A new model for the treatment of optical saturation for measuring Ne*(<sup>3</sup>P<sub>0</sub>) metastable atoms density down to 10<sup>10</sup> m<sup>−3</sup> by cavity ring-down spectroscopy

Abstract Cavity ring-down spectroscopy with a continuous wave diode laser at 653 nm is used for measuring the density of Ne*( 3 P 0 ) metastable atoms in low pressure Ne–Ar glow discharges. Non-exponential ring-down (RD) signals are observed due to the optical saturation, which decreases along the RD time with the decay of the intra-cavity laser power (ICLP). Gaussian absorption line profiles, with Lamb-dips at the line center, are obtained for different power levels from the time-varying rates of the RD decays. The amplitude of the deduced line profile decreases with the rise of the ICLP, thus of the optical saturation. As the laser saturation model described in books of W. Demtröder cannot account for the velocity-changing (VC) and the metastability-exchanging (MC) collisions between Ne*( 3 P 0 ) and ground state atoms, a new model for the treatment of the saturated absorption line profiles is developed here. The necessary use of the power broadened width of the absorption line for obtaining the spectral power density, hence the saturation parameter S , is demonstrated in this model. This model demonstrates the necessary use of the power-broadened width of the absorption line to obtain the spectral power density and hence the saturation parameter S . It predicts very well the line profiles obtained with 224 µ W at pressures between 0.1 and 3.2 Torr and provides the density of Ne*( 3 P 0 ) atoms down to a few 10 10 m −3 . It is found that VC and MC collisions significantly contribute to the refilling of the Bennet hole produced in the velocity distribution of Ne*( 3 P 0 ) atoms by the optical pumping. Consequently, Ne*( 3 P 0 ) atoms inside the laser beam volume are depleted, for all velocity classes. The refilling of the depleted laser volume by diffusion of Ne*( 3 P 0 ) atoms from the volume surrounding the laser beam and its consequence on the optical saturation is treated in an appendix.

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Publication Details

Journal
Journal of Physics D Applied Physics
Published
2025-08-14
DOI
https://doi.org/10.1088/1361-6463/adfb8b
Citations
1
Primary Topic
Atomic and Subatomic Physics Research
Type
article
Field-Weighted Citation Impact
1.25
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article

A new model for the treatment of optical saturation for measuring Ne*(3P0) metastable atoms density down to 1010 m−3 by cavity ring-down spectroscopy

Peter Macko
1 citations
Journal of Physics D Applied Physics
Atomic and Subatomic Physics Research
1.25
article

A new model for the treatment of optical saturation for measuring Ne*(3P0) metastable atoms density down to 1010 m−3 by cavity ring-down spectroscopy

Peter Macko
article en
1 citations

Abstract

Abstract Cavity ring-down spectroscopy with a continuous wave diode laser at 653 nm is used for measuring the density of Ne*( 3 P 0 ) metastable atoms in low pressure Ne–Ar glow discharges. Non-exponential ring-down (RD) signals are observed due to the optical saturation, which decreases along the RD time with the decay of the intra-cavity laser power (ICLP). Gaussian absorption line profiles, with Lamb-dips at the line center, are obtained for different power levels from the time-varying rates of the RD decays. The amplitude of the deduced line profile decreases with the rise of the ICLP, thus of the optical saturation. As the laser saturation model described in books of W. Demtröder cannot account for the velocity-changing (VC) and the metastability-exchanging (MC) collisions between Ne*( 3 P 0 ) and ground state atoms, a new model for the treatment of the saturated absorption line profiles is developed here. The necessary use of the power broadened width of the absorption line for obtaining the spectral power density, hence the saturation parameter S , is demonstrated in this model. This model demonstrates the necessary use of the power-broadened width of the absorption line to obtain the spectral power density and hence the saturation parameter S . It predicts very well the line profiles obtained with 224 µ W at pressures between 0.1 and 3.2 Torr and provides the density of Ne*( 3 P 0 ) atoms down to a few 10 10 m −3 . It is found that VC and MC collisions significantly contribute to the refilling of the Bennet hole produced in the velocity distribution of Ne*( 3 P 0 ) atoms by the optical pumping. Consequently, Ne*( 3 P 0 ) atoms inside the laser beam volume are depleted, for all velocity classes. The refilling of the depleted laser volume by diffusion of Ne*( 3 P 0 ) atoms from the volume surrounding the laser beam and its consequence on the optical saturation is treated in an appendix.

Journal of Physics D Applied PhysicsVol. 58(38)
Laboratoire Interdisciplinaire de Physique (FR)
Openalex Percentile: Top 18%
Atomic and Subatomic Physics Research
1.25
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