US2281041A - High frequency electron discharge tube - Google Patents

High frequency electron discharge tube Download PDF

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US2281041A
US2281041A US379559A US37955941A US2281041A US 2281041 A US2281041 A US 2281041A US 379559 A US379559 A US 379559A US 37955941 A US37955941 A US 37955941A US 2281041 A US2281041 A US 2281041A
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anode
grid
tube
electron discharge
high frequency
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US379559A
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Labin Emile
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International Standard Electric Corp
Burnett Wm T IP LLC
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International Standard Electric Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J19/00Details of vacuum tubes of the types covered by group H01J21/00
    • H01J19/28Non-electron-emitting electrodes; Screens
    • H01J19/32Anodes
    • H01J19/34Anodes forming part of the envelope
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2893/00Discharge tubes and lamps
    • H01J2893/0001Electrodes and electrode systems suitable for discharge tubes or lamps
    • H01J2893/0002Construction arrangements of electrode systems
    • H01J2893/0003Anodes forming part of vessel walls

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  • the present invention concerns structure of electron discharge tubes especially designed for operation at high frequencies.
  • the invention provides, according to certain characteristics thereof, arrangements and electrode structures for simple or multiple electron discharge tubes which permit the convenient application of feed connections or output connections in the forward transmission lines of the several electrodes.
  • the invention also provides arrangements for such connections.
  • Figs. 1 and 2 represent two simple electron discharge tube structures incorporating certain features of the invention
  • Fig. 3 shows an end view of these two structures
  • Figs. 4, 5 and 6 represent three embodiments of double electron discharge tubes incorporating certain characteristics of the invention.
  • Fig. 7 schematically represents an arrangement of a multiple tube according to the features ofthe invention.
  • the structure of the electron discharge tube represented in Fig. 1 comprises an envelope in which a vacuum is provided and which is constituted by tubular anode I, closed at one end by a base 2, and an insulation portion 3 of glass, for example, sealed onto widened portion 4 of the anode and joined to a press 5 by a tubulation or inverted annular press 6.
  • Anode l, base 2, widened portion 4, on the one hand, and the portion 3, the presses 5 and 8, on the other hand, may clearly each be formed of a single piece or on the other hand may be independently sealed together.
  • the lead-in connection of the anode consists, as shown, of a. cylinder I pressed upon it in intimate electrical and mechanical contact (for example, pressed on by force and brazed at its ends) which is joined by a conical portion 8 and a cylinder of larger diameter 9.
  • the grid of the tube consists of a grid of spiral wires or squirrel cage or other form around mounting bars such as represented at In. These mounting bars II! are fixed, for example, brazed, onto a piece ll having the form of truncated cone terminated at each side in cylindrical portions.
  • Conducting stems l2 extend to and join onto saidpiece on the opposite side from the active portion ID of the grid, said conducting stems being disp s d along the generatrixcs 0 an imaginary cylinder and serving as supporting connections and lead-out connections which pass through the annular press 6.
  • these stems l2 are fixed on the peripheryofa real conductive cylinder l3 which is coaxial with cylinder [9 of the anode.
  • the diameters of the cylinders 9 and I3 are the same ratio as the diameter of the anode I and the imaginary surface of grid in.
  • the joiningsurfaces Band although shown as truncated cones, are, so far as possible, formed in such manner as to follow the imaginary curves of junction which are theoretically required to preserve the uniform gradient between the structures of the anode and the grid.
  • the cathode structure consists of a filament l4 spirally wound, for example, on an imaginary cylinder coaxial to the cylinders of the grid and anode and supported and fed in known manner by two stems I5 and I6 which pass through the press 5.
  • the two stems l5 and [6 are placed as shown within the inside of a conductive screen I! in such manner as to form a shielded pair coaxial to the connecting cylinders I3 and 9 of the grid and anode.
  • the diameters of this screen I! and of the grids cylinder I 3 are in the same ratio as the diameter of the imaginary cylinders l0 and M of the active parts of the grid and filament.
  • This ratio is preferably provided in such a way as to have a value which is well known in the art of coaxial transmission lines.
  • the feeding of the electron discharge tube circuit is effected by means of a three conductor coaxial line 9, I3, H, as seen in plan view in Fig. 3.
  • an end cap I8 is provided on the grid to play the part of a screen between the grid cathode space of the base 2 of the anode.
  • the cathode and grid electrodes are first assembled in insulating portion 3 of the envelope, while said assembly is mounted. Then when the assembly is mounted in anode I, one can thus determine with precision the value of the capacity between base 2 and theanode and screen l8 of the grid.
  • Fig. 2 The structure represented in Fig. 2 is in general analogous to Fig. 1, especially in so far as the arrangement of the lead-out connections from the electrodes in the form of a three conductor coaxial line is concerned.
  • Fig. 2 The structure represented in Fig. 2 is in general analogous to Fig. 1, especially in so far as the arrangement of the lead-out connections from the electrodes in the form of a three conductor coaxial line is concerned.
  • QW Q ppo w o t e g d are extended arrangement of such a double tube.
  • conductors l5 and I6 supporting and feeding the filament pass through two sleeves 2
  • anode structure different from that of Fig. 1.
  • anode I is open at both ends and is sealed onto a balloon 25 made of glass, for example, and the outside cylinder 1 is extended all around this balloon, as shown at 26, whether it be by an external metalization of the balloon or by a continuous metal envelope or, by a metallic screen or trellis.
  • a balloon 25 made of glass, for example
  • the outside cylinder 1 is extended all around this balloon, as shown at 26, whether it be by an external metalization of the balloon or by a continuous metal envelope or, by a metallic screen or trellis.
  • anode- may be cooledif desired-in any suitable manner, eithernby circulatticn of-rcooling' fluid within a ski-rt which; is pro:- vided for. this; purpose around this; anode, or simply by providing on the surface ofjcylinder 1 little cooling wings.
  • the anode I may, moreover, consist either of ametal plate which is beatenout or shaped in some other-manner or a bar -which;isl hollowed out;so asto contain the other electrodes.
  • FIGs. 1 and 2 show three examples of such structures.
  • the cylindrical anode 21 is open at its two ends and on these ends are sealed insulated balloons 28 and 29 which may, for example, be of glass.
  • a short conductive tube 39 on, the open end of which is sealed insulating balloon 3
  • a grid structure consisting of an elongated cylinder 32 coaxial to anode 21' and supported at its center, by a stem 33, serving as a lead-irr conductor.
  • Stein 33. passes ,coaxially; through sleeve 30 andp'asses out of balloon 3! throu h seal 34, for instance, a.
  • Two coaxial lines may thenbe provided at the two ends of the structure in the manner shown in Figs- 1 and 2 by means of cylinders attached to anode 2'! and extending coaxially with respect to the axis of the complete structure, the other conductor of-these coaxial lines beingconstituted by cylinders forming the screen for the lead-in conductors of the cathodes.
  • a third coaxial line may, if desired, be provided betWeen the anode sleeve 30 and the grid conductor 33 in the same way.
  • a jacket for water or other cooling fluid,- may be provided around the anode. The continuityof. the-gridstructure avoids allvundesirable electron couplings between the ends-of the filaments and the anode.
  • These sleeves 45 and 48 carry sealed on to them insulating balloons 41 and idthrough which pass the lead-in conductors of. grids 4 9 and, 50, by means of seals 5
  • These conductors 49 and 50 may constitute. a parallel wire line.
  • the rest of the structurebeing identical to Fig. 4 will not be described in detail and the, same numerical references are assigned to corresponding elements, as. is the case also in the structure of Fig. 6.
  • a high frequency vacuum tube arrangement comprising a cylindrical anodeforming a part of the envelope, a grid electrode assembly arranged on a cylindrical surface of a given diameter arranged concentrically of said anode, a concentric transmission line externalof said envelope, means interconnecting said outer conductor and said anode, and means interconnecting said inner conductor and said grid, each of said interconnecting means comprising a generally conical tapering member, one of said conical members being disposed within the other of said conical members, whereby a substantially uniform gradient between the anode and the grid structures is obtained.
  • a high frequency tube arrangement according to claim 1 in which the respective radii of each of said members at any given point along the axis of said tube bears substantially the same ratio as the ratio of the respective radii of the conductors of said concentric transmission line.
  • a high frequency tube further comprising a cathode having a cylindrical surface concentrically arranged within said grid electrode assembly and means for energizing said cathode, comprising a shielded conductor pair, the shield of said pair being arranged concentrically within said inner conductor and having substantially the same diametral ratio to said iiuier conductor as said cathode cylinder has to said cylindrical surface.
  • a vacuum tube structure comprising an anode of substantially cylindrical form, glass bulbs sealed at each end of said anode, a tubular grid support mounted concentrically within said anode, a set of grid wires at each end of said tube cooperating with said anode, cathode structures arranged concentrically of said grid wire set and supported by leads through said glass bulbs, a further glass seal substantially at a longitudinal midpoint on the periphery of said anode, and a rod fastened substantially at the center or" said tubular support and extending generally radially of said anode and supported in said further glass seal to maintain said tubular support in position.
  • a vacuum tube structure further comprising cathode energizing leads arranged within said tubular support, said tubular support and said anode being provided with an opening substantially mid-way along their lengths, and means for supplying the filament heating current to said cathode energizing leads extending through said openings.

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Description

April 28, 1942. LABlN HIGH FREQUENCY ELECTRON DISCHARGE TUBE 3 Sheets-Sheet 1 Filed Feb. 19, 1941 FIG},
IN A AA A AAAA AAAAA -vvv-vvvvvv VYYY INVENTOR EM/LE LAB/N April ZS, 1942. E. LABIN HIGH FREQUENCY ELECTRON DIS CHARGE TUBE Filed Feb. 19, 1941 3 Sheets-Sheet 2 2s 29 41 35 52 27 as as I INVENTOH EM/LE LAB/N BY 1 I ATT NEY Patented Apr. 28, 1942 Emile Labin, New York, N. Y., assignor to International Standard Electric Corporation, New York, N. Y., a corporation of Delaware Application February 19, 1941, Serial No. 379,559
6 Claims.
The present invention concerns structure of electron discharge tubes especially designed for operation at high frequencies. In particular the invention provides, according to certain characteristics thereof, arrangements and electrode structures for simple or multiple electron discharge tubes which permit the convenient application of feed connections or output connections in the forward transmission lines of the several electrodes. In addition the invention also provides arrangements for such connections.
The invention will be described in detail in the following description in connection with several illustrative embodiments represented in the attached drawings, wherein Figs. 1 and 2 represent two simple electron discharge tube structures incorporating certain features of the invention;
Fig. 3 shows an end view of these two structures;
Figs. 4, 5 and 6 represent three embodiments of double electron discharge tubes incorporating certain characteristics of the invention; and
Fig. 7 schematically represents an arrangement of a multiple tube according to the features ofthe invention.
The structure of the electron discharge tube represented in Fig. 1 comprises an envelope in which a vacuum is provided and which is constituted by tubular anode I, closed at one end by a base 2, and an insulation portion 3 of glass, for example, sealed onto widened portion 4 of the anode and joined to a press 5 by a tubulation or inverted annular press 6. Anode l, base 2, widened portion 4, on the one hand, and the portion 3, the presses 5 and 8, on the other hand, may clearly each be formed of a single piece or on the other hand may be independently sealed together.
The lead-in connection of the anode consists, as shown, of a. cylinder I pressed upon it in intimate electrical and mechanical contact (for example, pressed on by force and brazed at its ends) which is joined by a conical portion 8 and a cylinder of larger diameter 9.
The grid of the tube consists of a grid of spiral wires or squirrel cage or other form around mounting bars such as represented at In. These mounting bars II! are fixed, for example, brazed, onto a piece ll having the form of truncated cone terminated at each side in cylindrical portions. Conducting stems l2 extend to and join onto saidpiece on the opposite side from the active portion ID of the grid, said conducting stems being disp s d along the generatrixcs 0 an imaginary cylinder and serving as supporting connections and lead-out connections which pass through the annular press 6. On the outside of the tube these stems l2 are fixed on the peripheryofa real conductive cylinder l3 which is coaxial with cylinder [9 of the anode. The diameters of the cylinders 9 and I3 are the same ratio as the diameter of the anode I and the imaginary surface of grid in. The joiningsurfaces Band ,although shown as truncated cones, are, so far as possible, formed in such manner as to follow the imaginary curves of junction which are theoretically required to preserve the uniform gradient between the structures of the anode and the grid.
The cathode structure consists of a filament l4 spirally wound, for example, on an imaginary cylinder coaxial to the cylinders of the grid and anode and supported and fed in known manner by two stems I5 and I6 which pass through the press 5. On the outside of the envelope the two stems l5 and [6 are placed as shown within the inside of a conductive screen I! in such manner as to form a shielded pair coaxial to the connecting cylinders I3 and 9 of the grid and anode. Here, also, the diameters of this screen I! and of the grids cylinder I 3 are in the same ratio as the diameter of the imaginary cylinders l0 and M of the active parts of the grid and filament. This ratio, as well as the previously mentioned one, is preferably provided in such a way as to have a value which is well known in the art of coaxial transmission lines. In this way the feeding of the electron discharge tube circuit is effected by means of a three conductor coaxial line 9, I3, H, as seen in plan view in Fig. 3.
In the embodiment shown, an end cap I8 is provided on the grid to play the part of a screen between the grid cathode space of the base 2 of the anode. With respect to the assembly, the cathode and grid electrodes are first assembled in insulating portion 3 of the envelope, while said assembly is mounted. Then when the assembly is mounted in anode I, one can thus determine with precision the value of the capacity between base 2 and theanode and screen l8 of the grid.
The structure represented in Fig. 2 is in general analogous to Fig. 1, especially in so far as the arrangement of the lead-out connections from the electrodes in the form of a three conductor coaxial line is concerned. In this figure,
the same reference characters as shown in Fig. 1 are applied to the corresponding elements. j.
QW Q ppo w o t e g d are extended arrangement of such a double tube.
and bent in such a way as to extend to and join electrically and mechanically around a metal plate provided with peripheral brim 20 for sealing to insulation portion 3 of the envelope and for electrical and mechanical attachment of the feed cylinder l3. Also, conductors l5 and I6 supporting and feeding the filament pass through two sleeves 2| and 22 of larger diameter which form part of theplate I9 and are sealed in insulating sleeves 23 and 24, which themselves are sealed to the conductive sleeves 2| and 22 extended to such a point as to avoid discharge along the insulation between the connections of grid and cathode.
At the other end of the tubeis shown an anode structure different from that of Fig. 1. In this tube anode I is open at both ends and is sealed onto a balloon 25 made of glass, for example, and the outside cylinder 1 is extended all around this balloon, as shown at 26, whether it be by an external metalization of the balloon or by a continuous metal envelope or, by a metallic screen or trellis. Such an end structure has the advantage compared to that of' Fig. 1, that. the
assembly .of the tube is facilitated. For before sealing the balloon 25 tools. may. be passed through! anode L. The capacity between the screen of gridlfi'and the base 26' of the anode is then not known, but is made very small in consequence of the relatively large spacing between said screen IB and the metallic coating926.
One sees that the section of Fig. 3 can again be consideredas applicable to the structure of Fig. 2, aside from the fact that the press 5 must be replaced by two insulating sleeves. 23 and 24. It is clear that the, anode-may be cooledif desired-in any suitable manner, eithernby circulatticn of-rcooling' fluid within a ski-rt which; is pro:- vided for. this; purpose around this; anode, or simply by providing on the surface ofjcylinder 1 little cooling wings. The anode I, may, moreover, consist either of ametal plate which is beatenout or shaped in some other-manner or a bar -which;isl hollowed out;so asto contain the other electrodes.
In addition,itisjclea-r that in the structures, as well as in those hereafterto be described, additional electrodes, for example, grids, could be added to the tubes-without departing from the In 'thecase where anode l is formedbyasolid bar, hollowed out to contain the other=electrodes-,
there is no need for a drawing to explain the It is sumcient to consider, for example, one of the Figs. 1 and,.2 and to complete it-by a structure which issymmetrical with respect to a plane perpendicular to the longitudinal axispassingnear the end'of the anode. However, such a structure will necessitate: pumping operations; unless a passage be established through the solid portion of the bar which serves asan anode.
A similar arrangement could clearly be adopted with a thin walled anode, such as represented in Figs. 1 and 2, the two end structures being sufiiciently spaced from each other. However, it may be advantageous in certain cases to abandon the three-conductor coaxial output line and use in its place two or several transmission lines extending from the electrodes of the arrangement. Figs. 4, 5 and 6 show three examples of such structures.
In the structure of Fig. 4, the cylindrical anode 21 is open at its two ends and on these ends are sealed insulated balloons 28 and 29 which may, for example, be of glass. In cylinder 2'! there is fixed, iorinstance by brazing, a short conductive tube 39 on, the open end of which is sealed insulating balloon 3|. On the inside of the air tight envelope thus formed, there is disposed a grid structure consisting of an elongated cylinder 32 coaxial to anode 21' and supported at its center, by a stem 33, serving as a lead-irr conductor. Stein 33. passes ,coaxially; through sleeve 30 andp'asses out of balloon 3! throu h seal 34, for instance, a. direct glassmetalsea-l asshown. At each end of tube 33 there are fixed, for example by-b'raz-ing, a'certainnumber of posts 35, 36, parallel to the generatrixes of thecylinder 33 on which are wrapped the grid" threads, not shown. On the inside of thesegrids and along their length aredisposed filamentary cathodes 3'! andflfi, respectively, carried by supporting and lead-in stems 39'and' 40 which pass through the balloons 28; and 29 through seals, such as shown for example at 4-! and: 42. Screens may, as shown at 43 and; 44. oe-provicled at the ends of the'grids-a'i and 38.
Two coaxial lines may thenbe provided at the two ends of the structure in the manner shown in Figs- 1 and 2 by means of cylinders attached to anode 2'! and extending coaxially with respect to the axis of the complete structure, the other conductor of-these coaxial lines beingconstituted by cylinders forming the screen for the lead-in conductors of the cathodes. A third coaxial line may, if desired, be provided betWeen the anode sleeve 30 and the grid conductor 33 in the same way. A jacket for water or other cooling fluid,- may be provided around the anode. The continuityof. the-gridstructure avoids allvundesirable electron couplings between the ends-of the filaments and the anode.
In such a double structure, it may nevertheless be desirable to be able to Withdraw energy from the grid. Consequently, asshown in. Fig.
. 5, one may provide on the anode 21 two other cylindrical sleeves 45 and 46, schematically dis- DOSGd'OIl each side of the axis. of the sleeve 30 and onthe other side. of the anode. These sleeves 45 and 48 carry sealed on to them insulating balloons 41 and idthrough which pass the lead-in conductors of. grids 4 9 and, 50, by means of seals 5| and 52, for example. These conductors 49 and 50 may constitute. a parallel wire line. The rest of the structurebeing identical to Fig. 4 will not be described in detail and the, same numerical references are assigned to corresponding elements, as. is the case also in the structure of Fig. 6.
In this Fig. 6, however, the two balloons28 and 29 attwo ends of the anode?! are no longer passedthrough by the lead-outs of the filaments of the two active structures. Thesestructures operate in the case of this figure with filaments 53 and 54 in series, fed by conductors 55 and'56 which extend longitudinally on the. inside of, the
grid cylinder and pass out at right angles, as shown through an insulating balloon 51 sealed to a fourth cylindrical sleeve 58 of he anode 2i. This lead-out is effected in the middle of the tube between the lead-out conductors of the grid.
Still another utilization of the structures described in the invention may be visualized for tubes which are no longer double but multiple. In this case schematically represented in plan view in Fig. 7 a certain number of simple structures are schematically assembled around an axis. Such an arrangement requires no additional description, being self-explanatory in accordance with the descriptions of the preceding figures.
Although the invention has been described in the case of certain particular examples of embodiments, it is clear that it is not limited thereto in any respect, but is, on the contrary, susceptible of numerous modifications and adaptations without departing from the domain of the invention. In particular all of the appropriate structures of filaments and grids may be used in devices incorporating the characteristics of the invention.
What is claimed is:
l. A high frequency vacuum tube arrangement comprising a cylindrical anodeforming a part of the envelope, a grid electrode assembly arranged on a cylindrical surface of a given diameter arranged concentrically of said anode, a concentric transmission line externalof said envelope, means interconnecting said outer conductor and said anode, and means interconnecting said inner conductor and said grid, each of said interconnecting means comprising a generally conical tapering member, one of said conical members being disposed within the other of said conical members, whereby a substantially uniform gradient between the anode and the grid structures is obtained.
2. A high frequency tube arrangement according to claim 1 in which the respective radii of each of said members at any given point along the axis of said tube bears substantially the same ratio as the ratio of the respective radii of the conductors of said concentric transmission line.
3. A high frequency tube according to claim 1, further comprising a cathode having a cylindrical surface concentrically arranged within said grid electrode assembly and means for energizing said cathode, comprising a shielded conductor pair, the shield of said pair being arranged concentrically within said inner conductor and having substantially the same diametral ratio to said iiuier conductor as said cathode cylinder has to said cylindrical surface.
A vacuum tube structure comprising an anode of substantially cylindrical form, glass bulbs sealed at each end of said anode, a tubular grid support mounted concentrically within said anode, a set of grid wires at each end of said tube cooperating with said anode, cathode structures arranged concentrically of said grid wire set and supported by leads through said glass bulbs, a further glass seal substantially at a longitudinal midpoint on the periphery of said anode, and a rod fastened substantially at the center or" said tubular support and extending generally radially of said anode and supported in said further glass seal to maintain said tubular support in position.
5. A vacuum tube structure according to claim 4;, further comprising output leads comprising rods connected at one end to symmetrically spaced points on said tubular support, and lateral extensions in said anode concentrically arranged outside each of said leads.
6. A vacuum tube structure according to claim further comprising cathode energizing leads arranged within said tubular support, said tubular support and said anode being provided with an opening substantially mid-way along their lengths, and means for supplying the filament heating current to said cathode energizing leads extending through said openings.
EMILE LABIN.
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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2421784A (en) * 1943-02-24 1947-06-10 Rca Corp Ultra high frequency apparatus
US2423444A (en) * 1944-01-07 1947-07-08 Bell Telephone Labor Inc Electronic discharge device for ultra high frequency energy generation
US2431337A (en) * 1943-05-07 1947-11-25 Standard Telephones Cables Ltd Electron discharge device for high frequency
US2450629A (en) * 1944-03-14 1948-10-05 Gen Electric Ultra high frequency magnetron generator
US2452061A (en) * 1946-01-19 1948-10-26 Raytheon Mfg Co Thermionic tube structure
US2461125A (en) * 1943-12-31 1949-02-08 Rca Corp Electron discharge device utilizing cavity resonators
US2469180A (en) * 1946-05-10 1949-05-03 Amperex Electronic Corp Self-contained high-frequency oscillator
US2472088A (en) * 1943-06-18 1949-06-07 Clarence A Boddie Oscillator tube

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2421784A (en) * 1943-02-24 1947-06-10 Rca Corp Ultra high frequency apparatus
US2431337A (en) * 1943-05-07 1947-11-25 Standard Telephones Cables Ltd Electron discharge device for high frequency
US2472088A (en) * 1943-06-18 1949-06-07 Clarence A Boddie Oscillator tube
US2461125A (en) * 1943-12-31 1949-02-08 Rca Corp Electron discharge device utilizing cavity resonators
US2423444A (en) * 1944-01-07 1947-07-08 Bell Telephone Labor Inc Electronic discharge device for ultra high frequency energy generation
US2450629A (en) * 1944-03-14 1948-10-05 Gen Electric Ultra high frequency magnetron generator
US2452061A (en) * 1946-01-19 1948-10-26 Raytheon Mfg Co Thermionic tube structure
US2469180A (en) * 1946-05-10 1949-05-03 Amperex Electronic Corp Self-contained high-frequency oscillator

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