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Fragmentation and Stillbirth of
Condensation in the Rapidly
Evaporative Cooling of a Dual
Species Bose Mixture
Shih-Chuan GouDepartment of Physics
National Chanhua University of Education
Outline
1. Review of Experimental Results
2. Stochastic Projected GPEs
3. Numerical Simulations
4. Summary
1. Experimental Results
1. Experimental Results
85 85 87 87
2
85 87
1a a
a
Phys. Rev. Lett. 101, 040402(2008)
1. Experimental Results
Phys. Rev. Lett. 101, 040402(2008)
85 87 2, 2 , 1, 1f fRb f m Rb f m
1. Experimental Results
• S. B. Papp et. al. reported that the two-component BEC
may fail to form if the particle number of one
component is too large at the start of evaporation. The
experiment is carried out in an extremely elongated
cigar-shape trap.
1. Experimental Results
Phys. Rev. Lett. 101, 040402(2008)
N85=1.2x104
N85=2.2x104
N87=1.4x105
N87=3x103
Fail to condense
2. Stochastic Projected GPEs
Phys. Rev. A 77, 033616 (2008).
The c-field theory
Scattering and growth of the
condensate particles
, ,, ,GP GP
B
t dW ti H t H t
t k T dt
x xx x
pP
2 22
, (BEC in rotation) 2
/ (random white noise)
GP
j B j j
j
H V g t m
dW k Tdt i
x x
x
2. Stochastic Projected GPEs
• The atoms are confined in an elongated trap with.
87 872 2.9Hz and 2 130Hzz r
2
( ) ( )
( ) exp2
i ri i ri
i i i
i
r z
m mr r
2 2
22 2 2
1,2
( ) 2 21
2 2GP i z ri zi ij
ji
ii j iH m r z g
m
22 2 21 2 121 2
12 21
1 2 1 2
24,
2
i r z ii r rii
i z r z r
m m am a m mg g g
m m m m m
2. Stochastic Projected GPEs
22
1,2
2( ) 2
2
1( )
2 2
: complex whi
,ˆ , ,
te noise
: s-wave scattering length
1,
s.
2
GP i i z c
iGP GP
i ij
ji
j B j
B
j
ii j i
ij
ii iii i i
dW t
H m z z gm z
dW k
iP H t H t i
t k T d
Tdt i
a
t
xx
x
x
Phys. Rev. A 77, 033616 (2008).
3. Numerical Resultand Fragmentation
3. Numerical Result
• Parameters:
1.aspect ratio of scattering length
α2 ≡ a2 /a1
α12≡a12/a1
2.T=100nK
3. Numerical Result
• Case of No Condensation
Phys. Rev. Lett. 101, 040402(2008)
3. Numerical Resultα2=0.515, α12=2.15
μRb87=120, μRb85=170
γ=0.03
3. Numerical Result
α2=0.515, α12=2.15
μ1=120, μ2=170, γ=0.03
3. Fragmentation
• Fragmentation of condensate means that
• there are more than one macroscopically
populated state in the system.
• In other word, there is more than one comparable
eigenvalue of one particle density matrix
(Onsager criterion).
3. Fragmentation
• We diagonalize the density matrix of each component to verify
the condensate is fragmented or not.
• (Averaging via a short time to approach the ensemble under
the ergodic hypothesis)
• If the order of number of occupied state approach to the
order of particle number,
→Fail To Condense
Phys. Rev. A 77, 033616 (2008)
/2
/2
( ) ( )1( )
( ) ( )
t ti i
it t
i i
t tt dt
t Tr t t
sN
3. Numerical Result
3. Numerical Result
• Asymmetrically Immiscible Case
Phys. Rev. Lett. 101, 040402(2008)
3. Numerical Result
α2=0.515, α12=2.15
μ1=325, μ2=166, γ=0.1
3. Numerical Result
α2=0.515, α12=2.15
μ1=325, μ2=166, γ=0.03
3. Numerical Result
3. Numerical Result
3. Numerical Result
Multi Domain Formation Induced by Modulation Instabilit in Two Component BEC, Phys. Rev. Lett. 93, 100402(2004)
3. Numerical Result
• Miscible Case
Phys. Rev. Lett. 101, 040402(2008)
3. Numerical Result
α2=7.88, α12=2.15
μ1=125, μ2=300, γ=0.12
3. Numerical Result
α2=7.88, α12=2.15
μ1=125, μ2=300, γ=0.12
3. Numerical Result
4. Summary
1. We apply the SPGPEs to dual-species condensate, and get a good
agreement with experimental results.
2. We verify three scenarios for the growth of phase-separated
condensates:
(1) The successful formation of two BECs without fragmentation.
(2) The formation of two BECs, yet one of them is fragmented.
(3) One species is condensed without fragmentation, while the other
is stillborn.
3. Attempt to simulate the synthetic cooling of 133Cs-87Rb mixture by
using SPGPE + PGPE.
Reference
• [1] S. B. Papp et. al., Phys. Rev. Lett. 101, 040402 (2008).
• [2] A. S. Bradley et. al., Phys. Rev. A 77, 033616 (2008).
• [3] Alexej I. Streltsov et. al., Phys. Rev. A 70, 053607 (2004).
• [4] M. Ueda, Fundamentals and New Frontiers of Bose-
Einstein Condensation(2010).
Thanks for your attention.