Journal
JOURNAL OF THE AMERICAN CERAMIC SOCIETY
Volume 104, Issue 4, Pages 1797-1805Publisher
WILEY
DOI: 10.1111/jace.17603
Keywords
phonons; Raman spectroscopy; yttrium; yttrium compounds
Categories
Funding
- Fundamental Research Funds for the Central Universities [G2019KY05103, G2020KY05103]
- Natural Science Foundation of Shaanxi Province [2020JM-117]
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In this study, the vibrational modes and lattice dynamics of C-type Y2O3 ceramics were investigated using vibrational spectra and DFT calculations. The frequency, phonon band structure, and density of phonon states were characterized, revealing the influence of different elements on the vibrational modes.
C-type Y2O3 ceramics (relative density similar to 94%) were prepared at 1500 degrees C for 2 hours with 1% wt. ZnO as sintering aid. The cell parameters of Y2O3 from Rietveld refinements are a = 10.6113(1) angstrom, V = 1194.8(1) angstrom(3). The vibrational modes / lattice dynamics of Y2O3 were investigated using vibrational spectra (Raman and infrared reflection spectra) and first-principle (DFT) calculations. Eight of the 22 predicted first-order Raman modes and 12 of 16 predicted IR modes are observed and reliably assigned. For the observed vibrational modes, an excellent linearity (f(exp) = 1.023f(theo), R-2 = 0.9999) between frequency from calculations (f(theo)) and that from measurements (f(exp)) is observed. Accordingly, the corrected frequency (f(cor)) of vibrational modes, phonon band structure, and density of phonon states (DOPS) of Y2O3 are presented, in which, the frequency of phonons of Y2O3 is <= 625.2 cm(-1) (wavelength >= 16.0 mu m) with a gap of 30.6 cm(-1) from 486.0 to 516.6 cm(-1) (wavelength 20.6 - 19.4 mu m) at room temperature. The modes with f(theo) >= 292.5 cm(-1) (f(cor) >= 299.2 cm(-1)) are dominated by the vibrations of O2- (light atom vibrations) and the vibrational modes with f(theo) <= 239.0 cm(-1) (f(cor) <= 244.5 cm(-1)) are dominated by the vibrations of both Y3+ and O2- (co-vibrations). The three modes T-u((7)) at 301.6 cm(-1), T-u((10)) at 333.7 cm(-1), and T-u((12)) at 369.7 cm(-1) of Y-O stretch vibrations dominate the phonon dielectric constant and dielectric loss of Y2O3 with more than 85% contributions.
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