4.6 Article

Parity-pair-mixing effects in nonlinear spectroscopy of HDO

Journal

OPTICS EXPRESS
Volume 30, Issue 26, Pages 46040-46059

Publisher

Optica Publishing Group
DOI: 10.1364/OE.474525

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Funding

  1. Nederlandse Organisatie voor Wetenschappelijk Onderzoek [16MYSTP]
  2. Horizon 2020 Framework Programme
  3. Nemzeti Kutatasi Fejlesztesi esInnovacios Hivatal
  4. [654148]
  5. [K138233]

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A non-linear spectroscopic study of the HDO molecule was performed using noise-immune cavity-enhanced optical-heterodyne molecular spectroscopy. Spectral perturbations, including distortions, shifts, and splittings, were observed, which were attributed to the AC-Stark effect and parity-pair mixing. The study achieved higher precision compared to Doppler-limited techniques.
A non-linear spectroscopic study of the HDO molecule is performed in the wavelength range of 1.36-1.42 mu m using noise-immune cavity-enhanced optical-heterodyne molecular spectroscopy (NICE-OHMS). More than 100 rovibrational Lamb dips are recorded, with an experimental precision of 2-20 kHz, related to the first overtone of the O-H stretch fundamental of HD16O and HD18O. Significant perturbations, including distortions, shifts, and splittings, have been observed for a number of Lamb dips. These spectral perturbations are traced back to an AC-Stark effect, arising due to the strong laser field applied in all saturation-spectroscopy experiments. The AC-Stark effect mixes parity pairs, that is pairs of rovibrational states whose assignment differs solely in the Kc quantum number, where Kc is part of the standard JKa,Kc asymmetric-top rotational label. Parity-pair mixing seems to be especially large for parity pairs with Ka >= 3, whereby their energy splittings become as small as a few MHz, resulting in multi-component asymmetric Lamb-dip profiles of gradually increasing complexity. These complex profiles often include crossover resonances. This effect is well known in saturation spectroscopy, but has not been reported in combination with parity-pair mixing. Parity-pair mixing is not seen in H216O and H 18 2 O, because their parity pairs correspond to ortho and para nuclear-spin isomers, whose interaction is prohibited. Despite the frequency shifts observed for HD16O and HD18O, the absolute accuracy of the detected transitions still exceeds that achievable by Doppler-limited techniques. (c) 2022 Optica Publishing Group under the terms of the Optica Open Access Publishing Agreement

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