Microscopic Formulation of Black Holes in String Theory
Justin R. David, Gautam Mandal, Spenta R. Wadia
TL;DR
This work presents a comprehensive microscopic formulation of the five-dimensional D1-D5 black hole within type IIB string theory, anchoring the entropy and Hawking radiation in a dual 1+1D N=(4,4) SCFT on a symmetric product M. By deriving the D1-D5 gauge theory, its Higgs/Higgs-bound state IR fixed point, and the AdS3/CFT2 correspondence, the authors reproduce the Bekenstein-Hawking entropy via Cardy formulas and match Hawking radiation rates to SCFT correlators, with non-renormalization theorems ensuring moduli-independence. The plan connects classical supergravity solutions to microscopic brane dynamics, clarifying the role of near-horizon AdS3×S3×T4 geometry, long-string sectors, and the symmetric-product orbifold, and extends to stringy AdS3 physics and Hawking-Page transitions. The analysis demonstrates a coherent, unitary account of black hole thermodynamics in this setting, offering a concrete realization of holography for a highly supersymmetric, highly controlled black hole system with broad implications for information, entropy counting, and radiation processes. Overall, the paper establishes a robust microscopic bridge between gravity and gauge/gravity duality in the D1-D5 context, providing precise agreements across semiclassical gravity and exact CFT techniques.
Abstract
In this Report we review the microscopic formulation of the five dimensional black hole of type IIB string theory in terms of the D1-D5 brane system. The emphasis here is more on the brane dynamics than on supergravity solutions. We show how the low energy brane dynamics, combined with crucial inputs from AdS/CFT correspondence, leads to a derivation of black hole thermodynamics and the rate of Hawking radiation. Our approach requires a detailed exposition of the gauge theory and conformal field theory of the D1-D5 system. We also discuss some applications of the AdS/CFT correspondence in the context of black hole formation in three dimensions by thermal transition and by collision of point particles.
