2019
DOI: 10.1016/bs.hpcre.2019.08.001
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Modeling intramolecular energy transfer in lanthanide chelates: A critical review and recent advances

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Cited by 77 publications
(74 citation statements)
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“…The europium ion is well known as a perfect probe for chemical surroundings, owing to its electronic configuration [ 16 , 17 , 18 ]. The luminescence spectra of the Eu complexes studied demonstrate the characteristic transitions of the Eu 3+ ion from the excited state 5 D 0 to the ground state 7 F J ( J = 0–4) as well as from the 5 D 1 state in the complex 9 ( Figure 5 ).…”
Section: Resultsmentioning
confidence: 99%
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“…The europium ion is well known as a perfect probe for chemical surroundings, owing to its electronic configuration [ 16 , 17 , 18 ]. The luminescence spectra of the Eu complexes studied demonstrate the characteristic transitions of the Eu 3+ ion from the excited state 5 D 0 to the ground state 7 F J ( J = 0–4) as well as from the 5 D 1 state in the complex 9 ( Figure 5 ).…”
Section: Resultsmentioning
confidence: 99%
“…As a result of such charge redistribution, ILCT state appears and participates in the sensitization of Ln 3+ ion luminescence. It should be noted also that in the case of Eu complexes, owing to the low redox potential of this ion, the ligand to metal charge transfer (LMCT) state may have low energy and cause the luminescence quenching [ 17 , 18 ]. Therefore, the energies of S 1 and T states are very important for the optimization of intraligand energy transfer, but charge transfer states can also have a dramatic influence on the efficiency of this transfer.…”
Section: Resultsmentioning
confidence: 99%
“…To rationalize these thermal dependences, we use time-dependent density functional theory and intramolecular energy transfer calculations (details in Supporting Information). The intramolecular energy transfer rates for Ln 3+ complexes were estimated based on a well-defined theory. …”
mentioning
confidence: 99%
“…In lanthanide spectroscopy, the electric dipole transitions between 2 S +1 L J and 2 S ′+1 L J ′ ′ states (| SLJ ⟩ → | S ′ L ′ J ′⟩) have to obey the selection rule on the J quantum number, | J – J ′| ≤ λ ≤ J + J ′ (with λ = 2, 4, and 6), for nonzero S ′ L ′ J ′ U (λ) SLJ matrix elements. , In this sense, the Eu 3+ ion has unique properties, especially regarding its emission spectrum where it is possible to directly obtain the Judd–Ofelt intensity parameters Ω λ (λ = 2, 4, and 6) in terms of the integrated areas under the emission curves . This is feasible due to the employment of the 5 D 0 → 7 F 1 emission as an internal reference.…”
Section: Conclusion On the Performances Of The Dlwgsmentioning
confidence: 99%
“…The radiative rate A 0→1 contribution of the 5 D 0 → 7 F 1 transition (in units of s –1 ) can be calculated as , where n is the refractive index which depends upon the wavelength λ and ν̃ is the wavenumber corresponding to the barycenter of the 5 D 0 → 7 F 1 transition.…”
Section: Conclusion On the Performances Of The Dlwgsmentioning
confidence: 99%