Abstract

On the basis of the state parameter of de Sitter space-time satisfying the first law of thermodynamics, we can derive some effective thermodynamic quantities. When the temperature of the black hole horizon is equal to that of the cosmological horizon, we think that the effective temperature of the space-time should have the same value. Using this condition, we obtain a differential equation of the entropy of the de Sitter black hole in the higher-dimensional de Rham, Gabadadze and Tolley (dRGT) massive gravity. Solving the differential equation, we obtain the corrected entropy and effective thermodynamic quantities of the de Sitter black hole. The results show that for multi-parameter black holes, the entropy satisfied differential equation is invariable with different independent state parameters. Therefore, the entropy of higher-dimensional dS black holes in dRGT massive gravity is only a function of the position of the black hole horizon, and is independent of other state parameters. It is consistent with the corresponding entropy of the black hole horizon and the cosmological horizon. The thermodynamic quantities of self-consistent de Sitter space-time are given theoretically, and the equivalent thermodynamic quantities have the second-order phase transformation similar to AdS black hole, but unlike AdS black hole, the equivalent temperature of de Sitter space-time has a maximum value. By satisfying the requirement of thermodynamic equilibrium and stability of space-time, the conditions for the existence of dS black holes in the universe are obtained.

Highlights

  • We regard the HBHRGT space-time as a thermodynamic system, for which the state parameters satisfy the first law of thermodynamics, Considering the connection between the black hole horizon and the cosmological horizon, we can derive the effective thermodynamic quantities and the corresponding first law of black hole thermodynamics

  • Studies on the effective temperature of de Sitter spacetime were based on the assumption that the space-time entropy is known [35,40,65–68], and the effective temperature of de Sitter space-time was obtained by using the spacetime thermodynamic quantity to satisfy the first law of thermodynamics

  • Hole horizon is equal to that of the cosmological horizon: T = T+ = Tc, the effective temperature Tef f obtained is not equal to that of the two horizons in general, that is Tef f = T, it is hard to be accepted by people

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Summary

Introduction

J. C (2020) 80:213 space-time were analyzed in paper [40] in which, on the basis of dimensional consistency, we assume that dS space-time’s entropy is a function in the form of Fn(x), with x = r+/rc (r+,c is the position of black hole horizon and cosmological horizon namely). The thermodynamic characteristics of de Sitter space-time are discussed on the basis of considering the correlation between black hole horizon and cosmological horizon. Effective temperature and entropy of higher-dimensional dS black holes in dRGT massive gravity (HBHRGT) space-time are obtained and the influence of coupling coefficients ci m2 on the effective temperature and entropy is analyzed. The total space-time entropy and effective temperature of HBHRGT satisfying the first law of thermodynamics are given on the basis of considering the correlation between the two horizons.

Higher-dimensional dS black holes in dRGT massive gravity
Effective thermodynamic quantity
Critical phenomena
Conclusion and discussion
Full Text
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