2021
DOI: 10.1016/j.jlumin.2020.117676
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Enhancement of blue emission in Ce3+, Eu2+ activated BaSiF6 downconversion phosphor by energy transfer mechanism: A photochromic phosphor

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Cited by 41 publications
(13 citation statements)
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“…The particle sizes were distributed over a submicrometre range that made them advantageous for solid‐state lighting. [ 36 ] The voids and porosity noted in the SEM micrographs may be due to the emission of gas and an inappropriate distribution of temperature, respectively, throughout the synthesis. [ 37,38 ] The anomaly of molecule size was due to the temperature gradient during sintering.…”
Section: Resultsmentioning
confidence: 99%
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“…The particle sizes were distributed over a submicrometre range that made them advantageous for solid‐state lighting. [ 36 ] The voids and porosity noted in the SEM micrographs may be due to the emission of gas and an inappropriate distribution of temperature, respectively, throughout the synthesis. [ 37,38 ] The anomaly of molecule size was due to the temperature gradient during sintering.…”
Section: Resultsmentioning
confidence: 99%
“…As demonstrated in Figure 9, slope log(x) vs log(I/s) was found to be −1.2447 for θ = 3.7341 and indicated that the exchange interaction was the predominant interaction accountable for concentration quenching in the RE emission for YZO:Sm 3+ phosphors. [ 36 ]…”
Section: Resultsmentioning
confidence: 99%
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“…This point where maximum intensity occurred with respect to concentration of ions or exposure rate is called a concentration quenching point and the phenomenon occurring here is known as a concentration quenching phenomenon. [19][20][21] On increasing exposure rate, TL glow curve intensity carries on diminishing after a particular exposure and the sample shows a concentration quenching effect. The different dose rate study shows the maximum intensity of the irradiated phosphor at 456 Gy observed at a peak centered at 200 C as displayed in Figure 6 which is useful in dosimetric properties.…”
Section: The Thermoluminescence Studiesmentioning
confidence: 99%
“…Therefore, there is usually energy transfer from Ce 3+ to Eu 2+ , whether in oxides, nitrides, fluorides, nitrogen oxides, phosphates, borates, silicates, or in most aluminate and aluminosilicate . In these host materials, when Ce 3+ and Eu 2+ are codoped, the Forster resonant energy transfer may perhaps occur, and a necessary condition for the realization of the energy transfer process is the existence of a sufficient spectral overlap between the emission of the donor and the absorption of the acceptor, and a suitable distance between the donor and the acceptor . In the vast majority of materials, the luminescence centers of Ce 3+ ions have higher energy than those of Eu 2+ ions; in other words, the emission spectra of Ce 3+ ions tend to overlap with the excitation spectra of Eu 2+ ions, and thus energy transfer from Ce 3+ to Eu 2+ can often occur.…”
Section: Introductionmentioning
confidence: 99%