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A study of chromic oxide decomposition in an RF argon plasma
Authors:P. Meubus  A. Huczko
Affiliation:(1) Applied Sciences Department, Université du Québec à Chicoutimi, G7H 2B1 Chicoutimi, P.Q., Canada;(2) Départment of Chemistry, Warsaw University, 02-093 Warsaw, Poland
Abstract:Vapor-phase thermal decomposition of chromic oxide in an rf argon plasma was studied using a new experimental system. Homogeneous and heterogeneous modes of reaction were compared, the overall process efficiency being substantially higher for the process carried out entirely in the vapor phase. Reaction products were collected along the reactor wall and studied by chemical methods as well as SEM, X-ray, and IR absorption. The collected powder was highly reactive, fine-grained, and of semiamorphous nature, the average particle size being well below 100 nm. Temperature profiles recorded below the coupling coil by spectroscopic methods were typical of an rf plasma, showing maxima slightly exceeding 5000 K, with the presence of off-axis peaks. Local Cr contents and concentration ratio eegr(Cr)/eegr(Cr2O3) in the plasma were determined from the deposition data obtained. A diffusion process was assumed for the wall-deposit buildup. The results obtained confirmed the advantages of using plasma vapor-phase systems, these being higher-efficiency processes and more reliable models than those obtained in the case of gas-solid plasma reactors, where solid particles are injected into the plasma. The thermal decomposition conversion of Cr2O3 into Cr was about 8 times higher in the homogeneous gas phase than in the plasma solid phase, all other conditions being equal.Nomenclature c velocity of light, cm × s–1 - CCrm metallic Cr content, % by wt. - CCrt total Cr content, % by wt. - D species diffusivity, cm2 · s–1 - E energy of excited level, eV - f oscillator strength - F rate of species deposition, mol · cm–2 · s–1 - g statistical weight - h Planck's constant, J · s–1 - I radial emission intensity for a given spectral line at a given radius in the plasma, W · sr–1 · cm–3 - k Boltzmann's constant, J · K–1 - l length of collected deposit, cm - m mass of collected deposit, g - M molar weight of Cr - MAra molar flow of axial argon, mmol · s–1 - MArp molar flow of peripheral argon, mmol · s–1 - MCr2O3 molar flow of evaporated Cr2O3, mmol · s–1 - eegr Cr(I) concentration, cm–3 - QT partition function at temperatureT - r reaction radius, cm - R radius of quartz tube, cm - t duration of deposition, s - T temperature, K - 
$$U_{{text{Cr}}_{text{2}} {text{O}}_{text{3}} }^{text{t}}$$
total extent of Cr2O3 decomposition into Cr, % - Z position of a plane normal to the plasma axis downward the lower turn of rf coil, cmGreek Letters beta molar ratio of Cr and Cr2O3 in deposit - lambda wavelength, nm - eegr species concentration, mol · cm–3
Keywords:RF plasma  thermal decomposition  chromium and chromic oxide  modelling and experiments
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