THE WAVE-FUNCTION OF A BLACK-HOLE AND THE DYNAMICAL ORIGIN OF ENTROPY

被引:81
作者
BARVINSKY, AO
FROLOV, VP
ZELNIKOV, AI
机构
[1] NUCL SAFETY INST,MOSCOW 113191,RUSSIA
[2] PN LEBEDEV PHYS INST,CIAR COSMOL PROGRAM,MOSCOW 117924,RUSSIA
来源
PHYSICAL REVIEW D | 1995年 / 51卷 / 04期
关键词
D O I
10.1103/PhysRevD.51.1741
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Recently it was proposed to explain the dynamical origin of the entropy of a black hole by identifying its dynamical degrees of freedom with the physical modes propagating in the black hole interior. The present paper contains the further development of this approach. The no-boundary proposal (analogous to the cosmological no-boundary wave function) is put forward for the pure quantum state of a black hole. This is a functional on the configuration space of physical fields (including the gravitational one) inhabiting the three-dimensional space of the Einstein-Rosen bridge topology. For linearized field perturbations on the Schwarzschild-Kruskal background this no-boundary wave function coincides with the Hartle-Hawking vacuum state. The invariant definition of interior and exterior modes is proposed and the duality existing between them is discussed. The density matrix H describing the internal state of a black hole is obtained by averaging over the exterior modes. The dynamical entropy, determined by -TrHlnH, is calculated. It is shown that the one-loop contribution to the dynamical entropy calculated for a given black hole background is divergent. The notion of an instant horizon is proposed, which separates the interior from the exterior of the black hole. It is argued that quantum fluctuations of the instant horizon inherent in the proposed formalism may give the necessary cutoff and provide a black hole with finite dynamical entropy. The relation between the dynamical entropy and the standard dynamical entropy and the standard Bekenstein-Hawking (thermodynamical) entropy is briefly discussed. © 1995 The American Physical Society.
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页码:1741 / 1763
页数:23
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