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Dunaevsky, A.; Raitses, Y.; Fisch, N. J.
Princeton Plasma Physics Lab., Princeton, NJ (United States). Funding organisation: US Department of Energy (United States); USDOE Office of Science (Seychelles) (US)2005
Princeton Plasma Physics Lab., Princeton, NJ (United States). Funding organisation: US Department of Energy (United States); USDOE Office of Science (Seychelles) (US)2005
AbstractAbstract
[en] Plasma acceleration from rf discharge in dielectric capillary was demonstrated. Observed plasma flow had ion energies of approximately 100 eV and electron energies of approximately 20 eV. The discharge was powered by a MHz-range rf generator and fed by Ar. Experimental results indicate possible validity of assumptions about formation of a potential difference at the open end of the capillary and presence of hot electron fraction in the capillary discharge. Simplicity and small dimensions of the source are attractive for micro-propulsion applications
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9 Aug 2005; 18 p; AC--20-76CH0373; Also available from OSTI as DE00842400; PURL: https://www.osti.gov/servlets/purl/842400-sfcab7/native/
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Dunaevsky, A.; Fisch, N.J.
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
AbstractAbstract
[en] The initial density and electron temperature at the surface of a ferroelectric plasma source were deduced from floating probe measurements in an expanding plasma. The method exploits negative charging of the floating probe capacitance by fast flows before the expanding plasma reaches the probe. The temporal profiles of the plasma density can be obtained from the voltage traces of the discharge of the charged probe capacitance by the ion current from the expanding plasma. The temporal profiles of the plasma density, at two different distances from the surface of the ferroelectric plasma source, could be further fitted by using the density profiles for the expanding plasma. This gives the initial values of the plasma density and electron temperature at the surface. The method could be useful for any pulsed discharge, which is accompanied by considerable electromagnetic noise, if the initial plasma parameters might be deduced from measurements in expanding plasma
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2 Oct 2003; 31 p; J--813; AC02-76CH03073; Also available from OSTI as DE00821515; PURL: https://www.osti.gov/servlets/purl/821515-LvZ4hz/native/
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Dunaevsky, A.; Raitses, Y.; Fisch, N.J.
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
AbstractAbstract
[en] The discharge parameters in Hall thrusters depend strongly on the yield of secondary electron emission from channel walls. Comparative measurements of the yield of secondary electron emission at low energies of primary electrons were performed for several dielectric materials used in Hall thrusters with segmented electrodes. The measurements showed that at low energies of primary electrons the actual energetic dependencies of the total yield of secondary electron emission could differ from fits, which are usually used in theoretical models. The observed differences might be caused by electron backscattering, which is dominant at lower energies and depends strongly on surface properties. Fits based on power or linear laws are relevant at higher energies of primary electrons, where the bulk material properties play a decisive role
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12 Feb 2003; 20 p; AC--02-76CH03073; Also available from OSTI as DE00812024; PURL: https://www.osti.gov/servlets/purl/812024-OfTLzr/native/
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Dunaevsky, A.; Fisch, N.J.
Princeton Plasma Physics Laboratory, Princeton, NJ (United States). Funding organisation: USDOE Office of Science (United States)2004
Princeton Plasma Physics Laboratory, Princeton, NJ (United States). Funding organisation: USDOE Office of Science (United States)2004
AbstractAbstract
[en] Ferroelectric plasma sources in vacuum are known as sources of ablative plasma, formed due to surface discharge. In this paper, observations of a gas discharge mode of operation of the ferroelectric plasma sources (FPS) are reported. The gas discharge appears at pressures between approximately 20 and approximately 80 Torr. At pressures of 1-20 Torr, there is a transition from vacuum surface discharge to the gas discharge, when both modes coexist and the surface discharges sustain the gas discharge. At pressures between 20 and 80 Torr, the surface discharges are suppressed, and FPS operate in pure gas discharge mode, with the formation of almost uniform plasma along the entire surface of the ceramics between strips. The density of the expanding plasma is estimated to be about 1013 cm-3 at a distance of 5.5 mm from the surface. The power consumption of the discharge is comparatively low, making it useful for various applications. This paper also presents direct measurements of the yield of secondary electron emission from ferroelectric ceramics, which, at low energies of primary electrons, is high and dependent on the polarization of the ferroelectric material
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8 Mar 2004; 11 p; AC02-76CH03073; Also available from OSTI as DE00827681; PURL: https://www.osti.gov/servlets/purl/827681-pjNLOA/native/
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Raitses, Y.; Staack, D.; Dunaevsky, A.; Fisch, N.J.
Princeton Plasma Physics Lab., Princeton, NJ (United States). Funding organisation: USDOE - Office of Science (Seychelles) (US)2005
Princeton Plasma Physics Lab., Princeton, NJ (United States). Funding organisation: USDOE - Office of Science (Seychelles) (US)2005
AbstractAbstract
[en] Carbon fiber velvet material provides exceptional sputtering resistance properties exceeding those for graphite and carbon composite materials. A 2 kW Hall thruster with segmented electrodes made of this material was operated in the discharge voltage range of 200-700 V. The arcing between the floating velvet electrodes and the plasma was visually observed, especially, during the initial conditioning time, which lasted for about 1 h. The comparison of voltage versus current and plume characteristics of the Hall thruster with and without segmented electrodes indicates that the magnetic insulation of the segmented thruster improves with the discharge voltage at a fixed magnetic field. The observations reported here also extend the regimes wherein the segmented Hall thruster can have a narrower plume than that of the conventional nonsegmented thruster
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1 Dec 2005; 24 p; AC02-76CH03073; Also available from OSTI as DE00934607; PURL: https://www.osti.gov/servlets/purl/934607-VN6nwI/; doi 10.2172/934607
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Dunaevsky, A.; Krasik, Ya.E; Eelstreiner, J.
Israel Physical Society 44. annual meeting. Program and abstracts1998
Israel Physical Society 44. annual meeting. Program and abstracts1998
AbstractAbstract
[en] A novel phenomenon of high frequency modulated electron beam generation is presented. Experiment was carried out with an electron diode having active source of the cathode plasma. Modulated electron beam with duration of > 1μs was generated during more than one hour with a frequency of 2Hz. The frequency of the modulation was found to be > 325MHz. The modulation of the beam current amplitude reaches > 30%. The generation of the modulated electron beam is accompanied by electromagnetic radiation with the same frequency and power of several tens of kW. Based on the experimental data a qualitative model of the observed phenomenon is described
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Weizmann Institute of Science, The Faculty of Physics, Rehovot (Israel); 196 p; 8 Apr 1998; p. 159; 44. annual meeting of the Israel Physical Society; Rehovot (Israel); 8 Apr 1998
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AbstractAbstract
[en] A review of experimental studies of the operation of cathodes made of metal-ceramic, velvet, corduroy, carbon fibers, carbon fabric, and different types of ferroelectrics is presented. These cathodes operated at electric fields in the range of 5-60 kV/cm that allowed the generation of electron beams with duration of several hundreds of nanoseconds while keeping a quasi-constant diode impedance. All cathodes had the same diameter and were tested in a diode powered by a high-voltage generator (300 kV, 85 Ω, 250 ns, ≤5 Hz). It was shown that the source of electrons for all the studied cathodes is a plasma which is formed as a result of surface discharges. Different types of electrical and optical diagnostics were used to study the formation and parameters of the plasma, the potential distribution inside the anode-cathode gap, and the uniformity and divergence of the extracted electron beam as a function of the amplitude and rise time of the accelerating pulse. Results of the lifetime of the tested cathodes and their compatibility with vacuum requirements are presented as well
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42. annual meeting of the Division of Plasma Physics of the American Physical Society; Quebec City, PQ (Canada); 23-27 Oct 2000; 10. international congress on plasma physics; Quebec City, PQ (Canada); 23-27 Oct 2000; (c) 2001 American Institute of Physics.; Country of input: International Atomic Energy Agency (IAEA)
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Raitses, Y.; Staack, D.; Dunaevsky, A.; Dorf, L.; Fisch, N.J.
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
Princeton Plasma Physics Lab., NJ (United States). Funding organisation: USDOE Office of Science (Seychelles) (US)2003
AbstractAbstract
[en] A 2-kW Hall thruster was developed, built, and operated in an upgraded vacuum facility. The thruster performance and parameters of the plasma flow were measured by new diagnostics for plume measurements and plasma measurements inside the thruster channel. The thruster demonstrated efficient operation in terms of propellant and current utilization efficiencies in the input power range of 0.5-3.5 kW. Preliminary measurements of the ion energy spectra from the thruster axis region and the distribution of plasma parameters in the vicinity of the thruster exit are reported
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1 Mar 2003; 14 p; AC--02-76CH03073; Also available from OSTI as DE00812923; PURL: https://www.osti.gov/servlets/purl/812923-aRccD9/native/
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Krasik, Ya. E.; Dunaevsky, A.; Felsteiner, J.; Dorfman, S.
Book of Program and Abstracts of the 45th Annual Meeting of the Israel Physical Society and the Second Conference of the Israel Plasma Science and Technology Association1999
Book of Program and Abstracts of the 45th Annual Meeting of the Israel Physical Society and the Second Conference of the Israel Plasma Science and Technology Association1999
AbstractAbstract
[en] We present experimental results of plasma formation on the surface of ferroelectric samples. Different poled and unpoled ferroelectric samples having a disk or tube form and made of Pb(Zr,Ti)03 or BaTi03 were tested. Using fast framing photography and different electric probes it was found that the application of a high-voltage driving pulse to the ferroelectric sample causes a fast surface plasma formation. This plasma formation occurs within a few nanoseconds from the start of the driving pulse for all the tested ferroelectric samples and the methods of applying the driving pulse. It was found that reversing the polarization of a ferroelectric does not play a significant role in the process of the plasma formation. Parameters of the plasma and of the neutral flow formed during the plasma formation versus the polarity and the amplitude of the driving pulse are presented. In addition we present experimental results of electron diode operation with an active plasma cathode. We studied the operation of planar and coaxial electron diodes under the application of an accelerating high-voltage pulse < 45 kV with repetition rate < 5 Hz or < 250 kV in a single mode operation. Electron beams with a current density of several hundreds of A/cm2 and a time duration of several hundreds of as were generated. It was shown that the parameters of the electron beam as well as the operation of the electron diode depend strongly on the method of the plasma formation and the time delay between the beginning of the plasma formation and the application of the high-voltage pulse
Source
Israel Physical Society (Israel); 228 p; 18 Mar 1999; p. 208; 45. Annual Meeting of the Israel Physical Society; Tel-Aviv (Israel); 18 Mar 1999; 2. Conference of the Israel Plasma Science and Technology Association; Tel-Aviv (Israel); 18 Mar 1999
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Dunaevsky, A.; Krasik, Ya. E.; Felsteiner, J.; Rosenberg, A.
Book of Program and Abstracts of the 45th Annual Meeting of the Israel Physical Society and the Second Conference of the Israel Plasma Science and Technology Association1999
Book of Program and Abstracts of the 45th Annual Meeting of the Israel Physical Society and the Second Conference of the Israel Plasma Science and Technology Association1999
AbstractAbstract
[en] We present a detailed study of the recently discovered modulation at frequencies of hundreds of MHz of an electron beam produced by a plasma cathode. The plasma cathode consists of a ferroelectric disk sample [BaTi03 or Pb(Zr,Ti)03] that is placed in a cylindrical metal box having an output window covered by a grid. The plasma is prepared by a non complete discharge which is ignited by a few kV driving pulse applied between a front electrode made of strips and a solid rear electrode. Experiments were carried out at accelerating voltages of < 45 kV and pulse duration of < 40 vs. It is found that the current modulation (depth of modulation 60% - 80%) appears only when the driving pulse is applied to the front electrode of the ferroelectric sample and the rear electrode is grounded. The modulation spectrum is quite narrow (< 3%), with harmonics at frequencies up to a few GHz. The basic frequency of modulation is found to depend on the length of the feed cable to the sample, the amplitude of accelerating voltage, and the anode-cathode gap. Active control of the frequency of the electron beam modulation in the range of 200 MHz - 420 MHz is demonstrated. Investigation of the plasma and the beam modulation properties and their dependence on the experimental parameters is presented. The results indicate the formation of a plasma at the vicinity of the front electrode of the ferroelectric sample during the modulation. In addition, we studied the potential distribution inside the cathode box between the front surface of the ferroelectric sample and the output cathode grid. The results are discussed within the framework of electrons oscillating in the potential well created by the positively charged plasma having feedback coupling with the input cable
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Israel Physical Society (Israel); 228 p; 18 Mar 1999; p. 216; 45. Annual Meeting of the Israel Physical Society; Tel-Aviv (Israel); 18 Mar 1999; 2. Conference of the Israel Plasma Science and Technology Association; Tel-Aviv (Israel); 18 Mar 1999
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