quantum coherence and interactions in many body systems
DESCRIPTION
Quantum coherence and interactions in many body systems. Eugene Demler Harvard University. Collaborators: Ehud Altman, Anton Burkov, Derrick Chang, Adilet Imambekov, Vladimir Gritsev , Mikhail Lukin, Giovanna Morigi, Anatoli Polkonikov. - PowerPoint PPT PresentationTRANSCRIPT
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Quantum coherence and interactions in many body systems
Collaborators:Ehud Altman, Anton Burkov, Derrick Chang, Adilet Imambekov, Vladimir Gritsev , Mikhail Lukin, Giovanna Morigi, Anatoli Polkonikov
Eugene Demler Harvard University
Funded by NSF, AFOSR, Harvard-MIT CUA
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Condensed matter physics
Atomic physics
Quantum optics
Quantumcoherence
Quantuminformation
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Quantum Optics with atoms andCondensed Matter Physics with photons
Interference of fluctuating condensatesFrom reduced contrast of fringes to correlation functionsDistribution function of fringe contrastNon-equilibrium dynamics probed in interference experiments
Luttinger liquid of photonsCan we get “fermionization” of photons?Non-equilibrium coherent dynamics of strongly interacting photons
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Interference experimentswith cold atoms
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Interference of independent condensates
Experiments: Andrews et al., Science 275:637 (1997)
Theory: Javanainen, Yoo, PRL 76:161 (1996)Cirac, Zoller, et al. PRA 54:R3714 (1996)Castin, Dalibard, PRA 55:4330 (1997)and many more
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Interference of two independent condensates
1
2
r
r+d
d
r’
Clouds 1 and 2 do not have a well defined phase difference.However each individual measurement shows an interference pattern
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Nature 4877:255 (1963)
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Interference of one dimensional condensatesExperiments: Schmiedmayer et al., Nature Physics (2005,2006)
Transverse imaging
long. imaging
trans.imaging
Longitudial imaging
Figures courtesy of J. Schmiedmayer
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x1
d
Amplitude of interference fringes,
Interference of one dimensional condensates
For identical condensates
Instantaneous correlation function
For independent condensates Afr is finite but is random
x2
Polkovnikov, Altman, Demler, PNAS 103:6125 (2006)
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Interference of two dimensional condensates
Ly
Lx
Lx
Experiments: Hadzibabic et al. Nature (2006)
Probe beam parallel to the plane of the condensates
Gati et al., PRL (2006)
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Interference of two dimensional condensates.Quasi long range order and the KT transition
Ly
Lx
Below KT transitionAbove KT transition
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x
z
Time of
flight
low temperature higher temperature
Typical interference patterns
Experiments with 2D Bose gasHadzibabic, Dalibard et al., Nature 441:1118 (2006)
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integration
over x axis
Dx
z
z
integration
over x axisz
x
integration distance Dx
(pixels)
Contrast afterintegration
0.4
0.2
00 10 20 30
middle Tlow T
high T
integration
over x axis z
Experiments with 2D Bose gasHadzibabic et al., Nature 441:1118 (2006)
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fit by:
integration distance Dx
Inte
grat
ed c
ontr
ast 0.4
0.2
00 10 20 30
low Tmiddle T
high T
if g1(r) decays exponentially with :
if g1(r) decays algebraically or exponentially with a large :
Exponent
central contrast
0.5
0 0.1 0.2 0.3
0.4
0.3high T low T
2
21
2 1~),0(
1~
x
D
x Ddxxg
DC
x
“Sudden” jump!?
Experiments with 2D Bose gasHadzibabic et al., Nature 441:1118 (2006)
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Fundamental noise in interference experiments
Amplitude of interference fringes is a quantum operator. The measured value of the amplitude will fluctuate from shot to shot. We want to characterize not only the averagebut the fluctuations as well.
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Shot noise in interference experiments
Interference with a finite number of atoms. How well can one measure the amplitude of interference fringes in a single shot?
One atom: NoVery many atoms: ExactlyFinite number of atoms: ?
Consider higher moments of the interference fringe amplitude
, , and so on
Obtain the entire distribution function of
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Shot noise in interference experiments
Interference of two condensates with 100 atoms in each cloud
Coherent states
Number states
Polkovnikov, Europhys. Lett. 78:10006 (1997)Imambekov, Gritsev, Demler, 2006 Varenna lecture notes
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Distribution function of fringe amplitudes for interference of fluctuating condensates
L is a quantum operator. The measured value of will fluctuate from shot to shot.
Higher moments reflect higher order correlation functions
Gritsev, Altman, Demler, Polkovnikov, Nature Physics (2006)Imambekov, Gritsev, Demler, cond-mat/0612011
We need the full distribution function of
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0 1 2 3 4
Pro
babi
lity
P(x
)
x
K=1 K=1.5 K=3 K=5
Interference of 1d condensates at T=0. Distribution function of the fringe contrast
Narrow distributionfor .Approaches Gumbeldistribution.
Width
Wide Poissoniandistribution for
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Interference of 1d condensates at finite temperature.
Distribution function of the fringe contrast
Luttinger parameter K=5
Experiments: Schmiedmayer et al.
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Interference of 2d condensates at finite temperature.
Distribution function of the fringe contrast
T=TKT
T=2/3 TKT
T=2/5 TKT
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From visibility of interference fringes to other problems in physics
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Quantum impurity problem: interacting one dimensionalelectrons scattered on an impurity
Conformal field theories with negative central charges: 2D quantum gravity, non-intersecting loop model, growth of random fractal stochastic interface, high energy limit of multicolor QCD, …
Interference between interacting 1d Bose liquids.Distribution function of the interference amplitude
is a quantum operator. The measured value of will fluctuate from shot to shot.How to predict the distribution function of
Yang-Lee singularity
2D quantum gravity,non-intersecting loops
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Fringe visibility and statistics of random surfaces
)(h
Proof of the Gumbel distribution of interfernece fringe amplitude for 1d weakly interacting bosons relied on the known relation between 1/f Noise and Extreme Value StatisticsT.Antal et al. Phys.Rev.Lett. 87, 240601(2001)
Fringe visibility
Roughness dh2
)(
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Non-equilibrium coherentdynamics of low dimensional Bose
gases probed in interference experiments
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Studying dynamics using interference experiments.Thermal decoherence
Prepare a system by splitting one condensate
Take to the regime of zero tunneling Measure time evolution
of fringe amplitudes
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Relative phase dynamics
Quantum regime
1D systems
2D systems
Classical regime
1D systems
2D systems
Burkov, Lukin, Demler, cond-mat/0701058
Experiments: Schmiedmayer et al.
Different from the earlier theoretical work based on a single mode approximation, e.g. Gardiner and Zoller, Leggett
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Quantum dynamics of coupled condensates. Studying Sine-Gordon model in interference experiments
J
Prepare a system by splitting one condensate
Take to the regime of finitetunneling. Systemdescribed by the quantum Sine-Gordon model
Measure time evolutionof fringe amplitudes
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Dynamics of quantum sine-Gordon model
Power spectrum
Gritsev, Demler, Lukin, Polkovnikov, cond-mat/0702343
A combination ofbroad featuresand sharp peaks.Sharp peaks dueto collective many-bodyexcitations: breathers
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Condensed matter physics with photons
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Luttinger liquid of photons
Tonks gas of photons:photon “fermionization”
Chang, Demler, Gritsev, Lukin, Morigi, unpublished
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Self-interaction effects for one-dimensional optical waves
kk0
Nonlinear polarization for isotropic medium
Envelope function
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Self-interaction effects for one-dimensional optical waves
Frame of reference moving with the group velocity
Gross-Pitaevskii type equation for light propagation
Competition of dispersion and non-linearity
Nonlinear Optics, Mills
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Self-interaction effects for one-dimensional optical waves
BEFORE: two level systems and insufficient mode confinement
Interaction corresponds to attraction.Physics of solitons (e.g. Drummond)
Weak non-linearity due to insufficient mode confining
Limit on non-linearity due to photon decay
NOW: EIT and tight mode confinement
Sign of the interaction can be tuned
Tight confinement of theelectromagnetic modeenhances nonlinearity
Strong non-linearity without lossescan be achieved using EIT
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Controlling self-interaction effects for photons
c
Imamoglu et al.,PRL 79:1467 (1997)
describes photons. We need to normalize to polaritons
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Tonks gas of photons
Photon fermionization
Crystal of photons
Is it realistic?Experimental signatures
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Tonks gas of atoms
Small – weakly interacting Bose gas
Large – Tonks gas. Fermionized bosons
Additional effects for for photons: Photons are moving with the group velocity Limit on the cross section of photon interacting with one atom
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Tonks gas of photons
Limit on strongly interacting 1d photon liquid due to finite group velocity
Concrete example: atoms in a hollow fiber
Experiments: Cornell et al. PRL 75:3253 (1995);Lukin, Vuletic, Zibrov et.al.
Theory: photonic crystal and non-linear mediumDeutsch et al., PRA 52:1394 (2005);Pritchard et al., cond-mat/0607277
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Atoms in a hollow fiber
k
Without using the “slow light” points
=1mA=10m2
Ltot=1cm
A – cross section of e-m mode
Typical numbers
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Experimental detection of the Luttinger liquid of photons
Control beam off.Coherent pulse of non-interacting photons enters the fiber.
Control beam switched on adiabatically.Converts the pulse into a Luttinger liquidof photons.
“Fermionization” of photons detected by observing oscillations in g2
c
K – Luttinger parameter
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Non-equilibrium dynamics of strongly correlated many-body systems
g2 for expanding Tonks gas with
adiabatic switching of interactions
100 photons after expansion
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Outlook
Atomic physics and quantum optics traditionally study non-equilibrium coherent quantum dynamics of relatively simple systems.
Condensed matter physics analyzes complicated electron systembut focuses on the ground state and small excitations around it.
We will need the expertise of both fields
Next challenge in studying quantum coherence:understand non-equilibrium coherent quantum dynamics of strongly correlated many-body systems
“…The primary objective of the JQI is to develop a world class research institute that will explore coherent quantum phenomena and thereby lay the foundation for engineering and controlling complex quantum systems…”
From the JQI web page http://jqi.umd.edu/