Abstract

Although BMPV black holes in flat space and in Taub-NUT space have identical near-horizon geometries, they have different indices from the microscopic analysis. For K3 compactification of type IIB theory, Sen et al. in a series of papers identified that the key to resolving this puzzle is the black hole hair modes: smooth, normalisable, bosonic and fermionic degrees of freedom living outside the horizon. In this paper, we extend their study to N = 4 CHL orbifold models. For these models, the puzzle is more challenging due to the presence of the twisted sectors. We identify hair modes in the untwisted as well as twisted sectors. We show that after removing the contributions of the hair modes from the microscopic partition functions, the 4d and 5d horizon partition functions agree. Special care is taken to present details on the smoothness analysis of hair modes for rotating black holes, thereby filling an essential gap in the literature.

Highlights

  • Charge limit string theory gives a perfect match with the Bekenstein-Hawking entropy of the corresponding black hole in the two-derivative theory

  • We show that after removing the contributions of the hair modes from the microscopic partition functions, the 4d and 5d horizon partition functions agree

  • We identify hair modes in the untwisted as well as twisted sectors and show that after removing the contributions of the hair modes from the microscopic partition functions, the 4d and 5d horizon partition functions perfectly match

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Summary

Supergravity set-up

We present relevant details on (2,0) supergravity coupled to nt number of tensor multiplets. If we consider pure (2, 0) theory coupled to nt tensor multiplets, we have the field content: a graviton, 4 left chiral gravitinos, 5 self-dual two-forms, nt anti-selfdual two-forms, 4nt fermions, and 5nt scalars. For the backgrounds we will work with, the scalars are set to constant values and the spin-1/2 fermions χαr are all set to zero With these conditions, the fermion sector field equations of motion simplify to ΓMNP DN ΨαP − HkMNP ΓN ΓkαβΨβP = 0, HsMNP ΓMN ΨαP = 0,. To discuss supersymmetry of black holes with hair, we will need the Killing spinor equations when the gravitino fields and the anti-self-dual fields are not set to zero.

BMPV black hole in flat space
Killing spinors
Smooth coordinates near the future horizon
Deformations of the BMPV black hole
Bosonic deformations generated by Garfinkle-Vachaspati transform
Fermionic deformations
BMPV black hole in Taub-NUT space
Deformations of the BMPV black hole in Taub-NUT space
Two-form field deformations
Hair removed 4d and 5d partition functions
Hair partition functions
Discussion
A The notion of weight
B Action of Lorentz boosts and null rotations on gravitino configurations
Full Text
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