Phase diagram of the Bose Kondo-Hubbard model
arXiv:1103.0245 · doi:10.1103/PhysRevA.84.053619
Abstract
We study a bosonic version of the Kondo lattice model with an on-site repulsion in the conduction band, implemented with alkali atoms in two bands of an optical lattice. Using both weak and strong-coupling perturbation theory, we find that at unit filling of the conduction bosons the superfluid to Mott insulator transition should be accompanied by a magnetic transition from a ferromagnet (in the superfluid) to a paramagnet (in the Mott insulator). Furthermore, an analytic treatment of Gutzwiller mean-field theory reveals that quantum spin fluctuations induced by the Kondo exchange cause the otherwise continuous superfluid to Mott-insulator phase transition to be first order. We show that lattice separability imposes a serious constraint on proposals to exploit excited bands for quantum simulations, and discuss a way to overcome this constraint in the context of our model by using an experimentally realized non-separable lattice. A method to probe the first-order nature of the transition based on collapses and revivals of the matter-wave field is also discussed.
10 pages, 5 figures, V2: extended discussion of effective Hamiltonians and mean-field theory, added Fig. 3
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- Variational principle for quantum impurity systems in and out of equilibrium: application to Kondo problems
- First order phase transitions in optical lattices with tunable three-body onsite interaction
- Confined p-band Bose-Einstein condensates
- Exotic phases of interacting p-band bosons
- Efficient variational approach to dynamics of a spatially extended bosonic Kondo model
- Finite temperature phase diagram of spin-1/2 bosons in two-dimensional optical lattice
- Bosonic Kondo-Hubbard model
- Mode folding in systems with local interaction: unitary and non-unitary transformations using tensor states
- Bosonic Peierls state emerging from the one-dimensional Ising-Kondo interaction