• Open Access

Berry phase engineering at oxide interfaces

D. J. Groenendijk, C. Autieri, T. C. van Thiel, W. Brzezicki, J. R. Hortensius, D. Afanasiev, N. Gauquelin, P. Barone, K. H. W. van den Bos, S. van Aert, J. Verbeeck, A. Filippetti, S. Picozzi, M. Cuoco, and A. D. Caviglia
Phys. Rev. Research 2, 023404 – Published 25 June 2020
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Abstract

Three-dimensional strontium ruthenate (SrRuO3) is an itinerant ferromagnet that features Weyl points acting as sources of emergent magnetic fields, anomalous Hall conductivity, and unconventional spin dynamics. Integrating SrRuO3 in oxide heterostructures is potentially a novel route to engineer emergent electrodynamics, but its electronic band topology in the two-dimensional limit remains unknown. Here we show that ultrathin SrRuO3 exhibits spin-polarized topologically nontrivial bands at the Fermi energy. Their band anticrossings show an enhanced Berry curvature and act as competing sources of emergent magnetic fields. We control their balance by designing heterostructures with symmetric (SrTiO3/SrRuO3/SrTiO3 and SrIrO3/SrRuO3/SrIrO3) and asymmetric interfaces (SrTiO3/SrRuO3/SrIrO3). Symmetric structures exhibit an interface-tunable single-channel anomalous Hall effect, while ultrathin SrRuO3 embedded in asymmetric structures shows humplike features consistent with multiple Hall contributions. The band topology of two-dimensional SrRuO3 proposed here naturally accounts for these observations and harmonizes a large body of experimental results.

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  • Received 15 January 2020
  • Revised 3 April 2020
  • Accepted 11 May 2020

DOI:https://doi.org/10.1103/PhysRevResearch.2.023404

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

D. J. Groenendijk1,*, C. Autieri2,3,*, T. C. van Thiel1,*,†, W. Brzezicki2,3,*, J. R. Hortensius1, D. Afanasiev1, N. Gauquelin4, P. Barone2, K. H. W. van den Bos4, S. van Aert4, J. Verbeeck4, A. Filippetti5,6, S. Picozzi2, M. Cuoco2,7,‡, and A. D. Caviglia1,§

  • 1Kavli Institute of Nanoscience, Delft University of Technology, P.O. Box 5046, 2600 GA Delft, Netherlands
  • 2Consiglio Nazionale delle Ricerche, CNR-SPIN, Italy
  • 3International Research Centre MagTop, Institute of Physics, Polish Academy of Sciences, Aleja Lotników 32/46, PL-02668 Warsaw, Poland
  • 4Electron Microscopy for Materials Science (EMAT), University of Antwerp, 2020 Antwerp, Belgium
  • 5Dipartimento di Fisica, Università di Cagliari, Cagliari, Monserrato 09042-I, Italy
  • 6CNR-IOM, Istituto Officina dei Materiali, Cittadella Universitaria, Cagliari, Monserrato 09042-I, Italy
  • 7Dipartimento di Fisica “E. R. Caianiello” Università degli Studi di Salerno, 84084 Fisciano, Italy

  • *These authors contributed equally to this work.
  • t.c.vanthiel@tudelft.nl
  • mario.cuoco@spin.cnr.it
  • §Corresponding author: a.caviglia@tudelft.nl

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Vol. 2, Iss. 2 — June - August 2020

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