Abstract

We study theoretically the Josephson effect between two time-reversal two-band superconductors, where we assume the equal-time spin-singlet ss-wave pair potential in each conduction band. %as well as the band asymmetry and the band hybridization in the normal state. The superconducting phase at the first band φ1φ_1 and that at the second band φ2φ_2 characterize a two-band superconducting state. We consider a Josephson junction where an insulating barrier separates two such two-band superconductors. By applying the tunnel Hamiltonian description, the Josephson current is calculated in terms of the anomalous Green's function on either side of the junction. We find that the Josephson current consists of three components which depend on three types of phase differences across the junction: the phase difference at the first band δφ1δφ_1, the phase difference at the second band δφ2δφ_2, and the difference at the center-of-mass phase δ(φ1+φ2)/2δ(φ_1+φ_2)/2. A Cooper pairs generated by the band hybridization carries the last current component. In some cases, the current-phase relationship deviates from the sinusoidal function as a result of time-reversal symmetry breaking down.

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