V. Wirth | Searcharxiv

arXiv2025

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

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.

physics.atom-ph↗

arXiv2025

Characterization of the electronic ground state of He$_2^+$ by high-resolution photoelectron spectroscopy

Excluding the very shallow potential minimum of the electronic ground state, all bound electronic states of He$_2$ have Rydberg character. Their potential-energy functions are similar to those of the He$_2^+$ states to which the Rydberg series converge. Photoionization and electron-impact ionization of the metastable $a~^3\Sigma_u^+$ state of He$_2$ are thus characterized by diagonal Franck-Condon factors and only provide access to low vibrational levels of the He$_2^+$ $X^+$ $^2\Sigma_u^+$ electronic ground state. For this reason, little experimental information is available on the excited vibrational levels of He$_2^+$. We report a measurement, by high-resolution photoelectron spectroscopy, of 17 vibrational levels of the $X^+$ $^2\Sigma_u^+$ state of $^4$He$_2^+$, with vibrational quantum number $v^+$ from 3 to 19 and covering more than 95% of the potential well. To access these states, we exploit a hump in the potential-energy function of the $c~^3\Sigma_g^+$ state, whose vibrational wavefunctions extend to large internuclear distance by quantum-mechanical tunneling through the potential barrier. Combining these results with data on the lowest ($v^+=0-2$) and highest ($v^+=22, 23$) vibrational levels of $^4$He$_2^+$, we derive a full map of the rovibrational structure of He$_2^+$ and, in a least-squares fit, an empirical effective potential-energy function that describes all experimental data within uncertainties. This function yields the positions of the 409 bound rovibrational levels and the positions and widths of the 74 shape resonances of the $X^+$ $^2\Sigma_u^+$ state of $^4$He$_2^+$. The dissociation energy of He$_2^+$ is $D{\rm e}=19,956.10(10)$ cm$^{-1}$ [$D_0(^4{\rm He}_2^+)=19,101.29(10)$ cm$^{-1}$].

physics.atom-ph↗