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Transition from a uni- to a bimodal interfacial charge distribution in [Formula: see text]/[Formula: see text] upon cooling.
Zwiebler, M; Di Gennaro, E; Hamann-Borrero, J E; Ritschel, T; Green, R J; Sawatzky, G A; Schierle, E; Weschke, E; Leo, A; Granozio, F Miletto; Geck, J.
  • Zwiebler M; Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062, Dresden, Germany.
  • Di Gennaro E; Dipartimento di Fisica "E. Pancini", Università di Napoli "Federico II", Complesso Universitario di Monte S. Angelo, Via Cintia, 80126, Naples, Italy.
  • Hamann-Borrero JE; CNR-SPIN, Complesso Universitario di Monte S. Angelo, Via Cintia, 80126, Naples, Italy.
  • Ritschel T; Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062, Dresden, Germany.
  • Green RJ; Institut für Festkörper- und Materialphysik, Technische Universität Dresden, 01062, Dresden, Germany.
  • Sawatzky GA; Stewart Blusson Quantum Matter Institute, University of British Columbia, Vancouver, V6T 1Z1, Canada.
  • Schierle E; Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, S7N 5E2, Canada.
  • Weschke E; Stewart Blusson Quantum Matter Institute, University of British Columbia, Vancouver, V6T 1Z1, Canada.
  • Leo A; Helmholtz-Zentrum Berlin, BESSY, Albert-Einstein-Str. 15, 12489, Berlin, Germany.
  • Granozio FM; Helmholtz-Zentrum Berlin, BESSY, Albert-Einstein-Str. 15, 12489, Berlin, Germany.
  • Geck J; Dipartimento di Fisica "E. R. Caianiello", Università degli Studi di Salerno, Fisciano, Italy.
Sci Rep ; 10(1): 18359, 2020 Oct 27.
Article en En | MEDLINE | ID: mdl-33110119
ABSTRACT
We present a combined resonant soft X-ray reflectivity and electric transport study of [Formula see text]/[Formula see text] field effect devices. The depth profiles with atomic layer resolution that are obtained from the resonant reflectivity reveal a pronounced temperature dependence of the two-dimensional electron liquid at the [Formula see text]/[Formula see text] interface. At room temperature the corresponding electrons are located close to the interface, extending down to 4 unit cells into the [Formula see text] substrate. Upon cooling, however, these interface electrons assume a bimodal depth distribution They spread out deeper into the [Formula see text] and split into two distinct parts, namely one close to the interface with a thickness of about 4 unit cells and another centered around 9 unit cells from the interface. The results are consistent with theoretical predictions based on oxygen vacancies at the surface of the [Formula see text] film and support the notion of a complex interplay between structural and electronic degrees of freedom.