Abstract:A hollow tube cathode using lanthanum hexaboride as the electron emitter has been designed and constructed. Tests in both argon and hydrogen indicate that this cathode is capable of producing over 800 A of electron current continuously, corresponding to over 25 A/cm(2) from the LaB(6). The cathode has been operated for over 300 h and exposed to air more than 100 times with no deterioration in emission. Projected lifetime is in excess of 3500 h for the sintered LaB(6) piece tested in this configuration. Constru… Show more
“…For instance, the LaB 6 thermionic cathode used for ignition of the hollow cathode discharge emission current of ϳ800 A and current density of ϳ25 A / cm 2 , described in Ref. 44, requires a heater with a power supply of 1 kW. An improved version of this electron source, 46 which operates at a vacuum Ͻ10 −4 Torr, requires a thermionic heater of 4.5 kW.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
confidence: 99%
“…In the case of MCDC with the FPS igniter, the required energy is hundreds of times less than in the case of thermionic cathode. 44,45 The compatibility of the cathodes with the high vacuum requirement is one of the key issues in diode operation at a high repetition rate. The deterioration of the background pressure during MCDC operation was studied using a calibrated Penning probe.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
confidence: 99%
“…A review concerning active plasma sources was already published 30 years ago by Kreindel,32 and recently a textbook 33 by Oks summarized the progress achieved for the past decades in research, development, and application of different types of plasma cathode. As examples of such plasma sources one can consider pulsed arc plasma sources, [34][35][36][37] hollow cathode operating in steady state [38][39][40][41][42] and pulsed [43][44][45][46] modes, hollow-anode plasma source, [47][48][49] and a ferroelectric plasma source ͑FPS͒. 50,51 Developed active plasma sources show long lifetime ͑Ͼ10 6 pulses͒, they operate at moderate vacuum ͑10 −4 Torr͒, and in general these sources are not sensitive to pollution.…”
Section: High-current Electron Beam Generation In a Diode With A Multmentioning
confidence: 99%
“…Let us note that some important applications require pulsed electron beams with a large cross-sectional area and current densities of several A / cm 2 . 18,33,36,57,58 Arc, 34,36 magnetron, 39,43 Penning, 33,36,39 and thermionic [40][41][42][44][45][46] sources were used for ignition of high-current hollow cathode plasma sources which can produce electron beams with a current density up to several tens of A / cm 2 under the application of an accelerating pulse with an amplitude up to several hundreds of kilovolts. However, all these methods of hollow cathode discharge ignition require relatively powerful power supplies.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
Articles you may be interested inEmittance of short-pulsed high-current ion beams formed from the plasma of the electron cyclotron resonance discharge sustained by high-power millimeter-wave gyrotron radiation Rev. Sci. Instrum. 85, 023307 (2014); 10.1063/1.4866651High-current long-duration uniform electron beam generation in a diode with multicapillary carbon-epoxy cathode
“…For instance, the LaB 6 thermionic cathode used for ignition of the hollow cathode discharge emission current of ϳ800 A and current density of ϳ25 A / cm 2 , described in Ref. 44, requires a heater with a power supply of 1 kW. An improved version of this electron source, 46 which operates at a vacuum Ͻ10 −4 Torr, requires a thermionic heater of 4.5 kW.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
confidence: 99%
“…In the case of MCDC with the FPS igniter, the required energy is hundreds of times less than in the case of thermionic cathode. 44,45 The compatibility of the cathodes with the high vacuum requirement is one of the key issues in diode operation at a high repetition rate. The deterioration of the background pressure during MCDC operation was studied using a calibrated Penning probe.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
confidence: 99%
“…A review concerning active plasma sources was already published 30 years ago by Kreindel,32 and recently a textbook 33 by Oks summarized the progress achieved for the past decades in research, development, and application of different types of plasma cathode. As examples of such plasma sources one can consider pulsed arc plasma sources, [34][35][36][37] hollow cathode operating in steady state [38][39][40][41][42] and pulsed [43][44][45][46] modes, hollow-anode plasma source, [47][48][49] and a ferroelectric plasma source ͑FPS͒. 50,51 Developed active plasma sources show long lifetime ͑Ͼ10 6 pulses͒, they operate at moderate vacuum ͑10 −4 Torr͒, and in general these sources are not sensitive to pollution.…”
Section: High-current Electron Beam Generation In a Diode With A Multmentioning
confidence: 99%
“…Let us note that some important applications require pulsed electron beams with a large cross-sectional area and current densities of several A / cm 2 . 18,33,36,57,58 Arc, 34,36 magnetron, 39,43 Penning, 33,36,39 and thermionic [40][41][42][44][45][46] sources were used for ignition of high-current hollow cathode plasma sources which can produce electron beams with a current density up to several tens of A / cm 2 under the application of an accelerating pulse with an amplitude up to several hundreds of kilovolts. However, all these methods of hollow cathode discharge ignition require relatively powerful power supplies.…”
Section: B Mcdc Assisted By Ferroelectric Plasma Sourcementioning
Articles you may be interested inEmittance of short-pulsed high-current ion beams formed from the plasma of the electron cyclotron resonance discharge sustained by high-power millimeter-wave gyrotron radiation Rev. Sci. Instrum. 85, 023307 (2014); 10.1063/1.4866651High-current long-duration uniform electron beam generation in a diode with multicapillary carbon-epoxy cathode
“…LaB 6 is known to have a comparably lower work function and is widely used as a thermionic emitter in many situations, not only in vacuum (e.g. in electron guns or electron microscopes) but also in hydrogen for plasma or neutral beam generation [6,7,8,9,10]. For hydrogen, which is also used in nuclear fusion experiments, there is no cathode poisoning of LaB 6 emitters [11].…”
We report here on a potentially significant improvement in the design of neutral pressure gauges of the so-called ASDEX-type which were first used in the Axially Symmetric Divertor EXperiment (ASDEX). Such gauges are considered state-of-the-art and are in wide use in fusion experiments, but they nonetheless suffer from a relatively high failure rate when operated at high magnetic field strengths for long times. This is therefore a significant concern for long-pulse, high-field experiments such as Wendelstein 7-X (W7-X) and ITER. The new design is much more robust. The improvement is to use a LaB 6 crystal instead of a tungsten wire as the thermionic emitter of electrons in the gauge. Such a LaB 6 prototype gauge was successfully operated for a total of 60 hours in B = 3.1 T, confirming the significantly improved robustness of the new design, and qualifying it for near-term operation in W7-X. With the LaB 6 crystal, an order of magnitude reduction in heating current is achieved, relative to the tungsten filament based gauges, from 15-20 A to 1-2 A. This reduces the Lorenz forces and the heating power by an order of magnitude also and is presumably the reason for the much improved robustness. The new gauge design, test environment setup at the superconducting magnet, and results from test operation are described.
Thermionic hollow cathodes have been widely used in wide variety of areas such as spacecraft electric propulsion systems, material processing and lasers for more than half a century as efficient electron sources. Especially in electric propulsion systems, hollow cathodes are being used as electron sources for propellant ionization and ion beam neutralization. Moreover, it is also a promising candidate for utilization as a stand-alone propulsion system in microsatellites or nanosatellites due to its small physical size, low power consumption and ease of operation. On the other hand, the small geometry of the typical orificed hollow cathodes makes the plasma diagnostics difficult which is why numerical studies become important for understanding the driving physical processes behind their operation, and the effects of the geometry and the operation parameters on cathode performance. In this paper, a global numerical model for the insert and orifice plasma of a hollow cathode is presented where volume averaged plasma parameters are considered for both regions. The results of this study show that the developed model can be used for designing and sizing orificed hollow cathodes as comparisons with the results of experimental and other numerical studies are in good agreement with the ones obtained from the developed model.
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