Upper Limit of Sound Speed in Nuclear Matter: A Harmonious Interplay of Transport Calculation and Perturbative Quantum Chromodynamic Constraint

Abstract Very recently, it has been shown that there is an upper bound on the squared sound speed of nuclear matter from the transport, which reads <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> . In this work, we demonstrate that this upper bound is corroborated by the reconstructed equation of state (EOS; modeled with a nonparametric method) for ultradense matter. The reconstruction integrates multimessenger observation for neutron stars, in particular, the latest radius measurements for PSR J0437–4715 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.36</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.63</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.95</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km), PSR J0030+0451 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.71</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.83</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, in the ST+PDT model), and PSR J0740+6620 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>12.49</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>1.28</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km) by NICER have been adopted. The result shows in all cases, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> upper limit for EOS will naturally yield the properties of matter near the center of the massive neutron star consistent with the causality-driven constraint from pQCD, where, in practice, the density in implementing the pQCD likelihood ( n L ) is applied at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mn>10</mml:mn> <mml:msub> <mml:mi>n</mml:mi> <mml:mi>s</mml:mi> </mml:msub> </mml:math> (where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mi>n</mml:mi> <mml:mi>s</mml:mi> </mml:msub> </mml:math> is the nuclear saturation density). We also note that there is a strong correlation for the maximum c s 2 with n L , and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> is somehow violated when n L = n c,TOV . The result indicates that a higher n L , even considering the uncertainties from statistics, is more natural. Moreover, the remarkable agreement between the outcomes derived from these two distinct and independent constraints (i.e., the transport calculation and pQCD boundary) lends strong support to their validity. In addition, the latest joint constraint for R 1.4 , R 2.0 , R 1.4 − R 2.0 , and M TOV are <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.94</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.68</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.77</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.99</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.67</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>−</mml:mo> <mml:msubsup> <mml:mrow> <mml:mn>0.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.27</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.42</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="

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Publication Details

Journal
The Astrophysical Journal
Published
2024-10-01
DOI
https://doi.org/10.3847/1538-4357/ad7503
Citations
6
Primary Topic
Pulsars and Gravitational Waves Research
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article
Field-Weighted Citation Impact
1.99

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article

Upper Limit of Sound Speed in Nuclear Matter: A Harmonious Interplay of Transport Calculation and Perturbative Quantum Chromodynamic Constraint

Yi-Zhong Fan, Yong-Jia Huang, Shao-Peng Tang, Ming-Zhe Han
6 citations
The Astrophysical Journal
Pulsars and Gravitational Waves Research
1.99
article

Upper Limit of Sound Speed in Nuclear Matter: A Harmonious Interplay of Transport Calculation and Perturbative Quantum Chromodynamic Constraint

Yi-Zhong Fan, Yong-Jia Huang, Shao-Peng Tang, Ming-Zhe Han
article en
6 citations

Abstract

Abstract Very recently, it has been shown that there is an upper bound on the squared sound speed of nuclear matter from the transport, which reads <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> . In this work, we demonstrate that this upper bound is corroborated by the reconstructed equation of state (EOS; modeled with a nonparametric method) for ultradense matter. The reconstruction integrates multimessenger observation for neutron stars, in particular, the latest radius measurements for PSR J0437–4715 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.36</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.63</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.95</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km), PSR J0030+0451 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.71</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.83</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, in the ST+PDT model), and PSR J0740+6620 ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>12.49</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>1.28</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km) by NICER have been adopted. The result shows in all cases, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> upper limit for EOS will naturally yield the properties of matter near the center of the massive neutron star consistent with the causality-driven constraint from pQCD, where, in practice, the density in implementing the pQCD likelihood ( n L ) is applied at <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mn>10</mml:mn> <mml:msub> <mml:mi>n</mml:mi> <mml:mi>s</mml:mi> </mml:msub> </mml:math> (where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msub> <mml:mi>n</mml:mi> <mml:mi>s</mml:mi> </mml:msub> </mml:math> is the nuclear saturation density). We also note that there is a strong correlation for the maximum c s 2 with n L , and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>≤</mml:mo> <mml:mn>0.781</mml:mn> </mml:math> is somehow violated when n L = n c,TOV . The result indicates that a higher n L , even considering the uncertainties from statistics, is more natural. Moreover, the remarkable agreement between the outcomes derived from these two distinct and independent constraints (i.e., the transport calculation and pQCD boundary) lends strong support to their validity. In addition, the latest joint constraint for R 1.4 , R 2.0 , R 1.4 − R 2.0 , and M TOV are <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.94</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.68</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.77</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>11.99</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.67</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.88</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mo>−</mml:mo> <mml:msubsup> <mml:mrow> <mml:mn>0.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.27</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.42</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km, and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="

The Astrophysical JournalVol. 974(2)
National Natural Science Foundation of China, Chinese Academy of Sciences, China Postdoctoral Science Foundation
Openalex Percentile: Top 14%
Pulsars and Gravitational Waves Research
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