TY - JOUR
T1 - Electron Energy-Loss Spectroscopy Study of the Electronic Structure ofα-Rhombohedral Boron
AU - Terauchi, Masami
AU - Kawamata, Yosuke
AU - Tanaka, Michiyoshi
AU - Takeda, Masatoshi
AU - Kimura, Kaoru
N1 - Funding Information:
The authors thank Dr. Y. Harada, Mr. M. Ishida, Dr. K. Tsuno and Mr. M. Kai of JEOL Ltd. for their great effort in constructing the high-resolution EELS microscope. They thank Mr. F. Sato for his skillful technical assistance. The present work was partly supported by a Grant-in-Aid from the Ministry of Education, Science, Sports and Culture, Japan.
PY - 1997/10
Y1 - 1997/10
N2 - Electron energy-loss spectra ofα-rhombohedral boron (α-r-B) were obtained from perfect crystalline areas of 180 nm diameter. The onset of the spectral intensity was observed at 2.4 eV (band gap energy). The volume plasmon peak due to thespvalence electrons is at 24.5 eV with a full width at half maximum of 7.5 eV. The real partε1(ω) and imaginary partε2(ω) of the dielectric function were obtained from the loss-function by Kramers-Kronig analysis. The value ofε1(0) was 6.5.ε2(ω) showed clear peaks, not observed inε2(ω) ofβ-rhombohedral boron (β-r-B) and amorphous boron (am-B). K-shell excitation spectra show several peaks, which are not observed in the spectra ofβ-r-B and am-B. The characteristic structure of the peaks showed good agreement with a recentab initiocalculation within the local density approximation.
AB - Electron energy-loss spectra ofα-rhombohedral boron (α-r-B) were obtained from perfect crystalline areas of 180 nm diameter. The onset of the spectral intensity was observed at 2.4 eV (band gap energy). The volume plasmon peak due to thespvalence electrons is at 24.5 eV with a full width at half maximum of 7.5 eV. The real partε1(ω) and imaginary partε2(ω) of the dielectric function were obtained from the loss-function by Kramers-Kronig analysis. The value ofε1(0) was 6.5.ε2(ω) showed clear peaks, not observed inε2(ω) ofβ-rhombohedral boron (β-r-B) and amorphous boron (am-B). K-shell excitation spectra show several peaks, which are not observed in the spectra ofβ-r-B and am-B. The characteristic structure of the peaks showed good agreement with a recentab initiocalculation within the local density approximation.
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U2 - 10.1006/jssc.1997.7336
DO - 10.1006/jssc.1997.7336
M3 - Article
AN - SCOPUS:0001085753
SN - 0022-4596
VL - 133
SP - 156
EP - 159
JO - Journal of Solid State Chemistry
JF - Journal of Solid State Chemistry
IS - 1
ER -