Title: Anti de Sitter Black Holes
1Anti de Sitter Black Holes
- Harvey Reall
- University of Nottingham
2Motivation
- 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
3Plan
- 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
4SUSY 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
5SUSY 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
6SUSY 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
75D 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)
85D 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)
95D 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
10Unequal 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
11General 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)
12CFT 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
13A 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?
14BPS 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
15BPS 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)
16New 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?
17Resolutions 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
18CFT 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
19No 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
20Weakly 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
21Superconformal 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
22Summary
- 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?