Abstract
An extended eight-component Bogoliubov-de Gennes equation is applied to study the Josephson effect between iron-based superconductors (SCs) with s±-wave pairing symmetry, separated by an ferromagnet (FM). The feature of damped oscillations of critical Josephson current as a function of FM thickness, the split of the peaks induced by the interband coupling is much different from that for the junction with the s±-wave SCs replaced by s++-wave ones. In particular, a 0−π transition as a function of interband coupling strength α is found to always exhibit with the corresponding dip shifting toward the larger α due to enhancing the spin polarization in the FM, while there exits no 0−π transition for the SC with s++-wave pairing symmetry. The two features can be used to identify the pairing symmetry in the iron pnictide SC different from the s++-wave one in MgB2. Experimentally, by adjusting the doping level in the s±-wave SCs, one can vary α.
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