holographic superconductors with higher curvature corrections sugumi kanno (durham) work w/ ruth...
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Holographic Superconductors with Higher Curvature Corrections
Sugumi Kanno (Durham)
work w/
Ruth Gregory (Durham)Jiro Soda (Kyoto)
arXiv:0907.3203, to appear in JHEP
2
Introduction
It would be very exciting if we could explain high temperature superconductivityfrom black hole physics.
We verify this numerically and analytically.
According to holographic superconductors, scalar condensation in black hole systemexists. This deserves further study in relation to the “no-hair” theorem from gravityperspective.
Holographic Superconductors
Since the stringy corrections in the bulk corresponds to the fluctuations from large N limit in holographic superconductors, it is expected the stringy corrections make holographic condensation harder.
Hartnoll, Herzog & Horowitz (2008)
・ the critical temperature is stable under stringy corrections.cT
What we are interested in is if
・ the universal relation between and : is stable under stringy corrections.8g cT g cT
Horowitz & Roberts (2008)g: The gap in the frequency dependent conductivity
3
52
12 S d x g R
L
2
2 2( )
r Mf r
L r
2
2
4( ) 1 1
2
rf r
L
242R R R R R
2
4
1M L
r
Gauss-Bonnet Black Hole
Action
BH solutions
2 2
2 2 2 2 22
( )( )
dr rds f r dt dx dy dz
f r L
2L , 0 2
2L 2
, 4L
Hawking temperature1/4
2 3/2
1( )
4H
H
r r
r MT f r
L L
Gauss-Bonnet term
Coupling constant >0
Constant of integration related to the ADM mass of BH
2effL
2eff
1L
Asymptotically vanishes.( )r
0
2 1/4( )Hr MLHorizon is at
0
When rH (=M ) decreases, temperature decreases(This is a nature of AdS spacetime)
… Chern-Simons limit
4
C
r
C
r
Gauss-Bonnet Superconductors – probe limit
Action (Maxwell field & charged complex scalar field)
2 25 21
4S d x g F F iA m
EOMs23 2
0r f
2 2
2
30
f m
f r f f
Regularity at Horizon (2) : ( ) 0Hr 4
( ) ( )3H H Hr r r
Asymtotic behaviors 2( )r
r
2
eff2 4 3L
L
Boundary condition in the asymptoric AdS region (2) : 0C is fixed
EOMs are nonlinear and coupled
( ) , , A r ( )r Static ansatz: ( )iA r( )rA r ( )i re 00
Mass of the scalar filed
Need 4 boundary conditions
Const. of Integrations
Solutions are completely determined
determined
According to AdS/CFT, we can interpret , so we want to calculateCO CHowever…We calculate this numerically first.
22
3m
L
5
Numerical Results
1/30.198cT
0.0001
1/30.186cT
0.1
1/30.171cT
0.2
1/30.158cT
0.25
CO
c
T
T
1
cT
O
Critical Temperature decrease
The effect of is to make condensation harder.
increase
Chern-Simons limit
1L
6
Towards analytic understanding
E.g.) The numerical solution for
r
Near horizon
4( ) ( )
3H H Hr r r N
ear a
sym
pto
tic AdS re
gio
n
C
r
21( ) ( ) ( ) ( )
2H H H H Hr r r r r r r r
b.c.
b.c.
Matching at somewhere
7
( ) (1) 1z z (1) 3
(1)4
Analytic approach
Change variable : Hrzr
EOMs2 2
4
1 20Hr
z z f
2 2
4 2 2
1 30Hrf
f z z f L f
2
2211 (1) (1) 1
2 2
Lz
4
222 2
15 3(1) (1) (1) 1
64 2 64 H
Lz
L r
0 1Hr r z
( ) (1) 1 z z
2( ) z z
( )z
Near horizon (z=1)
Near asymotoric AdS region (z=0)
(1)
2 2
411 1
1 2Hz
z z
r
z z f
21(1) 1
2z
(1) 0 3
(1) (1)4
Boundary Condition
Region :
2 2
4 2 21
1 1
1 3Hz
z z
rf
f z z f L f
21(1) 1
2z
2( )z qz ( )z D z D z
Solutions in the asymptotic region
(0) (1)z1
(0)2 q
21(0) (0) (0)
2z z D z
fixedHqr 0D
Boundary Condition
D z
Now, match these solutions smoothly at1
2z 1 1
, ,2 2
1
2z
1 1,
2 2
1
2z
'd
dz
8
3
3 24 1
2H
H
Br
Br L
Results of analytic calculation
Solutions
213(1)
8 2HrC
2 2
5 3 15 3(1) 8
2 2 64 2Hr
L L
Condensation is expressed by
: Critical temperature1/3
2 1cT BL L
11
213 3
3 3
13 22 1
8 2c
c c c
TT T
T T T T
O
2(1)
Go back to the original variable : Hr zr
HC r D 2
H
qr
2HBr
L 2
HrTL
Hawking temperature
3 3
2 3 3
21c
c
T T
L T T
COAdS/CFT dictionary gives a relation :
0 cT Tat0 cT Tfor
1/30.201 ( =0.0001)cT 1/30.196 ( =0.1)cT 1/30.191 ( =0.2)cT 1/30.188 ( =0.25)cT
1/30.198 ( =0.0001)cT 1/30.186 ( =0.1)cT 1/30.171 ( =0.2)cT 1/30.158 ( =0.25)cT
Numerical result
Good agreement!
1
2
1c
T
T
O Typical mean field theory result for the second order phase transition.
9
Conductivity of our boundary theory
Electromagnetic perturbations
If we see the asymptotic behavior of this solution,
2 22
2 2
1 k 20
fA A A
f r f r f f
4( ) ( ) H
irA r f r
A in the bulk AdS/CFT JGauge field Four-current on the CFT boundary
Consider perturbation of Aand its spatial components k x( , , ) ( )i i i ti iA t r x A r e e
B.c. near the horizon : ingoing wave function Hr The system is solvable.
(0) 2 2 2(2)eff(0)
2 2
k log
2
A LA rA A
r r
The conductivity is given by
(2)
(0)
k=0
2
2
A i
i A
: General solution
Arbitrary scale, which can be removed by an appropriate boundary counter term
Need to solve numerically with this b.c. toobtain , asymptotically.
( )A r(0)A (2)A
10
Conductivity and Universality
0.0001 0.152
c
TT
0.1 0.151
c
TT
0.2 0.152
c
TT
0.25 0.152
c
TT
realim
aginary
pole
exis
ts
0
0 0
0
pole
exis
ts
pole
exis
ts
pole
exis
ts
0.0001 0.1 0.2 0.25
The universal relation is unstable in the presence of GB correction.8g
cT
As increases, the gap frequency becomes large.
g g g g
11
Summary
The higher curvature corrections make the condensation harder.
The universal relation in conductivity is unstable under the higher curvature corrections.
We have found a crude but simple analytical explanation of condensation.
In the future, we will take into account the backreaction to the geometry.