Stability of compact stars in a uniform density background cloud

被引:0
|
作者
Singh, Ksh. Newton [1 ]
Maurya, S. K. [2 ,3 ]
Errehymy, A. [4 ]
Donmez, O. [5 ]
Myrzakulov, K. [6 ]
Smitha, T. T. [2 ]
机构
[1] Natl Def Acad, Dept Phys, Pune 411023, India
[2] Univ Nizwa, Coll Arts & Sci, Dept Math & Phys Sci, Nizwa 616, Oman
[3] Khazar Univ, Res Ctr Astrophys & Cosmol, 41 Mehseti St, Baku AZ1096, Azerbaijan
[4] Univ KwaZulu Natal, Astrophys Res Ctr, Sch Math Stat & Comp Sci, Private Bag X54001, ZA-4000 Durban, South Africa
[5] Amer Univ Middle East, Coll Engn & Technol, Egaila 54200, Kuwait
[6] LN Gumilyov Eurasian Natl Univ, Dept Gen & Theoret Phys, Astana 010008, Kazakhstan
来源
EUROPEAN PHYSICAL JOURNAL C | 2024年 / 84卷 / 12期
基金
新加坡国家研究基金会;
关键词
EQUATION-OF-STATE; NEUTRON-STAR; ANISOTROPIC SOLUTIONS; GENERAL-RELATIVITY; STRANGE STARS; F R; MATTER; GRAVITY; MASS; RADIUS;
D O I
10.1140/epjc/s10052-024-13661-1
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We are discussing a scenario where a compact star (neutron star, NS) is embedded in a thin, uniform density background cloud (a remnant cloud after a supernova or a cloud generated from the late stages of a star e.g., a planetary nebula or asymptotic red giant phases) and its effect on the stability of the compact star. Due to the thin background cloud, the spacetime geometry is minimally deformed allowing us to employ the technique of minimal geometric decoupling (MGD). Assuming a uniform background cloud density simplifies the problem, and through the MGD method, one can take Theta(t)(t)=Theta>0, where Theta is the density of the cloud. The background cloud interacts with the compact star through a coupling strength alpha. By varying alpha, one can tune the cloud density to analyze the stability of the embedded compact star. We found that for alpha<3x10(-5), all the thermodynamic quantities are well-behaved, indicating a stable configuration. Once the coupling parameter exceeds 3x10(-5), the adiabatic index drops below Gamma(max)', triggering a gravitational collapse. Beyond this limit of alpha, the pressure and speed of sound also become non-physical. At the end, we have used the M-R curve generated from the solution to determine the radii of a few compact stars, namely PSR J1614-2230, PSR J0952-0607, GW190814, and GW200210. Furthermore, we have discussed the possibility of the secondary component of GW200210 i.e. the less massive compact object with an upper mass of 3.3M(circle dot), which may be a stellar black hole with a Schwarzschild radius R-BH=9.746 km. However, if the mass is 2.83M(circle dot) as observed, then its predicted minimum radius is 10.74 km, corresponding to alpha=0. This radius is far beyond R-BH=8.357 km and therefore is most probably a massive NS in the mass gap.
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页数:9
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