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Home > Press > Detecting vibrational quantum beating in the predissociation dynamics of SF6 using time-resolved photoelectron spectroscopy

Figure 1: Schematic of SF6 predissociation dynamics and time-resolved photoelectron spectroscopy.

Credit
Ultrafast Science
Figure 1: Schematic of SF6 predissociation dynamics and time-resolved photoelectron spectroscopy. Credit Ultrafast Science

Abstract:
Quantum coherence is a fundamental mechanism driving ultrafast molecular reaction dynamics, playing a decisive role in processes such as light-induced ultrafast vision molecular isomerization and dissociation. However, due to the complexity of highly excited states in polyatomic molecules and interference from decoherence processes, directly observing vibrational quantum coherence signals from excited states has long been a major experimental challenge. This study, using time-resolved photoelectron spectroscopy, clearly resolves quantum beat signals resulting from interference between different vibrational states during the ultrafast predissociation dynamics of excited SF6 molecules. By combining high-precision calculations of the excited state potential energy surface and quantum dynamics simulations, the vibrational levels involved in the quantum coherence process are identified, and the lifetimes of the predissociating vibrational states are quantitatively analyzed. This work opens new avenues for understanding the role of quantum coherence in complex photo-induced ultrafast chemical reactions and ultimately for achieving active control over them.

Detecting vibrational quantum beating in the predissociation dynamics of SF6 using time-resolved photoelectron spectroscopy

Washington, DC | Posted on April 17th, 2026

As shown in Figure 1, the experiment employs an extreme ultraviolet (XUV) pump-ultraviolet (UV) probe scheme: an XUV pulse (14.1 eV) resonantly excitesSF6 molecules from the neutral ground state to a predissociative state. Subsequently, a time-delayed UV pulse (3.1 eV) ionizes the excited molecules to the ground state of the cation, and the kinetic energy of the emitted photoelectrons is recorded. The potential energy curves in Figure 1a show non-adiabatic coupling between the excited state and dissociative states, leading to predissociation of the nuclear wave packet, which causes a decay in photoelectron spectroscopy intensity as a function of pump-probe delay. In Figures 1b and 1c, a series of vibrational peaks spaced by approximately 0.1 eV appear in the high kinetic energy region, corresponding to ionization to different vibrational levels of the cationic ground state.

Figure 2 focuses on the structure of the main photoelectron spectroscopy peak, revealing the vibrational quantum beating. Figure 2a shows the experimentally measured photoelectron spectroscopy intensity as a function of delay time, exhibiting clear oscillatory behavior within approximately 300 fs (Figure 2b). By analyzing this oscillatory feature, the research team determined a period of 318 fs, corresponding to a vibrational energy level difference of 0.013 eV. This quantum beat signal demonstrates that multiple vibrational levels are coherently excited and their interference persists during the predissociation process. The figure also shows a slight blue shift of the peak position with increasing delay time, indicating differences in the lifetimes of the vibrational levels, providing a crucial clue for subsequent analysis. To identify the specific vibrational levels involved, based on ab initio calculations, the research term identified that the pump pulse resonantly excites three closely spaced vibrational eigenstates, where the energy difference between the two higher levels matches the experimentally observed beat period. The lifetimes of the three vibrational states obtained from wave packet dynamics simulations align with the decay trends extracted from the experiment.

This study, using time-resolved photoelectron spectroscopy, reports the first observation of vibrational quantum beating in the highly excited state predissociation of a polyatomic molecule, SF6, and identifies the participating vibrational levels and their lifetimes. This finding not only reveals the influence of the highly excited state potential energy surface structure on quantum coherence but also provides a new perspective for studying photochemical processes in complex molecular systems. In the future, combining this approach with broader bandwidth attosecond pump pulses holds promise for actively controlling electronic coherence motion, advancing the field of attochemistry.

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Contacts:
Pan Zhao
Ultrafast Science


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