US3859552A

US3859552A - Electron beam generator for transit-time electron discharge tubes

Info

Publication number: US3859552A
Application number: US331809A
Authority: US
Inventors: Richard Hechtel
Original assignee: Siemens AG
Current assignee: Siemens AG
Priority date: 1972-03-02
Filing date: 1973-02-12
Publication date: 1975-01-07
Anticipated expiration: 1992-01-07
Also published as: DE2210160B2; DE2210160C3; FR2173919B1; FR2173919A1; IT972629B; SE386005B; DE2210160A1; GB1357469A

Abstract

An electron beam generator for transit-time tubes employs a cathode for emission of an electron beam, a control grid spaced from the cathode, and an anode, the control grid having a section which surrounds a central portion of the emissive area of the cathode whereby emission from the area surrounded by the central portion can be controlled independently of the emission from the central portion.

Description

United States Patent 1191 Hechtel Jan. 7, 1975 1 ELECTRON BEAM GENERATOR FOR 3,121,181 2/1964 Van Barneveld et a1. 313/69 R R S ELECTRON DISCHARGE 3,132,275 5/1964 Merdinian 313/338 TUBES 3,377,492 4/1968 Oess 313/348 3,484,645 12/1969 Drees 313/348 [75] Inventor: Richard Hechtel, Redwood City, 3,500,110 3/1970 Winsor 3l5/3.5 Calif. 3,558,967 1/1971 Miriam 315/35 3,651,360 3/1972 Sommeria 313/82 [73] Ass1gnee: Siemens Aktiengesellschaft, Berlin,

Germany Primary Examiner-James W. Lawrence [22] Filed: Feb. 12, 1973 Assistant Examiner-Saxfield Chatmon, Jr.

Attorney, Agent, or Firm-Hi1l, Gross, Simpson, Van [21] Appl' 331309 Santen, Steadman, Chiara & Simpson [30] Foreign Application Priorlty Data ABSTRACT Mar. 2, 1972 Germany 2210160 An electron beam generator for transit-time tubes em- '[52] US. Cl ..313/449, 313/348, 313/457, ploys a cathode for emission of an electron beam, a 313/460; 315/3.6 control grid spaced from the cathode, and an anode, [51] Int; C11 .1. 1161129700 the Control g having a Section which Surrounds a [581 Field 01 Search 313/82, 69,338, 348; central portion of h mi r v of he h e 315/35, 35 whereby emission from the area surrounded by the central portion can be controlled independently of the [56] Refer n e Ci d emission from the central portion.

UNITED STATES PATENTS 7 Claims, 9 Drawing Figures 2,694,159 11/1954 Pierce 313/338 PATENTEU JAN 71975 SHEET 10F 3 PATENTEU 7i975 SHEET 2 [IF 3 ELECTRON BEAM GENERATOR FOR" I TRANSIT-TIME ELECTRON DISCHARGE TUBES.

BACKGROUND OF THE INVENTION 1. Field of the Invention Y I The present invention relates to electronbeamv generators, and more particularly to electron beam genera tors for transit time electronldischarge tubes having a cathode for emission of an electron beam, a control grid spaced from the cathode, and'an anode, and which features independent control of emission of an area surrounding the central portion of the cathode with referent power levels. The two-power levels may differ" from one another, for example by a factor of or 10. The lower power level is used'in normal operation for reasons of power economy, and thehigher power level is only used under 3ertain tir'cumstances, 5 .g.' Zn the event of interference from another transmittent In the case of a transit time tube, this type of power regulation can only be effectedthrough a-cont'rol of the electron beam current. A change in the beam voltage is unsuitable for this purpose,because-of-thephasere lationship which must-be mai'nt'aine dgbe'tween the elec-;

tron beam and the signal beam amplifierqThe nece'sfl sary adjustment of the beam vcurrent-.in an jelectron I beam generator is a very difficult problem, and one-- which has not thus far been satisfactorily1solyed..- At-} tempts to adjustthe beanicurrent'by varyingthe focus v ing or modulating electrode voltage or the anode 'v'olt-t age only produce undesirable modificationsin the elec tron-optical behavior of the-electron beam generator,

't b t' d't dbwu The same holds true if he cam curren IS a 1118 v y and 2 thermal-cathode area.

varying the voltage on a control electrode.

SUMMARY OF THEINVENTION I An object of the invention is to provide an electron-- following relationship holds "where F1 is'the arjea 'covered by the inner grid section grids, one of which is a so-called shadow grid which absorbs no current'are only a comparatively small amount of current; A 'double grid of this kind is described, for example, in German published application 1,764,860. The invention can be'practiced by splitting the area of jfthejcontrol grid andelectrically insulating the two partial areas from each other. In this manner, power level control of transit time tubes can be carried out by controlof the emission from the cathode of the electron beam generator, more specifically by applying potentials of different polarity to that of the cathode to the section of the. control grid vwhich surrounds the central area. This kind of current control requires only relatively small voltagechanges in order to switch the beam current from one value to another and is free ofany undesirable secondary electron-optical effects. It can be applied both in electron beam generators of the continuous-rating type, and also to pulsed electron beam generators.

In a preferred embodiment of the invention, for pulse operation, the electron beam generator has a control grid which comprises a first partial grid section surro'unding and mechanically-and electrically isolated from a second partial grid section which covers the central area of the emissive surface of the cathode.

An electron beam generator of this form, in which ".the inner partial grid section is 'circularand the outer section is'ring-shaped, has the following properties. The beam current I, is determined, in accordance with the applied potentials, by the relative areas'of the' two ,partial grid sections. If I, is the smaller of the two currents and l -is the larger of the twocurrents, then the 1 "As far as'the beam current I is concerned, three differentoperating conditionslcan be distinguished.

beam generator, in particular for O-type transit time] tubes, by which a transit time tube canbe operated at,

two different power levels'without. the production of unwanted disturbing electron-optical influencesq' The invention resides in the provision of an electron-- beam generator for transit timeitubes, comprising a v cathode for the emission ofanelectron beam, a control grid spaced from the cathode,'and an anode, wherein the control grid comprises"asectionlwhich' surroundsa" central portion of the emissivearea of the cathod'ef whereby the emission from the areaof the cathode sur'-; I rounding the central portion can be controlled independently of the emission from-the central portion f The section of the control grid which'surrounds the central portion of the emissive area of the cathode is not necessarily an annular'ring, since the electron beam may not have a circulancross section, and may, for excontrol grid or grids,

' tron beam generatorhas axial symmetry, in which 'the The inner partial grid section is positive and the outer partial grid section. is negative with respect to thecath ode; The voltage on the inner control grid section, in 1 relationto the cathode, is'about l/25th to l/50th of the anod e voltage. The voltage on the external partial grid section is of the same order magnitude, but of negative p ol'arity."

1 Both-partial grid sectionsare positive with respect to I the cathode. The voltages'applied to these grid sections are about l/25thtopl/50th of the, anode voltage.

,Bothof the partial grid sections are negativewith respect to the cathode. The voltage difference between the cathode and the partial grid sections is of the order of magnitude of l/SOth to 1/l00th of the anodecathode voltage. v

in a preferred embodiment of the invention the elecjjfijrst; partial grid section is in the form of an annular ring surrounding the second partial grid section which has a circular periphery. Consequently, and in accordance with equation 1, the following approximation holds true, provided that the radius of curvature of the cathode surface is not too small:

where D is the diameter of the inner partial grid section and D is the diameter of the cathode. From this relationship we obtained:

where d and d are the diameter of the electron beams corresponding to the currents I and 1 respectively. This equation (3) can also be written in the form Because the magnetic field required to focus a circular beam of a diameter d and current I is proportional to the ratio I/d, the same magnetic field can be employed for focusing beam currents I and 1 Therefore, in both cases a beam of constant diameter is obtained without necessity for electron-optical correction.

In another embodiment of the invention, the control grid has only one section and surrounds the central portion of the emissive area of the cathode which projects toward the anode so as to be flush with the surface of the control grid. This embodiment is particularly suitable for a continuous-rating electron beam generator. The electron beam generator behaves in a manner similar to that of one using an inner partial grid section, as far as two possible beam currents are concerned, but in order to completely block the beam current, the anode potential must be changed rather than the cathode potential.

BRIEF DESCRIPTION OF THE DRAWINGS Other objects, features and advantages of the invention, its organization, construction and operation will be best understood from the following detailed description of embodiments of the invention taken in conjunction with the accompanying drawings, on which:

FIG. 1 is a longitudinal sectional view of a first embodiment of an electron beam generator;

FIG. 2 is a plan view of the inner grid of the apparatus illustrated in FIG. 1;

- FIG. 3 is a plan view of the outer grid of the apparatus illustrated in FIG. 1;

FIG. 4 is a longitudinal sectional view of a second embodiment of an electron beam generator;

FIG. 5 is a plan view of the outer partial grid of the embodiment illustrated in FIG. 4;

FIG. 6 is a longitudinal sectional view of a third embodiment of an electron beam generator;

FIG. 7 is a plan view of the inner partial grid structure of the control grid of the apparatus illustrated in FIG.

FIG. 8 is a plan view of the outer partial grid of the control grid of the apparatus illustrated in FIG. 6; and

FIG. 9 is a plan view of the shadow grid of the apparatus illustrated in FIG. 6.

DESCRIPTION OF THE PREFERRED EMBODIMENTS grids of the control grid, with respect to the cathode, have been omitted from the drawings for reasons of simplicity and clarity.

Referring to FIG. 1, an axially-symmetrical electron beam generator of a transit time tube is illustrated as having a cathode 1, a focusing electrode 3 and a control grid 2 which comprises an inner partial grid 15 and an outer partial grid 18. The control grid 2 and the emissive area of the cathode l are of concave form and have a common center of curvature. The mechanical and electrical isolation of the two partial grids from one another and from the other components which carry potentials is provided by means of a carrier plate 7 for the inner partial grid 15 and a carrier plate 8 for the outer partial grid 18 with

openings

27 and 28 for receiving three supporting

bolts

23, 24, 25 of the focusing or modulating cylindrical electrode 3 and are in different planes and lead to the tube wall 11. In addition. the tube wall 11 is interrupted at appropriate points by insulating ceramic cylinders 9. The supporting bolts, of which the

bolts

23 and 24 are illustrated in FIG. 1, rest upon a support cylinder 26. The cathode itself is conventional and comprises a heating element 4 having a current supply lead 22 embedded in a ceramic disc 21, the mounting cylinder 26 resting on a base plate 10, and a plurality of radiation shields 6.

FIG. 2 is a plan viewof the inner partial grid 15 together with its mounting apparatus. The partial grid 15 comprises a number of radially-disposed spokes 13 connected together by a circular ring 12, a number of the spokes 13 being extended beyond the ring 12 as supporting stays 14. The supporting stays 14 terminate in a first carrier plate 7 which has good thermal conductivity. The openings 27 are provided for the passage of the supporting

bolts

23, 24, 25 of the focusing electrode 3.

FIG. 3 is a plan view of the outer partial grid 18 and its mounting apparatus. The partial grid 18 also comprises a number of radially disposed spokes 16 attached at their inner ends to a circular ring 17 and whose outer ends terminate in a second carrier plate 8 having good thermal conductivity. The partial grid 18 is provided with a plurality of openings 32 for receiving the supporting stay 14 of the inner partial grid 15. The openings 28 in the carrier plate 18 are provide for the passage of the supporting

bolts

23, 24, 25.

In the embodiment of the invention illustrated in FIG. 4, which also has an axially-symmetrical electron beam generator, there is no inner partial grid. In order to avoid unwanted electron-optical effects, a central area 19 of the emissive surface of the cathode. more specifically the area not covered by the ring-shaped outer partial grid 18, projects toward the anode so as to be flush with the surface of the control grid 18. Between the control grid 18 and the cathode 1 there is provided a shadow grid 20 which is supported by the support cylinder 26 of the focusing electrode 3 and which is at cathode potential when the electron beam generator is operating. This double grid structure and the emissive area of the cathode l are curved and the curve surfaces have a common center of curvature. As viewed from the center of curvature, the grid elements of the control grid and the shadow grid are in alignment. A focusing anode 30, which has an appropriate electron-optical shape, draws an electron current I, when the control grid 2 has a negative potential with respect to the cathode 1 applied thereto, and draws an electron current I from the cathode surface if the potential is positive. All of the other designed features correspond to those illustrated in FIG. 1. The use of this embodiment of the invention is recommended if the transit time tube is operating on a continuous-rating basis.

Referring to FIG. 5, the outer partial grid 18 of the apparatus illustrated in FIG. 4 is shown in greater detail. The grid elements comprise a plurality of radial spokes 16 which, as in the outer partial grid illustrated in FIG. 3, terminate in the carrier plate 8 having the openings 28 for receiving the

bolts

23, 24, 25.

FIG. 6 is a schematic longitudinal sectional view of the central part of a third embodiment of an electron beam generator which is primarily confined to the cathode surface and the control grid structure. The electron beam generator in this embodiment is again axially symmetrical and employs a double grid (control grid and shadow grid) the surfaces of which and the cathode surface have a common center of curvature. As viewed from the center curvature, the control grid and the shadow grid elements are in alignment. In this schematic illustration, the beam current boundaries have been illustrated by broken lines to correspond to the two different power levels of the tube, the boundary a representing the partial current I, and the boundary b representing the full current I FIGS. 7, 8 and 9 respectively illustrate in plan views the outer partial grid 18, the inner partial grid and the shadow grid of the apparatus illustrated in FIG. 6. In this embodiment the two partial grids of the control grid are formed such that the shadow grid, while in full alignment, can take the form ofa single mechanical structure which is therefore relatively simple to manufacture. All of the grids comprise predominately ringshaped elements with only a few radial spokes. If the shadow grid is placed at cathode potential and the two partial grids at a moderately high positive potential with respect to the cathode (l/lOth to l/lOOth of the anode voltage), then the current drawn by the partial grids is negligible. Typical values are between 0.01 and 0.1 percent of the total cathode current. The rules hereinbefore listed apply to the three operating conditiOnS (I0, [1,

The invention is not restricted to the embodiments illustrated. For example, the electron beam generator need not be axially-symmetrical, but can have a form which is suitable for the production of flat ribbon type beams. Moreover, the invention can be applied in a corresponding manner if the transit time tubes are to be operated not merely in two, but in several operating conditions.

Many other changes and modifications of my invention may become apparent to those skilled in the art without departing from the spirit and scope of the invention. I therefore intend to include within the patent warranted hereon all such changes and modifications as may reasonably and properly be included within the scope of my contribution to the art.

I claim:

1. An electron beam generator for transit time tubes with single beam operation at more than one power level and different beam cross sections corresponding to respective power levels and current intensities, comprising: a cathode for the emission of a single beam; a control grid spaced from said cathode; and an anode for receiving the electron beam, said control grid comprising a section which surrounds a central portion of the emissive area of said cathode for selectively receiving control potential for either blocking or permitting emission from the area of the cathode surrounding the central portion independently of the emission from the central portion to provide single beam operation with or without emission from said surrounding portion.

2. An electron beam generator, as claimed in claim 1, wherein said control grid comprises a first partial grid section and a second partial grid section, said first partial grid section surrounding and mechanically and electrically isolated from said second partial grid section, said second partial grid section covering the central area of the emissive surface of said cathode.

3. An electron beam generator for transit time tubes which operate at more than one power level, comprising: a cathode for the emission of an electron beam; a control grid spaced from said cathode; and an anode for receiving the electron beam, said control grid comprising a section which surrounds a central portion of the emissive area of said cathode for selectively receiving control potential for controlling the emission from the area of the cathode surrounding the central portion independently of the emission from the central portion, said control grid comprising a first partial grid section and a second partial grid section, said first partial grid section surrounding and mechanically and electrically isolated from said second partial grid section, said section partial grid section covering the central area of the emissive surface of said cathode, wherein said cathode is an axially-symmetrical cathode, wherein said second partial grid section comprises a plurality of radiallydisposed spokes, a circular ring connecting said plurality of radially disposed spokes together, some of said spokes extending beyond said ring as supporting stays, a first carrier plate for said second partial grid section, said supporting stays terminating in said first carrier plate, said first carrier plate having good thermal conductivity, said first partial grid section comprising a plurality of radially disposed spokes, a circular ring connected to the inner ends of the last-mentioned spokes, and a second carrier plate having good thermal conductivity and connected to the outer ends of the last-mentioned radially disposed spokes, said first partial grid section including means defining openings to accommodate said supporting stays of said second partial grid section, and said two carrier plates disposed in different planes.

4. An electron beam generator, as claimed in claim 1, wherein said central portion of the emissive area of said cathode projects towards said anode and lies flush with the surface of said control grid section which surrounds said central portion of the emissive area of said cathode.

5. An electron beam generator, as claimed in claim 1, wherein the emissive surface of said cathode and said control grid surface are concave and have a common center of curvature.

6. An electron beam generator, as claimed in claim 5, comprising a shadow grid disposed between said control grid and said cathode for operation at cathode potential, said shadow grid including grid elements which are aligned with those of said control grid as viewed from said cathode or from said common center of curvature.

7. An electron beam generator, as claimed in claim 1, comprising a shadow grid disposed between said control grid and said cathode for operation at cathode potential, said shadow grid including grid elements which are aligned with those of said control grid.

Claims

3. An electron beam generator for transit time tubes which operate at more than one power level, comprising: a cathode for the emission of an electron beam; a control grid spaced from said cathode; and an anode for receiving the electron beam, said control grid comprising a section which surrounds a central portion of the emissive area of said cathode for selectively receiving control potential for controlling the emission from the area of the cathode surrounding the central portion independently of the emission from the central portion, said control grid comprising a first partial grid section and a second partial grid section, said first partial grid section surrounding and mechanically and electrically isolated from said second partial grid section, said section partial grid section covering the central area of the emissive surface of said cathode, wherein said cathode is an axially-symmetrical cathode, wherein said second partial grid section comprises a plurality of radially-disposed spokes, a circular ring connecting said plurality of radially disposed spokes together, some of said spokes extending beyond said ring as supporting stays, a first carrier plate for said second partial grid section, said supporting stays terminating in said first carrier plate, said first carrier plate having good thermal conductivity, said first partial grid section comprising a plurality of radially disposed spokes, a circular ring connected to the inner ends of the last-mentioned spokes, and a second carrier plate having good thermal conductivity and connected to the outer ends of the last-mentioned radially disposed spokes, said first partial grid section including means defining openings to accommodate said supporting stays of said second partial grid section, and said two carrier plates disposed in different planes.