The Fourteenth Marcel Grossmann Meeting 2017
DOI: 10.1142/9789813226609_0189
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Geometries for black hole horizons

Abstract: The application of the blackfold effective theory to the perturbative construction of black holes in higher-dimensions is reviewed. Several solutions with non-trivial horizon geometry and topology are described, such as black helicoidal branes and helicoidal black rings. This hints into a very rich phase diagram for higher-dimensional neutral asymptotically flat black holes.

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Cited by 1 publication
(4 citation statements)
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“…16 On the other hand, the analysis performed here is more accurate for large modes m 1 for which, within this approach and up to second order, no elastic instability is found in any dimension D. This suggests that there is a value of ν that marks the onset for the elastic instability and that due to the requirement (4.7), our analysis is only valid for very thin rings which lie in a region of parameter space below that onset. 17 We observe in the work of [12] that the growth rate of the elastic instability for ν = 0.15 is close to zero, giving some rationale for this interpretation and, in addition, unpublished numerical results [41] substantiate this picture. It may be the case that signatures of the elastic instability appear at third or higher order but to push the blackfold approximation beyond second order is as a daunting task as it is useless since it would require a very high number of derivative corrections, making the effective theory impractical.…”
Section: Discussionsupporting
confidence: 57%
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“…16 On the other hand, the analysis performed here is more accurate for large modes m 1 for which, within this approach and up to second order, no elastic instability is found in any dimension D. This suggests that there is a value of ν that marks the onset for the elastic instability and that due to the requirement (4.7), our analysis is only valid for very thin rings which lie in a region of parameter space below that onset. 17 We observe in the work of [12] that the growth rate of the elastic instability for ν = 0.15 is close to zero, giving some rationale for this interpretation and, in addition, unpublished numerical results [41] substantiate this picture. It may be the case that signatures of the elastic instability appear at third or higher order but to push the blackfold approximation beyond second order is as a daunting task as it is useless since it would require a very high number of derivative corrections, making the effective theory impractical.…”
Section: Discussionsupporting
confidence: 57%
“…Besides having proved to be extremely useful in finding new black hole solutions [14][15][16][17][18] in asymptotically flat space, we demonstrate here that the blackfold approach [7,19] is a powerful tool for studying hydrodynamic (i.e. Gregory-Laflamme) and elastic instabilities of higher-dimensional black holes in the ultraspinning regime and away from it.…”
Section: Introductionmentioning
confidence: 75%
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