2015
DOI: 10.1039/c5cp05130d
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Engineering oxygen vacancies towards self-activated BaLuAlxZn4−xO7−(1−x)/2photoluminescent materials: an experimental and theoretical analysis

Abstract: Novel self-activated yellow-emitting BaLuAl x Zn 4Àx O 7À(1Àx)/2 photoluminescent materials were investigated by a combined experimental and theoretical analysis. The effects of Al/Zn composition modulation, calcination atmosphere and temperature on the crystal structure and photoluminescence properties have been studied via engineering oxygen vacancies. Accordingly, BaLuAl 0.91 Zn 3.09 O 7 prepared in an air atmosphere was found to be the stable crystalline phase with optimal oxygen content and gave a broad y… Show more

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Cited by 70 publications
(24 citation statements)
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“…The curve shape of CL 0.9 AB: x Sm 3+ was comparable to that of the host due to weak f–f transitions of Sm 3+ ions, while the bands in the range of 272–380 nm were observed for CL 0.9– x AB:0.1Ce 3+ , x Sm 3+ , ascribed to f–d absorptions of Ce 3+ ions. Generally, the band gap of the host material can be determined with the use of the following relation , where hv is the photon energy, A is the proportionality constant, and E g is the band gap. The values of n = 1/2 and n = 2 indicate the indirect and direct transitions respectively, and the F ( R ∞ ) value represents the Kubelka–Munk function, which is well-defined as where K , R , and S are the reflection, scattering coefficient, and absorption, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…The curve shape of CL 0.9 AB: x Sm 3+ was comparable to that of the host due to weak f–f transitions of Sm 3+ ions, while the bands in the range of 272–380 nm were observed for CL 0.9– x AB:0.1Ce 3+ , x Sm 3+ , ascribed to f–d absorptions of Ce 3+ ions. Generally, the band gap of the host material can be determined with the use of the following relation , where hv is the photon energy, A is the proportionality constant, and E g is the band gap. The values of n = 1/2 and n = 2 indicate the indirect and direct transitions respectively, and the F ( R ∞ ) value represents the Kubelka–Munk function, which is well-defined as where K , R , and S are the reflection, scattering coefficient, and absorption, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…Rare earth bearing oxide crystals are the basic luminescent materials in modern photonics and laser technology because of high emission efficiency, thermal and chemical stability, and different spectroscopic properties that can be tuned by composition [1][2][3][4][5][6][7][8][9]. One of the most interesting effects observed in rare-earth-doped photoluminescence materials is the frequency conversion from near infrared radiation of low photon energy to visible high photon energy radiation or upconversion (UC) [10][11][12][13][14][15][16][17][18][19][20].…”
Section: Introductionmentioning
confidence: 99%
“…Rare earth ion doped luminescent materials have been extensively studied in the fields of anti-counterfeiting, 1 lighting, 2 displays, 3 temperature sensing 4,26–28 and so on. 33–37 Due to the specific electronic structure of rare earth elements, the materials show rich luminescence color and intrinsic temperature dependence, etc . Among different rare earth ions, the Eu 2+ ion exhibits high efficiency, controllability and abundant luminescence characteristics, which have attracted more and more attention.…”
Section: Introductionmentioning
confidence: 99%