2022
DOI: 10.1016/j.radphyschem.2022.110284
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Luminescence and Judd-Ofelt analysis of gallium aluminum gadolinium yttrium borate scintillating glass doped with Dy3+

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Cited by 11 publications
(4 citation statements)
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“…The emission spectra under Gd 3+ excitation (λ Ex = 275 nm) in Fig. 5(b) represent the intensely sharp peak of Gd 3+ at 311 nm ( 6 P 7/2 → 8 S 7/2 ), 1,2,7,8,11,12) which matched to the excitation peak at 312 nm ( ) and 752 ( 4 F 9/2 → 6 H 9/2 ) nm 1,[7][8][9][10][11][12]21) were also observed and they were weak compared to Gd 3+ emission. After the excited Gd 3+ ion lowered its energy level from 6 I 7/2 to 6 P 7/2 by non-radiative relaxation (NR), the energy transfer (ET) then occurred from 6 P 7/2 of Gd 3+ to 4 L 19/2 of Dy 3+ as shown in Fig.…”
Section: Photoluminescence Spectra and Decay Curvesmentioning
confidence: 88%
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“…The emission spectra under Gd 3+ excitation (λ Ex = 275 nm) in Fig. 5(b) represent the intensely sharp peak of Gd 3+ at 311 nm ( 6 P 7/2 → 8 S 7/2 ), 1,2,7,8,11,12) which matched to the excitation peak at 312 nm ( ) and 752 ( 4 F 9/2 → 6 H 9/2 ) nm 1,[7][8][9][10][11][12]21) were also observed and they were weak compared to Gd 3+ emission. After the excited Gd 3+ ion lowered its energy level from 6 I 7/2 to 6 P 7/2 by non-radiative relaxation (NR), the energy transfer (ET) then occurred from 6 P 7/2 of Gd 3+ to 4 L 19/2 of Dy 3+ as shown in Fig.…”
Section: Photoluminescence Spectra and Decay Curvesmentioning
confidence: 88%
“…Especially the absorption at 317 nm (average) inside this board hump, possibly originated from the 8 S 7/2 → 6 P 7/2 transition of the Gd 3+ ion. 1,2,8,11,12) The Dy 3+ 8,9,12) The dominance of this absorption transition revealed the low-symmetric environment around Dy 3+ in the glass structure. The strength of most absorption peaks for Dy 3+ tends to increase with added Dy 2 O 3 content.…”
Section: Absorption Spectramentioning
confidence: 99%
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