CRITICAL-CURRENT, MAGNETIZATION RELAXATION AND ACTIVATION-ENERGIES FOR YBA2CU3O7 AND YBA2CU4O8 FILMS

By means of high-sensitivity capacitance torque magnetometers we have measured the superconducting current j(s) and the dynamic magnetic-mom ent relaxation of YBa2Cu3O7 and YBa2Cu4O8 films of typically 100 nm th ickness at temperatures between 2 K and T-c in magnetic fields up to 6 T. For the measurements of the dynamic relaxation rate Q = dlnj(s)/dl n(dB(e)/dt) magnetic-field sweep rates were varied between 0.5 and 40 mT/s. At low fields (typically 0.5 T) the dynamical relaxation rate ex hibits a plateau at Q approximate to 0.06 in YBa2Cu3O7 and 0.04 in YBa 2Cu4O8. At high fields (B-e = mu(0)H(e) approximate to 6 T) the platea us have completely disappeared and Q increases almost linearly with in creasing temperature. At all fields a sharp increase up to Q congruent to 1 is observed when the irreversibility line is approached. By mean s of the generalized inversion scheme (GIS), the j(s)(T, B-e) and and( T, B-e) data are used to determine the current dependent activation en ergy U(j, T, B-e) for thermally activated flux creep. Although the GIS does not make any a priori assumptions about the explicit functional dependences on T and j, the U(j, T = O, B-e) function derived from the experimental data by means of the GIS can remarkably well be describe d with the collective-creep interpolation formula U(j) = (U-c/mu)[ (j( c)/j)(mu)-1] with mu approximate to 0.6 for currents j > 0.15j(c)(T = 0, B-e) where j(c)(T = 0, B-e) is the critical current at T = 0, and w ith U-c depending on B-e. At lower current densities U(j, T = 0, B-e) does not diverge as j(-0.6) but shifts gradually to a weaker 1n(j(c)/j ) dependence. At low temperatures the current and relaxation data cann ot be explained in terms of a thermally activated flux-motion model. Q uantum creep has an influence up to similar to 13 K.