This study addresses the anomalous fluorescence of a rhodanine-based organic dye of interest for nonlinear optical applications. At room temperature, the dye exhibits weak fluorescence, while spectra collected in glassy 2Me-THF at 77 K show a surprising fluorescence intensity increase by several orders of magnitude with respect to room temperature. Moreover, a pronounced dependence of the fluorescence quantum yield on the excitation wavelength is observed, indicating a breakdown of Vavilov's rule, a corollary of Kasha's rule, which states that the fluorescence quantum yield is independent of the excitation energy. Quantum chemical calculations demonstrate the presence of a bright pi pi* excited state that lies very close in energy to a dark n pi* state. The subtle interplay between these two excited states with different natures is responsible for the intriguing spectral behavior of the dye. Specifically, experimental results are rationalized in terms of a population branching between the two excited states, which can be tuned upon varying the temperature or the excitation energy.
Freezing Out Vavilov's Rule: Temperature-Dependent Fluorescence of a Rhodanine Dye / Racchi, O.; Scurti, S.; Liotino, S.; Lanfranchi, A.; Painelli, A.; Comoretto, D.; Došlić, N.; Caretti, D.; Sissa, C.. - In: CHEMPHOTOCHEM. - ISSN 2367-0932. - 10:2(2026). [10.1002/cptc.202500255]
Freezing Out Vavilov's Rule: Temperature-Dependent Fluorescence of a Rhodanine Dye
Racchi O.;Painelli A.;Sissa C.
2026-01-01
Abstract
This study addresses the anomalous fluorescence of a rhodanine-based organic dye of interest for nonlinear optical applications. At room temperature, the dye exhibits weak fluorescence, while spectra collected in glassy 2Me-THF at 77 K show a surprising fluorescence intensity increase by several orders of magnitude with respect to room temperature. Moreover, a pronounced dependence of the fluorescence quantum yield on the excitation wavelength is observed, indicating a breakdown of Vavilov's rule, a corollary of Kasha's rule, which states that the fluorescence quantum yield is independent of the excitation energy. Quantum chemical calculations demonstrate the presence of a bright pi pi* excited state that lies very close in energy to a dark n pi* state. The subtle interplay between these two excited states with different natures is responsible for the intriguing spectral behavior of the dye. Specifically, experimental results are rationalized in terms of a population branching between the two excited states, which can be tuned upon varying the temperature or the excitation energy.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.


