Fluid black holes with electric field
Abstract We investigate the gravitational field of static perfect-fluid in the presence of electric field. We adopt the equation of state $$p(r)=-\rho (r)/3$$ p(r)=-ρ(r)/3 for the fluid in order to consider the closed ($$S_3$$ S3 ) or the open ($$H_3$$ H3 ) background spatial topology. Depending on...
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Series: | European Physical Journal C: Particles and Fields |
Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-019-6536-7 |
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doaj-95929200043a4da882ac36c01e48d1eb2020-11-24T23:51:55ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-01-0179111010.1140/epjc/s10052-019-6536-7Fluid black holes with electric fieldInyong Cho0School of Liberal Arts, Seoul National University of Science and TechnologyAbstract We investigate the gravitational field of static perfect-fluid in the presence of electric field. We adopt the equation of state $$p(r)=-\rho (r)/3$$ p(r)=-ρ(r)/3 for the fluid in order to consider the closed ($$S_3$$ S3 ) or the open ($$H_3$$ H3 ) background spatial topology. Depending on the scales of the mass, spatial-curvature and charge parameters (K, $$R_0$$ R0 , Q), there are several types of solutions in $$S_3$$ S3 and $$H_3$$ H3 classes. Out of them, the most interesting solution is the Reisner–Norström type of black hole. Due to the electric field, there are two horizons in the geometry. There exists a curvature singularity inside the inner horizon as usual. In addition, there exists a naked singularity at the antipodal point in $$S_3$$ S3 outside the outer horizon due to the fluid. Both of the singularities can be accessed only by radial null rays.http://link.springer.com/article/10.1140/epjc/s10052-019-6536-7 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Inyong Cho |
spellingShingle |
Inyong Cho Fluid black holes with electric field European Physical Journal C: Particles and Fields |
author_facet |
Inyong Cho |
author_sort |
Inyong Cho |
title |
Fluid black holes with electric field |
title_short |
Fluid black holes with electric field |
title_full |
Fluid black holes with electric field |
title_fullStr |
Fluid black holes with electric field |
title_full_unstemmed |
Fluid black holes with electric field |
title_sort |
fluid black holes with electric field |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2019-01-01 |
description |
Abstract We investigate the gravitational field of static perfect-fluid in the presence of electric field. We adopt the equation of state $$p(r)=-\rho (r)/3$$ p(r)=-ρ(r)/3 for the fluid in order to consider the closed ($$S_3$$ S3 ) or the open ($$H_3$$ H3 ) background spatial topology. Depending on the scales of the mass, spatial-curvature and charge parameters (K, $$R_0$$ R0 , Q), there are several types of solutions in $$S_3$$ S3 and $$H_3$$ H3 classes. Out of them, the most interesting solution is the Reisner–Norström type of black hole. Due to the electric field, there are two horizons in the geometry. There exists a curvature singularity inside the inner horizon as usual. In addition, there exists a naked singularity at the antipodal point in $$S_3$$ S3 outside the outer horizon due to the fluid. Both of the singularities can be accessed only by radial null rays. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-019-6536-7 |
work_keys_str_mv |
AT inyongcho fluidblackholeswithelectricfield |
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