2023
DOI: 10.1039/d3cp02458j
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NaGdF4:Eu3+ nanocrystalline: an in-depth study of energy transfer processes and Judd–Ofelt analysis using the luminescence excitation spectrum

Phan Van Do,
Nguyen Xuan Ca,
Luong Duy Thanh
et al.

Abstract: NaGdF4 nanocrystalline doped with different concentrations of Eu3+ ion have been synthesized by the precipitation method. The structure and morphology of the material were investigated through the measurements of the...

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Cited by 5 publications
(3 citation statements)
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“…In cubic phase, no splitting in the 5 D 0 → 7 F 1 band is observed, whereas in hexagonal, it splits into two. The band splits into multiple components when the structure is highly unsymmetric, as is our case (monoclinic) . The second-order parameter ( B 20 ) in crystal field expansion plays an important role in the mixing of wave functions and relates to the intensity of the 5 D 0 → 7 F 0 and 5 D 0 → 7 F 2 transitions by the following formula: , I false( 5 normalD 0 5 normalF 0 false) I false( 5 normalD 0 5 normalF 2 false) = 4 B 20 2 75 Δ 20 2 where Δ 20 (cm –1 ) is the energy gap from the 7 F 0 level to the 7 F 2 .…”
Section: Resultsmentioning
confidence: 98%
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“…In cubic phase, no splitting in the 5 D 0 → 7 F 1 band is observed, whereas in hexagonal, it splits into two. The band splits into multiple components when the structure is highly unsymmetric, as is our case (monoclinic) . The second-order parameter ( B 20 ) in crystal field expansion plays an important role in the mixing of wave functions and relates to the intensity of the 5 D 0 → 7 F 0 and 5 D 0 → 7 F 2 transitions by the following formula: , I false( 5 normalD 0 5 normalF 0 false) I false( 5 normalD 0 5 normalF 2 false) = 4 B 20 2 75 Δ 20 2 where Δ 20 (cm –1 ) is the energy gap from the 7 F 0 level to the 7 F 2 .…”
Section: Resultsmentioning
confidence: 98%
“…The band splits into multiple components when the structure is highly unsymmetric, as is our case (monoclinic) . The second-order parameter ( B 20 ) in crystal field expansion plays an important role in the mixing of wave functions and relates to the intensity of the 5 D 0 → 7 F 0 and 5 D 0 → 7 F 2 transitions by the following formula: , I false( 5 normalD 0 5 normalF 0 false) I false( 5 normalD 0 5 normalF 2 false) = 4 B 20 2 75 Δ 20 2 where Δ 20 (cm –1 ) is the energy gap from the 7 F 0 level to the 7 F 2 . For K 3 GdF 6 :5% Eu 3+ , the B 20 parameter is determined to be 691, 916, 900, and 707 cm –1 for K 3 GdF 6 :5% Eu 3+ (as prepared), K 3 GdF 6 :5% Eu 3+ (annealed at 300 °C), K 3 GdF 6 :5% Eu 3+ (annealed at 400 °C), and K 3 GdF 6 :5% Eu 3+ (annealed at 500 °C).…”
Section: Resultsmentioning
confidence: 98%
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