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Phys. Rev. B 73, 054417 (2006) [11 pages]

Magnetic excitations in the Zn-Mg-Tb icosahedral quasicrystal: An inelastic neutron scattering study

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Taku J. Sato*
Neutron Science Laboratory, Institute for Solid State Physics, University of Tokyo, 106-1 Shirakata, Tokai, Ibaraki 319-1106, Japan and SORST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012, Japan

Hiroyuki Takakura
Research Center for Molecular Thermodynamics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan and SORST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012, Japan

An Pang Tsai
Institute of Multidisciplinary Research for Advanced Materials, Tohoku University, Sendai 980-8577, Japan and SORST, Japan Science and Technology Agency, Kawaguchi, Saitama 332-0012, Japan

Kaoru Shibata
Japan Atomic Energy Research Institute, Tokai, Ibaraki 319-1195, Japan

Received 4 October 2005; published 10 February 2006

Low-temperature spin dynamics in the face-centered-icosahedral Zn-Mg-Tb quasicrystal has been investigated by inelastic neutron scattering around its spin-glass-like freezing temperature (Tf≃5.8 K). A single broad inelastic peak, centered at ω≃2.5 meV, was observed in the inelastic scattering spectrum at temperatures ranging from the base temperature up to ∼20 K. The inelastic peak energy is Q independent, whereas the peak intensity shows weak Q dependence, which is qualitatively similar to that observed for the elastic diffuse scattering. The inelasticity of spin excitations is hardly seen in canonical spin glasses and thus is a distinct feature of the Zn-Mg-Tb quasicrystal. We argue, with an aide of numerical simulation, that this broad inelastic peak can be interpreted as localized collective fluctuations of short-range-ordered spins in a dodecahedral spin cluster. In a much lower-energy region (ω<0.8 meV), we observed a strong quasielastic signal, appearing only above Tf; its peak width decreases as the temperature is lowered and vanishes at Tf. It is thus evident that the quasielastic signal corresponds to a slow spin dynamics that freezes at the macroscopic freezing temperature. The coexistence of the inelastic peak and quasielastic signal suggests that the short-range order in the single cluster is robustly formed but is dynamic for Tf<T<20 K. The macroscopic freezing at Tf is, thus, attributed to a random freezing of spin-cluster fluctuations.

© 2006 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.73.054417
DOI:
10.1103/PhysRevB.73.054417
PACS:
75.50.Kj, 61.44.Br, 78.70.Nx

*Electronic address: taku@issp.u-tokyo.ac.jp