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The Local Atomic Structure of Lal-xSrxCoO3: Effects Induced by The Spin-State and Non-Metal to Metal Transitions

Published online by Cambridge University Press:  10 February 2011

Despina Louca ,
J. L. Sarrao  and
G. H. Kwei
Despina Louca
Affiliation:
Los Alamos National Laboratory, Condensed Matter and Thermal Physics Group, MST-10, MS K764, Los Alamos, NM 87545.
J. L. Sarrao
Affiliation:
Los Alamos National Laboratory, Condensed Matter and Thermal Physics Group, MST-10, MS K764, Los Alamos, NM 87545.
G. H. Kwei
Affiliation:
Los Alamos National Laboratory, Condensed Matter and Thermal Physics Group, MST-10, MS K764, Los Alamos, NM 87545.
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Abstract

The pair density function (PDF) used in the analysis of pulsed neutron diffraction data of La1-xSrxCoO3 revealed new structural effects which are correlated to the susceptibility and transport transitions. The transition in the spin configuration of the Co ions from the low-spin (LS) to the high-spin (HS) state in the Co perovskite oxides can potentially induce structural distortions due to the coupling of the spin to the lattice and charge. The ground state of the pure compound, LaCoO3, is in the LS state and is non-magnetic. A transition occurs to the HS state at ∼ 50 K as indicated from the susceptibility measurements due to the thermal excitation of electrons to the eg level. The CoLSO6 octahedra associated with the Co ions in the LS configuration are distinguished from the CoHSO6 octahedra with the Co in the HS configuration because the CoLS-O bond length is shorter than the CoHS-O distance due to the different size of the corresponding Co ions. Such bond lengths are clearly identified in the local structure between 15 – 300 K. This finding is in contrast to the average structure which shows only one type of bond length in this temperature range but two types of bond lengths are suggested at considerably higher temperatures. This suggests that whereas the LS and HS CoO6-octahedra coexist, they are randomly distributed in the crystal lattice at lower temperatures and become ordered at higher temperatures. The introduction of charge carriers in the structure does not eliminate the coexistence of both the LS and HS states, indicating that with the transition to the ferromagnetic metallic state, the spin configuration is not entirely of the HS character and structural inhomogeneities are present.

Type
Research Article
Information
MRS Online Proceedings Library (OPL) , Volume 494: Symposium V – Science & Technology of Magnetic Oxides , 1997 , 107
Copyright
Copyright © Materials Research Society 1998

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