Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4

Topochemical reduction of the ordered double perovskite LaSrNiRuO6 with CaH2 yields LaSrNiRuO4, an extended oxide phase containing infinite sheets of apex-linked, square-planar Ni1+O4 and Ru2+O4 units ordered in a checkerboard arrangement. At room temperature the localized Ni1+ (d9, S = 1/2) and Ru2...

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Main Authors: Patino, M, Zeng, D, Bower, R, McGrady, J, Hayward, M
Format: Journal article
Published: American Chemical Society 2016
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author Patino, M
Zeng, D
Bower, R
McGrady, J
Hayward, M
author_facet Patino, M
Zeng, D
Bower, R
McGrady, J
Hayward, M
author_sort Patino, M
collection OXFORD
description Topochemical reduction of the ordered double perovskite LaSrNiRuO6 with CaH2 yields LaSrNiRuO4, an extended oxide phase containing infinite sheets of apex-linked, square-planar Ni1+O4 and Ru2+O4 units ordered in a checkerboard arrangement. At room temperature the localized Ni1+ (d9, S = 1/2) and Ru2+ (d6, S = 1) centers behave paramagnetically. However, on cooling below 250 K the system undergoes a cooperative phase transition in which the nickel spins align ferromagnetically, while the ruthenium cations appear to undergo a change in spin configuration to a diamagnetic spin state. Features of the low-temperature crystal structure suggest a symmetry lowering Jahn–Teller distortion could be responsible for the observed diamagnetism of the ruthenium centers.
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spelling oxford-uuid:822e4b3e-5865-4105-b594-529036a176472022-03-26T21:35:34ZCoupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:822e4b3e-5865-4105-b594-529036a17647Symplectic Elements at OxfordAmerican Chemical Society2016Patino, MZeng, DBower, RMcGrady, JHayward, MTopochemical reduction of the ordered double perovskite LaSrNiRuO6 with CaH2 yields LaSrNiRuO4, an extended oxide phase containing infinite sheets of apex-linked, square-planar Ni1+O4 and Ru2+O4 units ordered in a checkerboard arrangement. At room temperature the localized Ni1+ (d9, S = 1/2) and Ru2+ (d6, S = 1) centers behave paramagnetically. However, on cooling below 250 K the system undergoes a cooperative phase transition in which the nickel spins align ferromagnetically, while the ruthenium cations appear to undergo a change in spin configuration to a diamagnetic spin state. Features of the low-temperature crystal structure suggest a symmetry lowering Jahn–Teller distortion could be responsible for the observed diamagnetism of the ruthenium centers.
spellingShingle Patino, M
Zeng, D
Bower, R
McGrady, J
Hayward, M
Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title_full Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title_fullStr Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title_full_unstemmed Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title_short Coupled electronic and magnetic phase transition in the infinite-layer phase LaSrNiRuO4
title_sort coupled electronic and magnetic phase transition in the infinite layer phase lasrniruo4
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