We measured the microwave surface impedance of FeSe$_{ 0.4}$Te$_{ 0.6}$ single crystals with- and without external magnetic fields. The superfluid density exhibited a quadratic temperature dependence, indicating a strong pair-breaking effect. The flux-flow resistivity behaved as $\rho_f(B\ll B_{ \rm c2})/\rho_n=\alpha B/B_{ \rm c2}$. The observed $\alpha$ value of $\approx0.66$ was considerably smaller than that of other Fe-based materials ($\alpha\geq1$) and was attributed to a back-flow of superfluids remarkable in disordered superconductors. This is the first-time observation of the back-flow phenomenon caused by an origin other than the vortex pinning in multiple-band systems.
Categories: cond-mat.supr-con