Publication | Closed Access
Varying the Interpentacene Electronic Coupling to Tune Singlet Fission
89
Citations
54
References
2019
Year
We have designed and used four different spacers, denoted A-D, to connect two pentacenes and to probe the impact of intramolecular forces on the modulation of pentacene-pentacene interactions and, in turn, on the key steps in singlet fission (SF), that is, the <sup>1</sup>(S<sub>1</sub>S<sub>0</sub>)-to-<sup>1</sup>(T<sub>1</sub>T<sub>1</sub>) as well as <sup>1</sup>(T<sub>1</sub>T<sub>1</sub>)-to-<sup>5</sup>(T<sub>1</sub>T<sub>1</sub>) transitions by means of transient absorption and electron paramagnetic resonance measurements. In terms of the <sup>1</sup>(S<sub>1</sub>S<sub>0</sub>)-to-<sup>1</sup>(T<sub>1</sub>T<sub>1</sub>) transition, a superexchange mechanism, that is, coupling to a higher-lying CT state to generate a virtual intermediate, enables rapid SF in A-D. Sizeable electronic coupling in A and B opens, on one hand, an additional pathway, that is, the population of a real intermediate, and changes, on the other hand, the mechanism to that of hopping. In turn, A and B feature much higher <sup>1</sup>(T<sub>1</sub>T<sub>1</sub>) quantum yields than C and D, with a maximum value of 162% for A. In terms of the <sup>1</sup>(T<sub>1</sub>T<sub>1</sub>)-to-<sup>5</sup>(T<sub>1</sub>T<sub>1</sub>) transition, the sizable electronic coupling in A and B is counterproductive, and C and D give rise to higher <sup>5</sup>(T<sub>1</sub>T<sub>1</sub>)-to-(T<sub>1</sub> + T<sub>1</sub>) quantum yields than A and B, with a maximum value of 85% for D.
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