DETERMINATION OF ATOMIC AND MOLECULAR-PARTICLE DENSITIES AND TEMPERATURES IN A LOW-PRESSURE HYDROGEN HOLLOW-CATHODE DISCHARGE

Citation
W. Biel et al., DETERMINATION OF ATOMIC AND MOLECULAR-PARTICLE DENSITIES AND TEMPERATURES IN A LOW-PRESSURE HYDROGEN HOLLOW-CATHODE DISCHARGE, Plasma physics and controlled fusion, 39(5), 1997, pp. 661-681
Citations number
67
Categorie Soggetti
Phsycs, Fluid & Plasmas
ISSN journal
07413335
Volume
39
Issue
5
Year of publication
1997
Pages
661 - 681
Database
ISI
SICI code
0741-3335(1997)39:5<661:DOAAMD>2.0.ZU;2-F
Abstract
Atomic (H) and molecular (H-2) hydrogen densities and temperatures hav e been determined in a magnetized hollow cathode are plasma burning at low pressure (p = 4-40 Pa). Rayleigh scattering measurements are used to derive the sum of atomic and molecular densities, each weighted wi th its scattering cross section. Coherent anti-Stokes Raman scattering (CARS) has been used to determine the population density differences of rovibrational molecular H-2 states n(H2) (v, J) - n(H2)(v + 1, J). The CARS intensity of many rotational states (J less than or equal to 9) of H-2 can be detected and these levels are found to be populated a ccording to a Boltzmann distribution. In the low-pressure plasma only the fundamental vibrational band of H-2 can be found experimentally ow ing to the low particle densities. In order to evaluate the H-2 densit y properly from the measured CARS data, the H-2 vibrational population for v > 0 is calculated from a spatially one-dimensional diffusion re action model. Within the plasma centre the dissociation degree d = n(H )/(n(H) + 2n(H2)) approximate to 0.4 and about one third of the molecu lar hydrogen is found in vibrationally excited states. Here, the vibra tional temperature is about T-vib approximate to 5000 K, which far exc eeds the gas temperature of T-gas approximate to 1000-3000 K. The diss ociation degree and the vibrational distribution are mainly determined by electron-impact processes in the inner plasma region and recycling processes at the vessel walls, whereas the influence of inelastic neu tral-neutral collisions is rather marginal.