GB846897A - Magnetic electron lenses - Google Patents
Magnetic electron lensesInfo
- Publication number
- GB846897A GB846897A GB3258456A GB3258456A GB846897A GB 846897 A GB846897 A GB 846897A GB 3258456 A GB3258456 A GB 3258456A GB 3258456 A GB3258456 A GB 3258456A GB 846897 A GB846897 A GB 846897A
- Authority
- GB
- United Kingdom
- Prior art keywords
- pole pieces
- lens
- magnetic
- coils
- yokes
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000004075 alteration Effects 0.000 abstract 1
- 125000006850 spacer group Chemical group 0.000 abstract 1
- 230000007704 transition Effects 0.000 abstract 1
Classifications
-
- 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
- H01J29/58—Arrangements for focusing or reflecting ray or beam
- H01J29/64—Magnetic lenses
- H01J29/66—Magnetic lenses using electromagnetic means only
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/08—Deviation, concentration or focusing of the beam by electric or magnetic means
- G21K1/093—Deviation, concentration or focusing of the beam by electric or magnetic means by magnetic means
-
- 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
- H01J29/58—Arrangements for focusing or reflecting ray or beam
- H01J29/64—Magnetic lenses
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Electromagnetism (AREA)
- Magnetic Treatment Devices (AREA)
Abstract
846,897. Electron lenses. NATIONAL RESEARCH DEVELOPMENT CORPORATION. Oct. 17, 1957 [Oct. 25, 1956], No. 32584/56. Class 39(1). A magnetic lens for collimating rays emanating from a point O, Fig. 1, consists of a coil 4 wound uniformly on a magnetic member 1 to generate in the space between it and a second magnetic member 2 a leakage field which is zero at the centre and increases linearly, in opposite sign, towards either end of the space. Distortion of the field at the ends of the coil may be connected by additional coils wound around the non-magnetic spacers 3. In Fig. 3 the lens comprises two pairs of tapered pole pieces 6, 6 and 7, 7 energised by coils 9, 9 wound on the yokes 8, 8. The pole pieces may be energised instead by permanent magnets or, preferably, by yokes permanently magnetised to provide half the magnetising field required in combination with coils supplying the other half of the magnetising field. A magnetic screen 10 with a convex front may be provided and to compensate for the presence of the screen, the pole pieces 7 are slightly less tapered than the pole pieces 6 and are also slightly longer. The pole pieces may also be made to bulge in width between the yoke and the tip to avoid cylindrical aberration. The tips of the pole pieces may be bent outwards to secure a better field distribution and the pole pieces may be tapered in the horizontal plane to be convergent in the direction of the lens axis so as to reduce divergent action and to avoid sudden transition into the influence of the lens. The lens axis need not be central. The lenses may be used in the " flat " cathode ray tube of Specifications 739,496 and 794,257. In Fig. 4 the ends of the pole pieces are shown shaped to fit the tube envelope 12 and the yokes 13 and energising coils 9 are outside the envelope.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB3258456A GB846897A (en) | 1956-10-25 | 1956-10-25 | Magnetic electron lenses |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB3258456A GB846897A (en) | 1956-10-25 | 1956-10-25 | Magnetic electron lenses |
Publications (1)
Publication Number | Publication Date |
---|---|
GB846897A true GB846897A (en) | 1960-08-31 |
Family
ID=10340917
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB3258456A Expired GB846897A (en) | 1956-10-25 | 1956-10-25 | Magnetic electron lenses |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB846897A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2201523A1 (en) * | 1972-09-28 | 1974-04-26 | Thomson Csf | Normal incidence irradiation appts - for irradiation of curved surfaces by charged particles |
-
1956
- 1956-10-25 GB GB3258456A patent/GB846897A/en not_active Expired
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2201523A1 (en) * | 1972-09-28 | 1974-04-26 | Thomson Csf | Normal incidence irradiation appts - for irradiation of curved surfaces by charged particles |
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