Abstract

We calculate the rsponse of an N\ifmmode\times\else\texttimes\fi{}N array of resistively shunted Josephson junctions to an imposed current I=${\mathit{I}}_{\mathrm{dc}}$+${\mathit{I}}_{\mathrm{ac}}$sin(2\ensuremath{\pi}\ensuremath{\nu}t). In a transverse dc magnetic field of p/q==f flux quanta per plaquette of area, we find fractional giant Shapiro steps in the time-averaged voltage 〈V〉 at values 〈V〉=nNh\ensuremath{\nu}/2eq, n=1,2,3,..., in agreement with the measurements of Benz et al. At f=1/5, 2/5, and 1/3, we find additional fractional steps at 〈V〉=Nh\ensuremath{\nu}/(4e). A generalization of the model of Benz et al. accounts for both the fractional giant steps at p/q and the anomalous half-integer steps.

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