Abstract

Understanding the microscopic behavior of the black holes ingredients has been one of the important challenges in black holes physics during the past decades. In order to shed some light on the microscopic structure of black holes, in this paper, we explore a recently observed phenomenon for black holes namely reentrant phase transition, by employing the Ruppeiner geometry. Interestingly enough, we observe two properties for the phase behaviour of small black holes that leads to reentrant phase transition. They are correlated and they are of the interaction type. For the range of pressure in which the system underlies reentrant phase transition, it transits from large black holes phase to small one which possesses higher correlation than the other ranges of pressures. On the other hand, the type of interaction between small black holes near large/small transition line, differs for usual and reentrant phase transitions. Indeed, for usual case, the dominant interaction is repulsive whereas for reentrant case we encounter with an attractive interaction. We show that in reentrant phase transition case, the small black holes behave like a Bosonic gas whereas in the usual phase transition case, they behave like a quantum anyon gas.

Highlights

  • A reentrant phase transition (RPT) occurs when a monotonic variation of any thermodynamic quantity gives rise to more than one phase transition (PT) such that the initial and final states are macroscopically the same

  • In order to shed some light on the microscopic structure of black holes, in this paper, we explore a recently observed phenomenon for black holes namely reentrant phase transition, by employing the Ruppeiner geometry

  • We show that in the reentrant phase transition case, the small black holes behave like a bosonic gas whereas in the usual phase transition case, they behave like a quantum anyon gas

Read more

Summary

INTRODUCTION

A reentrant phase transition (RPT) occurs when a monotonic variation of any thermodynamic quantity gives rise to more than one phase transition (PT) such that the initial and final states are macroscopically the same. In [6], d-dimensional singly spinning Kerr-AdS BHs were studied and it was shown that RPT appears for d ≥ 6 In these two BH systems, an RPT is accompanied by a Hawking-Page (HP) phase transition. Compare the behaviors of Ricci scalar of Ruppeiner geometry R (referred to as Ruppeiner invariant) for the situations in which an RPT appears and try to infer its microscopic origin We do this in the case of BI-AdS BHs as well as singly spinning Kerr-AdS BHs. The sign of the Ruppeiner invariant indicates the dominant interaction between possible molecules of a BH (R > 0: repulsion, R < 0: attraction and R 1⁄4 0: no interaction) [21,22,23], while its magnitude is a measure of the average number Planck areas on the event horizon that are correlated with each other [24] (for more information, see [25,26] and references therein).

REVIEW OF BLACK HOLE RPT
BI-AdS black holes
Singly-spinning Kerr-AdS black holes
Reentrant phase transition
MICROSCOPIC ORIGIN OF THE BLACK HOLE RPT
SUMMARY AND CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call