2022
DOI: 10.1007/s10714-022-03008-0
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On black hole thermodynamics, singularity, and gravitational entropy

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Cited by 2 publications
(6 citation statements)
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“…Here r H is the radial coordinate at the event horizon, and ℓ 4 is the four-dimensional Planck length. (The extremal case is Q 2 = 4πℓ 2 4 M 2 , so indeed, as claimed above, the (specific) entropy in that case is one quarter of the corresponding Schwarzschild specific entropy, 4πMℓ 2 4 .) It is obvious in this case that the specific entropy is indeed a monotonically decreasing function of the charge, assuming the mass to be fixed.…”
Section: Jhep02(2023)072mentioning
confidence: 61%
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“…Here r H is the radial coordinate at the event horizon, and ℓ 4 is the four-dimensional Planck length. (The extremal case is Q 2 = 4πℓ 2 4 M 2 , so indeed, as claimed above, the (specific) entropy in that case is one quarter of the corresponding Schwarzschild specific entropy, 4πMℓ 2 4 .) It is obvious in this case that the specific entropy is indeed a monotonically decreasing function of the charge, assuming the mass to be fixed.…”
Section: Jhep02(2023)072mentioning
confidence: 61%
“…The celebrated Kerr black hole in the Cygnus X-1 system has many interesting properties. One of the less-discussed of these properties is that the specific entropy (that is, the entropy [1,2] per unit mass) of this black hole has only slightly more than half of the value it would have if it were a Schwarzschild black hole of the same mass. This can be deduced from the formula for the specific entropy of a Kerr black hole (see below) and from the fact that the angular momentum of the Cygnus X-1 black hole is close to the maximum value permitted by Cosmic Censorship: the angular momentum per mass squared (in Planck units), a * , which is unity for an exactly extremal Kerr black hole, is claimed in [3] to be at least 1 0.9696 for Cygnus X-1.…”
Section: Rotation and Black Hole Entropymentioning
confidence: 99%
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