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Published byΆνθεια Αναστασιάδης Modified over 6 years ago
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Effect of Faraday shields on capacitive coupling
D.D. Blackwell and F.F. Chen, 2D imaging of a helicon discharge, Plasma Sources Sci. Technol. 6, 569 (1997) No shield With shield
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m = +1 mode much stronger than m = –1
D.D. Blackwell and F.F. Chen, 2D imaging of a helicon discharge, Plasma Sources Sci. Technol. 6, 569 (1997) m = –1 m = +1
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Development of a time-resolved energy analyzer
D.D. Blackwell and F.F. Chen, Time-resolved measurements of the EEDF in a helicon plasma, Plasma Sources Sci. Technol. 10, 226 (2001) RF modulated electron gun for calibration 2-electrode gridded analyzer with RF response
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Time-resolved EEDFs show no fast electrons above a threshold of 10 -4
F.F. Chen and D.D. Blackwell, Upper limit to Landau damping in helicon discharges, Phys. Rev. Lett. 82, 2677 (1999) I-V swept by oscillating Vs I-V at two RF phases Loading resistance agrees with calculations w/o L.D. Injecting a current causes a beam-plasma instability
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Development of an RF J-dot probe
D.D. Blackwell, T.G. Madziwa, D. Arnush, and F.F. Chen, Evidence for Trivelpiece-Gould modes in a helicon discharge, LTP-106 (June, 2001)
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Evidence for Trivelpiece-Gould modes
D.D. Blackwell, T.G. Madziwa, D. Arnush, and F.F. Chen, Evidence for Trivelpiece-Gould modes in a helicon discharge, LTP-106 (June, 2001) "Wings" are seen in Jz but not in Bz. "Wings" are not predicted by theory if TG modes are neglected.
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