Abstract

Ab initio computation of two-dimensional electronic spectra is an expanding field, whose goal is improving upon simple, few-dimensional models often employed to explain experiments. Here, we propose an accurate and computationally affordable approach, based on the single-trajectory semiclassical thawed Gaussian approximation, to evaluate two-dimensional electronic spectra. Importantly, the method is exact for arbitrary harmonic potentials with mode displacement, changes in the mode frequencies, and inter-mode coupling (Duschinsky effect), but can also account partially for the anharmonicity of the involved potential energy surfaces. We test its accuracy on a set of model Morse potentials and use it to study anharmonicity and Duschinsky effects on the linear and two-dimensional electronic spectra of phenol. We find that in this molecule, the anharmonicity effects are weak, whereas the Duschinsky rotation and the changes in the mode frequencies must be included in accurate simulations. In contrast, the widely used displaced harmonic oscillator model captures only the basic physics of the problem but fails to reproduce the correct vibronic lineshape.

Highlights

  • Electronic spectroscopy allows us to study excited electronic states and light-induced nuclear dynamics

  • A swarm of trajectories could be used in Kubo-type calculations, where each trajectory is equipped with a phase, obtained from the time integral of the energy gap between the involved electronic states along the trajectory, and the correlation functions are averaged over the full ensemble;[5,6,7,8,9,10] these approaches are known as phase averaging,[11] Wigner-averaged classical limit,[12,13,14] or dephasing representation.[15,16,17]

  • The thawed Gaussian approximation, suffers from another form of error: as in linear spectroscopy, artificial negative peaks may appear in the two-dimensional spectra, which is most obvious in the nonrephasing spectrum of Fig. 2 around (ω1, ω3) ≈ (−1, −1)

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Summary

INTRODUCTION

Electronic spectroscopy allows us to study excited electronic states and light-induced nuclear dynamics. The approach is limited to modeling the molecule as a set of few uncoupled displaced harmonic oscillators (DHOs) Such a simple description is inadequate in systems that exhibit strong mode–mode coupling, changes in the force constants between the ground and excited electronic states, or anharmonicity effects. We analyze the effects of Duschinsky coupling and anharmonicity on the linear absorption and two-dimensional spectra of phenol

Third-order response function
Zero-temperature limit
Thawed Gaussian approximation
Two-dimensional electronic spectroscopy
One-dimensional models
On-the-fly ab initio calculations
Harmonic-Morse system
Morse–Morse system
CONCLUSIONS AND OUTLOOK
Full Text
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