“…Introduction of Pt-atoms at the Ni-sites creates remarkable modifications of the superconducting properties: the superconducting gap becomes isotropic and the material is pushed from the clean to the dirty limit. For example, variation of electronic specific heat C el as a function of temperature in the superconducting state in pure YNi 2 B 2 C follows a power law, C el ∼ (T/T c ) 3 (anisotropic energy gap) whereas it exhibits an exponential T-dependence in the material YNi 1.8 Pt 0.2 B 2 C (isotropic energy gap) [5,6]. T c is not affected significantly with the introduction of Pt (T c ∼ 12.2 K in YNi 1.8 Pt 0.2 B 2 C; T c = 15.5 K in YNi 2 B 2 C); however, variation of the upper critical field H c2 as a function of x clearly shows that the material passes from the clean limit to the dirty limit with the increase of x [7].…”