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Using a variational argument, we show that a two-dimensional (2D) crystal becomes defective in the presence of a random potential. The threshold pinning force and flow properties of a plastically deformed crystal are studied using a perturbation theory valid for weak pinning potential and strong driving force. In the case of a 2D flux-line lattice, it is shown that dislocations introduce extra dissipation in the system, thus increasing the total pinning force, and resulting in nonlinear I-V characteristics.
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Shi et al. (1991) studied this question.
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