  We show that ultracold atoms can be controlled in multi-band optical lattices
through spatially periodic Raman pulses for investigation of a class of
strongly correlated physics related to the Kondo problem. The underlying
dynamics of this system is described by a spin-dependent fermionic or bosonic
Kondo-Hubbard lattice model even if we have only spin-independent atomic
collision interaction. We solve the bosonic Kondo-Hubbard lattice model through
a mean-field approximation, and the result shows a clear phase transition from
the ferromagnetic superfluid to the Kondo-signet insulator at the integer
filling.
