2012
DOI: 10.1103/physrevb.86.214305
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Vibrational dynamics of single-crystal YVO4studied by polarized micro-Raman spectroscopy andab initiocalculations

Abstract: The vibrational properties of yttrium orthovanadate (YVO 4) single crystals, with tetragonal zircon structure, have been investigated by means of polarized micro-Raman spectroscopy and ab initio calculations. Raman spectra were taken at different polarizations and orientations carefully set by the use of a micromanipulator, so that all of the twelve Raman-active modes, expected on the basis of the group theory, were selected in turn and definitively assigned in wave number and symmetry. In particular the E g (… Show more

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Cited by 22 publications
(10 citation statements)
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References 48 publications
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“…These modes, and especially the two translational modes, are also absent in most of the Raman scattering measurements performed in other orthovanadates probably due to their weak Raman scattering cross-section [37,38]. Curiously, they have been found recently in polarized Raman measurements in YVO 4 at ambient pressure [39]. [14].…”
Section: A Raman Experimentsmentioning
confidence: 83%
“…These modes, and especially the two translational modes, are also absent in most of the Raman scattering measurements performed in other orthovanadates probably due to their weak Raman scattering cross-section [37,38]. Curiously, they have been found recently in polarized Raman measurements in YVO 4 at ambient pressure [39]. [14].…”
Section: A Raman Experimentsmentioning
confidence: 83%
“…We will start with the zircon-type structure. Different authors have performed a detailed group-theoretical analysis of phonons in the zircon-type structure [66,77]. In order to describe this structure a primitive cell can be chosen with only two formula units.…”
Section: Raman and Ir Spectramentioning
confidence: 99%
“…The external vibration at 157 cm −1 (B 1g (1)) can be attributed to the O–Y–O bending mode. The internal vibrations, which can be ascribed to the O–V–O bending and VO 4 stretching modes, are located at higher frequencies: 259 (B 2g ), 376 (A 1g (1)), 488 (B 1g (3)), 812 (B 1g (4)), 835 (E g (5)) and 888 cm −1 (A 1g (2)) 43 . The observed spectrum is dominated by the totally symmetrical vibration of VO 4 3− tetrahedron 32 .…”
Section: Resultsmentioning
confidence: 99%