Abstract

Coherent two-dimensional spectroscopy is a powerful tool for probing ultrafast quantum dynamics in complex systems. Several variants offer different types of information but typically require distinct beam geometries. Here we introduce population-based three-dimensional (3D) electronic spectroscopy and demonstrate the extraction of all fourth- and multiple sixth-order nonlinear signal contributions by employing 125-fold (1⨯5⨯5⨯5) phase cycling of a four-pulse sequence. Utilizing fluorescence detection and shot-to-shot pulse shaping in single-beam geometry, we obtain various 3D spectra of the dianion of TIPS-tetraazapentacene, a fluorophore with limited stability at ambient conditions. From this, we recover previously unknown characteristics of its electronic two-photon state. Rephasing and nonrephasing sixth-order contributions are measured without additional phasing that hampered previous attempts using noncollinear geometries. We systematically resolve all nonlinear signals from the same dataset that can be acquired in 8 min. The approach is generalizable to other incoherent observables such as external photoelectrons, photocurrents, or photoions.

Highlights

  • Coherent two-dimensional spectroscopy is a powerful tool for probing ultrafast quantum dynamics in complex systems

  • The great versatility of multidimensional techniques results from their ability to distinguish between specific nonlinear signal contributions

  • Such an approach should offer direct comparability between different signal contributions that is beneficial for interpretation purposes, especially because nonlinear signals show a strong dependence on the employed excitation conditions that might not be identical throughout separate measurements

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Summary

Introduction

Coherent two-dimensional spectroscopy is a powerful tool for probing ultrafast quantum dynamics in complex systems. As further shown in Supplementary Note 5 and Supplementary Fig. 7 and discussed in a similar scenario[61], the filtering effect by the laser spectrum removes from the complete manifold a number of pathways that involve the transition between |e0〉 and |g1〉, in the nonrephasing 1Q–0Q–1Q contribution.

Results
Conclusion

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