Coaxial waveguide

In the coaxial configuration, the energy is coupled via a coaxial waveguide inserted into the plasma chamber. A quartz tube substitutes the outer conductor of the waveguide. The plasma formed around the quartz tube acts as an outer conductor in such a way that a spatially extended surface wave is created, just in an equivalent ('inverse') situation to that found in the Surfatron source (where the plasma is inside the tube instead of outside).

Picture of Coaxial Plasma Waveguide

This plasma source is studied using PLASIMO. The EM module is coupled to the fluid non-local-thermal-equilibrium (non-LTE) description of a discharge (flow, temperatures and species densities), and it allows the construction of a 2D self-consistent multi-physics model for microwave induced plasmas.

The simulation results show the two dimensional distribution of electron temperature, electron density and gas temperature.

electron temperature distribution

A radial localization of electron density in coaxial plasma waveguide is observed. The simulation results are compared with experimental results. A very good agreement is reached. The figure below shows the radial plasma localization at pressure of 8 mbar.

radial plasma profile

The radial localization of electron density is a consequence of the radial distribution of the power density inside the plasma, the electron heat conduction and the radial dimensions. The figure below presents the power density profile at pressure of 3 mbar.

power density profile

The effect of the gas pressure on the plasma distribution is studied. The figure below shows the plasma density profiles for different values of the gas pressure.

plasme density profiles


[1] Rahimi S., Jimenez-Diaz M., Hubner S., Kemaneci E.H., Mullen J.J.A.M. van der and Dijk J. van. (2014). A two-dimensional modelling study of a coaxial plasma waveguide. Journal of Physics D: Applied Physics, 47, 125204. [ bib | read article ]