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The bulk charge distribution on a fractional Hall plateau has also been discussed recently by Jun’ichi Shiraishi and Mahito Kohmoto, Phys. Rev. B 54, 17 667 (1996). These authors base their work on an effective Chern-Simons theory for quantum Hall edges, which leads to a bulk response relation that is similar, but not identical, to ours. In our view the present approach, which is soundly based on the known microscopic of fractional Hall states, is more reliable.
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Phys. Rev. BL. Brey, J. J. Palacios, and C. Tejedor, 47, 13 884 (1993) for discussions applicable to the case of smooth electrostatically defined edges.
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Exceptions occur when the ground state has broken translational or broken spin-rotational symmetry, as expected at (Formula presented) in the absence of Zeeman coupling. See, for example, R. Cote, A. H. MacDonald, L. Brey, H. A. Fertig, S. M. Girvin, and H. T. C. Stoof, Phys. Rev. Lett. 78, 4825 (1997).
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