u‰‰ŽาF Huiqui Yuan ŽiNatinal High Magnetic Field Lab. Los Alamosj “๚ŽžF‚P‚QŒŽ@‚T“๚i…j@Œ฿Œใ‚RŽž‚O‚O•ช‚ฉ‚็ ๊ŠF ยŽRŠw‰@‘ๅŠw@—HŠw•”i‘Š–อŒดƒLƒƒƒ“ƒpƒXj‚k“‚UŠK@‚k‚U‚O‚RŽบ ‘่–ฺF uSuperconductivity in materials without inversion symmetryv —vŽ|F @The recent discovery of superconductivity in heavy fermion system CePt3Si has stimulated tremendous efforts to reveal the novel superconducting pairing state in materials lacking inversion symmetry. In this talk, I will present the results of magnetic penetration depth for the cubic systems Li2(Pd1-xPtx)3B and Y2C3. These materials lack inversion symmetry and show no evidence of magnetism or heavy fermion behavior, therefore providing us a great opportunity to study broken parity superconductivity. The low temperature penetration depth (T) shows an exponential behavior in Li2Pd3B, but follows a linear temperature dependence in Li2Pt3B. These results are best understood as arising from the admixing of spin-singlet and spin-triplet order parameters [H. Q. Yuan, et al., Phys. Rev. Lett. 97, 017006 (2006)], which is only allowed when inversion symmetry is broken. The triplet contribution is weak in Li2Pd3B, a BCS-like superconductor with an anisotropic gap. With increased spin-orbit coupling, the spin-triplet component dominates in Li2Pt3B, producing line nodes in the energy gap. Upon substituting Pd with Pt, we found that the triplet component eventually develops with increasing the Pt-content x. The existence of (T) ~ T over a wide Pd/Pt doping region indicates that the triplet state is rather robust against impurity scattering in non-centrosymmetric superconductors. In Y2C3, the low temperature penetration depth shows a weak linear temperature dependence, suggesting the existence of nodes in the superconducting energy gap. Again we attribute it to the admixture of spin singlet and spin-triplet states, as a result of broken inversion symmetry. --------------------------------- ‹ครF@ยŽRŠw‰@‘ๅŠw@—HŠw‰๏