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Phys. Rev. B 69, 214423 (2004) [7 pages]

Electron correlation in the two-dimensional triangle lattice of NaxCoO2

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J. Sugiyama1,*, J. H. Brewer2, E. J. Ansaldo3, B. Hitti3, M. Mikami4,†, Y. Mori4, and T. Sasaki4
1Toyota Central Research and Development Laboratories Inc., Nagakute, Aichi 480-1192, Japan
2TRIUMF, CIAR and Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1
3TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia, Canada V6T 2A3
4Department of Electrical Engineering, Osaka University, Suita, Osaka 563-8577, Japan

Received 2 October 2003; published 24 June 2004

Magnetism of layered cobaltites NaxCoO2 with x=0.6 and 0.9 has been investigated by a positive muon spin rotation and relaxation (μ+SR) spectroscopy together with magnetic susceptibility and specific-heat measurements, using single-crystal samples in the temperature range between 250 and 1.8 K. Zero-field-(ZF-) μ+SR measurements on Na0.9CoO2 indicate a transition from a paramagnetic to an incommensurate spin-density wave state (IC-SDW) at 19 K(=TSDW). The anisotropic ZF-μ+SR spectra suggest that the oscillating moments of the IC-SDW direct along the c axis. Since Na0.6CoO2 is paramagnetic down to 1.8 K, the magnitude of TSDW is found to strongly depend on x. This behavior is well explained using the Hubbard model within a mean-field approximation on two-dimensional triangular lattice in the CoO2 plane. Also, both the appearance of the IC-SDW state by the change in x and the magnitude of the electronic specific-heat parameter of Na0.6CoO2 indicate that NaxCoO2 is unlikely to be a typical strongly correlated electron system.

© 2004 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.69.214423
DOI:
10.1103/PhysRevB.69.214423
PACS:
76.75.+i, 75.30.Fv, 72.15.Jf, 65.40.Ba

*Electronic address: e0589@mosk.tytlabs.co.jp

Present address: National Institute of Advanced Industrial Science and technology, Ikeda, Osaka 563-8577, Japan.