US2828434A - Electron beam focussing device - Google Patents
Electron beam focussing device Download PDFInfo
- Publication number
- US2828434A US2828434A US387945A US38794553A US2828434A US 2828434 A US2828434 A US 2828434A US 387945 A US387945 A US 387945A US 38794553 A US38794553 A US 38794553A US 2828434 A US2828434 A US 2828434A
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- disc
- electron beam
- electron
- magnetic
- casing
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/02—Electrodes; Magnetic control means; Screens
- H01J23/08—Focusing arrangements, e.g. for concentrating stream of electrons, for preventing spreading of stream
- H01J23/087—Magnetic focusing arrangements
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
- H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
- H01J29/54—Arrangements for centring ray or beam
Definitions
- FIG. 2. /0 5 7 m 6 5 INVENTOR. /i I w. KLE/N w I 59/2 WA TTORNEY United States Patent@ ELECTRON BEAM FOCUSSING DEVICE Werner Klein, Korntal, Wurttemberg, and Walter Friz,
- Electron beams particularly those of high current density, and which are intended to maintain a constant cross-section over a certain length, are usually focussed by a homogeneous magnetic field extending over the entire length of the beam, and the vector of field intensity of which coincides with the direction of the beam.
- the electron gun systems are designed so as to produce a convergent beam of electrons. By this means it is possible to obtain a minimum beam cross-section at a predetermined point along the beam axis, behind which the beam spreads out again on account of the space charge.
- a so-called magnetic barrier i. e. a disc of a material having a magnetic susceptibility which is as high as possible, positioned normal to the field direction, and in the centrally arranged aperture of which the electron beam will achieve in the shortest distance the rise of the magnetic field strength to the full intensity. Without this disc the transition zone from the field-free space to the point of the full field intensity would be undesirably large.
- a small or secondary magnetic field intensity vector is employed, arranged vertically to the beam axis. This vector is producedby a disc coil which embraces the electron beam and the axis which is capable of being tilted toward the beam axis at will.
- Another arrangement comprises two pairs of coils, the axes of which are arranged vertically above each other, and
- the intensity and direction of the auxiliary magnetic field may be adjusted, which is required for the adjustment of the beam.
- These arrangements have the disadvantage that they produce a stray mag netic field, which spreads over the space required for adjusting the beam direction. This results in an undesired vortex motion of the beam in addition to the adjustment of the direction and results in a considerably deteriorated beam contour with respect to directing the beam through the steady magnetic field.
- cathode ray tubes it is known to use a permanent magnet, which is capable of being shifted along the neck of the cathode ray tube, for the adjustment of the beam.
- a disc of magnetic material for the adjustment 2,828,434 Patented Mar. 25, 1 958 of the beam in electric discharge tubes which employ magnetic means for focussing of the electron beam.
- the adjusting disc is mounted in a way that the angle, which is constituted by the beam and the axis of the disc, may be variably adjusted. Consequently there results a small section in the hold of the disc in which, by tilting the disc, the magnetic field is provided in the beam axis with an additional component, which is determinable by the tilting position of the disc, and with the aid of which the beam may be adjusted.
- the gun system 1 is surrounded by a screen 2 to screen it from interfering magnetic fields.
- the gun system is followed by a drift tube 3 of a non-magnetic material, to which the coil 4 is connected.
- the beam focussing coils 5 and 6 are interrupted by the wave guide 7 which constitutes the means for introducing input energy.
- the tube is surrounded by an adjusting disc 10 of magnetic material such as soft iron.
- the central aperture in the adjusting disc 10 embraces the tube as tightly as possible, and is chamfered at its edge to a knife edge in order to concentrate the magnetic lines of force.
- the screws 11 are threaded in mounting 13 to which are secured springs 14 fixed to the disc 10.
- springs 14 By adjustment of the screws 11 it is possible to exert a pressure upon the plane of the disc 10 via springs 14. This results in an angular displacement or tilting of the disc 10 whereby a fine adjustment of field at point 9 is obtained.
- the disc 1% may be made with an outer diameter somewhat larger than that of the focussing coils 5, 6, in order to serve as a magnetic shield and at the same time as a means for keeping stray fields away from the gun system.
- the arrangement is similar to that shown in Fig. 1, but for obtaining shielding against any external interference fields, the focussing coils 5 and 6 are entirely surrounded by an iron casing 8.
- This casing serves as a mounting for the adjusting disc 10 and constitutes the front sealing of the magnetic field.
- the air gap between the disc 10 and the iron casing S, is as small as possible.
- the disc 10 is suspended on the radially arranged flat springs 14 secured to the casing 8.
- the plane of the disc 10 may be adjustably inclined by means of the screws 11, whilst the screws 12 serve for centering of the disc, the screws 11 and 12 being threaded in the casing 8. It is preferable to use three screws 11 and three screws 12.
- An electron discharge device comprising means including an electron gun for projecting an electron beam along a path, magnetic focusing means for focusing said beam to maintain a substantially uniform diameter, mounted along said path, and means directing said beam into the magnetic field of said focusing means while shielding said gun from said field comprising a disc of magnetic material having an aperture through which the electron beam is directed, the edges of said aperture being closely adjacent to said beam, means for mounting said disc between said focusing means and said gun and adjusting means for varying the position of said disc.
- An electron discharge device comprising means in- 3 V eluding an electron gun for projecting an electron beam along a path, a magnetic focusing coil for focusing said beam surrounding the electron beam, a casing of magnetic material surrounding said coil for screening it from external fields, and means directing said beam into the magnetic field of said coil while shielding said gun from said field comprising a disc of magnetic material, substantially forming the closure for one end of said casing and having a central aperture through which the beam is directed, means for mounting said disc on said casing between said coil and said electron gun, and adjusting means forvarying the position of said disc with respect to the axis of the beam.
- An electron discharge device in which said adjusting means comprises, a plurality of spring members each having one end secured to said disc and the other end secured to said casing, means supported in said casing for moving said disc transversely of said beam path and means for varying the angle of the plane of said disc with respect to said path.
Description
March 25, 1958 w. KLEIN ET AL 2,823,434
ELECTRON BEAM FOCUSSING DEVICE Filed Oct. 23, 1953 Fle.
FIG. 2. /0 5 7 m 6 5 INVENTOR. /i I w. KLE/N w I 59/2 WA TTORNEY United States Patent@ ELECTRON BEAM FOCUSSING DEVICE Werner Klein, Korntal, Wurttemberg, and Walter Friz,
Stuttgart, Germany, assignors to International Standard Electric Corporation, New York, N. Y., a corporation of Delaware Application October 23, 1953, Serial No. 387,945
Claims priority, application Germany October 25, 1952 3 Claims. (Cl. 31384) Electron beams, particularly those of high current density, and which are intended to maintain a constant cross-section over a certain length, are usually focussed by a homogeneous magnetic field extending over the entire length of the beam, and the vector of field intensity of which coincides with the direction of the beam. Usually the electron gun systems are designed so as to produce a convergent beam of electrons. By this means it is possible to obtain a minimum beam cross-section at a predetermined point along the beam axis, behind which the beam spreads out again on account of the space charge. In order to obtain a uniform beam contour over a greater length it would be necessary to suddenly permit the magnetic field to become effective in its full strength at that particular point where the cross-section of the beam is of a minimum size usually called cross-over point. This requirement is difiicult to comply with in practice, although by employing suitable arrangements an approximation of this result may be obtained.
To this end there is arranged in most cases a so-called magnetic barrier, i. e. a disc of a material having a magnetic susceptibility which is as high as possible, positioned normal to the field direction, and in the centrally arranged aperture of which the electron beam will achieve in the shortest distance the rise of the magnetic field strength to the full intensity. Without this disc the transition zone from the field-free space to the point of the full field intensity would be undesirably large.
On account of the unavoidable tolerances with respect to the dimensions of the mechanical structure of the electron gun system, provison must be made for an adjustment serving to bring the electron beam into the exact direction when entering the magnetic field. For this purpose frequently a small or secondary magnetic field intensity vector is employed, arranged vertically to the beam axis. This vector is producedby a disc coil which embraces the electron beam and the axis which is capable of being tilted toward the beam axis at will. Another arrangement comprises two pairs of coils, the axes of which are arranged vertically above each other, and
each one of which cuts the beam axis in its vertical direction. Thus according to the D. C. admission of the coil or coils, the intensity and direction of the auxiliary magnetic field may be adjusted, which is required for the adjustment of the beam. These arrangements, however, have the disadvantage that they produce a stray mag netic field, which spreads over the space required for adjusting the beam direction. This results in an undesired vortex motion of the beam in addition to the adjustment of the direction and results in a considerably deteriorated beam contour with respect to directing the beam through the steady magnetic field.
In cathode ray tubes it is known to use a permanent magnet, which is capable of being shifted along the neck of the cathode ray tube, for the adjustment of the beam.
According to the present invention, however, there is provided a disc of magnetic material for the adjustment 2,828,434 Patented Mar. 25, 1 958 of the beam in electric discharge tubes which employ magnetic means for focussing of the electron beam. The adjusting disc is mounted in a way that the angle, which is constituted by the beam and the axis of the disc, may be variably adjusted. Consequently there results a small section in the hold of the disc in which, by tilting the disc, the magnetic field is provided in the beam axis with an additional component, which is determinable by the tilting position of the disc, and with the aid of which the beam may be adjusted.
Two embodiments of our invention as applied to an arrangement for projecting an electron beam into the coil space of a travelling wave tube are shown in Fig. 1 and Fig. 2, respectively, of the accompanying drawings.
Referring first to Fig. 1, the gun system 1 is surrounded by a screen 2 to screen it from interfering magnetic fields. The gun system is followed by a drift tube 3 of a non-magnetic material, to which the coil 4 is connected. The beam focussing coils 5 and 6 are interrupted by the wave guide 7 which constitutes the means for introducing input energy. At a point 9 in the drift space, which is substantially at or near the crossover point of the electron beam, the tube is surrounded by an adjusting disc 10 of magnetic material such as soft iron. The central aperture in the adjusting disc 10 embraces the tube as tightly as possible, and is chamfered at its edge to a knife edge in order to concentrate the magnetic lines of force. The screws 11 are threaded in mounting 13 to which are secured springs 14 fixed to the disc 10. By adjustment of the screws 11 it is possible to exert a pressure upon the plane of the disc 10 via springs 14. This results in an angular displacement or tilting of the disc 10 whereby a fine adjustment of field at point 9 is obtained. The disc 1% may be made with an outer diameter somewhat larger than that of the focussing coils 5, 6, in order to serve as a magnetic shield and at the same time as a means for keeping stray fields away from the gun system.
In the embodiment shown in Fig. 2 of the drawing, the arrangement is similar to that shown in Fig. 1, but for obtaining shielding against any external interference fields, the focussing coils 5 and 6 are entirely surrounded by an iron casing 8. This casing at the same time, serves as a mounting for the adjusting disc 10 and constitutes the front sealing of the magnetic field. The air gap between the disc 10 and the iron casing S, is as small as possible. The disc 10 is suspended on the radially arranged flat springs 14 secured to the casing 8. The plane of the disc 10 may be adjustably inclined by means of the screws 11, whilst the screws 12 serve for centering of the disc, the screws 11 and 12 being threaded in the casing 8. It is preferable to use three screws 11 and three screws 12.
While we have described above the principles of our invention in connection with specific apparatus, it is to be clearly understood that this description is made only by way of example and not as a limitation to the scope of our invention.
What is claimed is:
1. An electron discharge device comprising means including an electron gun for projecting an electron beam along a path, magnetic focusing means for focusing said beam to maintain a substantially uniform diameter, mounted along said path, and means directing said beam into the magnetic field of said focusing means while shielding said gun from said field comprising a disc of magnetic material having an aperture through which the electron beam is directed, the edges of said aperture being closely adjacent to said beam, means for mounting said disc between said focusing means and said gun and adjusting means for varying the position of said disc.
2. An electron discharge device comprising means in- 3 V eluding an electron gun for projecting an electron beam along a path, a magnetic focusing coil for focusing said beam surrounding the electron beam, a casing of magnetic material surrounding said coil for screening it from external fields, and means directing said beam into the magnetic field of said coil while shielding said gun from said field comprising a disc of magnetic material, substantially forming the closure for one end of said casing and having a central aperture through which the beam is directed, means for mounting said disc on said casing between said coil and said electron gun, and adjusting means forvarying the position of said disc with respect to the axis of the beam.
3. An electron discharge device according to claim 2 in which said adjusting means comprises, a plurality of spring members each having one end secured to said disc and the other end secured to said casing, means supported in said casing for moving said disc transversely of said beam path and means for varying the angle of the plane of said disc with respect to said path.
References Cited in the file of this patent UNITED STATES PATENTS 2,234,720 De Tar Mar. 11, 1941 2,305,384 Litton Dec. 22, 1942 2,440,403 Jackson Apr. 27, 1948 2,586,559 Page Feb. 19, 1952 2,608,668 Hines Aug. 26, 1952 2,741,718 Wang Apr. 10, 1956
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE315449X | 1952-10-25 |
Publications (1)
Publication Number | Publication Date |
---|---|
US2828434A true US2828434A (en) | 1958-03-25 |
Family
ID=6150214
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US387945A Expired - Lifetime US2828434A (en) | 1952-10-25 | 1953-10-23 | Electron beam focussing device |
Country Status (4)
Country | Link |
---|---|
US (1) | US2828434A (en) |
CH (1) | CH315449A (en) |
GB (1) | GB776648A (en) |
NL (1) | NL182200B (en) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2939045A (en) * | 1954-05-12 | 1960-05-31 | Applied Radiation Corp | Traveling wave tubes |
US2945153A (en) * | 1956-08-31 | 1960-07-12 | Rca Corp | Electron beam tube |
US2945980A (en) * | 1954-07-02 | 1960-07-19 | Applied Radiation Corp | Vacuum tube |
US2974246A (en) * | 1949-08-12 | 1961-03-07 | Int Standard Electric Corp | Electron gun for electron discharge tube |
US3001095A (en) * | 1957-02-15 | 1961-09-19 | Lorenz C Ag | Highly compressive gun system comprising a combined electrostatic and magnetic focusing |
US3052808A (en) * | 1959-06-11 | 1962-09-04 | Telefunken Gmbh | Beam centering device for travelling wave tubes |
US3092745A (en) * | 1958-06-25 | 1963-06-04 | Siemens Ag | Magnetic means for focusing and densifying the electron beam in traveling wave tubes |
US3133226A (en) * | 1960-10-07 | 1964-05-12 | Westinghouse Electric Corp | Magnetic structure for traveling wave tubes |
US3155866A (en) * | 1961-03-14 | 1964-11-03 | Bell Telephone Labor Inc | Magnetic focusing structure for traveling wave tubes |
FR2532435A1 (en) * | 1982-09-01 | 1984-03-02 | Tektronix Inc | END ADJUSTING DEVICE FOR ASSEMBLING MAGNETS |
US4555646A (en) * | 1981-10-07 | 1985-11-26 | Varian Associates, Inc. | Adjustable beam permanent-magnet-focused linear-beam microwave tube |
US4942336A (en) * | 1988-04-18 | 1990-07-17 | Kurt Amboss | Traveling-wave tube with confined-flow periodic permanent magnet focusing |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2234720A (en) * | 1939-08-10 | 1941-03-11 | Gen Electric | Electron discharge apparatus |
US2305884A (en) * | 1940-07-13 | 1942-12-22 | Int Standard Electric Corp | Electron beam concentrating system |
US2440403A (en) * | 1945-10-31 | 1948-04-27 | Pye Ltd | Focus coil suspension for cathoderay tubes |
US2586559A (en) * | 1950-02-23 | 1952-02-19 | Gen Electric | Multiple element electron lens arrangement |
US2608668A (en) * | 1950-06-17 | 1952-08-26 | Bell Telephone Labor Inc | Magnetically focused electron gun |
US2741718A (en) * | 1953-03-10 | 1956-04-10 | Sperry Rand Corp | High frequency apparatus |
-
0
- NL NLAANVRAGE7304880,A patent/NL182200B/en unknown
-
1953
- 1953-07-17 GB GB19878/53A patent/GB776648A/en not_active Expired
- 1953-10-23 US US387945A patent/US2828434A/en not_active Expired - Lifetime
- 1953-10-24 CH CH315449D patent/CH315449A/en unknown
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2234720A (en) * | 1939-08-10 | 1941-03-11 | Gen Electric | Electron discharge apparatus |
US2305884A (en) * | 1940-07-13 | 1942-12-22 | Int Standard Electric Corp | Electron beam concentrating system |
US2440403A (en) * | 1945-10-31 | 1948-04-27 | Pye Ltd | Focus coil suspension for cathoderay tubes |
US2586559A (en) * | 1950-02-23 | 1952-02-19 | Gen Electric | Multiple element electron lens arrangement |
US2608668A (en) * | 1950-06-17 | 1952-08-26 | Bell Telephone Labor Inc | Magnetically focused electron gun |
US2741718A (en) * | 1953-03-10 | 1956-04-10 | Sperry Rand Corp | High frequency apparatus |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2974246A (en) * | 1949-08-12 | 1961-03-07 | Int Standard Electric Corp | Electron gun for electron discharge tube |
US2939045A (en) * | 1954-05-12 | 1960-05-31 | Applied Radiation Corp | Traveling wave tubes |
US2945980A (en) * | 1954-07-02 | 1960-07-19 | Applied Radiation Corp | Vacuum tube |
US2945153A (en) * | 1956-08-31 | 1960-07-12 | Rca Corp | Electron beam tube |
US3001095A (en) * | 1957-02-15 | 1961-09-19 | Lorenz C Ag | Highly compressive gun system comprising a combined electrostatic and magnetic focusing |
US3092745A (en) * | 1958-06-25 | 1963-06-04 | Siemens Ag | Magnetic means for focusing and densifying the electron beam in traveling wave tubes |
US3052808A (en) * | 1959-06-11 | 1962-09-04 | Telefunken Gmbh | Beam centering device for travelling wave tubes |
US3133226A (en) * | 1960-10-07 | 1964-05-12 | Westinghouse Electric Corp | Magnetic structure for traveling wave tubes |
US3155866A (en) * | 1961-03-14 | 1964-11-03 | Bell Telephone Labor Inc | Magnetic focusing structure for traveling wave tubes |
US4555646A (en) * | 1981-10-07 | 1985-11-26 | Varian Associates, Inc. | Adjustable beam permanent-magnet-focused linear-beam microwave tube |
FR2532435A1 (en) * | 1982-09-01 | 1984-03-02 | Tektronix Inc | END ADJUSTING DEVICE FOR ASSEMBLING MAGNETS |
US4942336A (en) * | 1988-04-18 | 1990-07-17 | Kurt Amboss | Traveling-wave tube with confined-flow periodic permanent magnet focusing |
Also Published As
Publication number | Publication date |
---|---|
NL182200B (en) | |
CH315449A (en) | 1956-08-15 |
GB776648A (en) | 1957-06-12 |
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