Testing generalized spacetimes for black holes using the Hod function representation of the hoop conjecture

被引:1
|
作者
Nandi, K. K. [1 ,2 ]
Izmailov, R. N. [1 ]
Karimov, R. Kh [1 ]
Garipova, G. M. [1 ]
Volotskova, R. R. [1 ,3 ]
Potapov, A. A. [2 ]
机构
[1] M Akmullah Bashkir State Pedag Univ, Zeldovich Int Ctr Astrophys, 3A,October Revolut St, Ufa 450008, Russia
[2] Bashkir State Univ, Dept Phys & Astron, 47A,Lenin St, Sterlitamak 453103, RB, Russia
[3] Salavat Ind Coll, 27 Matrosova Blvd, Salavat 453259, RB, Russia
来源
EUROPEAN PHYSICAL JOURNAL C | 2022年 / 82卷 / 03期
关键词
TRAPPED SURFACES; INITIAL DATA; SINGULARITIES; ENERGY;
D O I
10.1140/epjc/s10052-022-10108-3
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
The hoop conjecture, due to Thorne, is a fundamental aspect of black holes in classical general relativity. Recently, generalized classes of regular spherically symmetric static black holes with arbitrary exponents coupled to nonlinear electrodynamics have been constructed in the literature. The conjecture in those spacetimes could be violated if only the asymptotic mass M-infinity is used. To avoid such violations, Hod earlier suggested the appropriate mass function and stated the conjecture in terms of what we call the Hod function. The conjecture can then be applied to any given static spacetime to test whether or not it represents black holes. It is shown here that the conjecture is protected in the above constructed class of generalized spacetimes thus supporting them as black holes. However, it is argued that there are factors, including violation of the conjecture, that militate against the proposed new class of solutions to be qualifying as black holes. Finally, we exemplify that the Hod mass M(r <= R) in the conjecture is exactly the matter counterpart of theMisner-Sharp geometrical quasilocal mass m(r <= R) of general relativity. Thus any conclusion based on Hod function is strictly a conclusion of general relativity.
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页数:9
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    R. R. Volotskova
    A. A. Potapov
    The European Physical Journal C, 2022, 82
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