KONOPLYA, Roman and A. ZHIDENKO. How general is the strong cosmic censorship bound for quasinormal modes? Journal of Cosmology and Astroparticle Physics. GB - Spojené království Velké Británie a, 2022, vol. 2022, No 11, p. "028-1"-"028-10", 10 pp. ISSN 1475-7516. Available from: https://dx.doi.org/10.1088/1475-7516/2022/11/028.
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Basic information
Original name How general is the strong cosmic censorship bound for quasinormal modes?
Authors KONOPLYA, Roman (804 Ukraine, belonging to the institution) and A. ZHIDENKO.
Edition Journal of Cosmology and Astroparticle Physics, GB - Spojené království Velké Británie a, 2022, 1475-7516.
Other information
Original language English
Type of outcome Article in a journal
Field of Study 10308 Astronomy
Country of publisher United Kingdom of Great Britain and Northern Ireland
Confidentiality degree is not subject to a state or trade secret
WWW URL
RIV identification code RIV/47813059:19630/22:A0000238
Organization unit Institute of physics in Opava
Doi http://dx.doi.org/10.1088/1475-7516/2022/11/028
Keywords in English quasinormal mode ;black hole;Cauchy horizon;gravitational waves / theory; gravity; modified gravity
Tags , RIV23
Tags International impact, Reviewed
Changed by Changed by: Mgr. Pavlína Jalůvková, učo 25213. Changed: 8/3/2023 12:08.
Abstract
Hod's proposal claims that the least damped quasinormal mode of a black hole must have the imaginary part smaller than half of the surface gravity at the event horizon. The Strong Cosmic Censorship in General Relativity implies that this bound must be even weaker: half of the surface gravity at the Cauchy horizon. The appealing question is whether these bounds are limited by the Einstein theory only? Here we will present numerical evidence that once the black hole size is much smaller than then the radius of the cosmological horizon, both the Hod's proposal and the strong cosmic censorship bound for quasinormal modes are satisfied for general spherically symmetric black holes in an arbitrary metric theory of gravity. The low-lying quasinormal frequencies have the universal behavior in this regime and do not depend on the near-horizon geometry, but only on the asymptotic parameters: the value of the cosmological constant and black hole mass.
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