There would be a perfect correspondence between the laws of classical thermodynamics and black hole thermodynamics, except for the apparent failure of black hole thermodynamics to correspond to the Third Law. The classical Third Law of Thermodynamics entails that as the absolute temperature, T, approaches zero, the entropy, S, also approaches zero. This discussion is based upon part of the work published by the author in 1995 that demonstrated that the most general form of the classical Third Law of Thermodynamics is satisfied by treating the area of the inner-event horizon as a measure of negative-entropy (negentropy)
For emergent gravity metrics, the presence of dark energy modifies the Hawking temperature. We show ...
AbstractWe find the entropy of Kehagias–Sfetsos black hole in the deformed Hořava–Lifshitz gravity b...
In black hole thermodynamics a cosmological constant contributes a pressure to the equation of stat...
We review and correct the classical critical exponents characterizing the transition from negative t...
We consider Reissner–Nordström black holes surrounded by quintessence where both a non-extremal even...
We reconsider the Kerr metric with cosmological term $\Lambda$ imposing the condition that the angul...
This first part of the series treats the Maxwell equations in the exterior of a slowly rotating Kerr...
We study the dynamical behavior of the BTZ(Banados-Teitelboim-Zanelli) black hole with the low-energ...
In the standard methodology for evaluating the Hawking radiation emanating from a black hole, the ba...
Quantum mechanics around black holes has shown to be one of the most fascinating fields of theoretic...
Interpreting the cosmological constant as a pressure, whose thermodynamically conjugate variable is ...
We introduce a 'quasi-topological` term [1] in D=1+1 dimensions and the entropy for black holes is c...
Five and six dimensional static, spherically symmetric, asymptotically Euclidean black holes, are un...
Hawking radiation is viewed as a tunnelling process. In this way the effect of self-gravitation give...
We study the contribution to entropy of Black Holes in D=2+1 dimensions from an extension of the Che...
For emergent gravity metrics, the presence of dark energy modifies the Hawking temperature. We show ...
AbstractWe find the entropy of Kehagias–Sfetsos black hole in the deformed Hořava–Lifshitz gravity b...
In black hole thermodynamics a cosmological constant contributes a pressure to the equation of stat...
We review and correct the classical critical exponents characterizing the transition from negative t...
We consider Reissner–Nordström black holes surrounded by quintessence where both a non-extremal even...
We reconsider the Kerr metric with cosmological term $\Lambda$ imposing the condition that the angul...
This first part of the series treats the Maxwell equations in the exterior of a slowly rotating Kerr...
We study the dynamical behavior of the BTZ(Banados-Teitelboim-Zanelli) black hole with the low-energ...
In the standard methodology for evaluating the Hawking radiation emanating from a black hole, the ba...
Quantum mechanics around black holes has shown to be one of the most fascinating fields of theoretic...
Interpreting the cosmological constant as a pressure, whose thermodynamically conjugate variable is ...
We introduce a 'quasi-topological` term [1] in D=1+1 dimensions and the entropy for black holes is c...
Five and six dimensional static, spherically symmetric, asymptotically Euclidean black holes, are un...
Hawking radiation is viewed as a tunnelling process. In this way the effect of self-gravitation give...
We study the contribution to entropy of Black Holes in D=2+1 dimensions from an extension of the Che...
For emergent gravity metrics, the presence of dark energy modifies the Hawking temperature. We show ...
AbstractWe find the entropy of Kehagias–Sfetsos black hole in the deformed Hořava–Lifshitz gravity b...
In black hole thermodynamics a cosmological constant contributes a pressure to the equation of stat...