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Massless radiation from heavy rotating string and Kerr/string correspondence
High Energy Physics - Theory · Submitted 9 Sep 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We also argue based on these quantities the Horowitz-Polchinski correspondence principle between rotating strings/Kerr black holes for non-extremal as well as extremal cases.
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The abstract, sentence by sentence
We calculate emission rates of a massless state from a highly excited rotating string in perturbative bosonic open string theory. By averaging huge degeneracies of initial string states with specifying the mass and a single component of the angular momentum, we find thermal spectrum in a wide range of the angular momentum. We derive the temperature that characterizes the thermal spectrum from the partition function of a single rotating string from which we also find the entropy and the angular velocity of rotating strings. We also argue based on these quantities the Horowitz-Polchinski correspondence principle between rotating strings/Kerr black holes for non-extremal as well as extremal cases. In the parameter region where the Kerr black holes exist, the thermal spectrum is comparable to scalar emissions from a rotating black hole.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We calculate emission rates of a massless state from a highly excited rotating string in perturbative bosonic open string theory. | contribution 0.99 | 0.96 | 0.08 | asserted 1.00 |
| s1 | By averaging huge degeneracies of initial string states with specifying the mass and a single component of the angular momentum, we find thermal spectrum in a wide range of the angular momentum. | result 0.87 | 0.96 | 0.22 | asserted 1.00 |
| s2 | We derive the temperature that characterizes the thermal spectrum from the partition function of a single rotating string from which we also find the entropy and the angular velocity of rotating strings. | result 0.56 | 0.97 | 0.11 | asserted 1.00 |
| s3 | We also argue based on these quantities the Horowitz-Polchinski correspondence principle between rotating strings/Kerr black holes for non-extremal as well as extremal cases. | interpretation 0.96 | 0.77 | 0.51 | hedged possibility 0.56 |
| s4 | In the parameter region where the Kerr black holes exist, the thermal spectrum is comparable to scalar emissions from a rotating black hole. | result 0.78 | 0.73 | 0.20 | asserted 0.82 |
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The paper
Original abstract
We calculate emission rates of a massless state from a highly excited rotating string in perturbative bosonic open string theory. By averaging huge degeneracies of initial string states with specifying the mass and a single component of the angular momentum, we find thermal spectrum in a wide range of the angular momentum. We derive the temperature that characterizes the thermal spectrum from the partition function of a single rotating string from which we also find the entropy and the angular velocity of rotating strings. We also argue based on these quantities the Horowitz-Polchinski correspondence principle between rotating strings/Kerr black holes for non-extremal as well as extremal cases. In the parameter region where the Kerr black holes exist, the thermal spectrum is comparable to scalar emissions from a rotating black hole.
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How the literature uses it
5 arXiv papers cite this in 8 sentences
Papers citing it · 5 sentences without a confident label
Uses its data or values 1 paper
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Also, in $J=O(M^2)$, $J$ should not be too close to $M^2$ for the approximation to be valid.] [equation] where the precise value of $c$ can be found in [ref] .
The correspondence between rotating black holes and fundamental strings · Sizes, shapes and degeneracies · 0.80
Cites it as background 2 papers
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Especially the detailed analysis of the Kerr black hole, which is astronomically the most familiar one, is not yet completed, though there are some proposals in this direction [ref] .
On Non-Chiral Extension of Kerr/CFT · Introduction · 0.91
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Some other applications of this procedure for the cross section of strings are found in [ref] .
Emission spectrum of soft massless states from heavy superstring · Introduction · 0.88
What it cites · 11 sentences without a confident label
Builds on 1 paper
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In this appendix, we shall demonstrate a calculation of the traces in Eqs. [ref], [ref], extending the calculation performed in [ref] .
Production cross section of rotating string · Calculation of traces · 0.99
Cites as support 3 papers
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This is indeed the case for the size of a string and a black hole [ref] .[The size of a highly excited string can be estimated by a random walk picture which provides $√(M)$, on the other hand the size of a black hole becomes on the order one at the correspondence point.
Self-interacting fundamental strings and black holes · The correspondence · 0.97
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This is indeed the case for the size of a string and a black hole [ref] .[The size of a highly excited string can be estimated by a random walk picture which provides $√(M)$, on the other hand the size of a black hole becomes on the order one at the correspondence point.
Self Gravitating Fundamental Strings · The correspondence · 0.97
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This is indeed the case for the size of a string and a black hole [ref] .[The size of a highly excited string can be estimated by a random walk picture which provides $√(M)$, on the other hand the size of a black hole becomes on the order one at the correspondence point.
Self-gravitating fundamental strings and black-holes · The correspondence · 0.97
Cites as background 8 papers
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The case of maximum angular momentum $J = N$ has been studied in [ref] etc.
Decay of long-lived massive closed superstring states: Exact results · Emission of massless states from rotating string · 0.81
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The case of maximum angular momentum $J = N$ has been studied in [ref] etc.
The decay of massive closed superstrings with maximum angular momentum · Emission of massless states from rotating string · 0.81
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The case of maximum angular momentum $J = N$ has been studied in [ref] etc.
Semiclassical decay of strings with maximum angular momentum · Emission of massless states from rotating string · 0.81
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