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We show that, in the absence of interlayer hopping, the {ν}=1/m quantum Hall states in double-layer systems contain a neutral gapless mode with linear dispersion, describing the relative fluctuations of the electron densities in the two layers. At finite temperature the system experiences a Kosterlitz-Thouless transition. In the presence of interlayer hopping an energy gap proportional to the square root of the hopping amplitude will be opened. In field theory this corresponds to a U(1) gauge field acquiring a mass due to the monopole-antimonopole plasma in the (2+1)-dimensional spacetime.
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Wen et al. (1992) studied this question.
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