Abstract

In General Relativity, addressing coupling to a non-linear electromagnetic field, together with a negative cosmological constant, we obtain the general static spherical symmetric black hole solution with magnetic charges, which is asymptotic to anti-de Sitter (AdS) space-times. In particular, for a degenerate case the solution becomes a Hayward–AdS black hole, which is regular everywhere in the full space-time. The existence of such a regular black hole solution preserves the weak energy condition, while the strong energy condition is violated. We then derive the first law and the Smarr formula of the black hole solution. We further discuss its thermodynamic properties and study the critical phenomena in the extended phase space where the cosmological constant is treated as a thermodynamic variable as well as the parameter associated with the non-linear electrodynamics. We obtain many interesting results such as: the Maxwell equal area law in the P{-}V (or S{-}T) diagram is violated and consequently the critical point (T_*,P_*) of the first order small–large black hole transition does not coincide with the inflection point (T_c,P_c) of the isotherms; the Clapeyron equation describing the coexistence curve of the Van der Waals (vdW) fluid is no longer valid; the heat capacity at constant pressure is finite at the critical point; the various exponents near the critical point are also different from those of the vdW fluid.

Highlights

  • 266 Page 2 of 14 of regular black holes could be non-linear electrodynamics

  • Some regular black hole solutions have been constructed in f (T ) gravity coupled to a non-linear electrodynamics [15]

  • The general static spherical symmetric black hole solution involves an extra Schwarzschild mass term such that the solution reduces to a Schwarzschild black hole in the neutral limit

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Summary

Einstein gravity coupled to non-linear electrodynamics

We consider Einstein gravity coupled to a non-linear electromagnetic field of the type. We consider static spherical symmetric black holes with magnetic charges. The most general ansatz is given by ds2 = − f dt2 + dr 2 + r 2d 2, f. Where f = f (r ) and d = dθ 2 + sin θ 2dφ denotes the metric of a unit 2-sphere, Qm is the total magnetic charge carried by the black hole. In [16], a general strategy will be developed for constructing exact black hole solutions with electric/magnetic charges in this gravity model. For our purposes, we focus on a well-known regular black hole model, namely the Hayward black hole [6] generalized in AdS space-time

Hayward–AdS black hole
The first law of thermodynamics
P–V criticality of Hayward–AdS black hole
Equation of state and Gibbs free energy
Critical exponents
With singularities
P–V criticality for canonical ensemble
Conclusion
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