Abstract

We propose a new class of vector fields to construct a conserved charge in a general field theory whose energy–momentum tensor is covariantly conserved. We show that there always exists such a vector field in a given field theory even without global symmetry. We also argue that the conserved current constructed from the (asymptotically) timelike vector field can be identified with the entropy current of the system. As a piece of evidence we show that the conserved charge defined therefrom satisfies the first law of thermodynamics for an isotropic system with a suitable definition of temperature. We apply our formulation to several gravitational systems such as the expanding universe, Schwarzschild and Banãdos, Teitelboim and Zanelli (BTZ) black holes, and gravitational plane waves. We confirm the conservation of the proposed entropy density under any homogeneous and isotropic expansion of the universe, the precise reproduction of the Bekenstein–Hawking entropy incorporating the first law of thermodynamics, and the existence of gravitational plane wave carrying no charge, respectively. We also comment on the energy conservation during gravitational collapse in simple models.

Highlights

  • A central mystery in theory of gravity is that while it is governed by fundamental physics laws, it contains black holes, which behave as thermodynamical objects.[1, 2]

  • We show that our entropy current density satisfies the first law of thermodynamics in isotropic systems, so that the shift vector vanishes and the matter energy momentum tensor is given by a perfect √fluid, characterized by P μ ν = P ḡ μ ν and d log

  • We have proposed a procedure to construct a conserved current in any field theory with covariantly conserved energy momentum tensor and interpreted it as the entropy current

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Summary

Introduction

A central mystery in theory of gravity is that while it is governed by fundamental physics laws, it contains black holes, which behave as thermodynamical objects.[1, 2]. We reached a definition to evaluate a total charge of matter by a volume integration of its charge distribution, and proposed a precise definition available on a general curved space–time with Killing vector fields.[20] This definition was recognized in early time,[21, 22] though the validity thereof has not been confirmed by explicit computation We confirmed that this reproduces known results on mass and angular momentum for classic black holes, and that it gives an additional contribution to the known mass formula of any compact star obtained by quasi-local energy.[20] (See Ref. 23.). We present our argument to reach this conclusion with application to several gravitational systems in what follows

Conservation condition
Intrinsic vector field
Entropy and Entropy Current
Analysis for geometry without horizon
The first law of thermodynamics
Case for black hole geometry
Friedmann–Lemaıtre–Robertson–Walker metric
Schwarzschild black hole
BTZ black hole
Exact gravitational plane wave
Discussion
Thick light shells
Matters with nonzero pressure
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