2018
DOI: 10.1111/php.12980
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Photophysical and Photoacoustic Properties of π‐Extended Curcumin Dyes. Effects of the Terminal Dimethylamino Electron‐donor and the Bridging Aryl Ring

Abstract: The synthesis, photophysical and photoacoustic characterization for a series of nine π-extended quadrupolar curcumin dyes is presented. A systematic evaluation of the π-bridging unit including the p-phenyl, naphth-4-yl, thien-2-yl and hybrid 4-naphthathien-2-yl groups is presented. Furthermore, evaluation of the strongly donating donor-π-acceptor-π-donor quadrupolar dimethylamino terminated derivatives is also included. Select dyes exhibit excited state absorption at increased laser fluence which translates to… Show more

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Cited by 7 publications
(4 citation statements)
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“…The UV–vis absorption spectrum of curcumin has a band centered at 466 nm, corresponding to the charge‐transfer involved in the lowest energy transition of quadrupolar donor‐ π ‐acceptor‐ π ‐donor curcuminoids (Figure 1D). [ 30 ] In comparison, the absorption spectrum of CCM‐CPDs displays a band at 285 nm with a broad shoulder at 320−360 nm, attributed to π → π * (conjugated C═C) and n → π * (C═O) transitions, respectively, further revealing the presence of oxygen‐rich functional groups in the CCM‐CPDs. [ 31 ] The CCM‐CPDs, upon excitation at 365 nm, exhibit a fluorescence spectrum with a maximum emission at 450 nm (Figure 1E).…”
Section: Resultsmentioning
confidence: 99%
“…The UV–vis absorption spectrum of curcumin has a band centered at 466 nm, corresponding to the charge‐transfer involved in the lowest energy transition of quadrupolar donor‐ π ‐acceptor‐ π ‐donor curcuminoids (Figure 1D). [ 30 ] In comparison, the absorption spectrum of CCM‐CPDs displays a band at 285 nm with a broad shoulder at 320−360 nm, attributed to π → π * (conjugated C═C) and n → π * (C═O) transitions, respectively, further revealing the presence of oxygen‐rich functional groups in the CCM‐CPDs. [ 31 ] The CCM‐CPDs, upon excitation at 365 nm, exhibit a fluorescence spectrum with a maximum emission at 450 nm (Figure 1E).…”
Section: Resultsmentioning
confidence: 99%
“…20 However, further excitation depends non-linearly on (high) laser fluence; and within biologically-allowed energy limits, RSAs are outperformed by ordinary PA emitters that simply absorb light more strongly. 29,30 We also argue that cycling RSAs between S1/Sn states may cause photoreactive damage to the chromophore or to biological tissues.…”
Section: Introductionmentioning
confidence: 88%
“…Biologically allowed energy limits dictate such low fluence in deep tissue that in practice, RSAs are outperformed by ordinary PA emitters that simply absorb light more strongly. [33,34] We also argue that cycling RSAs between S 1 /S n states may cause photoreactive damage to the chromophore or to biological tissues.…”
Section: Introductionmentioning
confidence: 89%