2019
DOI: 10.1140/epjc/s10052-019-7272-8
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Dynamical and thermal stabilities of nonlinearly charged AdS black holes

Abstract: In this paper, we study an extended phase space thermodynamics of a nonlinearly charged AdS black hole. We examine both the local and global stabilities, and possible phase transition of the black hole solutions. Finally, we compute quasi-normal modes via scalar perturbations and compare the obtained results with those of RN-AdS black hole. *

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Cited by 21 publications
(11 citation statements)
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“…The AdS/CFT correspondence suggest that for large e, quasinormal ringing becomes slower to settle down to thermal equilibrium and also, the frequency of the oscillation becomes smaller. Our results are very much consistent with literature work [42]. Figure 5 demonstrates the behavior of the effective potential versus the tortoise coordinater.…”
Section: A Wavelike Of Hayward Bh In Egb Gravitysupporting
confidence: 91%
See 1 more Smart Citation
“…The AdS/CFT correspondence suggest that for large e, quasinormal ringing becomes slower to settle down to thermal equilibrium and also, the frequency of the oscillation becomes smaller. Our results are very much consistent with literature work [42]. Figure 5 demonstrates the behavior of the effective potential versus the tortoise coordinater.…”
Section: A Wavelike Of Hayward Bh In Egb Gravitysupporting
confidence: 91%
“…In Figure 22 the imaginary part of quasinormal frequencies ω I increases and then decreases for different values of electric charge. For the increasing values of r 0 , the corresponding electric charge increases and ω I reaches to the maximum value [42]. Figure 23 shows the behavior V with increasing r 0 for different values of Q.…”
Section: Bh In 4d El Gravitymentioning
confidence: 97%
“…We should note that QNMs of regular black holes have been studied before [73]- [75]. The behavior of QNMs at the thermodynamics phase transitions has been studied in [76,77]. Moreover, the relation between the QNFs and the thermodynamical quantities at eikonal limit for static solution [78] and for rotating one [79] has been studied.…”
Section: Introductionmentioning
confidence: 99%
“…Our starting point is the following action in which gravity is coupled to nonlinear electrodynamics fields [117,118]…”
Section: Computation Of Weak Lensing By Non Linear Electrodynamics Black Hole Within the Gauss-bonnet Theoremmentioning
confidence: 99%
“…where R denotes the scalar curvature and L(F ) is a function of the invariant F := 1 4 F µν F µν andF := 1 4 F µν F µν built form Faraday tensor F = 1 2 F µν dx µ ∧ dx ν and its Hodge dual F. In this paper, we will deal with the non-linear electrodynamics terms L(F ) are explicitly given by [117,118]…”
Section: Computation Of Weak Lensing By Non Linear Electrodynamics Black Hole Within the Gauss-bonnet Theoremmentioning
confidence: 99%