{ "id": "cond-mat/0607069", "version": "v1", "published": "2006-07-04T08:14:39.000Z", "updated": "2006-07-04T08:14:39.000Z", "title": "Influence of the driving mechanism on the response of systems with athermal dynamics: the example of the random-field Ising model", "authors": [ "Xavier Illa", "Martin-Luc Rosinberg", "Eduard Vives" ], "comment": "11 pages, 11 figures", "journal": "Phys. Rev. B 74, 224403 (2006)", "doi": "10.1103/PhysRevB.74.224403", "categories": [ "cond-mat.dis-nn", "cond-mat.stat-mech" ], "abstract": "We investigate the influence of the driving mechanism on the hysteretic response of systems with athermal dynamics. In the framework of local-mean field theory at finite temperature (but neglecting thermallly activated processes), we compare the rate-independent hysteresis loops obtained in the random field Ising model (RFIM) when controlling either the external magnetic field $H$ or the extensive magnetization $M$. Two distinct behaviors are observed, depending on disorder strength. At large disorder, the $H$-driven and $M$-driven protocols yield identical hysteresis loops in the thermodynamic limit. At low disorder, when the $H$-driven magnetization curve is discontinuous (due to the presence of a macroscopic avalanche), the $M$-driven loop is re-entrant while the induced field exhibits strong intermittent fluctuations and is only weakly self-averaging. The relevance of these results to the experimental observations in ferromagnetic materials, shape memory alloys, and other disordered systems is discussed.", "revisions": [ { "version": "v1", "updated": "2006-07-04T08:14:39.000Z" } ], "analyses": { "keywords": [ "random-field ising model", "athermal dynamics", "driving mechanism", "yield identical hysteresis loops", "protocols yield identical hysteresis" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. B" }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable" } } }