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dc.contributor.authorAnninos, Den_US
dc.contributor.authorAnous, Ten_US
dc.date.accessioned2024-03-26T08:41:58Z
dc.date.issued2010-12-01en_US
dc.identifier.issn1126-6708en_US
dc.identifier.urihttps://qmro.qmul.ac.uk/xmlui/handle/123456789/95711
dc.description.abstractRotating black holes in de Sitter space are known to have interesting limits where the temperatures of the black hole and cosmological horizon are equal. We give a complete description of the thermal phase structure of all allowed rotating black hole configurations. Only one configuration, the rotating Nariai limit, has the black hole and cosmological horizons both in thermal and rotational equilibrium, in that both the temperatures and angular velocities of the two horizons coincide. The thermal evolution of the spacetime is shown to lead to the pure de Sitter spacetime, which is the most entropic configuration. We then provide a comprehensive study of the wave equation for a massless scalar in the rotating Nariai geometry. The absorption cross section at the black hole horizon is computed and a condition is found for when the scattering becomes superradiant. The boundary-to-boundary correlators at finite temperature are computed at future infinity. The quasinormal modes are obtained in explicit form. Finally, we obtain an expression for the expectation value of the number of particles produced at future infinity starting from a vacuum state with no incoming particles at past infinity. Some of our results are used to provide further evidence for a recent holographic proposal between the rotating Nariai geometry and a two-dimensional conformal field theory. © 2010 SISSA.en_US
dc.relation.ispartofJournal of High Energy Physicsen_US
dc.titleA de Sitter hoedownen_US
dc.typeArticle
dc.identifier.doi10.1007/JHEP08(2010)131en_US
pubs.issue8en_US
pubs.notesNot knownen_US
pubs.publication-statusPublisheden_US
pubs.volume2010en_US
rioxxterms.funderDefault funderen_US
rioxxterms.identifier.projectDefault projecten_US


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