tomimatsu-sato geometries and the kerr/cft...
TRANSCRIPT
TS & Kerr/CFT arXiv:1010.2803 – 1 / 15
Tomimatsu-Sato geometries and the
Kerr/CFT correspondance
Sanjeev Seahra (with J Gegenberg, H Liu and B Tippett)
Black holes VIII: May 13, 2011
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Introduction
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 2 / 15
� Kerr/CFT: attempt to obtain holographic description of extremalKerr black holes (originally)
� based on structure of near-horizon geometry
� CFT Cardy formula reproduces gravitational entropy
� many properties of CFT remain mysterious
� may be useful to look at to more examples of extremal spinninghorizons in GR
� e.g. extremal Kerr-Bolt (Ghezelbash 2009)
� here we consider generalization to the (admittedlypathological) Tomimatsu-Sato (1972) spacetimes
Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 3 / 15
Basic properties of Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 4 / 15
time
4D vacuum solutions of GR: [cf. Hikida and
Kodama 2003]
Basic properties of Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 4 / 15
time
4D vacuum solutions of GR:
stationary
[cf. Hikida and
Kodama 2003]
Basic properties of Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 4 / 15
time
4D vacuum solutions of GR:
stationary
axisymmetric
[cf. Hikida and
Kodama 2003]
Basic properties of Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 4 / 15
asymptotically flat
time
4D vacuum solutions of GR:
stationary
axisymmetric
[cf. Hikida and
Kodama 2003]
Basic properties of Tomimatsu-Sato spacetimes
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 4 / 15
asymptotically flat
time
4D vacuum solutions of GR:
stationary
axisymmetric
(Kerr black holes are special cases of TS solutions)
[cf. Hikida and
Kodama 2003]
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
The metric
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 5 / 15
fixed length scale
Ergoregion and closed timelike curves
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 6 / 15
signature of timelike tα andazimuthal φα Killing vectorsvaries over (ρ, z) plane:
Ergoregion and closed timelike curves
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 6 / 15
signature of timelike tα andazimuthal φα Killing vectorsvaries over (ρ, z) plane:
� ergosphere (tαtα > 0)
Ergoregion and closed timelike curves
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 6 / 15
signature of timelike tα andazimuthal φα Killing vectorsvaries over (ρ, z) plane:
� ergosphere (tαtα > 0)
� closed timelike curves(φαφα < 0)
Ergoregion and closed timelike curves
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 6 / 15
signature of timelike tα andazimuthal φα Killing vectorsvaries over (ρ, z) plane:
� ergosphere (tαtα > 0)
� closed timelike curves(φαφα < 0)
� conical singularity S withdeficit (excess):2πp2/(1− p2)
Ring singularity
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 7 / 15
Ring singularity
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 7 / 15
Ring singularity
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 7 / 15
Ring singularity
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 7 / 15
Killing horizons
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 8 / 15
Killing horizons
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 8 / 15
Killing horizons
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 8 / 15
Killing horizons
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 8 / 15
Killing horizons
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 8 / 15
Mass and angular momentum
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 9 / 15
Mass and angular momentum
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 9 / 15
Mass and angular momentum
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 9 / 15
Mass and angular momentum
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 9 / 15
Mass and angular momentum
Introduction
TS spacetimes
Basic properties
The metric
Ergoregion and CTCs
Ring singularity
Killing horizons
M and J
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 9 / 15
Properties of the “dual CFT”
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 10 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Near horizon extremal spinning (NHES) metric
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 11 / 15
Central charge
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 12 / 15
Calculation of the central charge of candidate CFT dual to NHESgeometry proceeds as in Kerr/CFT (Strominger et al 2009):
1. find diffeomorphisms ξn preserving selected BCs on metricfluctuations
2. use covariant formalism (Barnich and Compere 2008) to find(Virasoro) algebra of associated charges Qξn under Diracbracket
i{Qζm, Qζn} = (m−n)Qζm+ζn+γ2J∆m
(
m2 +2
γ2
)
δm+n,0
3. read off the central charge c = 6γr20/G = 12γ2J∆
(recover Kerr/CFT for γ = 1 and J∆ = JADM)
Central charge
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 12 / 15
Calculation of the central charge of candidate CFT dual to NHESgeometry proceeds as in Kerr/CFT (Strominger et al 2009):
1. find diffeomorphisms ξn preserving selected BCs on metricfluctuations
2. use covariant formalism (Barnich and Compere 2008) to find(Virasoro) algebra of associated charges Qξn under Diracbracket
i{Qζm, Qζn} = (m−n)Qζm+ζn+γ2J∆m
(
m2 +2
γ2
)
δm+n,0
3. read off the central charge c = 6γr20/G = 12γ2J∆
(recover Kerr/CFT for γ = 1 and J∆ = JADM)
Central charge
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 12 / 15
Calculation of the central charge of candidate CFT dual to NHESgeometry proceeds as in Kerr/CFT (Strominger et al 2009):
1. find diffeomorphisms ξn preserving selected BCs on metricfluctuations
2. use covariant formalism (Barnich and Compere 2008) to find(Virasoro) algebra of associated charges Qξn under Diracbracket
i{Qζm, Qζn} = (m−n)Qζm+ζn+γ2J∆m
(
m2 +2
γ2
)
δm+n,0
3. read off the central charge c = 6γr20/G = 12γ2J∆
(recover Kerr/CFT for γ = 1 and J∆ = JADM)
Central charge
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 12 / 15
Calculation of the central charge of candidate CFT dual to NHESgeometry proceeds as in Kerr/CFT (Strominger et al 2009):
1. find diffeomorphisms ξn preserving selected BCs on metricfluctuations
2. use covariant formalism (Barnich and Compere 2008) to find(Virasoro) algebra of associated charges Qξn under Diracbracket
i{Qζm, Qζn} = (m−n)Qζm+ζn+γ2J∆m
(
m2 +2
γ2
)
δm+n,0
3. read off the central charge c = 6γr20/G = 12γ2J∆
(recover Kerr/CFT for γ = 1 and J∆ = JADM)
Central charge
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 12 / 15
Calculation of the central charge of candidate CFT dual to NHESgeometry proceeds as in Kerr/CFT (Strominger et al 2009):
1. find diffeomorphisms ξn preserving selected BCs on metricfluctuations
2. use covariant formalism (Barnich and Compere 2008) to find(Virasoro) algebra of associated charges Qξn under Diracbracket
i{Qζm, Qζn} = (m−n)Qζm+ζn+γ2J∆m
(
m2 +2
γ2
)
δm+n,0
3. read off the central charge c = 6γr20/G = 12γ2J∆
(recover Kerr/CFT for γ = 1 and J∆ = JADM)
Temperature
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 13 / 15
The temperature of the candidate CFT found from analyzing scalarwave equation �Φ = 0 in NHES geometry
1. change from (t, r, φ) to (w±, y) coordinates such that � isrepresented by quadratic function of SL(2,R) generators
2. conformal symmetry broken by periodic identification ofw− ∼ w−e
2π/γ
3. induces a finite Unruh temperature for theSL(2,R)× SL(2,R) invariant vacuum according toco-rotating (t, r, φ) observers:
TL = (2πγ)−1
(again γ = 1 reproduces Kerr/CFT result)
Temperature
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 13 / 15
The temperature of the candidate CFT found from analyzing scalarwave equation �Φ = 0 in NHES geometry
1. change from (t, r, φ) to (w±, y) coordinates such that � isrepresented by quadratic function of SL(2,R) generators
2. conformal symmetry broken by periodic identification ofw− ∼ w−e
2π/γ
3. induces a finite Unruh temperature for theSL(2,R)× SL(2,R) invariant vacuum according toco-rotating (t, r, φ) observers:
TL = (2πγ)−1
(again γ = 1 reproduces Kerr/CFT result)
Temperature
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 13 / 15
The temperature of the candidate CFT found from analyzing scalarwave equation �Φ = 0 in NHES geometry
1. change from (t, r, φ) to (w±, y) coordinates such that � isrepresented by quadratic function of SL(2,R) generators
2. conformal symmetry broken by periodic identification ofw− ∼ w−e
2π/γ
3. induces a finite Unruh temperature for theSL(2,R)× SL(2,R) invariant vacuum according toco-rotating (t, r, φ) observers:
TL = (2πγ)−1
(again γ = 1 reproduces Kerr/CFT result)
Temperature
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 13 / 15
The temperature of the candidate CFT found from analyzing scalarwave equation �Φ = 0 in NHES geometry
1. change from (t, r, φ) to (w±, y) coordinates such that � isrepresented by quadratic function of SL(2,R) generators
2. conformal symmetry broken by periodic identification ofw− ∼ w−e
2π/γ
3. induces a finite Unruh temperature for theSL(2,R)× SL(2,R) invariant vacuum according toco-rotating (t, r, φ) observers:
TL = (2πγ)−1
(again γ = 1 reproduces Kerr/CFT result)
Temperature
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 13 / 15
The temperature of the candidate CFT found from analyzing scalarwave equation �Φ = 0 in NHES geometry
1. change from (t, r, φ) to (w±, y) coordinates such that � isrepresented by quadratic function of SL(2,R) generators
2. conformal symmetry broken by periodic identification ofw− ∼ w−e
2π/γ
3. induces a finite Unruh temperature for theSL(2,R)× SL(2,R) invariant vacuum according toco-rotating (t, r, φ) observers:
TL = (2πγ)−1
(again γ = 1 reproduces Kerr/CFT result)
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
� Geometric entropy: SBH =A∆
4G=
πr20G
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
� Geometric entropy: SBH =A∆
4G=
πr20G
� SCFT = SBH for all members NHES class including:
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
� Geometric entropy: SBH =A∆
4G=
πr20G
� SCFT = SBH for all members NHES class including:
� extremal Kerr
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
� Geometric entropy: SBH =A∆
4G=
πr20G
� SCFT = SBH for all members NHES class including:
� extremal Kerr
� extremal Kerr-Bolt
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
� Cardy formula: SCFT =1
3π2cTL =
πr20G
� Geometric entropy: SBH =A∆
4G=
πr20G
� SCFT = SBH for all members NHES class including:
� extremal Kerr
� extremal Kerr-Bolt
� Tomimatsu-Sato (sort of . . . )
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
Cardy formula
Introduction
TS spacetimes
The “dual CFT”
NHES metric
Central charge
Temperature
Cardy formula
Summary
TS & Kerr/CFT arXiv:1010.2803 – 14 / 15
Summary
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 15 / 15
� TS spacetime is a Kerrgeneralization that’s full of exoticfeatures ⇒ a “lesion study” ofKerr/CFT
� we have derived c and TL for a CFTthat may be dual to some portion ofTS spacetime
� CFT properties we calculated seemto be ignorant of ring singularity,CTC region, etc
� need to ask more probing questionsto determine if CFT is only dual toH±
Summary
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 15 / 15
� TS spacetime is a Kerrgeneralization that’s full of exoticfeatures ⇒ a “lesion study” ofKerr/CFT
� we have derived c and TL for a CFTthat may be dual to some portion ofTS spacetime
� CFT properties we calculated seemto be ignorant of ring singularity,CTC region, etc
� need to ask more probing questionsto determine if CFT is only dual toH±
Summary
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 15 / 15
� TS spacetime is a Kerrgeneralization that’s full of exoticfeatures ⇒ a “lesion study” ofKerr/CFT
� we have derived c and TL for a CFTthat may be dual to some portion ofTS spacetime
� CFT properties we calculated seemto be ignorant of ring singularity,CTC region, etc
� need to ask more probing questionsto determine if CFT is only dual toH±
Summary
Introduction
TS spacetimes
The “dual CFT”
Summary
TS & Kerr/CFT arXiv:1010.2803 – 15 / 15
� TS spacetime is a Kerrgeneralization that’s full of exoticfeatures ⇒ a “lesion study” ofKerr/CFT
� we have derived c and TL for a CFTthat may be dual to some portion ofTS spacetime
� CFT properties we calculated seemto be ignorant of ring singularity,CTC region, etc
� need to ask more probing questionsto determine if CFT is only dual toH±