Fractional Quantum Hall Effect and Wigner Crystal of Two-Flux Composite Fermions
arXiv:1407.7846 · doi:10.1103/PhysRevLett.113.246803
Abstract
In two-dimensional electron systems confined to GaAs quantum wells, as a function of either tilting the sample in magnetic field or increasing density, we observe multiple transitions of the fractional quantum Hall states (FQHSs) near filling factors and 5/4. The data reveal that these are spin-polarization transitions of interacting two-flux composite Fermions, which form their own FQHSs at these fillings. The fact that the reentrant integer quantum Hall effect near always develops following the transition to full spin polarization of the FQHS strongly links the reentrant phase to a pinned \emph{ferromagnetic} Wigner crystal of two-flux composite Fermions.
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