Upload
others
View
8
Download
0
Embed Size (px)
Citation preview
Yong P. ChenQuantum Matter and Devices Lab
Department of Physics andSchool of Electrical and Computer Engineering and
Birck Nanotechnology CenterPurdue University <[email protected]>
Expanding Atomic Quantum Gaseswith tunable interaction and disorder
---emulating dynamics and fluctuations in superfluids … and nuclear matter?
Brookhaven National Laboratory May 23, 2008
Nuclear Physics & RIKEN Theory Seminar
My question
Promising systems (studied in my lab): • Graphene --- Dirac/chiral fermions: Coulomb collapse, Klein paradox…..
• Ultracold quantum gases (Bose-Einstein condensates; degenerate fermions/BEC-BCS;Bose-fermi mixtures;….)
Advantages: Tunable system parameters (customer-designed Hamiltonians): You can watch the system (probe both density and phase) to evolve!
How can we design condensed matter experiments to emulate nuclear/high energy physics phenomena?(esp. those difficult to test in real NP/HEP experiments, i.e. accelerators)
Emulational physics?
Talk outline
• Brief review of cold atoms & BEC---examples of NP/HEP connection
• Tunable interaction and expanding BEC• Disordered BEC:
superfluid to insulator transitionevolution of quantum and density
fluctuations
Please stop me for questions!
Bose-Einstein Condensate
~1μK 50nK
[7Li]
[6Li][7Li]
Meet Our Atom: Lithium-77Li -- boson(3p+, 4n) + 3e-
6Li -- fermion(3p+, 3n) + 3e-
E
r(continuum)
Bose-EinsteinCondensation
(1)
(mF=2)
(0)(-1)
(-2)
(-1)(0)(1)
F=2
F=1
22S1/2
(Feshbach Resonance)of 7Li in (1,1) state
Tunable Interaction
“mean field” interaction ∝ a0
repulsive
attractive
rf evaporationN~few 106
T~10 μK
Magnetic trap (2,2) state [a<0]
~700K
Zeeman Slowing --------------> MOT ------>
N~few 1010
T~1mKlaser cooling:
ω(671nm)
υ ωF=-kυ B(1,1)
(2,2)Uoptical pumping --->
Experimental Creation of BEC
<---------------optical evaporation<-----------------
(1, 1) statego to high B
1 μK300 nK
BEC!
80nK N~105-106
z
(1030nm)
optical trap U
• in-situ imaging of cloud-- probe ground state wavefunction
• free expansion: momentum space translates into real space---probe phase coherence/fluctuation
•(“restricted-fly”) evolution dynamics in selective potentials
• excite and collective mode
How to Experimentally Probe an Atomic Gas
“sit”
“fly”
“kick”
Just watch it!
A golden decade of quantum gases of cold atomic quantum gases --- some highlights• Bose-Einstein Condensate (BEC) [1995] now in most alkali, H, He* and Yb, Cr
(Nobel prize, 2001)
• Fermionic Condensate/BCS-BEC crossover [2004-2005]2-
body
Inte
r.
B
BEC(bosonicmolecules)
BCS(cooperpairs)
kF|a| > 1“Feshbach Resonance”
(from Ketterle’05)
•atoms in optical lattices (eg., BEC/superfluid-Mott insulator) [2002-]
•atoms in optical disorder potential [2005-]
(Mott insulator)
M. Greiner et al., (2002)
(Anderson insulator)
Tunable System Parameters• interaction (repulsive, attractive, short
range, long range,isotropic/anisotropic)• random and period potentials• dimensionality (1-3D) and spatial
structure• quantum and density fluctuations • time-dependent perturbations……
Emulator for Quantum Systems [Feynman/DARPA]
NP/HEP Connections?• Expansion of quantum gases and
hydrodynamics [Thomas, Grimm, …] • Instabilities due to interaction ----
condensate collapse: “Bosenova”; dipolar collapse
• Bose-Fermi mixture and supersymmetry, “Goldstino” modes (K.Yang’08); models for string theory (Stoof’05)…
• Sound wave propagation: models for cosmology
Interaction and Expansion of BEC
200
150
100
50
0
-50
-100
Scat
terin
g Le
ngth
(a B)
1000800600400
Magnetic Field (G)
Li-7 in (1,1) state
(b) B=717G
(c) B=551G
(d) B=544G
(a)
0.005ms
0.3ms
1ms
3ms
6ms
9ms
11ms
544G: a<0 TOF images
0.5ms
1ms
3ms
6ms
9ms
11ms
551G: a<~1aB
TOF images
Dipolar Interaction and Dipolar Collapse at a>0
• Cr-52 BEC: a dipolar BEC (Pfau’05)
Disordered BEC, fluctuations
Collaborators: James Hitchcock, Dan Dries, Mark Junker, Chris Welford and Randy Hulet (Rice Univ.)
Yong P. Chen et al., PRA 77, 233632 (2008)
From Superfluids and Superconductors to Insulators..
Insulators:•technologically important
•intellectually important to understand conductors and superconductors/superfluids
What is the essence of superfluidity and superconductivity?
understanding by (temporarily) “escaping”...
band insulator (no carriers)
Way#1: no carriers
conductor (metal)
BUT...
How to get an insulator?
Interaction and DisorderFestkorperphysik ist
Schmutzphysik!(“Solid State Physics
is Dirty Physics”)
fundamental themes incondensed matter physics
disorder+interaction?
...
(di s
o rde
r) Anderson insulator
[superfluid/superconductor]metal (interaction)
Mott insulator
Disordered Superconductor
A. Goldman and N. Markovic, Physics Today 1998
Insulator
superconductor
increasingdisorder
Example: Thin film superconductors (eg., Bi)
• “granular superconductor”:local superconductorglobal insulator
(Ec>EJ)
• “homogeneous”:any local superconductivity?
SS
S S
SS
S
•How does disorder destroys superconducting order parameter |Ψ|eiθ
• superfluidity and phase coherence • “Bose glass”?• Dissipation mechanism? intermediate
metallic phase? (“Bose metal”)•Is (dirty) boson-picture sufficient (SC)?
Superfluid/Superconductor to Insulator Transition (SIT)See also: “dirty” superfluid, random J-junction arrays etc. – “dirty bosons”
(disorder induced)
Simulate bydisordered quantum gas(both bosons & fermions)
BEC: Coherent and Superfluid(d
iso r
d er) Anderson
insulator
Coherence =Superfluidity ?
Bose glass ?..
(from W. Ketterle website)
BEC: coherent matter wave:===> atom laser
Disordered BEC:87Rb: Ingusci (Florence,2005-2006),
Aspect (Paris,2005-2006), Ertmer (Hannover, 2005)7Li: us (Rice, 2006-)
(interaction)
Mott insulator
[superfluid/BEC]M. Greiner et al., Nature (2002)
transition to insulator~loss of coherence
a nanoscience“simulator”
.
diffusive plate(rough glass,CNT film etc)
IR (1030nm)
CCD
can image both disorder potential and atoms!
How to Generate Optical Disorder: Laser Speckle
Pot
entia
l Ene
rgy
distance372 75 248 5 124 25 0 124 25 248 5 372 75
Δz
2VD
<V(r)V(r’)>:• Disorder Strength
VD tunable from0 to few kHz
• Disorder correlation length(speckle size) Δz down to~ 15 μm (limited by diff.
plate/geometry)
laser speckle is a coherent phenomenon
(incoherent lightswon’t give speckle)
•BEC radial size <~ Δz==> effective 1D disorder!
2500
2000
1500
1000
500
0
(µm
)
25002000150010005000(µm)
372 75 248 5 124 25 0 124 25 248 5 372 75
BEC
trap+disorder
How to Probe it?“sit”• in-situ imaging of cloud
-- probe ground state wavefunction
“push”• excite and collective mode ---(damping) • slow push (transport)
“fly”• free expansion (after experiencing disorder)
---probe phase coherence/fluctuation•(“restricted-fly”) evolution dynamics in disorder
--- rate of expansion /transport
µ
Typical(Interacting) BEC:[Part 1 of Talk (SIT)]
N~105-106 atomsaxial size(z)~1mmradial size ~10 µmInteracting a~200aBchemical µ~kHzT<100nK
ondisorder:off
onoptical trap:
<~1s
experimental sequence:
372 75 248 5 124 25 0 124 25 248 5 372 75
BEC
disorder
trap
Transport Experiment
trap?
initial (VD= 0)
VD~0.3µVD~ µ
dafter offset:
VD= 0d=1.4mmτoffset~1s
Transport Experiment 1: Trap offset slowly --- “Dragging BEC through disorder”
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
0
200
400
600
800
1000
1200
1400
d 1400 μm 900 μm 500 μm 300 μm
Clo
ud C
ente
r (μm
)
VD / μ
d
372 75 248 5 124 25 0 124 25 248 5 372 75
d
Strong disorder pins BEC
Pinning of BEC by disorder
VD = 60Hz VD = 300HzVD = 0Hz
τevolve=75ms
200ms
300ms
500ms
600ms
800ms
950ms
Evolution of cloud following abruptly “shaking” trap (in ~5msec)
Transport Experiment 2: Trap offset abruptly --- dipole excitation
0 300 600 9000
200
400
600
-400
0
400
VD / μ
0.37 0.58 1.03
Evolution Time (ms)
(b)
VD / μ 0 0.08 0.16 0.24
Clo
ud C
ente
r (μm
)
(a)
Damping of Dipole Excitations
overdamped for VD >~0.3µ(fully pinned for VD >~µ)
dissipation/dampingsets in at very small VD
cloud moving speed~ BEC sound speed
(center)!exciting phase slips (vortices),phonons etc
372 75 248 5 124 25 0 124 25 248 5 372 75
Summary of transport properties
• We measure global transport <different from local-insulator probe such as Greiner>
Apparently 3 different regimes of transport:• High VD : inhibition of transport (global insulator)
“pinning point” (0.7-1µ) not universal value (dep on disorder realizationand measurement type) --- probably sensitive to high peaks in disorder?
• Small VD damps dipole excitation dissipation or dephasing? “metallic” regime? (cf: on lattice, DeMarco’07)dissipation mechanism --- “phase slips”, vortices ...??where does the energy go?
• Medium VD : overdamped transport what’s the transport mechanism? tunneling assisted?fate of this regime at T=0? --- “semiconductor” regime?
Time of Flight (TOF) Free Expansion
372 75 248 5 124 25 0 124 25 248 5 372 75
disorder
trap
BEC
TOF free expansion time (τ) [few ms]
Time of Flight probes phase coherence
Time of Flight (TOF) Free Expansion
disorder:
off
on
off
on
optical trap:
off
TOF free expansion time (τ) [few ms]
imaging cloud
<~1s
τTOF
0ms
1ms
2ms
3ms
6ms
8ms
0 Hz
note: color scale all relative!
VD
VD ~0.3µ
VD ~µ
0ms
1ms
2ms
3ms
6ms
8ms
increasing disorder...700 Hz
chemical potential µ~1 kHzτTOF
0ms
1ms
2ms
3ms
6ms
8ms
0 Hz
note: color scale all relative!
VD 200 Hz
(Random) interference “stripes”Yong P. Chen et al., PRA(2008)
-500 0 500
tTOF = 8 mstTOF = 0 ms (in-situ)
z (μm) z (μm)-500 0 500
VD/μ~0.3
VD/μ~0.5
VD/μ~1.0
VD/μ=0
0.00 0.25 0.50 0.75 1.000.0
0.2
0.4
0.6
0.8
1.0
1.2
8 ms TOFIn-situ
VD / μ
Con
trast
Density Fluctuations: In-situ vs TOF
Column density(phase-contrast imaging)
Random butreproducible interference fringes
Phase coherence
1400
1200
1000
800
600
400
200
0
arb
unit
5004003002001000
pixel
TOF: 4.5 ms 6 ms 9 ms 0 ms
Vd=500Hz
•not correspond to insitu disorder(though does vary with disorder realization)
•can be reproduced from shot-shot!•not sensitive to “hold time”--unlikely from random quantumfluctuation (in phase)
Features of the interference pattern
BEC phase fluctuation at t=0 ----> density fluctuation (t=τ)
n (r ) = Ψ (r ) 2 :
φ :
t=0
∂∂x
eikx( )= ikeikx
(phase ~ velocity) n (a
rb. u
nit)
25002000150010005000x (µm)
Numerics (GPE) show can be derivedand evolved from initial density fluctuation & phase coherent ground state(Clement &Sanchez-Palencia’07)
Disorder-inducedPhase fluctuation in BEC?
n(r) = Ψ(r) 2 :
φ :
t=0 t=τ
free expansion
∂∂x
eikx( )= ikeikx
(phase ~ velocity)
phase fluctuations also observed in elongated interacting BEC at finite TS.Dettmer et al., (W.Ertmer, Hanover), PRL2001
in our case: (quantum)phase fluctuation due to disorder instead of heating!
Lφ = Lφ (T ,<Vd >, B[a])
(Reproducible) Random Interference : Matterwave Speckle
llaser(coherentlightwave)
rough surface laser speckle
tBEC(coherentmatterwave)
laser speckle
atom-laser speckle
(for electrons, speckle==> universal conductance fluctuation)
Coherence
Note: in periodic potential (lattice), interference pattern (one-shot) occurs even w/o coherence
Random potential+reproducible “fluctuation” pattern=>coherence--mesoscopic physics
“interference” stripes <---coherence• reproducible• only BEC (not seen with thermal gas)• 1D modulation<--1D disorder
Reproducible TOF fringes in disordered 87Rb BEC: eg, D. Clement et al., arXiv. 0710.1984 (2007)
n (a
rb. u
nit)
25002000150010005000x (µm)
Digression: Speckle and Mescoscopic Physicsconductance through small conductors (wires, rings etc.):==>Universal Conductance Fluctuation (UCF)--- phase coherence transport
and analog of speckle for electron wavefunction
•mesoscopic: phase coherence L~ sample size•cold atoms/BEC excellent lab to study mesoscopic effects!
R.Webb’84
Strong Disorder:
VD(all 6ms TOF)
0Hz
B~720G (interacting)
8ms TOFVD/μ1
0.6
0.3
0.1
0.03
0
0ms (in-situ)
“tight binding”limit(random Josephson)[also in Rb exp]
insulator without phase coherence
[BEC/superfluid (coherent)]
disorder
lattice(Mott)
M. Greiner et al., (2002)
loss of phasecoherence
“granular” condensate/superfluid(global insulator)
each (superfluid) “grain”: number certain; (relative) phase random==> no macroscopic phase coherence
Medium Disorder: SIT and Phase Coherence
B~720G (interacting)
8ms TOFVD/μ1
0.6
0.3
0.1
0.03
0
[BEC/superfluid (coherent)]
disorder
0 ms (in-situ)
(cloud still connected)
Medium disorder:• during superfluid-insulator transition• system not yet “granular”• (global) superfluidity compromised
[losing phase rigidity]
• still has phase coherence
(not granular)
how is (global) superfluid order parameter suppressed?[mean field th broken down?/role of quantum fluctuations]
• Turn off the optical trap• Allow the condensate to evolve inside the
disorder• Turn off the disordered potential• (immediately) Image the cloud
Experimental Procedure
optical trap BEC
Exp#4: Fall/Flow in Disorder
Results• We Qualitatively compare the disordered
TOF images to a free expanding BEC
5 ms 10 ms
(no disorder)
(with disorder)[at this disorder strength strong stripes were observedin the free TOF experiment]
Localized confinement (trapping)?
• we see localized confinement few areas of the BEC
• Parts are confined for very long times (~20ms)
• Majority of the cloud “flows” away
10ms evolution in disorder
17ms evolution in disorder
[superfluid/superconductor]
disorder+interaction?
...
pinned solid(d
isor
der)
metal (interaction)
Bose glass
Quantum Coherence may be important even in insulators--- especially if you get them from a superfluid/superconductor
• “Bosonization” (eg. pair)
• Phase Coherence
• Phase Rigidity
3 steps:
And what about superfluidity &superconductivity?
φ φ φ φ φ
interaction
disorder
what’s the global phase diagramfor a disordered & interacting Bose (or Fermi) gas?(free space or trapped)
• drive quantum phase transition (cf. Q.Si and D.Natelson, NPA radio show)relevant for High Tc, heavy fermions materials, superfluid-insulator
transition, nuclear matter.....
Quantum/Phase fluctuations are interesting in Physics...
• even our fate ... :
(from http://map.gsfc.nasa.gov/)
atoms
Quantum Emulator?