hui deng stephan gotzinger david press yoshihisa yamamoto robin huang hui cao francesco tassone...
Post on 19-Dec-2015
217 views
TRANSCRIPT
Hui DengStephan Gotzinger
David PressYoshihisa
Yamamoto
Robin HuangHui Cao
Francesco Tassone
Gregor WeihsStanley Pau
(Former members)
Quantum Entanglement Project, SORST, JSTE.L. Ginzton Laboratory, Stanford University
andNational Institute of Informatics
BaCa Tec-Summer School, Würzburg, June 26 – July 01, 2005
2
Outline
• Microcavity exciton polaritons
• Polariton BEC vs. exciton BEC
• Non-equilibrium, quasi-equilibrium and thermal equilibrium BEC
• Final state stimulation in exciton-exciton scattering processes
• Amplification of exciton polaritons
• Dynamic condensation (lasing) of exciton polaritons in CdTe and GaAs MQW-microcavities
Polariton population per state N(k//)
Effective mass
Relaxation time polariton vs. lifetime 0
Momentum and real space distributions Chemical potential and polariton temperature Second order coherence function
• Transverse confinement of exciton polaritons
2
//
2
2
1
dk
Ed
Microcavity Exciton Polaritons
4
Wannier-Mott Excitons in Quantum Wells
Momentum eigenstate – A valence electron with and is excited to a conduction electron with andk ''k
Exciton state
mode index envelope function in k-space
plane wave hole electron
momentum eigenstate
5
kKkk
vkkkk
vKv
Kk
kkkkKKvC ˆˆ)
2( ˆˆ)
2
'())'(( |0,| '
',,
Exciton creation operator
)(1],[ *0,0,
dBexcvv anOCC Composite boson in the
1st order approximation
Exciton Hamiltonian
22 )(42
1)(
2
1phexkphexk
g
002g
kkkkkavCuP ˆˆˆ Diagonalize with polariton operator:
Hamiltonian of Coupled Cavity Photon-QW Exciton
Rabi-splitting: when cavity photon on resonance with bare exciton
k
kkkTPPhH ˆˆˆ
kkkkkkkkkkph
CaCaigCCexcaahH )ˆˆˆˆ(ˆˆˆˆˆ
k kk CCexchH ˆˆˆ0
QW Excitons and Microcavity Polaritons
6
1 or 2?
1 or 2?
r’A
rB
rA
r’B
e1 r’A h1 rA
e2 r’B h2 rB
~
+ e1 r’A h2 rA
e2 r’B h1 rB
e2 r’A h1 rA
e1 r’B h2 rB
e2 r’A h2 rA
e1 r’B h1 rB
ex2 rA ex1 rB
ex1 rA ex2 rB
+ 12
=
Two-Exciton State:
Spatial Correlation induced by Coulomb Interaction.
A composite particle (exciton) behaves as a “massive boson”.
Exciton as a Composite Boson
7
Polariton dispersion curves
Rabi splitting
exc0 = ph0
E
k //
QW exciton
Lower polariton
Upper plariton
Microcavity photon (mph ~ 10-5 me)
(mexc ~ 10-1 me)
(meff ~ 2 mph)
osc~ 1 THz
C. Weisbuch, et al. Phys. Rev. Lett. 69, 3314 (1992)
S. Jiang et al., Appl. Phys. Lett. 73, 3031 (1998)
Exciton Polariton Dispersion, Normal Mode Splitting and Oscillation
UP LP
OSC 1THz ~
8
Atom Cavity QED vs. Semiconductor Cavity QED
single-atom cavity QED many-atom cavity QED exciton cavity QED
single atom ensemble of atoms
QWs
d: atomic dipole momentV: optical mode volume
eigenstate of collective angular momentum
(J =N/2, N: # of atoms)
effective # of atomic oscillators:
S: cavity mode area, ~2m : Bohr radius, ~100
Non-equilibrium Polariton Laser vs. Equilibrium Polariton BEC
10
Dynamic vs. Equilibrium Condensation
Polariton decay vs. Two relaxation processes
exciton-phonon scattering
phonon phonon
k//
equilibrium is established with a lattice at lattice
exciton-exciton scattering
k//
equilibrium is established within polaritons at polariton
Non-equilibrium(multi-mode polariton laser)
Quasi-equilibrium(single-mode polariton laser)
Thermal equilibrium(polariton BEC)
0<polaritonlattice
polariton not defined
polariton0<lattice
polariton > Tlattice
polariton<lattice 0
polariton = Tlattice
Fragmentation of the condensate
Fock exchange term
Dynamic single-state condensation
Steady state single- state condensation
polariton decay
k//
polariton decay by leakage of photonic component at 0
leakage photon
11
Polariton BEC vs. Exciton BEC
Enemies of exciton BEC:Dissociation of excitons (screening, phase space filling)Disorder, localization and inhomogeneous broadening
Advantage of Polariton BECExtended phase coherence reinforced by a cavity field
suppressed localization, disorder and inhomogeneous broadening
Light effective mass by dressing a cavity field
mpolariton ~ 10-4 mexciton ~ 10-7 mH-atom
Enhanced binding energy/decreased Bohr radius in the very-strong-coupling regime
[J. B. Khurgin et. al., Solid State Commun. 117, 307 (2002)]
suppressed dissociation of excitonsPhotonic component out-coupling from the cavity with k conservation in contrast to spontaneous decay of an un-dressed exciton
direct experimental access to internal polariton population
higher critical temperaturelower particle density
Bosonic Final State Stimulation
13
Exciton-polariton Nonlinear Interaction
NLL HHH
))(( ))(( 21 bbbbUbbbbUH NL
h.c.bbbabbba ))((2
T ))((
2
T 21
same spins opposite spins
-3 -2 -1 0 1 2 30
0.5
1
1.5
2
2.5
3
3.5
U1
T1/2 T1/2
ExcitonLP UP
smaller spitting
Blue shift
, 21, nUnUh exc
• M. Kuwata-Gonokami et al., Phys. Rev. Lett. 79, 1341 (1997)• S. Schmitt-Rink, et al., Phys. Rev. B 32, 6601 (1985)• J. Fernandez-Rossier et al., Phys. Rev. B 54, 11582 (1996)• J. Inoue, et al., Phys. Rev. B 61, 2863 (2000)
)( bababbaaH exccavL
nTnT 21
14
Measurement of Exciton Interaction – Pump-probe experiments with optical heterodyne detection
Experimental results
Probe Energy
Experimental setup
Excitons with same spins
(theory)(experiment)
(Fermionic exchange + phase space filling)
(theory)(experiment)
(Fermionic exchange)
15
Idea:UP=background free measurement window
leakage from cavity phonon scattering exciton-exciton scattering
Stimulated
scattering
0 0 0, , , (1 )UPUP k LP k k LP k LP k LP
kUP
ndn a n b n n n
dt
exc. beamexc. beam
Spontaneous
scattering
16
Observation of Bosonic Final State Stimulationin exciton-exciton scattering in a GaAs SQW-Microcavity
nexc = 1.5109 cm-2
1.2
0.54
R. Huang et al., Phys. Rev. B 61, R7854 (2000)
• Upper-polariton emission decay time ~ 95 ps
• bottle-neck polariton decay time ~ 190 ps
Amplification of Exciton Polaritons —Probing Quantum Degeneracy
18
Strong Coupling to Weak Coupling Transition
Normal mode splitting at resonance (c=exc)
(weak coupling)
polaritoncavity photon
Exciton densities:A: 1.1108 cm-2 , B: 1.1109 cm-2 , C: 5.5109 cm-2 , D: 1.11010 cm-2 , E: 2.01010 cm-2 , F: 2.71010 cm-2 G:
4.41010 cm-2 , H: 6.61010 cm-2 , I: 1.11010 cm-2S. Jiang et al., Appl. Phys. Lett. 73, 3031 (1998)
19
1. Exciton localization and inhomogeneous broadening
Dressing QW excitons with a microcavity vacuum field
Strong coupling to weak coupling transition when an exciton decoherence rate exceeds a normal mode splitting.
Use of multiple QWs
Use of excitons with small Bohr radius
populationpolaritongivenafor1 QWexc
QWRabi
Nn
N
MQWsGaAs12
2*sat 1 Ban
DQWCdTe
2. Exciton saturation
QW excitons are easily trapped by a local minimum of a QW potential fluctuation.
Comparison of Exciton Properties
2510Binding Energy (meV)
2890Bohr Radius in QW(A)
504Saturation Density
(1010 cm-2)
CdTeGaAs
Obstacles and Tricks for Polariton Lasing
Rabiousinhomogene extended phase coherence
20
Gain=15
BareExcitonk// = 0:LP
Bottleneckeffect
Bottleneck Exciton decay rate = 120 ps
Gain decay rate = 60 ps
A CdTe QW exciton survives at higher densities due to small Bohr radius.
R. Huang et al., Phys. Rev. B 65, 165314 (2002)
Observation of Stimulated Scattering Gainin a CdTe DQW-Microcavity
A gain is provided by two-body exciton-exciton scattering.
21
Nexc=3.4x106 Gain =23
Nexc=1.6x106
Gain =5.4
Nexc = 0.41x106
Gain = 0.34
)exp( 2excNconstg
Probe (mW/cm2) Circles: 2104 Squares: 900
Rate equationsolutions
21exc
Nconstg Low Gain Regime High Gain Regime
R. Huang et al., Phys. Rev. B 65, 165314 (2002)
)1()1(2
lpexlplpexlpnnbnna
exciton-phononscattering
exciton-excitonscattering
lp
lp
lplp τ
nPndt
d
A. Imamoglu et al.Phys. Rev. A 53, 4250 (1996)
F. Tassone et al.,Phys. Rev. B 59, 10830 (1999)
Amplification of Polaritonsin a CdTe DQW-Microcavity
22
Spontaneous build-up of ground state populationPolariton effective massSpontaneous spin polarizationSecond order coherenceReal space distribution (spontaneous localization)Momentum space distribution (BE) (chemical potential and temperature)
Experimental evidence:
Dynamic Condensation (Lasing) of Exciton Polaritons
23
Polariton Lasing vs. Photon Lasing
109 1010 1011 1012
10-1
100
101
102
103
with inversion
Fig. 2
ph
oto
ns
pe
r ca
vity
mo
de
at
k||~
0
polariton, Elp=1.6166 eV
cavity mode, Ecav
=1.6477 eV
injected carrier density (cm-2)
po
lari
ton
s p
er
mo
de
at
k||~
0
100
no electronic inversion
lasing threshold observed without electronic population inversion
H. Deng et al., Proc. Natl. Acad. Sci., 100, 15318 (2003)
polariton laser
standard photonlaser
24
Effective Mass Measurement: Polariton and Photon Dispersions
-2 0 2
1.612
1.614
1.616
1.618
1.62
k|| (10 4 cm -1)
Ene
rgy
(eV
)
P/Pth
=7.6-2 0 2
1.646
1.648
1.65
1.652
1.654
k|| (10 4 cm -1)
Ene
rgy
(eV
)
photon laser P/P'
th=3
-2 0 2
1.612
1.614
1.616
1.618
1.62
k|| (10 4 cm -1)
Ene
rgy
(eV
)
P/Pth
=0.5
photon
polariton
Polariton Laser
Photon Laser
polariton mass measured to be ~ twice the photon mass
strong-coupling preserved above threshold
H. Deng et al., Proc. Natl. Acad. Sci., 100, 15318 (2003)
25
Spontaneous Spin Polarization
26
Second Order Coherence (Hanbury Brown-Twiss experiment)
21
21
2)()(
)()()()(
)2()()(
)(ˆ)(ˆ
)(ˆ)(ˆ)(ˆ)(ˆ)(
nn
jinin
tEtE
tEtEtEtEg i
single-mode coherent state
Poissonian light
single-mode thermal state
102 g
102 g
202 g
H. Deng et al., Science 298, 199 (2002)
The on-set of bosonic final state stimulation manifests itself by increased g (2)(0). A gradual decrease in g(2)(0) suggests non-standard macroscopic coherence.
27
Real Space Distribution
photon laserfitted spot size: 26 m
polariton lasersuppressed ‘expansion’
P/Pth = 1.5
polariton photon
below thresholdbroad Gaussian
above thresholdsteep central peak
28
0 0.5 1 1.5 2 2.5 3 3.5 40
0.2
0.4
0.6
0.8
1
1.2
1.4
k|| (104cm-1)
n (
k ||)
(a.u
.)
Momentum Space Distribution
Exp. Data
BE Fit
MB Fit
P/Pth =1.5
0 1 2 3 40
0.5
1
k|| (104cm-1)
n (k
||)
(a.u
.)
P/Pth =0.6
resolution
H. Deng et al., Proc. Natl. Acad. Sci., 100, 15318 (2003)
J . Keeling et al., Phys. Rev. Lett. 93, 226403 (2004)
The k-distribution is in agreement with BE distribution, except for the population at k11=0.
29
Chemical Potential and Effective Temperature
• chemical potential ~ -kBT at threshold• chemical potential zero above threshold
fitted polariton temperaturefitted (normalized) chemical potential
1 1.2 1.4 1.60
20
40
60
80
100
120
140
160
P/Pth
TL
P (K
)
1 1.2 1.4 1.60
0.5
1
1.5
2
P/Pth
=
- /
(kBT
)
1 1.2 1.4 1.6
-6
-4
-2
(me
V)
Tpolariton >> Tlattice
BEC threshold
H. Deng et al., Proc. Natl. Acad. Sci., 100, 15318 (2003)
From Non-equilibrium Polariton Laser To Equilibrium Polariton BEC
31
Relaxation Rate vs. Decay Rate of Polaritons
Non-equilibrium
Equilibrium
0 0
0
R R R
R relax
R
relax
cavity photon
dN N NP t
dt
dN N N
dt
E E
32
Future Prospects
Room temperature polariton laser (GaN (NTT) , ZnSe (Paderborn) , ·····)
Practical issues:Practical issues:
Very low-threshold and very fast (~psec) coherent light source
Theoretical issues:Theoretical issues:Bogoliubov theory predicting a squeezed ground state
F. Tassone et al., Phys.Rev.B59,10830(1999)F.P. Laussy et al., Phys. Rev. Lett. 93, 016402
(2004)
0 0exp vack k kb b b
phase-locked
Transverse confinement and long polariton lifetime by a 2D photonic crystal or microdisk cavity
BEC BCS phase transition Impurity bound exciton in homogeneous bulk (F. M. Marchetti, et al., arXiv:cond-mat/0405295)
Acknowledgement
Atac Imamoglu, David Snoke, Jacqueline Bloch, Regis Andres, Hiromi Ezaki
Transverse confinement by a cavity trap (V~10meV for 12 GaAs MQW)
33
-3 -2 -1 0 1 2 3
-10
-5
0QW exciton energy
cavity field amplitudeat MQWs
LP energy
en
erg
y (
me
V)
x (m)
pillar size, 5 m
Optical Trapping of Microcavity Polaritons
-4 -2 0 2 4 6 8
764
766
768
770
772
774
position on sample (mm), dy~7/3 dx
wav
ele
ng
th (
nm
)
detuning by reflection measuremnt
2 4 6 81010152025304050
exc
=768.8nm
pillar size (m)
LP
UP ~ 6.8 nm
A. Forchel (Würzburg)
34
UP
LP
condensate
normalstate
thick lines: quasi-particle excitations in the condensed phase upper line: creating a quasi-particle lower line: absorbing a quasi-particle
gap4g|
Coherent light
BEC-BCS Phase Transition
M.H. Szymanska et al., Solid State Comm. 124, 103 (2002)