Crystal structure and elementary properties of NaxCoO2 (x=0.32, 0.51, 0.6, 0.75, and 0.92) in the three-layer NaCoO2 family

被引:104
作者
Viciu, L. [1 ]
Bos, J. W. G.
Zandbergen, H. W.
Huang, Q.
Foo, M. L.
Ishiwata, S.
Ramirez, A. P.
Lee, M.
Ong, N. P.
Cava, R. J.
机构
[1] Princeton Univ, Dept Chem, Princeton, NJ 08540 USA
[2] Delf Inst Technol, Dept Nanosci, Natl Ctr HREM, Al Delf, Netherlands
[3] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[4] Waseda Univ, Dept Appl Phys, Tokyo 1698555, Japan
[5] Lucent Technol, Bell Labs, Murray Hill, NJ 07974 USA
[6] Princeton Univ, Dept Phys, Princeton, NJ 08540 USA
关键词
D O I
10.1103/PhysRevB.73.174104
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The crystal structures of NaxCoO2 phases based on three-layer NaCoO2, with x=0.32, 0.51, 0.60, 0.75, and 0.92, determined by powder neutron diffraction, are reported. The structures have triangular CoO2 layers interleaved by sodium ions, and evolve with variation in Na content in a more complex way than has been observed in the two-layer NaxCoO2 system. The phases with highest and lowest Na content studied (x=0.92 and 0.32) are trigonal, with three CoO2 layers per cell and octahedral Na ion coordination. The intermediate compositions have monoclinic structures. The x=0.75 compound has one CoO2 layer per cell, with Na in octahedral coordination and an incommensurate superlattice. The x=0.6 and 0.51 phases are also single layer, but the Na is found in trigonal prismatic coordination. The magnetic behavior of the phases is similar to that observed in the two-layer system. Both the susceptibility and the electronic contribution to the specific heat are largest for x=0.6.
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页数:10
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