By Michael A. Lieberman (auth.), H. Schlüter, A. Shivarova (eds.)
This quantity relies at the lectures on the NATO complex learn Institute, entitled "Advanced applied sciences in response to Wave and Beam Generated Plasmas", held at Sozopol, Bulgaria, from may possibly 22 until June 1, 1998. It attracted nearly a hundred contributors from sixteen varied nations. The assembly mixed forms of scientists from complex specialists to aspiring younger researchers. It geared toward stimulating destiny improvement via providing-across borders- cross-fertilization and exchanges among formerly unconnected teams. this can be mirrored within the contents of the amount which covers the lectures given. The e-book additionally comprises in a moment half forty three poster shows quite often from more youthful members with useful complementations and specifica tions to the lectures. With its themes the complex research Institute constitutes the 1st try and collect in an prepared demeanour 3 parts of labor on plasma applied sciences: complex efforts in accordance with wave generated---high frequency-····plasmas, on plasma assisted ion implantation and on electron beam generated plasmas.
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Additional info for Advanced Technologies Based on Wave and Beam Generated Plasmas
The arrow indicates the electron density at the gap for a given HF absorbed power, the corresponding plasma column extending from this value on toward z=O [ 15] Although the axial inhomogeneity inherent to SWDs sustained with traveling waves can be a shortcoming for some applications, it is a real positive feature as far as comparing modeling results with experiments is concerned. This is because the consecutive plasma slices z, z + dz can be considered as discharges sustained under identical conditions, but with different absorbed power density.
N in tlgure 7 . This "slotted'' pattern, obtained through polymer deposition on the dielectric plate, has a linear, not a circular symmetry. This means that S has one dominating Sx component in the \Vave· guiding plane (XY}, most probably O\ving to the £1ct that there are no Ev and Hx · components coming out :fi·om the launcher aperture. } Rectangular waveguide Dark region Figure 7 - Standing wave pattern along the dielectric disk of figure 6, obtained through polymer deposition on the disk surface [69l Dielectric Disk Circumferentially-jed from a Radial Line (Kimura, Yoshida and Mizuguchi, 1995; Yoshida, 1998).
The question of the dependence of 8 on the magnetic field intensity  and the reactor aspect ratio RIL [53,54] were also examined providing insight in the optimum reactor geometry and power transfer efficiency. The influence of collisionless damping on the wave absorption was also considered . Finally, the modeling of the surface-wave plasma source with its wave launcher was the occasion of adapting the equivalent circuit approach to provide the required frequency and tuning characteristics (see, for example, figure 2) without having to solve a full set of electromagnetic field equations.