We study a model for two-species hard-core bosons in one dimension. In this model, the same-species bosons have a hard-core condition at the same site, while different-species bosons are allowed to occupy the same site with a local interaction . At half-filling, by Jordan-Wigner transformation, the model can be exactly mapped to a fermionic Hubbard model. Due to this correspondence, the phase transition from superfluid () to Mott insulator () can be explained by simple one-band theory at half-filling. By using an exact diagonalization method adopting a modified Lanczos method, we obtain the ground states as a function of for the lattice size upto . We calculate directional current-current correlation functions in this model, which indicate that there are some remaining counter-flow in the Mott insulating region () and co-flow in the charge-density-wave region () for the finite lattices.

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