Microwave spectroscopic observation of a Wigner solid within the 1/2 fractional quantum Hall effect
arXiv:1504.08182 · doi:10.1103/PhysRevB.95.045417
Abstract
The fractional quantum Hall effect (FQHE) states at half integer Landau fillings () have long been of great interest, since they have correlations that differ from those of the fundamental Laughlin states found at odd denominators. At the FQHE has been observed in wide or double quantum wells, and is ascribed to the two-component Halperin-Laughlin state. excitations carry charge , like the carriers of states which are of interest in quantum computation. Further, such an excitation (quasiparticle or -hole) of has unequal, opposite charge in the top and bottom layers, and hence an up or down dipole moment. Here we report evidence for a Wigner solid (WS) of such dipolar quasiholes from a quantitative study of the microwave spectra of a wide quantum well (WQW) at close to 1/2.
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- Topological phase transition between composite-fermion and Pfaffian daughter states near ν = 1/2 FQHS
- The Quantum Hall Effect in the Absence of Disorder
- Valley-tunable, even-denominator fractional quantum Hall state in the lowest Landau level of an anisotropic system
- Interaction between Surface Acoustic Wave and Quantum Hall Effects
- Broadband Microwave Spectroscopy for Two-Dimensional Material Systems
- Fractional quantum Hall state at with energy gap up to 6 K, and possible transition from one- to two-component state
- Wigner solids of wide quantum wells near Landau filling
- Interlayer-correlated fractional quantum Hall state in a trilayer electron system