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Schumacher: Fusionsforschung – Eine Einf¨ uhrung (Wissenschaftliche Buchgesellschaft Darmstadt 1993) 20 5. J. H. Rutherford: Introduction to Plasma Physics (Institute of Physics Publishing, Bristol and Philadelphia 1995) 20 6. M. G. Teubner, Stuttgart 2003) 20 7. G. Franz: Oberfl¨ achentechnologie mit Niederdruckplasmen (Springer–Verlag, Berlin Heidelberg New York 1994) 20 2 Waves in Plasmas A. Piel Institut f¨ ur Experimentelle und Angewandte Physik, Christian-Albrechts-Univ. zu Kiel, Olshausenstr.

Using the Stixparameters, we find for the refractive index of the R-wave and L-wave 40 A. Piel 2 2 ωpi ωpe − NR = 1 − ω(ω − ωce ) ω(ω + ωci ) 2 2 ωpi ωpe − NL = 1 − ω(ω + ωce ) ω(ω − ωci ) 1/2 1/2 . 2 Cut-Offs and Resonances The refractive index for the R-wave has a resonance N 2 → ∞ at the electron cyclotron frequency ωce . Here the electric field vector and the electron have the same sense of rotation angular velocity about the magnetic field. The L-wave has a corresponding resonance at the ion cyclotron frequency ωci (Fig.

The strip sensor of 1 m length is part of a capacitance bridge. The radio frequency signal is produced by a Direct Digital Synthesis (DDS) oscillator, which is controlled by a Programmable Logic Device (PLD) that also handles the Analog Digital Conversion (ADC) and telemetry (TM) interface. (b) Mechanical arrangement of the impedance probe (IP), Langmuir probes (LP), resonance cone antennas (RC) and radio beacon (RABER) on the DEOS payloads.

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