We investigate the thermal physics of a Bose-Hubbard model with Rashba spin-orbit coupling starting from a strong coupling mean-field ground state. The essential role of the spin-orbit coupling is to promote condensation of the bosons at a finite wavevector . We find that the bosons display either homogeneous or phase-twisted or orbital ordered superfluid phases, depending on and the inter-species interaction strength . We show that an increase of leads to suppression of the critical interaction for the superfluid to Mott insulator transition in the ground state, and a reduction of the for superfluid to Bose-liquid transition at a fixed interaction. We capture the thermal broadening in the momentum distribution function, and the real space profiles of the thermally disordered magnetic textures, including their homogenization for . We provide a Landau theory based description of the ground state phase boundaries and thermal transition scales, and discuss experiments which can test our theory.

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