Fractional Quantum Hall State at with Energy Gap Up to 6 K and Possible Transition from the One- to Two-Component State
Phys. Rev. Lett. 135, 246603 – Published 9 December, 2025
DOI: https://doi.org/10.1103/ywpx-qm7d
Abstract
The fractional quantum Hall state (FQHS) observed in the lowest Landau level at filling factor in wide quantum wells has been enigmatic for decades because the two-dimensional electron system (2DES) has a bilayer charge distribution but with significant interlayer tunneling. Of particular interest is whether the FQHS in this system has a one-component (1C) or two-component (2C) origin; these are typically identified as the Pfaffian (non-Abelian) or the (Abelian) FQHSs, respectively. We report here our experimental study of the evolution of the correlated states of an ultrahigh-quality 2DES confined to a 72.5-nm-wide GaAs quantum well. At the lowest densities, the 2DES displays only odd-denominator FQHSs, and the ground state at is a composite fermion Fermi sea. As the density is increased, an FQHS emerges at , and becomes very strong. In a finite density range where the FQHS is strongest, we also observe its daughter FQHSs at and , consistent with the theoretically expected daughter states of a Pfaffian FQHS. At the highest densities, the 2DES becomes 2C, signaled by the emergence of a bilayer Wigner crystal state and the transitions of FQHSs flanking . The FQHS remains robust near this transition and, notably, its charge transport energy gap exhibits an upward cusp with a maximum value of about 6 K on the 1C side of the transition; this is the largest gap reported for any even-denominator FQHS. Our observation of the transition of the 2DES ground states near to 2C states at high densities, and our measurements of the robustness of the FQHS against charge distribution asymmetry, suggest that the FQHS also makes a transition from 1C to 2C. Such a transition from a non-Abelian to Abelian state can open avenues for topological quantum information and quantum criticality.