Abstract:In order to specify the mechanisms involved in a xenon dielectric barrier excimer lamp, an experimental work was undertaken using two different set-ups. One study, performed under selective multiphotonic excitation, is presented here and the other, of a dielectric barrier micro-discharge, will be published in another paper. In this work, excitation of the two lower atomic states of the 5p56s configuration was performed: the Xe5p56s(3P2) metastable state and the molecular g states correlated to it or to the Xe5… Show more
“…Hence at 294 K, the molecular structure for wavelengths below the resonant state can be attributed to Xe 2 (B 1 g ), and absorption arises in the repulsive part of the ground-state potential (e. g. R ∼ 3.9Å). Excitation of Xe 2 B 0 + g occurs at shorter wavelengths with a maximum around 290.2 nm according to Ledru et al [14] and Gornik et al [30]. At high pressures, particularly above 100 Torr, for either any excitation condition or any gas temperature, the shapes of emission spectra are similar (fig 4).…”
Section: Excitation Spectramentioning
confidence: 73%
“…In such conditions, recombination phenomena, electronic collisions or atomic collisions involving two excited species do not contribute to the formation and decay of excimers. According to the simplified kinetic scheme established in a previous work at room temperature [14] for the emission of the first continuum, after selectively populating the resonant state, the evolution of the concentration the different states is governed by the differential equations :…”
Abstract. The temporal dependence of VUV emissions of the first continuum of xenon at around 150 nm are investigated for pressures ranging from 10 to 100 Torr and for temperatures ranging from 200 to 300 K, after briefly and selectively populating exclusively the resonant or the metastable atomic states of the 5p 5 6s configuration. A kinetic and spectroscopic study was performed by analyzing the VUV post luminescence decay of xenon operating with such excitation conditions. Our results clearly show the temperature effects on the rate constants α 31 and α 32 of formation of excimers correlated respectively to the first resonant and the first metastable states by three-body collisions. The resulting reaction rates are obtained as a function of temperature T : α 31 = 3.90 × 10 −27 T −1.78 cm −6 s −1 , α 32 = 1.34 × 10 −27 T −1.70 cm −6 s −1 . For the whole pressure range, low temperatures favour the formation of xenon excimers and the efficiency of the three-body collisions in forming stabilized excimers increases with decreasing temperature
“…Hence at 294 K, the molecular structure for wavelengths below the resonant state can be attributed to Xe 2 (B 1 g ), and absorption arises in the repulsive part of the ground-state potential (e. g. R ∼ 3.9Å). Excitation of Xe 2 B 0 + g occurs at shorter wavelengths with a maximum around 290.2 nm according to Ledru et al [14] and Gornik et al [30]. At high pressures, particularly above 100 Torr, for either any excitation condition or any gas temperature, the shapes of emission spectra are similar (fig 4).…”
Section: Excitation Spectramentioning
confidence: 73%
“…In such conditions, recombination phenomena, electronic collisions or atomic collisions involving two excited species do not contribute to the formation and decay of excimers. According to the simplified kinetic scheme established in a previous work at room temperature [14] for the emission of the first continuum, after selectively populating the resonant state, the evolution of the concentration the different states is governed by the differential equations :…”
Abstract. The temporal dependence of VUV emissions of the first continuum of xenon at around 150 nm are investigated for pressures ranging from 10 to 100 Torr and for temperatures ranging from 200 to 300 K, after briefly and selectively populating exclusively the resonant or the metastable atomic states of the 5p 5 6s configuration. A kinetic and spectroscopic study was performed by analyzing the VUV post luminescence decay of xenon operating with such excitation conditions. Our results clearly show the temperature effects on the rate constants α 31 and α 32 of formation of excimers correlated respectively to the first resonant and the first metastable states by three-body collisions. The resulting reaction rates are obtained as a function of temperature T : α 31 = 3.90 × 10 −27 T −1.78 cm −6 s −1 , α 32 = 1.34 × 10 −27 T −1.70 cm −6 s −1 . For the whole pressure range, low temperatures favour the formation of xenon excimers and the efficiency of the three-body collisions in forming stabilized excimers increases with decreasing temperature
“…Before being filled with pure krypton or a mixture of synthetic air and krypton, the cell was pumped down to full range of 1000 Torr for high pressure conditions. This experimental set-up has been fully described in a previous work [14].…”
For the first time, absolute densities of atomic nitrogen in its ground state (N 4 S) have been measured in hot dry and humid air plasma columns under post-discharge regime. The determination of space-resolved absolute densities leads to obtain the dissociation degrees of molecular nitrogen in the plasma. The hot plasmas are generated inside an upstream gas-conditioning cell at 600 mbar when the air gas flow is directly injected at 10 slm in a microwave resonant cavity (2.45 GHz, 1 kW) placed in the downstream side. Density measurements based on laser induced fluorescence spectroscopy with two-photon excitation (TALIF), are more particularly performed along the radial and axial positions of the plasma column. Calibration of TALIF signals is performed in situ (i.e. in the same gas-conditioning cell but without plasma) using an air gas mixture containing krypton. Optical emission spectroscopy is considered to estimate the rotational gas temperature by adding a small amount of H 2 in dry air to better detect OH (A-X) spectra. The rotational temperatures in humid air plasma column (50% of humidity) are larger than those of dry air plasma column by practically 30% near the nozzle of resonant cavity on the axis of the plasma column. This is partly due to attachment heating processes initiated by water vapor. A maximum of the measured absolute nitrogen density is also observed near the nozzle which is also larger for humid air plasma column. The obtained dissociation degrees of molecular nitrogen in both dry and humid air plasma along the air plasma column are lower than the cases where only thermodynamic equilibrium is assumed.
“…The Franck-Condon simulation of the spectrum shape suggests that emission stems from a bound-free molecular transition never studied before. The states involved are assigned as the bound (3) Luminescence of rare gas excimers is studied for applications in the vacuum ultraviolet (VUV) [1]. It is worth recalling, for instance, the Xe-based high-energy particle detectors, in which the VUV scintillation light produced by the transit of an ionizing particle is detected [2].…”
mentioning
confidence: 99%
“…The kinetics of the processes leading to excimer formation and VUV emission has been clarified in spectral and time resolved experiments, in which lifetimes and rate constants are determined [1,7,11,12,13,18,21,22,23,24,25,26].…”
We present an investigation of the Xe2 excimer emission spectrum observed in the near infrared range about 7800 cm −1 in pure Xe gas and in an Ar (90%) -Xe (10%) mixture and obtained by exciting the gas with energetic electrons. The Franck-Condon simulation of the spectrum shape suggests that emission stems from a bound-free molecular transition never studied before. The states involved are assigned as the bound (3)0 + u state with 6p [1/2]0 atomic limit and the dissociative (1)0 + g state with 6s [3/2]1 limit. Comparison with the spectrum simulated by using theoretical potentials shows that the dissociative one does not reproduce correctly the spectrum features.
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