{ "id": "1908.06055", "version": "v1", "published": "2019-08-16T16:48:22.000Z", "updated": "2019-08-16T16:48:22.000Z", "title": "Itinerant ferromagnetism and intrinsic anomalous Hall effect in amorphous iron-germanium", "authors": [ "D. S. Bouma", "Z. Chen", "B. Zhang", "F. Bruni", "M. E. Flatté", "R. Streubel", "L. -W. Wang", "R. Q. Wu", "F. Hellman" ], "comment": "9 pages, 8 figures", "categories": [ "cond-mat.mes-hall", "cond-mat.mtrl-sci" ], "abstract": "The amorphous iron-germanium system ($a$-Fe$_x$Ge$_{1-x}$) lacks long-range structural order and hence lacks a meaningful Brillouin zone. The magnetization of $a$-Fe$_x$Ge$_{1-x}$ is well explained by the Stoner model for Fe concentrations $x$ above the onset of magnetic order around $x=0.4$, indicating that the local order of the amorphous structure preserves the spin-split density of states of the Fe-$3d$ states sufficiently to polarize the electronic structure despite $\\mathbf{k}$ being a bad quantum number. Measurements reveal an enhanced anomalous Hall resistivity $\\rho_{xy}^{\\mathrm{AH}}$ relative to crystalline FeGe; this $\\rho_{xy}^{\\mathrm{AH}}$ is compared to density functional theory calculations of the anomalous Hall conductivity to resolve its underlying mechanisms. The intrinsic mechanism, typically understood as the Berry curvature integrated over occupied $\\mathbf{k}$-states but equivalent to the density of curvature integrated over occupied energies in aperiodic materials, dominates the anomalous Hall conductivity of $a$-Fe$_x$Ge$_{1-x}$ ($0.38 \\leq x \\leq 0.61$).", "revisions": [ { "version": "v1", "updated": "2019-08-16T16:48:22.000Z" } ], "analyses": { "keywords": [ "intrinsic anomalous hall effect", "amorphous iron-germanium", "itinerant ferromagnetism", "anomalous hall conductivity", "lacks long-range structural order" ], "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable" } } }