2018
DOI: 10.1364/oe.26.023471
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Concentration dependent optical transition probabilities in ultra-small upconversion nanocrystals

Abstract: Transition probability is of vital importance for luminescence process, whereas the effects of doping concentration have not been explored in the Er:NaGdF. In this work, we investigate the radiative transition probabilities of Er highly doped NaGdF sub 10 nm nanocrystals using J-O theory. It is found that the transition probabilities vary with changing Er concentration, especially altering the ratio of ErH to S level, which is highly useful for optical thermometers as they are thermally coupled. To validate th… Show more

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Cited by 18 publications
(4 citation statements)
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“…Also, the measured lifetimes are obviously smaller than expected. On the basis of the J-O calculation of 80 mol.% Er 3+ doped NaGdF4, which is similar to NaErF4, transition probabilities of Er 3+ fall within 10 1~1 0 3 s -1 ( 4 S3/2:240 s -1 , 4 F9/2:640 s -1 , and 4 I9/2:70 s -1 ) [20].…”
Section: Anomalous Variation Of Lifetime Versus Temperaturementioning
confidence: 85%
“…Also, the measured lifetimes are obviously smaller than expected. On the basis of the J-O calculation of 80 mol.% Er 3+ doped NaGdF4, which is similar to NaErF4, transition probabilities of Er 3+ fall within 10 1~1 0 3 s -1 ( 4 S3/2:240 s -1 , 4 F9/2:640 s -1 , and 4 I9/2:70 s -1 ) [20].…”
Section: Anomalous Variation Of Lifetime Versus Temperaturementioning
confidence: 85%
“…In addition, as evidence for Er 3+ strong cross-relaxation, the intensity ratios of red against green emission (I 652 /I 538 ) should gradually increase with the increase of Er 3+ cross-relaxation, [45] even I 652 >I 538 . [46] However, for Er 3+ X ∕Yb 3+ 0.9−X :CsPbCl 3 , intensity ratios of I 652 /I 538 changed slowly from maximum value of 0.51 at 0.2 m Er 3+ to minimum value of 0.46 at 0.8 m Er 3+ , indicating that no severe cross relaxation occurred. No UCL was observed in Er 3+ singly doped perovskite, suggesting the presence of Yb 3+ excitation is essential for UCL, which resulted from the energy transfer from Yb 3+ to Er 3+ .…”
Section: Resultsmentioning
confidence: 93%
“…This can be mainly attributed to the combination of radiative and nonradiative decay behaviors. From one hand, the radiative transition rates of Er 3+ green (10 3 s −1 for 4 S 3/2 / 2 H 11/2 ) and red (10 2 s −1 for 4 F 9/2 ) emissions vary considerably [ 48 ], which partially contributes to the difference of green and red UCL decay-times. From another hand, nonradiative decay from upper state ( 4 F 7/2 ) to green states ( 4 S 3/2 / 2 H 11/2 ) is extremely fast, while the nonradiative decay that feeds the red state ( 4 S 3/2 → 4 F 9/2 ) is relatively slow, also leading to the prolonged decay-time of red UCL.…”
Section: Resultsmentioning
confidence: 99%