Intramolecular Polarization Induces Electron–Hole Charge Separation in Light-Harvesting Molecular Triads

Abstract

Artificial light-harvesting supramolecular structures reproduce the light-to-electrochemical energy transduction mechanisms observed in natural photosynthesis. Among them the prototypical carotenoid­(C)–porphyrin­(P)–fullerene­(C<sub>60</sub>) type of structures have been the most studied. Several experiments performed in such structures, and others alike, have shown that the photoexcited state <i>C</i>– <sup>1</sup><i>P</i>–<i>C</i><sub>60</sub> decays to the metastable charge-separated state <i>C</i>– <i>P</i><sup>•+</sup> −<i>C</i><sub>60</sub><sup>•–</sup> within a few picoseconds, whereas the final charge-separated state, <i>C</i><sup>•+</sup>– <i>P</i> −<i>C</i><sub>60</sub><sup>•–</sup>, is obtained within hundreds of picoseconds. This paper introduces a nonlinear polarizable extended Hückel Hamiltonian that describes the charge dynamics and charge-separation effects in such triads by means of quantum dynamics simulations performed on the photoexcited electron–hole pair. The results are interpreted on the basis of the discrete self-trapping equation and enlighten the role played by the polarizability on charge-separation phenomena

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