We have investigated the interaction of phonons with a two-dimensional electron gas in the fractional quantum Hall regime with phonon drag thermoelectric power (TEP). The TEPs at filling factors with the same even denominator are found to be identical; at other even-denominator filling factors they differ only by a constant factor. Treating these states as composite fermions, the findings are explained by a zero magnetic field theory for phonon drag. A maximum observed in the TEP at ν0ex0ex=0ex0ex1/2 is modeled by a weakly diverging effective mass of the composite fermions at this filling factor.
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Tieke et al. (1996) studied this question.
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