Abstract

We report on the lower critical field of fullerene superconductors derived from a "trapped magnetic moment" method. Superconducting ${\mathrm{K}}_{3}$${\mathrm{C}}_{60}$, ${\mathrm{Rb}}_{3}$${\mathrm{C}}_{60}$, and Rb${\mathrm{Cs}}_{2}$${\mathrm{C}}_{60}$ crystals and powders with shielding fractions between 3 and 100% were investigated. In contrast to all previous investigations made by other methods, the values of ${H}_{c1}$ are much smaller and of the order of 1 mT at $T=0$. We show that the smallness of ${H}_{c1}$ is not related to Josephson junctions and granularity, but is an intrinsic property of the fullerenes.

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