Gyromagnetron amplifier

• US 4,550,271 A
• Filed: 06/23/1983
• Issued: 10/29/1985
• Est. Priority Date: 06/23/1983
• Status: Expired due to Fees

• Current Assignee: the united states of america as represented by the secretary of the navy
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Lau, Yue-Ying, Barnett, Larry R.
• Primary Examiner(s): Chatmon, Saxfield
• Application Number:
  US06/507,258
• Time in Patent Office: 859 Days
• Field of Search: 372/2, 315/3, 315/4, 315/5, 315/5.13, 315/39, 315/39.3
• US Class Current: 315/4
• CPC Class Codes: H01J 25/025 with an electron stream following a helical path

Abstract

A gyromagnetron amplifier for radiation at millimeter wavelengths comprising a tapered waveguide tube with longitudinally running vanes in the walls of the tube with the number of vanes chosen to coincide with a desired cyclotron harmonic frequency to be amplified. A beam of spiralling mildly relativistic electrons with an energy of 100 keV or less is directed into the small end of the tapered waveguide tube. A tapered axial magnetic field is set up within the waveguide tube with a low value appropriate to the amplification of a cyclotron harmonic frequency. An electromagnetic wave to be amplified is launched into the waveguide tube to co-propagate and be amplified by the spiralling electron beam. This device is characterized by a wide bandwidth, a low operating magnetic field, a relatively low operating beam voltage, with high power, and the capability of continuous wave operation.

Claims

1. A method for efficiently amplifying radiation at millimeter wavelengths in a gyromagnetron waveguide tube comprising the steps of:

choosing a waveguide tube with longitudinally running vanes in the walls of the tube, with the number of vanes in the tube chosen to coincide with the number of a desired cyclotron harmonic to be amplified, and wherein the dimensions for the tube cross-section are chosen so that the desired cyclotron harmonic frequency is approximately equal to the cut-off frequency of a fundamental mode of the waveguide tube;

generating a magnetic field within said waveguide tube in a direction approximately parallel to the axis of said waveguide tube with a value appropriate to the cyclotron harmonic frequency chosen for amplification;

generating and directing a beam of spiralling mildly relativistic electrons with an energy of 100 keV or less into said waveguide tube to propagate longitudinally therein and to interact with the fringe electric fields set up between the vanes; and

launching electromagnetic energy to be amplified into said waveguide tube to co-propagate with the spiralling electron beam.

2. A method as defined in claim 1, wherein said waveguide tube choosing step includes the step of choosing a waveguide tube that is tapered longitudinally from a first end of small cross-section to a second end of large cross-section;

and

wherein said step of generating a magnetic field comprises the step of generating a tapered magnetic field following the taper of said waveguide tube.

3. A method as defined in claim 2, wherein said electron beam generating and directing step comprises the step of introducing the beam of electrons at the small first end of the waveguide tube to propagate longitudinally within the waveguide tube toward the larger second end.

4. A method as defined in claim 3, wherein said waveguide tube choosing step comprises the step of choosing a tube with six longitudinal vanes and wherein the dimensions of the tube are chosen so that the sixth cyclotron harmonic frequency is approximately equal to the cut-off frequency of a fundamental mode of the waveguide tube.

5. A method as defined in claim 1, wherein the number of vanes is greater than two.

6. A method as defined in claim 1, wherein the step of launching electromagnetic energy in said tube involves the use of a circulator for injecting the electromagnetic energy to be amplified into a larger second end of said tube to propagate toward a small first end of the tube until this electromagnetic energy is reflected at various points along the tapered waveguide tube.

7. A gyromagnetron amplifier comprising:

a longitudinally tapered waveguide tube which is tapered from a first end to a second end;

said waveguide tube having longitudinally running vanes in the walls thereof, with the number of vanes coinciding with the number of the desired cyclotron harmonic to be efficiently amplified, and wherein the dimensions for the tube are chosen so that the desired cyclotron harmonic frequency is approximately equal to the cut-off frequency of a fundamental mode of the waveguide tube;

means for generating a tapered magnetic field within said waveguide tube in a direction approximately parallel to the axis of said waveguide tube with a value appropriate to the cyclotron harmonic frequency chosen for amplification;

means for generating and directing a beam of spiralling mildly relativistic electrons with an energy of 100 keV or less into the small first end of said waveguide tube to propagate longitudinally therein and to interact with the fringe electric fields set up between said vanes; and

means for launching input electromagnetic energy into said waveguide tube to co-propagate with the spiralling electron beam to be efficiently amplified thereby.

8. A gyromagnetron amplifier as defined in claim 7, wherein said waveguide tube is circular in cross-section.

9. A gyromagnetron amplifier as defined in claim 7, wherein said waveguide tube has six longitudinally running vanes therein, and wherein the dimensions of the tubes are such that the sixth cyclotron harmonic frequency is approximately equal to the cut-off frequency of a fundamental mode of the waveguide tube.

10. A gyromagnetron amplifier as defined by claim 7, wherein said first end has a small cross-section and said second end has a large cross-section.

11. A gyromagnetron amplifier as defined in claim 10, wherein said launching means comprises a circulator for injecting the electromagnetic energy to be amplified into the larger second end of said waveguide tube to propagate toward said small first end until this electromagnetic energy are reflected at various points along the tapered waveguide tube for various frequency components.

12. A gyromagnetron amplifier as defined by claim 7, wherein the number of vanes is greater than two.