APS Logo

Interfacial tuning of chiral magnetic interactions for large topological Hall effects in LaMnO3/SrIrO3 heterostructures

Invited

Abstract

One of the most intriguing outcomes of symmetry breaking and spin-obit interactions in magnetic systems is the possibility to create non-collinear and chiral spin textures. The Dzyaloshinskii-Moriya interaction (DMI) results from strong spin-orbit coupling and broken inversion symmetry to generate magnetization rotations with fixed chirality. The discovery of magnetic skyrmions originating from strong DMI in metal thin films has led to an explosion of efforts to manipulate magnetic phases originating from interfaces. We have studied interface-induced magnetism in epitaxial 3d/5d iridate/manganite superlattices. In LaMnO3/SrIrO3 superlattices, we find a large additional topological Hall effect arising from the interaction of charge carriers with a noncoplanar chiral spin texture induced by interfacial DMI[1]. I will describe how the interfacial atomic layer stacking and symmetry enabled by the nonmagnetic A-sites determine the competition between collinear and chiral magnetic interactions originating from the oxide interface. Our findings [2] provide insight to the manipulation of chiral magnetism from atomic-scale control of exchange interactions at oxide interfaces.
References: [1] P. Bruno et al., Phys. Rev. Lett. 93, 096806 (2004). [2] E. Skoropata et al., Sci. Adv., 6, eeaz3902 (2020).

Presenters

  • Elizabeth Skoropata

    Oak Ridge National Lab, Paul Scherrer Institute

Authors

  • Elizabeth Skoropata

    Oak Ridge National Lab, Paul Scherrer Institute

  • John A Nichols

    Oak Ridge National Laboratory

  • Jong Mok Ok

    Oak Ridge National Lab, Oak Ridge National Laboratory

  • Rajesh V Chopdekar

    Advanced Light Source, Lawrence Berkeley National Lab, University of California, Davis, Lawrence Berkeley National Laboratory

  • Eun Sang Choi

    National High Magnetic Field Laboratory, Florida State University, National High Magnetic Field Laboratory, National High Magnetic Field Laboratory and Department of Physics, Florida State University, National High Magnetic Field Lab, Physics, Florida State University, National High Field Magnet Laboratory, Florida Sate University

  • Ankur Rastogi

    Oak Ridge National Laboratory

  • Changhee Sohn

    Oak Ridge National Laboratory

  • Xiang Gao

    Oak Ridge National Laboratory

  • Thomas Farmer

    Oak Ridge National Laboratory

  • Ryan Desautels

    Seagate Technology, Oak Ridge National Laboratory

  • Yongseong Choi

    Advanced Photon Source, Argonne National Laboratory, Argonne National Laboratory

  • Daniel Haskel

    Argonne National Laboratory, Advanced Photon Source, Argonne National Laboratory

  • John Freeland

    argonne national laboratory, Argonne National Laboratory, Advanced Photon Source, Argonne National Laboratory, Argonne National Laboratory, Advanced Photon Source, Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

  • Satoshi Okamoto

    Oak Ridge National Lab, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge National Laboratory

  • Matthew Brahlek

    Oak Ridge National Lab, Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge National Laboratory

  • Ho Nyung Lee

    Oak Ridge National Lab, Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge National Laboratory