June 30, 2025 to July 4, 2025
Europe/Vienna timezone

Femtosecond timed imaging of rotation and vibration of alkali dimers on the surface of helium nanodroplets

Jul 4, 2025, 3:20 PM
20m
Hot Topic Femtosecond and attosecond physics, reaction dynamics, coherent control, strong fields Ultrafast 4

Speaker

Henrik Høj Kristensen (Department of Chemistry, Aarhus University)

Description

Alkali dimers, Ak$_2$, residing on the surface of helium nanodroplets, are set into rotation and vibration, through the dynamic Stark effect, by a moderately intense 50-fs pump pulse. Coulomb explosion of dimers in the singlet X $^1\Sigma_g^+$ and triplet a $^3\Sigma_u^+$ state [1, 2], induced by an intense, delayed femtosecond probe pulse, is used to record the time-dependent nuclear motion.

Concerning rotation, the measured alignment traces for Na$_2$, K$_2$, and Rb$_2$ show distinct periodic features that differs qualitatively from the well-known alignment dynamics of linear molecules in either the gas phase or dissolved in liquid helium [3]. Instead, the observed alignment dynamics of Na$_2$ and K$_2$ in the a $^3\Sigma_u^+$ state and of K$_2$ and Rb$_2$ in the X $^1\Sigma_g^+$ state agree with that obtained from a 2D rigid rotor model, strongly indicating that the rotation of each dimer occurs in a plane - defined by the He droplet surface [4, 5].

Concerning vibration, the Coulomb explosion probe method enables us to measure the distribution of internuclear distances as a function of time. For K$_2$ in the a $^3\Sigma_u^+$ state, we observe a distinct oscillatory pattern caused by a two-state vibrational wave packet in the initial electronic state of the dimer. The wave packet is imaged for more than 250 vibrational periods with a precision better than 0.1 Å on its central position. Unlike the rotational motion, the vibration of the dimer is essentially unaffected by the presence of the He droplet [6].

References:
[1] H. H. Kristensen, et al. Phys. Rev. Lett. 128 (2022), 093201
[2] H. H. Kristensen, et al. Phys. Rev. A 107 (2023), 023104
[3] A. S. Chatterley, et al. Phys. Rev. Lett. 125 (2020), 013001
[4] L. Kranabetter, et al. Phys. Rev. Lett. 131 (2023), 053201
[5] H. H. Kristensen, et al., In preparation. (Available at arXiv:2502.14521 [physics.atm-clus])
[6] N. K. Jyde, et al. J. Chem. Phys. 161 (2024), 224301

Authors

Henrik Høj Kristensen (Department of Chemistry, Aarhus University) Lorenz Kranabetter (Department of Chemistry, Aarhus University) Areg Ghazaryan (Institute of Science and Technology Austria) Nicolaj Jyde (Department of Chemistry, Aarhus University) Jeppe Christensen (Department of Chemistry, Aarhus University) Emil Hansen (Department of Physics, Aarhus University) Constant Schouder (ISMO, CNRS, Université Paris-Saclay) Frank Jensen (Department of Chemistry, Aarhus University) Robert Zillich (Institute for Theoretical Physics, Johannes Kepler Universität) Mikhail Lemeshko (Institute of Science and Technology Austria) Henrik Stapelfeldt (Department of Chemistry, Aarhus University)

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