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    Precision Spectroscopy of the Fine and Hyperfine Structures of High Molecular Rydberg-Stark States: Metrology of Molecular Hydrogen Ions

    I. Doran1, L. Jeckel1, M. Beyer2, Ch. Jungen3, and F. Merkt1,4,5,*

    • *Contact author: frederic.merkt@phys.chem.ethz.ch

    Phys. Rev. Lett. 137, 063001 – Published 7 August, 2026

    DOI: https://doi.org/10.1103/5rsv-mb6x

    Abstract

    The Stark effect in autoionizing high-n Rydberg states decouples the Rydberg electron from the ion core through ℓ mixing with core-nonpenetrating high-ℓ states. The Rydberg states become long-lived, which is ideal for precision spectroscopy, and their structures reflect the fine and hyperfine structures of the ion-core levels. We report on precision measurements, in weak electric fields, of the fine and hyperfine structures of two distinct categories of high autoionizing molecular Rydberg-Stark states differing by the nature of the ion-core angular momentum: Rydberg states of para-H2 (total nuclear spin I=0,2) with a rotationally excited (N+=2) H2+ ion core and Rydberg states of ortho-D2 (I=0,2) with a rotationless (N+=0) ion core. The spectra reveal striking differences which are interpreted as arising from the dominance of anisotropic charge-quadrupole interactions between the rotating quadrupolar ion core and the Rydberg electron in para-H2 and the absence of such interactions in rotationless ortho-D2 Rydberg states. In ortho-D2, the dominant interaction, the magnetic Fermi-contact hyperfine interaction in the ion core, does not significantly affect the motion of the Rydberg electron. By analyzing these spectra based on a treatment combining multichannel quantum-defect theory and matrix diagonalization, we derive new experimental values of the hyperfine coupling constant bF=139.84(5)  MHz of D2+(v+=1,N+=0), the spin-rotation coupling constant ce=39.62(11)  MHz of H2+(v+=1,N+=2) and the fundamental vibrational interval of ortho-D2+ [47 279 980.8(1.9) MHz]. The approach followed here in the study of molecular Rydberg-Stark states is general and broadly applicable to measurements of the fine and hyperfine structures of molecular cations.

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