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Phys. Rev. B 72, 064418 (2005) [11 pages]

Appearance of a two-dimensional antiferromagnetic order in quasi-one-dimensional cobalt oxides

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J. Sugiyama1,*, H. Nozaki1, J. H. Brewer2, E. J. Ansaldo3, T. Takami4, H. Ikuta4, and U. Mizutani4
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 Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, 464-8603 Japan

Received 18 December 2004; revised 18 March 2005; published 10 August 2005

By means of muon spin rotation and relaxation (μ+SR) techniques, we have investigated the magnetism of quasi-one-dimensional (1D) cobalt oxides An+2Con+1O3n+3 (A=Ca, Sr, and Ba; n=1, 2, 3, 5, and ), in which the 1D CoO3 chain is surrounded by six equally spaced chains forming a triangular lattice in the ab plane, using polycrystalline samples, from room temperature down to 1.8 K. For the compounds with n=1–5, transverse field μ+SR experiments showed the existence of a magnetic transition below ∼100 K, although there were no clear anomalies in the susceptibility-vs-T curve. The onset temperature of the transition (Tcon) was found to decrease with n; from 100 K for n=1 to 60 K for n=5. A damped muon spin oscillation was observed only in the sample with n=1 (Ca3Co2O6), whereas only a fast relaxation obtained even at 1.8 K in the other three samples. Combining the fact that the paramagnetic Curie temperature ranges from −150 to −200 K for the compound with n=2 and 3, the μ+SR result indicates that a two-dimensional (2D) short-range antiferromagnetic (AF) order, which has been thought to be unlikely to exist at high T due to a relatively strong 1D ferromagnetic (F) interaction, appears below Tcon for all compounds with n=1–5; but quasistatic long-range AF order formed only in Ca3Co2O6, below 25 K. For BaCoO3 (n=), as T decreased from 300 K, 1D F order appeared below 53 K, and a sharp 2D AF transition occurred at 15 K.

© 2005 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.72.064418
DOI:
10.1103/PhysRevB.72.064418
PACS:
76.75.+i, 75.40.Cx, 75.50.Ee

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