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Physica A Statistical Mechanics and its Applications

Two-tag correlation functions in one-dimensional lattice gases

Satya N. Majumdar, Mustansir Barma

Published Sep 1, 1991• 30 citations
Publisher
DOI
10.1016/0378-4371(91)90174-b

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We investigate the thermodynamics of one-dimensional (1D) Bose gases in the strongly correlated regime. To this end, we prepare ensembles of independent 1D Bose gases in a two-dimensional optical lattice and perform high-resolution in situ imaging of the column-integrated density distribution. Using an inverse Abel transformation we derive effective one-dimensional line-density profiles and compare them to exact theoretical models. The high resolution allows for a direct thermometry of the trapped ensembles. The knowledge about the temperature enables us to extract thermodynamic equations of state such as the phase-space density, the entropy per particle, and the local pair-correlation function.
We study effects of the dipole-dipole interaction on fermionic cold atomic gases in two-dimensional optical lattice. We calculate spin and density correlation functions within the random-phase approximation. It is shown that the spin-correlation functions of spin components perpendicular to the lattice plane show a characteristic peak structure different from that of the parallel component. We study sss-wave and ddd-wave superfluidity induced by the spin and density correlations and show that the dipole-dipole interaction assists the ddd-wave superfluidity.
We investigate effects of optical lattice potential in one- and two-dimensional two-component trapped Fermi gases with population imbalances. Using the exact diagonalization and the density matrix renormalization group methods complementarily, we calculate the atom-density profile from the ground state many-body wave function as a function of attractive interaction strength for various population imbalances. The numerical results reveal that although a phase separation between the superfluid core and the shell cloud of excess atoms occurs as observed in experiments without the optical lattice, the population imbalance generally remains in the core region in contrast to the nonlattice cases. The essence of the numerical results in a strong attractive regime can be explained by an effective model composed of Cooper pairs and excess major fermions.