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Pohang, 2010
One-dimensional disordered Bose-Fermi mixtures in optical lattices
Gergely ZarándBudapest Univ. Technology and Economics
Collaborators:Francois Crépin & Pascal Simon (Orsay)
F. Crepin, G.Z., and P. Simon, to appear in PRL, arXiv:1005.2483;
Disordered 1D Bose-Fermi mixtures
Outline
The Bose Glass
Basic Experimental Methods
• Experiments• Creating disorder
• RG analysis and phase diagram• Replica Symmetry breaking• Physical observables
Conclusions
Interacting Bosons
Basic Experimental Methods
Trapping and (over)cooling atoms• Produce ion beam Rb, Na, Cs, K, Li,…• Laser cooling / Doppler Cooling / Zener slower / MOT traps
• Trapping the atoms (conservative traps)
• Evaporative cooling
• Detection:
Magnetic traps Dipol traps
below 1 μK (~20 kHz)
1-100 μK
Absorbtion imaging
(Hyperfine energy ~ 1 mK !)atoms10
K10~T9
Observation: Absorbtion imaging
TOF Detects momentum distribution of atoms :
Release atoms and then take a picture !
Spatial imaging
Absorption images after ballistic expansion of the cloud
(time-of-flight) from W. Ketterle
)/(~~)( 0 tmxpxt
Bose-Einstein condesation
Cold atoms: Highly tunable correlated systems
Tuning interactions:
Feschbach resonances:
Optical lattices 4/3~ sU
set 2~
REs
)(2 xV ma
)(Baa
1-3 dimensions
Bloch, Dalibard, and Zwerger, RMP 2008
Local interaction Scattering length
Recoil energy
Localizing atoms by disorder
Billy et al, Nature 453 2008
Map the wave functionMeasure localization length
Confining laser
speckle laser(disorder)
Rb87
The Bose Glass
Mott transition for Bosons
1ni
JU
UJ
Superfluid:
Insulator:
U
bosons on a lattice
1ni
sx nSFaaSF || 0
1in Superfluid for any J/U
Phase diagram
UJ /
1n
2n
n
SuperFluid
Mott Instulator
Incompressible state
nnnH U )1(2:0J
U/
0Jn
0 1
1
20T
Mott Insulator is incompressible !
Incompressible state
Mott Insulator is incompressible !
U/
0Jn
0 1
1
20T
01
nn:0J
Phase diagram
Bloch, et al. RMP 2008
Interacting bosons + disorder
Mott insulator
Bose glass
[Fisher, Weichman, Grinstein, Fisher, PRB 1989]
Bose-Glass
01
nn
01
nn
Measuring the Bose glass ?
[Fallani et al, PRL 98, 130404 (2007)]
Create quasirandom potential
Getting the Bose glass ?
[Fallani et al, PRL 98, 130404 (2007)]
Excitation spectrum
Bose glass ?
Mott insulatorSuperfluid condensate
disorder
Disordered Bosons in 1D
Bosonization of Bosons… [Haldane, Giamarchi]
Continuum field theory:
bH
Kinetic term compressibility
1n
.).()(1)( )(2 cheexxn xixibbx
bb
Density:
Bose field: )(2/1)( xibi
bexb
bK
Gas can be described in terms of density fluctuations
Luttinger liquid parameter bU 1bK
0bU bK
bKbb xx 2/1||
1~)0()(
Disorder in 1D Bose system
Disorder:
Forward scatteringBackward scattering
)(xb Gaussian static disorder field
)()( xnxVdxnH bbj
jjdis
Bosonize:
RG Analysis of Bosons
Giamarchi and Schulz, PRB 37, 325 (1988)
bK/13/2
bD
0
Luttinger liquid (superfluid) (quasi long-range order, weak repulsion)
Bose glassLocalized bosonsStrong repulsion
(non-perturbative)
*2/1||1~)0()(
bKbbx
x
?0/ tUb
tUb /
1D Disordered Bose-Fermi Mixtures
Interacting 1D Bose-Fermi systems
Hamiltonian:
)( fHfermions bosons interaction)( bH )( bfH
ftbt
bUbfU
Bosonization:
momentum densitybf
incommensurate
Remarks on bosonization of bosons and fermions… ( )
Fermions Bosons
1fK
1fK
bK non-interacting1bK Infinite repulsion
1fK no interactionrepulsive
attractive
Density: ....).()(1)( )(2,,,
,, cheexxnxixi
fbfbxfbfbfb
)()(2/1 .).()( xixixi
fffff echeex
)(2/1)( xi
bbbex
Fermion field Bose field
2/)( 1
||)sin(~)0()(
ff KK
Fff
x
xkx
bKbbx
x 2/1||1~)0()(
0bfU
Diagonalization:
(Wentzel-Bardeen instability)
Linear transformation
• sound velocity
• dimensionless coupling
• instability:• polaronic excitations/superconductivity?
1|| g
Cazalilla and Ho, PRL 2003; Mathey et al., PRL 2004
BF mixture + Disorder
Forward scattering can be guauged out
Add potential: )()()()( xxVdxxxVdx ffbb
backward scattering
Disorder correlations
Interaction-renormalized scaling dimensions
2/)0()(
,
,,
||1~
fb
fbfb ii ee
fbfb Kg ,,:0
• gsKb
f
vv
bbb ,/
Interaction generates effective attraction(~ phonons in superconductivity)
0g fbfb K ,,
Stabilizes SF + generates SC state
• for•
Renormalization group equation
fbfbX ,, 2
Relevance of disorder:
Feed-back of disorder:
Localization length:
Phase diagram
BFG
AG + SFB
LLBFG*
AG + SFB:
interacting Anderson glass +Bosonic Luttinger liquid (SF)
BFG:
Bosons and Fermions localized, but interacting
finitef
finite, bf
LL: Luttinger Liquid
BFG*:
Tiny bosonic localization length
Phase diagram (Rb-K mixture)
Capturing localized phase: Replica trick
Replica Trick:
replSn
a
n eZ afDa
bD
1
Replicated action:
nZZ n
n/)1(limlog
0
replica-interaction generated
Impurity average can be performed
Gaussian variational method
n
b
ba
n
c xxxG10
)( )0()(lim)0()(),(
Connected Green’s function:
Approximate Gaussian action:
),(),()(),(21 1* qqGqS n
bn
abn
aG
Find G that minimizes the Free energy
[Giamarchi and Le Doussal, PRB 53, 15206 (1996)]
GSGSSTeTGF G-Strln][
fnffnvKKK
vv
KK
vv
bnbbnvK
n
c
Iqvqg
qgIqvqG
ffbf
bf
bf
bf
bb
)()(
)()(),(][
221121
2122111)(
• Replica symmetry breaking (~ gap)
• ,
0b if bosons localizedif fermions localized0 f
0)(lim ,0
nfbI
n
2,, ~ fbfb
• and must be determined self-consistently
)(, nfbI fb,
Solution of resulting complicated integral equations:
AG + SFB:
BFG:
One-step replica symmetry breaking
two-step replica symmetry breaking
Bosonic localization: 2~ bb
RG
2-step RSB
How to measure ?
• TOF experiment ~),( Trnb)'()(
',
)'(RRe bb
RR
RRTriMb
*2/11
1~bKr
• Noise correlations
r
detects SF
Can detect SC pairing */2|'|1~)'()(
fKffRR
RR
• Bragg scattering
),( qSmeasures
Fully localized phase
Conclusions
• Disorder + BF interaction new phasesBose-Fermi glass, coexisting localized/LL phases
• For and mixtures parameters are within reach• Phase transitions can be detected by
• time of flight • noise correlations• Bragg scattering localized phases
LiLi 76
)0()( bb x
)0()( ff x
• Open question: bf
Composite fermion glass ?
bf
KRb 4087
F. Crepin, G.Z., and P. Simon, to appear in PRL, arXiv:1005.2483; and other papers under preparation
Localization of bosons by fermions
Ospelkaus et al. PRL 96, 180403 (2006)
Time of flight experimentRbK 8740 mixture
Without fermions
with fermions
Fourier transform of Wannier function '
',
)'()( RRRR
RRki aaekG
txmk /
Phase diagram
Bloch, et al. RMP 2008
Bosons in a trap:
potential )(zV
)(zV
eff
Shell structure
Interaction-renormalized scaling dimensions
fb
fbfb iiee
,
,,
2)0()(
||1~
4/:0 ,, fbfb Kg
2141
g
•• for
gsKb
f
v
v
bbb ,/
Interaction generates effective attraction…