At low Landau level filling of a two-dimensional electron system, typically associated with the formation of an electron crystal, we observe local minima in Rₓₓ at filling factors ν0ex0ex=0ex0ex2/11, 3/17, 3/19, 2/13, 1/7, 2/15, 2/17, and 1/9. Each of these developing fractional quantum Hall (FQHE) states appears only above a filling-factor-specific temperature. This can be interpreted as the melting of an electron crystal and subsequent FQHE liquid formation. The observed sequence of FQHE states follows the series of composite fermion states emanating from ν0ex0ex=0ex0ex1/6 and ν0ex0ex=0ex0ex1/8.
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Pan et al. (2002) studied this question.
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