Cosmology with the CFT-radiation matter

dc.creatorMyung, Y. S.
dc.date2001-11-15
dc.date.accessioned2026-07-07T11:31:57Z
dc.date.available2026-07-07T11:31:57Z
dc.descriptionWe review the relation between entropy bounds to rewrite Friedmann equation on the brane in terms of three entropy bounds: Bekenstein-Verlinde ($S_{BV}$); Bekenstein-Hawking bound ($S_{BH}$); Hubble bound ($S_H$). For a strongly coupled conformal field theory (CFT) with a dual 5-dimensional anti de Sitter Schwarzschild (AdSS$_5$) black hole, we can easily establish the connection between the Cardy-Verlinde formula on the CFT side and the entropy representation of Friedmann equation in cosmology. In this case its cosmological evolution for entropy is given by the semi-circle. However, for the matter-dominated case, we find that the cosmological evolution diagram takes a different form of the cycloid. Here we propose two different entropy relations for matter-dominated case. It turns out that the Verlinde's entropy relation so restricted that it may not be valid for the matter-dominated universe.
dc.description14 pages, Talk at the 7th Italian-Korean Symposium on Relativistic Astrophysics, Kimhae, Korea, 23-28 July 2001
dc.identifierhttps://arxiv.org/abs/hep-th/0111136
dc.identifierhttp://arxiv.org/abs/hep-th/0111136
dc.identifierJ.KoreanPhys.Soc.42:S105,2003
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/197439
dc.subjectHigh Energy Physics - Theory
dc.titleCosmology with the CFT-radiation matter
dc.typetext

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