H. Fujiki et al., Superconducting fluctuation, localization and electron-electron interaction corrections to the magnetoconductivity in three-dimensional aluminum films, PHYSICA C, 311(1-2), 1999, pp. 58-64
The magnetoconductivity (MC) of three-dimensional (3D) aluminum films with
various dirtiness has been measured in wide ranges of temperature and magne
tic field. (I) Near the superconducting transition temperature T-c, the MC
takes the minimum at a temperature-independent field H-m0. (2) Above H-m0,
MC shows H-1/2 dependence. From the detailed analysis of the H dependence o
f MC, it has been found that the magnitude of the coefficient of H-1/2 can
be explained qualitatively by only the sum of contribution from the weak lo
calization and electron-electron interaction. This experimental result indi
cates that the superconducting thermal fluctuation effect in the field is a
lmost suppressed by this finite field H-m0, of which values are about two t
imes as large as that of the mean-field upper critical field H-c2(0) as we
reported for 2D aluminum films. This circumstance is consistent with the ob
servation of a rapid suppression of the excess conductivity around 2H(c2)(0
) for 3D type II superconductors by Lue et al. [J.W. Lue, A.G. Montgomery,
R.E. Hake, Phys. Rev. B 11 (1975) 3393]. (C) 1999 Published by Elsevier Sci
ence B.V. All rights reserved.