{ "id": "0904.3805", "version": "v1", "published": "2009-04-24T06:54:16.000Z", "updated": "2009-04-24T06:54:16.000Z", "title": "Wigner Crystallization in a Quasi-3D Electronic System", "authors": [ "B. A. Piot", "Z. Jiang", "C. R. Dean", "L. W. Engel", "G. Gervais", "L. N. Pfeiffer", "K. W. West" ], "journal": "Nature Physics 4, 936 - 939 (2008)", "doi": "10.1038/nphys1094", "categories": [ "cond-mat.mes-hall", "cond-mat.other" ], "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.", "revisions": [ { "version": "v1", "updated": "2009-04-24T06:54:16.000Z" } ], "analyses": { "keywords": [ "quasi-3d electronic system", "wigner crystallization", "high magnetic field", "quantum phase", "disorder-pinned two-dimensional wigner crystal" ], "tags": [ "journal article" ], "publication": { "journal": "Nature Physics", "year": 2008, "month": "Dec", "volume": 4, "number": 12, "pages": 936 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2008NatPh...4..936P" } } }