Abstract
Based on the London equation, we use a rotor-free vector potential A and current measurements by a SQUID, to determine the superconducting (SC) Pearl length Λ and coherence length ξ 0, of ultra-thin, ring shaped, MoSi films, as a function of thickness d and temperature T. We find that T c and ξ 0 are functions of d and both jump at nm. At base temperature the SC stiffness, defined by , is an increasing function of T c . Similar behavior, known as the Uemura plot, exists in bulk layered superconductors, but with doping as an implicit parameter. We also provide the critical exponents of .
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