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Anti de Sitter Black Holes

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Anti de Sitter Black Holes Harvey Reall University of Nottingham Motivation Black hole entropy calculations all rely on 2d CFT Can we use AdS/CFT to calculate entropy ... – PowerPoint PPT presentation

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Title: Anti de Sitter Black Holes


1
Anti de Sitter Black Holes
  • Harvey Reall
  • University of Nottingham

2
Motivation
  • Black hole entropy calculations all rely on 2d
    CFT
  • Can we use AdS/CFT to calculate entropy of Dgt3
    AdS black holes?
  • D4 probably not, CFT not understood
  • D5 CFT is N4 SYM
  • Need supersymmetric AdS5 black holes to evade
    strong coupling problem

3
Plan
  • SUSY asymptotically flat black holes
  • SUSY AdS black holes in D3,4
  • SUSY AdS black holes in D5
  • CFT interpretation
  • Collaborators J. Gutowski, R. Roiban, H.
    Kunduri, J. Lucietti

4
SUSY 5D black holesHSR 02, Gutowski 04
  • 5D ungauged N1 sugra abelian vectors
  • Introduce coordinates adapted to horizon
  • Take near-horizon limit
  • Impose supersymmetry eqs on spatial
    cross-section of horizon
  • Can determine general solution for compact
    horizon

5
SUSY 5D black holesHSR 02, Gutowski 04
  • All possible near-horizon geometries
  • Which arise from asymp flat black holes?
  • Near-horizon BMPV from BMPV!
  • AdS3xS2 from BPS black rings Elvang et al 04
  • Flat T3 horizon unlikely Galloway 06

Near-horizon Horizon geometry
BMPV Squashed S3
AdS3 x S2 S1 x S2
Flat T3
6
SUSY AdS Black Holes
  • BPS limit of Reissner-Nordstrom-AdS is nakedly
    singular
  • D3 BTZ is SUSY black hole iff MJgt0
  • D4 Kerr-Newman-AdS (M,J,Q,P) saturates BPS
    bound if MM(Q), JJ(Q), P0 Kostalecky Perry
    95, Caldarelli Klemm 98
  • SUSY AdS black holes must rotate

7
5D SUSY AdS black holesGutowski HSR 04
  • Reduce IIB SUGRA on S5 to N1 D5 U(1)3 gauged
    SUGRA Cvetic et al 99
  • Canonical form for SUSY solutions involves
    specifying 4d Kähler base space Gauntlett
    Gutowski 03, Gutowski HSR 04
  • Choice of base space not obvious e.g. get AdS5
    from Bergman manifold SU(2,1)/U(2)

8
5D SUSY AdS black holesGutowski HSR 04
  • Seek SUSY black holes systematically by examining
    near-horizon geometry
  • In near-horizon limit, conditions for SUSY are
    equations on 3-manifold
  • General solution not known
  • Particular homogeneous S3 solution can be found
    (cf near-horizon BMPV)

9
5D SUSY AdS black holesGutowski HSR 04
  • Near-horizon solution motivates cohomogeneity-1
    Ansatz for full solution
  • First examples of SUSY AdS5 black holes!
  • Base space singular, cohomogeneity-1,
    asymptotically Bergman space
  • 1/16 BPS

10
Unequal Angular MomentaChong, Cvetic, Lü Pope
05
  • Guessed non-BPS charged rotating black hole
    solution of minimal gauged sugra
    (Einstein-Maxwell)
  • Cohomogeneity-2, 4 parameters (M,J1,J2,Q)
  • BPS limit 2 parameter solution with J1?J2

11
General solutionKunduri, Lucietti HSR 06
  • Determine base space of BPS solution of minimal
    gauged sugra singular, cohomogeneity-2,
    asymptotically Bergman
  • Plug into BPS eqs of U(1)3 gauged sugra, solve
  • BPS solution parametrized by J1, J2, Q1, Q2, Q3
    with one constraint
  • Expect non-BPS generalization with independent
    M,J,Q (2 more parameters)

12
CFT description
  • BPS AdS5 black hole microstates are 1/16 BPS
    states of N4 large N SYM on RxS3 (equivalently
    BPS local operators on R4)
  • States classified by SO(4)xSO(6) quantum numbers
    J,Q
  • Black hole quantum numbers O(N2)
  • Black hole entropy O(N2)
  • Entropy calculation count all 1/16 BPS states
    with same quantum numbers as black hole

13
A Puzzle
  • 1/16 BPS states have independent J,Q
  • Why do BPS black holes have a constraint relating
    J,Q?
  • Is there a more general family of SUSY black
    holes with independent J,Q?
  • But corresponding non-SUSY solution would need
    more than just conserved charges to specify it
  • BPS AdS black rings?

14
BPS AdS black rings?Kunduri, Lucietti HSR 06
  • Most general BPS near-horizon geometry in 5D
    gauged sugra not known
  • Assume existence of 2 rotational symmetries (true
    for all known 5d black holes) problem reduces to
    ODEs. 2 interesting solutions.
  • One solution is near-horizon geometry of known S3
    black holes
  • Another solution is a warped product AdS3xS2 with
    horizon topology S1xS2

15
BPS AdS black rings?Kunduri, Lucietti HSR 06
  • but with a conical singularity on S2
  • Cant eliminate singularity (without turning off
    cosmological constant)
  • BPS AdS black rings with 2 rotational symmetries
    do not exist
  • Oxidize to 10d warped product AdS3xM7 with
    M7S2xS5 (singular)

16
New 10d black holes?
  • Solution is locally isometric to AdS3xM7 solution
    of Gauntlett et al 06
  • They showed that solution can be made globally
    regular by choosing topology of M7 appropriately
    (not S2xS5)
  • Resulting solution cannot be reduced to 5d
  • Could this be near-horizon geometry of an
    asymptotically AdS5xS5 black hole?

17
Resolutions of the puzzle?
  • Are there BPS 10d black hole solutions that cant
    be reduced to 5d?
  • Are there BPS 5d black holes without 2 rotational
    symmetries?
  • Non-abelian BPS black holes?
  • Maybe we know most general black hole. 1/16 BPS
    states have 5 charges but perhaps only 4 charge
    subset has O(N2) entropy Berkooz et al 06

18
CFT entropy calculation?
  • Need to count 1/16 BPS states of N4 SU(N) SYM on
    RxS3 (or local operators on R4) with same quantum
    numbers O(N2) as black hole
  • Black hole entropy O(N2)
  • States typically descendents but need large
    entropy O(N2) in primaries

19
No 1/8 BPS black holesRoiban HSR 04,
Berenstein 05
  • 1/8 BPS primaries built from N1 superfields Xi,W
  • Commutators give descendents, so Xi, W can be
    treated as commuting
  • Diagonalize O(N) degrees of freedom so entropy
    of primaries of length O(N2) is O(N log N), too
    small for bulk horizon

20
Weakly coupled CFTRoiban HSR 04, Kinney,
Maldacena, Minwalla Raju 05
  • Goal at weak coupling, count operators in short
    1/16 BPS multiplets that cant become long at
    strong coupling
  • Too hard! Count everything instead
  • Find correct scaling of entropy with charge for
    large charge

21
Superconformal IndexKinney, Maldacena, Minwalla
Raju 05
  • Vanishing contribution from states in short
    multiplets that can combine into long ones
  • Independent of N at large N doesnt see black
    holes
  • Cancellation between bosonic and fermionic BPS
    states dual to black hole

22
Summary
  • There is a 4-parameter family of 1/16 BPS black
    holes in AdS5
  • Why only 4 parameters?
  • How do we calculate their entropy using N4 SYM?
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