Looking at extremal black holes from very far away
Near-extremal black holes are subject to large quantum effects, which modify their low-temperature thermodynamic behavior. Hitherto, these quantum effects were analyzed by separating the geometry into the near-horizon region and its exterior. It is desirable to understand and reproduce such correcti...
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Main Authors | , , , , |
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Format | Journal Article |
Language | English |
Published |
24.09.2024
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Subjects | |
Online Access | Get full text |
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Summary: | Near-extremal black holes are subject to large quantum effects, which modify
their low-temperature thermodynamic behavior. Hitherto, these quantum effects
were analyzed by separating the geometry into the near-horizon region and its
exterior. It is desirable to understand and reproduce such corrections from the
full higher-dimensional asymptotically flat or AdS geometry's perspective. We
address this question in this article and fill this gap. Specifically, we find
off-shell eigenmodes of the quadratic fluctuation operator of the Euclidean
gravitational dynamics, with eigenvalues that vanish linearly with temperature.
We illustrate this for BTZ and neutral black holes with hyperbolic horizons in
AdS in Einstein-Hilbert theory, and for the charged black holes in
Einstein-Maxwell theory. The linear scaling with Matsubara frequency, which is
a distinctive feature of the modes, together with the fact that their
wavefunctions localize close to the horizon as we approach extremality,
identifies them as responsible for the aforementioned quantum effects. We
provide a contour prescription to deal with the sign indefiniteness of the
Euclidean Einstein-Maxwell action, which we derive to aid our analysis. We also
resolve a technical puzzle regarding modes associated with rotational
isometries in stationary black hole spacetimes. |
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DOI: | 10.48550/arxiv.2409.16248 |