2015
DOI: 10.1039/c4tc02363c
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Intense multiphoton upconversion of Yb3+–Tm3+ doped β-NaYF4 individual nanocrystals by saturation excitation

Abstract: We report the intense multiphoton upconversion of β-NaYF4: Yb3+–Tm3+ individual nanocrystals benefiting from the perfect ladder-type electron configuration under saturation excitation.

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Cited by 59 publications
(35 citation statements)
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“…Because of the unique features of Pr 3+ ions, there are several different broad UCPL bands corresponding to Pr 3+ ions transitions . Especially, the UCPL peaks in blue (475 nm), green (523, 540, and 552 nm), and red (654 nm) are trichromatic elements of white light, due to 3 P 0 → 3 H 4 , 1 I 6 → 3 H 5 , 3 P 1 → 3 H 5 , 3 P 0 → 3 H 5 , 3 P 1 → 3 F 3 transitions of Pr 3+ ions (Figure ). Optimization of the sintering condition by monitoring the UCPL spectrum intensity was necessary as we control the sintering time (Figure A) and laser power density.…”
Section: Resultsmentioning
confidence: 99%
“…Because of the unique features of Pr 3+ ions, there are several different broad UCPL bands corresponding to Pr 3+ ions transitions . Especially, the UCPL peaks in blue (475 nm), green (523, 540, and 552 nm), and red (654 nm) are trichromatic elements of white light, due to 3 P 0 → 3 H 4 , 1 I 6 → 3 H 5 , 3 P 1 → 3 H 5 , 3 P 0 → 3 H 5 , 3 P 1 → 3 F 3 transitions of Pr 3+ ions (Figure ). Optimization of the sintering condition by monitoring the UCPL spectrum intensity was necessary as we control the sintering time (Figure A) and laser power density.…”
Section: Resultsmentioning
confidence: 99%
“…So far, most previous works in this field focus mainly on the cooperative multiphoton luminescence in which two or more rare-earth ions are generally involved. In this case, the laser excitation is initially absorbed by a sensitizer ion and subsequently transferred to an acceptor ion that is responsible for the upconversion luminescence [29][30][31][32]34]. In addition, the longest excitation wavelength used for generating the upconversion luminescence is about 1.5 μm.…”
Section: Upconversion Luminescence Under Multiphoton Excitation In Thmentioning
confidence: 98%
“…At high excitation intensities, these intermediate states are effectively populated, leading to the phenomenon of super saturation [27,28]. As a result, the number of simultaneously absorbed photons necessary for the upconversion is reduced and so is the excitation intensity required for upconversion [29][30][31][32][33][34]. In addition, these glasses are easy to be shaped and possess high transparency, low production cost, and good thermal stability.…”
Section: Introductionmentioning
confidence: 96%
“…Due to the saturation effect, the quantum yield would eventually approach a plateau at very high excitation intensities . In any conditions, upconversion luminescence, especially that promoted by a multi‐photon process, prefers high excitation intensity, analogous to the case of coherent nonlinear optical processes that necessitate high laser intensity. In other words, the upconversion system generate upconversion luminescence in a more efficient way at higher excitation intensities.…”
Section: Optical Responses Of Upconversion Systems To External Stimulimentioning
confidence: 99%