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Thermodynamics of AdS-Schwarzschild-like black hole in loop quantum gravity

Rui-Bo Wang, Shijie Ma, Lei You, Y.S. Tang, Yu-Hang Feng, Xian-Ru Hu, Jian-Bo Deng

2024The European Physical Journal C21 citationsDOIOpen Access PDF

Abstract

Abstract We obtained the metric of the Schwarzschild-like black hole with loop quantum gravity (LQG) corrections in anti-de Sitter (AdS) space-time, under the assumption that the cosmological constant is decoupled in LQG. We investigated its thermodynamics, including the equation of state, criticality, heat capacity, and Gibbs free energy. The $$P-v$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>P</mml:mi> <mml:mo>-</mml:mo> <mml:mi>v</mml:mi> </mml:mrow> </mml:math> graph was plotted, and the critical behavior was calculated. It was found that, due to the LQG effect, the quantum-corrected Schwarzschild-AdS black hole exhibits a critical point and a critical ratio of 7/18, which differs from the Reissner–Nordstr $$\ddot{\textrm{o}}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mtext>o</mml:mtext> <mml:mo>¨</mml:mo> </mml:mover> </mml:math> m-AdS black hole’s ratio of 3/8 (the same as that of the Van der Waals system) slightly. However, there are still some similarities compared to the Van der Waals system, such as the same critical exponents and a similar $$P-v$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>P</mml:mi> <mml:mo>-</mml:mo> <mml:mi>v</mml:mi> </mml:mrow> </mml:math> graph. Moreover, it is concluded that the energy-momentum tensor related to the black hole’s mass could violate the conventional first law of thermodynamics. This modified first law may violate the conservation of Gibbs free energy during the small black hole-large black hole phase transitions, potentially indicating the occurrence of the zeroth-order phase transition. The Joule–Thomson expansion was also studied. Interestingly, compared to the Schwarzschild-AdS black hole, the LQG effect leads to inversion points. The inversion curve divides the $$\left( P,T\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfenced> <mml:mi>P</mml:mi> <mml:mo>,</mml:mo> <mml:mi>T</mml:mi> </mml:mfenced> </mml:math> coordinate system into two regions: a heating region and a cooling region, as shown in detail by the inversion curves and isenthalpic curves. The results indicated that there is a minimum inversion mass, below which any black hole will not possess an inversion point.

Topics & Concepts

Loop quantum gravityPhysicsBlack hole thermodynamicsSchwarzschild radiusSchwarzschild metricBlack hole (networking)Loop (graph theory)Quantum gravityTheoretical physicsQuantumClassical mechanicsMathematical physicsThermodynamicsQuantum mechanicsGravitationMathematicsComputer scienceGeneral relativityEntropy (arrow of time)CombinatoricsLink-state routing protocolComputer networkRouting protocolRouting (electronic design automation)Black Holes and Theoretical PhysicsNoncommutative and Quantum Gravity TheoriesCosmology and Gravitation Theories
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