One can increase one-quarter the area of a black hole, A/4, to exceed the total thermodynamic entropy, S, by surrounding the hole with a perfectly reflecting shell and adiabatically squeezing it inward. A/4 can be made to exceed S by a factor of order unity before the shell enters the Planck regime, though practical limitations are much more restrictive. One interpretation is that the black hole entropy resides in its thermal atmosphere, and the shell restricts the atmosphere so that its entropy is less than A/4
We argue that the statistical entropy relevant for the thermal interactions of a black hole with its...
As early as 1902, Gibbs pointed out that systems whose partition function diverges, e.g. gravitation...
Using a simple analysis based on the measurement procedure for a quantized area we explain the 1/4 f...
In this paper we calculate the entropy of a thin spherical shell that contracts reversibly from infi...
AbstractBekenstein's generalized second law (GSL) of thermodynamics asserts that the sum of black-ho...
Applying the first and generalised second laws of thermodynamics for a realistic process of near cri...
Black holes have their own thermodynamics including notions of entropy and temperature and versions ...
The many low energy modes near a black hole horizon give the thermal atmosphere a divergent entropy ...
We show that essentially pure classical thermodynamics is sufficient to determine Bekenstein's formu...
Black hole (BH) thermodynamics was established by Bekenstein and Hawking, who made abstract theoreti...
AbstractRecently it is shown that the Bekenstein–Hawking entropy for black holes receives logarithmi...
One of the biggest puzzles in physics today is the reconciliation of quantum mechanics and general r...
Almost all of the entropy in the universe is in the form of Bekenstein-Hawking (BH) entropy of supe...
Black-hole physics mirrors thermodynamics in many respects. In-particular, it is widely believed tha...
Although we have convincing evidence that a black hole bears an entropy proportional to its surface ...
We argue that the statistical entropy relevant for the thermal interactions of a black hole with its...
As early as 1902, Gibbs pointed out that systems whose partition function diverges, e.g. gravitation...
Using a simple analysis based on the measurement procedure for a quantized area we explain the 1/4 f...
In this paper we calculate the entropy of a thin spherical shell that contracts reversibly from infi...
AbstractBekenstein's generalized second law (GSL) of thermodynamics asserts that the sum of black-ho...
Applying the first and generalised second laws of thermodynamics for a realistic process of near cri...
Black holes have their own thermodynamics including notions of entropy and temperature and versions ...
The many low energy modes near a black hole horizon give the thermal atmosphere a divergent entropy ...
We show that essentially pure classical thermodynamics is sufficient to determine Bekenstein's formu...
Black hole (BH) thermodynamics was established by Bekenstein and Hawking, who made abstract theoreti...
AbstractRecently it is shown that the Bekenstein–Hawking entropy for black holes receives logarithmi...
One of the biggest puzzles in physics today is the reconciliation of quantum mechanics and general r...
Almost all of the entropy in the universe is in the form of Bekenstein-Hawking (BH) entropy of supe...
Black-hole physics mirrors thermodynamics in many respects. In-particular, it is widely believed tha...
Although we have convincing evidence that a black hole bears an entropy proportional to its surface ...
We argue that the statistical entropy relevant for the thermal interactions of a black hole with its...
As early as 1902, Gibbs pointed out that systems whose partition function diverges, e.g. gravitation...
Using a simple analysis based on the measurement procedure for a quantized area we explain the 1/4 f...