High pressure mercury AC discharge tube exposed to coherent laser: optical, electrical and thermal aspects

Most optical emission line intensities remain unchanged for a mercury HID plasma, exposed to coherent argon ion laser beam Innova 308 C (476.5 nm) in points far from electrodes. Small raise of Hg-546.08 nm line is due to photo-excitation of Ar + ions, followed by excitation transfers through collisi...

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Veröffentlicht in:Journal of thermal analysis and calorimetry 2023-10, Vol.148 (20), p.10515-10529
Hauptverfasser: Harabor, Novac-Adrian, Harabor, Ana, Rotaru, Petre, Palarie, Ion
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Harabor, Ana
Rotaru, Petre
Palarie, Ion
description Most optical emission line intensities remain unchanged for a mercury HID plasma, exposed to coherent argon ion laser beam Innova 308 C (476.5 nm) in points far from electrodes. Small raise of Hg-546.08 nm line is due to photo-excitation of Ar + ions, followed by excitation transfers through collision processes from excited (Ar + ) * ions to Ar atoms, then from excited (Ar) * to Hg atoms. When the laser beam hits the electrode tip (photoelectric effect), the amount of electrons involved in plasma collisions increases: all characteristic emission spectral lines are intensifying. Electron temperature and concentration were also calculated. Differential Scanning Calorimetry performed in case of tungsten electrode with emissive material (Y 2 O 3 , BaCO 3 , CaCO 3 , WO 3 ), linear and non-isothermally heated (0.17 K s -1 ) in flowing air, from 290.61 to 1603.72 K (platinum crucible), revealed both endothermic (CaCO 3 and of BaCO 3 decompositions) and exothermal (obtaining CaWO 4 , BaWO 4 and Ba 3 WO 6 ) processes. Thermogravimetry Analysis showed a mass decrease of 0.498%, in 290.61−505.15 K temperature range, due to water release. Oxidation of tungsten electrode causes a significant mass increase of 17.292% in 809.15−1183.15 K range. BaWO 4 , Ba 3 WO 6 and WO 3 sublimations gave a mass fall of 6.757% in 1513.15−1603.72 K range. No thermal effects were recorded on heating in argon atmosphere, from 446.15 to 1596.15 K, in alumina crucible.
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Small raise of Hg-546.08 nm line is due to photo-excitation of Ar + ions, followed by excitation transfers through collision processes from excited (Ar + ) * ions to Ar atoms, then from excited (Ar) * to Hg atoms. When the laser beam hits the electrode tip (photoelectric effect), the amount of electrons involved in plasma collisions increases: all characteristic emission spectral lines are intensifying. Electron temperature and concentration were also calculated. Differential Scanning Calorimetry performed in case of tungsten electrode with emissive material (Y 2 O 3 , BaCO 3 , CaCO 3 , WO 3 ), linear and non-isothermally heated (0.17 K s -1 ) in flowing air, from 290.61 to 1603.72 K (platinum crucible), revealed both endothermic (CaCO 3 and of BaCO 3 decompositions) and exothermal (obtaining CaWO 4 , BaWO 4 and Ba 3 WO 6 ) processes. Thermogravimetry Analysis showed a mass decrease of 0.498%, in 290.61−505.15 K temperature range, due to water release. Oxidation of tungsten electrode causes a significant mass increase of 17.292% in 809.15−1183.15 K range. BaWO 4 , Ba 3 WO 6 and WO 3 sublimations gave a mass fall of 6.757% in 1513.15−1603.72 K range. 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Small raise of Hg-546.08 nm line is due to photo-excitation of Ar + ions, followed by excitation transfers through collision processes from excited (Ar + ) * ions to Ar atoms, then from excited (Ar) * to Hg atoms. When the laser beam hits the electrode tip (photoelectric effect), the amount of electrons involved in plasma collisions increases: all characteristic emission spectral lines are intensifying. Electron temperature and concentration were also calculated. Differential Scanning Calorimetry performed in case of tungsten electrode with emissive material (Y 2 O 3 , BaCO 3 , CaCO 3 , WO 3 ), linear and non-isothermally heated (0.17 K s -1 ) in flowing air, from 290.61 to 1603.72 K (platinum crucible), revealed both endothermic (CaCO 3 and of BaCO 3 decompositions) and exothermal (obtaining CaWO 4 , BaWO 4 and Ba 3 WO 6 ) processes. Thermogravimetry Analysis showed a mass decrease of 0.498%, in 290.61−505.15 K temperature range, due to water release. Oxidation of tungsten electrode causes a significant mass increase of 17.292% in 809.15−1183.15 K range. BaWO 4 , Ba 3 WO 6 and WO 3 sublimations gave a mass fall of 6.757% in 1513.15−1603.72 K range. 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Oxidation of tungsten electrode causes a significant mass increase of 17.292% in 809.15−1183.15 K range. BaWO 4 , Ba 3 WO 6 and WO 3 sublimations gave a mass fall of 6.757% in 1513.15−1603.72 K range. No thermal effects were recorded on heating in argon atmosphere, from 446.15 to 1596.15 K, in alumina crucible.</abstract><cop>Cham</cop><pub>Springer International Publishing</pub><doi>10.1007/s10973-023-12380-1</doi><tpages>15</tpages></addata></record>
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subjects Aluminum compounds
Analytical Chemistry
Argon ions
Calcium carbonate
Calorimetry
Chemistry
Chemistry and Materials Science
Collisions (Nuclear physics)
Crucibles
Electrodes
Electron energy
Emission
Excitation
Gas discharge tubes
Inorganic Chemistry
Laser beams
Lasers
Line spectra
Measurement Science and Instrumentation
Oxidation
Photoelectric effect
Photoelectricity
Physical Chemistry
Polymer Sciences
Scheelite
Temperature effects
Thermogravimetry
Tungsten oxides
Yttrium oxide
title High pressure mercury AC discharge tube exposed to coherent laser: optical, electrical and thermal aspects
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