Higher spin de Sitter quasinormal modes
Abstract We construct higher spin quasinormal modes algebraically in D-dimensional de Sitter spacetime using the ambient space formalism. The quasinormal modes fall into two nonunitary lowest-weight representations of so $$ \mathfrak{so} $$ (1, D). From a local QFT point of view, the lowest-weight q...
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2021
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oai:doaj.org-article:748a6142b2dd457db5860174b571cb5e2021-11-08T11:16:20ZHigher spin de Sitter quasinormal modes10.1007/JHEP11(2021)0251029-8479https://doaj.org/article/748a6142b2dd457db5860174b571cb5e2021-11-01T00:00:00Zhttps://doi.org/10.1007/JHEP11(2021)025https://doaj.org/toc/1029-8479Abstract We construct higher spin quasinormal modes algebraically in D-dimensional de Sitter spacetime using the ambient space formalism. The quasinormal modes fall into two nonunitary lowest-weight representations of so $$ \mathfrak{so} $$ (1, D). From a local QFT point of view, the lowest-weight quasinormal modes of massless higher spin fields are produced by gauge-invariant boundary conserved currents and boundary higher-spin Weyl tensors inserted at the southern pole of the past boundary. We also show that the quasinormal spectrum of a massless/massive spin-s field is precisely encoded in the Harish-Chandra character corresponding to the unitary massless/massive spin-s SO(1, D) representation.Zimo SunSpringerOpenarticleHigher Spin GravitySpace-Time SymmetriesNuclear and particle physics. Atomic energy. RadioactivityQC770-798ENJournal of High Energy Physics, Vol 2021, Iss 11, Pp 1-35 (2021) |
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Higher Spin Gravity Space-Time Symmetries Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 |
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Higher Spin Gravity Space-Time Symmetries Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 Zimo Sun Higher spin de Sitter quasinormal modes |
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Abstract We construct higher spin quasinormal modes algebraically in D-dimensional de Sitter spacetime using the ambient space formalism. The quasinormal modes fall into two nonunitary lowest-weight representations of so $$ \mathfrak{so} $$ (1, D). From a local QFT point of view, the lowest-weight quasinormal modes of massless higher spin fields are produced by gauge-invariant boundary conserved currents and boundary higher-spin Weyl tensors inserted at the southern pole of the past boundary. We also show that the quasinormal spectrum of a massless/massive spin-s field is precisely encoded in the Harish-Chandra character corresponding to the unitary massless/massive spin-s SO(1, D) representation. |
format |
article |
author |
Zimo Sun |
author_facet |
Zimo Sun |
author_sort |
Zimo Sun |
title |
Higher spin de Sitter quasinormal modes |
title_short |
Higher spin de Sitter quasinormal modes |
title_full |
Higher spin de Sitter quasinormal modes |
title_fullStr |
Higher spin de Sitter quasinormal modes |
title_full_unstemmed |
Higher spin de Sitter quasinormal modes |
title_sort |
higher spin de sitter quasinormal modes |
publisher |
SpringerOpen |
publishDate |
2021 |
url |
https://doaj.org/article/748a6142b2dd457db5860174b571cb5e |
work_keys_str_mv |
AT zimosun higherspindesitterquasinormalmodes |
_version_ |
1718442248942649344 |