TY - JOUR
T1 - Electron-energy-loss spectroscopy study of the electronic structure of a stable decagonal quasicrystal Al70Ni15Co15
AU - Terauchi, Masami
AU - Ueda, Hiroshi
AU - Tanaka, Michiyoshi
AU - Tsai, An Pang
AU - Inoue, Akihisa
AU - Masumoto, Tsuyoshi
N1 - Copyright:
Copyright 2016 Elsevier B.V., All rights reserved.
PY - 1998/6
Y1 - 1998/6
N2 - Electron-energy-loss spectra of a stable decagonal quasicrystal Al70Ni15Co15have been obtained from single-quasicrystal areas of 180 nm diameter. Excitationspectra Al L-shell electrons (L edge) show a sharp onset (Fermi edge) but asmall rise in intensity, indicating the presence of a pseudogap. The onset energyof Al L-edge spectra of the quasicrystal is higher than that of aluminium by0.4 eV, indicating an increase in the covalent nature in the bonding of thequasicrystalline phase as shown earlier by Terauchi et al. The spectra ofvalence electron excitation exhibit a volume plasmon peak at 17.0 eV with afull width at half-maximum (FWHM) value of 5.4 eV. The width showsa stronger damping of the volume plasmon than those sp metals (FWHM, 0.41.5 eV) and sp semiconductors (FWHM, 3-4eV). The origin of the strongdamping is attributed to interband transitions of the d electrons.
AB - Electron-energy-loss spectra of a stable decagonal quasicrystal Al70Ni15Co15have been obtained from single-quasicrystal areas of 180 nm diameter. Excitationspectra Al L-shell electrons (L edge) show a sharp onset (Fermi edge) but asmall rise in intensity, indicating the presence of a pseudogap. The onset energyof Al L-edge spectra of the quasicrystal is higher than that of aluminium by0.4 eV, indicating an increase in the covalent nature in the bonding of thequasicrystalline phase as shown earlier by Terauchi et al. The spectra ofvalence electron excitation exhibit a volume plasmon peak at 17.0 eV with afull width at half-maximum (FWHM) value of 5.4 eV. The width showsa stronger damping of the volume plasmon than those sp metals (FWHM, 0.41.5 eV) and sp semiconductors (FWHM, 3-4eV). The origin of the strongdamping is attributed to interband transitions of the d electrons.
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U2 - 10.1080/095008398178336
DO - 10.1080/095008398178336
M3 - Article
AN - SCOPUS:0032092531
SN - 0950-0839
VL - 77
SP - 351
EP - 357
JO - Philosophical Magazine Letters
JF - Philosophical Magazine Letters
IS - 6
ER -