Wigner Crystallization in a Quasi-3D Electronic System
arXiv:0904.3805 · doi:10.1038/nphys1094
Abstract
When a strong magnetic field is applied perpendicularly (along z) to a sheet confining electrons to two dimensions (x-y), highly correlated states emerge as a result of the interplay between electron-electron interactions, confinement and disorder. These so-called fractional quantum Hall (FQH) liquids form a series of states which ultimately give way to a periodic electron solid that crystallizes at high magnetic fields. This quantum phase of electrons has been identified previously as a disorder-pinned two-dimensional Wigner crystal with broken translational symmetry in the x-y plane. Here, we report our discovery of a new insulating quantum phase of electrons when a very high magnetic field, up to 45T, is applied in a geometry parallel (y-direction) to the two-dimensional electron sheet. Our data point towards this new quantum phase being an electron solid in a "quasi-3D" configuration induced by orbital coupling with the parallel field.
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- Colossal magnetoresistance in an ultra-clean weakly interacting 2D Fermi liquid
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- Low-frequency electromagnetic field in a Wigner crystal
- Phase transition from a composite fermion liquid to a Wigner solid in the lowest Landau level of ZnO