Summary
Both the event horizon equation and the radiation temperature of a rotating and arbitrarily accelerating non-stationary black hole are shown. The event horizon surface is no longer a sphere. The temperature and the spectral distribution of radiation depend on not only the time, but also the direction angles.
Similar content being viewed by others
References
Zhao Zheng andDai Xian-xin,Mod. Phys. Lett. A,7 (1992) 1771.
Zhao Zheng andLi Zhong-heng,Nuovo Cimento B,108 (1993) 785.
Yang Bo andZhao Zheng,Int. J. Theor. Phys.,32 (1993) 1237.
Zhao Zheng andDai Xian-xin,Chin. Phys. Lett.,8 (1991) 548.
Jing Jiliang, Yu Hongwei andWang Yongjiu,Chin. Phys. Lett.,9 (1992) 113.
Kinnersley W.,Phys. Rev.,186 (1969) 1335.
Damour T. andRuffini R.,Phys. Rev. D,14, (1976) 332.
Sannan S.,Gen. Rel. Grav.,20, (1988) 239.
Author information
Authors and Affiliations
Additional information
The authors of this paper have agreed to not receive the proofs for correction.
Work supported by the National Natural Science Foundation of China.
Rights and permissions
About this article
Cite this article
Ming-Chao, S., Ren, Z. & Zheng, Z. Hawking effect of a rotating, arbitrarily accelerating black hole. Nuovo Cimento B 110, 829–837 (1995). https://doi.org/10.1007/BF02820151
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02820151