Molecular helium represents a benchmark system for testing ab initio calculations on few-electron molecules. We report on the determination of the adiabatic ionization energy of the a 3 Σ þ u state of He 2 , corresponding to the energy interval between the a 3 Σ þ u (v 00 ¼ 0, N 00 ¼ 1) state of He 2 and the X þ 2 Σ þ u (v þ ¼ 0, N þ ¼ 1) state of He þ 2 , and of the lowest rotational interval of He þ 2. These measurements rely on the excitation of metastable He 2 molecules to high Rydberg states using frequency-comb-calibrated continuouswave UV radiation in a counterpropagating laser-beam setup. The observed Rydberg states were extrapolated to their series limit using multichannel quantum-defect theory. The ionization energy of He 2 (a 3 Σ þ u) and the lowest rotational interval of He þ 2 (X þ 2 Σ þ u) are 34 301.207 002ð23Þ AE 0.000 037 syst cm −1 and 70.937 589ð23Þ AE 0.000 060 syst cm −1 , respectively.
Multistage Zeeman deceleration was used to generate a slow, dense beam of translationally cold He_{2} molecules in the metastable a ^{3}Σ_{u}^{+} state. Precision measurements of the Rydberg spectrum of these molecules at high values of the principal quantum number n have been carried out. The spin-rotational state selectivity of the Zeeman-deceleration process was exploited to reduce the spectral congestion, minimize residual Doppler shifts, resolve the Rydberg series around n=200 and assign their fine structure. The ionization energy of metastable He_{2} and the lowest rotational interval of the X^{+} ^{2}Σ_{u}^{+} (ν^{+}=0) ground state of ^{4}He_{2}^{+} have been determined with unprecedented precision and accuracy by Rydberg-series extrapolation. Comparison with ab initio predictions of the rotational energy level structure of ^{4}He_{2}^{+} [W.-C. Tung, M. Pavanello, and L. Adamowicz, J. Chem. Phys. 136, 104309 (2012)] enabled us to quantify the magnitude of relativistic and quantum-electrodynamics contributions to the fundamental rotational interval of He_{2}^{+}.
Measuring spin-rotation intervals in molecular cations is challenging, particularly so when the ions do not have electric-dipole-allowed rovibrational transitions. We present a method, based on an angular-momentum basis transformation, to determine the spin-rotational fine structure of molecular ions from the fine structure of high Rydberg states. The method is illustrated by the determination of the so far unknown spin-rotation fine structure of the fundamentally important He_{2}^{+} ion in the X ^{2}Σ_{u}^{+} state. The fine-structure splittings of the v^{+}=0, N^{+}=1, 3, and 5 levels of He_{2}^{+} are 7.96(14), 17.91(32), and 28.0(6) MHz, respectively. The experiment relies on the use of single-mode cw radiation to record spectra of high Rydberg states of He_{2} from the a ^{3}Σ_{u}^{+} metastable state.
The term values of rotational levels of the first excited vibrational state of the electronic ground state of He2 + with rotational quantum number N + ≤ 13 have been determined with an accuracy of 1.2 × 10 −3 cm −1 (∼35 MHz) by MQDT-assisted Rydberg spectroscopy of metastable He2. Comparison of the experimental term values with the most accurate ab initio results for He2 + available in the literature [W.-C. Tung, M. Pavanello, and L. Adamowicz, J. Chem. Phys. 136, 104309 (2012)] reveals inconsistencies between theoretical and experimental results that increase with increasing rotational quantum number. The fundamental vibrational wavenumber of He2 + was determined to be 1628.3832(12) cm −1 by fitting effective molecular constants to the obtained term values.
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