{ "id": "cond-mat/9806061", "version": "v2", "published": "1998-06-04T14:16:37.000Z", "updated": "1998-08-26T17:16:29.000Z", "title": "Conductance Correlations Near Integer Quantum Hall Transitions", "authors": [ "Božidar Jovanović", "Ziqiang Wang" ], "comment": "4 pages, 4 figures, minor corrections, to appear in Phys. Rev. Lett", "journal": "Phys. Rev. Lett. 81, 2767 (1998)", "doi": "10.1103/PhysRevLett.81.2767", "categories": [ "cond-mat.mes-hall" ], "abstract": "In a disordered mesoscopic system, the typical spacing between the peaks and the valleys of the conductance as a function of Fermi energy $E_F$ is called the conductance energy correlation range $E_c$. Under the ergodic hypothesis, the latter is determined by the half-width of the ensemble averaged conductance correlation function: $F= < \\delta g(E_F) \\delta g(E_F + \\Delta E) >$. In ordinary diffusive metals, $E_c\\sim D/L^2$, where $D$ is the diffusion constant and $L$ is the linear dimension of the phase-coherent sample. However, near a quantum phase transition driven by the location of the Fermi energy $E_F$, the above picture breaks down. As an example of the latter, we study, for the first time, the conductance correlations near the integer quantum Hall transitions of which $E_F$ is a critical coupling constant. We point out that the behavior of $F$ is determined by the interplay between the static and the dynamic properties of the critical phenomena.", "revisions": [ { "version": "v2", "updated": "1998-08-26T17:16:29.000Z" } ], "analyses": { "keywords": [ "integer quantum hall transitions", "fermi energy", "conductance energy correlation range", "quantum phase transition driven", "ensemble averaged conductance correlation function" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. Lett." }, "note": { "typesetting": "TeX", "pages": 4, "language": "en", "license": "arXiv", "status": "editable" } } }