Developing fractional quantum Hall states at even-denominator fillings 1/6 and 1/8
arXiv:2502.17635 · doi:10.1103/PhysRevLett.134.046502
Abstract
In the extreme quantum limit, when the Landau level filling factor , the dominant electron-electron interaction in low-disorder two-dimensional electron systems leads to exotic many-body phases. The ground states at even-denominator 1/2 and 1/4 are typically Fermi seas of composite fermions carrying two and four flux quanta, surrounded by the Jain fractional quantum Hall states (FQHSs) at odd-denominator fillings and , where is an integer. For 1/5, an insulating behavior, which is generally believed to signal the formation of a pinned Wigner crystal, is seen. Our experiments on ultrahigh-quality, dilute, GaAs two-dimensional electron systems reveal developing FQHSs at and , manifested by magnetoresistance minima superimposed on the insulating background. In stark contrast to 1/2 and 1/4, however, we observe a pronounced, sharp minimum in magnetoresistance at 1/6 and a somewhat weaker minimum at 1/8, suggesting developing FQHSs, likely stabilized by the pairing of composite fermions that carry six and eight flux quanta. Our results signal the unexpected entry, in ultrahigh-quality samples, of FQHSs at even-denominator fillings 1/6 and 1/8, which are likely to harbor non-Abelian anyon excitations.
7+20 pages, 3+14 figures
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Cited by in corpus (8)
- Competing Many-Body Phases at Small Fillings in Ultrahigh-Quality GaAs 2D Hole Systems: Role of Landau Level Mixing
- Dispersion of neutral collective modes in partonic fractional quantum Hall states and its applications to paired states of composite fermions
- Extreme disorder in crystalline perovskite oxide: a new paradigm in quantum materials research
- Interplay of superconducting, metallic, and crystalline states of composite fermions at in wide quantum wells
- Interlayer-correlated fractional quantum Hall state in a trilayer electron system
- Cascade of fractional quantum Hall states in 2D system
- Time-dependent conserved operators for autonomous systems and quantization of resistance
- Disorder-induced strong-field strong-localization in 2D systems