2021
DOI: 10.1039/d0nh00627k
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Switching to the brighter lane: pathways to boost the absorption of lanthanide-doped nanoparticles

Abstract: The use of organic dyes, semiconductors, and plasmonic nanostructures are three of the most promising strategies to make lanthanide-doped nanoparticles brighter by means of increasing their absorption capabilities.

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Cited by 32 publications
(24 citation statements)
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“…Nevertheless, this comes at a cost in the form of low radiative transition probabilities, yielding poor Ln 3+ molar extinction coefficients in the order of 0.1-10 M −1 cm −1 . 85 Although different strategies aimed to improve the absorption (that translates to brightness) of RENPs have been developed, it still represents an important bottleneck for these nanomaterials. 85,86 Generally, RENPs are the result of embedding Ln 3+ within the crystalline structure of a proper dielectric host material which has three main fundamental roles: i) crystal structure asymmetry and crystal field can be used to increase the probability of the 4f-4f transitions; ii) low cutoff phonon energies reduce non-radiative quenching of the excited states, and iii) host matrix serves as a platform where different sensitizers and activators can be combined to achieve specific luminescent features.…”
Section: Renpsmentioning
confidence: 99%
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“…Nevertheless, this comes at a cost in the form of low radiative transition probabilities, yielding poor Ln 3+ molar extinction coefficients in the order of 0.1-10 M −1 cm −1 . 85 Although different strategies aimed to improve the absorption (that translates to brightness) of RENPs have been developed, it still represents an important bottleneck for these nanomaterials. 85,86 Generally, RENPs are the result of embedding Ln 3+ within the crystalline structure of a proper dielectric host material which has three main fundamental roles: i) crystal structure asymmetry and crystal field can be used to increase the probability of the 4f-4f transitions; ii) low cutoff phonon energies reduce non-radiative quenching of the excited states, and iii) host matrix serves as a platform where different sensitizers and activators can be combined to achieve specific luminescent features.…”
Section: Renpsmentioning
confidence: 99%
“…85 Although different strategies aimed to improve the absorption (that translates to brightness) of RENPs have been developed, it still represents an important bottleneck for these nanomaterials. 85,86 Generally, RENPs are the result of embedding Ln 3+ within the crystalline structure of a proper dielectric host material which has three main fundamental roles: i) crystal structure asymmetry and crystal field can be used to increase the probability of the 4f-4f transitions; ii) low cutoff phonon energies reduce non-radiative quenching of the excited states, and iii) host matrix serves as a platform where different sensitizers and activators can be combined to achieve specific luminescent features. [87][88][89] Page 22 of 48 Nanoscale Advances RENPs can be produced by multiple approaches, which can be generally split into syntheses performed in organic solvents, or in aqueous media.…”
Section: Renpsmentioning
confidence: 99%
“…In that regard, the absorption cross‐section of lanthanide sensitizers can be principally enhanced by coupling UCNPs with NIR‐absorbing dyes or quantum dots. Tethered NIR dyes harvest NIR excitation and transfer it to lanthanides via Föster or Dexter energy transfer mechanisms (Figure 6a) [107] . In addition, organic dyes radiatively decay much faster than lanthanide‐doped UCNPs with inherently forbidden optical transitions.…”
Section: Strategies For Enhancing Upconversion Luminescencementioning
confidence: 99%
“…Recently, triplet energy transfer (TET) from the triplet excited state (T 1 ) of NIR dye has been proposed as an ideal strategy to directly and efficiently enhance the UC emissions of Yb 3+ ‐doped UCNCs without the requirement of the complicated core/multishell structure [11] . Nearly 100 % energy transfer efficiency from long‐lived T 1 to Ln 3+ activators can be achieved, [12] which is difficult to realize based on the short‐lived S 1 of organic dyes [13] . Nevertheless, triplet state exciton concentration of NIR dye is usually low due to the forbidden nature of intersystem crossing (ISC) from S 1 to T 1 and the optical absorption transition between the spin‐zero ground state and the spin‐one triplet levels [12, 14] .…”
Section: Introductionmentioning
confidence: 99%