Mixed Dimensionality of Confined Conducting Electrons in the Surface Region of SrTiO3

N. C. Plumb, M. Salluzzo, E. Razzoli, M. Månsson, M. Falub, J. Krempasky, C. E. Matt, J. Chang, M. Schulte, J. Braun, H. Ebert, J. Minár, B. Delley, K.-J. Zhou, T. Schmitt, M. Shi, J. Mesot, L. Patthey, and M. Radović
Phys. Rev. Lett. 113, 086801 – Published 18 August 2014
PDFHTMLExport Citation

Abstract

Using angle-resolved photoemission spectroscopy, we show that the recently discovered surface state on SrTiO3 consists of nondegenerate t2g states with different dimensional characters. While the dxy bands have quasi-2D dispersions with weak kz dependence, the lifted dxz/dyz 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 dxz/dyz Fermi surface components are essentially the same for different sample preparations. Irradiating SrTiO3 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-EF electrons in the surface region.

  • Figure
  • Figure
  • Figure
  • Received 2 February 2014

DOI:https://doi.org/10.1103/PhysRevLett.113.086801

© 2014 American Physical Society

Authors & Affiliations

N. C. Plumb1,*, M. Salluzzo2, E. Razzoli1, M. Månsson3,4,5, M. Falub1, J. Krempasky1, C. E. Matt1,5, J. Chang1,4, M. Schulte6, J. Braun6, H. Ebert6, J. Minár6,7, B. Delley8, K.-J. Zhou1,†, T. Schmitt1, M. Shi1, J. Mesot1,4,5, L. Patthey1,9, and M. Radović1,4,9,‡

  • 1Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 2CNR-SPIN, Complesso Universitario Monte S. Angelo, Via Cinthia I-80126, Napoli, Italy
  • 3Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 4Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland
  • 5Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switzerland
  • 6Department Chemie, Ludwig-Maximilians-Universität München, 81377 München, Germany
  • 7New Technologies—Research Center, University of West Bohemia, Univerzitni 8, 306 14 Pilsen, Czech Republic
  • 8Condensed Matter Theory Group, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 9SwissFEL, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland

  • *nicholas.plumb@psi.ch
  • Present address: Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxon, OX11 0DE, United Kingdom.
  • milan.radovic@psi.ch

Article Text (Subscription Required)

Click to Expand

Supplemental Material (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 113, Iss. 8 — 22 August 2014

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×
×

Images

×

Sign up to receive regular email alerts from Physical Review Letters

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×