4.7 Article

Generalized Tolman-Oppenheimer-Volkoff model and neutron stars

Journal

PHYSICAL REVIEW D
Volume 106, Issue 8, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.106.084042

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This study aims to reproduce the relevant equations of the GTOV model using a modified anisotropic energy-momentum tensor, calculate the moment of inertia and tidal deformability of neutron stars, investigate the impact of each free parameter of the GTOV model on neutron star properties, explore the correlations among parameters, and examine the physical ranges of the parameters. The study reveals that the values of GTOV free parameters can be constrained to acceptable ranges, with the θ parameter playing a crucial role in controlling the maximum mass value of neutron stars.
This work is motivated by the existence of mapping the extended theory of gravity with a standard energy-momentum tensor to general relativity with a modified energy-momentum tensor. We construct a modified anisotropic energy-momentum tensor from a standard isotropic energy-momentum tensor by adding a geometrical correction to precisely reproduce the Tolman-Oppenheimer-Volkoff equations predicted by the generalized Tolman-Oppenheimer-Volkoff (GTOV) model. This construction aims to calculate the moment of inertia (I) and tidal deformability (A) of neutron stars (NSs) within the GTOV model. Therefore, we can comprehensively investigate the role of each free parameter of the GTOV model in NS properties. Furthermore, through this construction we can also utilize physically acceptable stability conditions for anisotropic stars to constrain the physical range of each parameter value and investigate the existence of a correlation among the parameters of the GTOV model. Except for a, we find that the values of the GTOV free parameters can be limited to acceptable ranges. We also find that the parameters 0, x, and /3 are correlated, and the parameter r -> 0. With these free parameter ranges in hand, we study the role of each parameter of the GTOV model in NS properties, including I and A. We also revisit the hyperon puzzle in NSs within the GTOV model. We find that the 0 parameter plays a crucial role in controlling the NS maximum mass value. We also find that the threshold k2 peak for NS is k2 0.167. Furthermore, if we use parameter sets with 0 1/4 -1, the mass-radius predictions are compatible with recent NICER data on PSR J0030 + 0451 and PSR J0740 + 6620.

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