The fractional quantum Hall effect (FQHE) arises from strong correlations between electrons
when they are confined to two dimensions and exposed to a strong magnetic field. The …

Fractional quantum Hall states (FQHSs) exemplify exotic phases of low-disorder two-
dimensional (2D) electron systems when electron-electron interaction dominates over the …

We predict that an incompressible fractional quantum Hall state is likely to form at ν= 3/8 as a
result of a chiral p-wave pairing of fully spin polarized composite fermions carrying four …

The Read-Rezayi wave function is one of the candidates for the fractional quantum Hall
effect at filling fraction ν= 2+ ⅗, and thereby also its hole conjugate at 2+ ⅖. We study a …

Numerical studies by Wójs, Yi, and Quinn have suggested that an unconventional fractional
quantum Hall effect is plausible at filling factors ν= 1/3 and 1/5, provided the interparticle …

The fractional quantum Hall effect at ν= 2+ 3/8, which has been definitively observed, is one
of the last fractions for which no viable explanation has so far been demonstrated. Our …

There is much interest in the realization of systems with p-wave pairing in one dimension or
chiral p-wave pairing in two dimensions, because these are believed to support Majorana …

By developing an algorithm for evaluating the basis states for the composite fermions with
negative effective magnetic field, we perform the composite-fermion-diagonalization study …

We show a generic formation of the primary magnetorotons in the collective modes of the
observed “unconventional” fractional quantum Hall effect states of the composite fermions at …

We use the circularly polarized resonant Rayleigh scattering (RRS) to study the quantum
Hall ferromagnet at ν= 1. At this filling factor, we observe a right-handed copolarized RRS …