{ "id": "1504.02082", "version": "v1", "published": "2015-04-08T19:14:56.000Z", "updated": "2015-04-08T19:14:56.000Z", "title": "Exchange and collective behavior of magnetic impurities in a disordered helical metal", "authors": [ "Hector Ochoa" ], "comment": "5 pages, 3 figures; comments are welcome", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el" ], "abstract": "We study the exchange interaction and the subsequent collective behavior of magnetic impurities embedded in a disordered two-dimensional (2D) helical metal. The exchange coupling follows a statistical distribution whose moments are calculated to the lowest order in $\\left(p_F\\ell\\right)^{-1}$, where $p_F$ is the Fermi momentum of itinerant electrons and $\\ell$ is the mean free path. We find that i) the first moment of the distribution decays exponentially, and ii) the variance of the interaction is long-range, however, it becomes independent of the orientation of the localized magnetic moments due to the locking between spin and momentum of the electrons that mediate the interaction. As consequence, long-range magnetic order tends to be suppressed, and a spin glass phase is stabilized at finite temperatures. The formalism is applied to the surface states of a three-dimensional (3D) topological insulator. The lack of a net magnetic moment in the glassy phase and the full randomization of spin polarization at distances larger than $\\ell$ excludes a spectral gap for surface states. Hence, non-magnetic disorder may explain the dispersion in results for photoemission experiments in magnetically-doped topological insulators.", "revisions": [ { "version": "v1", "updated": "2015-04-08T19:14:56.000Z" } ], "analyses": { "keywords": [ "magnetic impurities", "disordered helical metal", "collective behavior", "surface states", "long-range magnetic order tends" ], "note": { "typesetting": "TeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable" } } }