POLARITON CONDENSATION IN TRAP MICROCAVITIES: AN ANALYTICAL APPROACH C. Trallero-Giner, A. V....
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![Page 1: POLARITON CONDENSATION IN TRAP MICROCAVITIES: AN ANALYTICAL APPROACH C. Trallero-Giner, A. V. Kavokin and T. C. H. Liew Havana University and CINVESTAV-DF.](https://reader035.fdocuments.us/reader035/viewer/2022062620/551ae1e6550346f70d8b46bc/html5/thumbnails/1.jpg)
POLARITON CONDENSATION POLARITON CONDENSATION IN TRAP MICROCAVITIES: AN IN TRAP MICROCAVITIES: AN
ANALYTICAL APPROACHANALYTICAL APPROACH
C. Trallero-Giner, A. V. Kavokin and T. C. H. Liew
Havana University and CINVESTAV-DF
University of Southampton
Ecole Polytechnique Fédérale de Lausanne
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OUTLINEOUTLINE
• Introduction
• Analytical approaches
• Results
• Conclusions
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Introduction
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![Page 5: POLARITON CONDENSATION IN TRAP MICROCAVITIES: AN ANALYTICAL APPROACH C. Trallero-Giner, A. V. Kavokin and T. C. H. Liew Havana University and CINVESTAV-DF.](https://reader035.fdocuments.us/reader035/viewer/2022062620/551ae1e6550346f70d8b46bc/html5/thumbnails/5.jpg)
-Photons from a laser create electron-hole pairs or excitons.
-The excitons and photons interaction form a new quantum state= polaritonpolariton.
Peter Littlewood SCIENCE VOL 316
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2 dimensional GaAs-based microcavity structure.Spatial strep trap ( R. Balili, et al. Science 316, 1007 (2007))
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two dimensional Gross-Pitaievskii equation
The description of the linearly polarized exciton polariton condensate formed in a lateral trap semiconductor microcavity:
α1 and α2 – self-interaction parameter ω – trap frequencym – exciton-polariton mass
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-Explicit analytical representations for the whole range of the self-interactionparameter α1+α2.
The main goal
-To show the range of validity.
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Thomas-Fermi approach
Experimentally it is not always the case
Analytical approaches
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Variational methodFor non-linear differential equation the variationalmethod is not well establish.
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.1
0.2
0.3
0.4
0.5
0.6
Numeric solution
ThomasFermi
VariationalMethod
x / l0
Norm
ali
zed
ord
er p
aram
ete
r (l 0)1
/2 x/l 0)
a)
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Gross-Pitaievskii integral equation
-Green function
Green function formalism
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-spectral representation
-Integral representation
-harmonic oscillator wavefunctions
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Perturbative method
It is useful to get simple expressions for μIt is useful to get simple expressions for μ00
and Φand Φ00 through a perturbation approach. through a perturbation approach.
∫|Φ0(r)|2dr=N
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Ψ0=Φ0/√N
-small term
∫| Ψ0|2dr=1
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-must fulfill the non-linear equation system
T is a fourth-range tensor
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Energy Λ/2
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-3 -2 -1 0 1 2 3 4 5
-0,5
0,0
0,5
1,0
1,5Numerical solution Analytical solution
ner
gy/
Universal result
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The normalized order parameter Ψ0
Hn(z) the Hermite polynomial
Ei(z)-the exponential integral; γ-the Euler constant
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Ψ(r)= Φ(r)/√N
r→r/l
0.4 0.8 1.2 1.6 2.0 2.4 2.8
0.1
0.2
0.3
0.4
0.5
r
Norm
alized o
der para
mete
r
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The polaritons have two allowed spin projections
If the absence of external magnetic field the ‘‘parallel spins’’ and ‘‘anti-parallel spin’’ states of noninteracting polaritons are degenerate.
The effect of a magnetic fieldThe effect of a magnetic field
To find the order parameter in a magnetic field we start with the spinor GPE:
We are in presence of two independent circular polarized states Φ±
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-Ω is the magnetic field splitting
-two coupled spinor GPEs for the two circularly polarized components Φ±
-α1 the interaction of excitons with parallel spin-α2 the interaction of excitons with anti-parallel spin
The normalization ∫|Φ±|dr = N±Ψ± (r)= Φ± (r)/√N ±
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Λ1=α1N+ /(2l2ћω)
Λ12=α2N- /(2l2ћω)
η=N+/N-
EnergiesEnergies
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μ +=(E+-Ω))/ ћω =1+0.159*(Λ1+Λ12)+ 0.0036*F+(Λ1,Λ12)
μ -=(E-+Ω))/ ћω =1+0.159*(Λ1/ η +Λ12 η)+ 0.0036*F-(Λ1/ η , Λ12 η)
F+=(3Λ1+2Λ12)(Λ1/η+ηΛ12)+Λ12(Λ1+Λ12)
F-=(3Λ1/η+2Λ12η)(Λ1+Λ12)+(Λ1/η+ηΛ12)Λ12η
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0.5 1.0 1.5 2.0 2.5
1.2
1.3
1.4
1.5
μ +=(E+-Ω))/ ћω
μ -=(E-+Ω))/ ћω
Λ1=α1N+ /(2l2ћω)
Λ12=α2N- /(2l2ћω)
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0.4 0.8 1.2 1.6
1.1
1.2
1.3
1.4
+= ( E+-
-= ( E-+
μ +=1+0.159*(Λ1+Λ12)+0.0036*F+(Λ1,Λ12)
μ -=1+0.159*(Λ1/ η +Λ12 η)+0.0036*F-(Λ1, Λ12)
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Order parameter for the two circularly Order parameter for the two circularly polarized polarized ΨΨ±± components. components.
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Λ1=1Λ12=0.4
Ψ± = Φ±/√N±
η=N+/N- =1
=0.6 =0.40.5 1.0 1.5 2.0 2.5
0.1
0.2
0.3
0.4
0.5_(r):N+=0.6N--
r
Norm
alized o
der para
mete
r
_(r):N+=0.4N-
r)
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Conclusions-We have provided analytical solution for the exciton-polariton condensate formed in a lateral trap semiconductor microcavity.
-An absolute estimation of the accuracy of the method
−3 < Λ < 3
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ΛΛ versus versus the detuning parameter the detuning parameter δδTypical Values GaAs
N~105-106
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-We extended the method to find the ground state of the condensate in a magnetic field
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3/
N+/N
-<1
3
--Validity of the methodValidity of the method
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THANKSTHANKS