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Quantizing N=2 Multicenter Solutions

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arxiv 0807.4556 v1 pith:FKSZH3BN submitted 2008-07-29 hep-th

Quantizing N=2 Multicenter Solutions

classification hep-th
keywords solutionsquantumallowsblackboundcentersdimensionseffects
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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N=2 supergravity in four dimensions, or equivalently N=1 supergravity in five dimensions, has an interesting set of BPS solutions that each correspond to a number of charged centers. This set contains black holes, black rings and their bound states, as well as many smooth solutions. Moduli spaces of such solutions carry a natural symplectic form which we determine, and which allows us to study their quantization. By counting the resulting wavefunctions we come to an independent derivation of some of the wall-crossing formulae. Knowledge of the explicit form of these wavefunctions allows us to find quantum resolutions to some apparent classical paradoxes such as solutions with barely bound centers and those with an infinitely deep throat. We show that quantum effects seem to cap off the throat at a finite depth and we give an estimate for the corresponding mass gap in the dual CFT. This is an interesting example of a system where quantum effects cannot be neglected at macroscopic scales even though the curvature is everywhere small.

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Cited by 3 Pith papers

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  1. Black Hole Quantum Mechanics and Generalized Error Functions

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    Derives the general non-holomorphic completion for arbitrary n-center BPS black hole indices using localization on the refined Witten index in supersymmetric quantum mechanics, yielding generalized error functions fro...

  2. On conformal symmetry in large-$N$ quiver mechanics

    hep-th 2026-07 conditional novelty 6.0

    At large rank N, the fixed-point formula for the quiver superconformal index equals the Ω_uneq contribution to the microscopic scaling BPS index of Beaujard–Mondal–Pioline, a piece previously invisible on the Coulomb branch.

  3. Pure D-brane Black Holes: BPS Counting and non-BPS Vacua

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    The (1,1,1,5) and (1,1,1,6) D2-D2-D2-D6 BPS systems yield 2032 and 5616 vacua, matching U-duality, while the analogous non-BPS system has no zero-energy vacua and six doubly-degenerate low-energy minima.