Abstract

Hypericin has large potential in modern medicine and exhibits fascinating structural dynamics, such as multiple conformations and tautomerization. However, it is difficult to study individual conformers/tautomers, as they cannot be isolated due to the similarity of their chemical and physical properties. An approach to overcome this difficulty is to combine single molecule experiments with theoretical studies. Time‐dependent density functional theory (TD‐DFT) calculations reveal that tautomerization of hypericin occurs via a two‐step proton transfer with an energy barrier of 1.63 eV, whereas a direct single‐step pathway has a large activation energy barrier of 2.42 eV. Tautomerization in hypericin is accompanied by reorientation of the transition dipole moment, which can be directly observed by fluorescence intensity fluctuations. Quantitative tautomerization residence times can be obtained from the autocorrelation of the temporal emission behavior revealing that hypericin stays in the same tautomeric state for several seconds, which can be influenced by the embedding matrix. Furthermore, replacing hydrogen with deuterium further proves that the underlying process is based on tunneling of a proton. In addition, the tautomerization rate can be influenced by a λ/2 Fabry–Pérot microcavity, where the occupation of Raman active vibrations can alter the tunneling rate.

Highlights

  • Hypericin has large potential in modern medicine and exhibits fascinating its tautomeric state,[3,4,5] which is crucial for, e.g., drug design.[6]

  • We present a comprehensive investigation of the structural dynamics present in hypericin

  • Time-dependent density functional theory (TD-DFT) calculations show that the energy barriers for conformational transitions are significantly larger than values obtained by force field (FF) calculations

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Summary

Results and Discussion

The TDM leads, for a fixed electric field orientation, to a change of the excitation rate for each tautomer, resulting in multiple fluorescence intensity levels Such a behavior involving multiple process within the same temporal acquisition yields β2 1⁄4 0.3 and the tautomerization residence time τ2 1⁄4 14.7 s is the average of all involved processes. Tuning the cavity resonance to λc 1⁄4 712 nm corresonds to a Raman shift of %4850 cmÀ1 where the amplification of the Raman modes vanishes due to the large detuning

Conclusion
Experimental Section
Data Availability Statement
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