Spherically Symmetric Exact Vacuum Solutions in Einstein-Aether Theory

被引:13
|
作者
Oost, Jacob [1 ,2 ]
Mukohyama, Shinji [3 ,4 ]
Wang, Anzhong [1 ,5 ]
机构
[1] Baylor Univ, GCAP CASPER, Phys Dept, Waco, TX 76798 USA
[2] Odyssey Space Res, 1120 NASA Pkwy, Houston, TX 77058 USA
[3] Kyoto Univ, Yukawa Inst Theoret Phys, Ctr Gravitat Phys, Kyoto 6068502, Japan
[4] Univ Tokyo, Kavli Inst Phys & Math Universe WPI, Inst Adv Study, Kashiwa, Chiba 2778583, Japan
[5] Zhejiang Univ Technol, Inst Theoret Phys & Cosmol, Hangzhou 310023, Peoples R China
基金
日本学术振兴会; 中国国家自然科学基金;
关键词
Einstein-aether theory; spherical symmetry; exact solution; singularities; black holes; cosmological models; BLACK-HOLES;
D O I
10.3390/universe7080272
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We study spherically symmetric spacetimes in Einstein-aether theory in three different coordinate systems, the isotropic, Painleve-Gullstrand, and Schwarzschild coordinates, in which the aether is always comoving, and present both time-dependent and time-independent exact vacuum solutions. In particular, in the isotropic coordinates we find a class of exact static solutions characterized by a single parameter c14 in closed forms, which satisfies all the current observational constraints of the theory, and reduces to the Schwarzschild vacuum black hole solution in the decoupling limit (c14=0). However, as long as c14 not equal 0, a marginally trapped throat with a finite non-zero radius always exists, and on one side of it the spacetime is asymptotically flat, while on the other side the spacetime becomes singular within a finite proper distance from the throat, although the geometric area is infinitely large at the singularity. Moreover, the singularity is a strong and spacetime curvature singularity, at which both of the Ricci and Kretschmann scalars become infinitely large.
引用
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页数:24
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