Tuning structural, transport, and magnetic properties of epitaxial SrRuO3 through Ba substitution

Zeeshan Ali, Zhen Wang, Alessandro R. Mazza, Mohammad Saghayezhian, Roshan Nepal, Thomas Z. Ward, Yimei Zhu, and Jiandi Zhang
Phys. Rev. B 107, 144405 – Published 5 April 2023
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Abstract

The perovskite ruthenates (ARuO3, A=Ca, Ba, or Sr) exhibit unique properties owing to a subtle interplay of crystal structure and electronic-spin degrees of freedom. Here, we demonstrate an intriguing continuous tuning of crystal symmetry from orthorhombic to tetragonal (no octahedral rotations) phases in epitaxial SrRuO3 achieved via Ba substitution (Sr1xBaxRuO3 with 0x0.7). An initial Ba substitution to SrRuO3 not only changes the ferromagnetic properties, but also tunes the perpendicular magnetic anisotropy via flattening the Ru–O–Ru bond angle (to 180), resulting in the maximum Curie temperature and an extinction of RuO6 rotational distortions at x0.20. For x0.2, the reduction of RuO6 octahedral rotational distortion dominantly enhances the ferromagnetism in the system, though competing with the effect of the RuO6 tetragonal distortion. Further increasing Ba substitution (x>0.2) gradually enhances the tetragonal-type distortion, resulting in the tuning of Ru4d orbital occupancy and suppression of ferromagnetism. Our results demonstrate that isovalent substitution of the Asite cations significantly and controllably impacts both electronic and magnetic properties of perovskite oxides.

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  • Received 28 November 2022
  • Revised 29 January 2023
  • Accepted 17 March 2023

DOI:https://doi.org/10.1103/PhysRevB.107.144405

©2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Zeeshan Ali1,*, Zhen Wang1,2,3, Alessandro R. Mazza4,5, Mohammad Saghayezhian1, Roshan Nepal1, Thomas Z. Ward4, Yimei Zhu3,†, and Jiandi Zhang1,6,‡

  • 1Department of Physics & Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA
  • 2University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China
  • 3Condensed Matter Physics & Materials Science, Department, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 4Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 5Center for Integrated Nanotechnologies, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 6Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China

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Issue

Vol. 107, Iss. 14 — 1 April 2023

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