Abstract

We have measured the temperature and magnetic field dependencies of the zero bias resistance for several 2D arrays of small aluminum Josephson junctions. The normal state resistances R N of the junctions vary between 2.2 and 7.5 kω whereas the ratio of Josephson coupling energy E J to the charging energy E c ranges between 4.3 and 0.6, where E c=e 2/2C , C being the junction capacitance. The vortex mobility is deduced from the frustration ( i.e. the number of flux quantum per unit cell) dependence of zero bias resistance. The mobility decreases when the temperature is lowered, resulting in a decrease of resistance. Fitting the data to a simple exponential form, we find the barrier for the vortex hopping to be - aE J , with a≈0.3. For all arrays, there exists a crossover temperature T cr which separates the regime of thermally assisted hopping from that of quantum creep of vortices. For our samples, T cr is close to the theoretically predicted value of ω p/2π , where ω p=(8E JE c) 1/2 .

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