1979
DOI: 10.1103/physrevd.19.2821
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Instability of the Cauchy horizon of Reissner-Nordström black holes

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Cited by 88 publications
(82 citation statements)
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“…The fact that the CFT only appears to describe the region outside the Cauchy horizon may therefore be interpreted as an interesting manifestation of cosmic censorship in the AdS/CFT correspondence. It has previously been argued that violations of strong cosmic censorship in such charged black hole spacetimes are prevented by an instability of the Cauchy horizon: it is a surface of infinite blueshift [17], and is therefore unstable to generic perturbations of the exterior geometry [18]. It is not clear if the fact that the CFT sees the Cauchy horizon as the end of the classical spacetime in rotating black holes is a reflection of this instability, or represents a truly independent mechanism for enforcing cosmic censorship.…”
Section: Introductionmentioning
confidence: 99%
“…The fact that the CFT only appears to describe the region outside the Cauchy horizon may therefore be interpreted as an interesting manifestation of cosmic censorship in the AdS/CFT correspondence. It has previously been argued that violations of strong cosmic censorship in such charged black hole spacetimes are prevented by an instability of the Cauchy horizon: it is a surface of infinite blueshift [17], and is therefore unstable to generic perturbations of the exterior geometry [18]. It is not clear if the fact that the CFT sees the Cauchy horizon as the end of the classical spacetime in rotating black holes is a reflection of this instability, or represents a truly independent mechanism for enforcing cosmic censorship.…”
Section: Introductionmentioning
confidence: 99%
“…The Cauchy horizon has been shown to be both classically [4][5][6][7][8][9] and quantum mechanically unstable [10][11][12].…”
Section: Introductionmentioning
confidence: 99%
“…Building on the initial observation by Penrose [5] that the CH is a surface of infinite gravitational blueshift, it has been demonstrated that the CH is unstable to linear gravitational and electromagnetic perturbations [6,7]. Further investigations have demonstrated that the CH is transformed into a null, scalar curvature singularity when full nonlinear evolution is considered [8][9][10].…”
mentioning
confidence: 99%
“…As above, we wish to determine the flux of radiation measured by an observer crossing the CH, and so must calculate the amplitude F defined in Eq. (6). The part of the amplitude which may be divergent at the CH is…”
mentioning
confidence: 99%