Title: TFVS
1TFVS
Two atoms in a 1D Optical Lattice close to a
Feshbach Resonance
M. Wouters
In collaboration with G. Orso, L.P. Pitaevskii,
S. Stringari
NQS2005, Camerino, july 6th, 2005
2Motivation
Introduction
Experiments with ultra-cold atoms
M. Greiner, C. A. Regal, D.S. Jin, Proceedings of
ICAP-2004 (Rio de Janeiro) condmat/0502539
3Periodic Potential
Introduction
d
Recoil energy
sER
r
z1
z2
- Center of mass and relative motion dont
decouple - No nice analytical wave functions
G. Orso, L.P. Pitaevskii, S. Stringari, M.W.,
cond-mat/0503096, accepted to PRL
4Harmonic confinement
Introduction
Harmonic confinement in z-direction separation
of relative and c.om. motion
Bound state for any a!
1 D.S. Petrov, G.V. Shlyapnikov, Phys. Rev. A
64 (2000) 2 Z. Idziaszek and T. Calarco,
quant-ph/0410163
5Integral equation
Method
No separation of center of mass and relative
motion
Bethe-Peierls
takes regular part
Discrete translational symmetry
Q is quasi-momentum of the molecule
6Greens function
Method
Independent of energy and external potential
Handle the singularity
- Numerically
- Tight Binding
Analytically
7Qualitative picture
Results
0
8Binding energy
Results
Q 0
S20
10
5
0
9Critical scattering length
Results
Q 0
Q qB
10Binding energy at resonance
Results
Q 0
11Binding energy dispersion
Results
Center of mass motion and relative motion are
coupled
Binding energy depends on the quasi-momentum
S2.5
d/acr increases with quasi-momentum
12Band width dispersion
Results
The bandwidth depends strongly on the scattering
length (binding energy).
Possible to extract experimentally from Bloch
oscillations
13Effective mass dispersion
Results
Depends also strongly on the scattering length
(binding energy).
Possible to extract experimentally from
Bloch/dipole oscilations
14Conclusions/Perspectives
- Exact numerical method for any value of the laser
intensity and scattering length - Binding energy
- Tunneling properties
- 2D-3D optical lattices
- Scattering properties
- Analytical treatment
- Many body physics in 1D/2D/3D optical lattices
(coupled layers/tubes/Hubbard model)
15(No Transcript)
16Outline
Two atoms in a 1D Optical lattice close to a
Feshbach resonance
- Introduction
- Method
- Results
- Conclusions/Perspectives
17Resonant molecules
Introduction
Schrödinger Equation
Scattering length
For
Bound State
if
Matching the two expressions
18Resonant molecules
Introduction
more formal
with Green Function
Replace real interatomic potential with zero
range Pseudo-potential (Refs.)
where
if we choose
19Tight Binding
Method
Large s, small E
Ansatz
d/acr
Only lowest band contributes
Width of Wannier function
20Qualitative picture
Results
0