Active dielectric waveguide amplifier or oscillator using a high density charged particle beam

Claim 2

An RF slow wave particle beam amplifier device comprising: an evacuated waveguide structure included within an envelope, said waveguide structure having an internal cross sectional dimension which exceeds five times the wavelength of a predetermined RF frequency of a wave propagated therethrough, including a coaxial RF input window and a coaxial RF output window for providing entry and exit of a wave to and from said envelope, the waveguide structure comprising a hollow cylindrical, metal structure with a smooth inner wall; thermionic cathode means for generating and projecting a relatively high density electron particle beam providing an effective dielectric constant through said waveguide structure to provide an active, dielectric medium; means for providing an axial magnetic field through said waveguide structure for focusing, confining and causing rotation of the particles of said beam in said waveguide structure at a cyclotron frequency w c which is expressed by the equation: w.sub.c =hB.sub.O where h is the charge to mass ratio of said beam and B O is the magnetic flux density, including means for adjusting B O and h for shaping the beam geometry; means for generating and launching an elliptically polarized RF wave of predetermined millimeter waveband frequency onto said high density beam whereupon said active dielectric medium operates as a waveguide to guide said RF wave and transfer energy to said wave as the RF wave propagates on said beam when the drift velocity of said beam is substantially the same as or greater than the phase velocity of said RF wave; wherein the effective relative dielectric constant e r of said beam is expressed in the form of a diagonal matrix as: ##EQU9## where w p is the beam frequency, w c is the cyclotron frequency, w is the frequency of the RF wave, and W D is the Doppler shifted frequency of the RF wave according to the expression: ##EQU10## where u o is the drift velocity of the beam and v is the phase velocity of the wave in the beam; means for controlling the drift velocity of said particle beam in said waveguide structure by means of d.c. fed electrode; collector means for collecting said beam downstream at opposite end from said generating and projecting means; and means for receiving said RF wave emerging from said beam following propagation thereon.

Claim 3

The device as defined by claim 1 wherein said means for generating and projecting said beam provides at least one region which varies in density along its length.

Claim 4

The device as defined by claim 2 wherein said region of varying density comprises a region of increasing density where said RF wave is launched onto said high density beam.

Claim 5

The device as defined by claim 3 and additionally including a region of varying density going from a region of relatively high density to a region of less density where said RF wave emerges from said beam.

Claim 6

The device as defined by claim 1 and additionally including means for providing another magnetic field through said waveguide structure and comprising an energized electrical conductor axially located with respect to said waveguide structure.

Claim 7

The device as defined by claim 1 wherein said high density beam is located substantially along the central longitudinal axis of said hollow waveguide structure.

Claim 8

The device as defined by claim 1 wherein said beam is generally cylindrical in cross section.

Claim 9

The device as defined by claim 7 wherein said generally cylindrical cross sectional beam comprises a hollow beam of electrons.

Claim 10

The device as defined by claim 7 wherein said generally cylindrical beam comprises a substantially solid beam of electrons.

Claim 11

The device as defined by claim 9 and wherein said waveguide structure also acts as an envelope for said device.

Claim 12

The device as defined by claim 10 wherein said means for launching and receiving said RF wave are located in said waveguide structure.

Claim 13

The device of claim 1 wherein the said predetermined wave frequency is in the infrared frequency band.

Claim 14

The device of claim 1 wherein the said predetermined wave frequency is in the optical frequency band.

Claim 15

The device of claim 1 wherein said predetermined wave frequency is in the microwave frequency band.

Claim 16

The device of claim 1 wherein the said device is operated as a particle beam oscillator device.

Claim 17

An RF slow wave particle beam amplifier device comprising: an evacuated waveguide structure included within an envelope said waveguide structure having internal cross sectional dimension which exceeds five times the wavelength of a predetermined RF frequency of a wave propagated therethrough, including a coaxial RF input window and a coaxial RF output window for providing entry and exit of said wave to and from said envelope, the waveguide structure comprising a hollow cylindrical, metal structure with a smooth inner wall; thermionic cathode means for generating and projecting a relatively high density electron particle beam providing an effective dielectric constant through said waveguide structure to provide an active, dielectric medium; means for providing an axial magnetic field through said waveguide structure for focusing, confining and causing rotation of the particles of said beam in said waveguide structure at a cyclotron frequency w c which is expressed by the equation: w.sub.c =hB.sub.O where h is the charge to mass ratio of said beam and B O is the magnetic flux density, including means for adjusting B O and h for shaping the beam geometry; means for generating and launching an elliptically polarized RF wave of predetermined millimeter wave band frequency onto said high density beam whereupon said active dielectric medium operates as a waveguide to guide said RF wave and transfer energy to said wave as the RF wave propagates on said beam, when the drift velocity of said beam is substantially the same as or greater than the phase velocity of said RF wave; wherein the effective relative dielectric constant e r of said beam is expressed by the equation: ##EQU11## where w p is the beam frequency, w c is the cyclotron frequency and w is the frequency of the RF wave, wherein the effective, relative permeability u r of said beam is equal in magnitude to the relative permittivity or dielectric constant e r , wherein said RF wave propagates with a phase velocity v which is bounded by the equation: v>c/e.sub.r where c is the velocity of light in a vacuum, means for controlling the drift velocity of said particle beam in said waveguide structure by means of d.c. fed electrodes; collector means for collecting said beam downstream at opposite end from said generating and projecting means; and means for receiving said RF wave emerging from said beam following propagation thereon.

Claim 18

An RF slow wave particle beam amplifier device comprising: an evacuated waveguide structure included within an envelope said waveguide structure having internal cross sectional dimension which exceeds five times the wavelength of a predetermined RF frequency of a wave propagated therethrough, including a coaxial RF input window and a coaxial RF output window for providing entry and exit of said wave to and from said envelope, the waveguide structure comprising a hollow cylindrical, metal structure with a smooth inner wall; thermionic cathode means for generating and projecting a relatively high density electron particle beam providing an effective dielectric constant through said waveguide structure to provide an active, dielectric medium; means for providing an axial magnetic field through said waveguide structure for focusing, confining and causing rotation of the particles of said beam in said waveguide structure at a cyclotron frequency w c which is expressed by the equation: w.sub.c =hB.sub.O where h is the charge to mass ratio of said beam and B O is the magnetic flux density, including means for adjusting B O and h for shaping the beam geometry; means for generating and launching an elliptically polarized RF wave of predetermined millimeter wave band frequency onto said high density beam whereupon said active dielectric medium operates as a waveguide to guide said RF wave and transfer energy to said wave as the RF wave propagates on said beam, when the drift velocity of said beam is substantially the same as or greater than the phase velocity of said RF wave; wherein the effective relative dielectric constant e r of said beam is expressed by the equation: ##EQU11## where w p is the beam frequency, w c is the cyclotron frequency and w is the frequency of the RF wave, wherein the effective, relative permeability u r of said beam is equal in magnitude to the relative permittivity or dielectric constant e r , wherein said RF wave propagates with a phase velocity v which is bounded by the equation: v>c/e.sub.r where c is the velocity of light in a vacuum, means for controlling the drift velocity of said particle beam in said waveguide structure by means of d.c. fed electrodes; collector means for collecting said beam downstream at opposite end from said generating and projecting means; and means for receiving said RF wave emerging from said beam following propagation thereon.