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Structural evolution across the metal-insulator transition of strongly distorted Lu1−xScxNiO3 perovskites (x = 0, 0.1, 0.2)
Author(s) -
Qi Cui,
Ningning Wang,
J. A. Alonso,
François Fauth,
Jinguang Cheng
Publication year - 2020
Publication title -
materials research express
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.383
H-Index - 35
ISSN - 2053-1591
DOI - 10.1088/2053-1591/abcc8a
Subject(s) - non blocking i/o , monoclinic crystal system , materials science , orthorhombic crystal system , crystallography , antiferromagnetism , octahedron , ionic radius , bond length , perovskite (structure) , metal , ion , crystal structure , condensed matter physics , chemistry , physics , biochemistry , organic chemistry , metallurgy , catalysis
RNiO 3 perovskites have been described to present thermally driven metal-insulator transitions (at T MI ) as a function of the rare-earth ion size (R = Pr to Lu). Aiming to extend the stability range of RNiO 3 for smaller R 3+ ions, we prepared Lu 1−x Sc x NiO 3 (x = 0, 0.1, 0.2) perovskites, being Sc 3+ ions substantially smaller than Lu 3+ , by using a multi-anvil high-pressure synthesis device at 10 GPa. We have studied the structural evolution of Lu 0.9 Sc 0.1 NiO 3 by synchrotron x-ray diffraction (SXRD) from room temperature to 350 °C. The symmetry of the lattice evolves from monoclinic ( P2 1 /n ) to orthorhombic ( Pbnm ) upon heating across T MI (≈320 °C), with the existence of two chemically and crystallographically distinct nickel sites in the insulating, monoclinic regime, whereas the metallic phase has a single NiO 6 environment. A simultaneous structural and electronic transition implies an abrupt evolution of the lattice parameters and size of the NiO 6 octahedra upon entering the metallic regime, leading to the merging of the disproportionated Ni-O bond lengths. The magnetic properties correspond to the establishment of antiferromagnetic correlations at the Ni sublattice; a decrease of the T N ordering temperature from 122 K (x = 0) to 113 K (x = 0.2) is observed as the Sc content increases, which is concomitant with a more distorted perovskite structure.

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