2020
General parametrization of higher-dimensional black holes and its application to Einstein-Lovelock theory
KONOPLYA, Roman; Thomas PAPPAS and Zdeněk STUCHLÍKBasic information
Original name
General parametrization of higher-dimensional black holes and its application to Einstein-Lovelock theory
Authors
KONOPLYA, Roman (804 Ukraine, belonging to the institution); Thomas PAPPAS (300 Greece, belonging to the institution) and Zdeněk STUCHLÍK (203 Czech Republic, belonging to the institution)
Edition
Physical Review D, COLLEGE PK, AMER PHYSICAL SOC, 2020, 1550-7998
Other information
Language
English
Type of outcome
Article in a journal
Field of Study
10308 Astronomy
Country of publisher
United States of America
Confidentiality degree
is not subject to a state or trade secret
References:
Impact factor
Impact factor: 4.643 in 2014
RIV identification code
RIV/47813059:19630/20:A0000011
Organization unit
Institute of physics in Opava
UT WoS
000579342400015
EID Scopus
2-s2.0-85095114237
Keywords in English
NORMAL-MODES; SYMMETRICAL-SOLUTIONS; SPACE; THERMODYNAMICS
Tags
Tags
International impact, Reviewed
Links
GA19-03950S, research and development project.
Changed: 26/4/2022 19:12, Mgr. Pavlína Jalůvková
Abstract
V originále
Here we have developed the general parametrization for spherically symmetric and asymptotically flat black-hole spacetimes in an arbitrary metric theory of gravity. The parametrization is similar in spirit to the parametrized post-Newtonian approximation, but valid in the whole space outside the event horizon, including the near horizon region. This generalizes the continued-fraction expansion method in terms of a compact radial coordinate suggested by Rezzolla and Zhidenko [Phys. Rev. D 90, 084009 (2014)] for the four-dimensional case. As the first application of our higher-dimensional parametrization we have approximated black-hole solutions of the Einstein-Lovelock theory in various dimensions. This allows one to write down the black-hole solution which depends on many parameters (coupling constants in front of higher curvature terms) in a very compact analytic form, which depends only upon a few parameters of the parametrization. The approximate metric deviates from the exact (but extremely cumbersome) expressions by fractions of one percent even at the first order of the continued-fraction expansion, which is confirmed here by computation of observable quantities, such as quasinormal modes of the black hole.