2023ApJ...950..129N


Query : 2023ApJ...950..129N

2023ApJ...950..129N - Astrophys. J., 950, 129 (2023/June-3)

The Effect of f(R, T) Modified Gravity on the Mass and Radius of Pulsar HerX1.

NASHED G.G.L.

Abstract (from CDS):

Millisecond pulsars are the perfect testable to examine potential matter-geometry coupling and its physical consequences in the context of the recent Neutron Star Interior Composition Explorer discoveries. We apply the field equations of modified gravity, f(R, T) = R + αT, to a spherically symmetric spacetime, where R is the Ricci scalar, α is a dimensional parameter, and T is the matter of the geometry. Five unknown functions are present in the output system of differential equations, which consists of three equations. To close the system, we make explicit assumptions about the anisotropy and the radial metric potential, grr. We then solve the output differential equations and derive the explicit forms of the components of the energy-momentum tensor, i.e., density, radial, and tangential pressures. We look into the possibility that all of the physical parameters in the star can be reexpressed in terms of α and the compactness parameters, C = 2 GM Rc–2. We show that, for a given mass, the size permitted by Einstein's general relativity is less due to the matter-geometry coupling in f(R, T). The validity of the hypothesis was validated by observations from an extra 21 pulsars. To achieve a surface density that is compatible with a neutron core at nuclear saturation density, the mass-radius curve enables masses up to 3.35M⊙. We emphasize that although there is no assumption of an equation of state, the model fits well with a linear behavior. When comparing the surface densities of these 20 pulsars, we divided them into three groups. We show that these three groups are compatible with neutron cores.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Star formation - Gravitation

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 CXOGlb J002403.4-720451 LXB 00 24 03.494 -72 04 51.94           ~ 62 1
2 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
3 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
4 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
5 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
6 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0 14.290   O8III 714 0
7 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
8 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
9 PSR J0952-0607 Psr 09 52 08.319 -06 07 23.49           ~ 103 0
10 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1159 0
11 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
12 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
13 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
14 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2291 0
15 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
16 4U 1722-30 LXB 17 27 33.25 -30 48 07.4     12.50     ~ 278 1
17 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
18 KS 1731-260 LXB 17 34 13.46 -26 05 18.6       22.8 20.9 ~ 437 0
19 NAME TER 5 X-1 LXB 17 48 05.225 -24 46 47.66           ~ 229 1
20 [PLV2002] CX1 LXB 17 48 52.163 -20 21 32.40           ~ 213 1
21 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
22 RX J1856.6-3754 Psr 18 56 35.11 -37 54 30.5     25.7     ~ 456 0
23 PSR J2215+51 Psr 22 15 32.6869149432 +51 35 36.400854912           ~ 176 0
24 GRB 190425 GWE ~ ~           ~ 438 0

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