Journal
DIAMOND AND RELATED MATERIALS
Volume 18, Issue 9, Pages 1123-1128Publisher
ELSEVIER SCIENCE SA
DOI: 10.1016/j.diamond.2009.02.025
Keywords
B-C; BC3; BC2N; Superhard; Raman scattering
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Funding
- U.S. Department of Energy [DE-FG02-07ER46408]
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Ultraviolet (UV) Raman and visible Raman spectroscopies were applied to study the graphitic BCx (g-BCx) phases. The Raman spectra of the g-BCx phases excited with UV laser at 244 nm have one main peak: a G peak (approximately at 1590 cm(-1)), and do not have the D peak (around 1350 cm(-1)) characteristic for Raman spectra of disordered graphitic phases. The D peak can be detected in all g-BCx phases when green (534 nm) or near-infrared (785 nm) lasers are used for Raman scattering excitation. The positions of the G and D peaks were found to be independent (within the experimental errors) of the B/C ratio. The pattern of the peaks in UV Raman spectra of g-BC2.1 phase indicates that the additional peaks centered at 1089 cm(-1) should be assigned to the E-g mode of B4C vibration rather than to the T mode characteristic to amorphous graphite, The high signal-to-noise (S/N) ratio and lack of fluorescence of the UV Raman spectra allow an accurate measure of bandwidth and frequency of the G peaks. (C) 2009 Elsevier B.V. All rights reserved.
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