4.3 Article

Spacer-layer-tunable ferromagnetic half-metal-ferromagnetic insulator transition in SrVO3/SrTiO3 superlattice

Journal

ACTA PHYSICA SINICA
Volume 71, Issue 23, Pages -

Publisher

CHINESE PHYSICAL SOC
DOI: 10.7498/aps.71.20221765

Keywords

superlattice; metal-insulator transition; ferromagnetic half-metal; ferromagnetic insulator

Funding

  1. National Natural Science Foundation of China [82174528]
  2. Start-up Fund for Doctoral Research of Shandong Management University, China [SDMUD201901]
  3. Scientific Research Start-up Project of Shandong Management University, China [QH2020Z05]

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The transition from ferromagnetic half-metal to ferromagnetic insulator in SrVO3/SrTiO3 superlattices can be achieved by adjusting the number of SrTiO3 layers. Ti-V mixed defects play a crucial role in this metal-insulator transition.
In this work, the first-principle calculations based on density functional theory (DFT) are employed to investigate the electronic and magnetic properties of SrVO3/SrTiO3 (111) superlattices. The studies show that the transition from ferromagnetic half-metal to ferromagnetic insulator can be achieved by adjusting the thickness of the spacer-layer SrTiO3. The interlayer coupling between the SrVO3 sublayers can occur across two unit-cell (uc) distance of SrTiO3, and the superlattice is ferromagnetic half-metal. When the SrTiO3 sublayers are 3uc, a small band gap (about 0.28 eV) appears in the superlattice. When the SrTiO3 sublayers are more than 3uc, the superlattice has a large band gap and exhibits ferromagnetic insulating state. Further studies show that the Ti-V mixed defects play an important role in realizing the transition of metal-insulator. Compared with the ideal interface, the Ti-V mixed interface can inhibit the interlayer coupling and induce the transition of ferromagnetic half-metal to ferromagnetic insulator. These results provide a theoretical basis for the transition of ferromagnetic half-metal to ferromagnetic insulator by adjusting the number of SrTiO3 layers in SrVO3/SrTiO3 (111) superlattices.

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