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Bulk antiferromagnetism in Na0.82CoO2 single crystals

MPS-Authors
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Bayrakci,  S. P.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Bernhard,  C.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Chen,  D. P.
Scientific Facility Crystal Growth (Masahiko Isobe), Max Planck Institute for Solid State Research, Max Planck Society;

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Keimer,  B.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Kremer,  R. K.
Former Scientific Facilities, Max Planck Institute for Solid State Research, Max Planck Society;

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Lemmens,  P.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Lin,  C. T.
Scientific Facility Crystal Growth (Masahiko Isobe), Max Planck Institute for Solid State Research, Max Planck Society;

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Strempfer,  J.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Citation

Bayrakci, S. P., Bernhard, C., Chen, D. P., Keimer, B., Kremer, R. K., Lemmens, P., et al. (2004). Bulk antiferromagnetism in Na0.82CoO2 single crystals. Physical Review B, 69(10): 100410(R).


Cite as: https://hdl.handle.net/21.11116/0000-000E-FF95-B
Abstract
Susceptibility, specific heat, and muon spin rotation measurements on
high-quality single crystals of Na0.82CoO2 have revealed bulk
antiferromagnetism with Neel temperature T-N=19.8+/-0.1 K and an
ordered moment perpendicular to the CoO2 layers. The magnetic order
encompasses nearly 100% of the crystal volume. The susceptibility
exhibits a broad peak around 30 K, characteristic of two-dimensional
antiferromagnetic fluctuations. The in-plane resistivity is metallic at
high temperatures and exhibits a minimum at T-N.