Effective Tolman temperature induced by trace anomaly

Abstract Despite the finiteness of stress tensor for a scalar field on the four-dimensional Schwarzschild black hole in the Israel–Hartle–Hawking vacuum, the Tolman temperature in thermal equilibrium is certainly divergent on the horizon due to the infinite blue-shift of the Hawking temperature. The...

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Main Authors: Myungseok Eune, Yongwan Gim, Wontae Kim
Format: Article
Language:English
Published: SpringerOpen 2017-04-01
Series:European Physical Journal C: Particles and Fields
Subjects:
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-4812-y
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spelling doaj-772d6968ba024af49b798826caa33f382020-11-24T20:43:31ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-04-017741510.1140/epjc/s10052-017-4812-yEffective Tolman temperature induced by trace anomalyMyungseok Eune0Yongwan Gim1Wontae Kim2Department of Civil Engineering, Sangmyung UniversityDepartment of Physics, Sogang UniversityDepartment of Physics, Sogang UniversityAbstract Despite the finiteness of stress tensor for a scalar field on the four-dimensional Schwarzschild black hole in the Israel–Hartle–Hawking vacuum, the Tolman temperature in thermal equilibrium is certainly divergent on the horizon due to the infinite blue-shift of the Hawking temperature. The origin of this conflict is due to the fact that the conventional Tolman temperature was based on the assumption of a traceless stress tensor, which is, however, incompatible with the presence of the trace anomaly responsible for the Hawking radiation. Here, we present an effective Tolman temperature which is compatible with the presence of the trace anomaly by using the modified Stefan–Boltzmann law. Eventually, the effective Tolman temperature turns out to be finite everywhere outside the horizon, and so an infinite blue-shift of the Hawking temperature at the event horizon does not appear any more. In particular, it is vanishing on the horizon, so that the equivalence principle is exactly recovered at the horizon.http://link.springer.com/article/10.1140/epjc/s10052-017-4812-yBlack HoleProper TemperatureTangential PressureSymmetric Black HoleTrace Anomaly
collection DOAJ
language English
format Article
sources DOAJ
author Myungseok Eune
Yongwan Gim
Wontae Kim
spellingShingle Myungseok Eune
Yongwan Gim
Wontae Kim
Effective Tolman temperature induced by trace anomaly
European Physical Journal C: Particles and Fields
Black Hole
Proper Temperature
Tangential Pressure
Symmetric Black Hole
Trace Anomaly
author_facet Myungseok Eune
Yongwan Gim
Wontae Kim
author_sort Myungseok Eune
title Effective Tolman temperature induced by trace anomaly
title_short Effective Tolman temperature induced by trace anomaly
title_full Effective Tolman temperature induced by trace anomaly
title_fullStr Effective Tolman temperature induced by trace anomaly
title_full_unstemmed Effective Tolman temperature induced by trace anomaly
title_sort effective tolman temperature induced by trace anomaly
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2017-04-01
description Abstract Despite the finiteness of stress tensor for a scalar field on the four-dimensional Schwarzschild black hole in the Israel–Hartle–Hawking vacuum, the Tolman temperature in thermal equilibrium is certainly divergent on the horizon due to the infinite blue-shift of the Hawking temperature. The origin of this conflict is due to the fact that the conventional Tolman temperature was based on the assumption of a traceless stress tensor, which is, however, incompatible with the presence of the trace anomaly responsible for the Hawking radiation. Here, we present an effective Tolman temperature which is compatible with the presence of the trace anomaly by using the modified Stefan–Boltzmann law. Eventually, the effective Tolman temperature turns out to be finite everywhere outside the horizon, and so an infinite blue-shift of the Hawking temperature at the event horizon does not appear any more. In particular, it is vanishing on the horizon, so that the equivalence principle is exactly recovered at the horizon.
topic Black Hole
Proper Temperature
Tangential Pressure
Symmetric Black Hole
Trace Anomaly
url http://link.springer.com/article/10.1140/epjc/s10052-017-4812-y
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AT yongwangim effectivetolmantemperatureinducedbytraceanomaly
AT wontaekim effectivetolmantemperatureinducedbytraceanomaly
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