Abstract

We present evidence for the crossover between creep of individual vortices and collective creep of vortex bundles from measurements of the relaxation of the persistent currents in ${\mathrm{YBa}}_{2}$${\mathrm{Cu}}_{3}$${\mathrm{O}}_{7}$ single crystals over long periods of time. In the single-vortex regime at low fields the relaxation is fast and is characterized by an exponent \ensuremath{\mu}\ensuremath{\simeq}0.16, as predicted in the collective-creep scenario. With increasing field, collective bundling of vortices induces a slowdown of the relaxation, with a maximum \ensuremath{\mu}\ensuremath{\simeq}1.4. At even higher fields, \ensuremath{\mu} decreases again to about 1 as the size of the bundles grows.

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