Magnetic phase diagram of layered cobalt dioxide LixCoO2

被引:65
作者
Mukai, K. [1 ]
Ikedo, Y.
Nozaki, H.
Sugiyama, J.
Nishiyama, K.
Andreica, D.
Amato, A.
Russo, P. L.
Ansaldo, E. J.
Brewer, J. H.
Chow, K. H.
Ariyoshi, K.
Ohzuku, T.
机构
[1] Toyota Cent Res & Dev Labs Inc, Aichi 4801192, Japan
[2] High Energy Accelerator Res Org, Inst Mat Struct Sci, Tsukuba, Ibaraki 3050801, Japan
[3] Paul Scherrer Inst, Lab Muon Spin Spect, Villigen, Switzerland
[4] TRIUMF, Vancouver, BC V6T 2A3, Canada
[5] Univ British Columbia, Dept Phys & Astron, Vancouver, BC V6T 1Z1, Canada
[6] Univ Alberta, Dept Phys, Edmonton, AB T6G 2G7, Canada
[7] Osaka City Univ, Grad Sch Engn, Dept Appl Chem, Osaka 5588585, Japan
关键词
D O I
10.1103/PhysRevLett.99.087601
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The magnetism of LixCoO2 (LCO), which has a similar structure to NaxCoO2 (NCO), has been investigated by muon-spin spectroscopy and susceptibility measurements using samples with x=0.1-1 prepared by an electrochemical reaction. In the x range below 0.75, LCO was found to be Pauli paramagnetic down to 1.8 K, suggesting an intermediate- or weak-coupling regime, although disordered local moments, with volume fractions below similar to 20%, appear at low T for LCO with x >= 0.5. The phase diagram and interactions of LCO are thus strikingly different from NCO, while the differences cannot be explained simply by structural differences between the two systems.
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页数:4
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