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Rotating regular black holes in conformal massive gravity

Kimet JusufiInstitute of Physics, Faculty of Natural Sciences and Mathematics, Ss. Cyril and Methodius University, Arhimedova 3, 1000 Skopje, North MacedoniaMubasher JamilDepartment of Mathematics, School of Natural Sciences (SNS), National University of Sciences and Technology (NUST), H-12, Islamabad 44000, PakistanHrishikesh ChakrabartyCenter for Field Theory and Particle Physics and Department of Physics, Fudan University, 2005 Songhu Road, Shanghai, 200438, ChinaQiang WuInstitute for Theoretical Physics and Cosmology, Zhejiang University of Technology, Hangzhou, 310023, ChinaCosimo BambiCenter for Field Theory and Particle Physics and Department of Physics, Fudan University, 2005 Songhu Road, Shanghai, 200438, ChinaAnzhong WangGCAP-CASPER, Physics Department, Baylor University, Waco, Texas 76798-7316, USA
2020en
ABI

Аннотация

In this paper, we use a suitable conformal rescaling to construct static and rotating regular black holes in conformal massive gravity. The new metric is characterized by the mass $M$, the ``scalar charge'' $Q$, the angular momentum parameter $a$, the ``hair parameter'' $\ensuremath{\lambda}$, and the conformal scale factor encoded in the parameter $L$. We explore the shadow images and the deflection angles of relativistic massive particles in the spacetime geometry of a rotating regular black hole. For $\ensuremath{\lambda}\ensuremath{\ne}0$ and $Q>0$, the shadow is larger than the shadow of a Kerr black hole. In particular, if $\ensuremath{\lambda}<0$, the shadow radius increases considerably. For $\ensuremath{\lambda}\ensuremath{\ne}0$ and $Q<0$, the shadow is smaller than the shadow of a Kerr black hole. Additionally, we put observational constraints on the parameter $Q$ using the latest Event Horizon Telescope observation of the supermassive black hole M87*. Lastly, using the Gauss-Bonnet theorem, we show that the deflection angle of massive particles is strongly affected by the parameter $L$. The deflection angle might be used to distinguish rotating regular black holes from rotating singular black holes.

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