Two-gap superconductivity in R2Fe3Si5 (R=Lu, Sc) and Sc5Ir4Si10

R2Fe3Si5 (R = Sc, Y, Lu) contains nonmagnetic iron and has a relatively high superconducting transition temperature T-c among iron-containing superconductors. An anomalous temperature dependence of specific heat C(T) has been reported for polycrystalline samples down to 1 K. We have grown R2Fe3Si5 single crystals, confirmed the anomalous C(T) dependence, and found a second drop in specific heat below 1 K. In Lu2Fe3Si5, we can reproduce C(T) below T-c, assuming two distinct energy gaps 2 Delta(1)/k(B)T(c) = 4.4 and 2 Delta(2)/k(B)T(c) = 1.1, with nearly equal weights, indicating that Lu2Fe3Si5 is a two-gap superconductor similar to MgB2. Hall coefficient measurements and band structure calculation also support the multiband contributions to the normal-state properties. The specific heat in the Sc2Fe3Si5 single crystals also shows the two-gap feature. R5Ir4Si10 (R = Sc, rare earth) is also a superconductor where competition between superconductivity and the charge-density wave is known for rare earths but not for Sc. We have performed detailed specific heat measurements on Sc5Ir4Si10 single crystals and found that C(T) deviates slightly from the behavior expected for weak-coupling superconductors. C(T) for these superconductors can also be reproduced well by assuming two superconducting gaps.