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Physical Review A

Doppler-free three-photon spectroscopy of 3 snf Rydberg states of Mg

R. Beigang, D. Schmidt, Andre Timmermann

Published May 1, 1984• 10 citations
Publisher

Abstract

High-resolution two-photon resonant three-photon spectroscopy was applied to investigate the 3 $\mathrm{snf}$ Rydberg series of Mg. Hyperfine-induced level shifts were detected for the $^{1,3}F$ states of the odd isotope $^{25}\mathrm{Mg}$. From these measurements the hyperfine coupling constant ${a}_{3s}$ of the $^{25}\mathrm{Mg}^{+}$-ion ground state was derived.

DOI
10.1103/physreva.29.2581

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Doppler-free two-photon spectroscopy was applied to excite hyperfine-induced transitions from the $5{s}^{2}^{1}S_{0}$ ground state to the F=IF=IF=I component of the hyperfine multiplet of the 5sns3S15sns^{3}S_{1}5sns3S1​ Rydberg series of 87Sr^{87}\mathrm{Sr}87Sr (n=50,…,85n=50,\dots{},85n=50,…,85). The experimental data confirm the interpretation of hyperfine-induced singlet-triplet mixing which is related to the singlet-triplet energy separation.
A combined experimental and theoretical spectroscopic study of high-$n, 30\ensuremath{\lesssim}n\ensuremath{\lesssim}100$, triplet SSS and DDD Rydberg states in 87Sr^{87}\mathrm{Sr}87Sr is presented. 87Sr^{87}\mathrm{Sr}87Sr has a large nuclear spin I=9/2I=9/2I=9/2, and at high-nnn the hyperfine interaction becomes comparable to, or even larger than, the fine structure and singlet-triplet splittings, which poses a considerable challenge both for precision spectroscopy and for theory. For high-nSn SnS states, the hyperfine shifts are evaluated nonperturbatively, taking advantage of earlier spectroscopic data for the I=0I=0I=0 isotope 88Sr^{88}\mathrm{Sr}88Sr, which results in good agreement with the present measurements. For the DDD states, this procedure is reversed by first extracting from the present 87Sr^{87}\mathrm{Sr}87Sr measurements the energies of the 3D1,2,3{}^{3}{D}_{1,2,3}3D1,2,3​ states to be expected for isotopes without hyperfine structure (88Sr^{88}\mathrm{Sr}88Sr), which allows the determination of corrected quantum defects in the high-nnn limit.