1999
DOI: 10.1007/s100510050640
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Inelastic neutron scattering study of the dynamics of the AlNiCo decagonal phase

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Cited by 33 publications
(22 citation statements)
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“…In the range of 0.3 to 0.6 Å À1 one observes a rapid broadening of the observed excitation, whereas the dispersion relation bends over. 48,[50][51][52] This generally corresponds to the crossing of the acoustic branch with a dispersionless broad optical excitation or to a pseudo-gap opening as in the case of the i-Zn-Mg-Sc quasicrystal shown in Fig. 4.…”
Section: Phonons In Quasicrystalsmentioning
confidence: 96%
See 1 more Smart Citation
“…In the range of 0.3 to 0.6 Å À1 one observes a rapid broadening of the observed excitation, whereas the dispersion relation bends over. 48,[50][51][52] This generally corresponds to the crossing of the acoustic branch with a dispersionless broad optical excitation or to a pseudo-gap opening as in the case of the i-Zn-Mg-Sc quasicrystal shown in Fig. 4.…”
Section: Phonons In Quasicrystalsmentioning
confidence: 96%
“…51 For all phases there is a well defined acoustic mode for wavevectors smaller than 0.3 Å À1 with a width limited by the instrumental resolution and a linear dispersion. In the range of 0.3 to 0.6 Å À1 one observes a rapid broadening of the observed excitation, whereas the dispersion relation bends over.…”
Section: Phonons In Quasicrystalsmentioning
confidence: 99%
“…6,7 However, it is only recently that there has been increasing evidence for nonacoustic low-energy states that show up in the phonon DOS ͑Refs. 15 and 28, in excess heat capacity 11 or in an atypical low-temperature variation of the sound velocity.…”
Section: F Nonacoustic Excitations At Low Energiesmentioning
confidence: 99%
“…To measure the largest signal one should measure S(Q,) at high momentum transfer and close to a strong Bragg peak. Neutron scattering investigations were performed for different icosahedral [12][13][14][15] and decagonal 16 structures and it turned out that in spite of the fact that, structurally, decagonal and icosahedral QCs are rather different, and that their physical properties ͑e.g., elastic moduli͒ might be also very different, they exhibit many common vibrational features. The purpose of our paper is to propose a simple phenomenological model to try to obtain as much theoretical information concerning vibrations in QCs as is possible on a phenomenological level without specific microscopic treatment.…”
Section: Introductionmentioning
confidence: 99%