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Mean-field theory for the Mott-insulator–paired-superfluid phase transition in the two-species Bose-Hubbard model
The standard mean-field theory for the Mott-insulator–superfluid phase transition is not sufficient to describe the Mott-insulator–paired-superfluid phase transition. Therefore, by restricting the two-species Bose-Hubbard Hamiltonian to the subspace of paired particles, and using perturbation theory
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