Vibrational Spectra of the "One-Mode" (Y(1-x)La(x))(2)O(3) Solid Solution Ceramics

单模 (Y(1-x)La(x))(2)O(3) 固溶体陶瓷的振动光谱

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Abstract

Y(2)O(3) is widely used in IR windows and optoelectronics, but its vibrational and spectral properties under La(3+) substitutions remain unclear. This work investigates xLa(2)O(3)-(1-x)Y(2)O(3) with x = 0-0.2 via XRD, SEM, Raman, and IR spectroscopy to address the lack of comprehensive data on structure-property correlations. The solid solution (Y(1-x)La(x))(2)O(3) with 0 ≤ x < 0.15 was determined. The cell parameter a increases from 10.6113(5) Å to 10.7116(1) Å as x increases from 0 to 0.15 according to the Rietveld refinements. Both the Raman spectra and infrared (IR) reflection spectra show that (Y(1-x)La(x))(2)O(3) is a "one-mode" system, in which eight of the 22 theoretical first-order Raman modes and 12 of 16 theoretical IR modes for the (Y(1-x)La(x))(2)O(3) are recognized. A local vibrational mode at approximately 680 cm(-1) is observed in the Raman spectra as x > 0. The Raman modes and IR modes of (Y(1-x)La(x))(2)O(3) show red shift and obvious peak broadening as x increases, which is caused by the expansion of unit cell and local distortions of the crystal structure. As Y(3+) is substituted by La(3+), the extinction coefficient κ decreases significantly, which can lead to a lower IR absorption and should be beneficial for the IR window applications.

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