2003
DOI: 10.1134/1.1625058
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The near infrared (0.8−2.6µm) absorption spectrum of a dense sodium vapor and possible mechanisms of the spectrum formation

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Cited by 7 publications
(5 citation statements)
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“…al. 34 As it is shown here, one of the main features of the collision-induced absorption is a quadratic dependence of the absorption coefficient on the density and a weak dependence on the temperature. 35 Based on this model, we calculated the absorption coefficient in the target vapor up to 0.7 eV and fitted the dependence between the experimental data for the liquid target and the Bremsstrahlung coefficient given by Johnston and Dawson.…”
Section: Modeling Resultssupporting
confidence: 50%
“…al. 34 As it is shown here, one of the main features of the collision-induced absorption is a quadratic dependence of the absorption coefficient on the density and a weak dependence on the temperature. 35 Based on this model, we calculated the absorption coefficient in the target vapor up to 0.7 eV and fitted the dependence between the experimental data for the liquid target and the Bremsstrahlung coefficient given by Johnston and Dawson.…”
Section: Modeling Resultssupporting
confidence: 50%
“…It is also important to take into account the re-absorption of laser radiation in the evolving plasma after the reflection from the liquid target surface. For accurate modeling of the above-described processes, we used available data of the experimental optical properties for laser reflection from liquid tin; 16,17 then, since one of the main features of the collision-induced absorption is a quadratic dependence of the absorption coefficient on the density with a weak dependence on the temperature, 18 laser photons absorption in vapor was simulated with this approach and the inverse bremsstrahlung absorption was used for simulation of laser photons interaction with plasma. In our Monte Carlo modeling of laser photons absorption, reflection, and re-absorption in liquid/vapor/plasma as well as photon transport in plasma interplays with surface vaporization process.…”
Section: Introductionmentioning
confidence: 99%
“…Calculations of the tin target reflectivity give k target ¼ 0:84 for the Nd:YAG laser with k ¼ 1.064-lm, and k target ¼ 0:92 for the CO 2 laser with k ¼ 10.64-lm wavelength, based on the Sn optical data taken from the Ref. 23. The second and third media are a vapor/plasma mixture and a surrounding, welldeveloped plasma, which require special modeling of laser photon propagation.…”
Section: Mathematical and Physical Modelsmentioning
confidence: 99%