pith. sign in

arxiv: 2411.12413 · v3 · pith:5SLOY553new · submitted 2024-11-19 · ✦ hep-th · gr-qc

Attractor saddle for 5D black hole index

Pith reviewed 2026-05-23 08:38 UTC · model grok-4.3

classification ✦ hep-th gr-qc
keywords saddlesolutionblackformholeindexsupersymmetricanupam
0
0 comments X

The pith

The non-extremal saddle for the 5D BMPV black hole index is expressed in canonical harmonic-function form on a flat base, establishing supersymmetry and the new attractor property.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The work takes a complex finite-temperature solution previously built by another group for the supersymmetric index of a five-dimensional black hole with three charges. That solution saturates the BPS bound in the classical limit. The authors recast the same geometry using three harmonic functions defined on ordinary flat three-dimensional space. In this language the Killing spinor equations become manifestly satisfied, proving the configuration is supersymmetric. The same rewriting also makes visible an attractor mechanism in which the scalar fields flow to fixed values at the horizon independent of their asymptotic values. Because the base is flat, the construction stays within the standard five-dimensional supergravity framework without introducing new fields or dimensions. The result therefore supplies an explicit, checkable representative of the saddle that contributes to the black-hole index.

Core claim

We write this solution in a canonical form in terms of harmonic functions on three-dimensional flat base space, thereby showing that it is supersymmetric. We also show that it exhibits the new form of attraction.

Load-bearing premise

The solution constructed in arXiv:2308.00038 is the correct non-extremal saddle that saturates the BPS bound and reproduces the supersymmetric index in the classical limit; the present rewriting inherits all properties of that prior construction.

read the original abstract

In a recent paper, Anupam, Chowdhury, and Sen [arXiv:2308.00038] constructed the non-extremal saddle that reproduces the supersymmetric index of the BMPV black hole with three independent charges in the classical limit. This saddle solution is a finite temperature complex solution saturating the BPS bound. In this paper, we write this solution in a canonical form in terms of harmonic functions on three-dimensional flat base space, thereby showing that it is supersymmetric. We also show that it exhibits the new form of attraction.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The paper relies on the existence and uniqueness properties of harmonic functions on flat 3D space, the standard Killing-spinor equations of 5D N=2 supergravity, and the correctness of the saddle constructed in the referenced work. No new free parameters or invented entities are introduced in the abstract.

axioms (2)
  • standard math Harmonic functions on flat 3D Euclidean space satisfy the Laplace equation and generate supersymmetric solutions when used as building blocks for the metric and gauge fields.
    Invoked when the solution is rewritten in canonical harmonic-function form.
  • domain assumption The non-extremal saddle of arXiv:2308.00038 saturates the BPS bound and reproduces the supersymmetric index in the classical limit.
    The present work inherits all physical properties from that prior construction.

pith-pipeline@v0.9.0 · 5625 in / 1427 out tokens · 34095 ms · 2026-05-23T08:38:02.160346+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Non-supersymmetric F1-P black rings

    hep-th 2026-01 unverdicted novelty 7.0

    Singly and doubly spinning non-supersymmetric F1-P black ring solutions are constructed in 5D supergravity, with the doubly spinning case admitting an extremal limit where entropy S equals 2 pi times the S^2 angular m...

Reference graph

Works this paper leans on

30 extracted references · 30 canonical work pages · cited by 1 Pith paper · 10 internal anchors

  1. [1]

    Microscopic origin of the Bek enstein-Hawking entropy,

    A. Strominger and C. Vafa, “Microscopic origin of the Bek enstein-Hawking entropy,” Phys. Lett. B 379, 99-104 (1996) doi:10.1016/0370-2693(96)00345-0 [arXiv :hep- th/9601029 [hep-th]]

  2. [2]

    Black Hole Entropy Function, Attractors and Precision Counting of Microstates

    A. Sen, “Black Hole Entropy Function, Attractors and Pre cision Counting of Mi- crostates,” Gen. Rel. Grav. 40, 2249-2431 (2008) doi:10.1007/s10714-008-0626-4 [arXiv:0708.1270 [hep-th]]

  3. [3]

    Supersymmet ric indices factorize,

    L. V. Iliesiu, M. Kologlu and G. J. Turiaci, “Supersymmet ric indices factorize,” JHEP 05 (2023), 032 doi:10.1007/JHEP05(2023)032 [arXiv:2107.09 062 [hep-th]]

  4. [4]

    Maggiore, J

    M. Heydeman, L. V. Iliesiu, G. J. Turiaci and W. Zhao, “The statistical mechan- ics of near-BPS black holes,” J. Phys. A 55 (2022) no.1, 014004 doi:10.1088/1751- 8121/ac3be9 [arXiv:2011.01953 [hep-th]]

  5. [5]

    Mi croscopic origin of the Bekenstein-Hawking entropy of supersymmetric AdS 5 black holes,

    A. Cabo-Bizet, D. Cassani, D. Martelli and S. Murthy, “Mi croscopic origin of the Bekenstein-Hawking entropy of supersymmetric AdS 5 black holes,” JHEP 10 (2019), 062 doi:10.1007/JHEP10(2019)062 [arXiv:1810.11442 [hep -th]]

  6. [6]

    New forms of attraction: Attractor saddles for the black hole index,

    J. Boruch, L. V. Iliesiu, S. Murthy and G. J. Turiaci, “New forms of attraction: Attractor saddles for the black hole index,” [arXiv:2310.0 7763 [hep-th]]

  7. [7]

    Killing spinors for finite tempe rature Euclidean so- lutions at the BPS bound,

    S. Hegde and A. Virmani, “Killing spinors for finite tempe rature Euclidean so- lutions at the BPS bound,” JHEP 02, 203 (2024) doi:10.1007/JHEP02(2024)203 [arXiv:2311.09427 [hep-th]]. 19

  8. [8]

    S upersymmetric in- dex for small black holes,

    C. Chowdhury, A. Sen, P. Shanmugapriya and A. Virmani, “S upersymmetric in- dex for small black holes,” JHEP 04 (2024), 136 doi:10.1007/JHEP04(2024)136 [arXiv:2401.13730 [hep-th]]

  9. [9]

    Gravitational inde x of the heterotic string,

    Y. Chen, S. Murthy and G. J. Turiaci, “Gravitational inde x of the heterotic string,” JHEP 09 (2024), 041 doi:10.1007/JHEP09(2024)041 [arXiv:2402.03 297 [hep-th]]

  10. [10]

    Logarith mic correction to BPS black hole entropy from supersymmetric index at finite tempe rature,

    A. A. H., P. V. Athira, C. Chowdhury and A. Sen, “Logarith mic correction to BPS black hole entropy from supersymmetric index at finite tempe rature,” JHEP 03 (2024), 095 doi:10.1007/JHEP03(2024)095 [arXiv:2306.07 322 [hep-th]]

  11. [11]

    Revisiting logar ithmic correc- tion to five dimensional BPS black hole entropy,

    A. H. Anupam, C. Chowdhury and A. Sen, “Revisiting logar ithmic correc- tion to five dimensional BPS black hole entropy,” JHEP 05, 070 (2024) doi:10.1007/JHEP05(2024)070 [arXiv:2308.00038 [hep-th ]]

  12. [12]

    Supe rsymmetric Index for Half BPS Black Holes in N=2 Supergravity with Higher Curvatu re Corrections,

    S. Hegde, A. Sen, P. Shanmugapriya and A. Virmani, “Supe rsymmetric Index for Half BPS Black Holes in N=2 Supergravity with Higher Curvatu re Corrections,” [arXiv:2411.08260 [hep-th]]

  13. [13]

    Localization of the 5D supergravity action and Euclidean saddles for the black hole index,

    D. Cassani, A. Ruip´ erez and E. Turetta, “Localization of the 5D supergravity action and Euclidean saddles for the black hole index,” [arXiv:240 9.01332 [hep-th]]

  14. [14]

    All supersymmetric solutions of minimal supergravity in five dimensions

    J. P. Gauntlett, J. B. Gutowski, C. M. Hull, S. Pakis and H . S. Reall, “All supersym- metric solutions of minimal supergravity in five- dimension s,” Class. Quant. Grav. 20, 4587-4634 (2003) doi:10.1088/0264-9381/20/21/005 [arXi v:hep-th/0209114 [hep-th]]

  15. [15]

    One Ring to Rule Them All ... and in the Darkness Bind Them?

    I. Bena and N. P. Warner, “One ring to rule them all ... and in the darkness bind them?,” Adv. Theor. Math. Phys. 9, no.5, 667-701 (2005) doi:10.4310/ATMP.2005.v9.n5.a1 [arXiv:hep-th/0408106 [hep-th]]

  16. [16]

    General concentric black rings,

    J. P. Gauntlett and J. B. Gutowski, “General concentric black rings,” Phys. Rev. D 71, 045002 (2005) doi:10.1103/PhysRevD.71.045002 [arXiv:h ep-th/0408122 [hep- th]]

  17. [17]

    Bubbling supertubes and foami ng black holes,

    I. Bena and N. P. Warner, “Bubbling supertubes and foami ng black holes,” Phys. Rev. D 74, 066001 (2006) doi:10.1103/PhysRevD.74.066001 [arXiv:h ep-th/0505166 [hep-th]]. 20

  18. [18]

    Black holes, black rings and th eir microstates,

    I. Bena and N. P. Warner, “Black holes, black rings and th eir microstates,” Lect. Notes Phys. 755, 1-92 (2008) doi:10.1007/978-3-540-79523-0 1 [arXiv:hep- th/0701216 [hep-th]]

  19. [19]

    General Rotating Five Dimensional Black Holes of Toroidally Compactified Heterotic String

    M. Cvetic and D. Youm, “General rotating five-dimension al black holes of toroidally compactified heterotic string,” Nucl. Phys. B 476, 118-132 (1996) doi:10.1016/0550- 3213(96)00355-0 [arXiv:hep-th/9603100 [hep-th]]

  20. [20]

    General Nonextremal Rotating Charged AdS Black Holes in Five-dimensional $U(1)^3$ Gauged Supergravity: A Simple Construction Method

    S. Q. Wu, “General Nonextremal Rotating Charged AdS Bla ck Holes in Five- dimensional U(1)3 Gauged Supergravity: A Simple Construction Method,” Phys. Lett. B 707, 286-291 (2012) doi:10.1016/j.physletb.2011.12.031 [ar Xiv:1108.4159 [hep-th]]

  21. [21]

    Black Hole Entropy, Special Geometry and Strings

    T. Mohaupt, “Black hole entropy, special geometry and s trings,” Fortsch. Phys. 49, 3-161 (2001) doi:10.1002/1521-3978(200102)49:1/3<3::AID-PROP3>3.0.CO;2-# [arXiv:hep-th/0007195 [hep-th]]

  22. [22]

    Subtracted Geometry From Harrison Transformations

    A. Virmani, “Subtracted Geometry From Harrison Transf ormations,” JHEP 07, 086 (2012) doi:10.1007/JHEP07(2012)086 [arXiv:1203.5088 [h ep-th]]

  23. [23]

    Stationary BPS Solutions in N=2 Supergravity with R^2-Interactions

    G. Lopes Cardoso, B. de Wit, J. Kappeli and T. Mohaupt, “S tationary BPS solutions in N=2 supergravity with R**2 interactions,” JHEP 12 (2000), 019 doi:10.1088/1126- 6708/2000/12/019 [arXiv:hep-th/0009234 [hep-th]]

  24. [24]

    Stationary solutio ns of N=2 supergravity,

    K. Behrndt, D. Lust and W. A. Sabra, “Stationary solutio ns of N=2 supergravity,” Nucl. Phys. B 510 (1998), 264-288 doi:10.1016/S0550-3213(97)00633-0 [arX iv:hep- th/9705169 [hep-th]]

  25. [25]

    New connections b etween 4-D and 5-D black holes,

    D. Gaiotto, A. Strominger and X. Yin, “New connections b etween 4-D and 5-D black holes,” JHEP 02, 024 (2006) doi:10.1088/1126-6708/2006/02/024 [arXiv:h ep- th/0503217 [hep-th]]

  26. [26]

    Supersymmetric Completion of an R^2 Term in Five-Dimensional Supergravity

    K. Hanaki, K. Ohashi and Y. Tachikawa, “Supersymmetric Completion of an R**2 term in Five-dimensional Supergravity,” Prog. Theor. Phys. 117, 533 (2007) doi:10.1143/PTP.117.533 [arXiv:hep-th/0611329 [hep-th ]]

  27. [27]

    The Off-Shell 4D/ 5D Connection,

    N. Banerjee, B. de Wit and S. Katmadas, “The Off-Shell 4D/ 5D Connection,” JHEP 03, 061 (2012) doi:10.1007/JHEP03(2012)061 [arXiv:1112.53 71 [hep-th]]. 21

  28. [28]

    Supersymmetry, Localization and Quantum Entropy Function

    N. Banerjee, S. Banerjee, R. K. Gupta, I. Mandal and A. Se n, “Supersym- metry, Localization and Quantum Entropy Function,” JHEP 02, 091 (2010) doi:10.1007/JHEP02(2010)091 [arXiv:0905.2686 [hep-th] ]

  29. [29]

    Black hole mi crostate counting from the gravitational path integral,

    L. V. Iliesiu, S. Murthy and G. J. Turiaci, “Black hole mi crostate counting from the gravitational path integral,” [arXiv:2209.13602 [hep-th ]]

  30. [30]

    Revisiting localization for BPS black hole ent ropy,

    A. Sen, “Revisiting localization for BPS black hole ent ropy,” [arXiv:2302.13490 [hep- th]]. 22