{"paper":{"title":"Microscopic effects of Dy-doping in the topological insulator Bi2Te3","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"2), (2) ISIS Rutherford Appleton Laboratory United Kingdom, (3) Laboratory for Muon Spin Spectroscopy Paul Scherrer Institut Villigen Switzerland, 4), (4) Laboratorium f\\\"ur Festk\\\"orperphysik ETH-H\\\"onggerberg, (5) Diamond Light Source Didcot United Kingdom, (6) European Synchrotron Radiation Facility Grenoble France, (7) Centre for Materials Physics Durham University Durham United Kingdom, (8) School of Physics, (9) Swiss Light Source Paul Scherrer Institute Villigen Switzerland), A. I. Figueroa (5), Astronomy Cardiff University Cardiff United Kingdom, A. Suter (3), F. L. Pratt (2), G. van der Laan (5), J. A. Krieger (3, K. Kummer (6), L. B. Duffy (1, N.-J. Steinke (2), S. J. Blundell (1), S. Langridge (2), S. R. Giblin (8), T. Hesjedal (1) ((1) Clarendon Laboratory University of Oxford Oxford United Kingdom, T. Lancaster (7), T. Prokscha (3), V. N. Strocov (9), Z. Salman (3), Z\\\"urich Switzerland","submitted_at":"2018-08-06T14:44:39Z","abstract_excerpt":"Magnetic doping with transition metal ions is the most widely used approach to break timereversal symmetry in a topological insulator, a prerequisite for unlocking the TIs exotic potential. Recently, we reported the doping of Bi2Te3 thin films with rare earth ions, which, owing to their large magnetic moments, promise commensurately large magnetic gap openings in the topological surface states. However, only when doping with Dy has a sizable gap been observed in angle-resolved photoemission spectroscopy, which persists up to room-temperature. Although disorder alone could be ruled out as a cau"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.01938","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}