Gyrotron device
AssigneeThorn EMI-Varian Limited
InventorDudley Perring
Life of this patent
Estimating the term…
Abstract
A gyrotron device e.g. a gyrotron oscillator (FIG. 3) or a gyrotron amplifier (FIG. 4) in which a circular waveguide is dimensioned to operate in a transverse electric mode (TE.sub.01) as an interaction region at an RF frequency .omega..sub.o. An injection means directs a beam of electrons, in the form of a hollow cone, into the waveguide and a solenoid generates a magnetic field, extending axially along the waveguide, which causes the electrons in the beam to gyrate at the cyclotron frequency .omega..sub.c. A solenoid coil, mounted on the side of the injection means remote from the solenoid, is used to modify the magnetic field prevailing in the vicinity of the hollow cone, to cause the field lines to extend along the electron beam.
Claims7
A gyrotron device comprising,
- a waveguide, circular in cross-section, which is dimensioned to accommodate a predetermined transverse electric mode and to operate as an interaction region at a predetermined radio frequency,
- means for generating a magnetic field having field lines which, in said interaction region, are parallel to the axis of the waveguide and is of a strength sufficient to cause electrons, introduced into the interaction region, to gyrate at a predetermined cyclotron frequency (.omega..sub.c),
- injection means for introducing electrons into said interaction region, the injection means comprising a thermionic cathode for producing a beam of electrons in the form of a hollow cone which is centred on said axis and intersects said parallel field lines at a preset angle, and wherein each electron follows a linear trajectory from said cathode to the interaction region said angle being chosen to establish a preset component of velocity for said beam perpendicular to the axis of the waveguide, sufficient to cause electrons in the beam to gyrate as a result of their interaction with the parallel field lines at the cyclotron frequency and a preset component of velocity parallel to the axis of the waveguide sufficient to produce a plurality of cycles of the beam in the waveguide,
- and means for modifying the magnetic field prevailing in the vicinity of the hollow cone to constrain the field lines to run substantially parallel to the electron beam in the form of said hollow cone.
Dependencies are inferred from the claim text.