Phys. Rev. B 68, 224421 (2003) [9 pages]

Onset of antiferromagnetism in UPt3 via Th substitution studied by muon spin spectroscopy

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M. J. Graf1, A. de Visser2, C. P. Opeil1, J. C. Cooley3, J. L. Smith3, A. Amato4, C. Baines4, F. Gygax5, and A. Schenck5
1Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467, USA
2Van der Waals-Zeeman Institute, University of Amsterdam, 1018 XE Amsterdam, The Netherlands
3Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
4Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland
5Institute for Particle Physics of ETH Zürich, PSI CH-5232 Villigen, Switzerland

Received 27 June 2003; revised 8 September 2003; published 22 December 2003

Muon spin spectroscopy has been used to study in detail the onset of large-moment antiferromagnetism (LMAF) in UPt3 as induced by Th substitution. Zero-field experiments have been carried out on a series of polycrystalline U1-xThxPt3 (0<~x<~0.05) samples in the temperature range 0.04–10 K. At low Th content (x<~0.002) magnetic ordering on the time scale of the μSR experiment (10-8 s) is not detected. For x=0.005 a weak magnetic signal appears below T=2 K, while for 0.006<~x<~0.05, spontaneous oscillations in the μSR spectra signal the presence of the LMAF phase. The data are well described by a two-component depolarization function, combining the contribution of a polycrystalline antiferromagnet and a Kubo-Lorentzian response. However, the transition into the antiferromagnetic phase is quite broad. For x=0.01 and 0.02, a weak magnetic signal appears below about 7 K, which is well above the mean-field transition temperatures. The broadening may be a result of the effects of disorder on the time fluctuations associated with anomalous small-moment antiferromagnetism.


©2003 The American Physical Society

URL: http://link.aps.org/abstract/PRB/v68/e224421
DOI: 10.1103/PhysRevB.68.224421
PACS: 75.30.Kz, 71.27.+a, 74.70.Tx, 76.75.+i

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