Abstract
We discuss a model in which an applied field induces quantum nucleation of soliton-antisoliton (S-S') pairs in a pinned charge or spin density wave. Coulomb blockade prevents pair creation until the electric field exceeds a sharp threshold value, which can be much smaller than the classical depinning field. Above threshold, the pair creation events become correlated in time, by analogy to time-correlated single electron tunneling. We compute the phase polarization and find that, depending on parameters, the predicted phase polarization can either be extremely small below threshold, as observed in NbSe 3 , or quite substantial, as observed in blue bronze. The lack of significant phase polarization below threshold in NbSe 3 , indicated by several experiments, suggests that the measured threshold field is a quantum S-S' pair creation threshold rather than a classical depinning field.
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