Title: Quantum Monte Carlo methods
1- Quantum Monte Carlo methods
- applied to ultracold gases
-
- Stefano Giorgini
-
-
- Istituto Nazionale per la Fisica della Materia
Research and Development Center
on Bose-Einstein Condensation - Dipartimento di Fisica Università di Trento
BEC CNR-INFM meeting 2-3 May 2006
2- QMC simulations have become an important tool in
the study of dilute ultracold gases - Critical phenomena
- Shift of Tc in 3D Grüter et al. (97), Holzmann
and Krauth (99), Kashurnikov et al. (01) - Kosterlitz-Thouless Tc in 2D Prokofev et al.
(01) - Low dimensions
- Large scattering length in 1D and 2D Trento (04
- 05) - Quantum phase transitions in optical lattices
- Bose-Hubbard model in harmonic traps Batrouni et
al. (02) -
- Strongly correlated fermions
- BCS-BEC crossover Carlson et al. (03), Trento
(04 - 05) - Thermodynamics and Tc at unitarity Bulgac et
al. (06), Burovski et al. (06)
3- Continuous-space QMC methods
- Zero temperature
- Solution of the many-body Schrödinger equation
- Variational Monte Carlo
- Based on variational principle
- energy upper bound
- Diffusion Monte Carlo
- exact method for the ground state of Bose
systems -
- Fixed-node Diffusion Monte Carlo (fermions and
excited states) - exact for a given nodal surface ? energy
upper bound - Finite temperature
- Partition function of quantum many-body system
- Path Integral Monte Carlo
- exact method for Bose systems
-
4- Low dimensions large scattering length
5- 1D Hamiltonian
- if g1D large and negative (na1Dltlt1) metastable
gas-like state of hard-rods of size a1D
g1Dgt0 Lieb-Liniger Hamiltonian (1963) g1Dlt0
ground-state is a cluster state
(McGuire 1964)
Olshanii (1998)
at na1D ? 0.35 the inverse compressibility
vanishes
gas-like state rapidly disappears forming clusters
6- Correlations are stronger than in the
Tonks-Girardeau gas - (Super-Tonks regime)
Power-law decay in OBDM
Peak in static structure factor
Breathing mode in harmonic traps
TG
mean field
7- Equation of state of a 2D Bose gas
Universality and beyond mean-field effects
- hard disk
- soft disk
- zero-range
for zero-range potential mc20 at
na2D2?0.04 onset of instability for cluster
formation
8- BCS-BEC crossover in a Fermi gas at T0
-1/kFa
BCS
BEC
9Equation of state
beyond mean-field effects confirmed by study of
collective modes (Grimm)
BEC regime gas of molecules mass 2m - density
n/2 scattering length am
am0.6 a (four-body calculation of Petrov et
al.) am0.62(1) a (best fit to FN-DMC)
10- Frequency of radial mode (Innsbruck)
QMC equation of state
Mean-field equation of state
11JILA in traps
Condensate fraction
12- Static structure factor (Trento Paris ENS
collaboration) - ( can be measured in Bragg scattering experiments)
at large momentum transfer kF ?? k ??
1/a crossover from S(k)2 free
molecules to S(k)1 free atoms
13- New projects
- Unitary Fermi gas in an optical lattice (G.
Astrakharchik Barcelona) -
- d1/q?/2? lattice spacing
- Filling 1 one fermion of each spin component
per site (Zürich) - Superfluid-insulator transition
- single-band Hubbard Hamiltonian is inadequate
14(No Transcript)
15S20
16- Bose gas at finite temperature (S. Pilati
Barcelona) - Equation of state and universality
-
-
T ? Tc
T ? Tc
17- Pair-correlation function and bunching effect
-
- Temperature dependence of condensate fraction
and superfluid density - ( N. Prokofevs help on implemention of
worm-algorithm)
T 0.5 Tc