Study of fundamental processes affecting the structure of the cathode zone of nitrogen/titanium dc discharge

Abstract

Processes affecting the emission of the cathode zone plasma of a N 2 /Ti dc discharge were studied experimentally and theoretically. Light maxima occurring at the negative glow head (maximum II) are due to the electron-molecule excitation. Emission characteristics of this region, space distributions of lighting, dependence of the line intensity (I ) on the gas pressure (p) and current density (j d ) can be fully explained by the Monte Carlo (M-C) simulation of electron motion in this region. Emission characteristics of the space close to the cathode surface (maximum I) are complex, depending on the emitting species. Molecular lines are found to be emitted mostly due to the fast ion-N 2 interactions. The results of the analytical modelling of this process confirm the experimentally observed almost linear dependences of the intensities of these lines on the pressure and current density. Lines of atomic nitrogen are found to be due to the fast ion-N 2 interactions as well as to the fast ion-solid excitation, both accompanied by a dissociation. Particular attention was paid to the emission of sputtered material lighting in the space close to the cathode surface. This lighting results from the fast ion-sputtered atom interaction as well as from that of the sputtered atom with 'hot' atoms of the cathode surface layer. The experimentally observed dependences of the sputtered atom line intensity on the gas pressure (I ∼ 1/p) and the discharge current density (I ∼ j d × j d ) are qualitatively explained with a complex model that takes into account the analytical assessment of the energy distribution of bombarding ions, the M-C simulation of the ion-solid interaction and the M-C simulation of the motion of atoms roaming in the plasma phase. The plasma of the space close to the cathode surface (maximum I) of low-pressure discharges (∼0.1 Torr) is an effective light source for the optical emission spectroscopy of buffer gas and solid species.

Monte Carlo simulation of fast electrons and heavy particles in the CDS of nitrogen dc glow discharge

“…Considering the great variation of the electric field in the CDS of dc glow discharge, the MC model may be the most suitable one to simulate particle kinetics in the CDS of dc glow discharge under stable discharge conditions when the selfconsistent problem can be neglected. Recently, Wronski [14] has used the MC method to investigate the process affecting the emission of the cathode zone plasma of an N 2 /T i dc discharge.…”

Laser Gas–Assisted Nitriding of Ti Alloys

“…Details on the theory can be found in (157)(158)(159). Determining parameters are: l L ¼ cathode fall length, l N o ¼ number of ions entering the cathode fall region from the negative glow, l l ¼ mean free path for charge-exchange collision.…”

Characterization of Nitrogen Glow Discharge Plasma via Optical Emission Spectrum Simulation

“…Recently, PALMERO presented an approach to correlate optical emission lines from the argon plasma with the corresponding electron density and temperature [4] . In contrast to the monatomic gas discharges, the nitrogen plasma processes are more complicated not only because the species variety is fertile but also the nitrogen molecular spectrum and its optical emission processes are extremely perplexing [7,8] . In addition, people are short of the cross section data for nitrogen, especially the impact excitation and emission cross sections [7] .…”

“…In contrast to the monatomic gas discharges, the nitrogen plasma processes are more complicated not only because the species variety is fertile but also the nitrogen molecular spectrum and its optical emission processes are extremely perplexing [7,8] . In addition, people are short of the cross section data for nitrogen, especially the impact excitation and emission cross sections [7] . Therefore, most of the theoretical investigations mainly focus on simulations of certain characteristic lines, which aim at the explanation of the experimental measurements [3,7,9] although experimental studies on the OES in nitrogen plasma are rather common.…”

“…In addition, people are short of the cross section data for nitrogen, especially the impact excitation and emission cross sections [7] . Therefore, most of the theoretical investigations mainly focus on simulations of certain characteristic lines, which aim at the explanation of the experimental measurements [3,7,9] although experimental studies on the OES in nitrogen plasma are rather common. More importantly, to author's knowledge, no theoretical investigations on the OES, in a point of view of plasma process mechanisms and the connection between the spectrum and the micro-quantities using any model, have been reported yet.…”