Fractional quantum Hall state at ν=1/4 in a wide quantum well
arXiv:0903.4415 · doi:10.1103/PhysRevB.79.245325
Abstract
We investigate, with the help of Monte-Carlo and exact-diagonalization calculations in the spherical geometry, several compressible and incompressible candidate wave functions for the recently observed quantum Hall state at the filling factor in a wide quantum well. The quantum well is modeled as a two-component system by retaining its two lowest subbands. We make a direct connection with the phenomenological effective-bilayer model, which is commonly used in the description of a wide quantum well, and we compare our findings with the established results at in the lowest Landau level. At , the overlap calculations for the Halperin (5,5,3) and (7,7,1) states, the generalized Haldane-Rezayi state and the Moore-Read Pfaffian, suggest that the incompressible state is likely to be realized in the interplay between the Halperin (5,5,3) state and the Moore-Read Pfaffian. Our numerics shows the latter to be very susceptible to changes in the interaction coefficients, thus indicating that the observed state is of multicomponent nature.
14 pages, 8 figures; minor changes, accepted for publication in Phys. Rev. B
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- Observation of fractional quantum Hall effect at even-denominator 1/2 and 1/4 fillings in asymmetric wide quantum wells
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- Identification of topological order in the fractional quantum Hall state at
- Phase diagram of compressible and paired states in the quarter-filled Landau level
- Correlation-hole induced paired quantum Hall states in lowest Landau level
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