2017
DOI: 10.1016/j.optmat.2017.04.046
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Polarized spectral properties of Sm:CaGdAlO 4 crystal for reddish-orange laser

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Cited by 16 publications
(3 citation statements)
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“…The calculated Ω 2 , Ω 4 , and Ω 6 for Sm 3+ ‐doped YSZ are 5.46 × 10 −20 cm 2 , 10.70 × 10 −20 cm 2 , and 12.67 × 10 −20 cm 2 respectively. It should be noted that the magnitude of Ω 2 is inversely related to the site symmetry, but directly proportional to degree of covalency, whilst Ω 4 and Ω 6 are related to the viscosity and rigidity of the matrix . In the present study, the trend in Ω t was in the order Ω 2 < Ω 4 < Ω 6 , which is the same as that reported by Gurushantha et al for nanocrystalline samples, and is consistent with the conclusion from analysis of the emission data of a relatively high symmetry at the Sm 3+ site.…”
Section: Resultssupporting
confidence: 92%
See 1 more Smart Citation
“…The calculated Ω 2 , Ω 4 , and Ω 6 for Sm 3+ ‐doped YSZ are 5.46 × 10 −20 cm 2 , 10.70 × 10 −20 cm 2 , and 12.67 × 10 −20 cm 2 respectively. It should be noted that the magnitude of Ω 2 is inversely related to the site symmetry, but directly proportional to degree of covalency, whilst Ω 4 and Ω 6 are related to the viscosity and rigidity of the matrix . In the present study, the trend in Ω t was in the order Ω 2 < Ω 4 < Ω 6 , which is the same as that reported by Gurushantha et al for nanocrystalline samples, and is consistent with the conclusion from analysis of the emission data of a relatively high symmetry at the Sm 3+ site.…”
Section: Resultssupporting
confidence: 92%
“…Introduction of Sm 3+ into the YSZ host causes the degenerate energy level to split as a result of the influence of the Coulomb field and covalent overlap of the 4 f electron shell with ligand electron shells. The strong absorption bands at around 364, 406, 421, 466, 1071, 1219, 1347, and 1474 nm have been reported to correspond to transitions from the 6 H 5/2 ground state to the excited states 4 D 1/2 + 4 L 17/2 + 6 P 7/2 + 4 K 13/2 + 4 F 9/2 + 4 D 3/2 (364 nm), 4 G 11/2 + 4 L 15/2 + 4 K 11/2 + 6 P 3/2 + 4 F 7/2 + 4 L 13/2 + 6 P 5/2 + 4 P 5/2 (406 nm), 4 F 5/2 + 4 I 5/2 + 4 G 9/2 + 4 M 17/2 (421 nm), 4 G 7/2 + 4 I 9/2 + 4 M 15/2 + 4 I 11/2 + 4 I 13/2 (466 nm), 6 F 9/2 (1071 nm), 6 F 7/2 (1219 nm), 6 F 5/2 (1347 nm), and 6 F 3/2 + 6 H 15/2 + 6 F 1/2 (1474 nm) respectively. The appearance of these absorption peaks demonstrates that the Sm 3+ modified YSZ crystals have good responses to light in the visible‐NIR region.…”
Section: Resultsmentioning
confidence: 99%
“…The average decay time of the sample is then defined by (6) [49]: The fluorescence lifetimes for the 4 G5/2 → 6 H7/2 emission peak from YGG: Sm 3+ and YAG: Sm 3+ single crystals were then calculated to be 0.705 ms and 0.466 ms, respectively (Table 4). Thus, the fluorescence lifetime of YGG: Sm 3+ is not only longer than that of the YAG: Sm 3+ crystal, but it is also longer than those of CaGdAlO4: Sm 3+ (0.69 ms) and NaGd(MnO4): Sm 3+ crystals (0.5574 ms) [18,52,53]; this is probably the consequence of the greater intensity of its 4 G5/2 → 6 H7/2 emission peak, which allows for a greater participation of Sm 3+ ions in this transition and results in a longer fluorescence lifetime [54,55].…”
Section: Fluorescence Lifetime Measurementsmentioning
confidence: 93%