{ "id": "1206.0757", "version": "v2", "published": "2012-06-04T20:31:22.000Z", "updated": "2013-01-31T11:06:50.000Z", "title": "Ergodic vs diffusive decoherence in mesoscopic devices", "authors": [ "Thibaut Capron", "Christophe Texier", "Gilles Montambaux", "Dominique Mailly", "Andreas D. Wieck", "Laurent Saminadayar" ], "comment": "LaTeX, 5 pages, 4 pdf figures ; v2: revised version", "journal": "Phys. Rev. B 87, 041307(R) (2013)", "doi": "10.1103/PhysRevB.87.041307", "categories": [ "cond-mat.mes-hall", "cond-mat.dis-nn" ], "abstract": "We report on the measurement of phase coherence length in a high mobility two-dimensional electron gas patterned in two different geometries, a wire and a ring. The phase coherence length is extracted both from the weak localization correction in long wires and from the amplitude of the Aharonov-Bohm oscillations in a single ring, in a low temperature regime when decoherence is dominated by electronic interactions. We show that these two measurements lead to different phase coherence lengths, namely $L_{\\Phi}^\\mathrm{wire}\\propto T^{-1/3}$ and $L_{\\Phi}^\\mathrm{ring}\\propto T^{-1/2}$. This difference reflects the fact that the electrons winding around the ring necessarily explore the whole sample (ergodic trajectories), while in a long wire the electrons lose their phase coherence before reaching the edges of the sample (diffusive regime).", "revisions": [ { "version": "v2", "updated": "2013-01-31T11:06:50.000Z" } ], "analyses": { "subjects": [ "73.23.-b", "03.65.Ta", "75.20.Hr", "72.70.+m" ], "keywords": [ "phase coherence length", "mesoscopic devices", "diffusive decoherence", "high mobility two-dimensional electron gas" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review B", "year": 2013, "month": "Jan", "volume": 87, "number": 4, "pages": "041307" }, "note": { "typesetting": "PDFLaTeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013PhRvB..87d1307C" } } }