spectroscopy of ultracold bosons by periodic lattice modulations
DESCRIPTION
Spectroscopy of ultracold bosons by periodic lattice modulations. 2D. 1D. A. Iucci , C.Kollath, T. Giamarchi, W. Hofstetter, and U. Schollwöck. Superfluid-Mott insulating transition. Bose-Fermi mixtures. Mainz/München. Low-dimensional systems. LENS. disordered systems. ETHZ. - PowerPoint PPT PresentationTRANSCRIPT
1 A. Iucci Spectroscopy of ultracold bosons
Mainz/München
1D 2D
Spectroscopy of ultracold bosons by periodic lattice modulations
Superfluid-Mott insulating transition
Bose-Fermi mixtures
Low-dimensional systems
A. Iucci, C.Kollath, T. Giamarchi, W. Hofstetter, and U. Schollwöck
disordered systems
LENS
ETHZ
2 A. Iucci Spectroscopy of ultracold bosons
Probing cold atoms
noise measurement:
-> density-density correlations
time-of-flight measurement
-> momentum distribution
periodic lattice modulation
-> energy spectrum
ETHZ
Mainz/München
Mainz
& (in)commensurability
3 A. Iucci Spectroscopy of ultracold bosons
Experimental resultsResponse to a periodic modulation
periodic modulation of optical lattice height
T. Stöferle et al. PRL 92, 130403
ab
sorb
ed
en
erg
y
4 A. Iucci Spectroscopy of ultracold bosons
Bosonic atoms in an optical lattice
kinetic energyinteraction energy
1
†1
11
( 1) .2
.M
jj
j
M
jjj
J b bH n hn cU
periodic modulation of lattice height
-> time dependent J(t) and U(t)
explicitly time-dependent Hamiltonian
experimental parameter -> J and U
Methods: - adaptive t-DMRG- linear response
5 A. Iucci Spectroscopy of ultracold bosons
two particle hole excitations -> energy 2U
Strong interaction
single particle hole excitation -> energy U
response to periodic modulation -> creation of excitations
-> expect peaks at multiples of U
U 2U 3U ħ abso
rbed e
nerg
y
6 A. Iucci Spectroscopy of ultracold bosons
Energy absorption
L=24
L=32 at resonance
ħ=U
away of resonance
abso
rbed
en
erg
y
C. Kollath et al. cond-mat 2006
7 A. Iucci Spectroscopy of ultracold bosons
Energy absorption at commensurate filling
experiment
• peak at U
• small peak at U/2
• no peak at higher frequencies
U/J =72
?
U/J =95
abso
rpti
on r
ate
linear response: A. Iucci et al. accepted by PRA
U 2U
8 A. Iucci Spectroscopy of ultracold bosons
Energy absorption at incommensurate filling
• peak at U
• peak at 2U
experiment
ab
sorp
tion
rate
U/J =95
n~1.2
experiment
U/J =72
9 A. Iucci Spectroscopy of ultracold bosons
2U peak
corresponding processes
two particle-hole excitations single particle-hole excitation
2U peak measure of incommensurability
10 A. Iucci Spectroscopy of ultracold bosons
Intermediate interaction strength
peaks at U, 1.9 U, and 2.6 U
abso
rbed e
nerg
y
experimental results:
peaks at approx. U, 1.9 U, and 2.6 U
U/J =28
U 1.9U
2.6U
T. Stöferle et al. PRL 92, 130403
11 A. Iucci Spectroscopy of ultracold bosons
Energy absorption at incommensurate filling
• peaks at U, 2.1 U, and 2.6 U
• shift of position of energy eigenvalues
at incommensurate filling
U/J =9
n~1.2
a
bso
rpti
on r
ate
12 A. Iucci Spectroscopy of ultracold bosons
Positions of peaks
small system at incommensurate filling:
• position shifts,
• splitting of peaks
0.1 0.2 0.3
J/U
13 A. Iucci Spectroscopy of ultracold bosons
20% perturbation -> beyond linear response
absorption rate, 1% modulation (scaled)
absorption rate, 20% modulation
integrated absorption, 20% modulation
saturation effects occur
in height and width
14 A. Iucci Spectroscopy of ultracold bosons
Summary
occurence of higher frequency peaks for incommensurate filling: confining potential, temperature
shift in peak position stem from shift in energy
20% perturbation -> saturation effects in width and height
not described by linear response
full time-dependent calculation: adaptive t-DMRGmany more applications possible