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 |
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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. |
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ISSN: | 1144-0546 1369-9261 |
DOI: | 10.1039/d2nj04463c |