Abstract

The rates and outcomes of virtually all photophysical and photochemical processes are determined by conical intersections. These are regions of degeneracy between electronic states on the nuclear landscape of molecules where electrons and nuclei evolve on comparable timescales and thus become strongly coupled, enabling radiationless relaxation channels upon optical excitation. Due to their ultrafast nature and vast complexity, monitoring conical intersections experimentally is an open challenge. We present a simulation study on the ultrafast photorelaxation of uracil, based on a quantum description of the nuclei. We demonstrate an additional window into conical intersections obtained by recording the transient wavepacket coherence during this passage with an X-ray free-electron laser pulse. Two major findings are reported. First, we find that the vibronic coherence at the conical intersection lives for several hundred femtoseconds and can be measured during this entire time. Second, the time-dependent energy-splitting landscape of the participating vibrational and electronic states is directly extracted from Wigner spectrograms of the signal. These offer a physical picture of the quantum conical intersection pathways through visualizing their transient vibronic coherence distributions. The path of a nuclear wavepacket in the vicinity of the conical intersection is directly mapped by the proposed experiment.

Highlights

  • Our study offers a detailed picture of ultrafast nonadiabatic transitions at CoIns

  • Contrary to the common picture of precisely timed CoIn events, the coherence remains visible for several hundred femtoseconds. This is due to the delocalized nature of the quantum nuclear WP in the S2 state after photoexcitation, where small tails consecutively reach the CoIn

  • The coherence that is built decays due to the S1 WP evolving away from the CoIn toward the minimum, but it is constantly rebuilt by other parts arriving at the CoIn in the S2 state

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Summary

Introduction

The position and spread of the coherence in the nuclear phase space are determined by the WPs in S2 and S1. This is independent of whether the coherence is local (e.g., at the CoIn) or spread over a larger region.

Results
Conclusion

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