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The Charged Black Hole/String Transition
High Energy Physics - Theory · Submitted 24 Oct 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim For the two dimensional charged black hole, which is described by an exactly solvable worldsheet theory, a transition from the black hole to the string phase occurs when the Hawking temperature of the black hole reaches a limiting value, the temperature of free strings with the same mass and charge.
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We generalize the discussion of hep-th/0509170 to charged black holes. For the two dimensional charged black hole, which is described by an exactly solvable worldsheet theory, a transition from the black hole to the string phase occurs when the Hawking temperature of the black hole reaches a limiting value, the temperature of free strings with the same mass and charge. At this point a tachyon winding around Euclidean time in the Euclidean black hole geometry, which has a non-zero condensate, becomes massless at infinity, and the horizon of the black hole is infinitely smeared. For Reissner-Nordstrom black holes in d\ge 4 dimensions, the exact worldsheet CFT is not known, but we propose that it has similar properties. We check that the leading order solution is in good agreement with this proposal, and discuss the expected form of \alpha' corrections.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We generalize the discussion of hep-th/0509170 to charged black holes. | contribution 0.86 | 0.81 | 0.06 | asserted 0.93 |
| s1 | For the two dimensional charged black hole, which is described by an exactly solvable worldsheet theory, a transition from the black hole to the string phase occurs when the Hawking temperature of the black hole reaches a limiting value, the temperature of free strings with the same mass and charge. | result 0.96 | 0.60 | 0.70 | asserted 1.00 |
| s2 | At this point a tachyon winding around Euclidean time in the Euclidean black hole geometry, which has a non-zero condensate, becomes massless at infinity, and the horizon of the black hole is infinitely smeared. | result 0.84 | 0.53 | 0.19 | asserted 1.00 |
| s3 | For Reissner-Nordstrom black holes in d\ge 4 dimensions, the exact worldsheet CFT is not known, but we propose that it has similar properties. | limitation 0.42 | 0.38 | 0.11 | speculative 0.64 |
| s4 | We check that the leading order solution is in good agreement with this proposal, and discuss the expected form of \alpha' corrections. | result 0.53 | 0.92 | 0.12 | asserted 0.91 |
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Original abstract
We generalize the discussion of hep-th/0509170 to charged black holes. For the two dimensional charged black hole, which is described by an exactly solvable worldsheet theory, a transition from the black hole to the string phase occurs when the Hawking temperature of the black hole reaches a limiting value, the temperature of free strings with the same mass and charge. At this point a tachyon winding around Euclidean time in the Euclidean black hole geometry, which has a non-zero condensate, becomes massless at infinity, and the horizon of the black hole is infinitely smeared. For Reissner-Nordstrom black holes in d\ge 4 dimensions, the exact worldsheet CFT is not known, but we propose that it has similar properties. We check that the leading order solution is in good agreement with this proposal, and discuss the expected form of \alpha' corrections.
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References
How the literature uses it
12 arXiv papers cite this in 19 sentences
Papers citing it · 14 sentences without a confident label
Compares with it 1 paper
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(2.26) of [ref] .
Solvable time-like cosets and holography beyond $AdS$ · Thermodynamics of $SL(2,ℝ)×U(1) / U(1)$ · 0.97
Cites it as background 3 papers
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In the near-horizon geometry of the coincident fivebranes, the three-charge black holes are described by certain BPS black hole solutions in an asymptotically linear dilaton spacetime, which carry the charges $(P,W)$; see e.g. [ref] and references therein.
Three-Charge Black Holes and Quarter BPS States in Little String Theory · Introduction · 0.88
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When $β∼l_s$, it is widely believed that the black hole transitions into a state of highly excited fundamental strings [ref] (see also [ref] for relevant works).
Phases of String Stars in the Presence of a Spatial Circle · Introduction and summary · 0.81
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Familiar examples include the $SL(2,ℝ)/U(1)$ string black hole [ref] , the CGHS model [ref] , and charged string backgrounds [ref] .
Thermodynamic Regulation of Superradiance in a Charged Two-Dimensional Black Hole · Introduction · 0.99
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