Equivalent-circuit model that quantitatively describes domain-wall conductivity in ferroelectric LiNbO3

Manuel Zahn, Elke Beyreuther, Iuliia Kiseleva, Ahmed Samir Lotfy, Conor J. McCluskey, Jesi R. Maguire, Ahmet Suna, Michael Rüsing, J. Marty Gregg, and Lukas M. Eng
Phys. Rev. Applied 21, 024007 – Published 5 February 2024

Abstract

Ferroelectric domain wall (DW) conductivity (DWC) can be attributed to two separate mechanisms: (a) the injection/ejection of charge carriers across the Schottky barrier formed at the (metal-)electrode-DW junction and (b) the transport of those charge carriers along the DW. Current-voltage (I-U) characteristics, recorded at variable temperatures from LiNbO3 (LNO) DWs, are clearly able to differentiate between these two contributions. Practically, they allow us to directly quantify the physical parameters relevant to the two mechanisms (a) and (b) mentioned above. These are, for example, the resistance of the DW, the saturation current, the ideality factor, and the Schottky barrier height of the electrode-DW junction. Furthermore, the activation energies needed to initiate the thermally activated electronic transport along the DWs can be extracted. In addition, we show that electronic transport along LNO DWs can be elegantly viewed and interpreted in an adapted semiconductor picture based on a double-diode, double-resistor equivalent-circuit model, the R2D2 model. Finally, our R2D2 model was checked for its universality by successfully fitting the I-U curves of not only z-cut LNO bulk DWs, but equally of z-cut thin-film LNO DWs, and of x-cut thin-film DWs as reported in literature.

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  • Received 19 July 2023
  • Revised 18 November 2023
  • Accepted 10 January 2024

DOI:https://doi.org/10.1103/PhysRevApplied.21.024007

© 2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Manuel Zahn1,2, Elke Beyreuther1,*, Iuliia Kiseleva1, Ahmed Samir Lotfy3, Conor J. McCluskey4, Jesi R. Maguire4, Ahmet Suna4, Michael Rüsing1,5, J. Marty Gregg4, and Lukas M. Eng1,6

  • 1Institute of Applied Physics, Technische Universität Dresden, 01062 Dresden, Germany
  • 2Experimental Physics V, Center for Electronic Correlations and Magnetism, University of Augsburg, 86159 Augsburg, Germany
  • 3Department of Materials, ETH Zürich, 8093 Zürich, Switzerland
  • 4Center for Quantum Materials and Technologies, School of Mathematics and Physics, Queen’s University Belfast, Northern Ireland
  • 5Integrated Quantum Optics, Institute for Photonic Quantum Systems (PhoQS), Paderborn University, 33098 Paderborn, Germany
  • 6ct.qmat: Dresden-Würzburg Cluster of Excellence—EXC 2147, Technische Universität Dresden, 01062 Dresden, Germany

  • *elke.beyreuther@tu-dresden.de

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Vol. 21, Iss. 2 — February 2024

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