1997
DOI: 10.1007/bf02290866
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Ensembles of rings with a coumarin unit.

Abstract: We have investigated the luminescent spectral properties of 3- (2-R-thiazol-4-yl)coumarins (R = CH 3, CHeCN, Ar) and some isomeric 3-(4-R-thiazol-2-yl)coumarins (R = Ar) with substituents of different electronic types both in the coumarin and in the aryl moieties. We have obtained estimates of the rate constants for primary photophysical processes: emission of fluorescence and nonradiative degrtdation of the electronic excitation energy. We have calculated the matrix elements for the spin-orbit coupling operat… Show more

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“…The main spectral parameters and the corresponding values of photodecomposition quantum yields, Φ ph , are shown in Figures – and Table . The steady-state linear one-photon absorption (1PA) spectra of 1 and 2 (Figure , curves 1, 2) revealed relatively weak long wavelength absorption bands at ∼380–395 nm (maximum extinction coefficient, ε max ≈ (24–28) × 10 3 M –1 cm –1 ), with nearly structureless absorption contours and no substantial dependence on solvent polarity, which is typical for 3-thiazolylcoumarins in liquid medium at room temperature. ,, These 1PA bands can be attributed to a single π → π* electronic transition S 0 → S 1 in accordance with nearly constant values of excitation anisotropy r 0 (λ) (see Figure a,b, curves 1) over the spectral range λ ≥ 330–350 nm. These values of r 0 (λ) ≈ 0.3–0.35 are close to the theoretical limit and related to the comparatively small angle between the absorption and emission transition dipoles for S 0 → S 1 and S 1 → S 0 electronic transitions, respectively.…”
Section: Resultsmentioning
confidence: 98%
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“…The main spectral parameters and the corresponding values of photodecomposition quantum yields, Φ ph , are shown in Figures – and Table . The steady-state linear one-photon absorption (1PA) spectra of 1 and 2 (Figure , curves 1, 2) revealed relatively weak long wavelength absorption bands at ∼380–395 nm (maximum extinction coefficient, ε max ≈ (24–28) × 10 3 M –1 cm –1 ), with nearly structureless absorption contours and no substantial dependence on solvent polarity, which is typical for 3-thiazolylcoumarins in liquid medium at room temperature. ,, These 1PA bands can be attributed to a single π → π* electronic transition S 0 → S 1 in accordance with nearly constant values of excitation anisotropy r 0 (λ) (see Figure a,b, curves 1) over the spectral range λ ≥ 330–350 nm. These values of r 0 (λ) ≈ 0.3–0.35 are close to the theoretical limit and related to the comparatively small angle between the absorption and emission transition dipoles for S 0 → S 1 and S 1 → S 0 electronic transitions, respectively.…”
Section: Resultsmentioning
confidence: 98%
“…The development and investigation of different types of coumarin derivatives remain subjects of continuing interest for a number of important research areas, including organic electronics, , nonlinear optics, and lasing, 3D microfabrication and optical data storage, sensing technologies, biomedical probes and reactants, and one- and two-photon photodynamic therapy (PDT). , Coumarin derivatives exhibit a large variety of linear steady-state and time-resolved photophysical properties, which depend on the specific substituents in different positions of the molecular architecture ,,,,, and solute–solvent interactions. ,,,,, These characteristics afford the ability to tune emission efficiency, , the values of Stokes shifts, binding abilities, , and photochemical stability along with harnessing the fast relaxation processes in the ground and excited electronic states of coumarins for a number of applications. It should be mentioned that notable efforts were made for improving and making practical use of the two-photon absorption (2PA) properties of coumarin derivatives in the microfabrication, biomedicine, fluorescence microscopy, and PDT research fields.…”
Section: Introductionmentioning
confidence: 99%
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