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		<title>Time and Space</title>
		<description>Latest open access articles published in Time Space at https://www.mdpi.com/journal/timespace</description>
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	<title>Time and Space, Vol. 2, Pages 4: Relativity with or Without Light and Maxwell</title>
	<link>https://www.mdpi.com/2813-9526/2/2/4</link>
	<description>The complex relationship between Einstein&amp;amp;rsquo;s second postulate and the Maxwell electromagnetic theory is elucidated. A simple deduction of the main results of the Ignatowski approach to the theory of relativity is given. The peculiar status of the principle of relativity among the Maxwellians is illustrated.</description>
	<pubDate>2026-04-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 2, Pages 4: Relativity with or Without Light and Maxwell</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/2/2/4">doi: 10.3390/timespace2020004</a></p>
	<p>Authors:
		Dragan V. Redžić
		</p>
	<p>The complex relationship between Einstein&amp;amp;rsquo;s second postulate and the Maxwell electromagnetic theory is elucidated. A simple deduction of the main results of the Ignatowski approach to the theory of relativity is given. The peculiar status of the principle of relativity among the Maxwellians is illustrated.</p>
	]]></content:encoded>

	<dc:title>Relativity with or Without Light and Maxwell</dc:title>
			<dc:creator>Dragan V. Redžić</dc:creator>
		<dc:identifier>doi: 10.3390/timespace2020004</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2026-04-08</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2026-04-08</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/timespace2020004</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/2/2/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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        <item rdf:about="https://www.mdpi.com/2813-9526/2/2/3">

	<title>Time and Space, Vol. 2, Pages 3: Space System Time-Error Buildup and the Allan Deviation</title>
	<link>https://www.mdpi.com/2813-9526/2/2/3</link>
	<description>Relating the standard deviation of time-error buildup, &amp;amp;sigma;t(T), at some time T after synchronization to a clock&amp;amp;rsquo;s Allan deviation, &amp;amp;sigma;y(T), is problematic for several reasons. Notably, the stochastic integrals of various relevant noise types do not exist in closed form, and the standard deviation does not necessarily converge for the noise types of relevance for atomic clocks and crystal oscillators. Consequently, as an expedient, one often writes &amp;amp;sigma;t(T) = k&amp;amp;sigma;y(T)T, where k is a constant that depends on the noise type under consideration, as well as the statistical question of interest. Here, we consider the question of Clock Family Time-Error (CFTE) buildup and compute k for noise processes of relevance to atomic timekeeping in space. One of the interesting results of the present work is the k-value that we obtain for flicker frequency noise, which shows a dependence on the time after synchronization.</description>
	<pubDate>2026-03-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 2, Pages 3: Space System Time-Error Buildup and the Allan Deviation</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/2/2/3">doi: 10.3390/timespace2020003</a></p>
	<p>Authors:
		James Camparo
		</p>
	<p>Relating the standard deviation of time-error buildup, &amp;amp;sigma;t(T), at some time T after synchronization to a clock&amp;amp;rsquo;s Allan deviation, &amp;amp;sigma;y(T), is problematic for several reasons. Notably, the stochastic integrals of various relevant noise types do not exist in closed form, and the standard deviation does not necessarily converge for the noise types of relevance for atomic clocks and crystal oscillators. Consequently, as an expedient, one often writes &amp;amp;sigma;t(T) = k&amp;amp;sigma;y(T)T, where k is a constant that depends on the noise type under consideration, as well as the statistical question of interest. Here, we consider the question of Clock Family Time-Error (CFTE) buildup and compute k for noise processes of relevance to atomic timekeeping in space. One of the interesting results of the present work is the k-value that we obtain for flicker frequency noise, which shows a dependence on the time after synchronization.</p>
	]]></content:encoded>

	<dc:title>Space System Time-Error Buildup and the Allan Deviation</dc:title>
			<dc:creator>James Camparo</dc:creator>
		<dc:identifier>doi: 10.3390/timespace2020003</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2026-03-25</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2026-03-25</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/timespace2020003</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/2/2/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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        <item rdf:about="https://www.mdpi.com/2813-9526/2/1/2">

	<title>Time and Space, Vol. 2, Pages 2: Quantum-Spacetime Perspective on the KM3-230213A Neutrino</title>
	<link>https://www.mdpi.com/2813-9526/2/1/2</link>
	<description>The announcement of the KM3-230213A neutrino is generating a flood of astrophysics studies, mostly investigating its origin. We here focus on aspects of this observation that could be relevant for research programs on quantum gravity and spacetime quantization. It is at least amusing that KM3-230213A most likely traveled billions of light-years, but its rest-frame existence only lasted less than 0.1 seconds and ended with it being hit by a nucleon of Planckian energy. In addition, and perhaps more significantly, KM3-230213A is a remarkable probe of the types of microscopic structure of spacetime conjectured in some quantum-spacetime scenarios, and according to one of these scenarios, there is a candidate source: the gamma-ray burst GRB090401B observed 14 years earlier.</description>
	<pubDate>2026-02-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 2, Pages 2: Quantum-Spacetime Perspective on the KM3-230213A Neutrino</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/2/1/2">doi: 10.3390/timespace2010002</a></p>
	<p>Authors:
		Giovanni Amelino-Camelia
		Giacomo D’Amico
		Giuseppe Fabiano
		Domenico Frattulillo
		Giulia Gubitosi
		Alessandro Moia
		Giacomo Rosati
		</p>
	<p>The announcement of the KM3-230213A neutrino is generating a flood of astrophysics studies, mostly investigating its origin. We here focus on aspects of this observation that could be relevant for research programs on quantum gravity and spacetime quantization. It is at least amusing that KM3-230213A most likely traveled billions of light-years, but its rest-frame existence only lasted less than 0.1 seconds and ended with it being hit by a nucleon of Planckian energy. In addition, and perhaps more significantly, KM3-230213A is a remarkable probe of the types of microscopic structure of spacetime conjectured in some quantum-spacetime scenarios, and according to one of these scenarios, there is a candidate source: the gamma-ray burst GRB090401B observed 14 years earlier.</p>
	]]></content:encoded>

	<dc:title>Quantum-Spacetime Perspective on the KM3-230213A Neutrino</dc:title>
			<dc:creator>Giovanni Amelino-Camelia</dc:creator>
			<dc:creator>Giacomo D’Amico</dc:creator>
			<dc:creator>Giuseppe Fabiano</dc:creator>
			<dc:creator>Domenico Frattulillo</dc:creator>
			<dc:creator>Giulia Gubitosi</dc:creator>
			<dc:creator>Alessandro Moia</dc:creator>
			<dc:creator>Giacomo Rosati</dc:creator>
		<dc:identifier>doi: 10.3390/timespace2010002</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2026-02-24</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2026-02-24</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/timespace2010002</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/2/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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        <item rdf:about="https://www.mdpi.com/2813-9526/2/1/1">

	<title>Time and Space, Vol. 2, Pages 1: Clock Synchronization with Kuramoto Oscillators for Space Systems</title>
	<link>https://www.mdpi.com/2813-9526/2/1/1</link>
	<description>As space systems evolve towards cis-lunar missions and beyond, the demand for precise yet low-size, -weight, and -power (SWaP) clocks and synchronization methods becomes increasingly critical. We introduce a novel clock synchronization approach based on the Kuramoto oscillator model that facilitates the creation of an ensemble timescale for satellite constellations. Unlike traditional ensembling algorithms, the proposed Kuramoto method leverages nearest-neighbor interactions to achieve collective synchronization. This method simplifies the communication architecture and data-sharing requirements, making it well suited for dynamically connected networks such as proliferated low Earth orbit (pLEO) and lunar or Martian constellations, where intersatellite links may frequently change. Through simulations incorporating realistic noise models for small-scale atomic clocks, we demonstrate that the Kuramoto ensemble can yield an improvement in stability on the order of 1/&amp;amp;radic;N, while mitigating the impact of constellation fragmentation and defragmentation. The results indicate that the Kuramoto oscillator-based algorithm can potentially deliver performance comparable to established techniques like Equal Weights Frequency Averaging (EWFA), yet with enhanced scalability and resource efficiency critical for future spaceborne PNT and communication systems.</description>
	<pubDate>2026-01-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 2, Pages 1: Clock Synchronization with Kuramoto Oscillators for Space Systems</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/2/1/1">doi: 10.3390/timespace2010001</a></p>
	<p>Authors:
		Nathaniel Ristoff
		Hunter Kettering
		James Camparo
		</p>
	<p>As space systems evolve towards cis-lunar missions and beyond, the demand for precise yet low-size, -weight, and -power (SWaP) clocks and synchronization methods becomes increasingly critical. We introduce a novel clock synchronization approach based on the Kuramoto oscillator model that facilitates the creation of an ensemble timescale for satellite constellations. Unlike traditional ensembling algorithms, the proposed Kuramoto method leverages nearest-neighbor interactions to achieve collective synchronization. This method simplifies the communication architecture and data-sharing requirements, making it well suited for dynamically connected networks such as proliferated low Earth orbit (pLEO) and lunar or Martian constellations, where intersatellite links may frequently change. Through simulations incorporating realistic noise models for small-scale atomic clocks, we demonstrate that the Kuramoto ensemble can yield an improvement in stability on the order of 1/&amp;amp;radic;N, while mitigating the impact of constellation fragmentation and defragmentation. The results indicate that the Kuramoto oscillator-based algorithm can potentially deliver performance comparable to established techniques like Equal Weights Frequency Averaging (EWFA), yet with enhanced scalability and resource efficiency critical for future spaceborne PNT and communication systems.</p>
	]]></content:encoded>

	<dc:title>Clock Synchronization with Kuramoto Oscillators for Space Systems</dc:title>
			<dc:creator>Nathaniel Ristoff</dc:creator>
			<dc:creator>Hunter Kettering</dc:creator>
			<dc:creator>James Camparo</dc:creator>
		<dc:identifier>doi: 10.3390/timespace2010001</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2026-01-15</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2026-01-15</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/timespace2010001</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/2/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2813-9526/1/1/5">

	<title>Time and Space, Vol. 1, Pages 5: Model of Space-Time as an Elastic Medium: State of the Art and Perspectives on the Knowledge of Time</title>
	<link>https://www.mdpi.com/2813-9526/1/1/5</link>
	<description>This paper presents a theoretical framework modeling space-time as a quantized elastic medium. This elastic model is not intended to replace general relativity, but to offer a complementary mechanical interpretation in the approximation of the weak gravitational field. The goal is not to redefine gravity, but to explore whether this elastic formalism can simplify certain aspects of space-time dynamics, provide new insights, and generate falsifiable predictions&amp;amp;mdash;particularly in contexts where analytical solutions in general relativity are difficult to obtain. As originally envisaged by A. Sakharov, who associated general relativity with the concept of space-time behaving like an elastic medium, this paper introduces the notion of the &amp;amp;ldquo;elasther&amp;amp;rdquo; and reinterprets gravitational effects, time dilation, and phenomena commonly attributed to dark energy and dark matter through analogies with established mechanical principles such as Hooke&amp;amp;rsquo;s law, thermal expansion, and creep.</description>
	<pubDate>2025-12-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 1, Pages 5: Model of Space-Time as an Elastic Medium: State of the Art and Perspectives on the Knowledge of Time</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/1/1/5">doi: 10.3390/timespace1010005</a></p>
	<p>Authors:
		David Izabel
		</p>
	<p>This paper presents a theoretical framework modeling space-time as a quantized elastic medium. This elastic model is not intended to replace general relativity, but to offer a complementary mechanical interpretation in the approximation of the weak gravitational field. The goal is not to redefine gravity, but to explore whether this elastic formalism can simplify certain aspects of space-time dynamics, provide new insights, and generate falsifiable predictions&amp;amp;mdash;particularly in contexts where analytical solutions in general relativity are difficult to obtain. As originally envisaged by A. Sakharov, who associated general relativity with the concept of space-time behaving like an elastic medium, this paper introduces the notion of the &amp;amp;ldquo;elasther&amp;amp;rdquo; and reinterprets gravitational effects, time dilation, and phenomena commonly attributed to dark energy and dark matter through analogies with established mechanical principles such as Hooke&amp;amp;rsquo;s law, thermal expansion, and creep.</p>
	]]></content:encoded>

	<dc:title>Model of Space-Time as an Elastic Medium: State of the Art and Perspectives on the Knowledge of Time</dc:title>
			<dc:creator>David Izabel</dc:creator>
		<dc:identifier>doi: 10.3390/timespace1010005</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2025-12-18</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2025-12-18</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>5</prism:startingPage>
		<prism:doi>10.3390/timespace1010005</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/1/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2813-9526/1/1/4">

	<title>Time and Space, Vol. 1, Pages 4: Optical Measurements of Binary Buffer-Gas Partial Pressures for Vapor-Cell Atomic Clocks</title>
	<link>https://www.mdpi.com/2813-9526/1/1/4</link>
	<description>In vapor-cell atomic clocks, a buffer gas is employed to slow the collision rate of atoms with the vapor-cell&amp;amp;rsquo;s walls, which dephases the atomic coherence and thereby contributes to the 0-0 hyperfine transition&amp;amp;rsquo;s linewidth. However, the buffer gas also gives rise to a temperature-dependent pressure shift in the hyperfine transition, &amp;amp;Delta;&amp;amp;nu;hfs. As a consequence, the clock&amp;amp;rsquo;s frequency develops a temperature dependence, manifesting as a clock environmental sensitivity, which can degrade the clock&amp;amp;rsquo;s long-term frequency stability. To mitigate this problem, it is routine to employ a buffer-gas mixture in a vapor cell. With an appropriate choice of buffer gases, d[&amp;amp;Delta;&amp;amp;nu;hfs]/dT = 0 at a vapor temperature Tc, &amp;amp;ldquo;zeroing out&amp;amp;rdquo; the clock&amp;amp;rsquo;s buffer-gas temperature sensitivity. Unfortunately, Tc depends on the exact mix of buffer-gas partial pressures, and if not properly achieved, Tc will be far from the vapor temperature that yields useful atomic clock signals, To. Therefore, understanding buffer-gas partial pressures in sealed vapor cells is crucial for optimizing a vapor cell clock&amp;amp;rsquo;s performance, yet, to date, there have been no easy means for measuring buffer-gas partial pressures non-destructively in sealed glass vapor cells. Here, we demonstrate an optical technique that can accurately assess partial pressures in binary buffer-gas mixtures. Moreover, this technique is relatively simple and can be easily implemented.</description>
	<pubDate>2025-10-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 1, Pages 4: Optical Measurements of Binary Buffer-Gas Partial Pressures for Vapor-Cell Atomic Clocks</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/1/1/4">doi: 10.3390/timespace1010004</a></p>
	<p>Authors:
		Andrew Householder
		James Camparo
		</p>
	<p>In vapor-cell atomic clocks, a buffer gas is employed to slow the collision rate of atoms with the vapor-cell&amp;amp;rsquo;s walls, which dephases the atomic coherence and thereby contributes to the 0-0 hyperfine transition&amp;amp;rsquo;s linewidth. However, the buffer gas also gives rise to a temperature-dependent pressure shift in the hyperfine transition, &amp;amp;Delta;&amp;amp;nu;hfs. As a consequence, the clock&amp;amp;rsquo;s frequency develops a temperature dependence, manifesting as a clock environmental sensitivity, which can degrade the clock&amp;amp;rsquo;s long-term frequency stability. To mitigate this problem, it is routine to employ a buffer-gas mixture in a vapor cell. With an appropriate choice of buffer gases, d[&amp;amp;Delta;&amp;amp;nu;hfs]/dT = 0 at a vapor temperature Tc, &amp;amp;ldquo;zeroing out&amp;amp;rdquo; the clock&amp;amp;rsquo;s buffer-gas temperature sensitivity. Unfortunately, Tc depends on the exact mix of buffer-gas partial pressures, and if not properly achieved, Tc will be far from the vapor temperature that yields useful atomic clock signals, To. Therefore, understanding buffer-gas partial pressures in sealed vapor cells is crucial for optimizing a vapor cell clock&amp;amp;rsquo;s performance, yet, to date, there have been no easy means for measuring buffer-gas partial pressures non-destructively in sealed glass vapor cells. Here, we demonstrate an optical technique that can accurately assess partial pressures in binary buffer-gas mixtures. Moreover, this technique is relatively simple and can be easily implemented.</p>
	]]></content:encoded>

	<dc:title>Optical Measurements of Binary Buffer-Gas Partial Pressures for Vapor-Cell Atomic Clocks</dc:title>
			<dc:creator>Andrew Householder</dc:creator>
			<dc:creator>James Camparo</dc:creator>
		<dc:identifier>doi: 10.3390/timespace1010004</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2025-10-24</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2025-10-24</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/timespace1010004</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/1/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2813-9526/1/1/3">

	<title>Time and Space, Vol. 1, Pages 3: Time Domain Statistics for Evaluating Residual Noise, Including Instabilities in Time/Frequency Transfer Systems</title>
	<link>https://www.mdpi.com/2813-9526/1/1/3</link>
	<description>The instabilities in time and frequency transfer systems, a form of residual noise, can contribute significantly to the total uncertainty in time or frequency comparisons. Understanding the characteristics of transfer instabilities is increasingly important with the new high-stability optical frequency standards being developed. First-difference statistics such as the rms Time Interval Error (TIErms), the Frequency Transfer Uncertainty (FTU), and ADEVS (a novel use of the Allan deviation equation) provide a more direct and accurate measure of residual noise than second-difference statistics such as the Allan Deviation (ADEV), the Modified Allan Deviation (MDEV), and the Time Deviation (TDEV). A unifying discussion on the use of existing first-difference statistics with residual noise, introduced individually in two previous publications, is presented here. Simulated noise data is then analyzed to illustrate the differences in the various statistics. Their strengths and weaknesses are discussed. The impact of pre-averaging phase (time) data is also shown.</description>
	<pubDate>2025-06-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 1, Pages 3: Time Domain Statistics for Evaluating Residual Noise, Including Instabilities in Time/Frequency Transfer Systems</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/1/1/3">doi: 10.3390/timespace1010003</a></p>
	<p>Authors:
		Thomas Parker
		</p>
	<p>The instabilities in time and frequency transfer systems, a form of residual noise, can contribute significantly to the total uncertainty in time or frequency comparisons. Understanding the characteristics of transfer instabilities is increasingly important with the new high-stability optical frequency standards being developed. First-difference statistics such as the rms Time Interval Error (TIErms), the Frequency Transfer Uncertainty (FTU), and ADEVS (a novel use of the Allan deviation equation) provide a more direct and accurate measure of residual noise than second-difference statistics such as the Allan Deviation (ADEV), the Modified Allan Deviation (MDEV), and the Time Deviation (TDEV). A unifying discussion on the use of existing first-difference statistics with residual noise, introduced individually in two previous publications, is presented here. Simulated noise data is then analyzed to illustrate the differences in the various statistics. Their strengths and weaknesses are discussed. The impact of pre-averaging phase (time) data is also shown.</p>
	]]></content:encoded>

	<dc:title>Time Domain Statistics for Evaluating Residual Noise, Including Instabilities in Time/Frequency Transfer Systems</dc:title>
			<dc:creator>Thomas Parker</dc:creator>
		<dc:identifier>doi: 10.3390/timespace1010003</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2025-06-08</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2025-06-08</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/timespace1010003</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/1/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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	<title>Time and Space, Vol. 1, Pages 2: When the Anomalistic, Draconitic and Sidereal Orbital Periods Do Not Coincide: The Impact of Post-Keplerian Perturbing Accelerations</title>
	<link>https://www.mdpi.com/2813-9526/1/1/2</link>
	<description>In a purely Keplerian picture, the anomalistic, draconitic and sidereal orbital periods of a test particle orbiting a massive body coincide with each other. Such degeneracy is removed when post-Keplerian perturbing acceleration enters the equations of motion, yielding generally different corrections to the Keplerian period for the three aforementioned characteristic orbital timescales. They are analytically worked out in the case of the accelerations induced by the general relativistic post-Newtonian gravitoelectromagnetic fields and, to the Newtonian level, by the oblateness of the central body. The resulting expressions hold for completely general orbital configurations and spatial orientations of the spin axis of the primary. Astronomical systems characterized by extremely accurate measurements of orbital periods like transiting exoplanets and binary pulsars may offer potentially viable scenarios for measuring such post-Keplerian features of motion, at least in principle. As an example, the sidereal period of the brown dwarf WD1032 + 011 b is currently known with an uncertainty as small as ≃10−5s, while its predicted post-Newtonian gravitoelectric correction amounts to 0.07s; however, the accuracy with which the Keplerian period can be calculated is just 572 s. For double pulsar PSR J0737–3039, the largest relativistic correction to the anomalistic period amounts to a few tenths of a second, given a measurement error of such a characteristic orbital timescale as small as ≃10−6s. On the other hand, the Keplerian term can be currently calculated just to a ≃9 s accuracy. In principle, measuring at least two of the three characteristic orbital periods for the same system independently would cancel out their common Keplerian component, provided that their difference is taken into account.</description>
	<pubDate>2024-07-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 1, Pages 2: When the Anomalistic, Draconitic and Sidereal Orbital Periods Do Not Coincide: The Impact of Post-Keplerian Perturbing Accelerations</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/1/1/2">doi: 10.3390/timespace1010002</a></p>
	<p>Authors:
		Lorenzo Iorio
		</p>
	<p>In a purely Keplerian picture, the anomalistic, draconitic and sidereal orbital periods of a test particle orbiting a massive body coincide with each other. Such degeneracy is removed when post-Keplerian perturbing acceleration enters the equations of motion, yielding generally different corrections to the Keplerian period for the three aforementioned characteristic orbital timescales. They are analytically worked out in the case of the accelerations induced by the general relativistic post-Newtonian gravitoelectromagnetic fields and, to the Newtonian level, by the oblateness of the central body. The resulting expressions hold for completely general orbital configurations and spatial orientations of the spin axis of the primary. Astronomical systems characterized by extremely accurate measurements of orbital periods like transiting exoplanets and binary pulsars may offer potentially viable scenarios for measuring such post-Keplerian features of motion, at least in principle. As an example, the sidereal period of the brown dwarf WD1032 + 011 b is currently known with an uncertainty as small as ≃10−5s, while its predicted post-Newtonian gravitoelectric correction amounts to 0.07s; however, the accuracy with which the Keplerian period can be calculated is just 572 s. For double pulsar PSR J0737–3039, the largest relativistic correction to the anomalistic period amounts to a few tenths of a second, given a measurement error of such a characteristic orbital timescale as small as ≃10−6s. On the other hand, the Keplerian term can be currently calculated just to a ≃9 s accuracy. In principle, measuring at least two of the three characteristic orbital periods for the same system independently would cancel out their common Keplerian component, provided that their difference is taken into account.</p>
	]]></content:encoded>

	<dc:title>When the Anomalistic, Draconitic and Sidereal Orbital Periods Do Not Coincide: The Impact of Post-Keplerian Perturbing Accelerations</dc:title>
			<dc:creator>Lorenzo Iorio</dc:creator>
		<dc:identifier>doi: 10.3390/timespace1010002</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2024-07-05</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2024-07-05</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/timespace1010002</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/1/1/2</prism:url>
	
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	<title>Time and Space, Vol. 1, Pages 1: Introducing Time and Space</title>
	<link>https://www.mdpi.com/2813-9526/1/1/1</link>
	<description>Time is an essential element in today’s world, spreading over multiple applications that range from societal activities up to those requiring the highest precision for scientific purposes [...]</description>
	<pubDate>2024-04-25</pubDate>

	<content:encoded><![CDATA[
	<p><b>Time and Space, Vol. 1, Pages 1: Introducing Time and Space</b></p>
	<p>Time and Space <a href="https://www.mdpi.com/2813-9526/1/1/1">doi: 10.3390/timespace1010001</a></p>
	<p>Authors:
		Elisa Arias
		</p>
	<p>Time is an essential element in today’s world, spreading over multiple applications that range from societal activities up to those requiring the highest precision for scientific purposes [...]</p>
	]]></content:encoded>

	<dc:title>Introducing Time and Space</dc:title>
			<dc:creator>Elisa Arias</dc:creator>
		<dc:identifier>doi: 10.3390/timespace1010001</dc:identifier>
	<dc:source>Time and Space</dc:source>
	<dc:date>2024-04-25</dc:date>

	<prism:publicationName>Time and Space</prism:publicationName>
	<prism:publicationDate>2024-04-25</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Editorial</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/timespace1010001</prism:doi>
	<prism:url>https://www.mdpi.com/2813-9526/1/1/1</prism:url>
	
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