Abstract:
A high-power microwave/mm-wave oscillator is filled with an ionizable gas at a pressure of about 1-20 mTorr, into which an electron beam (34) is injected at a high current density of at least about 1 amp/cm2, but typically 50-100 A/cm2. A plasma is formed which inhibits space-charge blowup of the beam, thereby eliminating the prior requirement of a magnet system to control the beam. The system functions as a slow-wave tube to produce narrow-band microwaves for a gas pressure of about 1-5 mTorr, and as a plasma wave tube to produce broadband microwave/mm-wave radiation for a gas pressure of about 10-20 mTorr. A new high output, hollow-cathode-plasma electron gun is employed in which a metal oxide layer is formed on the inner surface to enhance the secondary electron yield; a cathode (2), grid (4), and extraction anode (12) have respective sets of multiple apertures (30) which are mutually aligned to yield a high perveance beam; the cathode, grid, and anode are curved to geometrically focus the beam, and a beam with a circular cross-section is generated.
Abstract:
A plasma wave tube and associated operating method are described in which a pair of cold-cathode electron beam generators discharge counterpropagating electron beams (2, 4) into an ionizable gas, preferably hydrogen or a noble gas, within a waveguide housing (6). A voltage within the approximate range of 4-20 kV relative to the waveguide housing is applied to the cathodes (14, 16) to produce electron beams with current densities of at least about 1 amp/cm2. The beams form a plasma (8) within the gas and couple with the plasma to produce electron plasma waves, which are non-linearly coupled to radiate electromagnetic energy in the microwave to mm-wave region. A magnetic field (Bo) is established within the waveguide between the cathodes to confine the plasma, and to control the beam discharge impedance. The gas pressure is held within the approximate range of 1-100 mTorr, preferably about 10-30 mTorr, to damp plasma instabilities and sustain the beam voltages, while the magnetic field is within the approximate range of 100-500 Gauss. A very rapid frequency slewing or chirping is achieved with a relatively high magnetic field that reduces the discharge impedance to the lower end of the permissible range. Frequency-stabilized operation is achieved with a lower magnetic field that increases the discharge impedance so that the beam current changes very slowly with time.
Abstract:
A plasma wave tube and associated operating method are described in which a pair of cold-cathode electron beam generators discharge counterpropagating electron beams (2, 4) into an ionizable gas, preferably hydrogen or a noble gas, within a waveguide housing (6). A voltage within the approximate range of 4-20 kV relative to the waveguide housing is applied to the cathodes (14, 16) to produce electron beams with current densities of at least about 1 amp/cm2. The beams form a plasma (8) within the gas and couple with the plasma to produce electron plasma waves, which are non-linearly coupled to radiate electromagnetic energy in the microwave to mm-wave region. A magnetic field (Bo) is established within the waveguide between the cathodes to confine the plasma, and to control the beam discharge impedance. The gas pressure is held within the approximate range of 1-100 mTorr, preferably about 10-30 mTorr, to damp plasma instabilities and sustain the beam voltages, while the magnetic field is within the approximate range of 100-500 Gauss. A very rapid frequency slewing or chirping is achieved with a relatively high magnetic field that reduces the discharge impedance to the lower end of the permissible range. Frequency-stabilized operation is achieved with a lower magnetic field that increases the discharge impedance so that the beam current changes very slowly with time.
Abstract:
A plasma wave tube is described in which a pair of counterpropagating electron beams (6, 8) are injected into a waveguide housing (2) in which a plasma is formed, preferably by an array of fine wire anodes (4). The electron beams couple with the plasma to produce electron plasma waves, which radiate electromagnetic energy for beam voltages and currents above established threshold levels. A rapid control over output frequency is achieved by controlling the plasma discharge current, while the output power can be controlled by controlling the voltage and/or current levels of the electron beams.
Abstract:
Est décrit un tube à ondes plasmiques dans lequel une paire de faisceaux d'électrons (6, 8) se propageant dans des sens contraires sont injectés dans une cage de guide d'ondes (2) dans laquelle un plasma est formé, de préférence par un réseau d'anodes en fils fins (4). Les faisceaux d'électrons se couplent avec le plasma pour produire des ondes plasmiques électroniques, lesquelles rayonnent une énergie électromagnétique pour des tensions et des courants de faisceaux supérieurs aux niveaux de seuil établis. Une rapide modulation de la fréquence de sortie est réalisée par modulation du courant de décharge de plasma, tandis que la puissance de sortie peut être modulée par modulation des niveaux de tension et/ou de courant des faisceaux d'électrons.
Abstract:
Energie is converted by launching a bundle of discrete self-contained electrons. The bundle is guided along a path defined by a channel (584) in a dielectric (582). Energy from the bundle is transferred by a charge transfer mechanism to a slow wave electrical conductor (588) while the bundle is guided along the path. Energy transferred to the slow wave conductor from the bundle is coupled to a load (590).
Abstract:
A plasma wave tube is described in which a pair of counterpropagating electron beams (6, 8) are injected into a waveguide housing (2) in which a plasma is formed, preferably by an array of fine wire anodes (4). The electron beams couple with the plasma to produce electron plasma waves, which radiate electromagnetic energy for beam voltages and currents above established threshold levels. A rapid control over output frequency is achieved by controlling the plasma discharge current, while the output power can be controlled by controlling the voltage and/or current levels of the electron beams.
Abstract:
A plasma wave tube is described in which a pair of counterpropagating electron beams are injected into a waveguide housing in which a plasma is formed, prefeferably by an array of fine wire anodes. The electron beams couple with the plasma to produce electron plasma waves, which radiate electromagnetic energy for beam voltages and currents above established threshold levels. A rapid control over output frequency is achieved by controlling the plasma discharge current, while the output power can be controlled by controlling the voltage and/or current levels of the electron beams.