<p>We study quantum corrections in the gravitational path integral around nearly 1/16-BPS black holes in asymptotically <i>AdS</i><sub>5</sub> × <i>S</i><sup>5</sup> space, dual to heavy states in 4D <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N} \)</EquationSource> </InlineEquation> = 4 super Yang-Mills. The analysis provides a gravitational explanation of why 1/16-BPS black holes exhibit an exact degeneracy at large <i>N</i> and why all such states have the same charges, confirming the belief that the superconformal index precisely counts the entropy of extremal black holes. We show the presence of a gap of order <i>N</i><sup>−2</sup> between the 1/16-BPS black holes and the lightest near-BPS black holes within the same charge sector. This is the first example of such a gap for black hole states within the context of <i>AdS</i><sub>5</sub> holography. We also derive the spectrum of near-BPS states that lie above this gap. Our computation relies on finding the correct version of the <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N} \)</EquationSource> </InlineEquation> = 2 super-Schwarzian theory which captures the breaking of the SU(1, 1|1) symmetry when the black hole has finite temperature and non-zero chemical potential. Finally, we comment on possible stringy and non-perturbative corrections that can affect the black hole spectrum.</p>

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BPS and near-BPS black holes in AdS5 and their spectrum in \( \mathcal{N} \) = 4 SYM

  • J. Boruch,
  • M. Heydeman,
  • L. V. Iliesiu,
  • G. J. Turiaci

摘要

We study quantum corrections in the gravitational path integral around nearly 1/16-BPS black holes in asymptotically AdS5 × S5 space, dual to heavy states in 4D N \( \mathcal{N} \) = 4 super Yang-Mills. The analysis provides a gravitational explanation of why 1/16-BPS black holes exhibit an exact degeneracy at large N and why all such states have the same charges, confirming the belief that the superconformal index precisely counts the entropy of extremal black holes. We show the presence of a gap of order N−2 between the 1/16-BPS black holes and the lightest near-BPS black holes within the same charge sector. This is the first example of such a gap for black hole states within the context of AdS5 holography. We also derive the spectrum of near-BPS states that lie above this gap. Our computation relies on finding the correct version of the N \( \mathcal{N} \) = 2 super-Schwarzian theory which captures the breaking of the SU(1, 1|1) symmetry when the black hole has finite temperature and non-zero chemical potential. Finally, we comment on possible stringy and non-perturbative corrections that can affect the black hole spectrum.