2015
DOI: 10.1016/j.sab.2015.02.016
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Emission and absorption spectroscopy study of Ar excited states in 13.56MHz argon plasma operating at sub-atmospheric to atmospheric pressure

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Cited by 13 publications
(8 citation statements)
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“…50 In such motion-limited discharges, the contribution of the VDF shape to the final line broadening is dominant (including the thermalized case, i.e., the Doppler broadening), whereas the other broadening mechanisms are negligible. 51 The other broadenings mechanisms such as resonant, Stark, or Van der Vaals broadening become essential only at high pressure, 52 which is out of scope of this paper.…”
Section: On the Velocity Distribution Function In Hipimsmentioning
confidence: 99%
“…50 In such motion-limited discharges, the contribution of the VDF shape to the final line broadening is dominant (including the thermalized case, i.e., the Doppler broadening), whereas the other broadening mechanisms are negligible. 51 The other broadenings mechanisms such as resonant, Stark, or Van der Vaals broadening become essential only at high pressure, 52 which is out of scope of this paper.…”
Section: On the Velocity Distribution Function In Hipimsmentioning
confidence: 99%
“…Sub‐atmospheric discharge has been attracting great attention due to its valuable applications in many fields such as material processing, biological, and medical treatments . Most existing sub‐atmospheric discharges, including dielectric barrier discharge, capacitive discharge and cascaded arc, however, involve direct contact between plasma and electrode, which results in low energy efficiency and short life span because of the formed plasma sheath on the surface of electrode . Therefore, it is of practical interest to explore new discharge scheme that has no contact between plasma and electrode and can work efficiently in sub‐atmospheric environment.…”
Section: Introductionmentioning
confidence: 99%
“…The line absorption profile induced by Van der Waals contribution has the Lorentzian shape, and its FWHM (Δ ν VAN in s −1 ) can be expressed as normalΔνVAN= C1Ngas where C 1 = 3 × 10 16 ν 0 2 C 0.4 ( T gas / µ ) 0.6 is the unit of cm 3 s −1 , N gas is the neutral (ground state) density in cm −3 , and µ is the reduced mass (in amu) of nitrogen, i.e., is 14.0067/2 = 7.00335. Further, the width (FWHM) of the resonance broadening is given by normalΔνVAN C2Ngas where C 2 = 8.62 × 10 −29 ν 0 2 ν res f osc √( g 2 / g 1 ).c is the unit in cm 3 s −1 .…”
Section: Methodsmentioning
confidence: 99%
“…In Equation (5), the Gaussian contribution (Dn G ) can be evaluated by the familiar expression Dn G ¼ 7.16 Â 10 À7 n 0 √(T gas /M). [18,23,24] Here, T gas is the gas temperature, M (amu) is the atomic mass of the radiating (radical) species in the plasmas, and v 0 is the central frequency of the absorption line. Further, knowing the gas pressure and concentration of the neutrals, the Lorentzian contribution (Dn L ) of the Voigt profile (FWHM) can be calculated.…”
Section: Vuvas and Oesmentioning
confidence: 99%
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