We study the dependence of the transport properties of square Josephson Junction arrays with the direction of the applied dc current, both experimentally and numerically. We present computational simulations of current--voltage curves at finite temperatures for a single vortex in an array of L×L junctions (Ha²/Φ₀=f=1/L²), and experimental measurements in 100×1000 arrays under a low magnetic field corresponding to f≈0.02. We find that the transverse voltage vanishes only in the directions of maximum symmetry of the square lattice: the [10] and [01] direction (parallel bias) and the [11] direction (diagonal bias). For orientations different from the symmetry directions, we find a finite transverse voltage that depends strongly on the angle φ of the current. We find that vortex motion is pinned in the [10] direction (φ=0), meaning that the voltage response is insensitive to small changes in the orientation of the current near φ=0. We call this phenomenon orientational pinning. This leads to a finite transverse critical current for a bias at φ=0 and to a transverse voltage for a bias at φ≠0. On the other hand, for diagonal bias in the [11] direction the behavior is highly unstable against small variations of φ, leading to a rapid change from zero transverse voltage to a large transverse voltage within a few degrees. This last behavior is in good agreement with our measurements in arrays with a quasidiagonal current drive.
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Marconi et al. (2000) studied this question.
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