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26 April 2024
 
  » arxiv » 2009.06020

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Tailoring the magnetic states by controlling octahedral cation arrangement in double perovskite
S. Majumder ; M. Tripathi ; R. Raghunathan ; P. Rajput ; S. N. Jha ; D. O. de Souza ; L. Olivi ; R. J. Choudhary ; D. M. Phase ;
Date 13 Sep 2020
AbstractThe predictability of any characteristic functional aspect in a double perovskite (DP) system has always been compromised by its strong dependence over the inevitably present anti-site disorders (ASD). Here, we aim to precisely map the qualitative and quantitative factors concerning ASD with respect to the corresponding observables describing the magnetic and electronic state in epitaxial Sm$_{2} $NiMnO$_{6} $ (SNMO) DP thin films. The concentration and distribution patterns of ASD are effectively controlled by optimizing growth conditions and estimated on both local and global scales utilizing extended X-ray absorption fine structure and bulk magnetometry. Depending upon the mis-site defect densities, the nature of disorder distribution can vary from homogeneous to partially segregated patches. The magnetic behavior of SNMO compromises between long range FM ordering and short scale AFM interactions originated from ordered Ni-O-Mn and disordered Ni-O-Ni or Mn-O-Mn bonds, respectively, which can be modified substantially by controlling B-site cation arrangement. With increasing ASD, systematic shift in transition temperatures, drastic drop in saturation moment along with deviation from uniaxial anisotropy behavior, reduction in anisotropy energy and increase in defect dimension involving moment pinning efficiency are observed. However, $ Ni^{2+}+Mn^{4+} longrightarrow Ni^{3+}+Mn^{3+} $ charge fluctuation mediated signatures of mixed valence characters are found to be independent of cation disorder densities. Inter competing magnetic interactions from Sm vs Ni-Mn sublattice results in metastable magnetic ground state with manifolds of uneven free energy landscape configurations. This work provides a route-map to tailor the magnetic phase transitions, anisotropy behavior and magnetization reversal mechanism by engineering the ASD fractions in a general DP system.
Source arXiv, 2009.06020
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