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What is a chiral 2d CFT? And what does it have to do with extremal black holes?

Vijay Balasubramanian, Jan de Boer, M. M. Sheikh-Jabbari, Joan Simon

TL;DR

This work analyzes the holographic description of near-horizon extremal black holes, showing that the $AdS_2$ throat with electric flux arises as a self-dual orbifold of $AdS_3$ and is dual to a $2d$ CFT subjected to DLCQ. The DLCQ procedure freezes the non-chiral sector, leaving a single chiral Virasoro symmetry and implying no AdS$_2$ dynamics, consistent with stability considerations. The authors connect this to Kerr/CFT, compute the relevant central charge, and argue that chiral CFTs in extremal black hole duals are best understood as DLCQ limits of ordinary $2d$ CFTs, enabling Cardy entropy counting. They discuss two-boundary global versions, AdS$_2$ fragmentation, and directions for explicit bulk–boundary dictionaries and string theory embeddings.

Abstract

The near horizon limit of the extremal BTZ black hole is a``self-dual orbifold'' of AdS_3. This geometry has a null circle on its boundary, and thus the dual field theory is a Discrete Light Cone Quantized (DLCQ) two dimensional CFT. The same geometry can be compactified to two dimensions giving AdS_2 with a constant electric field. The kinematics of the DLCQ show that in a consistent quantum theory of gravity in these backgrounds there can be no dynamics in AdS_2, which is consistent with older ideas about instabilities in this space. We show how the necessary boundary conditions eliminating AdS_2 fluctuations can be implemented, leaving one copy of a Virasoro algebra as the asymptotic symmetry group. Our considerations clarify some aspects of the chiral CFTs appearing in proposed dual descriptions of the near-horizon degrees of freedom of extremal black holes.

What is a chiral 2d CFT? And what does it have to do with extremal black holes?

TL;DR

This work analyzes the holographic description of near-horizon extremal black holes, showing that the throat with electric flux arises as a self-dual orbifold of and is dual to a CFT subjected to DLCQ. The DLCQ procedure freezes the non-chiral sector, leaving a single chiral Virasoro symmetry and implying no AdS dynamics, consistent with stability considerations. The authors connect this to Kerr/CFT, compute the relevant central charge, and argue that chiral CFTs in extremal black hole duals are best understood as DLCQ limits of ordinary CFTs, enabling Cardy entropy counting. They discuss two-boundary global versions, AdS fragmentation, and directions for explicit bulk–boundary dictionaries and string theory embeddings.

Abstract

The near horizon limit of the extremal BTZ black hole is a``self-dual orbifold'' of AdS_3. This geometry has a null circle on its boundary, and thus the dual field theory is a Discrete Light Cone Quantized (DLCQ) two dimensional CFT. The same geometry can be compactified to two dimensions giving AdS_2 with a constant electric field. The kinematics of the DLCQ show that in a consistent quantum theory of gravity in these backgrounds there can be no dynamics in AdS_2, which is consistent with older ideas about instabilities in this space. We show how the necessary boundary conditions eliminating AdS_2 fluctuations can be implemented, leaving one copy of a Virasoro algebra as the asymptotic symmetry group. Our considerations clarify some aspects of the chiral CFTs appearing in proposed dual descriptions of the near-horizon degrees of freedom of extremal black holes.

Paper Structure

This paper contains 7 sections, 65 equations.