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Precision Spectroscopy of the Fine Structure in the $\boldsymbol{a\;{}^3Σ_u^+(v=0)}$ and $\boldsymbol{c\;{}^3Σ_g^+(v=4)}$ States of the Helium Dimer (2508.08060v1)

Published 11 Aug 2025 in physics.atom-ph and physics.chem-ph

Abstract: With four electrons, He$_2$ is one of very few molecules for which first-principles quantum-chemical calculations that include the treatment of nonadiabatic, relativistic and quantum-electrodynamics corrections are possible. Precise spectroscopic measurements are needed as references to test these calculations. We report here on a spectroscopic measurement of the $c$ $3\Sigma_g+\leftarrow a$ $3\Sigma_u+$ electronic transition of $4$He$_2$ at a precision ($\Delta \nu/\nu$) of $2.5\times 10{-10}$ and with full resolution of the rotational, spin-spin and spin-rotational fine structures. The investigation focuses on transitions to the rotational levels of the $c$ $3\Sigma_g+(v=4)$ state, located energetically above the He$(1$ $1S_0) + $He$(2$ $3S_1)$ dissociation limit and decaying by tunneling predissociation through a barrier in the $c$ state. The new data include a full map of the energy levels of the $a$ $3\Sigma_u+(v=0)$ and $c$ $3\Sigma_g+(v=4)$ states with rotational quantum numbers $N$ up to 9 and 10, respectively, and full sets of fine-structure intervals in these levels for comparison with first-principles calculations from a parallel investigation [B. R\'acsai, P. Jeszenszki, A. Marg\'ocsy and E. Maty\'us, arXiv:2506.23879v1 (2025)]. The new data were combined with data from earlier measurements of the spectrum of the $c-a$ band system of $4$He$_2$ to derive full sets of molecular constants for the $a$ $3\Sigma_u+(v=0)$ and $c$ $3\Sigma_g+(v=4)$ states with much improved precision over previous experimental results. A pronounced broadening of the linewidths of the transitions to the $c$ $3\Sigma_g+(v=4,N=10)$ fine-structure levels is attributed to tunneling predissociation through a barrier in the potential of the $c$ state and is quantitatively accounted for by calculations of the predissociation widths.

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