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From Fundamental Strings to Small Black Holes
High Energy Physics - Theory · Submitted 12 Jul 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We give evidence in favour of a string/black hole transition in the case of BPS fundamental string states of the Heterotic string.
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The abstract, sentence by sentence
We give evidence in favour of a string/black hole transition in the case of BPS fundamental string states of the Heterotic string. Our analysis goes beyond the counting of degrees of freedom and considers the evolution of dynamical quantities in the process. As the coupling increases, the string states decrease their size up to the string scale when a small black hole is formed. We compute the absorption cross section for several fields in both the black hole and the perturbative string phases. At zero frequency, these cross sections can be seen as order parameters for the transition. In particular, for the scalars fixed at the horizon the cross section evolves to zero when the black hole is formed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We give evidence in favour of a string/black hole transition in the case of BPS fundamental string states of the Heterotic string. | result 0.78 | 0.91 | 0.88 | hedged possibility 0.72 |
| s1 | Our analysis goes beyond the counting of degrees of freedom and considers the evolution of dynamical quantities in the process. | contribution 0.96 | 0.93 | 0.05 | asserted 0.99 |
| s2 | As the coupling increases, the string states decrease their size up to the string scale when a small black hole is formed. | result 0.99 | 0.79 | 0.31 | asserted 1.00 |
| s3 | We compute the absorption cross section for several fields in both the black hole and the perturbative string phases. | contribution 0.60 | 0.95 | 0.05 | asserted 1.00 |
| s4 | At zero frequency, these cross sections can be seen as order parameters for the transition. | interpretation 0.93 | 0.71 | 0.11 | asserted 0.69 |
| s5 | In particular, for the scalars fixed at the horizon the cross section evolves to zero when the black hole is formed. | result 0.98 | 0.90 | 0.11 | asserted 0.99 |
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The paper
Original abstract
We give evidence in favour of a string/black hole transition in the case of BPS fundamental string states of the Heterotic string. Our analysis goes beyond the counting of degrees of freedom and considers the evolution of dynamical quantities in the process. As the coupling increases, the string states decrease their size up to the string scale when a small black hole is formed. We compute the absorption cross section for several fields in both the black hole and the perturbative string phases. At zero frequency, these cross sections can be seen as order parameters for the transition. In particular, for the scalars fixed at the horizon the cross section evolves to zero when the black hole is formed.
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How the literature uses it
7 arXiv papers cite this in 12 sentences
Papers citing it · 8 sentences without a confident label
Cites it as support 1 paper
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In particular in [ref] , convincing evidence was given in favour of a string/BH transition in dynamical processes of emission and absorption.
Pair Production of small Black Holes in Heterotic String Theories · Conclusions and oulook · 0.97
Cites it as background 3 papers
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The idea of correspondence between black holes and massive string states suggested by Susskind [ref] was elaborated in a number of papers [ref] .
Curvature-corrected dilatonic black holes and black hole -- string transition · Introduction · 0.97
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In the past, a few attempts have been made to study such issues: [ref] , [ref] and especially [ref] , [ref] (see also [ref] ).
Self-interacting fundamental strings and black holes · The String-Black Holes correspondence principle · 0.98
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In the past, a few attempts have been made to study such issues: [ref] , [ref] (see also [ref] ).
Entropy of String States at fixed Mass and Size · The String-Black Holes correspondence principle · 1.00
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