2017
DOI: 10.1007/jhep05(2017)094
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On the black hole interior in string theory

Abstract: Abstract:The potential behind the horizon of an eternal black hole in classical theories is described in terms of data that is available to an external observer -the reflection coefficient of a wave that scatters on the black hole. In GR and perturbative string theory (in α ), the potential is regular at the horizon and it blows up at the singularity. The exact reflection coefficient, that is known for the SL(2, R) k /U(1) black hole and includes nonperturbative α effects, seems however to imply that there is … Show more

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Cited by 10 publications
(15 citation statements)
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“…This conclusion seems to fit neatly with claims made in [8,3] that the potential associated with the SL(2, R) k /U (1) BH blows up just behind the horizon. The unusual properties of (10) suggests that its backreaction is likely to be non-standard and could drastically modify the BH interior.…”
supporting
confidence: 78%
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“…This conclusion seems to fit neatly with claims made in [8,3] that the potential associated with the SL(2, R) k /U (1) BH blows up just behind the horizon. The unusual properties of (10) suggests that its backreaction is likely to be non-standard and could drastically modify the BH interior.…”
supporting
confidence: 78%
“…Outside the SL(2, R) k /U (1) BH the operator O is positive while inside the BH it is negative. Some indirect evidence from the exact reflection coefficient of [7] was provided that the SL(2, R) k /U (1) BH interior is not empty in classical string theory [8,3]. These papers, however, did not explain how come the SL(2, R) k /U (1) BH is not empty or what it is filled with.…”
mentioning
confidence: 99%
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“…To understand the limitations of such a procedure, a concrete avenue would be to further investigate strings on the SL(2, R)/U (1) cigar background, which has Rindler space as a parametric limit (see e.g. [37,[66][67][68][69][70][71][72][73][74]).…”
Section: Resultsmentioning
confidence: 99%