Cardy-Verlinde Formula and asymptotically flat rotating Charged black holes
Jiliang Jing

TL;DR
This paper extends the Cardy-Verlinde formula to various asymptotically flat rotating charged black holes in Einstein-Maxwell and string theories, analyzing their entropy bounds and revealing tighter bounds than Bekenstein's in some cases.
Contribution
It generalizes the Cardy-Verlinde formula to several black hole solutions and explores their entropy bounds, including new unified expressions and tighter bounds than Bekenstein's.
Findings
The Cardy-Verlinde formula is adapted to Kerr-Newman, EMDA, Kaluza-Klein, and Sen black holes.
The entropy bounds for Kaluza-Klein and Sen black holes are tighter than Bekenstein's bound.
Unified entropy bounds are derived for EMDA, Kaluza-Klein, and Sen black holes.
Abstract
The Cardy-Verlinde formula is generalized to the asymptotically flat rotating charged black holes in the Einstein-Maxwell theory and low-energy effective field theory describing string by using some typical spacetimes, such as the Kerr-Newman, Einstein-Maxwell-dilaton-axion, Kaluza-Klein, and Sen black holes. For the Kerr-Newman black hole, the definition of the Casimir energy takes the same form as that of the Kerr-Newman-AdS and Kerr-Newman-dS black holes, while the Cardy-Verlinde formula possesses different from since the Casimir energy does not appear in the extensive energy. The Einstein-Maxwell-dilaton-axion, Kaluza-Klein, and Sen black holes have special property: The definition of the Casimir energy for these black holes is similar to that of the Kerr-Newman black hole, but the Cardy-Verlinde formula takes the same form as that of the Kerr black hole. Furthermore, we…
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Taxonomy
TopicsBlack Holes and Theoretical Physics · Cosmology and Gravitation Theories · Quantum Electrodynamics and Casimir Effect
