2012
DOI: 10.1016/j.jallcom.2012.02.105
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Preparation and characteristics of core–shell structure Y3Al5O12:Yb3+@SiO2 nanoparticles

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Cited by 15 publications
(3 citation statements)
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“…Figure 11a also depicts that the higher the thickness of YAG:Ce shell, the higher is the maximum intensity in the PL spectrum. As can be seen, SiO 2 @YAG:Ce (1.0 at.% Ce) nanoparticles show the highest emission, compared to commercial and synthesized SiO 2 /YAG:Ce mixture composite, that is in agreement with similar works in this field [20][21][22][48][49][50][51]. The increased PL intensity of YAG:Ce in the core-shell state is believed to result from the inhibition of surface states in YAG:Ce nanoparticles and the higher light extraction at the SiO 2 /YAG:Ce interface.…”
Section: Photoluminescence (Pl) and Diffuse Transmission Spectra (Dtssupporting
confidence: 90%
“…Figure 11a also depicts that the higher the thickness of YAG:Ce shell, the higher is the maximum intensity in the PL spectrum. As can be seen, SiO 2 @YAG:Ce (1.0 at.% Ce) nanoparticles show the highest emission, compared to commercial and synthesized SiO 2 /YAG:Ce mixture composite, that is in agreement with similar works in this field [20][21][22][48][49][50][51]. The increased PL intensity of YAG:Ce in the core-shell state is believed to result from the inhibition of surface states in YAG:Ce nanoparticles and the higher light extraction at the SiO 2 /YAG:Ce interface.…”
Section: Photoluminescence (Pl) and Diffuse Transmission Spectra (Dtssupporting
confidence: 90%
“…To resolve this problem, besides other well-established techniques, the method based on semiconductor photocatalysts is a promising solution to degrade organic pollutants in wastewater [1][2][3][4][5]. To date, the semiconductor TiO 2 has undoubtedly proven to be one of the most excellent photocatalysts for the oxidative decomposition of many organic compounds [6][7][8]. Unfortunately, due to its wide band-gap of 3.2 eV, TiO 2 can only responds to ultraviolet irradiation but not to visible light that accounts for 43% of the incoming solar energy [9].…”
Section: Introductionmentioning
confidence: 99%
“…Notably, except excited by the 980 nm, the Yb 3+ ions can also be excited at 940 and 915 nm lasers and then transfer energy to Ho 3+ ions by ET process [32][33]. To further explore the in uence of different excitation sources on the emission spectra for the SrF 2 :Yb 3+ /Ho 3+ NCs, we further investigate the photoluminescence properties of SrF 2 :Yb 3+ /Ho 3+ (12/0.1 mol%) NCs under the 980, 940 and 915 nm excitations with the same pumping power density (11 W cm -2 ), as shown in Figure 4.…”
Section: And Ucl Propertiesmentioning
confidence: 99%