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Room-temperature transparent oxide spin electronics: A conducting interface in LaFeO3−SrTiO3

Ripudaman Kaur1,2,*, Anamika Kumari1,*, Shinjini Paul3, Mohd Anas4, Bibek Ranjan Satapathy1, Sanjeev Kumar2, V. K. Malik4, P. Mahadevan3, D. D. Sarma5,6 et al.

Suvankar Chakraverty1,†

  • 1Quantum Materials and Devices Unit, Institute of Nano Science and Technology, Mohali, Punjab 140306, India
  • 2Applied Science Department, Punjab Engineering College (Deemed to be University), Sector-12, Chandigarh 160012, India
  • 3S. N. Bose National Centre for Basic Sciences, Kolkata, West Bengal 700106, India
  • 4Department of Physics, Indian Institute of Technology Roorkee, Roorkee 247667, India
  • 5CSIR-National Institute for Interdisciplinary Science and Technology (CSIR-NIIST), Industrial Estate P.O., Pappanamcode, Thiruvananthapuram 695019, India
  • 6Solid State and Structural Chemistry Unit, Indian Institute of Science Bengaluru, Karnataka 560012, India

  • *These authors contributed equally to this work.
  • †suvankar.chakraverty@gmail.com

Phys. Rev. B 109, L201114 – Published 14 May, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L201114

Abstract

The quest for realizing highly spin-polarized conduction in materials at room temperature is one of the central themes of materials physics. We report on the realization of a conducting interface in LaFeO3 (LFO)-SrTiO3 (STO) that demonstrates spin-polarization signatures, namely, negative magnetoresistance (MR) and anomalous Hall resistivity >150 K and even up to room temperature. However, the same system shows positive MR and normal Hall effect at temperatures <150 K. From density functional theory calculations, we find that this is related to the structural transition of the substrate, amplified here as the changes happen at the interface. This leads to a net spin polarization of the interface states at the Fermi energy in the high-temperature phase, allowing for an anomalous Hall effect and negative MR. In addition, this interface appears to be almost transparent in the entire range of visible light. Our observation might be viewed as a step toward room-temperature transparent oxide spintronics.

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