Photon regions, shadow observables, and constraints from M87*of a charged rotating black hole

被引:40
|
作者
Meng, Yuan [1 ]
Kuang, Xiao-Mei [1 ]
Tang, Zi-Yu [2 ,3 ]
机构
[1] Yangzhou Univ, Ctr Gravitat & Cosmol, Coll Phys Sci & Technol, Yangzhou 225009, Peoples R China
[2] UCAS, Hangzhou Inst Adv Study, Sch Fundamental Phys & Math Sci, Hangzhou 310024, Peoples R China
[3] Univ Chinese Acad Sci, Sch Phys Sci, Beijing 100049, Peoples R China
关键词
GRAVITY;
D O I
10.1103/PhysRevD.106.064006
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Inspired by the observations of the supermassive black hole M87* by the Event Horizon Telescope (EHT), a remarkable surge in black hole physics is to use the black hole shadow's observables to distinguish between general relativity and modified theories of gravity, which could also help to reveal the astrophysical nature of the central black hole in the EHT observation. In this paper, we study a charged rotating black hole in conformal gravity, in which the term related to the charge has different falloffs from the usual Kerr-Newman (KN) black hole. We investigate the spacetime properties including the horizons, ergospheres, and photon regions; then, we show the boundary of the black hole shadow and investigate its characteristic observables. These features closely depend on the spin and charge parameters, which are compared with those in Kerr and KN black holes. Then, presupposing that M87* is a charged rotating black hole in conformal gravity, we constrain the black hole parameters via the observational constraints from EHT. We find that the constraints on the inferred circularity deviation (delta C ?0.1) and shadow axial ratio (1 ? D-x ? 4/3) for M87* are satisfied for the entire parameter space of the charged rotating black hole in conformal gravity. However, the shadow angular diameter theta(d) = 42 +/- 3 mu as gives an upper bound on the parameter space. Our findings indicate that the current charged rotating black hole in conformal gravity could be a candidate for astrophysical black holes. Moreover, the EHT observation of the axial ratio Dx may help us to distinguish between a Kerr black hole and the current charged rotating black hole in conformal gravity in some parameter space.
引用
收藏
页数:17
相关论文
共 50 条
  • [1] Hybrid Mapping of the Black Hole Shadow in M87
    Carilli, Chris L.
    Thyagarajan, Nithyanandan
    [J]. ASTROPHYSICAL JOURNAL, 2022, 924 (02):
  • [2] Shadow of Kerr black hole surrounded by a cloud of strings in Rastall gravity and constraints from M87
    Sun, Qi
    Zhang, Yu
    Xie, Chen-Hao
    Li, Qi-Quan
    [J]. PHYSICS OF THE DARK UNIVERSE, 2024, 46
  • [3] Black Hole Spin Signature in the Black Hole Shadow of M87 in the Flaring State
    Kawashima, Tomohisa
    Kino, Motoki
    Akiyama, Kazunori
    [J]. ASTROPHYSICAL JOURNAL, 2019, 878 (01):
  • [4] The shadow of M87*black hole within rational nonlinear electrodynamics
    Kruglov, S. I.
    [J]. MODERN PHYSICS LETTERS A, 2020, 35 (35)
  • [5] Strong gravitational lensing and shadow constraint from M87*of slowly rotating Kerr-like black hole
    Kuang, Xiao-Mei
    Ovgun, Ali
    [J]. ANNALS OF PHYSICS, 2022, 447
  • [6] Chandra and the black hole in M87
    Di Matteo, T
    Allen, SW
    Fabian, AC
    Wilson, AS
    Young, AJ
    [J]. LIGHTHOUSES OF THE UNIVERSE: THE MOST LUMINOUS CELESTIAL OBJECTS AND THEIR USE FOR COSMOLOGY, 2002, : 443 - 449
  • [7] The 'quiescent' black hole in M87
    Reynolds, CS
    DiMatteo, T
    Fabian, AC
    Hwang, U
    Canizares, CR
    [J]. MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1996, 283 (04) : L111 - L116
  • [8] Spin of the M87 Black Hole
    Garofalo, David
    [J]. ANNALEN DER PHYSIK, 2020, 532 (04)
  • [9] The shadows of accelerating Kerr-Newman black hole and constraints from M87
    Sui, Tao-Tao
    Fu, Qi-Ming
    Guo, Wen-Di
    [J]. PHYSICS LETTERS B, 2023, 845
  • [10] Spins of the supermassive black hole in M87: New constraints from tev observations
    Wang, Jian-Min
    Li, Yan-Rong
    Wang, Jian-Cheng
    Zhang, Shu
    [J]. ASTROPHYSICAL JOURNAL LETTERS, 2008, 676 (02): : L109 - L112