Entropy of quantum-corrected black holes

dc.creatorMatyjasek, Jerzy
dc.date2006-10-05
dc.date.accessioned2026-07-07T10:24:32Z
dc.date.available2026-07-07T10:24:32Z
dc.descriptionThe approximate renormalized one-loop effective action of the quantized massive scalar, spinor and vector field in a large mass limit, i.e., the lowest order of the DeWitt-Schwinger expansion involves the coincidence limit of the Hadamard-DeWitt coefficient a3. Building on this and using Wald's approach we shall construct the general expression describing entropy of the spherically-symmetric static black hole being the solution of the semi-classical field equations. For the concrete case of the quantum-corrected Reissner-Nordstrom black hole this result coincides, as expected, with the entropy obtained by integration of the first law of black hole thermodynamics with a suitable choice of the integration constant. The case of the extremal quantum corrected black hole is briefly considered.
dc.identifierhttps://arxiv.org/abs/gr-qc/0610020
dc.identifierhttp://arxiv.org/abs/gr-qc/0610020
dc.identifierPhys.Rev.D74:104030,2006
dc.identifierdoi:10.1103/PhysRevD.74.104030
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/176225
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleEntropy of quantum-corrected black holes
dc.typetext

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