Quasinormal modes in Schwarschild black holes due to arbitrary spin fields

dc.creatorShu, Fu-Wen
dc.creatorShen, You-Gen
dc.date2005-01-30
dc.date2005-05-31
dc.date.accessioned2026-07-07T10:48:17Z
dc.date.available2026-07-07T10:48:17Z
dc.descriptionThe Newman-Penrose formalism is used to deal with the massless scalar, neutrino, electromagnetic, gravitino and gravitational quasinormal modes (QNMs) in Schwarzschild black holes in a united form. The quasinormal mode frequencies evaluated by using the 3rd-order WKB potential approximation show that the boson perturbations and the fermion perturbations behave in a contrary way for the variation of the oscillation frequencies with spin, while this is no longer true for the damping's, which variate with $s$ in a same way both for boson and fermion perturbations.
dc.description11 pages, 3 figures
dc.identifierhttps://arxiv.org/abs/gr-qc/0501098
dc.identifierhttp://arxiv.org/abs/gr-qc/0501098
dc.identifierPhys.Lett.B619:340-346,2005
dc.identifierdoi:10.1016/j.physletb.2005.05.077
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/183826
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleQuasinormal modes in Schwarschild black holes due to arbitrary spin fields
dc.typetext

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