First 1-hydroxy-1-imidazole-based ESIPT emitter with an OHO intramolecular hydrogen bond: ESIPT-triggered TICT and speciation in solution

Search for new types of ESIPT-capable molecules is crucial for understanding the factors controlling the ESIPT photoreaction. In this paper, we present combined experimental and theoretical studies of the proton transfer capabilities of [5-(4-fluorophenyl)-1-hydroxy-4-methyl-1 H -imidazol-2-yl](phen...

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Veröffentlicht in:New journal of chemistry 2022-12, Vol.46 (47), p.2284-22817
Hauptverfasser: Shekhovtsov, Nikita A, Ryadun, Alexey A, Plyusnin, Victor F, Nikolaenkova, Elena B, Tikhonov, Alexsei Ya, Bushuev, Mark B
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Zusammenfassung:Search for new types of ESIPT-capable molecules is crucial for understanding the factors controlling the ESIPT photoreaction. In this paper, we present combined experimental and theoretical studies of the proton transfer capabilities of [5-(4-fluorophenyl)-1-hydroxy-4-methyl-1 H -imidazol-2-yl](phenyl)methanone ( HL ) featuring a short intramolecular OHO hydrogen bond (OO 2.57 ) between the proton-donating 1-hydroxy-1 H -imidazole moiety and the proton-accepting benzoyl group as a pre-requisite for the ESIPT process. This compound is the first representative of a new class of ESIPT-capable molecules, 1-hydroxy-1 H -imidazoles with oxygen-containing proton-accepting groups. In solutions, HL can exist in a variety of ESIPT-capable and ESIPT-incapable species. The emissions of HL in non-protic solvents, CH 2 Cl 2 and MeCN, and in the solid state occur with max in a narrow range of 455470 nm. The emission of HL in MeCN is excitation wavelength dependent with a shoulder appearing near 400 nm under high energy excitation. This emission is dominated by the S 1 S 0 transition in the ESIPT-capable ( N -hydroxy) form of HL and is contributed by the luminescence of the ESIPT-incapable forms. In a protic solvent, EtOH, the emission maximum shifts to max = 413 nm. In solutions, the photoluminescence quantum yield (PLQY) of HL is on the order of 0.1%. In contradistinction to solutions, a rigid molecular environment in the solid state prevents the HL molecules from being conformationally converted and the only form of HL to be found in crystals is the ESIPT-capable one, which leads to an excitation wavelength independent emission with an enhanced PLQY of ca. 5%. The ESIPT photoreaction in the ESIPT-capable form of HL proceeds after overcoming a small energy barrier and ends up at an ESIPT-triggered TICT state followed by a non-radiative deactivation through an S 1 /S 0 conical intersection. In MeCN solution, a 2-aroyl-1-hydroxy-1 H -imidazole-based ESIPT emitter exists in a series of forms and shows rather rare excitation wavelength-dependent emission.
ISSN:1144-0546
1369-9261
DOI:10.1039/d2nj04463c