2011
DOI: 10.1016/j.jssc.2011.02.018
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Phonons in isostructural (ND,Yb):Y Gd1−(VO4) laser crystals: A Raman scattering study

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Cited by 12 publications
(4 citation statements)
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“…The additional IR peak is assigned to the asymmetric stretching vibration (ν 3 ) of VO 4 groups, demonstrating the formation of VO 4 groups. Likewise, we also conduct Raman spectra of KBCP 2– x V x ( x = 0 and 0.2) samples (Figure b) and clearly observe Raman peaks of bending vibrations (385 (ν 2 ) and 341 (ν 2 ) cm –1 ) and stretching vibrations (914 (ν 1 ), 855 (ν 3 ), and 821 (ν 3 ) cm –1 ) of VO 4 groups in the x = 0.2 sample when compared with the x = 0 sample, supporting the results of IR spectra. These findings corroborate our idea that the replacement of P 5+ in the KBCP compound with V 5+ ions is capable of affording the desired VO 4 groups.…”
Section: Resultssupporting
confidence: 79%
“…The additional IR peak is assigned to the asymmetric stretching vibration (ν 3 ) of VO 4 groups, demonstrating the formation of VO 4 groups. Likewise, we also conduct Raman spectra of KBCP 2– x V x ( x = 0 and 0.2) samples (Figure b) and clearly observe Raman peaks of bending vibrations (385 (ν 2 ) and 341 (ν 2 ) cm –1 ) and stretching vibrations (914 (ν 1 ), 855 (ν 3 ), and 821 (ν 3 ) cm –1 ) of VO 4 groups in the x = 0.2 sample when compared with the x = 0 sample, supporting the results of IR spectra. These findings corroborate our idea that the replacement of P 5+ in the KBCP compound with V 5+ ions is capable of affording the desired VO 4 groups.…”
Section: Resultssupporting
confidence: 79%
“…The spectroscopic investigation of SRS in tetragonal GdVO 4 singles crystal at “helium temperature” yielded the manifestation of several cascaded and cross‐cascaded χ (3) ‐nonlinear effects under participation of four fundamental ( ω SRS1 ≈ 887 cm −1 , ω SRS2 ≈ 812 cm −1 , ω SRS3 ≈ 823 cm −1 , ω SRS7 ≈ 385 cm −1 ) and two combined ( ω SRS5C ≈ 1699 cm −1 and ω SRS6C ≈ 75 cm −1 ) SRS‐promoting phonon modes, where the fundamental mode with energy of ω SRS3 ≈ 823 cm −1 was observed for the first time. Despite the fact that the vibration properties of REVO 4 crystals having the D4h19‐tetragonal zircon (ZrSiO 4 )‐type structure are well studied (see, e.g., ) and earlier discovered “room‐temperature” SRS modes had been reliably assigned to their fundamental phonon modes (see. e.g., ), we now briefly consider the vibrational nature of the aforementioned “helium‐temperature” χ (3) ‐active modes.…”
Section: Spectra Of χ(3)‐nonlinear Lasingmentioning
confidence: 99%
“…Table 2 Their frequencies are very close in the free complex and are more than twice less than the frequency of stretching mode ν 1 . In crystals the characteristic frequency ranges of these modes are: A 1 (ν 1 ) -800-900, E(ν 2 ) -300-450, F 2 (ν 3 ) -700-900, F 2 (ν 4 ) -300-450 см -1 [24][25][26][27][28][29][30]. In aqueous solutions of (VO 4 ) 3− containing salts the frequencies are:…”
Section: Group Theoretical Analysis and Polarization Rulesmentioning
confidence: 99%