Bayesian analysis of the neutron star equation of state and model comparison: Insights from PSR <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi mathvariant="normal">J</mml:mi> <mml:mn>0437</mml:mn> <mml:m

We perform a comprehensive Bayesian analysis to constrain the neutron star (NS) equation of state (EoS) using a wide range of terrestrial and astrophysical data. The terrestrial inputs include quantities related to symmetric nuclear matter (SNM) and symmetry energy up to two times saturation density (${\ensuremath{\rho}}_{0}\ensuremath{\simeq}0.16\text{ }\text{ }{\mathrm{fm}}^{\ensuremath{-}3}$), derived from finite nuclei and heavy ion collisions (HIC). The astrophysical constraints incorporate NS radii and tidal deformabilities from recent Neutron Star Interior Composition Explorer (NICER) observations and GW170817, respectively. We consider five different EoS models: Taylor, $n/3$, Skyrme, relative mean field, and sound speed (CS), and analyze them by sequentially updating the priors with (i) chiral effective field theory ($\ensuremath{\chi}\mathrm{EFT}$)-based pure neutron matter, (ii) terrestrial, empirical, and earlier astrophysical data, (iii) case (ii) including NICER radii of PSR $\mathrm{J}0437+4715$ and $\mathrm{J}0614+3329$, (iv) all data combined, and (v) excluding empirical nuclear inputs. We also perform Bayesian model comparison, which favors the Skyrme model under all combined data [scenario (iv)], yielding tight constraints on symmetry energy parameters: ${L}_{0}=56\ifmmode\pm\else\textpm\fi{}3\text{ }\text{ }\mathrm{MeV}$ and ${K}_{\mathrm{sym}0}=\ensuremath{-}132\ifmmode\pm\else\textpm\fi{}15\text{ }\text{ }\mathrm{MeV}$, and also on SNM parameters: ${K}_{0}=265\ifmmode\pm\else\textpm\fi{}12\text{ }\text{ }\mathrm{MeV}$ and ${Q}_{0}=\ensuremath{-}366\ifmmode\pm\else\textpm\fi{}43\text{ }\text{ }\mathrm{MeV}$. The mass-radius and mass--tidal deformability posterior distributions are also well constrained. The radius and tidal deformability of a $1.4{M}_{\ensuremath{\bigodot}}$ neutron star are found to be ${R}_{1.4}=11.85\ifmmode\pm\else\textpm\fi{}0.11\text{ }\text{ }\mathrm{km}$ and ${\mathrm{\ensuremath{\Lambda}}}_{1.4}=354\ifmmode\pm\else\textpm\fi{}25$, respectively.

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Journal
Physical review. D/Physical review. D.
Published
2025-11-10
DOI
https://doi.org/10.1103/2fz9-xlv1
Primary Topic
Pulsars and Gravitational Waves Research
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article
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article

Bayesian analysis of the neutron star equation of state and model comparison: Insights from PSR <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi mathvariant="normal">J</mml:mi> <mml:mn>0437</mml:mn> <mml:m

Sk Md Adil Imam, N. K. Patra
Physical review. D/Physical review. D.
Pulsars and Gravitational Waves Research
article

Bayesian analysis of the neutron star equation of state and model comparison: Insights from PSR <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:mi mathvariant="normal">J</mml:mi> <mml:mn>0437</mml:mn> <mml:m

Sk Md Adil Imam, N. K. Patra
article en

Abstract

We perform a comprehensive Bayesian analysis to constrain the neutron star (NS) equation of state (EoS) using a wide range of terrestrial and astrophysical data. The terrestrial inputs include quantities related to symmetric nuclear matter (SNM) and symmetry energy up to two times saturation density (${\ensuremath{\rho}}_{0}\ensuremath{\simeq}0.16\text{ }\text{ }{\mathrm{fm}}^{\ensuremath{-}3}$), derived from finite nuclei and heavy ion collisions (HIC). The astrophysical constraints incorporate NS radii and tidal deformabilities from recent Neutron Star Interior Composition Explorer (NICER) observations and GW170817, respectively. We consider five different EoS models: Taylor, $n/3$, Skyrme, relative mean field, and sound speed (CS), and analyze them by sequentially updating the priors with (i) chiral effective field theory ($\ensuremath{\chi}\mathrm{EFT}$)-based pure neutron matter, (ii) terrestrial, empirical, and earlier astrophysical data, (iii) case (ii) including NICER radii of PSR $\mathrm{J}0437+4715$ and $\mathrm{J}0614+3329$, (iv) all data combined, and (v) excluding empirical nuclear inputs. We also perform Bayesian model comparison, which favors the Skyrme model under all combined data [scenario (iv)], yielding tight constraints on symmetry energy parameters: ${L}_{0}=56\ifmmode\pm\else\textpm\fi{}3\text{ }\text{ }\mathrm{MeV}$ and ${K}_{\mathrm{sym}0}=\ensuremath{-}132\ifmmode\pm\else\textpm\fi{}15\text{ }\text{ }\mathrm{MeV}$, and also on SNM parameters: ${K}_{0}=265\ifmmode\pm\else\textpm\fi{}12\text{ }\text{ }\mathrm{MeV}$ and ${Q}_{0}=\ensuremath{-}366\ifmmode\pm\else\textpm\fi{}43\text{ }\text{ }\mathrm{MeV}$. The mass-radius and mass--tidal deformability posterior distributions are also well constrained. The radius and tidal deformability of a $1.4{M}_{\ensuremath{\bigodot}}$ neutron star are found to be ${R}_{1.4}=11.85\ifmmode\pm\else\textpm\fi{}0.11\text{ }\text{ }\mathrm{km}$ and ${\mathrm{\ensuremath{\Lambda}}}_{1.4}=354\ifmmode\pm\else\textpm\fi{}25$, respectively.

Physical review. D/Physical review. D.Vol. 112(10)
Universidad Andrés Bello (CL), Chinese University of Hong Kong (HK), Chinese University of Hong Kong, Shenzhen (CN)
Openalex Percentile: Top 77%
Pulsars and Gravitational Waves Research
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