2023ApJS..269...35M


Query : 2023ApJS..269...35M

2023ApJS..269...35M - Astrophys. J., Suppl. Ser., 269, 35 (2023/December-0)

The Effect of Gravitational Decoupling on Constraining the Mass and Radius for the Secondary Component of GW190814 and Other Self-bound Strange Stars in f(Q) Gravity Theory.

MAURYA S.K., SINGH K.N., GOVENDER M., MUSTAFA G. and RAY S.

Abstract (from CDS):

Inspired by the conundrum of the gravitational event GW190814, which brings to light the coalescence of a 23 M⊙ black hole with a yet-to-be-determined secondary component, we look to modeling compact objects within the framework of $f({ \mathcal Q })$ gravity by employing the method of gravitational decoupling. We impose a quadratic equation of state (EOS) for the interior matter distribution, which in the appropriate limit reduces to the MIT bag model. The governing field equations arising from gravitational decoupling bifurcate into the $\rho ={\theta }_{0}^{0}$ and ${p}_{r}={\theta }_{1}^{1}$ sectors, leading to two distinct classes of solutions. Both families of solutions are subjected to rigorous tests, qualifying them to describe a plethora of compact objects, including neutron stars, strange stars, and the possible progenitor of the secondary component of GW190814. Using observational data of mass-radius relations for compact objects LMC X-4, Cen X-3, PSR J1614-2230, and PSR J0740+6620, we show that it is possible to generate stellar masses and radii beyond 2.0 M⊙ for neutron stars. Our findings reveal that the most suitable and versatile model in this framework is the quadratic EOS, which accounts for a range of low-mass stars and typical stellar candidates describing the secondary component of GW190814.

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

Journal keyword(s): Compact objects - Neutron stars - Theoretical models

Simbad objects: 9

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Number of rows : 9
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 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
2 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0 14.290   O8III 714 0
3 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
4 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1159 0
5 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
6 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
7 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
8 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
9 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1

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