2016
DOI: 10.1016/j.optmat.2015.11.004
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The 1.53μm spectroscopic properties of Er3+/Ce3+/Yb3+ tri-doped tellurite glasses containing silver nanoparticles

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Cited by 35 publications
(9 citation statements)
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“…In order to achieve bright NIR-IIb emission, suppression of upconversion emission is important, which can be achieved through reducing the electron numbers in the 4 I 11/2 state and correspondingly enhancing the population of the 4 I 13/2 level. 40 The energy difference of the two energy levels of 2 F 7/2 and 2 F 5/2 of Ce 3+ ions is 2300 cm −1 , which is approximated to the energy spacing between 4 I 11/2 and 4 I 13/2 of Er 3+ ions (3700 cm −1 ). Based on this, the cross relaxation between Ce 3+ ( 2 F 7/2 → 2 F 5/2 ) and Er 3+ ( 4 I 11/2 → 4 I 13/2 ) takes place, leading to the transition of electrons from the 4 I 11/2 to 4 I 13/2 level by nonradiative decay.…”
Section: Resultsmentioning
confidence: 98%
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“…In order to achieve bright NIR-IIb emission, suppression of upconversion emission is important, which can be achieved through reducing the electron numbers in the 4 I 11/2 state and correspondingly enhancing the population of the 4 I 13/2 level. 40 The energy difference of the two energy levels of 2 F 7/2 and 2 F 5/2 of Ce 3+ ions is 2300 cm −1 , which is approximated to the energy spacing between 4 I 11/2 and 4 I 13/2 of Er 3+ ions (3700 cm −1 ). Based on this, the cross relaxation between Ce 3+ ( 2 F 7/2 → 2 F 5/2 ) and Er 3+ ( 4 I 11/2 → 4 I 13/2 ) takes place, leading to the transition of electrons from the 4 I 11/2 to 4 I 13/2 level by nonradiative decay.…”
Section: Resultsmentioning
confidence: 98%
“…Nonetheless, the downshifting emission process is competitive with the upconversion emission process, since they are highly dependent on the intermediate 4 I 11/2 state of Er 3+ . In order to achieve bright NIR-IIb emission, suppression of upconversion emission is important, which can be achieved through reducing the electron numbers in the 4 I 11/2 state and correspondingly enhancing the population of the 4 I 13/2 level . The energy difference of the two energy levels of 2 F 7/2 and 2 F 5/2 of Ce 3+ ions is 2300 cm –1 , which is approximated to the energy spacing between 4 I 11/2 and 4 I 13/2 of Er 3+ ions (3700 cm –1 ).…”
Section: Resultsmentioning
confidence: 99%
“…The downshifted 1525 nm emission was mainly attributed to nonradiative decay from the 4 I 11/2 to the 4 I 13/2 level (Figure i). A Ce-doping strategy was adopted to facilitate the downshifting process of the Er ion through enhancing the nonradiative decay of Er 3+ ( 4 I 11/2 → 4 I 13/2 ) by using the cross-relaxation between Er and Ce ions. ,, All of these characteristics have ensured a bright NIR-IIb emission for further biomedical applications. After the core was coated with an inert shell, the NIR-IIb emission was significantly enhanced by ∼2 times due to the decreased surface quenching effect (Figure j).…”
Section: Results and Discussionmentioning
confidence: 99%
“…It is noted that both the downshifting and UC emitting processes are all highly related to the intermediate 4 I 11/2 state of Er 3+ , presenting a competitive emission process. Therefore, to achieve highly efficient NIR-IIb emission, a suppressed UC emission by decreasing the population of the 4 I 11/2 state and simultaneously increasing the electron numbers in the 4 I 13/2 level are demanded. , Fortunately, the energy level difference between the 2 F 5/2 and the 2 F 7/2 state of Ce 3+ is about 2300 cm –1 , which is approximated to the energy level spacing of 4 I 11/2 and 4 I 13/2 (about 3700 cm –1 ) of Er 3+ , enabling phonon-mediated nonradiative decay from the 4 I 11/2 to the 4 I 13/2 level of Er 3+ via the efficient cross relaxation (CR, Figure c) between Er 3+ ( 4 I 11/2 → 4 I 13/2 ) and Ce 3+ ( 2 F 7/2 → 2 F 5/2 ). Moreover, Dai’s group proposed a Ce 3+ doping strategy to boost the 1525 emission in NaYbF 4 -based core/shell nanoparticles for high temporal resolution brain vessel imaging.…”
Section: Resultsmentioning
confidence: 99%