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Mixed dimensionality of confined conducting electrons in the surface region of SrTiO3.
Plumb, N C; Salluzzo, M; Razzoli, E; Månsson, M; Falub, M; Krempasky, J; Matt, C E; Chang, J; Schulte, M; Braun, J; Ebert, H; Minár, J; Delley, B; Zhou, K-J; Schmitt, T; Shi, M; Mesot, J; Patthey, L; Radovic, M.
Afiliación
  • Plumb NC; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Salluzzo M; CNR-SPIN, Complesso Universitario Monte S. Angelo, Via Cinthia I-80126, Napoli, Italy.
  • Razzoli E; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Månsson M; Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland and Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switz
  • Falub M; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Krempasky J; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Matt CE; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switzerland.
  • Chang J; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Schulte M; Department Chemie, Ludwig-Maximilians-Universität München, 81377 München, Germany.
  • Braun J; Department Chemie, Ludwig-Maximilians-Universität München, 81377 München, Germany.
  • Ebert H; Department Chemie, Ludwig-Maximilians-Universität München, 81377 München, Germany.
  • Minár J; Department Chemie, Ludwig-Maximilians-Universität München, 81377 München, Germany and New Technologies-Research Center, University of West Bohemia, Univerzitni 8, 306 14 Pilsen, Czech Republic.
  • Delley B; Condensed Matter Theory Group, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Zhou KJ; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Schmitt T; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Shi M; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Mesot J; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland and Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switzerland.
  • Patthey L; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and SwissFEL, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
  • Radovic M; Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland and Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland and SwissFEL, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland.
Phys Rev Lett ; 113(8): 086801, 2014 Aug 22.
Article en En | MEDLINE | ID: mdl-25192117
ABSTRACT
Using angle-resolved photoemission spectroscopy, we show that the recently discovered surface state on SrTiO(3) consists of nondegenerate t(2g) states with different dimensional characters. While the d(xy) bands have quasi-2D dispersions with weak k(z) dependence, the lifted d(xz)/d(yz) bands show 3D dispersions that differ significantly from bulk expectations and signal that electrons associated with those orbitals permeate the near-surface region. Like their more 2D counterparts, the size and character of the d(xz)/d(yz) Fermi surface components are essentially the same for different sample preparations. Irradiating SrTiO(3) in ultrahigh vacuum is one method observed so far to induce the "universal" surface metallic state. We reveal that during this process, changes in the oxygen valence band spectral weight that coincide with the emergence of surface conductivity are disproportionate to any change in the total intensity of the O 1s core level spectrum. This signifies that the formation of the metallic surface goes beyond a straightforward chemical doping scenario and occurs in conjunction with profound changes in the initial states and/or spatial distribution of near-E(F) electrons in the surface region.
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Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2014 Tipo del documento: Article País de afiliación: Suiza
Buscar en Google
Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2014 Tipo del documento: Article País de afiliación: Suiza