Fig. 5: Cavity potential energy surface of photoisomerization reaction. | Communications Chemistry

Fig. 5: Cavity potential energy surface of photoisomerization reaction.

From: Unveiling the role of dark states in dynamic control of azopyrrole photoisomerization by light-matter interaction

Fig. 5

Represent modified polaritonic surfaces for {g/ωR = a) 0.0543, b) 0.1086, c) 0.1257} that result in the experimentally observed Rabi splitting ranging from weak (a; 1 w% azopyrrole; at equilibrium), over strong (b; 1 w% azopyrrole), to ultra-strong (c; 1.5w% azopyrrole) for a frequency of the cavity mode chosen to be in resonance with the theoretically predicted absorption energy S0 to S1 of 427 nm. df Transition-state barriers for different reaction paths on the S1 (lower polariton) surface of the combined system with the absorption spectrum of the bare system as a gray line in the background. Higher transparency of a data point corresponds to a smaller matter contribution, i.e., a higher photonic fraction of the polariton.

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