2017
DOI: 10.1016/j.ceramint.2016.12.032
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Improved photoluminescence properties of BaAl 2 Si 2 O 8 :Eu 3+ ,Tb 3+ phosphors by doping Tb 3+

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Cited by 35 publications
(4 citation statements)
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“…The excitation spectrum at 612 nm consisted of a broadband peak and a set of sharp line peaks. The broadband peak was 200–330 nm, originating from O 2− → Eu 3+ charge migration [16, 17]; the broadband peak of the excitation image at 544 nm was located at 200–320 nm, which was caused by 4f 8 –4f 7 5d 1 due to the Tb 3+ spin [4, 21, 22]; Figure 7b,c shows the emission spectrum of LMA:2%Tb 3+ , 5%Eu 3+ under an excitation of 274‐nm ultraviolet light, with weak emission bands, located at 438 nm ( 5 D 3 → 7 F 4 ), 451 nm ( 5 D 3 → 7 F 3 ), and 467 nm ( 7 F 0 → 5 D 2 ), showing the transition in the blue region [23]. These weak emission bands were due to the fact that the low‐energy multiphonon vibrations of AlO 4 − and AlO 4 2− groups in the lattice cannot completely bridge the high‐energy states of Eu 3+ and Tb 3+ ( 5 D 3 , 5 D 2 , 5 D 0 ) energy levels, so these emission peaks were very weak [2]; the figure shows that the characteristic peaks of Tb 3+ were 486 nm ( 5 D 4 → 7 F 6 ) and 544 nm ( 5 D 4 → 7 F 5 ) [21, 22] and the characteristic peaks of Eu 3+ were 577 nm ( 5 D 0 → 7 F 0 ), 588 nm ( 5 D 0 → 7 F 1 ), and 614 nm ( 5 D 0 → 7 F 2 ) [16, 17, 24, 25].…”
Section: Resultsmentioning
confidence: 99%
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“…The excitation spectrum at 612 nm consisted of a broadband peak and a set of sharp line peaks. The broadband peak was 200–330 nm, originating from O 2− → Eu 3+ charge migration [16, 17]; the broadband peak of the excitation image at 544 nm was located at 200–320 nm, which was caused by 4f 8 –4f 7 5d 1 due to the Tb 3+ spin [4, 21, 22]; Figure 7b,c shows the emission spectrum of LMA:2%Tb 3+ , 5%Eu 3+ under an excitation of 274‐nm ultraviolet light, with weak emission bands, located at 438 nm ( 5 D 3 → 7 F 4 ), 451 nm ( 5 D 3 → 7 F 3 ), and 467 nm ( 7 F 0 → 5 D 2 ), showing the transition in the blue region [23]. These weak emission bands were due to the fact that the low‐energy multiphonon vibrations of AlO 4 − and AlO 4 2− groups in the lattice cannot completely bridge the high‐energy states of Eu 3+ and Tb 3+ ( 5 D 3 , 5 D 2 , 5 D 0 ) energy levels, so these emission peaks were very weak [2]; the figure shows that the characteristic peaks of Tb 3+ were 486 nm ( 5 D 4 → 7 F 6 ) and 544 nm ( 5 D 4 → 7 F 5 ) [21, 22] and the characteristic peaks of Eu 3+ were 577 nm ( 5 D 0 → 7 F 0 ), 588 nm ( 5 D 0 → 7 F 1 ), and 614 nm ( 5 D 0 → 7 F 2 ) [16, 17, 24, 25].…”
Section: Resultsmentioning
confidence: 99%
“…In recent years, phosphors doped with rare earth ions to achieve white light emission using aluminate as the substrate have advantages such as high color index, high quantum efficiency, wide excitation range, light emission in the visible range, and low cost; these phosphors are the widely studied fluorescent materials [2]. Of these, Eu 3+ and Tb 3+ are widely used because of advantages such as rich electronic energy levels, high light conversion rate, sharp linear bands, and high luminescence color purity [3,4]. Min et al [5] prepared orange-red phosphor LaMgAl 11 O 19 :Sm 3+ using the high-temperature solid-state method and studied its phase composition, crystal structure, thermal stability, and luminescence properties; Wen et al [6] prepared yellow-red phosphor LaMgAl 11 O 19 :Dy 3+ using the solid-state method.…”
Section: Introductionmentioning
confidence: 99%
“…When the concentration is 0.003, the luminous intensity is at the highest value. Due to the effect of concentration quenching, the luminous intensity of phosphor decreases with the increasing of Mn 4+ concentration [34]. [29,38,39].…”
Section: Photoluminescence Propertiesmentioning
confidence: 99%
“…As the synthesis temperature was changed from 1,000 C to 1,300 C, the intensities of the three emission peaks of Sr ions in the Sr 2-x SiO 4 -xEu phosphors, it is necessary to consider the critical concentration of the Eu 3+ ions, the volume of the unit cell, and the number of cations in the unit cell and then calculating the critical energy transfer distance. [28][29][30] The critical energy transfer distance (R o ) for the concentration quenching in the Sr 2-x SiO 4 -xEu phosphors can be calculated using the formula: R o = 2[(3 V)/(4πx c N)] 1/3 , where N,…”
mentioning
confidence: 99%