Local structure of LiNiO2 studied by neutron diffraction -: art. no. 064410

被引:87
作者
Chung, JH
Proffen, T
Shamoto, S
Ghorayeb, AM
Croguennec, L
Tian, W
Sales, BC
Jin, R
Mandrus, D
Egami, T
机构
[1] Univ Penn, Dept Mat Sci & Engn, Philadelphia, PA 19104 USA
[2] Univ Penn, Res Struct Matter Lab, Philadelphia, PA 19104 USA
[3] Los Alamos Natl Lab, Lujan Ctr, Los Alamos, NM 87545 USA
[4] JAERI, Neutron Sci Res Ctr, Tokai, Ibaraki 3191195, Japan
[5] Univ Aix Marseille 3, CNRS, UMR 6137, Lab Mat & Microelect Provence, F-13397 Marseille, France
[6] CNRS, Inst Chim Mat Condensee Bordeaux, F-33608 Pessac, France
[7] Univ Tennessee, Dept Phys & Astron, Knoxville, TN 37996 USA
[8] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
[9] Univ Tennessee, Dept Mat Sci & Engn, Knoxville, TN 37996 USA
关键词
D O I
10.1103/PhysRevB.71.064410
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The nature of the magnetic state of LiNiO2 has been controversial. In this compound Ni spins (S=1/2) form a triangular lattice with the possibility of magnetic frustration, but the exact state of spin correlation has not yet been known in spite of the extensive research work. A factor that complicates understanding of the magnetic state is the orbital state of Ni3+ which is a Jahn-Teller (JT) ion. While there is no signature of long-range Jahn-Teller distortion, local JT distortion has been suspected. We have performed neutron diffraction and atomic pair-density function analyses up to unprecedented large distances to discover a number of unusual features, such as anomalous peak broadening, local JT distortion, sharp oxygen-oxygen distance correlations, and inverted temperature dependence of medium range correlation. These observations are best explained by local orbital ordering of Ni3+ ions into three sublattices. This orbital ordering, however, cannot develop into long-range order because of the strain field it generates, and domains of about 10 nm in size are formed. Domains are susceptible to random pinning by impurities (site disorder) resulting in the loss of structural long-range order. We suggest that this local orbital ordering is the basis for the complex magnetic properties observed in this compound.
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