy-based characteristic indicator U&amp;amp;isin;[0,1), which quantitatively evaluates portfolio performance under customizable investment preferences, effectively capturing the trade-off between expected return and risk. The number of qubits required scales with the number of stocks N in the pool, and the number of Hamiltonian terms is O(N2). Numerical simulations show that the algorithm provides consistent and reasonable assessment results on both training and test datasets under different investment preferences (aggressive or conservative), validating the capability of the characteristic indicator to extract intrinsic information from the portfolios. Additionally, by incorporating warm-starting and digitized counterdiabatic techniques, the algorithm achieves improved scalability and faster convergence. Our work presents a flexible and practical algorithmic framework for applying quantum computing in the financial domain.</p>
	]]></content:encoded>

	<dc:title>A Two-Step Quantum Approximate Optimization Algorithm for Portfolio Optimization and Risk Assessment</dc:title>
			<dc:creator>Boxuan Wu</dc:creator>
			<dc:creator>Lei Wang</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020045</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-07</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-07</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>45</prism:startingPage>
		<prism:doi>10.3390/quantum8020045</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/45</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/44">

	<title>Quantum Reports, Vol. 8, Pages 44: Breakdown of Bell Factorization from Non-Injective Effective Descriptions</title>
	<link>https://www.mdpi.com/2624-960X/8/2/44</link>
	<description>Violations of Bell inequalities are commonly interpreted as evidence for nonlocal influences or as constraints on realist descriptions. We show that the failure of Bell-type factorizability arises naturally when observable outcomes are obtained through a non-injective mapping from an underlying configuration space. In this setting, the standard factorization assumption can be viewed as an implicit requirement that observable variables admit a jointly factorizable completion at the underlying level. We demonstrate that this requirement need not hold when the mapping from underlying configurations to observables is many-to-one. The resulting breakdown of probabilistic factorization does not rely on superluminal dynamics or hidden causal influences, but follows from information loss under projection. Observable outcomes correspond to equivalence classes of underlying configurations, preventing the assignment of independent local variables. We illustrate this mechanism with an explicit toy model producing Bell&amp;amp;ndash;CHSH violations while preserving operational no-signalling and statistical independence of measurement settings. The model is not intended to reproduce quantum correlations quantitatively, and may exceed the Tsirelson bound; its role is to isolate the structural origin of the violation. This analysis does not contradict Bell&amp;amp;rsquo;s theorem, but identifies a class of effective descriptions for which its factorizability assumption does not apply. The framework preserves locality at the underlying level, introduces no additional hidden-variable dynamics, and does not modify quantum mechanics. It clarifies how classical factorization is recovered in regimes where the effective mapping becomes approximately injective. In the operator language of quantum theory, the same mechanism admits a natural reformulation in terms of reduction to an effective observable subalgebra by a noncommutative conditional expectation.</description>
	<pubDate>2026-05-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 44: Breakdown of Bell Factorization from Non-Injective Effective Descriptions</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/44">doi: 10.3390/quantum8020044</a></p>
	<p>Authors:
		Jérôme Beau
		</p>
	<p>Violations of Bell inequalities are commonly interpreted as evidence for nonlocal influences or as constraints on realist descriptions. We show that the failure of Bell-type factorizability arises naturally when observable outcomes are obtained through a non-injective mapping from an underlying configuration space. In this setting, the standard factorization assumption can be viewed as an implicit requirement that observable variables admit a jointly factorizable completion at the underlying level. We demonstrate that this requirement need not hold when the mapping from underlying configurations to observables is many-to-one. The resulting breakdown of probabilistic factorization does not rely on superluminal dynamics or hidden causal influences, but follows from information loss under projection. Observable outcomes correspond to equivalence classes of underlying configurations, preventing the assignment of independent local variables. We illustrate this mechanism with an explicit toy model producing Bell&amp;amp;ndash;CHSH violations while preserving operational no-signalling and statistical independence of measurement settings. The model is not intended to reproduce quantum correlations quantitatively, and may exceed the Tsirelson bound; its role is to isolate the structural origin of the violation. This analysis does not contradict Bell&amp;amp;rsquo;s theorem, but identifies a class of effective descriptions for which its factorizability assumption does not apply. The framework preserves locality at the underlying level, introduces no additional hidden-variable dynamics, and does not modify quantum mechanics. It clarifies how classical factorization is recovered in regimes where the effective mapping becomes approximately injective. In the operator language of quantum theory, the same mechanism admits a natural reformulation in terms of reduction to an effective observable subalgebra by a noncommutative conditional expectation.</p>
	]]></content:encoded>

	<dc:title>Breakdown of Bell Factorization from Non-Injective Effective Descriptions</dc:title>
			<dc:creator>Jérôme Beau</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020044</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-02</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-02</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>44</prism:startingPage>
		<prism:doi>10.3390/quantum8020044</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/44</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/43">

	<title>Quantum Reports, Vol. 8, Pages 43: Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes</title>
	<link>https://www.mdpi.com/2624-960X/8/2/43</link>
	<description>We analyze noise in a quantum-enhanced fiber optic gyroscope (FOG), focusing on one of the leading sources of phase uncertainty&amp;amp;mdash;uncorrelated photon saturation. Taking a squeezed state input as a source for N00N states, we compute the uncorrelated false coincidence counts at the optimal phase bias and determine an upper limit to the squeezed amplitude &amp;amp;xi; which allows for sub-shot noise precision. As examples, we apply parameters of present-day quantum FOG experiments and determine the maximum possible precision enhancement based on their respective &amp;amp;xi; and optimal phase bias points. With the aim of supporting future FOG setups with higher N00N state fluxes, our result highlights the need to transition to multimode states to bypass the &amp;amp;xi; limitation, such as photon pairs generated by the dynamical Casimir effect.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 43: Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/43">doi: 10.3390/quantum8020043</a></p>
	<p>Authors:
		Stefan Evans
		Joanna N. Ptasinski
		</p>
	<p>We analyze noise in a quantum-enhanced fiber optic gyroscope (FOG), focusing on one of the leading sources of phase uncertainty&amp;amp;mdash;uncorrelated photon saturation. Taking a squeezed state input as a source for N00N states, we compute the uncorrelated false coincidence counts at the optimal phase bias and determine an upper limit to the squeezed amplitude &amp;amp;xi; which allows for sub-shot noise precision. As examples, we apply parameters of present-day quantum FOG experiments and determine the maximum possible precision enhancement based on their respective &amp;amp;xi; and optimal phase bias points. With the aim of supporting future FOG setups with higher N00N state fluxes, our result highlights the need to transition to multimode states to bypass the &amp;amp;xi; limitation, such as photon pairs generated by the dynamical Casimir effect.</p>
	]]></content:encoded>

	<dc:title>Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes</dc:title>
			<dc:creator>Stefan Evans</dc:creator>
			<dc:creator>Joanna N. Ptasinski</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020043</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>43</prism:startingPage>
		<prism:doi>10.3390/quantum8020043</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/43</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/42">

	<title>Quantum Reports, Vol. 8, Pages 42: Many Body in General Relativity: A Thermal Equivalence Principle</title>
	<link>https://www.mdpi.com/2624-960X/8/2/42</link>
	<description>In this paper, we review the physics of many bodies in the context of general relativity. Starting from the stress&amp;amp;ndash;energy tensor for one body and moving onto those for a swarm of bodies and for a perfect fluid, we review the relativistic hydrodynamics, kinetic theory, and statistical physics of N identical bodies. We conclude our excursion with a thermal equivalence principle in physics.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 42: Many Body in General Relativity: A Thermal Equivalence Principle</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/42">doi: 10.3390/quantum8020042</a></p>
	<p>Authors:
		Riccardo Fantoni
		</p>
	<p>In this paper, we review the physics of many bodies in the context of general relativity. Starting from the stress&amp;amp;ndash;energy tensor for one body and moving onto those for a swarm of bodies and for a perfect fluid, we review the relativistic hydrodynamics, kinetic theory, and statistical physics of N identical bodies. We conclude our excursion with a thermal equivalence principle in physics.</p>
	]]></content:encoded>

	<dc:title>Many Body in General Relativity: A Thermal Equivalence Principle</dc:title>
			<dc:creator>Riccardo Fantoni</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020042</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>42</prism:startingPage>
		<prism:doi>10.3390/quantum8020042</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/42</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/41">

	<title>Quantum Reports, Vol. 8, Pages 41: Verifying Quantum Network Nonlocality Based on the Extended Mermin Inequality</title>
	<link>https://www.mdpi.com/2624-960X/8/2/41</link>
	<description>This work proposes an extended Mermin inequality based on a hybrid classical model that involves only one classical source, with the remaining sources being post-quantum. In a chain-structured quantum network consisting of hybrid Einstein&amp;amp;ndash;Podolsky&amp;amp;ndash;Rosen (EPR) pairs and Greenberger&amp;amp;ndash;Horne&amp;amp;ndash;Zeilinger (GHZ) states, joint measurements are performed at the central node, while local measurements are conducted at the peripheral nodes. This setup shows that the obtained quantum correlations can violate the proposed inequality with fewer measurement settings, thereby verifying network nonlocality. Furthermore, we extend this method to chain networks of arbitrary length n and show that the proposed inequality remains effective in verifying network nonlocality.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 41: Verifying Quantum Network Nonlocality Based on the Extended Mermin Inequality</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/41">doi: 10.3390/quantum8020041</a></p>
	<p>Authors:
		Xinyue Li
		Yan-Han Yang
		Ming-Xing Luo
		</p>
	<p>This work proposes an extended Mermin inequality based on a hybrid classical model that involves only one classical source, with the remaining sources being post-quantum. In a chain-structured quantum network consisting of hybrid Einstein&amp;amp;ndash;Podolsky&amp;amp;ndash;Rosen (EPR) pairs and Greenberger&amp;amp;ndash;Horne&amp;amp;ndash;Zeilinger (GHZ) states, joint measurements are performed at the central node, while local measurements are conducted at the peripheral nodes. This setup shows that the obtained quantum correlations can violate the proposed inequality with fewer measurement settings, thereby verifying network nonlocality. Furthermore, we extend this method to chain networks of arbitrary length n and show that the proposed inequality remains effective in verifying network nonlocality.</p>
	]]></content:encoded>

	<dc:title>Verifying Quantum Network Nonlocality Based on the Extended Mermin Inequality</dc:title>
			<dc:creator>Xinyue Li</dc:creator>
			<dc:creator>Yan-Han Yang</dc:creator>
			<dc:creator>Ming-Xing Luo</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020041</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>41</prism:startingPage>
		<prism:doi>10.3390/quantum8020041</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/41</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/40">

	<title>Quantum Reports, Vol. 8, Pages 40: Ultrafast Helicity-Controlled Spin Dynamics in Curved Time: A Photonic Pathway to Geometry-Driven Spin Transport</title>
	<link>https://www.mdpi.com/2624-960X/8/2/40</link>
	<description>Controlling spin dynamics conventionally requires external magnetic fields, strong electric bias, or material-specific spin&amp;amp;ndash;orbit interactions, while the temporal reference frame remains fixed. Here we introduce curved-time spintronics, a framework in which a synthetic lapse field, implemented through GHz surface-acoustic-wave (SAW) modulation, reshapes the effective flow of time experienced by spinor, magnonic, and photon&amp;amp;ndash;spin degrees of freedom. Using a curved-time Schr&amp;amp;ouml;dinger&amp;amp;ndash;Pauli model, we show that it renormalizes the Larmor frequency, modifies SOC-driven splittings, and produces helicity-dependent spin precession under circularly polarized excitation. Strikingly, a spatial lapse gradient induces a Hall-like transverse drift even when in the absence of any external electric field or intrinsic Berry curvature, demonstrating that time geometry alone can generate transverse transport. Time-domain simulations confirm curvature-driven Hall response across graphene, carbon nanotubes, and generic Dirac platforms, establishing a material-agnostic, field-free mechanism for transverse spin manipulation. We further predict curvature-dependent spin diffusion, temporal magnon focusing, and helicity-selective entanglement generation, and propose pump&amp;amp;ndash;probe detection via ultrafast Kerr rotation synchronized to SAW-driven lapse modulation. These results position engineered time geometry as a new spintronic control axis, enabling Hall-like effects, spin transport, and chiral phase manipulation without relying on intrinsic material properties, magnetic fields, or electric gating.</description>
	<pubDate>2026-05-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 40: Ultrafast Helicity-Controlled Spin Dynamics in Curved Time: A Photonic Pathway to Geometry-Driven Spin Transport</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/40">doi: 10.3390/quantum8020040</a></p>
	<p>Authors:
		Mohammad Mohammadiaria
		</p>
	<p>Controlling spin dynamics conventionally requires external magnetic fields, strong electric bias, or material-specific spin&amp;amp;ndash;orbit interactions, while the temporal reference frame remains fixed. Here we introduce curved-time spintronics, a framework in which a synthetic lapse field, implemented through GHz surface-acoustic-wave (SAW) modulation, reshapes the effective flow of time experienced by spinor, magnonic, and photon&amp;amp;ndash;spin degrees of freedom. Using a curved-time Schr&amp;amp;ouml;dinger&amp;amp;ndash;Pauli model, we show that it renormalizes the Larmor frequency, modifies SOC-driven splittings, and produces helicity-dependent spin precession under circularly polarized excitation. Strikingly, a spatial lapse gradient induces a Hall-like transverse drift even when in the absence of any external electric field or intrinsic Berry curvature, demonstrating that time geometry alone can generate transverse transport. Time-domain simulations confirm curvature-driven Hall response across graphene, carbon nanotubes, and generic Dirac platforms, establishing a material-agnostic, field-free mechanism for transverse spin manipulation. We further predict curvature-dependent spin diffusion, temporal magnon focusing, and helicity-selective entanglement generation, and propose pump&amp;amp;ndash;probe detection via ultrafast Kerr rotation synchronized to SAW-driven lapse modulation. These results position engineered time geometry as a new spintronic control axis, enabling Hall-like effects, spin transport, and chiral phase manipulation without relying on intrinsic material properties, magnetic fields, or electric gating.</p>
	]]></content:encoded>

	<dc:title>Ultrafast Helicity-Controlled Spin Dynamics in Curved Time: A Photonic Pathway to Geometry-Driven Spin Transport</dc:title>
			<dc:creator>Mohammad Mohammadiaria</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020040</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-05-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-05-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>40</prism:startingPage>
		<prism:doi>10.3390/quantum8020040</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/40</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/39">

	<title>Quantum Reports, Vol. 8, Pages 39: Experimental Proof That Bell&amp;rsquo;s Inequality Cannot Falsify Local Realism, Together with Corresponding Cause Analysis and Conjectures</title>
	<link>https://www.mdpi.com/2624-960X/8/2/39</link>
	<description>Conventional tests of Bell&amp;amp;rsquo;s inequality rely on entangled photon pairs. Here, we replace entangled pairs with two independent photons of orthogonal polarization and demonstrate that Bell&amp;amp;rsquo;s inequality is still violated. Given the inherent local realism of independent photons, this experiment proves that Bell&amp;amp;rsquo;s inequality cannot falsify the local realism of photons. We thus conjecture that the violation of Bell&amp;amp;rsquo;s inequality by entangled photon pairs originates from their orthogonal polarizations rather than the breakdown of local realism. To interpret this unexpected violation with independent photons, we further substitute the two photons with two monochromatic light beams and calculate the transmittance correlation through polarizers via Malus&amp;amp;rsquo;s law and Karl Pearson&amp;amp;rsquo;s correlation formula. We show that this correlation also defies Bell&amp;amp;rsquo;s inequality. Retracing the derivation of Bell&amp;amp;rsquo;s inequality reveals that its validity is restricted to binary events, which accounts for the observed violation with light beams. Finally, we propose a thought experiment involving the gradual attenuation of light intensity down to the single-photon regime and hypothesize that single-photon transmission through a polarizer does not constitute a binary event. This hypothesis provides a unified interpretation for both our experimental findings and all canonical Bell inequality tests reported to date.</description>
	<pubDate>2026-04-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 39: Experimental Proof That Bell&amp;rsquo;s Inequality Cannot Falsify Local Realism, Together with Corresponding Cause Analysis and Conjectures</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/39">doi: 10.3390/quantum8020039</a></p>
	<p>Authors:
		Ting Zhou
		</p>
	<p>Conventional tests of Bell&amp;amp;rsquo;s inequality rely on entangled photon pairs. Here, we replace entangled pairs with two independent photons of orthogonal polarization and demonstrate that Bell&amp;amp;rsquo;s inequality is still violated. Given the inherent local realism of independent photons, this experiment proves that Bell&amp;amp;rsquo;s inequality cannot falsify the local realism of photons. We thus conjecture that the violation of Bell&amp;amp;rsquo;s inequality by entangled photon pairs originates from their orthogonal polarizations rather than the breakdown of local realism. To interpret this unexpected violation with independent photons, we further substitute the two photons with two monochromatic light beams and calculate the transmittance correlation through polarizers via Malus&amp;amp;rsquo;s law and Karl Pearson&amp;amp;rsquo;s correlation formula. We show that this correlation also defies Bell&amp;amp;rsquo;s inequality. Retracing the derivation of Bell&amp;amp;rsquo;s inequality reveals that its validity is restricted to binary events, which accounts for the observed violation with light beams. Finally, we propose a thought experiment involving the gradual attenuation of light intensity down to the single-photon regime and hypothesize that single-photon transmission through a polarizer does not constitute a binary event. This hypothesis provides a unified interpretation for both our experimental findings and all canonical Bell inequality tests reported to date.</p>
	]]></content:encoded>

	<dc:title>Experimental Proof That Bell&amp;amp;rsquo;s Inequality Cannot Falsify Local Realism, Together with Corresponding Cause Analysis and Conjectures</dc:title>
			<dc:creator>Ting Zhou</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020039</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-25</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-25</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>39</prism:startingPage>
		<prism:doi>10.3390/quantum8020039</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/39</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/38">

	<title>Quantum Reports, Vol. 8, Pages 38: From Proportional Stationarity to Curvature&amp;ndash;Strain Balance: A Variational Bridge for Equilibrium Ratios</title>
	<link>https://www.mdpi.com/2624-960X/8/2/38</link>
	<description>Variational models describe deformation and stability through the first and second variations in an underlying functional, but the relationship between these responses is seldom expressed as an intrinsic equilibrium quantity of the model itself. A canonical curvature&amp;amp;ndash;strain representation for equilibrium ratios arising in variational field settings is developed. For a twice Fr&amp;amp;eacute;chet differentiable functional and an admissible perturbation generator, strain is defined as normalized first-order response and curvature as normalized second-order response along the generator direction. Their quotient defines a curvature&amp;amp;ndash;strain ratio that measures proportional balance between deformation and curvature within the model. The main result shows that this curvature&amp;amp;ndash;strain ratio is a canonical representative of a response ratio already implicit in the variational data. Under canonical normalization, the curvature&amp;amp;ndash;strain ratio coincides with the quotient of second- and first-order response, and stationarity of the curvature&amp;amp;ndash;strain ratio is equivalent to proportional stationarity of that response quotient along the admissible flow. A further theorem establishes transfer of local isolation: when the second-variation operator satisfies standard hypotheses such as compact resolvent and non-degeneracy of the constrained extremum, isolated equilibrium ratios persist in the curvature&amp;amp;ndash;strain representation for the same operator-theoretic reasons. Quadratic scalar and Maxwell-type models illustrate the construction. The paper establishes a mathematically controlled curvature&amp;amp;ndash;strain representation of equilibrium ratios within ordinary variational theory, with emphasis on the analysis of variational response and equilibrium balance.</description>
	<pubDate>2026-04-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 38: From Proportional Stationarity to Curvature&amp;ndash;Strain Balance: A Variational Bridge for Equilibrium Ratios</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/38">doi: 10.3390/quantum8020038</a></p>
	<p>Authors:
		Robert Castro
		</p>
	<p>Variational models describe deformation and stability through the first and second variations in an underlying functional, but the relationship between these responses is seldom expressed as an intrinsic equilibrium quantity of the model itself. A canonical curvature&amp;amp;ndash;strain representation for equilibrium ratios arising in variational field settings is developed. For a twice Fr&amp;amp;eacute;chet differentiable functional and an admissible perturbation generator, strain is defined as normalized first-order response and curvature as normalized second-order response along the generator direction. Their quotient defines a curvature&amp;amp;ndash;strain ratio that measures proportional balance between deformation and curvature within the model. The main result shows that this curvature&amp;amp;ndash;strain ratio is a canonical representative of a response ratio already implicit in the variational data. Under canonical normalization, the curvature&amp;amp;ndash;strain ratio coincides with the quotient of second- and first-order response, and stationarity of the curvature&amp;amp;ndash;strain ratio is equivalent to proportional stationarity of that response quotient along the admissible flow. A further theorem establishes transfer of local isolation: when the second-variation operator satisfies standard hypotheses such as compact resolvent and non-degeneracy of the constrained extremum, isolated equilibrium ratios persist in the curvature&amp;amp;ndash;strain representation for the same operator-theoretic reasons. Quadratic scalar and Maxwell-type models illustrate the construction. The paper establishes a mathematically controlled curvature&amp;amp;ndash;strain representation of equilibrium ratios within ordinary variational theory, with emphasis on the analysis of variational response and equilibrium balance.</p>
	]]></content:encoded>

	<dc:title>From Proportional Stationarity to Curvature&amp;amp;ndash;Strain Balance: A Variational Bridge for Equilibrium Ratios</dc:title>
			<dc:creator>Robert Castro</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020038</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-22</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>38</prism:startingPage>
		<prism:doi>10.3390/quantum8020038</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/38</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/37">

	<title>Quantum Reports, Vol. 8, Pages 37: Quantum Image Representation with Enhanced Intensity Preservation and Fidelity (IP-QIR)</title>
	<link>https://www.mdpi.com/2624-960X/8/2/37</link>
	<description>Quantum image representation (QIR) is the basic idea behind quantum image processing. It explains how a normal image is converted into quantum states so that it can be processed using quantum computers. The commonly used models for QIR are Flexible Representation of Quantum Images (FRQIs) and Novel Enhanced Quantum Representation (NEQR). Though these approaches highlight the potential of quantum-based image encoding, the limitation of practical applicability on Noisy Intermediate-Scale Quantum (NISQ) devices exists. In this paper, we propose an intensity-preserving quantum image representation (IP-QIR) scheme that aims to maintain accurate grayscale intensity information while significantly reducing quantum resource usage. The proposed method employs a controlled rotation-based encoding strategy, where pixel intensities are embedded into the measurement probability of a single intensity qubit, and spatial information is represented using position qubits. To further enhance feasibility on near-term quantum hardware, the framework operates on small image patches instead of full-resolution images, thereby reducing circuit depth and overall complexity. The performance of the proposed IP-QIR approach is evaluated through IBM Qiskit simulations on three types of grayscale images: synthetic image patches, synthetic aperture radar (SAR) images, and medical tuberculosis (TB) chest X-ray images. Experimental results demonstrate that IP-QIR achieves better intensity preservation than FRQIs and NEQR, with fidelity values reaching up to 84.12% for both SAR and medical datasets. In addition, IP-QIR represents a 4&amp;amp;times;4 image patch using only five qubits, which significantly reduces the qubit requirement when compared to NEQR, while still preserving high reconstruction accuracy.</description>
	<pubDate>2026-04-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 37: Quantum Image Representation with Enhanced Intensity Preservation and Fidelity (IP-QIR)</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/37">doi: 10.3390/quantum8020037</a></p>
	<p>Authors:
		Vrushali Nikam
		Shirish Sane
		Manish Motghare
		</p>
	<p>Quantum image representation (QIR) is the basic idea behind quantum image processing. It explains how a normal image is converted into quantum states so that it can be processed using quantum computers. The commonly used models for QIR are Flexible Representation of Quantum Images (FRQIs) and Novel Enhanced Quantum Representation (NEQR). Though these approaches highlight the potential of quantum-based image encoding, the limitation of practical applicability on Noisy Intermediate-Scale Quantum (NISQ) devices exists. In this paper, we propose an intensity-preserving quantum image representation (IP-QIR) scheme that aims to maintain accurate grayscale intensity information while significantly reducing quantum resource usage. The proposed method employs a controlled rotation-based encoding strategy, where pixel intensities are embedded into the measurement probability of a single intensity qubit, and spatial information is represented using position qubits. To further enhance feasibility on near-term quantum hardware, the framework operates on small image patches instead of full-resolution images, thereby reducing circuit depth and overall complexity. The performance of the proposed IP-QIR approach is evaluated through IBM Qiskit simulations on three types of grayscale images: synthetic image patches, synthetic aperture radar (SAR) images, and medical tuberculosis (TB) chest X-ray images. Experimental results demonstrate that IP-QIR achieves better intensity preservation than FRQIs and NEQR, with fidelity values reaching up to 84.12% for both SAR and medical datasets. In addition, IP-QIR represents a 4&amp;amp;times;4 image patch using only five qubits, which significantly reduces the qubit requirement when compared to NEQR, while still preserving high reconstruction accuracy.</p>
	]]></content:encoded>

	<dc:title>Quantum Image Representation with Enhanced Intensity Preservation and Fidelity (IP-QIR)</dc:title>
			<dc:creator>Vrushali Nikam</dc:creator>
			<dc:creator>Shirish Sane</dc:creator>
			<dc:creator>Manish Motghare</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020037</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-22</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>37</prism:startingPage>
		<prism:doi>10.3390/quantum8020037</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/37</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/36">

	<title>Quantum Reports, Vol. 8, Pages 36: Bipolar Entropy vs. Entropy/Negentropy: From Quantum Emergence to Agentic AI&amp;amp;QI with Collectively Entangled Bipolar Strings ER &amp;ge;&amp;ge; EPR</title>
	<link>https://www.mdpi.com/2624-960X/8/2/36</link>
	<description>While the quantum emergence of spacetime is becoming a major research topic in physics, the quantum emergence of intelligence has not been widely researched in quantum information science (QIS). Following causal-logical quantum gravity theory, bipolar entropy vs. entropy and negative entropy (or negentropy) are reviewed and distinguished for quantum emergence/submergence of quantum agent (QA) and quantum intelligence (QI) in algebraic terms. This work refers to QA as an entangled bipolar string/superstring in bipolar dynamic equilibrium (BDE) and QI being centered on logically definable causality in regularity, mind-light-matter unity, and brain-universe similarity. ER = EPR is extended to ER &amp;amp;ge;&amp;amp;ge; EPR for the mathematical scalability of bipolar strings and their collective entanglement. The extension leads to a number of conjectures, testable predictions, and theorems. The term &amp;amp;ldquo;equilibraton&amp;amp;rdquo; is proposed as a type of EPR or bipolar generic string to serve as an entropic stitch to collectively hold the universe together as a quantum entanglement in BDE with ubiquitous, regulated local emergence and submergence of QA&amp;amp;amp;QI. Equilibraton leads to the concept of bipolar entropy square&amp;amp;mdash;a complete entropic solution to the background issue in quantum gravity. With complete background independence, energy/information conservational bipolar entropy, energy/information invariance, bipolar entropy non-additivity, and equilibrium-based plateau concavity are introduced. The nature of the one-dimensional arrow of time is conjectured. As a unification of order and disorder for equilibrium-based regulation, bipolar entropy bridges QA&amp;amp;amp;QI to agentic AI, where quantum-bio-economics can be viewed as a topological intervention of a natural dynamic equilibrium in a social or natural world. Use cases are reviewed to illustrate the practical and theoretical aspects of bipolar entropy in business management, quantum-bio-economics, quantum cryptography, physics, and biology. Eddington&amp;amp;ndash;Einstein&amp;amp;rsquo;s comments on entropy are revisited. It is expected that bipolar entropy will bring quantum emergence/submergence to agentic AI&amp;amp;amp;QI for entangled machine thinking and imagination as a naturally scalable and testable foundation of real-world quantum gravity, quantum information science (QIS), quantum cognition, and quantum biology (QCQB) to enhance Large Language AI Models (LLMs) and machine intelligence.</description>
	<pubDate>2026-04-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 36: Bipolar Entropy vs. Entropy/Negentropy: From Quantum Emergence to Agentic AI&amp;amp;QI with Collectively Entangled Bipolar Strings ER &amp;ge;&amp;ge; EPR</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/36">doi: 10.3390/quantum8020036</a></p>
	<p>Authors:
		Wen-Ran Zhang
		Hengyu Zhang
		</p>
	<p>While the quantum emergence of spacetime is becoming a major research topic in physics, the quantum emergence of intelligence has not been widely researched in quantum information science (QIS). Following causal-logical quantum gravity theory, bipolar entropy vs. entropy and negative entropy (or negentropy) are reviewed and distinguished for quantum emergence/submergence of quantum agent (QA) and quantum intelligence (QI) in algebraic terms. This work refers to QA as an entangled bipolar string/superstring in bipolar dynamic equilibrium (BDE) and QI being centered on logically definable causality in regularity, mind-light-matter unity, and brain-universe similarity. ER = EPR is extended to ER &amp;amp;ge;&amp;amp;ge; EPR for the mathematical scalability of bipolar strings and their collective entanglement. The extension leads to a number of conjectures, testable predictions, and theorems. The term &amp;amp;ldquo;equilibraton&amp;amp;rdquo; is proposed as a type of EPR or bipolar generic string to serve as an entropic stitch to collectively hold the universe together as a quantum entanglement in BDE with ubiquitous, regulated local emergence and submergence of QA&amp;amp;amp;QI. Equilibraton leads to the concept of bipolar entropy square&amp;amp;mdash;a complete entropic solution to the background issue in quantum gravity. With complete background independence, energy/information conservational bipolar entropy, energy/information invariance, bipolar entropy non-additivity, and equilibrium-based plateau concavity are introduced. The nature of the one-dimensional arrow of time is conjectured. As a unification of order and disorder for equilibrium-based regulation, bipolar entropy bridges QA&amp;amp;amp;QI to agentic AI, where quantum-bio-economics can be viewed as a topological intervention of a natural dynamic equilibrium in a social or natural world. Use cases are reviewed to illustrate the practical and theoretical aspects of bipolar entropy in business management, quantum-bio-economics, quantum cryptography, physics, and biology. Eddington&amp;amp;ndash;Einstein&amp;amp;rsquo;s comments on entropy are revisited. It is expected that bipolar entropy will bring quantum emergence/submergence to agentic AI&amp;amp;amp;QI for entangled machine thinking and imagination as a naturally scalable and testable foundation of real-world quantum gravity, quantum information science (QIS), quantum cognition, and quantum biology (QCQB) to enhance Large Language AI Models (LLMs) and machine intelligence.</p>
	]]></content:encoded>

	<dc:title>Bipolar Entropy vs. Entropy/Negentropy: From Quantum Emergence to Agentic AI&amp;amp;amp;QI with Collectively Entangled Bipolar Strings ER &amp;amp;ge;&amp;amp;ge; EPR</dc:title>
			<dc:creator>Wen-Ran Zhang</dc:creator>
			<dc:creator>Hengyu Zhang</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020036</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-20</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-20</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>36</prism:startingPage>
		<prism:doi>10.3390/quantum8020036</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/36</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/35">

	<title>Quantum Reports, Vol. 8, Pages 35: Quantum Correlations in Classical Systems</title>
	<link>https://www.mdpi.com/2624-960X/8/2/35</link>
	<description>A classical fluid splitter produces the same patterns of energy redistribution as a Stern&amp;amp;ndash;Gerlach quantum device, with rotationally invariant coefficients of correlation between molecular paths. Alternative settings express a cosine squared relationship, leading to Tsirelson-type Bell violations with outcome independence. This result confirms the Correspondence Principle of quantum mechanics, where individual detection events express system-level properties according to Born&amp;amp;rsquo;s Rule. Kochen&amp;amp;ndash;Specker contextuality and Bell Locality are not formally contradicted, but their interpretation is in question. Current definitions of &amp;amp;ldquo;Local Realism&amp;amp;rdquo; are limited to intrinsic particle properties. In contrast, quantum-like correlations require the acknowledgement of ensemble effects on dynamically inseparable entities, even when those entities are observed one at a time.</description>
	<pubDate>2026-04-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 35: Quantum Correlations in Classical Systems</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/35">doi: 10.3390/quantum8020035</a></p>
	<p>Authors:
		Ghenadie N. Mardari
		</p>
	<p>A classical fluid splitter produces the same patterns of energy redistribution as a Stern&amp;amp;ndash;Gerlach quantum device, with rotationally invariant coefficients of correlation between molecular paths. Alternative settings express a cosine squared relationship, leading to Tsirelson-type Bell violations with outcome independence. This result confirms the Correspondence Principle of quantum mechanics, where individual detection events express system-level properties according to Born&amp;amp;rsquo;s Rule. Kochen&amp;amp;ndash;Specker contextuality and Bell Locality are not formally contradicted, but their interpretation is in question. Current definitions of &amp;amp;ldquo;Local Realism&amp;amp;rdquo; are limited to intrinsic particle properties. In contrast, quantum-like correlations require the acknowledgement of ensemble effects on dynamically inseparable entities, even when those entities are observed one at a time.</p>
	]]></content:encoded>

	<dc:title>Quantum Correlations in Classical Systems</dc:title>
			<dc:creator>Ghenadie N. Mardari</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020035</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-18</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-18</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>35</prism:startingPage>
		<prism:doi>10.3390/quantum8020035</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/35</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/34">

	<title>Quantum Reports, Vol. 8, Pages 34: Quantum-Informational History Optimization Theory (QIHOT): A Single-History Selection Framework with Consistency Results</title>
	<link>https://www.mdpi.com/2624-960X/8/2/34</link>
	<description>We present Quantum-Informational History Optimization Theory (QIHOT) as a formal proposal for selecting a single realized quantum history from a space of dynamically admissible histories subject to boundary constraints. In the present paper, we restrict attention to finite-dimensional and toy-model settings, where the framework can be stated explicitly. QIHOT separates two levels: a dynamical prior over admissible histories generated by standard quantum evolution, and an informational selection rule that reweights those histories by an entropy-based cost functional. Within this structure, we show that standard Born statistics are recovered in symmetric-cost measurement scenarios when the prior is the usual Hilbert-space quantum prior. We further formulate conditions under which operational no-signaling is preserved, provided the selection functional factorizes locally for spacelike-separated regions. A fully worked two-outcome model illustrates how the framework interpolates between coherent evolution and measurement-like branch selection. We contrast QIHOT with the Many-Worlds Interpretation, the Transactional Interpretation, the Consistent Histories formalism, the Schwinger&amp;amp;ndash;Keldysh formalism, and Lagrangian-based retrocausal models, highlighting structural similarities and key differences. We emphasize that the present paper develops QIHOT as a scoped formal proposal with partial consistency results rather than as a complete replacement for quantum theory. Possible extensions to consciousness and cosmology are deferred to brief outlook-level discussion.</description>
	<pubDate>2026-04-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 34: Quantum-Informational History Optimization Theory (QIHOT): A Single-History Selection Framework with Consistency Results</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/34">doi: 10.3390/quantum8020034</a></p>
	<p>Authors:
		Freeman Hui
		</p>
	<p>We present Quantum-Informational History Optimization Theory (QIHOT) as a formal proposal for selecting a single realized quantum history from a space of dynamically admissible histories subject to boundary constraints. In the present paper, we restrict attention to finite-dimensional and toy-model settings, where the framework can be stated explicitly. QIHOT separates two levels: a dynamical prior over admissible histories generated by standard quantum evolution, and an informational selection rule that reweights those histories by an entropy-based cost functional. Within this structure, we show that standard Born statistics are recovered in symmetric-cost measurement scenarios when the prior is the usual Hilbert-space quantum prior. We further formulate conditions under which operational no-signaling is preserved, provided the selection functional factorizes locally for spacelike-separated regions. A fully worked two-outcome model illustrates how the framework interpolates between coherent evolution and measurement-like branch selection. We contrast QIHOT with the Many-Worlds Interpretation, the Transactional Interpretation, the Consistent Histories formalism, the Schwinger&amp;amp;ndash;Keldysh formalism, and Lagrangian-based retrocausal models, highlighting structural similarities and key differences. We emphasize that the present paper develops QIHOT as a scoped formal proposal with partial consistency results rather than as a complete replacement for quantum theory. Possible extensions to consciousness and cosmology are deferred to brief outlook-level discussion.</p>
	]]></content:encoded>

	<dc:title>Quantum-Informational History Optimization Theory (QIHOT): A Single-History Selection Framework with Consistency Results</dc:title>
			<dc:creator>Freeman Hui</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020034</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-16</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-16</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>34</prism:startingPage>
		<prism:doi>10.3390/quantum8020034</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/34</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/33">

	<title>Quantum Reports, Vol. 8, Pages 33: Copy-Time Geometry from Gauge-Coded Quantum Cellular Automata: Emergent Gravity and a Golden Relation for Singlet-Scalar Dark Matter</title>
	<link>https://www.mdpi.com/2624-960X/8/2/33</link>
	<description>We formulate the Quantum Information Copy Time (QICT) framework for conserved charges under strictly local quantum dynamics and isolate its logically strongest consequence. The theorem-level core is a receiver-optimised variational speed-limit inequality: after projection away from the conserved zero mode, the copy time is bounded from below by the inverse square root of a Liouvillian-squared receiver susceptibility times a local encoding seminorm. This statement is written in a finite-volume operator framework and does not require a diffusive ansatz. We then examine what follows only after additional infrared assumptions. Under a single diffusive slow-mode hypothesis, the variational inequality reduces to the practical scaling relation used in the benchmark computations. That reduction is treated as conditional and is stress-tested numerically rather than promoted by rhetoric. Within the anomaly-free Abelian span relevant for one Standard-Model-like generation, hypercharge selection is elevated to theorem-level status; by contrast, minimal gauge-algebra uniqueness remains explicitly conditional on additional model-selection axioms. The remainder of the manuscript is organised as an explicitly documented closure programme built on top of this core. In that closure, a gauge-coded QCA construction, a microscopic benchmark for the transport normalisation, and an electroweak matching convention are combined to produce a resonance-centred Higgs-portal singlet-scalar mass band together with direct-detection, invisible-width, and relic-consistency checks. These latter results are presented as model-dependent consequences of an explicit closure ansatz rather than as deductions from locality alone.</description>
	<pubDate>2026-04-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 33: Copy-Time Geometry from Gauge-Coded Quantum Cellular Automata: Emergent Gravity and a Golden Relation for Singlet-Scalar Dark Matter</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/33">doi: 10.3390/quantum8020033</a></p>
	<p>Authors:
		Mohamed Sacha
		</p>
	<p>We formulate the Quantum Information Copy Time (QICT) framework for conserved charges under strictly local quantum dynamics and isolate its logically strongest consequence. The theorem-level core is a receiver-optimised variational speed-limit inequality: after projection away from the conserved zero mode, the copy time is bounded from below by the inverse square root of a Liouvillian-squared receiver susceptibility times a local encoding seminorm. This statement is written in a finite-volume operator framework and does not require a diffusive ansatz. We then examine what follows only after additional infrared assumptions. Under a single diffusive slow-mode hypothesis, the variational inequality reduces to the practical scaling relation used in the benchmark computations. That reduction is treated as conditional and is stress-tested numerically rather than promoted by rhetoric. Within the anomaly-free Abelian span relevant for one Standard-Model-like generation, hypercharge selection is elevated to theorem-level status; by contrast, minimal gauge-algebra uniqueness remains explicitly conditional on additional model-selection axioms. The remainder of the manuscript is organised as an explicitly documented closure programme built on top of this core. In that closure, a gauge-coded QCA construction, a microscopic benchmark for the transport normalisation, and an electroweak matching convention are combined to produce a resonance-centred Higgs-portal singlet-scalar mass band together with direct-detection, invisible-width, and relic-consistency checks. These latter results are presented as model-dependent consequences of an explicit closure ansatz rather than as deductions from locality alone.</p>
	]]></content:encoded>

	<dc:title>Copy-Time Geometry from Gauge-Coded Quantum Cellular Automata: Emergent Gravity and a Golden Relation for Singlet-Scalar Dark Matter</dc:title>
			<dc:creator>Mohamed Sacha</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020033</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-13</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>33</prism:startingPage>
		<prism:doi>10.3390/quantum8020033</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/33</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/32">

	<title>Quantum Reports, Vol. 8, Pages 32: The Informational Economy Functional: A Variational Principle for Decoherence and Classical Emergence</title>
	<link>https://www.mdpi.com/2624-960X/8/2/32</link>
	<description>The emergence of classicality through quantum decoherence is commonly described from complementary perspectives emphasizing stability (environment-induced superselection), objectivity (Quantum Darwinism), or physical feasibility (information thermodynamics). In realistic open quantum systems, however, these aspects coexist and compete under finite physical resources. In this work we argue that classical structure selection is most naturally understood as a resource-constrained, multi-objective process. We introduce the Informational Economy Functional (IEF), an effective accounting framework that places loss of distinguishability, energetic dissipation, and the generation of redundantly accessible records on equal footing. The associated Principle of Informational Economy characterizes emergent classical structures as those achieving an optimal compromise among stability, objectivity, and energetic feasibility. Classicality is thus neither maximally stable, nor maximally redundant, nor maximally energy-efficient, but instead reflects a Pareto-optimal balance shaped by environmental constraints. The IEF yields falsifiable predictions concerning pointer-structure variability, redundancy deformation, and resource-sensitive trade-offs, and suggests concrete experimental tests in continuously monitored quantum platforms. Classical reality is thereby reinterpreted as the most economical configuration in which information can stably form, propagate, and persist.</description>
	<pubDate>2026-04-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 32: The Informational Economy Functional: A Variational Principle for Decoherence and Classical Emergence</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/32">doi: 10.3390/quantum8020032</a></p>
	<p>Authors:
		Wan Zheng
		</p>
	<p>The emergence of classicality through quantum decoherence is commonly described from complementary perspectives emphasizing stability (environment-induced superselection), objectivity (Quantum Darwinism), or physical feasibility (information thermodynamics). In realistic open quantum systems, however, these aspects coexist and compete under finite physical resources. In this work we argue that classical structure selection is most naturally understood as a resource-constrained, multi-objective process. We introduce the Informational Economy Functional (IEF), an effective accounting framework that places loss of distinguishability, energetic dissipation, and the generation of redundantly accessible records on equal footing. The associated Principle of Informational Economy characterizes emergent classical structures as those achieving an optimal compromise among stability, objectivity, and energetic feasibility. Classicality is thus neither maximally stable, nor maximally redundant, nor maximally energy-efficient, but instead reflects a Pareto-optimal balance shaped by environmental constraints. The IEF yields falsifiable predictions concerning pointer-structure variability, redundancy deformation, and resource-sensitive trade-offs, and suggests concrete experimental tests in continuously monitored quantum platforms. Classical reality is thereby reinterpreted as the most economical configuration in which information can stably form, propagate, and persist.</p>
	]]></content:encoded>

	<dc:title>The Informational Economy Functional: A Variational Principle for Decoherence and Classical Emergence</dc:title>
			<dc:creator>Wan Zheng</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020032</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-10</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-10</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>32</prism:startingPage>
		<prism:doi>10.3390/quantum8020032</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/32</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/31">

	<title>Quantum Reports, Vol. 8, Pages 31: Fixed Spectral Data and the Dynamics of Spacetime Geometry</title>
	<link>https://www.mdpi.com/2624-960X/8/2/31</link>
	<description>We identify a fundamental tension between general relativity and spectral geometry arising from the global, nonlocal character of spectral data versus the local causal dynamics of spacetime. To resolve this, we postulate spectral invariance, &amp;amp;delta;&amp;amp;Lambda;n=0, requiring the eigenvalues of the Laplace&amp;amp;ndash;Beltrami operator to remain fixed under physical evolution. This condition yields a compensatory relation between metric deformations and eigenfunction amplitudes, suggesting a kinematic coupling linking energy distribution to spacetime curvature. From the second variation of the associated energy functional, we derive a rank-4 tensor proportional to the inverse DeWitt supermetric on superspace and a contracted rank-2 tensor proportional to the spacetime metric, and we recover a invariance law of the energy functional in configuration space. Spectral invariance may suggest a framework in which geometry and energy are co-defined through fixed spectral data.</description>
	<pubDate>2026-04-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 31: Fixed Spectral Data and the Dynamics of Spacetime Geometry</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/31">doi: 10.3390/quantum8020031</a></p>
	<p>Authors:
		Jacob Yan Gurevich
		</p>
	<p>We identify a fundamental tension between general relativity and spectral geometry arising from the global, nonlocal character of spectral data versus the local causal dynamics of spacetime. To resolve this, we postulate spectral invariance, &amp;amp;delta;&amp;amp;Lambda;n=0, requiring the eigenvalues of the Laplace&amp;amp;ndash;Beltrami operator to remain fixed under physical evolution. This condition yields a compensatory relation between metric deformations and eigenfunction amplitudes, suggesting a kinematic coupling linking energy distribution to spacetime curvature. From the second variation of the associated energy functional, we derive a rank-4 tensor proportional to the inverse DeWitt supermetric on superspace and a contracted rank-2 tensor proportional to the spacetime metric, and we recover a invariance law of the energy functional in configuration space. Spectral invariance may suggest a framework in which geometry and energy are co-defined through fixed spectral data.</p>
	]]></content:encoded>

	<dc:title>Fixed Spectral Data and the Dynamics of Spacetime Geometry</dc:title>
			<dc:creator>Jacob Yan Gurevich</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020031</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-08</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-08</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>31</prism:startingPage>
		<prism:doi>10.3390/quantum8020031</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/31</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/30">

	<title>Quantum Reports, Vol. 8, Pages 30: QGeo: A Python Package for Calculating Geodesic Control Functions for Quantum Computing</title>
	<link>https://www.mdpi.com/2624-960X/8/2/30</link>
	<description>We present a new Python package that uses the formalism of geometric quantum complexity to numerically compute metric-dependent geometric cost and control functions associated with preparing a given unitary transformation on a quantum computer. The numerical procedure we implement is presented and discussed. Analyzed quantum circuits include: the quantum Fourier transform for up to four qubits, a random circuit with depth 100, and a circuit for analyzing the evolution of a fermionic chain with several lattice sites.</description>
	<pubDate>2026-04-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 30: QGeo: A Python Package for Calculating Geodesic Control Functions for Quantum Computing</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/30">doi: 10.3390/quantum8020030</a></p>
	<p>Authors:
		Sean T. Crowe
		Joshua J. Leiter
		John P. T. Stenger
		Zachary L. Barvian
		Joseph A. Diaz
		Shoshana Kinzel
		Joanna N. Ptasinski
		Daniel Gunlycke
		</p>
	<p>We present a new Python package that uses the formalism of geometric quantum complexity to numerically compute metric-dependent geometric cost and control functions associated with preparing a given unitary transformation on a quantum computer. The numerical procedure we implement is presented and discussed. Analyzed quantum circuits include: the quantum Fourier transform for up to four qubits, a random circuit with depth 100, and a circuit for analyzing the evolution of a fermionic chain with several lattice sites.</p>
	]]></content:encoded>

	<dc:title>QGeo: A Python Package for Calculating Geodesic Control Functions for Quantum Computing</dc:title>
			<dc:creator>Sean T. Crowe</dc:creator>
			<dc:creator>Joshua J. Leiter</dc:creator>
			<dc:creator>John P. T. Stenger</dc:creator>
			<dc:creator>Zachary L. Barvian</dc:creator>
			<dc:creator>Joseph A. Diaz</dc:creator>
			<dc:creator>Shoshana Kinzel</dc:creator>
			<dc:creator>Joanna N. Ptasinski</dc:creator>
			<dc:creator>Daniel Gunlycke</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020030</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-04-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-04-01</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>30</prism:startingPage>
		<prism:doi>10.3390/quantum8020030</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/30</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/29">

	<title>Quantum Reports, Vol. 8, Pages 29: A Derivation of the Entangled State Representation by the Slice Theorem of the Wigner Operator</title>
	<link>https://www.mdpi.com/2624-960X/8/2/29</link>
	<description>The Wigner operator&amp;amp;rsquo;s normal ordering form is deduced by using the method of integration within the ordered product of operators, and the operator&amp;amp;rsquo;s Weyl ordering symbol is employed. The integration theory within the Weyl ordering product of operators is applied, and the Wigner operator&amp;amp;rsquo;s Weyl ordering form is deduced. Then, the Wigner operator&amp;amp;rsquo;s slice theorem is proposed, which helps project and display a new pure-state density operator. Thus, the quantization of classical tomography theory is realized. We illustrate the derivation of the bi- and tri-partite entangled state representations, respectively, which completes the argument.</description>
	<pubDate>2026-03-26</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 29: A Derivation of the Entangled State Representation by the Slice Theorem of the Wigner Operator</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/29">doi: 10.3390/quantum8020029</a></p>
	<p>Authors:
		Ke Zhang
		Hongyi Fan
		</p>
	<p>The Wigner operator&amp;amp;rsquo;s normal ordering form is deduced by using the method of integration within the ordered product of operators, and the operator&amp;amp;rsquo;s Weyl ordering symbol is employed. The integration theory within the Weyl ordering product of operators is applied, and the Wigner operator&amp;amp;rsquo;s Weyl ordering form is deduced. Then, the Wigner operator&amp;amp;rsquo;s slice theorem is proposed, which helps project and display a new pure-state density operator. Thus, the quantization of classical tomography theory is realized. We illustrate the derivation of the bi- and tri-partite entangled state representations, respectively, which completes the argument.</p>
	]]></content:encoded>

	<dc:title>A Derivation of the Entangled State Representation by the Slice Theorem of the Wigner Operator</dc:title>
			<dc:creator>Ke Zhang</dc:creator>
			<dc:creator>Hongyi Fan</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020029</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-26</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-26</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>29</prism:startingPage>
		<prism:doi>10.3390/quantum8020029</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/29</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/2/28">

	<title>Quantum Reports, Vol. 8, Pages 28: Optimality of Quantum Adiabatic Search Algorithm and Its Circuit Model</title>
	<link>https://www.mdpi.com/2624-960X/8/2/28</link>
	<description>In this paper, we study two aspects of quantum adiabatic evolution for a prototypical search problem: the optimality of the corresponding algorithm and its relation to the quantum circuit model. Firstly, we propose a general framework for proving the square-root speedup of the quantum adiabatic algorithm to be optimal over classical computation, which is readily applicable to the case of multiple targets. Through this framework, we also find that it is possible to further reduce the time complexity by increasing the physical energy of the system, encompassing results from previous works. Secondly, we find that, on the one hand, when the quantum adiabatic algorithm that achieves quadratic speedup is implemented on a quantum circuit, the time slice needed is always consistent with its time complexity, which also encompasses previous results; on the other hand, however, if a further algorithmic improvement is considered, the time slice always remains invariant. This phenomenon represents a significant observation with potential applications. We anticipate that the main results of this paper will interest the quantum adiabatic computation community and may help us to design efficient quantum algorithms for practical problems in the future.</description>
	<pubDate>2026-03-26</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 28: Optimality of Quantum Adiabatic Search Algorithm and Its Circuit Model</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/2/28">doi: 10.3390/quantum8020028</a></p>
	<p>Authors:
		Jie Sun
		Zhimin Zhang
		Songfeng Lu
		</p>
	<p>In this paper, we study two aspects of quantum adiabatic evolution for a prototypical search problem: the optimality of the corresponding algorithm and its relation to the quantum circuit model. Firstly, we propose a general framework for proving the square-root speedup of the quantum adiabatic algorithm to be optimal over classical computation, which is readily applicable to the case of multiple targets. Through this framework, we also find that it is possible to further reduce the time complexity by increasing the physical energy of the system, encompassing results from previous works. Secondly, we find that, on the one hand, when the quantum adiabatic algorithm that achieves quadratic speedup is implemented on a quantum circuit, the time slice needed is always consistent with its time complexity, which also encompasses previous results; on the other hand, however, if a further algorithmic improvement is considered, the time slice always remains invariant. This phenomenon represents a significant observation with potential applications. We anticipate that the main results of this paper will interest the quantum adiabatic computation community and may help us to design efficient quantum algorithms for practical problems in the future.</p>
	]]></content:encoded>

	<dc:title>Optimality of Quantum Adiabatic Search Algorithm and Its Circuit Model</dc:title>
			<dc:creator>Jie Sun</dc:creator>
			<dc:creator>Zhimin Zhang</dc:creator>
			<dc:creator>Songfeng Lu</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8020028</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-26</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-26</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>28</prism:startingPage>
		<prism:doi>10.3390/quantum8020028</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/2/28</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/27">

	<title>Quantum Reports, Vol. 8, Pages 27: Coupled-Field Dynamical Relaxation for QUBO and Ising Optimizations</title>
	<link>https://www.mdpi.com/2624-960X/8/1/27</link>
	<description>This work presents a classical theoretical framework in which combinatorial optimization emerges from the nonlinear relaxation of coupled real-valued phase fields governed by a global Lyapunov energy functional. Each computational element (CF-bit) evolves in a bistable periodic potential while pairwise interactions encode problem-specific couplings, enabling gradient-descent minimization of QUBO and Ising objective functions. The key contribution is an explicit global energy functional from which all dynamics are derived, guaranteeing monotonic energy descent under damping. This distinguishes the approach from several existing oscillator-based Ising architectures where the governing dynamics contain non-gradient terms and an explicit global Lyapunov functional has not been derived in their standard formulations. Numerical simulations on instances up to 20 bits demonstrate deterministic phase-locking convergence, with optional transient noise improving the exploration of rugged landscapes. While limited in scale and not overcoming NP-hardness, this work provides a conceptual framework showing how discrete optimization can emerge from continuous classical dynamics with a mathematically transparent energy structure.</description>
	<pubDate>2026-03-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 27: Coupled-Field Dynamical Relaxation for QUBO and Ising Optimizations</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/27">doi: 10.3390/quantum8010027</a></p>
	<p>Authors:
		Doron Kwiat
		</p>
	<p>This work presents a classical theoretical framework in which combinatorial optimization emerges from the nonlinear relaxation of coupled real-valued phase fields governed by a global Lyapunov energy functional. Each computational element (CF-bit) evolves in a bistable periodic potential while pairwise interactions encode problem-specific couplings, enabling gradient-descent minimization of QUBO and Ising objective functions. The key contribution is an explicit global energy functional from which all dynamics are derived, guaranteeing monotonic energy descent under damping. This distinguishes the approach from several existing oscillator-based Ising architectures where the governing dynamics contain non-gradient terms and an explicit global Lyapunov functional has not been derived in their standard formulations. Numerical simulations on instances up to 20 bits demonstrate deterministic phase-locking convergence, with optional transient noise improving the exploration of rugged landscapes. While limited in scale and not overcoming NP-hardness, this work provides a conceptual framework showing how discrete optimization can emerge from continuous classical dynamics with a mathematically transparent energy structure.</p>
	]]></content:encoded>

	<dc:title>Coupled-Field Dynamical Relaxation for QUBO and Ising Optimizations</dc:title>
			<dc:creator>Doron Kwiat</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010027</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-23</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-23</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>27</prism:startingPage>
		<prism:doi>10.3390/quantum8010027</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/27</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/26">

	<title>Quantum Reports, Vol. 8, Pages 26: A Technical Review of Quantum Computing Use Cases for Finance and Economics</title>
	<link>https://www.mdpi.com/2624-960X/8/1/26</link>
	<description>Quantum computing has been rapidly evolving as a field, with innovations driven by industry, academia, and government institutions. The technology has the potential to accelerate computation for solving complex problems across multiple industrial sectors. Finance and economics, with many problems exhibiting computationally heavy requirements, comprise a high-profile sector where quantum computing could have a significant impact. Therefore, it is important to identify and understand to what extent the technology could find utility in the sector. This technical review is written for quantum applications researchers, quantitative analysts in finance and economics, and researchers in related mathematical sciences. It is divided into two parts: (i) a survey of quantum algorithms pertinent to problems in finance and economics, and (ii) mapping of several use cases in the sector to the potential quantum algorithms presented in part (i). We discuss some challenges on the pathway to achieving quantum advantage. Ultimately, this review aims to be a catalyst for interdisciplinary research that will accelerate the advent of the practical advantages of quantum technologies to solve complex problems in this sector.</description>
	<pubDate>2026-03-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 26: A Technical Review of Quantum Computing Use Cases for Finance and Economics</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/26">doi: 10.3390/quantum8010026</a></p>
	<p>Authors:
		Manqoba Q. Hlatshwayo
		Manav Babel
		Dalila Islas-Sanchez
		Konstantinos Georgopoulos
		</p>
	<p>Quantum computing has been rapidly evolving as a field, with innovations driven by industry, academia, and government institutions. The technology has the potential to accelerate computation for solving complex problems across multiple industrial sectors. Finance and economics, with many problems exhibiting computationally heavy requirements, comprise a high-profile sector where quantum computing could have a significant impact. Therefore, it is important to identify and understand to what extent the technology could find utility in the sector. This technical review is written for quantum applications researchers, quantitative analysts in finance and economics, and researchers in related mathematical sciences. It is divided into two parts: (i) a survey of quantum algorithms pertinent to problems in finance and economics, and (ii) mapping of several use cases in the sector to the potential quantum algorithms presented in part (i). We discuss some challenges on the pathway to achieving quantum advantage. Ultimately, this review aims to be a catalyst for interdisciplinary research that will accelerate the advent of the practical advantages of quantum technologies to solve complex problems in this sector.</p>
	]]></content:encoded>

	<dc:title>A Technical Review of Quantum Computing Use Cases for Finance and Economics</dc:title>
			<dc:creator>Manqoba Q. Hlatshwayo</dc:creator>
			<dc:creator>Manav Babel</dc:creator>
			<dc:creator>Dalila Islas-Sanchez</dc:creator>
			<dc:creator>Konstantinos Georgopoulos</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010026</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-17</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>26</prism:startingPage>
		<prism:doi>10.3390/quantum8010026</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/26</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/25">

	<title>Quantum Reports, Vol. 8, Pages 25: Theory of Spacetime Impedance: A Reactive Framework for the Electromagnetic, Gravitational, and Quantum Structure of the Vacuum</title>
	<link>https://www.mdpi.com/2624-960X/8/1/25</link>
	<description>This work presents the Theory of Spacetime Impedance (TSI), a phenomenological framework in which the vacuum is modeled as a distributed reactive medium with an effective RLC structure. At the classical level, the vacuum is characterized by permeability, &amp;amp;mu;0, permittivity, &amp;amp;epsilon;0, and impedance, Z0, so that the speed of light follows from the vacuum&amp;amp;rsquo;s constitutive reactive properties. The TSI introduces a reactive&amp;amp;ndash;dissipative term, RH, as an effective mechanism associated with irreversibility, decoherence, and entropy production, providing a physical basis for the arrow of time. At the quantum level, TSI incorporates a quantum RLC triad associated with the electron, defined by quantum inductance, LK, quantum capacitance, CK, and von Klitzing resistance, RK. When normalized by the Compton wavelength, these quantities admit a direct comparison with &amp;amp;mu;0 and &amp;amp;epsilon;0, identifying the fine-structure constant as an impedance scaling factor between classical and quantum regimes. Within this unified reactive picture, inductive, capacitive, and resistive responses are respectively associated with gravitation, electromagnetism, and thermodynamic irreversibility, offering a complementary bridge across quantum, relativistic, and macroscopic domains.</description>
	<pubDate>2026-03-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 25: Theory of Spacetime Impedance: A Reactive Framework for the Electromagnetic, Gravitational, and Quantum Structure of the Vacuum</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/25">doi: 10.3390/quantum8010025</a></p>
	<p>Authors:
		Felipe Bosa
		</p>
	<p>This work presents the Theory of Spacetime Impedance (TSI), a phenomenological framework in which the vacuum is modeled as a distributed reactive medium with an effective RLC structure. At the classical level, the vacuum is characterized by permeability, &amp;amp;mu;0, permittivity, &amp;amp;epsilon;0, and impedance, Z0, so that the speed of light follows from the vacuum&amp;amp;rsquo;s constitutive reactive properties. The TSI introduces a reactive&amp;amp;ndash;dissipative term, RH, as an effective mechanism associated with irreversibility, decoherence, and entropy production, providing a physical basis for the arrow of time. At the quantum level, TSI incorporates a quantum RLC triad associated with the electron, defined by quantum inductance, LK, quantum capacitance, CK, and von Klitzing resistance, RK. When normalized by the Compton wavelength, these quantities admit a direct comparison with &amp;amp;mu;0 and &amp;amp;epsilon;0, identifying the fine-structure constant as an impedance scaling factor between classical and quantum regimes. Within this unified reactive picture, inductive, capacitive, and resistive responses are respectively associated with gravitation, electromagnetism, and thermodynamic irreversibility, offering a complementary bridge across quantum, relativistic, and macroscopic domains.</p>
	]]></content:encoded>

	<dc:title>Theory of Spacetime Impedance: A Reactive Framework for the Electromagnetic, Gravitational, and Quantum Structure of the Vacuum</dc:title>
			<dc:creator>Felipe Bosa</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010025</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-16</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-16</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>25</prism:startingPage>
		<prism:doi>10.3390/quantum8010025</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/25</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/24">

	<title>Quantum Reports, Vol. 8, Pages 24: Defining Quantum Agents: Formal Foundations, Architectures, and NISQ-Era Prototypes</title>
	<link>https://www.mdpi.com/2624-960X/8/1/24</link>
	<description>Quantum computing offers potential computational advantages, yet its integration into autonomous decision-making systems remains largely unexplored. This paper addresses the need for a unified framework that systematically combines quantum computation with agent-based artificial intelligence. We examine how quantum technologies can enhance the capabilities of autonomous agents and, conversely, how agentic AI can support the advancement of quantum systems. We analyze both directions of this synergy and present conceptual and technical foundations for future quantum&amp;amp;ndash;agentic platforms. Our work introduces a formal definition of quantum agents and outlines architectures that integrate quantum computing with agent-based systems. As concrete proof-of-concept implementations, we develop and evaluate three quantum agent prototypes: (i) a Grover-based decision agent for quantum search-driven action selection, (ii) a variational quantum reinforcement learning agent for adaptive policy learning in a multi-armed bandit setting, and (iii) an adaptive quantum image encryption agent that autonomously selects encryption strategies based on entropy-driven feedback. These prototypes demonstrate practical realizations of quantum agency in decision-making, learning, and security contexts under NISQ-era constraints. Furthermore, we discuss application domains including quantum-enhanced optimization, hybrid quantum&amp;amp;ndash;classical orchestration, autonomous quantum workflow management, and secure quantum information processing. By bridging these fields, we introduce a structured theoretical and architectural framework for quantum&amp;amp;ndash;agentic systems, providing formal definitions, system models, and early operational prototypes that illustrate the feasibility of quantum-enhanced agency under NISQ constraints.</description>
	<pubDate>2026-03-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 24: Defining Quantum Agents: Formal Foundations, Architectures, and NISQ-Era Prototypes</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/24">doi: 10.3390/quantum8010024</a></p>
	<p>Authors:
		Eldar Sultanow
		Madjid Tehrani
		Siddhant Dutta
		William J. Buchanan
		Muhammad Shahbaz Khan
		</p>
	<p>Quantum computing offers potential computational advantages, yet its integration into autonomous decision-making systems remains largely unexplored. This paper addresses the need for a unified framework that systematically combines quantum computation with agent-based artificial intelligence. We examine how quantum technologies can enhance the capabilities of autonomous agents and, conversely, how agentic AI can support the advancement of quantum systems. We analyze both directions of this synergy and present conceptual and technical foundations for future quantum&amp;amp;ndash;agentic platforms. Our work introduces a formal definition of quantum agents and outlines architectures that integrate quantum computing with agent-based systems. As concrete proof-of-concept implementations, we develop and evaluate three quantum agent prototypes: (i) a Grover-based decision agent for quantum search-driven action selection, (ii) a variational quantum reinforcement learning agent for adaptive policy learning in a multi-armed bandit setting, and (iii) an adaptive quantum image encryption agent that autonomously selects encryption strategies based on entropy-driven feedback. These prototypes demonstrate practical realizations of quantum agency in decision-making, learning, and security contexts under NISQ-era constraints. Furthermore, we discuss application domains including quantum-enhanced optimization, hybrid quantum&amp;amp;ndash;classical orchestration, autonomous quantum workflow management, and secure quantum information processing. By bridging these fields, we introduce a structured theoretical and architectural framework for quantum&amp;amp;ndash;agentic systems, providing formal definitions, system models, and early operational prototypes that illustrate the feasibility of quantum-enhanced agency under NISQ constraints.</p>
	]]></content:encoded>

	<dc:title>Defining Quantum Agents: Formal Foundations, Architectures, and NISQ-Era Prototypes</dc:title>
			<dc:creator>Eldar Sultanow</dc:creator>
			<dc:creator>Madjid Tehrani</dc:creator>
			<dc:creator>Siddhant Dutta</dc:creator>
			<dc:creator>William J. Buchanan</dc:creator>
			<dc:creator>Muhammad Shahbaz Khan</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010024</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-13</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>24</prism:startingPage>
		<prism:doi>10.3390/quantum8010024</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/24</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/23">

	<title>Quantum Reports, Vol. 8, Pages 23: Proportional Stationarity and Structural Stability in Perturbative Field Theories</title>
	<link>https://www.mdpi.com/2624-960X/8/1/23</link>
	<description>We formulate a structural stability criterion for dimensionless physical constants within standard perturbative field frameworks. The analysis introduces a response-ratio functional &amp;amp;Gamma;=&amp;amp;kappa;/&amp;amp;tau;, defined from second-order sensitivity and first-order deformation measures associated with admissible variations in a field configuration. Stability is characterized by proportional stationarity of &amp;amp;Gamma;, expressed as a first-order operator condition along transformation flows. The framework characterizes, within a declared variational model, when invariance of fixed constants can be represented as a stationarity condition. Under compactness and convexity assumptions typical of variational systems, stationary response ratios arise as isolated solutions of the associated operator equation; more general settings permit continuous spectra. Explicit functional definitions are provided within a conventional analytic setting, and the criterion is illustrated in representative classical field models. The results position proportional stationarity as a model-relative structural consistency condition for perturbative stability; isolation is conditional on compactness and non-degeneracy hypotheses, and continuous families may occur outside that regime. Limitations and possible extensions, including discretized spacetime formulations, are discussed.</description>
	<pubDate>2026-03-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 23: Proportional Stationarity and Structural Stability in Perturbative Field Theories</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/23">doi: 10.3390/quantum8010023</a></p>
	<p>Authors:
		Robert Castro
		</p>
	<p>We formulate a structural stability criterion for dimensionless physical constants within standard perturbative field frameworks. The analysis introduces a response-ratio functional &amp;amp;Gamma;=&amp;amp;kappa;/&amp;amp;tau;, defined from second-order sensitivity and first-order deformation measures associated with admissible variations in a field configuration. Stability is characterized by proportional stationarity of &amp;amp;Gamma;, expressed as a first-order operator condition along transformation flows. The framework characterizes, within a declared variational model, when invariance of fixed constants can be represented as a stationarity condition. Under compactness and convexity assumptions typical of variational systems, stationary response ratios arise as isolated solutions of the associated operator equation; more general settings permit continuous spectra. Explicit functional definitions are provided within a conventional analytic setting, and the criterion is illustrated in representative classical field models. The results position proportional stationarity as a model-relative structural consistency condition for perturbative stability; isolation is conditional on compactness and non-degeneracy hypotheses, and continuous families may occur outside that regime. Limitations and possible extensions, including discretized spacetime formulations, are discussed.</p>
	]]></content:encoded>

	<dc:title>Proportional Stationarity and Structural Stability in Perturbative Field Theories</dc:title>
			<dc:creator>Robert Castro</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010023</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-13</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>23</prism:startingPage>
		<prism:doi>10.3390/quantum8010023</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/23</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/22">

	<title>Quantum Reports, Vol. 8, Pages 22: The Periodic Table as an Emergent Helicoidal Manifold: A Unified Information-Theoretic Analysis of the Atomic Elements Z = 1&amp;ndash;103</title>
	<link>https://www.mdpi.com/2624-960X/8/1/22</link>
	<description>Here we perform a detailed information-theoretic (IT) analysis of atomic electron densities in the periodic table, from hydrogen (Z = 1) to lawrencium (Z = 103). By use of the Shannon entropy, the Fisher information and the disequilibrium functionals in both position and momentum spaces as fundamental descriptors of the atomic densities, the periodic table can be represented in a three-dimensional information space as a continuous, highly ordered manifold. The analysis shows that chemical periodicity naturally emerges as a helicoidal manifold (reminiscent of a helix) at the coordinates of a 3D theoretic-information space (Shannon, Fisher, Disequilibrium), with each period forming one segment within the continuous global trajectory. We find information-theoretic signatures of shell structure, sub-shell filling, and electron-configuration anomalies, such as the familiar irregularities seen in chromium and copper. Therefore, the helicoidal character emerges naturally and is not imposed a priori. Further, through the uncertainty principle of the complementary analysis in momentum space, more insights are gained by exposing maximal information-theoretic differentiation for lighter atoms and compression among heavy elements. Notably, momentum-space analysis reveals that hydrogen occupies a natural intermediate position between helium and lithium based on kinetic energy distribution&amp;amp;mdash;contrasting with IT position-space results that emphasize hydrogen&amp;amp;rsquo;s unique delocalized electron density. Indeed, the 3D IT representation of the elements in position space aligns with the view that H does not belong to either the alkali metals or the halogens, but rather stands as a unique, standalone element. This complementary perspective provides new quantitative support for understanding hydrogen&amp;amp;rsquo;s dual chemical nature, providing new quantitative insight into ongoing debates about hydrogen&amp;amp;rsquo;s optimal periodic table position. Furthermore, by considering triadic relationships and complexity properties in relation to the L&amp;amp;oacute;pez&amp;amp;ndash;Mancini&amp;amp;ndash;Ruiz (LMC) and Fisher&amp;amp;ndash;Shannon (FS) functionals, we show that atomic complexity increases monotonically along with nuclear charge, and we provide a quantitative measure of how organized atomic electron densities are distributed throughout the periodic system. Based on our IT analyses, the fundamental character of periodicity could be addressed by employing helicoidal representations that highlight the characteristics of hydrogen, while simultaneously preserving the autonomy of the blocks of elements.</description>
	<pubDate>2026-03-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 22: The Periodic Table as an Emergent Helicoidal Manifold: A Unified Information-Theoretic Analysis of the Atomic Elements Z = 1&amp;ndash;103</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/22">doi: 10.3390/quantum8010022</a></p>
	<p>Authors:
		Rodolfo O. Esquivel
		Hazel Vázquez-Hernández
		Jonathan Ornelas-Muñoz
		</p>
	<p>Here we perform a detailed information-theoretic (IT) analysis of atomic electron densities in the periodic table, from hydrogen (Z = 1) to lawrencium (Z = 103). By use of the Shannon entropy, the Fisher information and the disequilibrium functionals in both position and momentum spaces as fundamental descriptors of the atomic densities, the periodic table can be represented in a three-dimensional information space as a continuous, highly ordered manifold. The analysis shows that chemical periodicity naturally emerges as a helicoidal manifold (reminiscent of a helix) at the coordinates of a 3D theoretic-information space (Shannon, Fisher, Disequilibrium), with each period forming one segment within the continuous global trajectory. We find information-theoretic signatures of shell structure, sub-shell filling, and electron-configuration anomalies, such as the familiar irregularities seen in chromium and copper. Therefore, the helicoidal character emerges naturally and is not imposed a priori. Further, through the uncertainty principle of the complementary analysis in momentum space, more insights are gained by exposing maximal information-theoretic differentiation for lighter atoms and compression among heavy elements. Notably, momentum-space analysis reveals that hydrogen occupies a natural intermediate position between helium and lithium based on kinetic energy distribution&amp;amp;mdash;contrasting with IT position-space results that emphasize hydrogen&amp;amp;rsquo;s unique delocalized electron density. Indeed, the 3D IT representation of the elements in position space aligns with the view that H does not belong to either the alkali metals or the halogens, but rather stands as a unique, standalone element. This complementary perspective provides new quantitative support for understanding hydrogen&amp;amp;rsquo;s dual chemical nature, providing new quantitative insight into ongoing debates about hydrogen&amp;amp;rsquo;s optimal periodic table position. Furthermore, by considering triadic relationships and complexity properties in relation to the L&amp;amp;oacute;pez&amp;amp;ndash;Mancini&amp;amp;ndash;Ruiz (LMC) and Fisher&amp;amp;ndash;Shannon (FS) functionals, we show that atomic complexity increases monotonically along with nuclear charge, and we provide a quantitative measure of how organized atomic electron densities are distributed throughout the periodic system. Based on our IT analyses, the fundamental character of periodicity could be addressed by employing helicoidal representations that highlight the characteristics of hydrogen, while simultaneously preserving the autonomy of the blocks of elements.</p>
	]]></content:encoded>

	<dc:title>The Periodic Table as an Emergent Helicoidal Manifold: A Unified Information-Theoretic Analysis of the Atomic Elements Z = 1&amp;amp;ndash;103</dc:title>
			<dc:creator>Rodolfo O. Esquivel</dc:creator>
			<dc:creator>Hazel Vázquez-Hernández</dc:creator>
			<dc:creator>Jonathan Ornelas-Muñoz</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010022</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>22</prism:startingPage>
		<prism:doi>10.3390/quantum8010022</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/22</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/21">

	<title>Quantum Reports, Vol. 8, Pages 21: A Possible Connection Between Quantum Mechanics and Spacetime</title>
	<link>https://www.mdpi.com/2624-960X/8/1/21</link>
	<description>Recent developments in holographic gravity suggest that spacetime structure may be deeply related to quantum mechanics. In this work, from a different perspective, we demonstrate that wave&amp;amp;ndash;particle duality can be interpreted as the uncertainty of spacetime for the particle. Summarizing all possible trajectories in conventional path integral quantum mechanics can be transformed into the summation of all possible spacetime metrics. Furthermore, we emphasize that in conventional quantum gravity, it is possible that the classical matter fields correspond to quantum spacetime. We argue that this is not quite reasonable and propose a new path integral quantum gravity model based on the new interpretation of wave&amp;amp;ndash;particle duality. In this model, the aforementioned drawback of conventional quantum gravity naturally disappears.</description>
	<pubDate>2026-03-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 21: A Possible Connection Between Quantum Mechanics and Spacetime</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/21">doi: 10.3390/quantum8010021</a></p>
	<p>Authors:
		Hong Wang
		Jin Wang
		</p>
	<p>Recent developments in holographic gravity suggest that spacetime structure may be deeply related to quantum mechanics. In this work, from a different perspective, we demonstrate that wave&amp;amp;ndash;particle duality can be interpreted as the uncertainty of spacetime for the particle. Summarizing all possible trajectories in conventional path integral quantum mechanics can be transformed into the summation of all possible spacetime metrics. Furthermore, we emphasize that in conventional quantum gravity, it is possible that the classical matter fields correspond to quantum spacetime. We argue that this is not quite reasonable and propose a new path integral quantum gravity model based on the new interpretation of wave&amp;amp;ndash;particle duality. In this model, the aforementioned drawback of conventional quantum gravity naturally disappears.</p>
	]]></content:encoded>

	<dc:title>A Possible Connection Between Quantum Mechanics and Spacetime</dc:title>
			<dc:creator>Hong Wang</dc:creator>
			<dc:creator>Jin Wang</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010021</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-11</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-11</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>21</prism:startingPage>
		<prism:doi>10.3390/quantum8010021</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/21</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/20">

	<title>Quantum Reports, Vol. 8, Pages 20: Curvature, Memory and Emergent Time in Cosmological Dynamics</title>
	<link>https://www.mdpi.com/2624-960X/8/1/20</link>
	<description>We present a covariant geometric extension of General Relativity formulated within a controlled effective field theory framework. The gravitational action is supplemented by curvature-dependent operators parametrized by three coefficients &amp;amp;alpha;, &amp;amp;beta;, and &amp;amp;gamma;, chosen such that the resulting field equations remain second order in time derivatives and free of Ostrogradsky instabilities. In a homogeneous and isotropic cosmological background, the modified dynamics generically replaces the classical Big Bang singularity with a smooth, nonsingular bounce driven by a repulsive curvature core proportional to a&amp;amp;minus;6. A distinctive feature of the framework is the presence of a geometric slip term proportional to H&amp;amp;#729;, which encodes curvature-memory effects at the level of the background evolution without introducing additional propagating degrees of freedom. This term dynamically correlates the expansion rate with its temporal variation, leading to effective ultraviolet damping and enhanced dynamical stability across the high-curvature regime. As a consequence, the cosmological solutions admit the definition of an intrinsic relational time variable that is strictly monotonic throughout the evolution, including across the bounce. The emergent temporal ordering arises purely from geometric dynamics and does not rely on matter clocks, nonlocality, or fundamental violations of time-reversal or CPT symmetry. We discuss the consistency of the framework within its effective field theory domain of validity and comment on its implications for the conceptual problems of singularity resolution and the emergence of time in cosmology.</description>
	<pubDate>2026-03-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 20: Curvature, Memory and Emergent Time in Cosmological Dynamics</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/20">doi: 10.3390/quantum8010020</a></p>
	<p>Authors:
		Iñaki Del Amo Castillo
		</p>
	<p>We present a covariant geometric extension of General Relativity formulated within a controlled effective field theory framework. The gravitational action is supplemented by curvature-dependent operators parametrized by three coefficients &amp;amp;alpha;, &amp;amp;beta;, and &amp;amp;gamma;, chosen such that the resulting field equations remain second order in time derivatives and free of Ostrogradsky instabilities. In a homogeneous and isotropic cosmological background, the modified dynamics generically replaces the classical Big Bang singularity with a smooth, nonsingular bounce driven by a repulsive curvature core proportional to a&amp;amp;minus;6. A distinctive feature of the framework is the presence of a geometric slip term proportional to H&amp;amp;#729;, which encodes curvature-memory effects at the level of the background evolution without introducing additional propagating degrees of freedom. This term dynamically correlates the expansion rate with its temporal variation, leading to effective ultraviolet damping and enhanced dynamical stability across the high-curvature regime. As a consequence, the cosmological solutions admit the definition of an intrinsic relational time variable that is strictly monotonic throughout the evolution, including across the bounce. The emergent temporal ordering arises purely from geometric dynamics and does not rely on matter clocks, nonlocality, or fundamental violations of time-reversal or CPT symmetry. We discuss the consistency of the framework within its effective field theory domain of validity and comment on its implications for the conceptual problems of singularity resolution and the emergence of time in cosmology.</p>
	]]></content:encoded>

	<dc:title>Curvature, Memory and Emergent Time in Cosmological Dynamics</dc:title>
			<dc:creator>Iñaki Del Amo Castillo</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010020</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-03-06</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-03-06</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>20</prism:startingPage>
		<prism:doi>10.3390/quantum8010020</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/19">

	<title>Quantum Reports, Vol. 8, Pages 19: Quantum-Inspired Classical Convolutional Neural Network for Automated Bone Cancer Detection from X-Ray Images</title>
	<link>https://www.mdpi.com/2624-960X/8/1/19</link>
	<description>Accurate and early detection of bone cancer is critical for improving patient outcomes, yet conventional radiographic interpretation remains limited by subjectivity and variability. Conventional AI models often struggle with complex multi-modal noise distributions, non-convex and topologically entangled latent manifolds, extreme class imbalance in rare oncological conditions, and heterogeneous data fusion constraints. To address these challenges, we present a Quantum-Inspired Classical Convolutional Neural Network (QC-CNN) inspired by quantum analogies for automated bone cancer detection in radiographic images. The proposed architecture integrates classical convolutional layers for hierarchical feature extraction with a classical variational layer motivated by high-dimensional Hilbert space analogies for enhanced pattern discrimination. A curated and annotated dataset of bone X-ray images was utilized, partitioned into training, validation, and independent test cohorts. The QC-CNN was optimized using stochastic gradient descent (SGD) with adaptive learning rate scheduling, and regularization strategies were applied to mitigate overfitting. Quantitative evaluation demonstrated superior diagnostic performance, achieving high accuracy, precision, recall, F1-score, and area under the receiver operating characteristic curve (AUC). Results highlight the ability of classical CNN with quantum-inspired design to capture non-linear correlations and subtle radiographic biomarkers that classical CNNs may overlook. This study establishes QC-CNN as a promising framework for quantum-analogy motivated medical image analysis, providing evidence of its utility in oncology and underscoring its potential for translation into clinical decision-support systems for early bone cancer diagnosis. All computations in the present study are performed using classical algorithms, with quantum-inspired concepts serving as a conceptual framework for model design and motivating future extensions.</description>
	<pubDate>2026-02-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 19: Quantum-Inspired Classical Convolutional Neural Network for Automated Bone Cancer Detection from X-Ray Images</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/19">doi: 10.3390/quantum8010019</a></p>
	<p>Authors:
		Naveen Joy
		Sonet Daniel Thomas
		Aparna Rajan
		Lijin Varghese
		Aswathi Balakrishnan
		Amritha Thaikkad
		Vidya Niranjan
		Abhithaj Jayanandan
		Rajesh Raju
		</p>
	<p>Accurate and early detection of bone cancer is critical for improving patient outcomes, yet conventional radiographic interpretation remains limited by subjectivity and variability. Conventional AI models often struggle with complex multi-modal noise distributions, non-convex and topologically entangled latent manifolds, extreme class imbalance in rare oncological conditions, and heterogeneous data fusion constraints. To address these challenges, we present a Quantum-Inspired Classical Convolutional Neural Network (QC-CNN) inspired by quantum analogies for automated bone cancer detection in radiographic images. The proposed architecture integrates classical convolutional layers for hierarchical feature extraction with a classical variational layer motivated by high-dimensional Hilbert space analogies for enhanced pattern discrimination. A curated and annotated dataset of bone X-ray images was utilized, partitioned into training, validation, and independent test cohorts. The QC-CNN was optimized using stochastic gradient descent (SGD) with adaptive learning rate scheduling, and regularization strategies were applied to mitigate overfitting. Quantitative evaluation demonstrated superior diagnostic performance, achieving high accuracy, precision, recall, F1-score, and area under the receiver operating characteristic curve (AUC). Results highlight the ability of classical CNN with quantum-inspired design to capture non-linear correlations and subtle radiographic biomarkers that classical CNNs may overlook. This study establishes QC-CNN as a promising framework for quantum-analogy motivated medical image analysis, providing evidence of its utility in oncology and underscoring its potential for translation into clinical decision-support systems for early bone cancer diagnosis. All computations in the present study are performed using classical algorithms, with quantum-inspired concepts serving as a conceptual framework for model design and motivating future extensions.</p>
	]]></content:encoded>

	<dc:title>Quantum-Inspired Classical Convolutional Neural Network for Automated Bone Cancer Detection from X-Ray Images</dc:title>
			<dc:creator>Naveen Joy</dc:creator>
			<dc:creator>Sonet Daniel Thomas</dc:creator>
			<dc:creator>Aparna Rajan</dc:creator>
			<dc:creator>Lijin Varghese</dc:creator>
			<dc:creator>Aswathi Balakrishnan</dc:creator>
			<dc:creator>Amritha Thaikkad</dc:creator>
			<dc:creator>Vidya Niranjan</dc:creator>
			<dc:creator>Abhithaj Jayanandan</dc:creator>
			<dc:creator>Rajesh Raju</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010019</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-25</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-25</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>19</prism:startingPage>
		<prism:doi>10.3390/quantum8010019</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/18">

	<title>Quantum Reports, Vol. 8, Pages 18: On the Unitarity of the Stueckelberg Wave Equation and Measurement as Bayesian Update from Maximum Entropy Prior Distribution</title>
	<link>https://www.mdpi.com/2624-960X/8/1/18</link>
	<description>The Stueckelberg wave equation is transformed into a quantum telegraph equation and a set of stationary states is obtained as unitary solutions. As it has been shown previously that this PDE relates to the Dirac operator, and on the other hand it is a linearized Hamilton&amp;amp;ndash;Jacobi&amp;amp;ndash;Bellman PDE, from which the Schr&amp;amp;ouml;dinger equation can be deduced in a nonrelativistic limit, it is clear that it is the key equation in relativistic quantum mechanics. We give a Bayesian interpretation for the measurement problem. The stationary solution is understood as a maximum entropy prior distribution and measurement is understood as a Bayesian update. We discuss the interpretation of the single electron experiments in the light of finite speed propagation of the transition probability field and how it relates to the interpretation of quantum mechanics more broadly.</description>
	<pubDate>2026-02-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 18: On the Unitarity of the Stueckelberg Wave Equation and Measurement as Bayesian Update from Maximum Entropy Prior Distribution</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/18">doi: 10.3390/quantum8010018</a></p>
	<p>Authors:
		Jussi Lindgren
		</p>
	<p>The Stueckelberg wave equation is transformed into a quantum telegraph equation and a set of stationary states is obtained as unitary solutions. As it has been shown previously that this PDE relates to the Dirac operator, and on the other hand it is a linearized Hamilton&amp;amp;ndash;Jacobi&amp;amp;ndash;Bellman PDE, from which the Schr&amp;amp;ouml;dinger equation can be deduced in a nonrelativistic limit, it is clear that it is the key equation in relativistic quantum mechanics. We give a Bayesian interpretation for the measurement problem. The stationary solution is understood as a maximum entropy prior distribution and measurement is understood as a Bayesian update. We discuss the interpretation of the single electron experiments in the light of finite speed propagation of the transition probability field and how it relates to the interpretation of quantum mechanics more broadly.</p>
	]]></content:encoded>

	<dc:title>On the Unitarity of the Stueckelberg Wave Equation and Measurement as Bayesian Update from Maximum Entropy Prior Distribution</dc:title>
			<dc:creator>Jussi Lindgren</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010018</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-22</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>18</prism:startingPage>
		<prism:doi>10.3390/quantum8010018</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/17">

	<title>Quantum Reports, Vol. 8, Pages 17: Enhancement of the Shift in the Photonic Spin Hall Effect and Its Application for Cancer Cell Detection</title>
	<link>https://www.mdpi.com/2624-960X/8/1/17</link>
	<description>The photonic spin Hall effect (PSHE) originates from the spin&amp;amp;ndash;orbit interaction (SOI) of light. The literature indicates that the transverse spin-dependent shift, &amp;amp;delta;H&amp;amp;minus; (SDS), from the PSHE is weak (in the nanometer range) and difficult to measure directly. This study utilizes a plasmonic structure to improve the &amp;amp;delta;H&amp;amp;minus; in the PSHE. The obtained results of this study demonstrate that the inclusion of silicon nitride (Si3N4) significantly enhances the &amp;amp;delta;H&amp;amp;minus; relative to its absence; however, plasmonic material is present in both cases. The enhanced shifts exhibit a significant dependence on the resonance angle (&amp;amp;theta;r) and the thickness of layers of the PSHE structure to attain the maximum increase in &amp;amp;delta;H&amp;amp;minus; of 350.82 &amp;amp;micro;m at the plasmonic resonance condition. A systematic analysis of the centroid positions of the reflected beam indicates a distinct and constant separation of opposing spin components. Further, the improved &amp;amp;delta;H&amp;amp;minus; is utilized in cancer cell detection, as changes in the refractive index (RI) of cells facilitate the identification of cancer cells from healthy to cancerous. All examined cell types demonstrate that cancerous cells had a greater &amp;amp;delta;H&amp;amp;minus; than normal cells, owing to their elevated effective RI. These results illustrate that the proposed plasmonic-assisted PSHE structure offers significant enhancement and a high sensitivity of 439.30 &amp;amp;micro;m/RIU for label-free detection of cancer cells.</description>
	<pubDate>2026-02-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 17: Enhancement of the Shift in the Photonic Spin Hall Effect and Its Application for Cancer Cell Detection</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/17">doi: 10.3390/quantum8010017</a></p>
	<p>Authors:
		Alka Verma
		Devanshi Katiyar
		Vimal Mishra
		Rajeev Gupta
		Yogendra Kumar Prajapati
		</p>
	<p>The photonic spin Hall effect (PSHE) originates from the spin&amp;amp;ndash;orbit interaction (SOI) of light. The literature indicates that the transverse spin-dependent shift, &amp;amp;delta;H&amp;amp;minus; (SDS), from the PSHE is weak (in the nanometer range) and difficult to measure directly. This study utilizes a plasmonic structure to improve the &amp;amp;delta;H&amp;amp;minus; in the PSHE. The obtained results of this study demonstrate that the inclusion of silicon nitride (Si3N4) significantly enhances the &amp;amp;delta;H&amp;amp;minus; relative to its absence; however, plasmonic material is present in both cases. The enhanced shifts exhibit a significant dependence on the resonance angle (&amp;amp;theta;r) and the thickness of layers of the PSHE structure to attain the maximum increase in &amp;amp;delta;H&amp;amp;minus; of 350.82 &amp;amp;micro;m at the plasmonic resonance condition. A systematic analysis of the centroid positions of the reflected beam indicates a distinct and constant separation of opposing spin components. Further, the improved &amp;amp;delta;H&amp;amp;minus; is utilized in cancer cell detection, as changes in the refractive index (RI) of cells facilitate the identification of cancer cells from healthy to cancerous. All examined cell types demonstrate that cancerous cells had a greater &amp;amp;delta;H&amp;amp;minus; than normal cells, owing to their elevated effective RI. These results illustrate that the proposed plasmonic-assisted PSHE structure offers significant enhancement and a high sensitivity of 439.30 &amp;amp;micro;m/RIU for label-free detection of cancer cells.</p>
	]]></content:encoded>

	<dc:title>Enhancement of the Shift in the Photonic Spin Hall Effect and Its Application for Cancer Cell Detection</dc:title>
			<dc:creator>Alka Verma</dc:creator>
			<dc:creator>Devanshi Katiyar</dc:creator>
			<dc:creator>Vimal Mishra</dc:creator>
			<dc:creator>Rajeev Gupta</dc:creator>
			<dc:creator>Yogendra Kumar Prajapati</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010017</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-17</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>17</prism:startingPage>
		<prism:doi>10.3390/quantum8010017</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/16">

	<title>Quantum Reports, Vol. 8, Pages 16: A Probability Model for the Bell Experiment</title>
	<link>https://www.mdpi.com/2624-960X/8/1/16</link>
	<description>The Bell inequality constrains the outcomes of measurements on pairs of distant entangled particles. The Bell contradiction states that the Bell inequality is inconsistent with the calculated outcomes of these quantum experiments. This contradiction led many to question the underlying assumptions, viz. so-called realism and locality. The probability model underlying the Bell inequality is generally left implicit. We propose an explicit probability model for the CHSH version of the Bell experiment. This model has only two simultaneously observable detector settings per measurement, and therefore does not assume realism. The quantum expectation now becomes a conditional expectation, given the two detector settings. This probability model is in full agreement with both quantum mechanics and experiments. As a result, the model satisfies the Bell inequality; there are no so-called violations. We extend this model to include a hidden variable. This extended model is not Bell-separable. This non-separability implies that the model is non-deterministic or non-local (or both).</description>
	<pubDate>2026-02-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 16: A Probability Model for the Bell Experiment</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/16">doi: 10.3390/quantum8010016</a></p>
	<p>Authors:
		Kees van Hee
		Kees van Berkel
		Jan de Graaf
		</p>
	<p>The Bell inequality constrains the outcomes of measurements on pairs of distant entangled particles. The Bell contradiction states that the Bell inequality is inconsistent with the calculated outcomes of these quantum experiments. This contradiction led many to question the underlying assumptions, viz. so-called realism and locality. The probability model underlying the Bell inequality is generally left implicit. We propose an explicit probability model for the CHSH version of the Bell experiment. This model has only two simultaneously observable detector settings per measurement, and therefore does not assume realism. The quantum expectation now becomes a conditional expectation, given the two detector settings. This probability model is in full agreement with both quantum mechanics and experiments. As a result, the model satisfies the Bell inequality; there are no so-called violations. We extend this model to include a hidden variable. This extended model is not Bell-separable. This non-separability implies that the model is non-deterministic or non-local (or both).</p>
	]]></content:encoded>

	<dc:title>A Probability Model for the Bell Experiment</dc:title>
			<dc:creator>Kees van Hee</dc:creator>
			<dc:creator>Kees van Berkel</dc:creator>
			<dc:creator>Jan de Graaf</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010016</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-14</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-14</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>16</prism:startingPage>
		<prism:doi>10.3390/quantum8010016</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/15">

	<title>Quantum Reports, Vol. 8, Pages 15: Quantum Omni-Synthesis I: Core Field-Theoretical Framework</title>
	<link>https://www.mdpi.com/2624-960X/8/1/15</link>
	<description>The Quantum Omni-Synthesis (QOS) framework is inspired by the cosmological constant problem, the dark sector, and the tension that arises when gravity is treated as purely geometrical while quantum fields remain defined on a fixed background. QOS adopts the working hypothesis that the dominant components of the dark sector correspond to two complementary energetic tendencies already familiar from known physics: confining, binding-dominated behavior and dispersive, propagating behavior. For clarity of interpretation, these are referred to as implosive and explosive energy, respectively. This terminology is not intended to redefine cosmological dark matter or dark energy, but to provide an effective language for tracking how different forms of energy contribute to localization, propagation, and gravitational coupling across scales. QOS postulates that every field configuration admits a decomposition of its local energy density into these two complementary components. A dimensionless scalar quantity, the Quantized Gravity Coupling Parameter &amp;amp;sigmaf;(x), quantifies the local fraction of implosive energy. Spacetime curvature in QOS is generated primarily by the implosive fraction, while explosive energy contributes to propagation and vacuum activity without sourcing gravity at the same strength. In this paper, a field-theoretical realization of this idea is presented for a single real scalar field. A QOS-modified Lagrangian is introduced in which the kinetic term is weighted by a factor A(&amp;amp;psi;,&amp;amp;nabla;&amp;amp;psi;)=1&amp;amp;minus;&amp;amp;sigmaf;2(&amp;amp;psi;,&amp;amp;nabla;&amp;amp;psi;) that encodes the local balance between gradient and potential energy. From this Lagrangian, the nonlinear field equation and the corresponding energy momentum tensor are derived in full generality, including the effects of the functional dependence of A on the field and its derivatives. An effective Ricci tensor is constructed as R&amp;amp;mu;&amp;amp;nu;eff=R&amp;amp;mu;&amp;amp;nu;+f&amp;amp;mu;&amp;amp;nu;, where the correction f&amp;amp;mu;&amp;amp;nu; is expressed in terms of derivatives of &amp;amp;Phi;=ln(1&amp;amp;minus;&amp;amp;sigmaf;2) and arises from the energetic weighting rather than an independent scalar degree of freedom. The resulting QOS field equation couples this scalar sector to curvature without introducing a separate Brans&amp;amp;ndash;Dicke-like field.</description>
	<pubDate>2026-02-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 15: Quantum Omni-Synthesis I: Core Field-Theoretical Framework</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/15">doi: 10.3390/quantum8010015</a></p>
	<p>Authors:
		Stefalo Acha
		</p>
	<p>The Quantum Omni-Synthesis (QOS) framework is inspired by the cosmological constant problem, the dark sector, and the tension that arises when gravity is treated as purely geometrical while quantum fields remain defined on a fixed background. QOS adopts the working hypothesis that the dominant components of the dark sector correspond to two complementary energetic tendencies already familiar from known physics: confining, binding-dominated behavior and dispersive, propagating behavior. For clarity of interpretation, these are referred to as implosive and explosive energy, respectively. This terminology is not intended to redefine cosmological dark matter or dark energy, but to provide an effective language for tracking how different forms of energy contribute to localization, propagation, and gravitational coupling across scales. QOS postulates that every field configuration admits a decomposition of its local energy density into these two complementary components. A dimensionless scalar quantity, the Quantized Gravity Coupling Parameter &amp;amp;sigmaf;(x), quantifies the local fraction of implosive energy. Spacetime curvature in QOS is generated primarily by the implosive fraction, while explosive energy contributes to propagation and vacuum activity without sourcing gravity at the same strength. In this paper, a field-theoretical realization of this idea is presented for a single real scalar field. A QOS-modified Lagrangian is introduced in which the kinetic term is weighted by a factor A(&amp;amp;psi;,&amp;amp;nabla;&amp;amp;psi;)=1&amp;amp;minus;&amp;amp;sigmaf;2(&amp;amp;psi;,&amp;amp;nabla;&amp;amp;psi;) that encodes the local balance between gradient and potential energy. From this Lagrangian, the nonlinear field equation and the corresponding energy momentum tensor are derived in full generality, including the effects of the functional dependence of A on the field and its derivatives. An effective Ricci tensor is constructed as R&amp;amp;mu;&amp;amp;nu;eff=R&amp;amp;mu;&amp;amp;nu;+f&amp;amp;mu;&amp;amp;nu;, where the correction f&amp;amp;mu;&amp;amp;nu; is expressed in terms of derivatives of &amp;amp;Phi;=ln(1&amp;amp;minus;&amp;amp;sigmaf;2) and arises from the energetic weighting rather than an independent scalar degree of freedom. The resulting QOS field equation couples this scalar sector to curvature without introducing a separate Brans&amp;amp;ndash;Dicke-like field.</p>
	]]></content:encoded>

	<dc:title>Quantum Omni-Synthesis I: Core Field-Theoretical Framework</dc:title>
			<dc:creator>Stefalo Acha</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010015</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-13</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/quantum8010015</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/14">

	<title>Quantum Reports, Vol. 8, Pages 14: Position Operators in Terms of Converging Finite-Dimensional Matrices and Their Intertwining with Geometry, Transport, and Gauge</title>
	<link>https://www.mdpi.com/2624-960X/8/1/14</link>
	<description>The position operator r^ appears as i&amp;amp;part;p in wave mechanics, while its matrix form (e.g., under a Bloch basis) is well known diverging in diagonals, causing difficulties in basis transformation, observable yielding, etc. We aim to find a convergent r-matrix (CRM) to improve the existing divergent r-matrix (DRM), and investigate its influence at both the conceptual and the application levels. A key modification is increasing the familiar substitution of r^ by i&amp;amp;part;p to i&amp;amp;sum;j&amp;amp;part;kj, namely the N-th Weyl algebra. Resolving the divergence makes r-matrix rigorously defined, and we are able to show r-matrix is distinct from a spin matrix in terms of its defining principles, transformation behavior, and the observable it yields. Conceptually, the CRM fills the logical gap between the r-matrix and the Berry connection (this unremarked vagueness has caused the diagonal divergence). In application, we focus on transport, and discover that the Hermitian matrix is not identical with the associative Hermitian operator, i.e., rm,n=rn,m*&amp;amp;#8654;r^=r^&amp;amp;dagger;, which subtly affects the celebrated Berry curvature formula for adiabatic current. We also discuss how such a non-representation CRM can contribute to building a unified transport theory.</description>
	<pubDate>2026-02-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 14: Position Operators in Terms of Converging Finite-Dimensional Matrices and Their Intertwining with Geometry, Transport, and Gauge</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/14">doi: 10.3390/quantum8010014</a></p>
	<p>Authors:
		Boqun Song
		Jonathan D. H. Smith
		Jigang Wang
		</p>
	<p>The position operator r^ appears as i&amp;amp;part;p in wave mechanics, while its matrix form (e.g., under a Bloch basis) is well known diverging in diagonals, causing difficulties in basis transformation, observable yielding, etc. We aim to find a convergent r-matrix (CRM) to improve the existing divergent r-matrix (DRM), and investigate its influence at both the conceptual and the application levels. A key modification is increasing the familiar substitution of r^ by i&amp;amp;part;p to i&amp;amp;sum;j&amp;amp;part;kj, namely the N-th Weyl algebra. Resolving the divergence makes r-matrix rigorously defined, and we are able to show r-matrix is distinct from a spin matrix in terms of its defining principles, transformation behavior, and the observable it yields. Conceptually, the CRM fills the logical gap between the r-matrix and the Berry connection (this unremarked vagueness has caused the diagonal divergence). In application, we focus on transport, and discover that the Hermitian matrix is not identical with the associative Hermitian operator, i.e., rm,n=rn,m*&amp;amp;#8654;r^=r^&amp;amp;dagger;, which subtly affects the celebrated Berry curvature formula for adiabatic current. We also discuss how such a non-representation CRM can contribute to building a unified transport theory.</p>
	]]></content:encoded>

	<dc:title>Position Operators in Terms of Converging Finite-Dimensional Matrices and Their Intertwining with Geometry, Transport, and Gauge</dc:title>
			<dc:creator>Boqun Song</dc:creator>
			<dc:creator>Jonathan D. H. Smith</dc:creator>
			<dc:creator>Jigang Wang</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010014</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/quantum8010014</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/13">

	<title>Quantum Reports, Vol. 8, Pages 13: Ergotropy from Geometric Phases in a Dephasing Qubit</title>
	<link>https://www.mdpi.com/2624-960X/8/1/13</link>
	<description>We analyze the geometric phase and dynamic phase acquired by a qubit coupled to an environment through pure dephasing, establishing a direct connection between phase accumulation and ergotropy. We show that the dynamic phase depends solely on the incoherent ergotropy, reflecting its purely energetic origin. In contrast, the geometric phase exhibits a nontrivial dependence on both the coherent and incoherent contributions to the total ergotropy, encoding the interplay between coherence, dissipation, and energy extraction. By performing a perturbative expansion in the qubit&amp;amp;ndash;environment coupling strength, we demonstrate that, in the weak-coupling and long-time regime, the geometric phase becomes determined exclusively by the incoherent ergotropy, which coincides with the asymptotic value of the total ergotropy reached under decoherence. These results provide a clear physical distinction between dynamic and geometric phases in open quantum systems and establish geometric phases as sensitive probes of energetic resources. Furthermore, in superconducting circuit implementations, our findings suggest that the ergotropy of a two-level system could be inferred indirectly from geometric-phase measurements using standard techniques such as quantum state tomography.</description>
	<pubDate>2026-02-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 13: Ergotropy from Geometric Phases in a Dephasing Qubit</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/13">doi: 10.3390/quantum8010013</a></p>
	<p>Authors:
		Fernando C. Lombardo
		Paula I. Villar
		</p>
	<p>We analyze the geometric phase and dynamic phase acquired by a qubit coupled to an environment through pure dephasing, establishing a direct connection between phase accumulation and ergotropy. We show that the dynamic phase depends solely on the incoherent ergotropy, reflecting its purely energetic origin. In contrast, the geometric phase exhibits a nontrivial dependence on both the coherent and incoherent contributions to the total ergotropy, encoding the interplay between coherence, dissipation, and energy extraction. By performing a perturbative expansion in the qubit&amp;amp;ndash;environment coupling strength, we demonstrate that, in the weak-coupling and long-time regime, the geometric phase becomes determined exclusively by the incoherent ergotropy, which coincides with the asymptotic value of the total ergotropy reached under decoherence. These results provide a clear physical distinction between dynamic and geometric phases in open quantum systems and establish geometric phases as sensitive probes of energetic resources. Furthermore, in superconducting circuit implementations, our findings suggest that the ergotropy of a two-level system could be inferred indirectly from geometric-phase measurements using standard techniques such as quantum state tomography.</p>
	]]></content:encoded>

	<dc:title>Ergotropy from Geometric Phases in a Dephasing Qubit</dc:title>
			<dc:creator>Fernando C. Lombardo</dc:creator>
			<dc:creator>Paula I. Villar</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010013</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>13</prism:startingPage>
		<prism:doi>10.3390/quantum8010013</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/12">

	<title>Quantum Reports, Vol. 8, Pages 12: Quantum Molecular Dynamics</title>
	<link>https://www.mdpi.com/2624-960X/8/1/12</link>
	<description>We formulate a new quantum many-body simulation method for a general quantum fluid at any given temperature. Unlike the path integral Monte Carlo method, our method evolves, in imaginary time, the density matrix from its initial delta function condition to its final thermal form in an amount of time equal to the inverse temperature. It does this with a molecular dynamics scheme applied to a classical Hamiltonian that has the same functional form as the one for the quantum mechanical Hamiltonian according to the properties of the continuous representation of John R. Klauder. We then end up with the thermal density matrix, which can be used to extract thermal averages of observables using the Monte Carlo method equally well in any statistics.</description>
	<pubDate>2026-02-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 12: Quantum Molecular Dynamics</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/12">doi: 10.3390/quantum8010012</a></p>
	<p>Authors:
		Riccardo Fantoni
		</p>
	<p>We formulate a new quantum many-body simulation method for a general quantum fluid at any given temperature. Unlike the path integral Monte Carlo method, our method evolves, in imaginary time, the density matrix from its initial delta function condition to its final thermal form in an amount of time equal to the inverse temperature. It does this with a molecular dynamics scheme applied to a classical Hamiltonian that has the same functional form as the one for the quantum mechanical Hamiltonian according to the properties of the continuous representation of John R. Klauder. We then end up with the thermal density matrix, which can be used to extract thermal averages of observables using the Monte Carlo method equally well in any statistics.</p>
	]]></content:encoded>

	<dc:title>Quantum Molecular Dynamics</dc:title>
			<dc:creator>Riccardo Fantoni</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010012</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-06</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-06</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>12</prism:startingPage>
		<prism:doi>10.3390/quantum8010012</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/11">

	<title>Quantum Reports, Vol. 8, Pages 11: Random Walks and Spin Projections</title>
	<link>https://www.mdpi.com/2624-960X/8/1/11</link>
	<description>The purpose of this article is to highlight the connections between two seemingly distinct domains: random walks and the distribution of angular-momentum projections in quantum physics (the magnetic quantum numbers m). It is well known that there is indeed a deep mathematical link between the two, via the vector composition of angular momenta and rotational symmetry. Random walks are considered in the framework of an interpretation of the probability of microstates in statistical physics. The ideas presented in this work aim to illustrate the relevance of this perspective for modeling angular momentum in atomic physics.</description>
	<pubDate>2026-02-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 11: Random Walks and Spin Projections</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/11">doi: 10.3390/quantum8010011</a></p>
	<p>Authors:
		Jean-Christophe Pain
		</p>
	<p>The purpose of this article is to highlight the connections between two seemingly distinct domains: random walks and the distribution of angular-momentum projections in quantum physics (the magnetic quantum numbers m). It is well known that there is indeed a deep mathematical link between the two, via the vector composition of angular momenta and rotational symmetry. Random walks are considered in the framework of an interpretation of the probability of microstates in statistical physics. The ideas presented in this work aim to illustrate the relevance of this perspective for modeling angular momentum in atomic physics.</p>
	]]></content:encoded>

	<dc:title>Random Walks and Spin Projections</dc:title>
			<dc:creator>Jean-Christophe Pain</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010011</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-02-02</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-02-02</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>11</prism:startingPage>
		<prism:doi>10.3390/quantum8010011</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/10">

	<title>Quantum Reports, Vol. 8, Pages 10: Quantum Chemistry of Strongly Correlated Electron Systems: Quantum Coherence of Open-Shell Molecular Systems Constructed by Chemical Methods: Organometallic Conjugation and Confinement</title>
	<link>https://www.mdpi.com/2624-960X/8/1/10</link>
	<description>Electronic and spin structures of open-shell molecules and clusters were investigated as possible building blocks for the construction of one- and two-dimensional quantum spin alignment systems which exhibited several characteristic quantum properties of strongly correlated electron systems: high-Tc superconductivity, quantum spin coherence, entanglement, etc. Ab initio calculations were performed to elucidate effective exchange integrals (J) for 3d transition metal oxides, providing the J-model for high-Tc superconductivity. Theoretical investigations such as Monte Carlo simulation, molecular mechanics and quantum mechanical calculations were performed to elucidate effective chemical procedures for through-bond alignments of open-shell transition metal ions by organometallic conjugation and through-space confinements of molecular spins such as molecular oxygen by molecular confinement materials. Theoretical simulations have elucidated the importance of appropriate confinement materials for alignments of molecular spins desired for quantum coherence and quantum sensing. Equivalent transformations among coherent states of superconductors, trapped ion, neutral atom, molecular spin, molecular exciton, etc., are also discussed on theoretical and conceptual grounds such as quantum entanglement and decoherence.</description>
	<pubDate>2026-01-31</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 10: Quantum Chemistry of Strongly Correlated Electron Systems: Quantum Coherence of Open-Shell Molecular Systems Constructed by Chemical Methods: Organometallic Conjugation and Confinement</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/10">doi: 10.3390/quantum8010010</a></p>
	<p>Authors:
		Takashi Kawakami
		Satoru Yamada
		Masateru Taniguchi
		Kizashi Yamaguchi
		</p>
	<p>Electronic and spin structures of open-shell molecules and clusters were investigated as possible building blocks for the construction of one- and two-dimensional quantum spin alignment systems which exhibited several characteristic quantum properties of strongly correlated electron systems: high-Tc superconductivity, quantum spin coherence, entanglement, etc. Ab initio calculations were performed to elucidate effective exchange integrals (J) for 3d transition metal oxides, providing the J-model for high-Tc superconductivity. Theoretical investigations such as Monte Carlo simulation, molecular mechanics and quantum mechanical calculations were performed to elucidate effective chemical procedures for through-bond alignments of open-shell transition metal ions by organometallic conjugation and through-space confinements of molecular spins such as molecular oxygen by molecular confinement materials. Theoretical simulations have elucidated the importance of appropriate confinement materials for alignments of molecular spins desired for quantum coherence and quantum sensing. Equivalent transformations among coherent states of superconductors, trapped ion, neutral atom, molecular spin, molecular exciton, etc., are also discussed on theoretical and conceptual grounds such as quantum entanglement and decoherence.</p>
	]]></content:encoded>

	<dc:title>Quantum Chemistry of Strongly Correlated Electron Systems: Quantum Coherence of Open-Shell Molecular Systems Constructed by Chemical Methods: Organometallic Conjugation and Confinement</dc:title>
			<dc:creator>Takashi Kawakami</dc:creator>
			<dc:creator>Satoru Yamada</dc:creator>
			<dc:creator>Masateru Taniguchi</dc:creator>
			<dc:creator>Kizashi Yamaguchi</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010010</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-31</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-31</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>10</prism:startingPage>
		<prism:doi>10.3390/quantum8010010</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/9">

	<title>Quantum Reports, Vol. 8, Pages 9: Comparative Analysis of Quantum Technology Policies in the United States and China: Strategic Directions and Philosophical Foundations</title>
	<link>https://www.mdpi.com/2624-960X/8/1/9</link>
	<description>Quantum technology, a critical 21st-century strategic frontier science, has been a key technological competition between China and the U.S. This study employs natural language processing (NLP) techniques and a technology analytical framework to analyze the quantum technology policies of both countries. While the U.S. emphasized free-market innovation and global technological leadership on quantum technology from 2018 to 2024, China prioritized government-led development and socioeconomic stability. Moreover, the Chinese government adopts a systematic top-down approach characterized by government planning and direct intervention. However, the U.S. fosters innovation through market mechanisms and industry-academia collaboration. U.S. policies have gradually shifted from pure technological innovation to national security considerations. On the other hand, China has moved from breakthrough research to industrial deployment and application. These policy differences reflect distinct political systems and governance models, which may also resonate with their respective cultural traditions and philosophical foundations. Our findings fill a critical gap in comparative quantum technology policy research, offering significant insights for policymakers, researchers, and international stakeholders.</description>
	<pubDate>2026-01-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 9: Comparative Analysis of Quantum Technology Policies in the United States and China: Strategic Directions and Philosophical Foundations</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/9">doi: 10.3390/quantum8010009</a></p>
	<p>Authors:
		Shangkun Wang
		Chunle Ni
		</p>
	<p>Quantum technology, a critical 21st-century strategic frontier science, has been a key technological competition between China and the U.S. This study employs natural language processing (NLP) techniques and a technology analytical framework to analyze the quantum technology policies of both countries. While the U.S. emphasized free-market innovation and global technological leadership on quantum technology from 2018 to 2024, China prioritized government-led development and socioeconomic stability. Moreover, the Chinese government adopts a systematic top-down approach characterized by government planning and direct intervention. However, the U.S. fosters innovation through market mechanisms and industry-academia collaboration. U.S. policies have gradually shifted from pure technological innovation to national security considerations. On the other hand, China has moved from breakthrough research to industrial deployment and application. These policy differences reflect distinct political systems and governance models, which may also resonate with their respective cultural traditions and philosophical foundations. Our findings fill a critical gap in comparative quantum technology policy research, offering significant insights for policymakers, researchers, and international stakeholders.</p>
	]]></content:encoded>

	<dc:title>Comparative Analysis of Quantum Technology Policies in the United States and China: Strategic Directions and Philosophical Foundations</dc:title>
			<dc:creator>Shangkun Wang</dc:creator>
			<dc:creator>Chunle Ni</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010009</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-23</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-23</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>9</prism:startingPage>
		<prism:doi>10.3390/quantum8010009</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/8">

	<title>Quantum Reports, Vol. 8, Pages 8: Bell&amp;ndash;CHSH Under Setting-Dependent Selection: Sharp Total-Variation Bounds and an Experimental Audit Protocol</title>
	<link>https://www.mdpi.com/2624-960X/8/1/8</link>
	<description>Bell&amp;amp;ndash;CHSH is an inequality about unconditional expectations: under measurement independence, Bell locality, and bounded outcomes, the CHSH value satisfies S&amp;amp;le;2. Experimental correlators, however, are often computed on an accepted subset of trials defined by detection logic, coincidence matching, quality cuts, and analysis windows. We model this by an acceptance probability &amp;amp;gamma;(a,b,&amp;amp;lambda;)&amp;amp;isin;[0,1] and the resulting accepted hidden-variable law &amp;amp;nu;ab obtained by weighting the measurement-independent prior &amp;amp;rho; by &amp;amp;gamma; and renormalizing. If &amp;amp;nu;ab depends on the setting pair then the four correlators entering CHSH are expectations under four different measures, and a Bell-local measurement-independent model can yield Sobs&amp;amp;gt;2 by selection alone. We quantify the required setting dependence in total variation (TV) distance. For any reference law &amp;amp;mu; we prove the sharp bound Sobs&amp;amp;le;2+2&amp;amp;sum;q&amp;amp;isin;QTV(&amp;amp;nu;q,&amp;amp;mu;) for a CHSH quartet Q. Optimizing over &amp;amp;mu; yields the intrinsic dispersion bound Sobs&amp;amp;le;2+2&amp;amp;Delta;Q, and, in particular, Sobs&amp;amp;le;min{4,2+6DQ}, where DQ is the quartet TV diameter. The constants are optimal. Consequently, reproducing Tsirelson&amp;amp;rsquo;s value 22 within Bell-local measurement-independent models via setting-dependent acceptance requires &amp;amp;Delta;Q&amp;amp;ge;2&amp;amp;minus;1 (hence, DQ&amp;amp;ge;(2&amp;amp;minus;1)/3). We then propose a two-lane experimental audit protocol: (i) prior-relative fair-sampling diagnostics using tags recorded on all trials, and (ii) prior-free dispersion diagnostics using accepted-tag distributions across settings, with &amp;amp;Delta;Q,X computable by linear programming on finite tag alphabets.</description>
	<pubDate>2026-01-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 8: Bell&amp;ndash;CHSH Under Setting-Dependent Selection: Sharp Total-Variation Bounds and an Experimental Audit Protocol</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/8">doi: 10.3390/quantum8010008</a></p>
	<p>Authors:
		Parker Emmerson (Yaohushuason)
		</p>
	<p>Bell&amp;amp;ndash;CHSH is an inequality about unconditional expectations: under measurement independence, Bell locality, and bounded outcomes, the CHSH value satisfies S&amp;amp;le;2. Experimental correlators, however, are often computed on an accepted subset of trials defined by detection logic, coincidence matching, quality cuts, and analysis windows. We model this by an acceptance probability &amp;amp;gamma;(a,b,&amp;amp;lambda;)&amp;amp;isin;[0,1] and the resulting accepted hidden-variable law &amp;amp;nu;ab obtained by weighting the measurement-independent prior &amp;amp;rho; by &amp;amp;gamma; and renormalizing. If &amp;amp;nu;ab depends on the setting pair then the four correlators entering CHSH are expectations under four different measures, and a Bell-local measurement-independent model can yield Sobs&amp;amp;gt;2 by selection alone. We quantify the required setting dependence in total variation (TV) distance. For any reference law &amp;amp;mu; we prove the sharp bound Sobs&amp;amp;le;2+2&amp;amp;sum;q&amp;amp;isin;QTV(&amp;amp;nu;q,&amp;amp;mu;) for a CHSH quartet Q. Optimizing over &amp;amp;mu; yields the intrinsic dispersion bound Sobs&amp;amp;le;2+2&amp;amp;Delta;Q, and, in particular, Sobs&amp;amp;le;min{4,2+6DQ}, where DQ is the quartet TV diameter. The constants are optimal. Consequently, reproducing Tsirelson&amp;amp;rsquo;s value 22 within Bell-local measurement-independent models via setting-dependent acceptance requires &amp;amp;Delta;Q&amp;amp;ge;2&amp;amp;minus;1 (hence, DQ&amp;amp;ge;(2&amp;amp;minus;1)/3). We then propose a two-lane experimental audit protocol: (i) prior-relative fair-sampling diagnostics using tags recorded on all trials, and (ii) prior-free dispersion diagnostics using accepted-tag distributions across settings, with &amp;amp;Delta;Q,X computable by linear programming on finite tag alphabets.</p>
	]]></content:encoded>

	<dc:title>Bell&amp;amp;ndash;CHSH Under Setting-Dependent Selection: Sharp Total-Variation Bounds and an Experimental Audit Protocol</dc:title>
			<dc:creator>Parker Emmerson (Yaohushuason)</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010008</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-23</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-23</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>8</prism:startingPage>
		<prism:doi>10.3390/quantum8010008</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/7">

	<title>Quantum Reports, Vol. 8, Pages 7: Pushing the Limits of Large Language Models in Quantum Operations</title>
	<link>https://www.mdpi.com/2624-960X/8/1/7</link>
	<description>What is the fastest Artificial Intelligence Large Language Model (AI LLM) for generating quantum operations? To answer this, we present the first benchmarking study comparing popular and publicly available AI models tasked with creating quantum gate designs. The Wolfram Mathematica framework was used to interface with the six AI LLMs, including Google Gemini 2.0 Flash, Anthropic Claude 3 Haiku, WolframLLM Notebook Assistant For Mathematica V14.3.0.0, OpenAI ChatGPT Omni 4 Mini, Google Gemma 3 4b 1t, and DeepSeek Chat V3. Our novel study found the following: (1) Gemini 2.0 Flash is overall the fastest AI LLM of the models tested in producing average quantum gate designs at 2.66101 s, factoring in the &amp;amp;ldquo;thinking&amp;amp;rdquo; execution time and ServiceConnect network latencies. (2) On average, four out of the ten quantum operations that the six LLMs produced compiled in Python version 3.13.5 (40.8% success rate). (3) Quantum operations averaged approximately 21&amp;amp;ndash;45 Lines of Code (omitting nonsensical outliers). (4) DeepSeek Chat V3 produced the shortest code with an average of 21.6 lines. This comparison evaluates the time taken by each AI LLM platform to generate quantum operations (including ServiceConnect networking times). These findings highlight a promising horizon where publicly available Large Language Models can become fast collaborators with quantum computers, enabling rapid quantum gate synthesis and paving the way for greater interoperability between two remarkable and cutting-edge technologies.</description>
	<pubDate>2026-01-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 7: Pushing the Limits of Large Language Models in Quantum Operations</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/7">doi: 10.3390/quantum8010007</a></p>
	<p>Authors:
		Dayton C. Closser
		Zbigniew J. Kabala
		</p>
	<p>What is the fastest Artificial Intelligence Large Language Model (AI LLM) for generating quantum operations? To answer this, we present the first benchmarking study comparing popular and publicly available AI models tasked with creating quantum gate designs. The Wolfram Mathematica framework was used to interface with the six AI LLMs, including Google Gemini 2.0 Flash, Anthropic Claude 3 Haiku, WolframLLM Notebook Assistant For Mathematica V14.3.0.0, OpenAI ChatGPT Omni 4 Mini, Google Gemma 3 4b 1t, and DeepSeek Chat V3. Our novel study found the following: (1) Gemini 2.0 Flash is overall the fastest AI LLM of the models tested in producing average quantum gate designs at 2.66101 s, factoring in the &amp;amp;ldquo;thinking&amp;amp;rdquo; execution time and ServiceConnect network latencies. (2) On average, four out of the ten quantum operations that the six LLMs produced compiled in Python version 3.13.5 (40.8% success rate). (3) Quantum operations averaged approximately 21&amp;amp;ndash;45 Lines of Code (omitting nonsensical outliers). (4) DeepSeek Chat V3 produced the shortest code with an average of 21.6 lines. This comparison evaluates the time taken by each AI LLM platform to generate quantum operations (including ServiceConnect networking times). These findings highlight a promising horizon where publicly available Large Language Models can become fast collaborators with quantum computers, enabling rapid quantum gate synthesis and paving the way for greater interoperability between two remarkable and cutting-edge technologies.</p>
	]]></content:encoded>

	<dc:title>Pushing the Limits of Large Language Models in Quantum Operations</dc:title>
			<dc:creator>Dayton C. Closser</dc:creator>
			<dc:creator>Zbigniew J. Kabala</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010007</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-19</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-19</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>7</prism:startingPage>
		<prism:doi>10.3390/quantum8010007</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/6">

	<title>Quantum Reports, Vol. 8, Pages 6: Counterfactual Quantum Control: Review and Applications</title>
	<link>https://www.mdpi.com/2624-960X/8/1/6</link>
	<description>Counterfactual quantum control is a novel control method, in which no actual material particles or energy are transported and exchanged between the controller and the controlled. By introducing the quantum Zeno effect where the evolution of a quantum system can be suppressed by continuous observation, this paper presents a review of research progress in counterfactual quantum control. The basic concept of counterfactual quantum control is presented and macro counterfactual quantum control is thoroughly discussed. In addition, related experimental verification and applied exploration are also discussed. This review paper covers the progress toward counterfactual quantum communication, non-invasive imaging and specific applications.</description>
	<pubDate>2026-01-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 6: Counterfactual Quantum Control: Review and Applications</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/6">doi: 10.3390/quantum8010006</a></p>
	<p>Authors:
		Na Hai
		Zijian Liu
		Bowen Zhang
		Tingyu Li
		Xiuqing Yang
		Zhenghong Li
		</p>
	<p>Counterfactual quantum control is a novel control method, in which no actual material particles or energy are transported and exchanged between the controller and the controlled. By introducing the quantum Zeno effect where the evolution of a quantum system can be suppressed by continuous observation, this paper presents a review of research progress in counterfactual quantum control. The basic concept of counterfactual quantum control is presented and macro counterfactual quantum control is thoroughly discussed. In addition, related experimental verification and applied exploration are also discussed. This review paper covers the progress toward counterfactual quantum communication, non-invasive imaging and specific applications.</p>
	]]></content:encoded>

	<dc:title>Counterfactual Quantum Control: Review and Applications</dc:title>
			<dc:creator>Na Hai</dc:creator>
			<dc:creator>Zijian Liu</dc:creator>
			<dc:creator>Bowen Zhang</dc:creator>
			<dc:creator>Tingyu Li</dc:creator>
			<dc:creator>Xiuqing Yang</dc:creator>
			<dc:creator>Zhenghong Li</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010006</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-19</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-19</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>6</prism:startingPage>
		<prism:doi>10.3390/quantum8010006</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/5">

	<title>Quantum Reports, Vol. 8, Pages 5: The Entropy Field Structure and the Recursive Collapse of the Electron: A Thermodynamic Foundation for Quantum Behavior</title>
	<link>https://www.mdpi.com/2624-960X/8/1/5</link>
	<description>Conventional quantum mechanics treats the electron as a point-like particle endowed with intrinsic properties&amp;amp;mdash;mass, charge, and spin&amp;amp;mdash;that are inserted as axioms rather than derived from first principles. Here, we propose a thermodynamic reformulation of the electron grounded in entropy field dynamics, based on S-Theory. In this framework, the electron is composed of three distinct entropic components: Score (a collapsed entropy core from configurational mass), SEM (a structured electromagnetic entropy field from charge), and Sthermal (a diffuse entropy component from ambient interactions). We show that spin emerges as a rotating SEM shell around Score, and that electron collapse&amp;amp;mdash;as in quantum measurement&amp;amp;mdash;can be modeled as a Recursive Amplification of Sfield (RAS) process driven by entropic feedback. Through mathematical formulation and high-resolution simulations, we demonstrate how the S-field components evolve under entropic excitation, culminating in a collapse threshold defined by local entropy density matching. This model not only explains the emergence of quantum properties but also offers a thermodynamic mechanism for electron&amp;amp;ndash;photon interaction, wavefunction collapse, and spin generation, revealing the inner structure and dynamics of one of nature&amp;amp;rsquo;s most fundamental particles.</description>
	<pubDate>2026-01-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 5: The Entropy Field Structure and the Recursive Collapse of the Electron: A Thermodynamic Foundation for Quantum Behavior</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/5">doi: 10.3390/quantum8010005</a></p>
	<p>Authors:
		John T. Solomon
		</p>
	<p>Conventional quantum mechanics treats the electron as a point-like particle endowed with intrinsic properties&amp;amp;mdash;mass, charge, and spin&amp;amp;mdash;that are inserted as axioms rather than derived from first principles. Here, we propose a thermodynamic reformulation of the electron grounded in entropy field dynamics, based on S-Theory. In this framework, the electron is composed of three distinct entropic components: Score (a collapsed entropy core from configurational mass), SEM (a structured electromagnetic entropy field from charge), and Sthermal (a diffuse entropy component from ambient interactions). We show that spin emerges as a rotating SEM shell around Score, and that electron collapse&amp;amp;mdash;as in quantum measurement&amp;amp;mdash;can be modeled as a Recursive Amplification of Sfield (RAS) process driven by entropic feedback. Through mathematical formulation and high-resolution simulations, we demonstrate how the S-field components evolve under entropic excitation, culminating in a collapse threshold defined by local entropy density matching. This model not only explains the emergence of quantum properties but also offers a thermodynamic mechanism for electron&amp;amp;ndash;photon interaction, wavefunction collapse, and spin generation, revealing the inner structure and dynamics of one of nature&amp;amp;rsquo;s most fundamental particles.</p>
	]]></content:encoded>

	<dc:title>The Entropy Field Structure and the Recursive Collapse of the Electron: A Thermodynamic Foundation for Quantum Behavior</dc:title>
			<dc:creator>John T. Solomon</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010005</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-17</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>5</prism:startingPage>
		<prism:doi>10.3390/quantum8010005</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/4">

	<title>Quantum Reports, Vol. 8, Pages 4: The Informational Birth of the Universe: A Theory of Everything from Quantum Complexity</title>
	<link>https://www.mdpi.com/2624-960X/8/1/4</link>
	<description>We propose a unified theoretical framework grounded in a Primordial Quantum Field (PQF)&amp;amp;mdash;a continuous, non-local informational substrate that precedes space-time and matter. The PQF is represented by a wave functional evolving in an abstract configuration space, where physical properties emerge through the self-organization of complexity. We introduce a novel physical quantity&amp;amp;mdash;complexity entropy Sc[&amp;amp;#981;]&amp;amp;mdash;which quantifies the structural organization of the PQF. Unlike traditional entropy measures (Shannon, von Neumann, Kolmogorov), Sc[&amp;amp;#981;] captures non-trivial coherence and functional correlations. We demonstrate how complexity gradients induce an emergent geometry, from which spacetime curvature, physical constants, and the arrow of time arise. The model predicts measurable phenomena such as entanglement waves and reinterprets dark energy as informational coherence pressure, suggesting empirical pathways for testing via highly correlated quantum systems.</description>
	<pubDate>2026-01-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 4: The Informational Birth of the Universe: A Theory of Everything from Quantum Complexity</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/4">doi: 10.3390/quantum8010004</a></p>
	<p>Authors:
		Gastón Sanglier Contreras
		Roberto Alonso González-Lezcano
		Eduardo J. López Fernández
		</p>
	<p>We propose a unified theoretical framework grounded in a Primordial Quantum Field (PQF)&amp;amp;mdash;a continuous, non-local informational substrate that precedes space-time and matter. The PQF is represented by a wave functional evolving in an abstract configuration space, where physical properties emerge through the self-organization of complexity. We introduce a novel physical quantity&amp;amp;mdash;complexity entropy Sc[&amp;amp;#981;]&amp;amp;mdash;which quantifies the structural organization of the PQF. Unlike traditional entropy measures (Shannon, von Neumann, Kolmogorov), Sc[&amp;amp;#981;] captures non-trivial coherence and functional correlations. We demonstrate how complexity gradients induce an emergent geometry, from which spacetime curvature, physical constants, and the arrow of time arise. The model predicts measurable phenomena such as entanglement waves and reinterprets dark energy as informational coherence pressure, suggesting empirical pathways for testing via highly correlated quantum systems.</p>
	]]></content:encoded>

	<dc:title>The Informational Birth of the Universe: A Theory of Everything from Quantum Complexity</dc:title>
			<dc:creator>Gastón Sanglier Contreras</dc:creator>
			<dc:creator>Roberto Alonso González-Lezcano</dc:creator>
			<dc:creator>Eduardo J. López Fernández</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010004</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-12</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/quantum8010004</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/3">

	<title>Quantum Reports, Vol. 8, Pages 3: Quantum Anomalies as Intrinsic Algebraic Curvature: A Unified AQFT Interpretation of Renormalization Ambiguities</title>
	<link>https://www.mdpi.com/2624-960X/8/1/3</link>
	<description>Quantum anomalies are traditionally understood as classical symmetries that fail to survive quantization, while experimental &amp;amp;ldquo;anomalies&amp;amp;rdquo; denote deviations between theoretical predictions and measured values. In this work, we develop a unified framework in which both phenomena can be interpreted through the lens of algebraic quantum field theory (AQFT). Building on the renormalization group viewed as an extension problem, we show that renormalization ambiguities correspond to nontrivial elements of Hochschild cohomology, giving rise to a deformation of the observable algebra A&amp;amp;lowast;B=AB+&amp;amp;epsilon;&amp;amp;omega;(A,B), where &amp;amp;omega; is a Hochschild 2-cocycle. We interpret &amp;amp;omega; as an intrinsic algebraic curvature of the net of local algebras, namely the (local) Hochschild class that measures the obstruction to trivializing infinitesimal scheme changes by inner redefinitions under locality and covariance constraints. The transported product is associative; its first-order expansion is associative up to O(&amp;amp;epsilon;2) while preserving the &amp;amp;lowast;-structure and Ward identities to the first order. We prove the existence of nontrivial cocycles in the perturbative AQFT setting, derive the conditions under which the deformed product respects positivity and locality, and establish the compatibility with current conservation. The construction provides a direct algebraic bridge to standard cohomological anomalies (chiral, trace, and gravitational) and yields correlated deformations of physical amplitudes. Fixing the small deformation parameter &amp;amp;epsilon; from the muon (g&amp;amp;minus;2) discrepancy, we propagate the framework to predictions for the electron (g&amp;amp;minus;2), charged lepton EDMs, and other low-energy observables. This approach reduces reliance on ad hoc form-factor parametrizations by organizing first-order scheme-induced deformations into correlation laws among low-energy observables. We argue that interpreting quantum anomalies as manifestations of algebraic curvature opens a pathway to a unified, testable account of renormalization ambiguities and their phenomenological consequences. We emphasize that the framework does not eliminate renormalization or quantum anomalies; rather, it repackages the finite renormalization freedom of pAQFT into cohomological data and relates it functorially to standard anomaly classes.</description>
	<pubDate>2026-01-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 3: Quantum Anomalies as Intrinsic Algebraic Curvature: A Unified AQFT Interpretation of Renormalization Ambiguities</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/3">doi: 10.3390/quantum8010003</a></p>
	<p>Authors:
		Andrei T. Patrascu
		</p>
	<p>Quantum anomalies are traditionally understood as classical symmetries that fail to survive quantization, while experimental &amp;amp;ldquo;anomalies&amp;amp;rdquo; denote deviations between theoretical predictions and measured values. In this work, we develop a unified framework in which both phenomena can be interpreted through the lens of algebraic quantum field theory (AQFT). Building on the renormalization group viewed as an extension problem, we show that renormalization ambiguities correspond to nontrivial elements of Hochschild cohomology, giving rise to a deformation of the observable algebra A&amp;amp;lowast;B=AB+&amp;amp;epsilon;&amp;amp;omega;(A,B), where &amp;amp;omega; is a Hochschild 2-cocycle. We interpret &amp;amp;omega; as an intrinsic algebraic curvature of the net of local algebras, namely the (local) Hochschild class that measures the obstruction to trivializing infinitesimal scheme changes by inner redefinitions under locality and covariance constraints. The transported product is associative; its first-order expansion is associative up to O(&amp;amp;epsilon;2) while preserving the &amp;amp;lowast;-structure and Ward identities to the first order. We prove the existence of nontrivial cocycles in the perturbative AQFT setting, derive the conditions under which the deformed product respects positivity and locality, and establish the compatibility with current conservation. The construction provides a direct algebraic bridge to standard cohomological anomalies (chiral, trace, and gravitational) and yields correlated deformations of physical amplitudes. Fixing the small deformation parameter &amp;amp;epsilon; from the muon (g&amp;amp;minus;2) discrepancy, we propagate the framework to predictions for the electron (g&amp;amp;minus;2), charged lepton EDMs, and other low-energy observables. This approach reduces reliance on ad hoc form-factor parametrizations by organizing first-order scheme-induced deformations into correlation laws among low-energy observables. We argue that interpreting quantum anomalies as manifestations of algebraic curvature opens a pathway to a unified, testable account of renormalization ambiguities and their phenomenological consequences. We emphasize that the framework does not eliminate renormalization or quantum anomalies; rather, it repackages the finite renormalization freedom of pAQFT into cohomological data and relates it functorially to standard anomaly classes.</p>
	]]></content:encoded>

	<dc:title>Quantum Anomalies as Intrinsic Algebraic Curvature: A Unified AQFT Interpretation of Renormalization Ambiguities</dc:title>
			<dc:creator>Andrei T. Patrascu</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010003</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2026-01-07</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2026-01-07</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/quantum8010003</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/2">

	<title>Quantum Reports, Vol. 8, Pages 2: Why Geometry Should Not Be Quantized: A Causal-Medium Unification of Gravity and Quantum Mechanics</title>
	<link>https://www.mdpi.com/2624-960X/8/1/2</link>
	<description>We revisit the premise that spacetime geometry must be quantized and show that this assumption is not physically required. Just as one does not quantize pressure or temperature, quantizing the metric treats a macroscopic continuum variable as if it were microscopic. We develop an alternative approach, Chronon Field Theory (ChFT), in which a smooth timelike covector &amp;amp;Phi;&amp;amp;mu; obeys a unified variational principle&amp;amp;mdash;the Temporal Coherence Principle (TCP). In appropriate long-wavelength and low-vorticity regimes, the TCP dynamics yield an emergent Lorentzian metric and reproduce the Einstein field equations to leading order. Phase-coherent excitations exhibit a universal invariant speed and admit an eikonal limit that reproduces Hamilton&amp;amp;ndash;Jacobi and Schr&amp;amp;ouml;dinger-type dynamics. Despite the presence of a microscopic causal alignment field, exact operational Lorentz invariance is preserved because all observers and measuring devices co-emerge from the same causal medium. The framework predicts small higher-order dispersive corrections to relativistic propagation while maintaining a universal causal cone, with effects constrained by fast radio burst and multi-messenger observations. ChFT thus provides a compact effective description in which gravitational and quantum dynamics emerge from a single coherence principle, without postulating quantum geometry at the fundamental level.</description>
	<pubDate>2025-12-31</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 2: Why Geometry Should Not Be Quantized: A Causal-Medium Unification of Gravity and Quantum Mechanics</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/2">doi: 10.3390/quantum8010002</a></p>
	<p>Authors:
		Bin Li
		</p>
	<p>We revisit the premise that spacetime geometry must be quantized and show that this assumption is not physically required. Just as one does not quantize pressure or temperature, quantizing the metric treats a macroscopic continuum variable as if it were microscopic. We develop an alternative approach, Chronon Field Theory (ChFT), in which a smooth timelike covector &amp;amp;Phi;&amp;amp;mu; obeys a unified variational principle&amp;amp;mdash;the Temporal Coherence Principle (TCP). In appropriate long-wavelength and low-vorticity regimes, the TCP dynamics yield an emergent Lorentzian metric and reproduce the Einstein field equations to leading order. Phase-coherent excitations exhibit a universal invariant speed and admit an eikonal limit that reproduces Hamilton&amp;amp;ndash;Jacobi and Schr&amp;amp;ouml;dinger-type dynamics. Despite the presence of a microscopic causal alignment field, exact operational Lorentz invariance is preserved because all observers and measuring devices co-emerge from the same causal medium. The framework predicts small higher-order dispersive corrections to relativistic propagation while maintaining a universal causal cone, with effects constrained by fast radio burst and multi-messenger observations. ChFT thus provides a compact effective description in which gravitational and quantum dynamics emerge from a single coherence principle, without postulating quantum geometry at the fundamental level.</p>
	]]></content:encoded>

	<dc:title>Why Geometry Should Not Be Quantized: A Causal-Medium Unification of Gravity and Quantum Mechanics</dc:title>
			<dc:creator>Bin Li</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010002</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-31</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-31</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/quantum8010002</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/8/1/1">

	<title>Quantum Reports, Vol. 8, Pages 1: On-Line Prediction of the Quantum Density Matrix</title>
	<link>https://www.mdpi.com/2624-960X/8/1/1</link>
	<description>Time evolution of open quantum systems is governed by the master equation. The master equation, which is a matrix formalism, is the time derivative of the density matrix, which contains the complete information on the state of a quantum system. Instead of implementing successive measurements on repeated identically prepared systems, which are inevitably imperfect and can only be performed a limited number of times, a state estimator can be designed to obtain the whole information about the state of a quantum system represented in a density matrix. Trace-one and positive semi-definite properties of the density matrix arising from physical constraints have to be preserved during state estimation in quantum systems. To address this challenge, we present a projection technique that incorporates Dykstra&amp;amp;rsquo;s algorithm and physical constraints into state estimation. This technique, which is an iterative method, ensures convergence and includes a designed oracle that projects the estimated state into intersections of admissible closed convex sets. The oracle structure is constructed using Hilbert projection, which looks for the best approximation of the projected estimated state within a Hilbert space into a closed convex set. According to the Hilbert projection theorem, this proposed oracle guarantees the existence and uniqueness of the best approximation of the projected state.</description>
	<pubDate>2025-12-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 8, Pages 1: On-Line Prediction of the Quantum Density Matrix</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/8/1/1">doi: 10.3390/quantum8010001</a></p>
	<p>Authors:
		Mehrzad Soltani
		Mark J. Balas
		</p>
	<p>Time evolution of open quantum systems is governed by the master equation. The master equation, which is a matrix formalism, is the time derivative of the density matrix, which contains the complete information on the state of a quantum system. Instead of implementing successive measurements on repeated identically prepared systems, which are inevitably imperfect and can only be performed a limited number of times, a state estimator can be designed to obtain the whole information about the state of a quantum system represented in a density matrix. Trace-one and positive semi-definite properties of the density matrix arising from physical constraints have to be preserved during state estimation in quantum systems. To address this challenge, we present a projection technique that incorporates Dykstra&amp;amp;rsquo;s algorithm and physical constraints into state estimation. This technique, which is an iterative method, ensures convergence and includes a designed oracle that projects the estimated state into intersections of admissible closed convex sets. The oracle structure is constructed using Hilbert projection, which looks for the best approximation of the projected estimated state within a Hilbert space into a closed convex set. According to the Hilbert projection theorem, this proposed oracle guarantees the existence and uniqueness of the best approximation of the projected state.</p>
	]]></content:encoded>

	<dc:title>On-Line Prediction of the Quantum Density Matrix</dc:title>
			<dc:creator>Mehrzad Soltani</dc:creator>
			<dc:creator>Mark J. Balas</dc:creator>
		<dc:identifier>doi: 10.3390/quantum8010001</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-22</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-22</prism:publicationDate>
	<prism:volume>8</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/quantum8010001</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/8/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/64">

	<title>Quantum Reports, Vol. 7, Pages 64: Quantum-Enhanced Facial Biometrics: A Hybrid Framework with Post-Quantum Security</title>
	<link>https://www.mdpi.com/2624-960X/7/4/64</link>
	<description>Face recognition systems are widely used for biometric authentication but face two major problems. First, processing high-resolution images and large databases requires extensive computational time. Second, emerging quantum computers threaten to break the encryption methods that protect stored facial templates. Quantum computers will soon be able to decrypt current security systems, putting biometric data at permanent risk since facial features cannot be changed like passwords. This paper presents a solution that uses quantum computing to speed up face recognition while adding quantum-resistant security. It applies quantum principal component analysis (QPCA) and the SWAP test to reduce the computational complexity and implement lattice-based cryptography, which quantum computers cannot break. Experimental evaluation demonstrates a significant overall speedup with improved accuracy. The proposed framework achieves a significant improvement in performance, provides 125-bit security against quantum attacks and compresses the data storage requirements significantly. These results demonstrate that quantum-enhanced face recognition can solve both the speed and security challenges facing current biometric systems, making it practical for real-world deployment as quantum technology advances.</description>
	<pubDate>2025-12-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 64: Quantum-Enhanced Facial Biometrics: A Hybrid Framework with Post-Quantum Security</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/64">doi: 10.3390/quantum7040064</a></p>
	<p>Authors:
		Satinder Singh
		Avnish Thakur
		Moin Hasan
		Guneet Singh Bhatia
		</p>
	<p>Face recognition systems are widely used for biometric authentication but face two major problems. First, processing high-resolution images and large databases requires extensive computational time. Second, emerging quantum computers threaten to break the encryption methods that protect stored facial templates. Quantum computers will soon be able to decrypt current security systems, putting biometric data at permanent risk since facial features cannot be changed like passwords. This paper presents a solution that uses quantum computing to speed up face recognition while adding quantum-resistant security. It applies quantum principal component analysis (QPCA) and the SWAP test to reduce the computational complexity and implement lattice-based cryptography, which quantum computers cannot break. Experimental evaluation demonstrates a significant overall speedup with improved accuracy. The proposed framework achieves a significant improvement in performance, provides 125-bit security against quantum attacks and compresses the data storage requirements significantly. These results demonstrate that quantum-enhanced face recognition can solve both the speed and security challenges facing current biometric systems, making it practical for real-world deployment as quantum technology advances.</p>
	]]></content:encoded>

	<dc:title>Quantum-Enhanced Facial Biometrics: A Hybrid Framework with Post-Quantum Security</dc:title>
			<dc:creator>Satinder Singh</dc:creator>
			<dc:creator>Avnish Thakur</dc:creator>
			<dc:creator>Moin Hasan</dc:creator>
			<dc:creator>Guneet Singh Bhatia</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040064</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-15</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-15</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>64</prism:startingPage>
		<prism:doi>10.3390/quantum7040064</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/64</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/63">

	<title>Quantum Reports, Vol. 7, Pages 63: The Dirac Equation in a Linear Potential and Quantized Electromagnetic Field: Spin&amp;ndash;Rest Entanglement</title>
	<link>https://www.mdpi.com/2624-960X/7/4/63</link>
	<description>We derive the exact eigenfunctions and energy equation for a Dirac particle in a monochromatic quantized electromagnetic plane wave and a confining scalar linear potential. It is shown that the system&amp;amp;rsquo;s energy spectrum exhibits a forbidden region that vanishes when the particle&amp;amp;ndash;field interaction is switched off. We then analyze the effect of particle&amp;amp;ndash;field coupling on quantum entanglement between the particle&amp;amp;rsquo;s spin and the remaining degrees of freedom. Our results show that the profile of the spin&amp;amp;ndash;rest entanglement, measured by negativity and Von Neumann entropy, follows the energy profile of the state: it is monotonic when the energy is monotonic, and non-monotonic otherwise. These results may provide insights into quantum correlations in Dirac-like systems describing low-energy excitations of graphene and trapped ions.</description>
	<pubDate>2025-12-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 63: The Dirac Equation in a Linear Potential and Quantized Electromagnetic Field: Spin&amp;ndash;Rest Entanglement</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/63">doi: 10.3390/quantum7040063</a></p>
	<p>Authors:
		Yassine Chargui
		Sultan Al-Harbi
		</p>
	<p>We derive the exact eigenfunctions and energy equation for a Dirac particle in a monochromatic quantized electromagnetic plane wave and a confining scalar linear potential. It is shown that the system&amp;amp;rsquo;s energy spectrum exhibits a forbidden region that vanishes when the particle&amp;amp;ndash;field interaction is switched off. We then analyze the effect of particle&amp;amp;ndash;field coupling on quantum entanglement between the particle&amp;amp;rsquo;s spin and the remaining degrees of freedom. Our results show that the profile of the spin&amp;amp;ndash;rest entanglement, measured by negativity and Von Neumann entropy, follows the energy profile of the state: it is monotonic when the energy is monotonic, and non-monotonic otherwise. These results may provide insights into quantum correlations in Dirac-like systems describing low-energy excitations of graphene and trapped ions.</p>
	]]></content:encoded>

	<dc:title>The Dirac Equation in a Linear Potential and Quantized Electromagnetic Field: Spin&amp;amp;ndash;Rest Entanglement</dc:title>
			<dc:creator>Yassine Chargui</dc:creator>
			<dc:creator>Sultan Al-Harbi</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040063</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-12</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>63</prism:startingPage>
		<prism:doi>10.3390/quantum7040063</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/63</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/62">

	<title>Quantum Reports, Vol. 7, Pages 62: Quantum Monogamy with Predetermined Events</title>
	<link>https://www.mdpi.com/2624-960X/7/4/62</link>
	<description>The concept of correlation appears straightforward: measurement outcomes coincide, and patterns emerge. For any record of events, the coefficients are uniquely determined. Thus, if correlations change spontaneously, as seen in quantum monogamy, then individual behavior must have changed first. Surprisingly, this is not always true. When two observables are mutually exclusive, they cannot coincide objectively and need to be grouped across time. Yet, sectioning the flow of events into &amp;amp;ldquo;iterations&amp;amp;rdquo; is not trivial in this case. Even with blind windows of coincidence, the same order of outcomes can produce different coefficients of correlation, depending on the number of joint measurements. Therefore, quantum monogamy can happen with fixed pre-determined events. A new concept (&amp;amp;ldquo;subjective correlation&amp;amp;rdquo;) is required to explain this phenomenon.</description>
	<pubDate>2025-12-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 62: Quantum Monogamy with Predetermined Events</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/62">doi: 10.3390/quantum7040062</a></p>
	<p>Authors:
		Ghenadie N. Mardari
		</p>
	<p>The concept of correlation appears straightforward: measurement outcomes coincide, and patterns emerge. For any record of events, the coefficients are uniquely determined. Thus, if correlations change spontaneously, as seen in quantum monogamy, then individual behavior must have changed first. Surprisingly, this is not always true. When two observables are mutually exclusive, they cannot coincide objectively and need to be grouped across time. Yet, sectioning the flow of events into &amp;amp;ldquo;iterations&amp;amp;rdquo; is not trivial in this case. Even with blind windows of coincidence, the same order of outcomes can produce different coefficients of correlation, depending on the number of joint measurements. Therefore, quantum monogamy can happen with fixed pre-determined events. A new concept (&amp;amp;ldquo;subjective correlation&amp;amp;rdquo;) is required to explain this phenomenon.</p>
	]]></content:encoded>

	<dc:title>Quantum Monogamy with Predetermined Events</dc:title>
			<dc:creator>Ghenadie N. Mardari</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040062</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-11</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-11</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>62</prism:startingPage>
		<prism:doi>10.3390/quantum7040062</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/62</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/61">

	<title>Quantum Reports, Vol. 7, Pages 61: Geometric Origin of Quantum Waves from Finite Action</title>
	<link>https://www.mdpi.com/2624-960X/7/4/61</link>
	<description>Quantum mechanics postulates wave&amp;amp;ndash;particle duality and assigns amplitudes of the form eiS/&amp;amp;#8463;, yet no existing formulation explains why physical observables depend only on the phase of the action. Here we show that if the quantum of action &amp;amp;#8463;geom is finite, the classical action manifold R becomes compact under the identification S&amp;amp;equiv;S+2&amp;amp;pi;&amp;amp;#8463;geom, yielding a U(1) action space on which only modular action is observable. Wave interference then follows as a geometric necessity: a finite action quantum forces physical amplitudes to live on a circle, while the classical limit arises when the modular spacing 2&amp;amp;pi;&amp;amp;#8463;geom becomes negligible compared with macroscopic actions. We formulate this as a compact-action theorem. Chronon Field Theory (ChFT) provides the physical origin of &amp;amp;#8463;geom: its causal field &amp;amp;Phi;&amp;amp;mu; carries a quantized symplectic flux &amp;amp;#8750;&amp;amp;omega;=&amp;amp;#8463;geom, making Planck&amp;amp;rsquo;s constant a geometric topological invariant rather than an imposed parameter. Within this medium, the Real&amp;amp;ndash;Now&amp;amp;ndash;Front (RNF) supplies a local reconstruction rule that reproduces the structure of the Feynman path integral, the Schr&amp;amp;ouml;dinger evolution, the Born rule, and macroscopic definiteness as consequences of geometric compatibility rather than supplemental postulates. Phenomenologically, identifying the electron as the minimal chronon soliton&amp;amp;mdash;carrying the fundamental unit of symplectic flux&amp;amp;mdash;links its spin, charge, and stability to topological properties of the chronon field, yielding concrete experimental signatures. Thus the compact-action/RNF framework provides a unified geometric origin for quantum interference, measurement, and matter, together with falsifiable predictions of ChFT.</description>
	<pubDate>2025-12-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 61: Geometric Origin of Quantum Waves from Finite Action</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/61">doi: 10.3390/quantum7040061</a></p>
	<p>Authors:
		Bin Li
		</p>
	<p>Quantum mechanics postulates wave&amp;amp;ndash;particle duality and assigns amplitudes of the form eiS/&amp;amp;#8463;, yet no existing formulation explains why physical observables depend only on the phase of the action. Here we show that if the quantum of action &amp;amp;#8463;geom is finite, the classical action manifold R becomes compact under the identification S&amp;amp;equiv;S+2&amp;amp;pi;&amp;amp;#8463;geom, yielding a U(1) action space on which only modular action is observable. Wave interference then follows as a geometric necessity: a finite action quantum forces physical amplitudes to live on a circle, while the classical limit arises when the modular spacing 2&amp;amp;pi;&amp;amp;#8463;geom becomes negligible compared with macroscopic actions. We formulate this as a compact-action theorem. Chronon Field Theory (ChFT) provides the physical origin of &amp;amp;#8463;geom: its causal field &amp;amp;Phi;&amp;amp;mu; carries a quantized symplectic flux &amp;amp;#8750;&amp;amp;omega;=&amp;amp;#8463;geom, making Planck&amp;amp;rsquo;s constant a geometric topological invariant rather than an imposed parameter. Within this medium, the Real&amp;amp;ndash;Now&amp;amp;ndash;Front (RNF) supplies a local reconstruction rule that reproduces the structure of the Feynman path integral, the Schr&amp;amp;ouml;dinger evolution, the Born rule, and macroscopic definiteness as consequences of geometric compatibility rather than supplemental postulates. Phenomenologically, identifying the electron as the minimal chronon soliton&amp;amp;mdash;carrying the fundamental unit of symplectic flux&amp;amp;mdash;links its spin, charge, and stability to topological properties of the chronon field, yielding concrete experimental signatures. Thus the compact-action/RNF framework provides a unified geometric origin for quantum interference, measurement, and matter, together with falsifiable predictions of ChFT.</p>
	]]></content:encoded>

	<dc:title>Geometric Origin of Quantum Waves from Finite Action</dc:title>
			<dc:creator>Bin Li</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040061</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-08</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-08</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>61</prism:startingPage>
		<prism:doi>10.3390/quantum7040061</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/61</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/60">

	<title>Quantum Reports, Vol. 7, Pages 60: Classical and Quantum Linear Wave Equations: Review, Applications and Perspectives</title>
	<link>https://www.mdpi.com/2624-960X/7/4/60</link>
	<description>Theories of modern physics are based on dynamical equations that describe the evolution of particles and waves in space and time. In classical physics, particles and waves are described by different equations, but this distinction disappears in quantum physics, which is predominantly based on wave-like equations. The main purpose of this paper is to present a comprehensive review of all known classical and quantum linear wave equations for scalar wavefunctions, and to discuss their origin and applications to a broad range of physical problems.</description>
	<pubDate>2025-12-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 60: Classical and Quantum Linear Wave Equations: Review, Applications and Perspectives</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/60">doi: 10.3390/quantum7040060</a></p>
	<p>Authors:
		Zdzislaw E. Musielak
		</p>
	<p>Theories of modern physics are based on dynamical equations that describe the evolution of particles and waves in space and time. In classical physics, particles and waves are described by different equations, but this distinction disappears in quantum physics, which is predominantly based on wave-like equations. The main purpose of this paper is to present a comprehensive review of all known classical and quantum linear wave equations for scalar wavefunctions, and to discuss their origin and applications to a broad range of physical problems.</p>
	]]></content:encoded>

	<dc:title>Classical and Quantum Linear Wave Equations: Review, Applications and Perspectives</dc:title>
			<dc:creator>Zdzislaw E. Musielak</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040060</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-05</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-05</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>60</prism:startingPage>
		<prism:doi>10.3390/quantum7040060</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/60</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/59">

	<title>Quantum Reports, Vol. 7, Pages 59: A New Space-Time Theory Unravels the Origins of Classical Mechanics for the Dirac Equation</title>
	<link>https://www.mdpi.com/2624-960X/7/4/59</link>
	<description>The Feynman path integral plays a central role in quantum mechanics, linking classical action to propagators and relating quantum electrodynamics (QED) to Feynman diagrams. However, the path-integral formulations used in non-relativistic quantum mechanics and in QED are neither unified nor directly connected. This suggests the existence of a missing path integral that bridges relativistic action and the Dirac equation at the single-particle level. In this work, we analyze the consistency and completeness of existing path-integral theories and identify a spinor path integral that fills this gap. Starting from a relativistic action written in spinor form, we construct a spacetime path integral whose kernel reproduces the Dirac Hamiltonian. The resulting formulation provides a direct link between the relativistic classical action and the Dirac equation, and it naturally extends the scalar relativistic path integral developed in our earlier work. Beyond establishing this structural connection, the spinor path integral offers a new way to interpret the origin of classical mechanics for the Dirac equation and suggests a spacetime mechanism for spin and quantum nonlocal correlations. These features indicate that the spinor path integral can serve as a unifying framework for existing path-integral approaches and as a starting point for further investigations into the spacetime structure of quantum mechanics.</description>
	<pubDate>2025-12-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 59: A New Space-Time Theory Unravels the Origins of Classical Mechanics for the Dirac Equation</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/59">doi: 10.3390/quantum7040059</a></p>
	<p>Authors:
		Wei Wen
		</p>
	<p>The Feynman path integral plays a central role in quantum mechanics, linking classical action to propagators and relating quantum electrodynamics (QED) to Feynman diagrams. However, the path-integral formulations used in non-relativistic quantum mechanics and in QED are neither unified nor directly connected. This suggests the existence of a missing path integral that bridges relativistic action and the Dirac equation at the single-particle level. In this work, we analyze the consistency and completeness of existing path-integral theories and identify a spinor path integral that fills this gap. Starting from a relativistic action written in spinor form, we construct a spacetime path integral whose kernel reproduces the Dirac Hamiltonian. The resulting formulation provides a direct link between the relativistic classical action and the Dirac equation, and it naturally extends the scalar relativistic path integral developed in our earlier work. Beyond establishing this structural connection, the spinor path integral offers a new way to interpret the origin of classical mechanics for the Dirac equation and suggests a spacetime mechanism for spin and quantum nonlocal correlations. These features indicate that the spinor path integral can serve as a unifying framework for existing path-integral approaches and as a starting point for further investigations into the spacetime structure of quantum mechanics.</p>
	]]></content:encoded>

	<dc:title>A New Space-Time Theory Unravels the Origins of Classical Mechanics for the Dirac Equation</dc:title>
			<dc:creator>Wei Wen</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040059</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-12-03</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-12-03</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>59</prism:startingPage>
		<prism:doi>10.3390/quantum7040059</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/59</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/58">

	<title>Quantum Reports, Vol. 7, Pages 58: Quantum Behavior in a Non-Bonded Interaction of BN (+, &amp;minus;, 0) B @ (5, 5) BN: Second-Order Jahn&amp;ndash;Teller Effect Causes Symmetry Breaking</title>
	<link>https://www.mdpi.com/2624-960X/7/4/58</link>
	<description>The anion, cation, and radical structural forms of B2N (&amp;amp;minus;,0,+) were studied in the case of symmetry breaking (SB) inside a (5, 5) BN nanotube ring and were also compared in terms of non-covalent interaction between these two parts. The non-bonded system of B2N (&amp;amp;minus;,0,+) and the (5, 5) BN nanotube not only causes SB for BNB but also creates an energy barrier in the range of 10&amp;amp;minus;3 Hartree of due to this non-bonded interaction. Moreover, several SBs appear via asymmetry stretching and symmetry bending normal mode interactions according to the multiple second-order Jahn&amp;amp;ndash;Teller effect. We also demonstrated that the twin minimum of BNB&amp;amp;rsquo;s potential curve arises from the lack of a proper wave function with permutation symmetry, as well as abnormal charge distribution. Through this investigation, considerable enhancements in the energy barriers due to the SB effect were also observed during the electrostatic interaction of BNB (both radical and cation) with the BN nanotube ring. Additionally, these values were not observed for the isolated B2N (&amp;amp;minus;,0,+) forms. This non-bonded complex operates as a quantum rotatory model and as a catalyst for producing a range of spectra in the IR region due to the alternative attraction and repulsion forces.</description>
	<pubDate>2025-11-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 58: Quantum Behavior in a Non-Bonded Interaction of BN (+, &amp;minus;, 0) B @ (5, 5) BN: Second-Order Jahn&amp;ndash;Teller Effect Causes Symmetry Breaking</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/58">doi: 10.3390/quantum7040058</a></p>
	<p>Authors:
		Majid Monajjemi
		Fatemeh Mollaamin
		</p>
	<p>The anion, cation, and radical structural forms of B2N (&amp;amp;minus;,0,+) were studied in the case of symmetry breaking (SB) inside a (5, 5) BN nanotube ring and were also compared in terms of non-covalent interaction between these two parts. The non-bonded system of B2N (&amp;amp;minus;,0,+) and the (5, 5) BN nanotube not only causes SB for BNB but also creates an energy barrier in the range of 10&amp;amp;minus;3 Hartree of due to this non-bonded interaction. Moreover, several SBs appear via asymmetry stretching and symmetry bending normal mode interactions according to the multiple second-order Jahn&amp;amp;ndash;Teller effect. We also demonstrated that the twin minimum of BNB&amp;amp;rsquo;s potential curve arises from the lack of a proper wave function with permutation symmetry, as well as abnormal charge distribution. Through this investigation, considerable enhancements in the energy barriers due to the SB effect were also observed during the electrostatic interaction of BNB (both radical and cation) with the BN nanotube ring. Additionally, these values were not observed for the isolated B2N (&amp;amp;minus;,0,+) forms. This non-bonded complex operates as a quantum rotatory model and as a catalyst for producing a range of spectra in the IR region due to the alternative attraction and repulsion forces.</p>
	]]></content:encoded>

	<dc:title>Quantum Behavior in a Non-Bonded Interaction of BN (+, &amp;amp;minus;, 0) B @ (5, 5) BN: Second-Order Jahn&amp;amp;ndash;Teller Effect Causes Symmetry Breaking</dc:title>
			<dc:creator>Majid Monajjemi</dc:creator>
			<dc:creator>Fatemeh Mollaamin</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040058</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-30</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-30</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>58</prism:startingPage>
		<prism:doi>10.3390/quantum7040058</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/58</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/57">

	<title>Quantum Reports, Vol. 7, Pages 57: Sequential Quantum Measurements and the Instrumental Group Algebra</title>
	<link>https://www.mdpi.com/2624-960X/7/4/57</link>
	<description>Many of the most fundamental observables&amp;amp;mdash;position, momentum, phase point, and spin direction&amp;amp;mdash;cannot be measured by an instrument that obeys the orthogonal projection postulate. Continuous-in-time measurements provide the missing theoretical framework to make physical sense of such observables. The elements of the time-dependent instrument define a group called the instrumental group (IG). Relative to the IG, all of the time dependence is contained in a certain function called the Kraus-operator density (KOD), which evolves according to a classical Kolmogorov equation. Unlike the Lindblad master equation, the KOD Kolmogorov equation is a direct expression of how the elements of the instrument (not just the total quantum channel) evolve. Shifting from continuous measurements to sequential measurements more generally, the structure of combining instruments in sequence is shown to correspond to the convolution of their KODs. This convolution promotes the IG to an involutive Banach algebra (a structure that goes all the way back to the origins of POVM and C*-algebra theory), which will be called the instrumental group algebra (IGA). The IGA is the true home of the KOD, similar to how the dual of a von Neumann algebra is the true home of the density operator. Operators on the IGA, which play the analogous role for KODs as superoperators play for density operators, are called ultraoperators and various important examples are discussed. Certain ultraoperator&amp;amp;ndash;superoperator intertwining relationships are also considered throughout, including the relationship between the KOD Kolmogorov equation and the Lindblad master equation. The IGA is also shown to have actually two distinct involutions: one respected by the convolution ultraoperators and the other by the quantum channel superoperators. Finally, the KOD Kolmogorov generators are derived for jump processes and more general diffusive processes.</description>
	<pubDate>2025-11-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 57: Sequential Quantum Measurements and the Instrumental Group Algebra</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/57">doi: 10.3390/quantum7040057</a></p>
	<p>Authors:
		Christopher S. Jackson
		</p>
	<p>Many of the most fundamental observables&amp;amp;mdash;position, momentum, phase point, and spin direction&amp;amp;mdash;cannot be measured by an instrument that obeys the orthogonal projection postulate. Continuous-in-time measurements provide the missing theoretical framework to make physical sense of such observables. The elements of the time-dependent instrument define a group called the instrumental group (IG). Relative to the IG, all of the time dependence is contained in a certain function called the Kraus-operator density (KOD), which evolves according to a classical Kolmogorov equation. Unlike the Lindblad master equation, the KOD Kolmogorov equation is a direct expression of how the elements of the instrument (not just the total quantum channel) evolve. Shifting from continuous measurements to sequential measurements more generally, the structure of combining instruments in sequence is shown to correspond to the convolution of their KODs. This convolution promotes the IG to an involutive Banach algebra (a structure that goes all the way back to the origins of POVM and C*-algebra theory), which will be called the instrumental group algebra (IGA). The IGA is the true home of the KOD, similar to how the dual of a von Neumann algebra is the true home of the density operator. Operators on the IGA, which play the analogous role for KODs as superoperators play for density operators, are called ultraoperators and various important examples are discussed. Certain ultraoperator&amp;amp;ndash;superoperator intertwining relationships are also considered throughout, including the relationship between the KOD Kolmogorov equation and the Lindblad master equation. The IGA is also shown to have actually two distinct involutions: one respected by the convolution ultraoperators and the other by the quantum channel superoperators. Finally, the KOD Kolmogorov generators are derived for jump processes and more general diffusive processes.</p>
	]]></content:encoded>

	<dc:title>Sequential Quantum Measurements and the Instrumental Group Algebra</dc:title>
			<dc:creator>Christopher S. Jackson</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040057</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-30</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-30</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>57</prism:startingPage>
		<prism:doi>10.3390/quantum7040057</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/57</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/56">

	<title>Quantum Reports, Vol. 7, Pages 56: Applications of Gaussian Boson Sampling to Solve Some Chemistry Problems</title>
	<link>https://www.mdpi.com/2624-960X/7/4/56</link>
	<description>Quantum computers, due to their superposition and entanglement properties, provide significant advantages in solving certain problems compared with classical computers. Therefore, it is crucial to identify issues that can be efficiently solved by noisy intermediate-scale quantum (NISQ) systems. Xanadu has introduced the X8 quantum chip, based on integrated photonic technology, along with important photonic platforms such as Strawberry Fields and Gaussian Boson Sampling (GBS), to solve specific computational problems. In this review article, after reviewing Boson Sampling (BS) and Gaussian Boson Sampling (GBS), we discuss the relationship between GBS and graph theory, including how graphs can be encoded in GBS. Some applications of GBS, particularly molecular docking and molecular vibrations, are also considered. The future goal of this study is to identify problems that can be represented as small graphs and solved using GBS with a limited number of optical modes.</description>
	<pubDate>2025-11-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 56: Applications of Gaussian Boson Sampling to Solve Some Chemistry Problems</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/56">doi: 10.3390/quantum7040056</a></p>
	<p>Authors:
		Samaneh Bagheri Novir
		</p>
	<p>Quantum computers, due to their superposition and entanglement properties, provide significant advantages in solving certain problems compared with classical computers. Therefore, it is crucial to identify issues that can be efficiently solved by noisy intermediate-scale quantum (NISQ) systems. Xanadu has introduced the X8 quantum chip, based on integrated photonic technology, along with important photonic platforms such as Strawberry Fields and Gaussian Boson Sampling (GBS), to solve specific computational problems. In this review article, after reviewing Boson Sampling (BS) and Gaussian Boson Sampling (GBS), we discuss the relationship between GBS and graph theory, including how graphs can be encoded in GBS. Some applications of GBS, particularly molecular docking and molecular vibrations, are also considered. The future goal of this study is to identify problems that can be represented as small graphs and solved using GBS with a limited number of optical modes.</p>
	]]></content:encoded>

	<dc:title>Applications of Gaussian Boson Sampling to Solve Some Chemistry Problems</dc:title>
			<dc:creator>Samaneh Bagheri Novir</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040056</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-28</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-28</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>56</prism:startingPage>
		<prism:doi>10.3390/quantum7040056</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/56</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/55">

	<title>Quantum Reports, Vol. 7, Pages 55: Quaternionic and Octonionic Frameworks for Quantum Computation: Mathematical Structures, Models, and Fundamental Limitations</title>
	<link>https://www.mdpi.com/2624-960X/7/4/55</link>
	<description>We develop detailed quaternionic and octonionic frameworks for quantum computation grounded on normed division algebras. Our central result is to prove the polynomial computational equivalence of quaternionic and complex quantum models: Computation over H is polynomially equivalent to the standard complex quantum circuit model and hence captures the same complexity class BQP up to polynomial reductions. Over H, we construct a complete model&amp;amp;mdash;quaternionic qubits on right H-modules with quaternion-valued inner products, unitary dynamics, associative tensor products, and universal gate sets&amp;amp;mdash;and establish polynomial equivalence with the standard complex model; routes for implementation at fidelities exceeding 99% via pulse-level synthesis on current hardware are discussed. Over O, non-associativity yields path-dependent evolution, ambiguous adjoints/inner products, non-associative tensor products, and possible failure of energy conservation outside associative sectors. We formalize these obstructions and systematize four mitigation strategies: Confinement to associative subalgebras, G2-invariant codes, dynamical decoupling of associator terms, and a seven-factor algebraic decomposition for gate synthesis. The results delineate the feasible quaternionic regime from the constrained octonionic landscape and point to applications in symmetry-protected architectures, algebra-aware simulation, and hypercomplex learning.</description>
	<pubDate>2025-11-26</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 55: Quaternionic and Octonionic Frameworks for Quantum Computation: Mathematical Structures, Models, and Fundamental Limitations</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/55">doi: 10.3390/quantum7040055</a></p>
	<p>Authors:
		Johan Heriberto Rúa Muñoz
		Jorge Eduardo Mahecha Gómez
		Santiago Pineda Montoya
		</p>
	<p>We develop detailed quaternionic and octonionic frameworks for quantum computation grounded on normed division algebras. Our central result is to prove the polynomial computational equivalence of quaternionic and complex quantum models: Computation over H is polynomially equivalent to the standard complex quantum circuit model and hence captures the same complexity class BQP up to polynomial reductions. Over H, we construct a complete model&amp;amp;mdash;quaternionic qubits on right H-modules with quaternion-valued inner products, unitary dynamics, associative tensor products, and universal gate sets&amp;amp;mdash;and establish polynomial equivalence with the standard complex model; routes for implementation at fidelities exceeding 99% via pulse-level synthesis on current hardware are discussed. Over O, non-associativity yields path-dependent evolution, ambiguous adjoints/inner products, non-associative tensor products, and possible failure of energy conservation outside associative sectors. We formalize these obstructions and systematize four mitigation strategies: Confinement to associative subalgebras, G2-invariant codes, dynamical decoupling of associator terms, and a seven-factor algebraic decomposition for gate synthesis. The results delineate the feasible quaternionic regime from the constrained octonionic landscape and point to applications in symmetry-protected architectures, algebra-aware simulation, and hypercomplex learning.</p>
	]]></content:encoded>

	<dc:title>Quaternionic and Octonionic Frameworks for Quantum Computation: Mathematical Structures, Models, and Fundamental Limitations</dc:title>
			<dc:creator>Johan Heriberto Rúa Muñoz</dc:creator>
			<dc:creator>Jorge Eduardo Mahecha Gómez</dc:creator>
			<dc:creator>Santiago Pineda Montoya</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040055</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-26</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-26</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>55</prism:startingPage>
		<prism:doi>10.3390/quantum7040055</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/55</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/54">

	<title>Quantum Reports, Vol. 7, Pages 54: Brownian Particles and Matter Waves</title>
	<link>https://www.mdpi.com/2624-960X/7/4/54</link>
	<description>In view of the remarkable progress in microrheology to monitor the random motion of Brownian particles with a size as small as a few nanometers, and given that de Broglie matter waves have been experimentally observed for large molecules of comparable nanometer size, we examine whether Brownian particles can manifest a particle-wave duality without employing a priori arguments from quantum decoherence. First, we examine the case where Brownian particles are immersed in a memoryless viscous fluid with a time-independent diffusion coefficient, and the requirement for the Brownian particles to manifest a particle-wave duality leads to the untenable result that the diffusion coefficient has to be proportional to the inverse time, therefore, diverging at early times. This finding agrees with past conclusions published in the literature, that quantum mechanics is not equivalent to a Markovian diffusion process. Next, we examine the case where the Brownian particle is trapped in a harmonic potential well with and without dissipation. Both solutions of the Fokker&amp;amp;ndash;Planck equation for the case with dissipation, and of the Schr&amp;amp;ouml;dinger equation for the case without dissipation, lead to the same physically acceptable result&amp;amp;mdash;that for the Brownian particle to manifest a particle-wave duality, its mean kinetic energy kBT/2 needs to be &amp;amp;frac12; the ground-state energy, E0=12&amp;amp;#8463;&amp;amp;omega; of the quantum harmonic oscillator. Our one-dimensional calculations show that for this to happen, the trapping needs to be very strong so that a Brownian particle with mass m and radius R needs to be embedded in an extremely stiff solid with shear modulus, G proportional to m/RkBT/&amp;amp;#8463;2.</description>
	<pubDate>2025-11-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 54: Brownian Particles and Matter Waves</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/54">doi: 10.3390/quantum7040054</a></p>
	<p>Authors:
		Nicos Makris
		</p>
	<p>In view of the remarkable progress in microrheology to monitor the random motion of Brownian particles with a size as small as a few nanometers, and given that de Broglie matter waves have been experimentally observed for large molecules of comparable nanometer size, we examine whether Brownian particles can manifest a particle-wave duality without employing a priori arguments from quantum decoherence. First, we examine the case where Brownian particles are immersed in a memoryless viscous fluid with a time-independent diffusion coefficient, and the requirement for the Brownian particles to manifest a particle-wave duality leads to the untenable result that the diffusion coefficient has to be proportional to the inverse time, therefore, diverging at early times. This finding agrees with past conclusions published in the literature, that quantum mechanics is not equivalent to a Markovian diffusion process. Next, we examine the case where the Brownian particle is trapped in a harmonic potential well with and without dissipation. Both solutions of the Fokker&amp;amp;ndash;Planck equation for the case with dissipation, and of the Schr&amp;amp;ouml;dinger equation for the case without dissipation, lead to the same physically acceptable result&amp;amp;mdash;that for the Brownian particle to manifest a particle-wave duality, its mean kinetic energy kBT/2 needs to be &amp;amp;frac12; the ground-state energy, E0=12&amp;amp;#8463;&amp;amp;omega; of the quantum harmonic oscillator. Our one-dimensional calculations show that for this to happen, the trapping needs to be very strong so that a Brownian particle with mass m and radius R needs to be embedded in an extremely stiff solid with shear modulus, G proportional to m/RkBT/&amp;amp;#8463;2.</p>
	]]></content:encoded>

	<dc:title>Brownian Particles and Matter Waves</dc:title>
			<dc:creator>Nicos Makris</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040054</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-13</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>54</prism:startingPage>
		<prism:doi>10.3390/quantum7040054</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/54</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/53">

	<title>Quantum Reports, Vol. 7, Pages 53: Is Quantum Field Theory Necessarily &amp;ldquo;Quantum&amp;rdquo;?</title>
	<link>https://www.mdpi.com/2624-960X/7/4/53</link>
	<description>The mathematical universe of the quantum topos, which is formulated on the basis of classical Boolean snapshots, delivers a neo-realist description of quantum mechanics that preserves realism. The main contribution of this article is developing formal objectivity in physical theories beyond quantum mechanics in the topos-theory approach. It will be shown that neo-realist responses to non-perturbative structures of quantum field theory do not preserve realism. In this regard, the method of Feynman graphons is applied to reframe the task of describing objectivity in quantum field theory in terms of replacing the standard Hilbert-space/operator-algebra ontology with a new context category built from a certain family of topological Hopf subalgebras of the topological Hopf algebra of renormalization as algebraic/combinatorial data tied to non-perturbative structures. This topological-Hopf-algebra ontology, which is independent of instrumentalist probabilities, enables us to reconstruct gauge field theories on the basis of the mathematical universe of the non-perturbative topos. The non-Boolean logic of the non-perturbative topos cannot be recovered by classical Boolean snapshots, which is in contrast to the quantum-topos reformulation of quantum mechanics. The article formulates a universal version of the non-perturbative topos to show that quantum field theory is a globally and locally neo-realist theory which can be reconstructed independent of the standard Hilbert-space/operator-algebra ontology. Formal objectivity of the universal non-perturbative topos offers a new route to build objective semantics for non-perturbative structures.</description>
	<pubDate>2025-11-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 53: Is Quantum Field Theory Necessarily &amp;ldquo;Quantum&amp;rdquo;?</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/53">doi: 10.3390/quantum7040053</a></p>
	<p>Authors:
		Ali Shojaei-Fard
		</p>
	<p>The mathematical universe of the quantum topos, which is formulated on the basis of classical Boolean snapshots, delivers a neo-realist description of quantum mechanics that preserves realism. The main contribution of this article is developing formal objectivity in physical theories beyond quantum mechanics in the topos-theory approach. It will be shown that neo-realist responses to non-perturbative structures of quantum field theory do not preserve realism. In this regard, the method of Feynman graphons is applied to reframe the task of describing objectivity in quantum field theory in terms of replacing the standard Hilbert-space/operator-algebra ontology with a new context category built from a certain family of topological Hopf subalgebras of the topological Hopf algebra of renormalization as algebraic/combinatorial data tied to non-perturbative structures. This topological-Hopf-algebra ontology, which is independent of instrumentalist probabilities, enables us to reconstruct gauge field theories on the basis of the mathematical universe of the non-perturbative topos. The non-Boolean logic of the non-perturbative topos cannot be recovered by classical Boolean snapshots, which is in contrast to the quantum-topos reformulation of quantum mechanics. The article formulates a universal version of the non-perturbative topos to show that quantum field theory is a globally and locally neo-realist theory which can be reconstructed independent of the standard Hilbert-space/operator-algebra ontology. Formal objectivity of the universal non-perturbative topos offers a new route to build objective semantics for non-perturbative structures.</p>
	]]></content:encoded>

	<dc:title>Is Quantum Field Theory Necessarily &amp;amp;ldquo;Quantum&amp;amp;rdquo;?</dc:title>
			<dc:creator>Ali Shojaei-Fard</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040053</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-01</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>53</prism:startingPage>
		<prism:doi>10.3390/quantum7040053</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/53</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/52">

	<title>Quantum Reports, Vol. 7, Pages 52: The Radical Pair Mechanism and Its Quantum Role in Plant Reactive Oxygen Species Production Under Hypomagnetic Fields</title>
	<link>https://www.mdpi.com/2624-960X/7/4/52</link>
	<description>The Earth&amp;amp;rsquo;s geomagnetic field (GMF) is a fundamental environmental signal for plants, with its perception rooted in quantum biology. Specifically, the radical pair mechanism (RPM) explains how this weak force influences electron spin states in metabolic pathways, providing a framework for its profound biological impact. Research shows that a hypomagnetic field (hMF) directly reduces the production of reactive oxygen species (ROS), creating a quantum signature in plants. This is a counterintuitive finding, as it suggests the plant perceives less oxidative stress and, in response, downregulates its antioxidant defenses. This multi-level effect, from a quantum trigger to molecular and metabolic changes, ultimately affects the plant&amp;amp;rsquo;s growth and phenotype. This review suggests a possible link between the GMF and plant health, identifying the GMF as a potential physiological modulator. Manipulating the magnetic field could therefore be a novel strategy for improving crop resilience and growth. However, the fact that some effects cannot be fully explained by the RPM suggests other quantum mechanisms are involved, paving the way for future research into these undiscovered processes and their potential inheritance across generations.</description>
	<pubDate>2025-11-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 52: The Radical Pair Mechanism and Its Quantum Role in Plant Reactive Oxygen Species Production Under Hypomagnetic Fields</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/52">doi: 10.3390/quantum7040052</a></p>
	<p>Authors:
		Massimo E. Maffei
		</p>
	<p>The Earth&amp;amp;rsquo;s geomagnetic field (GMF) is a fundamental environmental signal for plants, with its perception rooted in quantum biology. Specifically, the radical pair mechanism (RPM) explains how this weak force influences electron spin states in metabolic pathways, providing a framework for its profound biological impact. Research shows that a hypomagnetic field (hMF) directly reduces the production of reactive oxygen species (ROS), creating a quantum signature in plants. This is a counterintuitive finding, as it suggests the plant perceives less oxidative stress and, in response, downregulates its antioxidant defenses. This multi-level effect, from a quantum trigger to molecular and metabolic changes, ultimately affects the plant&amp;amp;rsquo;s growth and phenotype. This review suggests a possible link between the GMF and plant health, identifying the GMF as a potential physiological modulator. Manipulating the magnetic field could therefore be a novel strategy for improving crop resilience and growth. However, the fact that some effects cannot be fully explained by the RPM suggests other quantum mechanisms are involved, paving the way for future research into these undiscovered processes and their potential inheritance across generations.</p>
	]]></content:encoded>

	<dc:title>The Radical Pair Mechanism and Its Quantum Role in Plant Reactive Oxygen Species Production Under Hypomagnetic Fields</dc:title>
			<dc:creator>Massimo E. Maffei</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040052</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-11-01</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-11-01</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>52</prism:startingPage>
		<prism:doi>10.3390/quantum7040052</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/52</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/51">

	<title>Quantum Reports, Vol. 7, Pages 51: Translating the Nearest Convex Hull Classifier from Classical to Quantum Computing</title>
	<link>https://www.mdpi.com/2624-960X/7/4/51</link>
	<description>The nearest convex hull (NCH) classifier is a promising algorithm for the classification of biosignals, such as electroencephalography (EEG) signals, especially when adapted to the classification of symmetric positive definite matrices. In this paper, we implemented a version of this classifier that can execute either on a traditional computer or a quantum simulator, and we tested it against state-of-the-art classifiers for EEG classification. This article addresses the practical challenges of adapting a classical algorithm to one that can be executed on a quantum computer or a quantum simulator. One of these challenges is to find a formulation of the classification problem that is quadratic, is binary, and accepts only linear constraints&amp;amp;mdash;that is, an objective function that can be solved using a variational quantum algorithm. In this article, we present two approaches to solve this problem, both compatible with continuous variables. Finally, we evaluated, for the first time, the performance of the NCH classifier on real EEG data using both quantum and classical optimization methods. We selected a particularly challenging dataset, where classical optimization typically performs poorly, and demonstrated that the nearest convex hull classifier was able to generalize with a modest performance. One lesson from this case study is that, by separating the objective function from the solver, it becomes possible to allow an existing classical algorithm to run on a quantum computer, as long as an appropriate objective function&amp;amp;mdash;quadratic and binary&amp;amp;mdash;can be found.</description>
	<pubDate>2025-10-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 51: Translating the Nearest Convex Hull Classifier from Classical to Quantum Computing</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/51">doi: 10.3390/quantum7040051</a></p>
	<p>Authors:
		Grégoire Cattan
		Anton Andreev
		Quentin Barthélemy
		</p>
	<p>The nearest convex hull (NCH) classifier is a promising algorithm for the classification of biosignals, such as electroencephalography (EEG) signals, especially when adapted to the classification of symmetric positive definite matrices. In this paper, we implemented a version of this classifier that can execute either on a traditional computer or a quantum simulator, and we tested it against state-of-the-art classifiers for EEG classification. This article addresses the practical challenges of adapting a classical algorithm to one that can be executed on a quantum computer or a quantum simulator. One of these challenges is to find a formulation of the classification problem that is quadratic, is binary, and accepts only linear constraints&amp;amp;mdash;that is, an objective function that can be solved using a variational quantum algorithm. In this article, we present two approaches to solve this problem, both compatible with continuous variables. Finally, we evaluated, for the first time, the performance of the NCH classifier on real EEG data using both quantum and classical optimization methods. We selected a particularly challenging dataset, where classical optimization typically performs poorly, and demonstrated that the nearest convex hull classifier was able to generalize with a modest performance. One lesson from this case study is that, by separating the objective function from the solver, it becomes possible to allow an existing classical algorithm to run on a quantum computer, as long as an appropriate objective function&amp;amp;mdash;quadratic and binary&amp;amp;mdash;can be found.</p>
	]]></content:encoded>

	<dc:title>Translating the Nearest Convex Hull Classifier from Classical to Quantum Computing</dc:title>
			<dc:creator>Grégoire Cattan</dc:creator>
			<dc:creator>Anton Andreev</dc:creator>
			<dc:creator>Quentin Barthélemy</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040051</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-28</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-28</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>51</prism:startingPage>
		<prism:doi>10.3390/quantum7040051</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/51</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/50">

	<title>Quantum Reports, Vol. 7, Pages 50: Experimental Investigation on Quantum Channel Noise Simulation and Information Security Threshold Based on Two-Photon Four-Qubit Hyper-Entanglement Systems</title>
	<link>https://www.mdpi.com/2624-960X/7/4/50</link>
	<description>Due to the important role of quantum information technology in the future development of science and technology, researchers have extensively studied the preparation, characterization, and application of quantum systems. It is of great significance to further study the universality and generalization of multi-qubit entangled states. Especially in quantum communication, the actual quantum system is always affected by various noises from the environment. Noise has a significant impact on the properties of the actual quantum system, so we study the effects of noise on a prepared two-photon four-qubit state by two methods. We experimentally simulated the most common bit-flip noise in quantum systems. The law of evolution of the fidelity of two-dimensional four-qubit states and violation of the Mermin inequality and the Ardehali inequality for LR under different levels of bit-flip noise are investigated. The experimental results show that entanglement fidelity and nonlocality can be used to judge the degree of noise interference in the quantum channel and, thus, judge the security of the quantum communication channel. This judgment is of great significance for the realization of practical long-distance multi-node quantum communication.</description>
	<pubDate>2025-10-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 50: Experimental Investigation on Quantum Channel Noise Simulation and Information Security Threshold Based on Two-Photon Four-Qubit Hyper-Entanglement Systems</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/50">doi: 10.3390/quantum7040050</a></p>
	<p>Authors:
		Jiaqiang Zhao
		Haoxiang Qin
		Lianzhen Cao
		Yang Yang
		Xia Liu
		Qinwei Zhang
		Huaixin Lu
		Kellie Ann Driscoll
		Meijiao Wang
		</p>
	<p>Due to the important role of quantum information technology in the future development of science and technology, researchers have extensively studied the preparation, characterization, and application of quantum systems. It is of great significance to further study the universality and generalization of multi-qubit entangled states. Especially in quantum communication, the actual quantum system is always affected by various noises from the environment. Noise has a significant impact on the properties of the actual quantum system, so we study the effects of noise on a prepared two-photon four-qubit state by two methods. We experimentally simulated the most common bit-flip noise in quantum systems. The law of evolution of the fidelity of two-dimensional four-qubit states and violation of the Mermin inequality and the Ardehali inequality for LR under different levels of bit-flip noise are investigated. The experimental results show that entanglement fidelity and nonlocality can be used to judge the degree of noise interference in the quantum channel and, thus, judge the security of the quantum communication channel. This judgment is of great significance for the realization of practical long-distance multi-node quantum communication.</p>
	]]></content:encoded>

	<dc:title>Experimental Investigation on Quantum Channel Noise Simulation and Information Security Threshold Based on Two-Photon Four-Qubit Hyper-Entanglement Systems</dc:title>
			<dc:creator>Jiaqiang Zhao</dc:creator>
			<dc:creator>Haoxiang Qin</dc:creator>
			<dc:creator>Lianzhen Cao</dc:creator>
			<dc:creator>Yang Yang</dc:creator>
			<dc:creator>Xia Liu</dc:creator>
			<dc:creator>Qinwei Zhang</dc:creator>
			<dc:creator>Huaixin Lu</dc:creator>
			<dc:creator>Kellie Ann Driscoll</dc:creator>
			<dc:creator>Meijiao Wang</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040050</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-22</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-22</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>50</prism:startingPage>
		<prism:doi>10.3390/quantum7040050</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/50</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/49">

	<title>Quantum Reports, Vol. 7, Pages 49: From Fibonacci Anyons to B-DNA and Microtubules via Elliptic Curves</title>
	<link>https://www.mdpi.com/2624-960X/7/4/49</link>
	<description>By imposing finite order constraints on Fibonacci anyon braid relations, we construct the finite quotient G=Z5&amp;amp;#8906;2I, where 2I is the binary icosahedral group. The Gr&amp;amp;ouml;bner basis decomposition of its SL(2,C) character variety yields elliptic curves whose L-function derivatives L&amp;amp;prime;(E,1) remarkably match fundamental biological structural ratios. Specifically, we demonstrate that the Birch&amp;amp;ndash;Swinnerton-Dyer conjecture&amp;amp;rsquo;s central quantity: the derivative L&amp;amp;prime;(E,1) of the L-function at 1 encodes critical cellular geometries: the crystalline B-DNA pitch-to-diameter ratio (L&amp;amp;prime;(E,1)=1.730 matching 34&amp;amp;Aring;/20&amp;amp;Aring;=1.70), the B-DNA pitch to major groove width (L&amp;amp;prime;=1.58) and, additionally, the fundamental cytoskeletal scaling relationship where L&amp;amp;prime;(E,1)=3.570&amp;amp;asymp;25/7, precisely matching the microtubule-to-actin diameter ratio. This pattern extends across the hierarchy Z5&amp;amp;#8906;2P with 2P&amp;amp;isin;{2O,2T,2I} (binary octahedral, tetrahedral, icosahedral groups), where character tables of 2O explain genetic code degeneracies while 2T yields microtubule ratios. The convergence of multiple independent mathematical pathways on identical biological values suggests that evolutionary optimization operates under deep arithmetic-geometric constraints encoded in elliptic curve L-functions. Our results position the BSD conjecture not merely as abstract number theory, but as encoding fundamental organizational principles governing cellular architecture. The correspondence reveals arithmetic geometry as the mathematical blueprint underlying major biological structural systems, with Gross&amp;amp;ndash;Zagier theory providing the theoretical framework connecting quantum topology to the helical geometries that are essential for life.</description>
	<pubDate>2025-10-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 49: From Fibonacci Anyons to B-DNA and Microtubules via Elliptic Curves</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/49">doi: 10.3390/quantum7040049</a></p>
	<p>Authors:
		Michel Planat
		</p>
	<p>By imposing finite order constraints on Fibonacci anyon braid relations, we construct the finite quotient G=Z5&amp;amp;#8906;2I, where 2I is the binary icosahedral group. The Gr&amp;amp;ouml;bner basis decomposition of its SL(2,C) character variety yields elliptic curves whose L-function derivatives L&amp;amp;prime;(E,1) remarkably match fundamental biological structural ratios. Specifically, we demonstrate that the Birch&amp;amp;ndash;Swinnerton-Dyer conjecture&amp;amp;rsquo;s central quantity: the derivative L&amp;amp;prime;(E,1) of the L-function at 1 encodes critical cellular geometries: the crystalline B-DNA pitch-to-diameter ratio (L&amp;amp;prime;(E,1)=1.730 matching 34&amp;amp;Aring;/20&amp;amp;Aring;=1.70), the B-DNA pitch to major groove width (L&amp;amp;prime;=1.58) and, additionally, the fundamental cytoskeletal scaling relationship where L&amp;amp;prime;(E,1)=3.570&amp;amp;asymp;25/7, precisely matching the microtubule-to-actin diameter ratio. This pattern extends across the hierarchy Z5&amp;amp;#8906;2P with 2P&amp;amp;isin;{2O,2T,2I} (binary octahedral, tetrahedral, icosahedral groups), where character tables of 2O explain genetic code degeneracies while 2T yields microtubule ratios. The convergence of multiple independent mathematical pathways on identical biological values suggests that evolutionary optimization operates under deep arithmetic-geometric constraints encoded in elliptic curve L-functions. Our results position the BSD conjecture not merely as abstract number theory, but as encoding fundamental organizational principles governing cellular architecture. The correspondence reveals arithmetic geometry as the mathematical blueprint underlying major biological structural systems, with Gross&amp;amp;ndash;Zagier theory providing the theoretical framework connecting quantum topology to the helical geometries that are essential for life.</p>
	]]></content:encoded>

	<dc:title>From Fibonacci Anyons to B-DNA and Microtubules via Elliptic Curves</dc:title>
			<dc:creator>Michel Planat</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040049</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-17</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>49</prism:startingPage>
		<prism:doi>10.3390/quantum7040049</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/49</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/48">

	<title>Quantum Reports, Vol. 7, Pages 48: Epistemic Signatures of Fisher Information in Finite Fermions Systems</title>
	<link>https://www.mdpi.com/2624-960X/7/4/48</link>
	<description>Beginning with Mandelbrot&amp;amp;rsquo;s insight that Fisher information may admit a thermodynamic interpretation, a growing body of work has connected this information-theoretic measure to fluctuation&amp;amp;ndash;dissipation relations, thermodynamic geometry, and phase transitions. Yet, these connections have largely remained at the level of formal analogies. In this work, we provide what is, to our knowledge, the first explicit realization of the epistemic-to-physical transition of Fisher information within a finite interacting quantum system. Specifically, we analyze a model of N fermions occupying two degenerate levels and coupled by a spin-flip interaction of strength V, treated in the grand canonical ensemble at inverse temperature &amp;amp;beta;. We compute the Fisher information FN(V) associated with the sensitivity of the thermal state to changes in V, and show that it becomes an observer-independent, experimentally meaningful quantity: it encodes fluctuations, tracks entropy variations, and reveals structural transitions induced by interactions. Our findings thus demonstrate that Fisher information, originally conceived as an inferential and epistemic measure, can operate as a bona fide thermodynamic observable in quantum many-body physics, bridging the gap between information-theoretic foundations and measurable physical law.</description>
	<pubDate>2025-10-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 48: Epistemic Signatures of Fisher Information in Finite Fermions Systems</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/48">doi: 10.3390/quantum7040048</a></p>
	<p>Authors:
		Angelo Plastino
		Victoria Vampa
		</p>
	<p>Beginning with Mandelbrot&amp;amp;rsquo;s insight that Fisher information may admit a thermodynamic interpretation, a growing body of work has connected this information-theoretic measure to fluctuation&amp;amp;ndash;dissipation relations, thermodynamic geometry, and phase transitions. Yet, these connections have largely remained at the level of formal analogies. In this work, we provide what is, to our knowledge, the first explicit realization of the epistemic-to-physical transition of Fisher information within a finite interacting quantum system. Specifically, we analyze a model of N fermions occupying two degenerate levels and coupled by a spin-flip interaction of strength V, treated in the grand canonical ensemble at inverse temperature &amp;amp;beta;. We compute the Fisher information FN(V) associated with the sensitivity of the thermal state to changes in V, and show that it becomes an observer-independent, experimentally meaningful quantity: it encodes fluctuations, tracks entropy variations, and reveals structural transitions induced by interactions. Our findings thus demonstrate that Fisher information, originally conceived as an inferential and epistemic measure, can operate as a bona fide thermodynamic observable in quantum many-body physics, bridging the gap between information-theoretic foundations and measurable physical law.</p>
	]]></content:encoded>

	<dc:title>Epistemic Signatures of Fisher Information in Finite Fermions Systems</dc:title>
			<dc:creator>Angelo Plastino</dc:creator>
			<dc:creator>Victoria Vampa</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040048</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-14</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-14</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>48</prism:startingPage>
		<prism:doi>10.3390/quantum7040048</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/48</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/47">

	<title>Quantum Reports, Vol. 7, Pages 47: Quantum Simulation of Variable-Speed Multidimensional Wave Equations via Clifford-Assisted Pauli Decomposition</title>
	<link>https://www.mdpi.com/2624-960X/7/4/47</link>
	<description>The simulation of multidimensional wave propagation with variable material parameters is a computationally intensive task, with applications from seismology to electromagnetics. While quantum computers offer a promising path forward, their algorithms are often analyzed in the abstract oracle model, which can mask the high gate-level complexity of implementing those oracles. We present a framework for constructing a quantum algorithm for the multidimensional wave equation with a variable speed profile. The core of our method is a decomposition of the system Hamiltonian into sets of mutually commuting Pauli strings, paired with a dedicated diagonalization procedure that uses Clifford gates to minimize simulation cost. Within this framework, we derive explicit bounds on the number of quantum gates required for Trotter&amp;amp;ndash;Suzuki-based simulation. Our analysis reveals significant computational savings for structured block-model speed profiles compared to general cases. Numerical experiments in three dimensions confirm the practical viability and performance of our approach. Beyond providing a concrete, gate-level algorithm for an important class of wave problems, the techniques introduced here for Hamiltonian decomposition and diagonalization enrich the general toolbox of quantum simulation.</description>
	<pubDate>2025-10-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 47: Quantum Simulation of Variable-Speed Multidimensional Wave Equations via Clifford-Assisted Pauli Decomposition</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/47">doi: 10.3390/quantum7040047</a></p>
	<p>Authors:
		Boris Arseniev
		Igor Zacharov
		</p>
	<p>The simulation of multidimensional wave propagation with variable material parameters is a computationally intensive task, with applications from seismology to electromagnetics. While quantum computers offer a promising path forward, their algorithms are often analyzed in the abstract oracle model, which can mask the high gate-level complexity of implementing those oracles. We present a framework for constructing a quantum algorithm for the multidimensional wave equation with a variable speed profile. The core of our method is a decomposition of the system Hamiltonian into sets of mutually commuting Pauli strings, paired with a dedicated diagonalization procedure that uses Clifford gates to minimize simulation cost. Within this framework, we derive explicit bounds on the number of quantum gates required for Trotter&amp;amp;ndash;Suzuki-based simulation. Our analysis reveals significant computational savings for structured block-model speed profiles compared to general cases. Numerical experiments in three dimensions confirm the practical viability and performance of our approach. Beyond providing a concrete, gate-level algorithm for an important class of wave problems, the techniques introduced here for Hamiltonian decomposition and diagonalization enrich the general toolbox of quantum simulation.</p>
	]]></content:encoded>

	<dc:title>Quantum Simulation of Variable-Speed Multidimensional Wave Equations via Clifford-Assisted Pauli Decomposition</dc:title>
			<dc:creator>Boris Arseniev</dc:creator>
			<dc:creator>Igor Zacharov</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040047</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-13</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>47</prism:startingPage>
		<prism:doi>10.3390/quantum7040047</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/47</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/46">

	<title>Quantum Reports, Vol. 7, Pages 46: Destructive Interference as a Path to Resolving the Quantum Measurement Problem</title>
	<link>https://www.mdpi.com/2624-960X/7/4/46</link>
	<description>Over the past several decades, there has been an accelerating trend to ever more accurate quantum sensors: sensors of time intervals (i.e., atomic clocks), sensors of magnetic fields (i.e., quantum magnetometers), and sensors of inertial motions (i.e., atom interferometers), to name just a few. With this trend has come a renewed interest in the problem of quantum mechanical measurement (i.e., collapse of the wavefunction), and though there have been many attempts to resolve the problem, there is still no wholly accepted resolution. Here, we discuss a little-explored path for resolving the issue that exploits wavefunction phase. To illustrate this path&amp;amp;rsquo;s potential, we consider the notion of &amp;amp;ldquo;eigenphase&amp;amp;rdquo; sets that are disjoint among orthogonal eigenvectors. Wavefunction collapse then occurs because of constructive/destructive interference when a classical measuring device &amp;amp;ldquo;phase-locks&amp;amp;rdquo; to an incoming wavefunction. While the present work examines one method for exploiting wavefunction phase, its primary purpose is to more generally re-focus attention on wavefunction phase as a means for resolving the measurement problem that avoids many other solutions&amp;amp;rsquo; problematic aspects.</description>
	<pubDate>2025-10-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 46: Destructive Interference as a Path to Resolving the Quantum Measurement Problem</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/46">doi: 10.3390/quantum7040046</a></p>
	<p>Authors:
		James Camparo
		</p>
	<p>Over the past several decades, there has been an accelerating trend to ever more accurate quantum sensors: sensors of time intervals (i.e., atomic clocks), sensors of magnetic fields (i.e., quantum magnetometers), and sensors of inertial motions (i.e., atom interferometers), to name just a few. With this trend has come a renewed interest in the problem of quantum mechanical measurement (i.e., collapse of the wavefunction), and though there have been many attempts to resolve the problem, there is still no wholly accepted resolution. Here, we discuss a little-explored path for resolving the issue that exploits wavefunction phase. To illustrate this path&amp;amp;rsquo;s potential, we consider the notion of &amp;amp;ldquo;eigenphase&amp;amp;rdquo; sets that are disjoint among orthogonal eigenvectors. Wavefunction collapse then occurs because of constructive/destructive interference when a classical measuring device &amp;amp;ldquo;phase-locks&amp;amp;rdquo; to an incoming wavefunction. While the present work examines one method for exploiting wavefunction phase, its primary purpose is to more generally re-focus attention on wavefunction phase as a means for resolving the measurement problem that avoids many other solutions&amp;amp;rsquo; problematic aspects.</p>
	]]></content:encoded>

	<dc:title>Destructive Interference as a Path to Resolving the Quantum Measurement Problem</dc:title>
			<dc:creator>James Camparo</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040046</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-10</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-10</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>46</prism:startingPage>
		<prism:doi>10.3390/quantum7040046</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/46</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/45">

	<title>Quantum Reports, Vol. 7, Pages 45: Many-Body Effects in a Molecular Quantum NAND Tree</title>
	<link>https://www.mdpi.com/2624-960X/7/4/45</link>
	<description>Molecules provide the smallest possible circuits in which quantum interference and electron correlation can be engineered to perform logical operations, including the universal NAND gate. We investigate a chemically encoded quantum NAND tree based on alkynyl-extended iso-polyacetylene backbones, where inputs are set by end-group substitution and outputs are read from the presence or absence of transmission nodes. Using quantum many-body transport theory, we show that NAND behavior persists in the presence of dynamic correlations, but that the nodal positions and their chemical shifts depend sensitively on electron&amp;amp;ndash;electron interactions. This sensitivity highlights the potential of these systems not only to probe the strength of electronic correlations but also to harness them in shaping logical response. The thermopower is identified as a chemically robust readout of gate logic, providing discrimination margins that greatly exceed typical experimental uncertainties, in an observable governed primarily by the variation of transport rather than its absolute magnitude.</description>
	<pubDate>2025-10-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 45: Many-Body Effects in a Molecular Quantum NAND Tree</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/45">doi: 10.3390/quantum7040045</a></p>
	<p>Authors:
		Justin P. Bergfield
		</p>
	<p>Molecules provide the smallest possible circuits in which quantum interference and electron correlation can be engineered to perform logical operations, including the universal NAND gate. We investigate a chemically encoded quantum NAND tree based on alkynyl-extended iso-polyacetylene backbones, where inputs are set by end-group substitution and outputs are read from the presence or absence of transmission nodes. Using quantum many-body transport theory, we show that NAND behavior persists in the presence of dynamic correlations, but that the nodal positions and their chemical shifts depend sensitively on electron&amp;amp;ndash;electron interactions. This sensitivity highlights the potential of these systems not only to probe the strength of electronic correlations but also to harness them in shaping logical response. The thermopower is identified as a chemically robust readout of gate logic, providing discrimination margins that greatly exceed typical experimental uncertainties, in an observable governed primarily by the variation of transport rather than its absolute magnitude.</p>
	]]></content:encoded>

	<dc:title>Many-Body Effects in a Molecular Quantum NAND Tree</dc:title>
			<dc:creator>Justin P. Bergfield</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040045</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-10-10</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-10-10</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>45</prism:startingPage>
		<prism:doi>10.3390/quantum7040045</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/45</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/4/44">

	<title>Quantum Reports, Vol. 7, Pages 44: Digital Forensics of Quantum Computing: The Role of Quantum Entanglement in Digital Forensics&amp;mdash;Current Status and Future Directions</title>
	<link>https://www.mdpi.com/2624-960X/7/4/44</link>
	<description>As quantum computing advances, traditional digital forensic techniques face significant risks due to the vulnerability of classical cryptographic algorithms to quantum attacks. This review explores the emerging field of quantum digital forensics, with a particular focus on the role of quantum entanglement in enhancing the integrity, authenticity, and confidentiality of digital evidence. It compares classical and quantum forensic mechanisms, examines entanglement-based quantum key distribution (QKD), quantum hash functions, and quantum digital signatures (QDS), and discusses the challenges in practical implementation, such as scalability, hardware limitations, and legal admissibility. The paper also reviews various entanglement detection methods critical to the validation of quantum states used in forensic processes.</description>
	<pubDate>2025-09-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 44: Digital Forensics of Quantum Computing: The Role of Quantum Entanglement in Digital Forensics&amp;mdash;Current Status and Future Directions</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/4/44">doi: 10.3390/quantum7040044</a></p>
	<p>Authors:
		Shatha Alhazmi
		Khaled Elleithy
		Abdelrahman Elleithy
		</p>
	<p>As quantum computing advances, traditional digital forensic techniques face significant risks due to the vulnerability of classical cryptographic algorithms to quantum attacks. This review explores the emerging field of quantum digital forensics, with a particular focus on the role of quantum entanglement in enhancing the integrity, authenticity, and confidentiality of digital evidence. It compares classical and quantum forensic mechanisms, examines entanglement-based quantum key distribution (QKD), quantum hash functions, and quantum digital signatures (QDS), and discusses the challenges in practical implementation, such as scalability, hardware limitations, and legal admissibility. The paper also reviews various entanglement detection methods critical to the validation of quantum states used in forensic processes.</p>
	]]></content:encoded>

	<dc:title>Digital Forensics of Quantum Computing: The Role of Quantum Entanglement in Digital Forensics&amp;amp;mdash;Current Status and Future Directions</dc:title>
			<dc:creator>Shatha Alhazmi</dc:creator>
			<dc:creator>Khaled Elleithy</dc:creator>
			<dc:creator>Abdelrahman Elleithy</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7040044</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-30</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-30</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>44</prism:startingPage>
		<prism:doi>10.3390/quantum7040044</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/4/44</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/43">

	<title>Quantum Reports, Vol. 7, Pages 43: Parametric Resonance via Neuronal Microtubules: Filtering Optical Signals by Tryptophan Qubits</title>
	<link>https://www.mdpi.com/2624-960X/7/3/43</link>
	<description>This paper aims to address the possibility of parametric resonance effects in microtubules via tryptophan qubits, using the Hamiltonian of the cavity quantum electrodynamics (QED) model involving photons in a waveguide and the surrounding environment. The time evolution equations for qubits and photons are derived using the input&amp;amp;ndash;output formulation. Input signals with a 560 nm wavelength are amplified by Rabi oscillations for tryptophan qubits in excited states. Here, the qubits organized in multiple layers are all in excited states. When an appropriate decay to the environment occurs as internal loss, which is prepared in multiple layers, we find binary patterns of the parametric amplification of input signals and the reduction of output signals. This property might help us to understand the information processing of optical signals by filtering them with the use of tryptophan residues in microtubules and diffused nonlocal processing spreading over the whole brain in the form of holograms.</description>
	<pubDate>2025-09-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 43: Parametric Resonance via Neuronal Microtubules: Filtering Optical Signals by Tryptophan Qubits</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/43">doi: 10.3390/quantum7030043</a></p>
	<p>Authors:
		Akihiro Nishiyama
		Shigenori Tanaka
		Jack Adam Tuszynski
		</p>
	<p>This paper aims to address the possibility of parametric resonance effects in microtubules via tryptophan qubits, using the Hamiltonian of the cavity quantum electrodynamics (QED) model involving photons in a waveguide and the surrounding environment. The time evolution equations for qubits and photons are derived using the input&amp;amp;ndash;output formulation. Input signals with a 560 nm wavelength are amplified by Rabi oscillations for tryptophan qubits in excited states. Here, the qubits organized in multiple layers are all in excited states. When an appropriate decay to the environment occurs as internal loss, which is prepared in multiple layers, we find binary patterns of the parametric amplification of input signals and the reduction of output signals. This property might help us to understand the information processing of optical signals by filtering them with the use of tryptophan residues in microtubules and diffused nonlocal processing spreading over the whole brain in the form of holograms.</p>
	]]></content:encoded>

	<dc:title>Parametric Resonance via Neuronal Microtubules: Filtering Optical Signals by Tryptophan Qubits</dc:title>
			<dc:creator>Akihiro Nishiyama</dc:creator>
			<dc:creator>Shigenori Tanaka</dc:creator>
			<dc:creator>Jack Adam Tuszynski</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030043</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-17</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>43</prism:startingPage>
		<prism:doi>10.3390/quantum7030043</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/43</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/42">

	<title>Quantum Reports, Vol. 7, Pages 42: Topologically Protected Quantum Teleportation via Majorana Zero Modes: A Perspective on Scalability and Decoherence Immunity</title>
	<link>https://www.mdpi.com/2624-960X/7/3/42</link>
	<description>We present a topologically protected teleportation protocol based on projective parity measurements between spatially separated Majorana zero modes (MZMs), eliminating the need for dynamic braiding. Unlike conventional teleportation schemes, our method preserves logical information through nonlocal encoding and suppresses decoherence exponentially with Majorana separation. We provide a rigorous mathematical framework that includes six theorems and a lemma, proving fidelity bounds, no entropy increase under ideal QND parity measurement under quantum non-demolition (QND) measurements, and compliance with the no-cloning theorem. We demonstrate that all correction operations lie within the Clifford group, enabling efficient, fault-tolerant implementation. Furthermore, we outline a scalable architecture for multi-qubit teleportation and relate our framework to recent experimental advances in quantum-dot-based Kitaev chains and superconducting nanowire platforms. These results position Majorana-based teleportation as a thermodynamically stable and experimentally viable approach to scalable quantum information transfer. All operations discussed are Clifford-only; achieving universality requires non-Clifford resources and lies outside our scope.</description>
	<pubDate>2025-09-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 42: Topologically Protected Quantum Teleportation via Majorana Zero Modes: A Perspective on Scalability and Decoherence Immunity</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/42">doi: 10.3390/quantum7030042</a></p>
	<p>Authors:
		Horace T. Crogman
		To Dang
		Daniel Erenso
		</p>
	<p>We present a topologically protected teleportation protocol based on projective parity measurements between spatially separated Majorana zero modes (MZMs), eliminating the need for dynamic braiding. Unlike conventional teleportation schemes, our method preserves logical information through nonlocal encoding and suppresses decoherence exponentially with Majorana separation. We provide a rigorous mathematical framework that includes six theorems and a lemma, proving fidelity bounds, no entropy increase under ideal QND parity measurement under quantum non-demolition (QND) measurements, and compliance with the no-cloning theorem. We demonstrate that all correction operations lie within the Clifford group, enabling efficient, fault-tolerant implementation. Furthermore, we outline a scalable architecture for multi-qubit teleportation and relate our framework to recent experimental advances in quantum-dot-based Kitaev chains and superconducting nanowire platforms. These results position Majorana-based teleportation as a thermodynamically stable and experimentally viable approach to scalable quantum information transfer. All operations discussed are Clifford-only; achieving universality requires non-Clifford resources and lies outside our scope.</p>
	]]></content:encoded>

	<dc:title>Topologically Protected Quantum Teleportation via Majorana Zero Modes: A Perspective on Scalability and Decoherence Immunity</dc:title>
			<dc:creator>Horace T. Crogman</dc:creator>
			<dc:creator>To Dang</dc:creator>
			<dc:creator>Daniel Erenso</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030042</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-11</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-11</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>42</prism:startingPage>
		<prism:doi>10.3390/quantum7030042</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/42</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/41">

	<title>Quantum Reports, Vol. 7, Pages 41: Memory Management Strategies for Software Quantum Simulators</title>
	<link>https://www.mdpi.com/2624-960X/7/3/41</link>
	<description>Software quantum simulators are essential tools for designing and testing quantum algorithms on classical computing architectures, especially given the current limitations of physical quantum hardware. This work focuses on studying and evaluating memory management strategies for scalable quantum state simulation. We examine full-state representation, dynamic state pruning, shared-memory parallelization with OpenMP, distributed memory execution using MPI, and error-bounded floating-point compression with ZFP. These techniques are implemented in a prototype simulator and assessed using the quantum Fourier transform as a benchmark, with performance compared against leading open-source simulators such as Intel-QS, QuEST, and qsim. The results show the trade-offs between computational overhead and memory efficiency, and demonstrate that hybrid approaches combining distributed memory and compression can significantly extend the number of qubits that can be simulated. This work contributes practical insights for improving the scalability of software quantum simulators on classical hardware through optimized memory usage.</description>
	<pubDate>2025-09-09</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 41: Memory Management Strategies for Software Quantum Simulators</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/41">doi: 10.3390/quantum7030041</a></p>
	<p>Authors:
		Gilberto Díaz
		Luiz Steffenel
		Carlos Barrios
		Jean Couturier
		</p>
	<p>Software quantum simulators are essential tools for designing and testing quantum algorithms on classical computing architectures, especially given the current limitations of physical quantum hardware. This work focuses on studying and evaluating memory management strategies for scalable quantum state simulation. We examine full-state representation, dynamic state pruning, shared-memory parallelization with OpenMP, distributed memory execution using MPI, and error-bounded floating-point compression with ZFP. These techniques are implemented in a prototype simulator and assessed using the quantum Fourier transform as a benchmark, with performance compared against leading open-source simulators such as Intel-QS, QuEST, and qsim. The results show the trade-offs between computational overhead and memory efficiency, and demonstrate that hybrid approaches combining distributed memory and compression can significantly extend the number of qubits that can be simulated. This work contributes practical insights for improving the scalability of software quantum simulators on classical hardware through optimized memory usage.</p>
	]]></content:encoded>

	<dc:title>Memory Management Strategies for Software Quantum Simulators</dc:title>
			<dc:creator>Gilberto Díaz</dc:creator>
			<dc:creator>Luiz Steffenel</dc:creator>
			<dc:creator>Carlos Barrios</dc:creator>
			<dc:creator>Jean Couturier</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030041</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-09</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-09</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>41</prism:startingPage>
		<prism:doi>10.3390/quantum7030041</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/41</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/40">

	<title>Quantum Reports, Vol. 7, Pages 40: Interference in Complex Canonical Variables Is Not Quantum</title>
	<link>https://www.mdpi.com/2624-960X/7/3/40</link>
	<description>We formally represent the quantum interference of a single qubit embodied by a photon in the Mach&amp;amp;ndash;Zehnder interferometer using the classical Hamiltonian framework but with complex canonical variables. Although all operations on a single qubit can be formally expressed using complex classical Hamiltonian dynamics, we show that the resulting system is still not a proper qubit. The reason for this is that it is not capable of getting entangled to another bona fide qubit and hence it does not have the information-processing capacity of a fully-fledged quantum system. This simple example powerfully illustrates the difficulties faced by hybrid quantum&amp;amp;ndash;classical models in accounting for the full range of behaviour of quantum systems.</description>
	<pubDate>2025-09-09</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 40: Interference in Complex Canonical Variables Is Not Quantum</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/40">doi: 10.3390/quantum7030040</a></p>
	<p>Authors:
		Chiara Marletto
		Vlatko Vedral
		</p>
	<p>We formally represent the quantum interference of a single qubit embodied by a photon in the Mach&amp;amp;ndash;Zehnder interferometer using the classical Hamiltonian framework but with complex canonical variables. Although all operations on a single qubit can be formally expressed using complex classical Hamiltonian dynamics, we show that the resulting system is still not a proper qubit. The reason for this is that it is not capable of getting entangled to another bona fide qubit and hence it does not have the information-processing capacity of a fully-fledged quantum system. This simple example powerfully illustrates the difficulties faced by hybrid quantum&amp;amp;ndash;classical models in accounting for the full range of behaviour of quantum systems.</p>
	]]></content:encoded>

	<dc:title>Interference in Complex Canonical Variables Is Not Quantum</dc:title>
			<dc:creator>Chiara Marletto</dc:creator>
			<dc:creator>Vlatko Vedral</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030040</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-09</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-09</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>40</prism:startingPage>
		<prism:doi>10.3390/quantum7030040</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/40</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/39">

	<title>Quantum Reports, Vol. 7, Pages 39: A Review on Models and Applications of Quantum Computing</title>
	<link>https://www.mdpi.com/2624-960X/7/3/39</link>
	<description>This manuscript is intended for readers who have a general interest in the subject of quantum computation and provides an overview of the most significant developments in the field. It begins by introducing foundational concepts from quantum mechanics&amp;amp;mdash;such as superposition, entanglement, and the no-cloning theorem&amp;amp;mdash;that underpin quantum computation. The primary computational models are discussed, including gate-based (circuit) quantum computing, adiabatic quantum computing, measurement-based quantum computing and the quantum Turing machine. A selection of significant quantum algorithms are reviewed, notably Grover&amp;amp;rsquo;s search algorithm, Shor&amp;amp;rsquo;s factoring algorithm, and Quantum Singular Value Transformation (QSVT), which enables efficient solutions to linear algebra problems on quantum devices. To assess practical performance, we compare quantum and classical implementations of support vector machines (SVMs) using several synthetic datasets. These experiments offer insight into the capabilities and limitations of near-term quantum classifiers relative to classical counterparts. Finally, we review leading quantum programming platforms&amp;amp;mdash;including Qiskit, PennyLane, and Cirq&amp;amp;mdash;and discuss their roles in bridging theoretical models with real-world quantum hardware. The paper aims to provide a concise yet comprehensive guide for those looking to understand both the theoretical foundations and applied aspects of quantum computing.</description>
	<pubDate>2025-09-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 39: A Review on Models and Applications of Quantum Computing</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/39">doi: 10.3390/quantum7030039</a></p>
	<p>Authors:
		Eduard Grigoryan
		Sachin Kumar
		Placido Rogério Pinheiro
		</p>
	<p>This manuscript is intended for readers who have a general interest in the subject of quantum computation and provides an overview of the most significant developments in the field. It begins by introducing foundational concepts from quantum mechanics&amp;amp;mdash;such as superposition, entanglement, and the no-cloning theorem&amp;amp;mdash;that underpin quantum computation. The primary computational models are discussed, including gate-based (circuit) quantum computing, adiabatic quantum computing, measurement-based quantum computing and the quantum Turing machine. A selection of significant quantum algorithms are reviewed, notably Grover&amp;amp;rsquo;s search algorithm, Shor&amp;amp;rsquo;s factoring algorithm, and Quantum Singular Value Transformation (QSVT), which enables efficient solutions to linear algebra problems on quantum devices. To assess practical performance, we compare quantum and classical implementations of support vector machines (SVMs) using several synthetic datasets. These experiments offer insight into the capabilities and limitations of near-term quantum classifiers relative to classical counterparts. Finally, we review leading quantum programming platforms&amp;amp;mdash;including Qiskit, PennyLane, and Cirq&amp;amp;mdash;and discuss their roles in bridging theoretical models with real-world quantum hardware. The paper aims to provide a concise yet comprehensive guide for those looking to understand both the theoretical foundations and applied aspects of quantum computing.</p>
	]]></content:encoded>

	<dc:title>A Review on Models and Applications of Quantum Computing</dc:title>
			<dc:creator>Eduard Grigoryan</dc:creator>
			<dc:creator>Sachin Kumar</dc:creator>
			<dc:creator>Placido Rogério Pinheiro</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030039</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-09-04</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-09-04</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>39</prism:startingPage>
		<prism:doi>10.3390/quantum7030039</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/39</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/38">

	<title>Quantum Reports, Vol. 7, Pages 38: A Novel QCA Design of Energy-Efficient Three-Input AND/OR Circuit</title>
	<link>https://www.mdpi.com/2624-960X/7/3/38</link>
	<description>One of the nanoscale technologies that shows its capability of implementing integrated digital circuits with low power, high speed, and high density is quantum-dot cellular automata (QCA). The fundamental device for designing and implementing circuits in QCA is majority logic. In this paper, a novel energy-efficient QCA design of three-input AND/OR logic functions is proposed. This design can perform both AND and OR logic operations using the same structure with an achievement of 58% and 64% approximate reductions in power consumption compared to majority-based structures, and 31% and 32% approximate reductions in power consumption compared to the best available circuits, respectively. In addition, other physical constraints such as area and latency are improved and have better or similar results compared to the best existing circuits. The proposed circuit can be considered as a fundamental and better alternative to the majority gate for energy-efficient circuit design in QCA. This will pave the way for developing efficient large-scale QCA-based sequential and combinational circuits.</description>
	<pubDate>2025-08-31</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 38: A Novel QCA Design of Energy-Efficient Three-Input AND/OR Circuit</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/38">doi: 10.3390/quantum7030038</a></p>
	<p>Authors:
		Amjad Almatrood
		</p>
	<p>One of the nanoscale technologies that shows its capability of implementing integrated digital circuits with low power, high speed, and high density is quantum-dot cellular automata (QCA). The fundamental device for designing and implementing circuits in QCA is majority logic. In this paper, a novel energy-efficient QCA design of three-input AND/OR logic functions is proposed. This design can perform both AND and OR logic operations using the same structure with an achievement of 58% and 64% approximate reductions in power consumption compared to majority-based structures, and 31% and 32% approximate reductions in power consumption compared to the best available circuits, respectively. In addition, other physical constraints such as area and latency are improved and have better or similar results compared to the best existing circuits. The proposed circuit can be considered as a fundamental and better alternative to the majority gate for energy-efficient circuit design in QCA. This will pave the way for developing efficient large-scale QCA-based sequential and combinational circuits.</p>
	]]></content:encoded>

	<dc:title>A Novel QCA Design of Energy-Efficient Three-Input AND/OR Circuit</dc:title>
			<dc:creator>Amjad Almatrood</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030038</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-08-31</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-08-31</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>38</prism:startingPage>
		<prism:doi>10.3390/quantum7030038</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/38</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/37">

	<title>Quantum Reports, Vol. 7, Pages 37: HHL Algorithm for Tensor-Decomposable Matrices</title>
	<link>https://www.mdpi.com/2624-960X/7/3/37</link>
	<description>We use the HHL algorithm to retrieve a quantum state holding the algebraic normal form (ANF) of a Boolean function. Unlike the standard HHL applications, we do not describe the cipher as an exponentially big system of equations. Rather, we perform a set of small matrix inversions which correspond to the Boolean M&amp;amp;ouml;bius transform. This creates a superposition holding information about the ANF in the form |Af&amp;amp;#10217;=1C&amp;amp;sum;I=02n&amp;amp;minus;1cI|I&amp;amp;#10217;, where cI is the coefficient of the ANF and C is a scaling factor. The procedure has a time complexity of O~(n) for a Boolean function with n-bit input. We also propose two approaches by which some information about the ANF can be extracted from such a state. Next, we use a similar approach, the Dual Boolean M&amp;amp;ouml;bius transform, to compute the preimage under the algebraic transition matrix. We show that such a matrix is well-suited for the HHL algorithm when the attacker gets oracle access in the Q2 setting to the Boolean function.</description>
	<pubDate>2025-08-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 37: HHL Algorithm for Tensor-Decomposable Matrices</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/37">doi: 10.3390/quantum7030037</a></p>
	<p>Authors:
		Cezary Pilaszewicz
		Marian Margraf
		</p>
	<p>We use the HHL algorithm to retrieve a quantum state holding the algebraic normal form (ANF) of a Boolean function. Unlike the standard HHL applications, we do not describe the cipher as an exponentially big system of equations. Rather, we perform a set of small matrix inversions which correspond to the Boolean M&amp;amp;ouml;bius transform. This creates a superposition holding information about the ANF in the form |Af&amp;amp;#10217;=1C&amp;amp;sum;I=02n&amp;amp;minus;1cI|I&amp;amp;#10217;, where cI is the coefficient of the ANF and C is a scaling factor. The procedure has a time complexity of O~(n) for a Boolean function with n-bit input. We also propose two approaches by which some information about the ANF can be extracted from such a state. Next, we use a similar approach, the Dual Boolean M&amp;amp;ouml;bius transform, to compute the preimage under the algebraic transition matrix. We show that such a matrix is well-suited for the HHL algorithm when the attacker gets oracle access in the Q2 setting to the Boolean function.</p>
	]]></content:encoded>

	<dc:title>HHL Algorithm for Tensor-Decomposable Matrices</dc:title>
			<dc:creator>Cezary Pilaszewicz</dc:creator>
			<dc:creator>Marian Margraf</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030037</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-08-19</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-08-19</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>37</prism:startingPage>
		<prism:doi>10.3390/quantum7030037</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/37</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/36">

	<title>Quantum Reports, Vol. 7, Pages 36: Quantum-Enhanced Algorithmic Fairness and the Advancement of AI Integrity and Responsibility</title>
	<link>https://www.mdpi.com/2624-960X/7/3/36</link>
	<description>In the evolving digital landscape, the pervasive influence of artificial intelligence (AI) on social media platforms reveals a compelling paradox: the capability to provide personalized experiences juxtaposed with inherent biases reminiscent of human imperfections. Such biases prompt rigorous contemplation on matters of fairness, equity, and societal ramifications, and penetrate the foundational essence of AI. Within this intricate context, the present work ventures into novel domains by examining the potential of quantum computing as a viable remedy for bias in artificial intelligence. The conceptual framework of the quantum sentinel is presented&amp;amp;mdash;an innovative approach that employs quantum principles for the detection and scrutiny of biases in AI algorithms. Furthermore, the study poses and investigates the question of whether the integration of advanced quantum computing to address AI bias is seen as an excessive measure or a requisite advancement commensurate with the intricacy of the issue. By intertwining quantum mechanics, AI bias, and the philosophical considerations they induce, this research fosters a discourse on the journey toward ethical AI, thus establishing a foundation for an ethically conscious and balanced digital environment. We also show that the quantum Zeno effect can protect SVM hyperplanes from bias through targeted simulations.</description>
	<pubDate>2025-08-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 36: Quantum-Enhanced Algorithmic Fairness and the Advancement of AI Integrity and Responsibility</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/36">doi: 10.3390/quantum7030036</a></p>
	<p>Authors:
		Akhil Chintalapati
		Khashbat Enkhbat
		Ramanathan Annamalai
		Geraldine Bessie Amali
		Fatih Ozaydin
		Mathew Mithra Noel
		</p>
	<p>In the evolving digital landscape, the pervasive influence of artificial intelligence (AI) on social media platforms reveals a compelling paradox: the capability to provide personalized experiences juxtaposed with inherent biases reminiscent of human imperfections. Such biases prompt rigorous contemplation on matters of fairness, equity, and societal ramifications, and penetrate the foundational essence of AI. Within this intricate context, the present work ventures into novel domains by examining the potential of quantum computing as a viable remedy for bias in artificial intelligence. The conceptual framework of the quantum sentinel is presented&amp;amp;mdash;an innovative approach that employs quantum principles for the detection and scrutiny of biases in AI algorithms. Furthermore, the study poses and investigates the question of whether the integration of advanced quantum computing to address AI bias is seen as an excessive measure or a requisite advancement commensurate with the intricacy of the issue. By intertwining quantum mechanics, AI bias, and the philosophical considerations they induce, this research fosters a discourse on the journey toward ethical AI, thus establishing a foundation for an ethically conscious and balanced digital environment. We also show that the quantum Zeno effect can protect SVM hyperplanes from bias through targeted simulations.</p>
	]]></content:encoded>

	<dc:title>Quantum-Enhanced Algorithmic Fairness and the Advancement of AI Integrity and Responsibility</dc:title>
			<dc:creator>Akhil Chintalapati</dc:creator>
			<dc:creator>Khashbat Enkhbat</dc:creator>
			<dc:creator>Ramanathan Annamalai</dc:creator>
			<dc:creator>Geraldine Bessie Amali</dc:creator>
			<dc:creator>Fatih Ozaydin</dc:creator>
			<dc:creator>Mathew Mithra Noel</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030036</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-08-11</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-08-11</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Perspective</prism:section>
	<prism:startingPage>36</prism:startingPage>
		<prism:doi>10.3390/quantum7030036</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/36</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/35">

	<title>Quantum Reports, Vol. 7, Pages 35: Classical Encryption Demonstration with BB84 Quantum Protocol-Inspired Coherent States Using Reduced Graphene Oxide</title>
	<link>https://www.mdpi.com/2624-960X/7/3/35</link>
	<description>This study explores the integration of reduced graphene oxide (rGO) into an optoelectronic XOR logic gate to enhance BB84 protocol encryption in quantum communication systems. The research leverages the nonlinear optical properties of rGO, specifically its nonlinear refraction characteristics, in combination with a Michelson interferometer to implement an optoelectronic XOR gate. rGO samples were deposited using the Langmuir&amp;amp;ndash;Blodgett technique and characterized in morphology and structure. The optical setup utilized a frequency-modulated laser signal for the interferometer and a pulsed laser system that generates the quantum information carrier. This integration of quantum encryption with nonlinear optical materials offers enhanced security against classical attacks while providing adaptability for various applications from secure communications to quantum AI.</description>
	<pubDate>2025-08-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 35: Classical Encryption Demonstration with BB84 Quantum Protocol-Inspired Coherent States Using Reduced Graphene Oxide</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/35">doi: 10.3390/quantum7030035</a></p>
	<p>Authors:
		Alexia Lopez-Bastida
		Pablo Córdova-Morales
		Donato Valdez-Pérez
		Adrian Martinez-Rivas
		José M. de la Rosa-Vázquez
		Carlos Torres-Torres
		</p>
	<p>This study explores the integration of reduced graphene oxide (rGO) into an optoelectronic XOR logic gate to enhance BB84 protocol encryption in quantum communication systems. The research leverages the nonlinear optical properties of rGO, specifically its nonlinear refraction characteristics, in combination with a Michelson interferometer to implement an optoelectronic XOR gate. rGO samples were deposited using the Langmuir&amp;amp;ndash;Blodgett technique and characterized in morphology and structure. The optical setup utilized a frequency-modulated laser signal for the interferometer and a pulsed laser system that generates the quantum information carrier. This integration of quantum encryption with nonlinear optical materials offers enhanced security against classical attacks while providing adaptability for various applications from secure communications to quantum AI.</p>
	]]></content:encoded>

	<dc:title>Classical Encryption Demonstration with BB84 Quantum Protocol-Inspired Coherent States Using Reduced Graphene Oxide</dc:title>
			<dc:creator>Alexia Lopez-Bastida</dc:creator>
			<dc:creator>Pablo Córdova-Morales</dc:creator>
			<dc:creator>Donato Valdez-Pérez</dc:creator>
			<dc:creator>Adrian Martinez-Rivas</dc:creator>
			<dc:creator>José M. de la Rosa-Vázquez</dc:creator>
			<dc:creator>Carlos Torres-Torres</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030035</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-08-11</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-08-11</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>35</prism:startingPage>
		<prism:doi>10.3390/quantum7030035</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/35</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/34">

	<title>Quantum Reports, Vol. 7, Pages 34: Variance-Based Uncertainty Relations: A Concise Review of Inequalities Discovered Since 1927</title>
	<link>https://www.mdpi.com/2624-960X/7/3/34</link>
	<description>A brief review of various existing mathematical formulations of the uncertainty relations in quantum mechanics, containing variances of two or more non-commuting operators, is given. In particular, inequalities for the products of higher-order moments of a coordinate and a momentum are considered, as well as inequalities making the uncertainty relations more accurate when additional information about a quantum system is available (for example, the correlation coefficient or the degree of mixing of a quantum state characterized by the trace of the squared statistical operator). The special cases of two, three, and four operators are discussed in detail.</description>
	<pubDate>2025-08-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 34: Variance-Based Uncertainty Relations: A Concise Review of Inequalities Discovered Since 1927</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/34">doi: 10.3390/quantum7030034</a></p>
	<p>Authors:
		Viktor V. Dodonov
		</p>
	<p>A brief review of various existing mathematical formulations of the uncertainty relations in quantum mechanics, containing variances of two or more non-commuting operators, is given. In particular, inequalities for the products of higher-order moments of a coordinate and a momentum are considered, as well as inequalities making the uncertainty relations more accurate when additional information about a quantum system is available (for example, the correlation coefficient or the degree of mixing of a quantum state characterized by the trace of the squared statistical operator). The special cases of two, three, and four operators are discussed in detail.</p>
	]]></content:encoded>

	<dc:title>Variance-Based Uncertainty Relations: A Concise Review of Inequalities Discovered Since 1927</dc:title>
			<dc:creator>Viktor V. Dodonov</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030034</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-08-05</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-08-05</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>34</prism:startingPage>
		<prism:doi>10.3390/quantum7030034</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/34</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/33">

	<title>Quantum Reports, Vol. 7, Pages 33: Generalizing Coherent States with the Fox H Function</title>
	<link>https://www.mdpi.com/2624-960X/7/3/33</link>
	<description>In the present scenario, coherent states of a quantum harmonic oscillator are generalized with positive Fox H auxiliary functions. The novel generalized coherent states provide canonical coherent states and Mittag-Leffler or Wright generalized coherent states, as particular cases, and resolve the identity operator, over the Fock space, with a weight function that is the product of a Fox H function and a Wright generalized hypergeometric function. The novel generalized coherent states, or the corresponding truncated generalized coherent states, are characterized by anomalous statistics for large values of the number of excitations: the corresponding decay laws exhibit, for determined values of the involved parameters, various behaviors that depart from exponential and inverse-power-law decays, or their product. The analysis of the Mandel Q factor shows that, for small values of the label, the statistics of the number of excitations becomes super-Poissonian, or sub-Poissonian, by simply choosing sufficiently large values of one of the involved parameters. The time evolution of a generalized coherent state interacting with a thermal reservoir and the purity are analyzed.</description>
	<pubDate>2025-07-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 33: Generalizing Coherent States with the Fox H Function</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/33">doi: 10.3390/quantum7030033</a></p>
	<p>Authors:
		Filippo Giraldi
		</p>
	<p>In the present scenario, coherent states of a quantum harmonic oscillator are generalized with positive Fox H auxiliary functions. The novel generalized coherent states provide canonical coherent states and Mittag-Leffler or Wright generalized coherent states, as particular cases, and resolve the identity operator, over the Fock space, with a weight function that is the product of a Fox H function and a Wright generalized hypergeometric function. The novel generalized coherent states, or the corresponding truncated generalized coherent states, are characterized by anomalous statistics for large values of the number of excitations: the corresponding decay laws exhibit, for determined values of the involved parameters, various behaviors that depart from exponential and inverse-power-law decays, or their product. The analysis of the Mandel Q factor shows that, for small values of the label, the statistics of the number of excitations becomes super-Poissonian, or sub-Poissonian, by simply choosing sufficiently large values of one of the involved parameters. The time evolution of a generalized coherent state interacting with a thermal reservoir and the purity are analyzed.</p>
	]]></content:encoded>

	<dc:title>Generalizing Coherent States with the Fox H Function</dc:title>
			<dc:creator>Filippo Giraldi</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030033</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-07-28</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-07-28</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>33</prism:startingPage>
		<prism:doi>10.3390/quantum7030033</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/33</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/32">

	<title>Quantum Reports, Vol. 7, Pages 32: Efficient Encoding of the Traveling Salesperson Problem on a Quantum Computer</title>
	<link>https://www.mdpi.com/2624-960X/7/3/32</link>
	<description>We propose an amplitude encoding of the traveling salesperson problem along with a method for calculating the cost function using a probability distribution obtained on a quantum computer. Our encoding requires a number of qubits that grows logarithmically with the number of cities. We propose to calculate the cost function using a nonlinear function of expectation values of quantum operators. This is in contrast to the typical method of evaluating the cost function by summing expectation values of quantum operators. We demonstrate our method using a variational quantum eigensolver algorithm to find the shortest route for a given graph. We find that there is a broad range in the hyperparameters of the optimization procedure for which the best route is found.</description>
	<pubDate>2025-07-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 32: Efficient Encoding of the Traveling Salesperson Problem on a Quantum Computer</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/32">doi: 10.3390/quantum7030032</a></p>
	<p>Authors:
		John P. T. Stenger
		Sean T. Crowe
		Joseph A. Diaz
		Ramiro Rodriguez
		Daniel Gunlycke
		Joanna N. Ptasinski
		</p>
	<p>We propose an amplitude encoding of the traveling salesperson problem along with a method for calculating the cost function using a probability distribution obtained on a quantum computer. Our encoding requires a number of qubits that grows logarithmically with the number of cities. We propose to calculate the cost function using a nonlinear function of expectation values of quantum operators. This is in contrast to the typical method of evaluating the cost function by summing expectation values of quantum operators. We demonstrate our method using a variational quantum eigensolver algorithm to find the shortest route for a given graph. We find that there is a broad range in the hyperparameters of the optimization procedure for which the best route is found.</p>
	]]></content:encoded>

	<dc:title>Efficient Encoding of the Traveling Salesperson Problem on a Quantum Computer</dc:title>
			<dc:creator>John P. T. Stenger</dc:creator>
			<dc:creator>Sean T. Crowe</dc:creator>
			<dc:creator>Joseph A. Diaz</dc:creator>
			<dc:creator>Ramiro Rodriguez</dc:creator>
			<dc:creator>Daniel Gunlycke</dc:creator>
			<dc:creator>Joanna N. Ptasinski</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030032</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-07-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-07-17</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>32</prism:startingPage>
		<prism:doi>10.3390/quantum7030032</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/32</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/31">

	<title>Quantum Reports, Vol. 7, Pages 31: A Comparative Analysis of a Nonlinear Phase Space Evolution of SU(2) and SU(1,1) Coherent States</title>
	<link>https://www.mdpi.com/2624-960X/7/3/31</link>
	<description>We carried out a comparative study of the phase space evolution of SU(2) and SU(1,1) coherent states generated by the same nonlinear two-mode Hamiltonian. We analyze the dynamics of the Wigner functions in the respective phase spaces and discuss the principal associated physical effects: the squeezing of the appropriate observables and the Schr&amp;amp;ouml;dinger&amp;amp;rsquo;s cat state generation characteristic of both the considered symmetry groups.</description>
	<pubDate>2025-07-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 31: A Comparative Analysis of a Nonlinear Phase Space Evolution of SU(2) and SU(1,1) Coherent States</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/31">doi: 10.3390/quantum7030031</a></p>
	<p>Authors:
		Rodrigo D. Aceves
		Miguel Baltazar
		Iván F. Valtierra
		Andrei B. Klimov
		</p>
	<p>We carried out a comparative study of the phase space evolution of SU(2) and SU(1,1) coherent states generated by the same nonlinear two-mode Hamiltonian. We analyze the dynamics of the Wigner functions in the respective phase spaces and discuss the principal associated physical effects: the squeezing of the appropriate observables and the Schr&amp;amp;ouml;dinger&amp;amp;rsquo;s cat state generation characteristic of both the considered symmetry groups.</p>
	]]></content:encoded>

	<dc:title>A Comparative Analysis of a Nonlinear Phase Space Evolution of SU(2) and SU(1,1) Coherent States</dc:title>
			<dc:creator>Rodrigo D. Aceves</dc:creator>
			<dc:creator>Miguel Baltazar</dc:creator>
			<dc:creator>Iván F. Valtierra</dc:creator>
			<dc:creator>Andrei B. Klimov</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030031</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-07-05</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-07-05</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>31</prism:startingPage>
		<prism:doi>10.3390/quantum7030031</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/31</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/30">

	<title>Quantum Reports, Vol. 7, Pages 30: Neutrino Mixing Matrix with SU(2)4 Anyon Braids</title>
	<link>https://www.mdpi.com/2624-960X/7/3/30</link>
	<description>We recently classified baryonic matter in the ground and first excited states thanks to the discrete group of braids inherent to SU(2)2 Ising anyons. Remarkably, the braids of SU(2)4 anyons allow the neutrino mixing matrix to be generated with an accuracy close to measurements. This is an improvement over the model based on tribimaximal neutrino mixing, which predicts a vanishing solar neutrino angle &amp;amp;theta;13, which has now been ruled out. The discrete group of braids for SU(2)4 anyons is isomorphic to the small group (162,14), generated by a diagonal matrix &amp;amp;sigma;1=R and a symmetric complex matrix &amp;amp;sigma;2=FRF&amp;amp;minus;1, where the (3&amp;amp;times;3) matrices F and R correspond to the fusion and exchange of anyons, respectively. We make use of the Takagi decomposition &amp;amp;sigma;2=UTDU of &amp;amp;sigma;2, where U is the expected PMNS unitary matrix and D is real and diagonal. We obtain agreement with the experimental results in about the 3&amp;amp;sigma; range for the complex entries of the PMNS matrix with the angles &amp;amp;theta;13&amp;amp;sim;10&amp;amp;deg;, &amp;amp;theta;12&amp;amp;sim;30&amp;amp;deg;, &amp;amp;theta;23&amp;amp;sim;38&amp;amp;deg;, and &amp;amp;delta;CP&amp;amp;sim;240&amp;amp;deg;. Potential physical consequences of our model are discussed.</description>
	<pubDate>2025-06-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 30: Neutrino Mixing Matrix with SU(2)4 Anyon Braids</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/30">doi: 10.3390/quantum7030030</a></p>
	<p>Authors:
		Michel Planat
		</p>
	<p>We recently classified baryonic matter in the ground and first excited states thanks to the discrete group of braids inherent to SU(2)2 Ising anyons. Remarkably, the braids of SU(2)4 anyons allow the neutrino mixing matrix to be generated with an accuracy close to measurements. This is an improvement over the model based on tribimaximal neutrino mixing, which predicts a vanishing solar neutrino angle &amp;amp;theta;13, which has now been ruled out. The discrete group of braids for SU(2)4 anyons is isomorphic to the small group (162,14), generated by a diagonal matrix &amp;amp;sigma;1=R and a symmetric complex matrix &amp;amp;sigma;2=FRF&amp;amp;minus;1, where the (3&amp;amp;times;3) matrices F and R correspond to the fusion and exchange of anyons, respectively. We make use of the Takagi decomposition &amp;amp;sigma;2=UTDU of &amp;amp;sigma;2, where U is the expected PMNS unitary matrix and D is real and diagonal. We obtain agreement with the experimental results in about the 3&amp;amp;sigma; range for the complex entries of the PMNS matrix with the angles &amp;amp;theta;13&amp;amp;sim;10&amp;amp;deg;, &amp;amp;theta;12&amp;amp;sim;30&amp;amp;deg;, &amp;amp;theta;23&amp;amp;sim;38&amp;amp;deg;, and &amp;amp;delta;CP&amp;amp;sim;240&amp;amp;deg;. Potential physical consequences of our model are discussed.</p>
	]]></content:encoded>

	<dc:title>Neutrino Mixing Matrix with SU(2)4 Anyon Braids</dc:title>
			<dc:creator>Michel Planat</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030030</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-06-23</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-06-23</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>30</prism:startingPage>
		<prism:doi>10.3390/quantum7030030</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/30</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/3/29">

	<title>Quantum Reports, Vol. 7, Pages 29: Contextual Hidden Fields Preclude the Derivation of Bell-Type Inequalities</title>
	<link>https://www.mdpi.com/2624-960X/7/3/29</link>
	<description>We show that loophole-free Bell-type no-go theorems cannot be derived in theories involving local hidden fields. At the time of measurement, a contextuality loophole appears because each particle&amp;amp;rsquo;s electromagnetic field interacts with the field of its respective apparatus, preventing the expression of the probability density as a function independent of the orientation of the measuring devices. Then, we use the dynamical evolution of the probability distribution to show that the spin-correlation integral cannot be expressed in terms of initial Cauchy data restricted to the particles. A measurement independence loophole ensues, which prevents the usage of the non-contextual correlation integrals required to demonstrate the CHSH-Bell inequality. We propose that correlated fields are the missing hidden variable triggering the coupled nonlinear oscillations of the particles, which bring about the synchronicities observed in the Einstein&amp;amp;ndash;Podolsky&amp;amp;ndash;Rosen&amp;amp;ndash;Bohm (EPRB) experiment.</description>
	<pubDate>2025-06-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 29: Contextual Hidden Fields Preclude the Derivation of Bell-Type Inequalities</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/3/29">doi: 10.3390/quantum7030029</a></p>
	<p>Authors:
		Álvaro G. López
		</p>
	<p>We show that loophole-free Bell-type no-go theorems cannot be derived in theories involving local hidden fields. At the time of measurement, a contextuality loophole appears because each particle&amp;amp;rsquo;s electromagnetic field interacts with the field of its respective apparatus, preventing the expression of the probability density as a function independent of the orientation of the measuring devices. Then, we use the dynamical evolution of the probability distribution to show that the spin-correlation integral cannot be expressed in terms of initial Cauchy data restricted to the particles. A measurement independence loophole ensues, which prevents the usage of the non-contextual correlation integrals required to demonstrate the CHSH-Bell inequality. We propose that correlated fields are the missing hidden variable triggering the coupled nonlinear oscillations of the particles, which bring about the synchronicities observed in the Einstein&amp;amp;ndash;Podolsky&amp;amp;ndash;Rosen&amp;amp;ndash;Bohm (EPRB) experiment.</p>
	]]></content:encoded>

	<dc:title>Contextual Hidden Fields Preclude the Derivation of Bell-Type Inequalities</dc:title>
			<dc:creator>Álvaro G. López</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7030029</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-06-20</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-06-20</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>29</prism:startingPage>
		<prism:doi>10.3390/quantum7030029</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/3/29</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/28">

	<title>Quantum Reports, Vol. 7, Pages 28: The Quantum Measurement Problem</title>
	<link>https://www.mdpi.com/2624-960X/7/2/28</link>
	<description>Measurements play a specific role in quantum mechanics; only measurements allow us to catch a glimpse of the eluding physical reality. However, there is something deeply unsatisfactory with this specificity&amp;amp;mdash;a measurement is itself a physical process! Several varying modes of coping with this dilemma have been proposed and this article tries to describe how a now-century-long discussion has led to new insights about the transition from the quantum to the classical world. Starting from the pioneer&amp;amp;rsquo;s view of the quantum measurement problem, it follows the development of formalisms, the interest from philosophers for its new aspects on reality and how different interpretations of quantum mechanics have tried to support our classically working brains in understanding quantum phenomena. Decoherence is a main topic and its role in measurement processes exemplified. The question of whether the quantum measurement problem is now solved is left open for the readers&amp;amp;rsquo; own judgment.</description>
	<pubDate>2025-06-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 28: The Quantum Measurement Problem</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/28">doi: 10.3390/quantum7020028</a></p>
	<p>Authors:
		Erik B. Karlsson
		</p>
	<p>Measurements play a specific role in quantum mechanics; only measurements allow us to catch a glimpse of the eluding physical reality. However, there is something deeply unsatisfactory with this specificity&amp;amp;mdash;a measurement is itself a physical process! Several varying modes of coping with this dilemma have been proposed and this article tries to describe how a now-century-long discussion has led to new insights about the transition from the quantum to the classical world. Starting from the pioneer&amp;amp;rsquo;s view of the quantum measurement problem, it follows the development of formalisms, the interest from philosophers for its new aspects on reality and how different interpretations of quantum mechanics have tried to support our classically working brains in understanding quantum phenomena. Decoherence is a main topic and its role in measurement processes exemplified. The question of whether the quantum measurement problem is now solved is left open for the readers&amp;amp;rsquo; own judgment.</p>
	]]></content:encoded>

	<dc:title>The Quantum Measurement Problem</dc:title>
			<dc:creator>Erik B. Karlsson</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020028</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-06-13</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-06-13</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>28</prism:startingPage>
		<prism:doi>10.3390/quantum7020028</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/28</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/27">

	<title>Quantum Reports, Vol. 7, Pages 27: Quantization on the Ideal Boundary and the Finite Widths of Resonances</title>
	<link>https://www.mdpi.com/2624-960X/7/2/27</link>
	<description>Conformal field theory is quantized on the ideal boundary of a Riemann surface, and the effect on the widths of the resonances of the quantum states is evaluated. The resonances on a surface can be recast in terms of eigenfunctions of a differential operator on the Mandelstam plane. Cusps in this plane, representing Landau singularities, reflect a divergence in the coupling. A cusp on the Riemann surface similarly causes a divergence in the scattering amplitude. The interpretation of the string diagram indicates that the self-interaction of the string in the vicinity of the cusp causes it to implode, which would require an infinite coupling. A consistent physical interpretation of cusps on surfaces requires supersymmetry. The study of unitary minimal models and N = 2 superminimal models indicates that there can exist a set of resonances at the cusps and ends of the surfaces. The uncertainty in the masses of six types of particles at a finite set of cusps is infinitesimal. Tachyon condensation on the ideal boundary would introduce an uncertainty in the mass of a charged particle. The widths of charged particle resonances at the ends of infinite-genus surfaces is not negligible and can be traced to the coupling with tachyons.</description>
	<pubDate>2025-06-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 27: Quantization on the Ideal Boundary and the Finite Widths of Resonances</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/27">doi: 10.3390/quantum7020027</a></p>
	<p>Authors:
		Simon Davis
		</p>
	<p>Conformal field theory is quantized on the ideal boundary of a Riemann surface, and the effect on the widths of the resonances of the quantum states is evaluated. The resonances on a surface can be recast in terms of eigenfunctions of a differential operator on the Mandelstam plane. Cusps in this plane, representing Landau singularities, reflect a divergence in the coupling. A cusp on the Riemann surface similarly causes a divergence in the scattering amplitude. The interpretation of the string diagram indicates that the self-interaction of the string in the vicinity of the cusp causes it to implode, which would require an infinite coupling. A consistent physical interpretation of cusps on surfaces requires supersymmetry. The study of unitary minimal models and N = 2 superminimal models indicates that there can exist a set of resonances at the cusps and ends of the surfaces. The uncertainty in the masses of six types of particles at a finite set of cusps is infinitesimal. Tachyon condensation on the ideal boundary would introduce an uncertainty in the mass of a charged particle. The widths of charged particle resonances at the ends of infinite-genus surfaces is not negligible and can be traced to the coupling with tachyons.</p>
	]]></content:encoded>

	<dc:title>Quantization on the Ideal Boundary and the Finite Widths of Resonances</dc:title>
			<dc:creator>Simon Davis</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020027</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-06-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-06-12</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>27</prism:startingPage>
		<prism:doi>10.3390/quantum7020027</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/27</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/26">

	<title>Quantum Reports, Vol. 7, Pages 26: Innovative Designs and Insights into Quantum Thermal Machines</title>
	<link>https://www.mdpi.com/2624-960X/7/2/26</link>
	<description>We present a comprehensive theoretical investigation about the operational regions of quantum systems, specifically examining their roles as working media functioning between two thermal reservoirs in quantum thermal machines (QTMs). This study provides relevant and novel insights, including a complete spectrum of QTMs within the operational region of these quantum systems, and introduces new QTM designs never before described in the literature. Additionally, this work introduces a standardized and cohesive classification scheme for QTMs, ensuring robustness in nomenclature and operational distinctions, which enhances both theoretical understanding and practical application. Notably, one of these designs directly addresses the need for a more appropriate explanation of the operation of a laser (or maser) as a QTM. Initial calculations were performed to achieve results applicable to any quantum system subjected to rules analogous to those used in classical thermal machine studies. These results were then used to analyze two-level quantum systems as the working medium of QTMs in the Otto cycle. In particular, we analyzed two specific quantum systems: the laser and a spinless electron in a one-dimensional quantum ring, yielding consistent and innovative results. Overall, this study offers valuable insights into the operation and classification of QTMs, establishing a clear and unified framework for their nomenclature while opening new avenues for the design and enhancement of these devices.</description>
	<pubDate>2025-06-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 26: Innovative Designs and Insights into Quantum Thermal Machines</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/26">doi: 10.3390/quantum7020026</a></p>
	<p>Authors:
		Aline Duarte Lúcio
		Moises Rojas
		Cleverson Filgueiras
		</p>
	<p>We present a comprehensive theoretical investigation about the operational regions of quantum systems, specifically examining their roles as working media functioning between two thermal reservoirs in quantum thermal machines (QTMs). This study provides relevant and novel insights, including a complete spectrum of QTMs within the operational region of these quantum systems, and introduces new QTM designs never before described in the literature. Additionally, this work introduces a standardized and cohesive classification scheme for QTMs, ensuring robustness in nomenclature and operational distinctions, which enhances both theoretical understanding and practical application. Notably, one of these designs directly addresses the need for a more appropriate explanation of the operation of a laser (or maser) as a QTM. Initial calculations were performed to achieve results applicable to any quantum system subjected to rules analogous to those used in classical thermal machine studies. These results were then used to analyze two-level quantum systems as the working medium of QTMs in the Otto cycle. In particular, we analyzed two specific quantum systems: the laser and a spinless electron in a one-dimensional quantum ring, yielding consistent and innovative results. Overall, this study offers valuable insights into the operation and classification of QTMs, establishing a clear and unified framework for their nomenclature while opening new avenues for the design and enhancement of these devices.</p>
	]]></content:encoded>

	<dc:title>Innovative Designs and Insights into Quantum Thermal Machines</dc:title>
			<dc:creator>Aline Duarte Lúcio</dc:creator>
			<dc:creator>Moises Rojas</dc:creator>
			<dc:creator>Cleverson Filgueiras</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020026</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-06-04</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-06-04</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>26</prism:startingPage>
		<prism:doi>10.3390/quantum7020026</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/26</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/25">

	<title>Quantum Reports, Vol. 7, Pages 25: Developing and Analyzing the Defect-Based Surface Codes Using Optimization Algorithms</title>
	<link>https://www.mdpi.com/2624-960X/7/2/25</link>
	<description>Fault tolerance is crucial for enabling large-scale quantum computations, with surface codes emerging as prominent error correction techniques due to their high error threshold and reliance on nearest-neighbor interactions. Despite the advantages of surface codes, they demand a substantial number of qubits to encode a single logical qubit, making them resource-intensive. Two primary approaches exist to encode multiple logical qubits: patch-based and defect-based. This study focuses on the latter approach, which involves creating holes in the surface code for logical qubit encoding. With the defect-based approach, we need to account for trade-offs between the number of logical qubits and the logical error rates, so we employ an optimization algorithm to evaluate the maximum number of logical qubits for a given error rate. Through a series of experiments, we assess the limitations of the defect-based approach and investigate the impact of various hole types on logical qubit encoding.</description>
	<pubDate>2025-05-31</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 25: Developing and Analyzing the Defect-Based Surface Codes Using Optimization Algorithms</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/25">doi: 10.3390/quantum7020025</a></p>
	<p>Authors:
		Samira Sayedsalehi
		Nader Bagherzadeh
		Alberto A. Del Barrio
		Guillermo Botella
		Ratko Pilipović
		</p>
	<p>Fault tolerance is crucial for enabling large-scale quantum computations, with surface codes emerging as prominent error correction techniques due to their high error threshold and reliance on nearest-neighbor interactions. Despite the advantages of surface codes, they demand a substantial number of qubits to encode a single logical qubit, making them resource-intensive. Two primary approaches exist to encode multiple logical qubits: patch-based and defect-based. This study focuses on the latter approach, which involves creating holes in the surface code for logical qubit encoding. With the defect-based approach, we need to account for trade-offs between the number of logical qubits and the logical error rates, so we employ an optimization algorithm to evaluate the maximum number of logical qubits for a given error rate. Through a series of experiments, we assess the limitations of the defect-based approach and investigate the impact of various hole types on logical qubit encoding.</p>
	]]></content:encoded>

	<dc:title>Developing and Analyzing the Defect-Based Surface Codes Using Optimization Algorithms</dc:title>
			<dc:creator>Samira Sayedsalehi</dc:creator>
			<dc:creator>Nader Bagherzadeh</dc:creator>
			<dc:creator>Alberto A. Del Barrio</dc:creator>
			<dc:creator>Guillermo Botella</dc:creator>
			<dc:creator>Ratko Pilipović</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020025</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-05-31</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-05-31</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>25</prism:startingPage>
		<prism:doi>10.3390/quantum7020025</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/25</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/24">

	<title>Quantum Reports, Vol. 7, Pages 24: Theory and Applications of Quantum Hashing</title>
	<link>https://www.mdpi.com/2624-960X/7/2/24</link>
	<description>We review recent results on quantum one-way functions, including quantum fingerprinting or quantum hashing (we use these two terms as synonyms even though they have very small difference). This includes the analysis of their properties, different modifications, circuit implementation on an IBM Q platform, as well as on an experimental quantum setup. We discuss computational aspects of quantum hashing, its cryptographic properties and possible usage in communication protocols and algorithms.</description>
	<pubDate>2025-05-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 24: Theory and Applications of Quantum Hashing</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/24">doi: 10.3390/quantum7020024</a></p>
	<p>Authors:
		Farid Ablayev
		Kamil Khadiev
		Alexander Vasiliev
		Mansur Ziiatdinov
		</p>
	<p>We review recent results on quantum one-way functions, including quantum fingerprinting or quantum hashing (we use these two terms as synonyms even though they have very small difference). This includes the analysis of their properties, different modifications, circuit implementation on an IBM Q platform, as well as on an experimental quantum setup. We discuss computational aspects of quantum hashing, its cryptographic properties and possible usage in communication protocols and algorithms.</p>
	]]></content:encoded>

	<dc:title>Theory and Applications of Quantum Hashing</dc:title>
			<dc:creator>Farid Ablayev</dc:creator>
			<dc:creator>Kamil Khadiev</dc:creator>
			<dc:creator>Alexander Vasiliev</dc:creator>
			<dc:creator>Mansur Ziiatdinov</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020024</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-05-15</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-05-15</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>24</prism:startingPage>
		<prism:doi>10.3390/quantum7020024</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/24</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/23">

	<title>Quantum Reports, Vol. 7, Pages 23: Evolving Probability Representations of Entangled Cat States in the Potentials of Harmonic and Inverted Oscillators</title>
	<link>https://www.mdpi.com/2624-960X/7/2/23</link>
	<description>We determine the evolving probability representation of entangled cat states in the potential of either the harmonic oscillator or the inverted oscillator, assuming that the states are initially prepared in the potential of the harmonic oscillator. Such states have several applications in quantum information processing. The inverted quantum harmonic oscillator, where the potential energy corresponds to imaginary frequencies of the oscillator, can be applied in relation to cosmological problems. We also determine the evolving probability representation of cat states of an oscillating spin-1/2 particle of the inverted oscillator, in which the time evolution of the spin state is described by an arbitrary unitary operator. The properties of the determined entangled probability distributions are discussed.</description>
	<pubDate>2025-05-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 23: Evolving Probability Representations of Entangled Cat States in the Potentials of Harmonic and Inverted Oscillators</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/23">doi: 10.3390/quantum7020023</a></p>
	<p>Authors:
		Matyas Mechler
		Margarita A. Man’ko
		Vladimir I. Man’ko
		Peter Adam
		</p>
	<p>We determine the evolving probability representation of entangled cat states in the potential of either the harmonic oscillator or the inverted oscillator, assuming that the states are initially prepared in the potential of the harmonic oscillator. Such states have several applications in quantum information processing. The inverted quantum harmonic oscillator, where the potential energy corresponds to imaginary frequencies of the oscillator, can be applied in relation to cosmological problems. We also determine the evolving probability representation of cat states of an oscillating spin-1/2 particle of the inverted oscillator, in which the time evolution of the spin state is described by an arbitrary unitary operator. The properties of the determined entangled probability distributions are discussed.</p>
	]]></content:encoded>

	<dc:title>Evolving Probability Representations of Entangled Cat States in the Potentials of Harmonic and Inverted Oscillators</dc:title>
			<dc:creator>Matyas Mechler</dc:creator>
			<dc:creator>Margarita A. Man’ko</dc:creator>
			<dc:creator>Vladimir I. Man’ko</dc:creator>
			<dc:creator>Peter Adam</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020023</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-05-02</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-05-02</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>23</prism:startingPage>
		<prism:doi>10.3390/quantum7020023</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/23</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/22">

	<title>Quantum Reports, Vol. 7, Pages 22: Probability Representation of Quantum States: Tomographic Representation in Standard Potentials and Peres&amp;ndash;Horodecki Criterion for Probabilities</title>
	<link>https://www.mdpi.com/2624-960X/7/2/22</link>
	<description>In connection with the International Year of Quantum Science and Technology, a review of joint works of the Lebedev Institute and the Mexican research group at UNAM is presented, especially related to solving the old problem of the state description, not only by wave functions but also by conventional probability distributions analogous to quasiprobability distributions, like the Wigner function. Also, explicit expressions of tomographic representations describing the quantum states of particles moving in known potential wells are obtained and briefly discussed. In particular, we present the examples of the tomographic distributions for the free evolution, finite and infinite potential wells, and the Morse potential. Additional to this, an extension of the Peres&amp;amp;ndash;Horodecki separability criteria for momentum probability distributions is presented in the case of bipartite, asymmetrical, real states.</description>
	<pubDate>2025-04-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 22: Probability Representation of Quantum States: Tomographic Representation in Standard Potentials and Peres&amp;ndash;Horodecki Criterion for Probabilities</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/22">doi: 10.3390/quantum7020022</a></p>
	<p>Authors:
		Julio A. López-Saldívar
		Margarita A. Man’ko
		Vladimir I. Man’ko
		</p>
	<p>In connection with the International Year of Quantum Science and Technology, a review of joint works of the Lebedev Institute and the Mexican research group at UNAM is presented, especially related to solving the old problem of the state description, not only by wave functions but also by conventional probability distributions analogous to quasiprobability distributions, like the Wigner function. Also, explicit expressions of tomographic representations describing the quantum states of particles moving in known potential wells are obtained and briefly discussed. In particular, we present the examples of the tomographic distributions for the free evolution, finite and infinite potential wells, and the Morse potential. Additional to this, an extension of the Peres&amp;amp;ndash;Horodecki separability criteria for momentum probability distributions is presented in the case of bipartite, asymmetrical, real states.</p>
	]]></content:encoded>

	<dc:title>Probability Representation of Quantum States: Tomographic Representation in Standard Potentials and Peres&amp;amp;ndash;Horodecki Criterion for Probabilities</dc:title>
			<dc:creator>Julio A. López-Saldívar</dc:creator>
			<dc:creator>Margarita A. Man’ko</dc:creator>
			<dc:creator>Vladimir I. Man’ko</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020022</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-24</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-24</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>22</prism:startingPage>
		<prism:doi>10.3390/quantum7020022</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/22</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/21">

	<title>Quantum Reports, Vol. 7, Pages 21: Simulating Methylamine Using a Symmetry-Adapted, Qubit Excitation-Based Variational Quantum Eigensolver</title>
	<link>https://www.mdpi.com/2624-960X/7/2/21</link>
	<description>Understanding the capabilities of quantum computer devices and computing the required resources to solve realistic tasks remain critical challenges associated with achieving useful quantum computational advantage. We present a study aimed at reducing the quantum resource overhead in quantum chemistry simulations using the variational quantum eigensolver (VQE). Our approach achieves up to a two-orders-of magnitude reduction in the required number of two-qubit operations for variational problem-inspired ansatzes. We propose and analyze optimization strategies that combine various methods, including molecular point-group symmetries, compact excitation circuits, different types of excitation sets, and qubit tapering. To validate the compatibility and accuracy of these strategies, we first test them on small molecules such as LiH and BeH2, then apply the most efficient ones to restricted active-space simulations of methylamine. We complete our analysis by computing the resources required for full-valence, active-space simulations of methylamine (26 qubits) and formic acid (28 qubits) molecules. Our best-performing optimization strategy reduces the two-qubit gate count for methylamine from approximately 600,000 to about 12,000 and yields a similar order-of-magnitude improvement for formic acid. This resource analysis represents a valuable step towards the practical use of quantum computers and the development of better methods for optimizing computing resources.</description>
	<pubDate>2025-04-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 21: Simulating Methylamine Using a Symmetry-Adapted, Qubit Excitation-Based Variational Quantum Eigensolver</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/21">doi: 10.3390/quantum7020021</a></p>
	<p>Authors:
		Konstantin M. Makushin
		Aleksey K. Fedorov
		</p>
	<p>Understanding the capabilities of quantum computer devices and computing the required resources to solve realistic tasks remain critical challenges associated with achieving useful quantum computational advantage. We present a study aimed at reducing the quantum resource overhead in quantum chemistry simulations using the variational quantum eigensolver (VQE). Our approach achieves up to a two-orders-of magnitude reduction in the required number of two-qubit operations for variational problem-inspired ansatzes. We propose and analyze optimization strategies that combine various methods, including molecular point-group symmetries, compact excitation circuits, different types of excitation sets, and qubit tapering. To validate the compatibility and accuracy of these strategies, we first test them on small molecules such as LiH and BeH2, then apply the most efficient ones to restricted active-space simulations of methylamine. We complete our analysis by computing the resources required for full-valence, active-space simulations of methylamine (26 qubits) and formic acid (28 qubits) molecules. Our best-performing optimization strategy reduces the two-qubit gate count for methylamine from approximately 600,000 to about 12,000 and yields a similar order-of-magnitude improvement for formic acid. This resource analysis represents a valuable step towards the practical use of quantum computers and the development of better methods for optimizing computing resources.</p>
	]]></content:encoded>

	<dc:title>Simulating Methylamine Using a Symmetry-Adapted, Qubit Excitation-Based Variational Quantum Eigensolver</dc:title>
			<dc:creator>Konstantin M. Makushin</dc:creator>
			<dc:creator>Aleksey K. Fedorov</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020021</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-21</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-21</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>21</prism:startingPage>
		<prism:doi>10.3390/quantum7020021</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/21</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/20">

	<title>Quantum Reports, Vol. 7, Pages 20: Diffusion in a Comb-Structured Media: Non-Local Terms and Stochastic Resetting</title>
	<link>https://www.mdpi.com/2624-960X/7/2/20</link>
	<description>We examine the dynamics of a system influenced by a backbone structure, incorporating linear non-local terms that account for both irreversible and reversible processes, such as absorption and adsorption&amp;amp;ndash;desorption. Additionally, we introduce stochastic resetting to analyze its effects on the system&amp;amp;rsquo;s behavior from both analytical and numerical perspectives. Our findings reveal a rich spectrum of dynamics, emphasizing connections to anomalous diffusion and providing new insights into transport phenomena in complex environments.</description>
	<pubDate>2025-04-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 20: Diffusion in a Comb-Structured Media: Non-Local Terms and Stochastic Resetting</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/20">doi: 10.3390/quantum7020020</a></p>
	<p>Authors:
		Ervin Kaminski Lenzi
		Derik William Gryczak
		Luciano Rodrigues da Silva
		Haroldo Valentin Ribeiro
		Rafael Soares Zola
		</p>
	<p>We examine the dynamics of a system influenced by a backbone structure, incorporating linear non-local terms that account for both irreversible and reversible processes, such as absorption and adsorption&amp;amp;ndash;desorption. Additionally, we introduce stochastic resetting to analyze its effects on the system&amp;amp;rsquo;s behavior from both analytical and numerical perspectives. Our findings reveal a rich spectrum of dynamics, emphasizing connections to anomalous diffusion and providing new insights into transport phenomena in complex environments.</p>
	]]></content:encoded>

	<dc:title>Diffusion in a Comb-Structured Media: Non-Local Terms and Stochastic Resetting</dc:title>
			<dc:creator>Ervin Kaminski Lenzi</dc:creator>
			<dc:creator>Derik William Gryczak</dc:creator>
			<dc:creator>Luciano Rodrigues da Silva</dc:creator>
			<dc:creator>Haroldo Valentin Ribeiro</dc:creator>
			<dc:creator>Rafael Soares Zola</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020020</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-14</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-14</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>20</prism:startingPage>
		<prism:doi>10.3390/quantum7020020</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/19">

	<title>Quantum Reports, Vol. 7, Pages 19: Towards a Multiqudit Quantum Processor Based on a 171Yb+ Ion String: Realizing Basic Quantum Algorithms</title>
	<link>https://www.mdpi.com/2624-960X/7/2/19</link>
	<description>We demonstrate a quantum processor based on a 3D linear Paul trap that uses Yb+171 ions with eight individually controllable four-level qudits (ququarts), which is computationally equivalent to a sixteen-qubit quantum processor. The design of the developed ion trap provides high secular frequencies and a low heating rate, which, together with individual addressing and readout optical systems, allows executing quantum algorithms. In each of the eight ions, we use four electronic levels coupled by E2 optical transition at 435 nm for qudit encoding. We present the results of single- and two-qubit operations benchmarking and realizing basic quantum algorithms, including the Bernstein&amp;amp;ndash;Vazirani and Grover&amp;amp;rsquo;s search algorithms as well as H2 and LiH molecular simulations. Our results pave the way to scalable qudit-based quantum processors using trapped ions.</description>
	<pubDate>2025-04-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 19: Towards a Multiqudit Quantum Processor Based on a 171Yb+ Ion String: Realizing Basic Quantum Algorithms</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/19">doi: 10.3390/quantum7020019</a></p>
	<p>Authors:
		Ilia V. Zalivako
		Anastasiia S. Nikolaeva
		Alexander S. Borisenko
		Andrei E. Korolkov
		Pavel L. Sidorov
		Kristina P. Galstyan
		Nikita V. Semenin
		Vasilii N. Smirnov
		Mikhail A. Aksenov
		Konstantin M. Makushin
		Evgeniy O. Kiktenko
		Aleksey K. Fedorov
		Ilya A. Semerikov
		Ksenia Yu. Khabarova
		Nikolay N. Kolachevsky
		</p>
	<p>We demonstrate a quantum processor based on a 3D linear Paul trap that uses Yb+171 ions with eight individually controllable four-level qudits (ququarts), which is computationally equivalent to a sixteen-qubit quantum processor. The design of the developed ion trap provides high secular frequencies and a low heating rate, which, together with individual addressing and readout optical systems, allows executing quantum algorithms. In each of the eight ions, we use four electronic levels coupled by E2 optical transition at 435 nm for qudit encoding. We present the results of single- and two-qubit operations benchmarking and realizing basic quantum algorithms, including the Bernstein&amp;amp;ndash;Vazirani and Grover&amp;amp;rsquo;s search algorithms as well as H2 and LiH molecular simulations. Our results pave the way to scalable qudit-based quantum processors using trapped ions.</p>
	]]></content:encoded>

	<dc:title>Towards a Multiqudit Quantum Processor Based on a 171Yb+ Ion String: Realizing Basic Quantum Algorithms</dc:title>
			<dc:creator>Ilia V. Zalivako</dc:creator>
			<dc:creator>Anastasiia S. Nikolaeva</dc:creator>
			<dc:creator>Alexander S. Borisenko</dc:creator>
			<dc:creator>Andrei E. Korolkov</dc:creator>
			<dc:creator>Pavel L. Sidorov</dc:creator>
			<dc:creator>Kristina P. Galstyan</dc:creator>
			<dc:creator>Nikita V. Semenin</dc:creator>
			<dc:creator>Vasilii N. Smirnov</dc:creator>
			<dc:creator>Mikhail A. Aksenov</dc:creator>
			<dc:creator>Konstantin M. Makushin</dc:creator>
			<dc:creator>Evgeniy O. Kiktenko</dc:creator>
			<dc:creator>Aleksey K. Fedorov</dc:creator>
			<dc:creator>Ilya A. Semerikov</dc:creator>
			<dc:creator>Ksenia Yu. Khabarova</dc:creator>
			<dc:creator>Nikolay N. Kolachevsky</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020019</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-12</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-12</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>19</prism:startingPage>
		<prism:doi>10.3390/quantum7020019</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/18">

	<title>Quantum Reports, Vol. 7, Pages 18: Quantum Classical Algorithm for the Study of Phase Transitions in the Hubbard Model via Dynamical Mean-Field Theory</title>
	<link>https://www.mdpi.com/2624-960X/7/2/18</link>
	<description>Modeling many-body quantum systems is widely regarded as one of the most promising applications for near-term noisy quantum computers. However, in the near term, system size limitation will remain a severe barrier for applications in materials science or strongly correlated systems. A promising avenue of research is to combine many-body physics with machine learning for the classification of distinct phases. We present a workflow that synergizes quantum computing, many-body theory, and quantum machine learning (QML) for studying strongly correlated systems. In particular, it can capture a putative quantum phase transition of the stereotypical strongly correlated system, the Hubbard model. Following the recent proposal of the hybrid quantum-classical algorithm for the two-site dynamical mean-field theory (DMFT), we present a modification that allows the self-consistent solution of the single bath site DMFT. The modified algorithm can be generalized for multiple bath sites. This approach is used to generate a database of zero-temperature wavefunctions of the Hubbard model within the DMFT approximation. We then use a QML algorithm to distinguish between the metallic phase and the Mott insulator phase to capture the metal-to-Mott insulator phase transition. We train a recently proposed quantum convolutional neural network (QCNN) and then utilize the QCNN as a quantum classifier to capture the phase transition region. This work provides a recipe for application to other phase transitions in strongly correlated systems and represents an exciting application of small-scale quantum devices realizable with near-term technology.</description>
	<pubDate>2025-04-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 18: Quantum Classical Algorithm for the Study of Phase Transitions in the Hubbard Model via Dynamical Mean-Field Theory</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/18">doi: 10.3390/quantum7020018</a></p>
	<p>Authors:
		Anshumitra Baul
		Herbert Fotso
		Hanna Terletska
		Ka-Ming Tam
		Juana Moreno
		</p>
	<p>Modeling many-body quantum systems is widely regarded as one of the most promising applications for near-term noisy quantum computers. However, in the near term, system size limitation will remain a severe barrier for applications in materials science or strongly correlated systems. A promising avenue of research is to combine many-body physics with machine learning for the classification of distinct phases. We present a workflow that synergizes quantum computing, many-body theory, and quantum machine learning (QML) for studying strongly correlated systems. In particular, it can capture a putative quantum phase transition of the stereotypical strongly correlated system, the Hubbard model. Following the recent proposal of the hybrid quantum-classical algorithm for the two-site dynamical mean-field theory (DMFT), we present a modification that allows the self-consistent solution of the single bath site DMFT. The modified algorithm can be generalized for multiple bath sites. This approach is used to generate a database of zero-temperature wavefunctions of the Hubbard model within the DMFT approximation. We then use a QML algorithm to distinguish between the metallic phase and the Mott insulator phase to capture the metal-to-Mott insulator phase transition. We train a recently proposed quantum convolutional neural network (QCNN) and then utilize the QCNN as a quantum classifier to capture the phase transition region. This work provides a recipe for application to other phase transitions in strongly correlated systems and represents an exciting application of small-scale quantum devices realizable with near-term technology.</p>
	]]></content:encoded>

	<dc:title>Quantum Classical Algorithm for the Study of Phase Transitions in the Hubbard Model via Dynamical Mean-Field Theory</dc:title>
			<dc:creator>Anshumitra Baul</dc:creator>
			<dc:creator>Herbert Fotso</dc:creator>
			<dc:creator>Hanna Terletska</dc:creator>
			<dc:creator>Ka-Ming Tam</dc:creator>
			<dc:creator>Juana Moreno</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020018</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-04</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-04</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>18</prism:startingPage>
		<prism:doi>10.3390/quantum7020018</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/17">

	<title>Quantum Reports, Vol. 7, Pages 17: Analysis of D-Wave Topologies with k-Hop-Based Graph Metrics</title>
	<link>https://www.mdpi.com/2624-960X/7/2/17</link>
	<description>In this paper, we present a graph-based analysis of the topology of D-Wave quantum computers, focusing on the Pegasus, Chimera, and Zephyr architectures. We investigate these topologies under different parameter settings using k-hop-based graph metrics. Each of these architectures comprises distinct subgraphs in which qubits are interconnected according to specific patterns dictated by their implementation. Our study pursues two primary objectives. First, we analyze the structural properties of the Chimera, Pegasus, and Zephyr topologies, examining their scalability and connectivity characteristics. Second, we evaluate the behavior of graph-based density and redundancy metrics within these architectures. The inherent symmetries of these quantum hardware designs provide a unique opportunity to systematically assess the effectiveness of these metrics across varying connectivity patterns. By leveraging these symmetries, our findings not only enhance the understanding of these topological structures but also offer deeper insights into the reliability and applicability of the proposed metrics in the broader context of quantum hardware design.</description>
	<pubDate>2025-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 17: Analysis of D-Wave Topologies with k-Hop-Based Graph Metrics</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/17">doi: 10.3390/quantum7020017</a></p>
	<p>Authors:
		Csaba Biró
		Gábor Kusper
		</p>
	<p>In this paper, we present a graph-based analysis of the topology of D-Wave quantum computers, focusing on the Pegasus, Chimera, and Zephyr architectures. We investigate these topologies under different parameter settings using k-hop-based graph metrics. Each of these architectures comprises distinct subgraphs in which qubits are interconnected according to specific patterns dictated by their implementation. Our study pursues two primary objectives. First, we analyze the structural properties of the Chimera, Pegasus, and Zephyr topologies, examining their scalability and connectivity characteristics. Second, we evaluate the behavior of graph-based density and redundancy metrics within these architectures. The inherent symmetries of these quantum hardware designs provide a unique opportunity to systematically assess the effectiveness of these metrics across varying connectivity patterns. By leveraging these symmetries, our findings not only enhance the understanding of these topological structures but also offer deeper insights into the reliability and applicability of the proposed metrics in the broader context of quantum hardware design.</p>
	]]></content:encoded>

	<dc:title>Analysis of D-Wave Topologies with k-Hop-Based Graph Metrics</dc:title>
			<dc:creator>Csaba Biró</dc:creator>
			<dc:creator>Gábor Kusper</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020017</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-04-02</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-04-02</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>17</prism:startingPage>
		<prism:doi>10.3390/quantum7020017</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/16">

	<title>Quantum Reports, Vol. 7, Pages 16: In-Field Quantum-Protected Control-Based Key Distribution with a Lossy Urban Fiber Link</title>
	<link>https://www.mdpi.com/2624-960X/7/2/16</link>
	<description>Quantum cryptography protocols offering unconditional protection open great rout to full information security in quantum era. Yet, implementing these protocols using the existing fiber networks remains challenging due to high signal losses reducing the efficiency of these protocols to zero. The recently proposed quantum-protected control-based key distribution (QCKD) addresses this issue by physically controlling interceptable losses and ensuring that leaked quantum states remain non-orthogonal. Here, we present the first in-field development and demonstration of the QCKD over an urban fiber link characterized by substantial losses. Using information-theoretic considerations, we configure the system ensuring security and investigate the interplay between line losses and secret key rates. As an example, we present calculation for the communication distance 4 km, QCKD rate 490 bits per second, and find that the corresponding system&amp;amp;rsquo;s total loss is about 1.628 decibels. Our results, backed by the statistical analysis of the secret key, confirm QCKD&amp;amp;rsquo;s robustness under real-world conditions, and establish it as a practical solution for quantum-safe communications over existing fiber infrastructures.</description>
	<pubDate>2025-03-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 16: In-Field Quantum-Protected Control-Based Key Distribution with a Lossy Urban Fiber Link</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/16">doi: 10.3390/quantum7020016</a></p>
	<p>Authors:
		Vladlen Statiev
		Abdufattokh Ashurov
		Vladimir Semenov
		Dmitrii Kozliuk
		Vladislav Zemlyanov
		Aleksei Kodukhov
		Valeria Pastushenko
		Valerii Vinokur
		Markus Pflitsch
		</p>
	<p>Quantum cryptography protocols offering unconditional protection open great rout to full information security in quantum era. Yet, implementing these protocols using the existing fiber networks remains challenging due to high signal losses reducing the efficiency of these protocols to zero. The recently proposed quantum-protected control-based key distribution (QCKD) addresses this issue by physically controlling interceptable losses and ensuring that leaked quantum states remain non-orthogonal. Here, we present the first in-field development and demonstration of the QCKD over an urban fiber link characterized by substantial losses. Using information-theoretic considerations, we configure the system ensuring security and investigate the interplay between line losses and secret key rates. As an example, we present calculation for the communication distance 4 km, QCKD rate 490 bits per second, and find that the corresponding system&amp;amp;rsquo;s total loss is about 1.628 decibels. Our results, backed by the statistical analysis of the secret key, confirm QCKD&amp;amp;rsquo;s robustness under real-world conditions, and establish it as a practical solution for quantum-safe communications over existing fiber infrastructures.</p>
	]]></content:encoded>

	<dc:title>In-Field Quantum-Protected Control-Based Key Distribution with a Lossy Urban Fiber Link</dc:title>
			<dc:creator>Vladlen Statiev</dc:creator>
			<dc:creator>Abdufattokh Ashurov</dc:creator>
			<dc:creator>Vladimir Semenov</dc:creator>
			<dc:creator>Dmitrii Kozliuk</dc:creator>
			<dc:creator>Vladislav Zemlyanov</dc:creator>
			<dc:creator>Aleksei Kodukhov</dc:creator>
			<dc:creator>Valeria Pastushenko</dc:creator>
			<dc:creator>Valerii Vinokur</dc:creator>
			<dc:creator>Markus Pflitsch</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020016</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-03-28</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-03-28</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>16</prism:startingPage>
		<prism:doi>10.3390/quantum7020016</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/2/15">

	<title>Quantum Reports, Vol. 7, Pages 15: Superoperator Approach to the Lindbladian Dynamics of a Mirror-Field System</title>
	<link>https://www.mdpi.com/2624-960X/7/2/15</link>
	<description>We use superoperator techniques to solve the master equation for the interaction between a single-mode quantized field and a single mechanical mode of a moving mirror, which is coupled to a zero-temperature reservoir that damps its amplitude. The solution we provide allows for its application in any initial state of the combined system. Furthermore, we obtain solutions to the stationary master equation for an initial number state for the field that is consistent with the result obtained for the average number of phonons.</description>
	<pubDate>2025-03-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 15: Superoperator Approach to the Lindbladian Dynamics of a Mirror-Field System</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/2/15">doi: 10.3390/quantum7020015</a></p>
	<p>Authors:
		Marco A. García-Márquez
		Héctor M. Moya-Cessa
		</p>
	<p>We use superoperator techniques to solve the master equation for the interaction between a single-mode quantized field and a single mechanical mode of a moving mirror, which is coupled to a zero-temperature reservoir that damps its amplitude. The solution we provide allows for its application in any initial state of the combined system. Furthermore, we obtain solutions to the stationary master equation for an initial number state for the field that is consistent with the result obtained for the average number of phonons.</p>
	]]></content:encoded>

	<dc:title>Superoperator Approach to the Lindbladian Dynamics of a Mirror-Field System</dc:title>
			<dc:creator>Marco A. García-Márquez</dc:creator>
			<dc:creator>Héctor M. Moya-Cessa</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7020015</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-03-24</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-03-24</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/quantum7020015</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/2/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/1/14">

	<title>Quantum Reports, Vol. 7, Pages 14: On the Holographic Spectral Effects of Time-Interval Subdivisions</title>
	<link>https://www.mdpi.com/2624-960X/7/1/14</link>
	<description>Drawing on formal parallels between scalar diffraction theory and quantum mechanics, it is demonstrated that quantum wavefunction propagation requires a holographic model of time. Measurable time manifests between interactions as a duration which is encoded in the frequency domain. It is thus a unified entity, and attempts to subdivide these intervals introduce oscillatory artifacts or spectral broadening, altering the system&amp;amp;rsquo;s physical characteristics. Analogous to spatial holograms, where information is distributed across interference patterns, temporal intervals encode information as a discrete whole. This framework challenges the concept of continuous time evolution, suggesting instead that discrete trajectories define a frequency spectrum which holographically constructs the associated time interval, giving rise to the experimentally observed energy spread of particles in applications such as time-bin entanglement, ultra-fast light pulses, and the temporal double slit. A generalized model of quantum wavefunction propagation based on recursive Fourier transforms is discussed, and novel applications are proposed, including starlight analysis and quantum cryptography.</description>
	<pubDate>2025-03-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 14: On the Holographic Spectral Effects of Time-Interval Subdivisions</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/1/14">doi: 10.3390/quantum7010014</a></p>
	<p>Authors:
		Sky Nelson-Isaacs
		</p>
	<p>Drawing on formal parallels between scalar diffraction theory and quantum mechanics, it is demonstrated that quantum wavefunction propagation requires a holographic model of time. Measurable time manifests between interactions as a duration which is encoded in the frequency domain. It is thus a unified entity, and attempts to subdivide these intervals introduce oscillatory artifacts or spectral broadening, altering the system&amp;amp;rsquo;s physical characteristics. Analogous to spatial holograms, where information is distributed across interference patterns, temporal intervals encode information as a discrete whole. This framework challenges the concept of continuous time evolution, suggesting instead that discrete trajectories define a frequency spectrum which holographically constructs the associated time interval, giving rise to the experimentally observed energy spread of particles in applications such as time-bin entanglement, ultra-fast light pulses, and the temporal double slit. A generalized model of quantum wavefunction propagation based on recursive Fourier transforms is discussed, and novel applications are proposed, including starlight analysis and quantum cryptography.</p>
	]]></content:encoded>

	<dc:title>On the Holographic Spectral Effects of Time-Interval Subdivisions</dc:title>
			<dc:creator>Sky Nelson-Isaacs</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7010014</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-03-19</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-03-19</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/quantum7010014</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/1/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/1/13">

	<title>Quantum Reports, Vol. 7, Pages 13: Thermodynamic and Magnetic Properties of Weakly Interacting Electron Gas Localized in a CdSe Cylindrical Core&amp;ndash;Shell Quantum Dot</title>
	<link>https://www.mdpi.com/2624-960X/7/1/13</link>
	<description>The thermodynamic and magnetic properties of weakly interacting electron gas localized in a CdSe cylindrical core&amp;amp;ndash;shell quantum dot in the presence of axial magnetic field are investigated. The entropy, mean energy, and heat capacity of such a gas are determined, and its magnetic properties (magnetization and diamagnetic susceptibility) are studied. The possibilities of controlling thermodynamic parameters by changing the geometric parameters of quantum dots are shown. Calculations show that this gas has diamagnetic properties. These results provide insights into the features of physical processes occurring in thin core&amp;amp;ndash;shell quantum systems, which have potential applications in opto- and nanoelectronics.</description>
	<pubDate>2025-03-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 13: Thermodynamic and Magnetic Properties of Weakly Interacting Electron Gas Localized in a CdSe Cylindrical Core&amp;ndash;Shell Quantum Dot</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/1/13">doi: 10.3390/quantum7010013</a></p>
	<p>Authors:
		Levon Tadevosyan
		Hayk Ghaltaghchyan
		Yevgeni Mamasakhlisov
		Hayk Sarkisyan
		</p>
	<p>The thermodynamic and magnetic properties of weakly interacting electron gas localized in a CdSe cylindrical core&amp;amp;ndash;shell quantum dot in the presence of axial magnetic field are investigated. The entropy, mean energy, and heat capacity of such a gas are determined, and its magnetic properties (magnetization and diamagnetic susceptibility) are studied. The possibilities of controlling thermodynamic parameters by changing the geometric parameters of quantum dots are shown. Calculations show that this gas has diamagnetic properties. These results provide insights into the features of physical processes occurring in thin core&amp;amp;ndash;shell quantum systems, which have potential applications in opto- and nanoelectronics.</p>
	]]></content:encoded>

	<dc:title>Thermodynamic and Magnetic Properties of Weakly Interacting Electron Gas Localized in a CdSe Cylindrical Core&amp;amp;ndash;Shell Quantum Dot</dc:title>
			<dc:creator>Levon Tadevosyan</dc:creator>
			<dc:creator>Hayk Ghaltaghchyan</dc:creator>
			<dc:creator>Yevgeni Mamasakhlisov</dc:creator>
			<dc:creator>Hayk Sarkisyan</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7010013</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-03-17</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-03-17</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>13</prism:startingPage>
		<prism:doi>10.3390/quantum7010013</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/1/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/1/12">

	<title>Quantum Reports, Vol. 7, Pages 12: Practical Implementation of Unconditionally Secure File Transfer Application with QKD and OTP</title>
	<link>https://www.mdpi.com/2624-960X/7/1/12</link>
	<description>With the looming threat of quantum computers capable of breaking classical encryption and the uncertainty regarding the security of post-quantum encryption algorithms, some highly sensitive applications aim for the highest level of security in information transfer: unconditional security. In this work we present an architecture and a practical implementation of a user-friendly unconditionally secure file transfer client based on quantum key distribution and one time pad cipher. We test the implementation on the live QKD research infrastructure within POLITEHNICA Bucharest, thus proving the approach is feasible for real information transfer use-cases.</description>
	<pubDate>2025-03-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 12: Practical Implementation of Unconditionally Secure File Transfer Application with QKD and OTP</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/1/12">doi: 10.3390/quantum7010012</a></p>
	<p>Authors:
		Alin-Bogdan Popa
		Bogdan-Calin Ciobanu
		Pantelimon George Popescu
		</p>
	<p>With the looming threat of quantum computers capable of breaking classical encryption and the uncertainty regarding the security of post-quantum encryption algorithms, some highly sensitive applications aim for the highest level of security in information transfer: unconditional security. In this work we present an architecture and a practical implementation of a user-friendly unconditionally secure file transfer client based on quantum key distribution and one time pad cipher. We test the implementation on the live QKD research infrastructure within POLITEHNICA Bucharest, thus proving the approach is feasible for real information transfer use-cases.</p>
	]]></content:encoded>

	<dc:title>Practical Implementation of Unconditionally Secure File Transfer Application with QKD and OTP</dc:title>
			<dc:creator>Alin-Bogdan Popa</dc:creator>
			<dc:creator>Bogdan-Calin Ciobanu</dc:creator>
			<dc:creator>Pantelimon George Popescu</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7010012</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-03-14</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-03-14</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>12</prism:startingPage>
		<prism:doi>10.3390/quantum7010012</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/1/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2624-960X/7/1/11">

	<title>Quantum Reports, Vol. 7, Pages 11: Practitioners&amp;rsquo; Rule of Thumb for Quantum Volume</title>
	<link>https://www.mdpi.com/2624-960X/7/1/11</link>
	<description>Quantum volume (QV) is a widely recognized metric for assessing the practical capabilities of quantum computers, as it provides an estimate of the largest quantum circuit that can be reliably executed. However, measuring QV on a real device requires comparing experimental outcomes with ideal theoretical results&amp;amp;mdash;a process that rapidly becomes computationally expensive. By examining the cumulative impact of errors in two-qubit gates, we present a simple, accessible `rule of thumb&amp;amp;rsquo; that relates the quantum volume directly to the average error rate of native gates. Our formula shows a strong agreement with experimental data from leading quantum computing platforms, including both superconducting and trapped-ion systems. This straightforward model offers a clear, intuitive guideline for predicting quantum hardware performance, enabling more informed decisions regarding circuit design and resource allocation.</description>
	<pubDate>2025-02-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Quantum Reports, Vol. 7, Pages 11: Practitioners&amp;rsquo; Rule of Thumb for Quantum Volume</b></p>
	<p>Quantum Reports <a href="https://www.mdpi.com/2624-960X/7/1/11">doi: 10.3390/quantum7010011</a></p>
	<p>Authors:
		Emanuele G. Dalla Torre
		</p>
	<p>Quantum volume (QV) is a widely recognized metric for assessing the practical capabilities of quantum computers, as it provides an estimate of the largest quantum circuit that can be reliably executed. However, measuring QV on a real device requires comparing experimental outcomes with ideal theoretical results&amp;amp;mdash;a process that rapidly becomes computationally expensive. By examining the cumulative impact of errors in two-qubit gates, we present a simple, accessible `rule of thumb&amp;amp;rsquo; that relates the quantum volume directly to the average error rate of native gates. Our formula shows a strong agreement with experimental data from leading quantum computing platforms, including both superconducting and trapped-ion systems. This straightforward model offers a clear, intuitive guideline for predicting quantum hardware performance, enabling more informed decisions regarding circuit design and resource allocation.</p>
	]]></content:encoded>

	<dc:title>Practitioners&amp;amp;rsquo; Rule of Thumb for Quantum Volume</dc:title>
			<dc:creator>Emanuele G. Dalla Torre</dc:creator>
		<dc:identifier>doi: 10.3390/quantum7010011</dc:identifier>
	<dc:source>Quantum Reports</dc:source>
	<dc:date>2025-02-28</dc:date>

	<prism:publicationName>Quantum Reports</prism:publicationName>
	<prism:publicationDate>2025-02-28</prism:publicationDate>
	<prism:volume>7</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>11</prism:startingPage>
		<prism:doi>10.3390/quantum7010011</prism:doi>
	<prism:url>https://www.mdpi.com/2624-960X/7/1/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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