When attempting to prepare Rb2NaCo60, one obtains a phase-separated materia
l, consisting of the energetically more stable superconducting Rb3C60 and n
onsuperconducting NaxC60. This sample exhibits a very sharp superconducting
transition temperature at 26.3 K. The decrease in T-c with respect to that
of pure-phase Rb3C60 is explained as the result of the decrease in density
of states in Josephson-like junctions formed between the two phases. This
composition displays a large volume fraction of superconductivity, and all
measurements of superconducting parameters are extremely well defined, impl
ying high phase purity of the Rb3C60. The zero temperature values of the up
per and lower critical magnetic fields are H-c2(0) = 165 kOe and H-c1(0) =
62 Oe, calculated from measurements of the field dependence of the magnetiz
ation as a function of temperature. The coherence length and penetration de
pth are 44 Angstrom and 3400 Angstrom, significantly higher than earlier li
terature estimates. (C) 1999 Elsevier Science B.V. All rights reserved.