US3094615A - Charged particle beam-viewing arrangement - Google Patents
Charged particle beam-viewing arrangement Download PDFInfo
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- US3094615A US3094615A US835528A US83552859A US3094615A US 3094615 A US3094615 A US 3094615A US 835528 A US835528 A US 835528A US 83552859 A US83552859 A US 83552859A US 3094615 A US3094615 A US 3094615A
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- particle beam
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- faraday cage
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/29—Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
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- This invention relates to apparatus for the acceleration of charged particles to high energy and in particular to a device for viewing and measuring the beam of charged particles produced by such apparatus. Particle accelerators are used to produce ion beams which then may be employed to bombard specific targets for the production of nuclear reactions useful in physical research.
- FIG. 1 is a sectional view of a device through which the charged-particle beam to be measured travels and which device is equipped with a beam-viewing arrangement constructed in accordance with the invention and so positioned that the fiuorescible target is in the path of the charged-particle beam;
- FIG. 2 is a sectional view along the line 22 of FIG. 1;
- FIG. 3 is a view similar to a portion of that of FIG. 1 but showing the device adjusted so that the Faraday cage is in the path of the charged-particle beam;
- FIG. 4 is a view similiar to that of FIG. 3 but showing the device positioned so that neither the fiuorescible target nor the Faraday cage is in the path of the chargedparticle beam.
- FIGS. 1 and 2 therein is shown a portion of the tube extension 1 of a charged particle accelerator.
- the particle accelerator is not shown in any greater detail since the construction thereof has no bearing on the invention which is concerned merely with a measurement and detection of a charged-particle beam however created.
- the location of the charged-particle beam is indicated by the line 2.
- a Faraday cage 3 and a current indicating means such as fiuorescible target 4 which may comprise, for example, a quartz slab are mounted upon a shaft 5 which extends through the wall of the tube extension 1 and which is rotatable by means of the handle or lever 6.
- the Faraday cage 3 and quartz slab 4 are mounted substantially Patented June 18, 1963 ice parallel to each other and in FIGS.
- the lever 6 is so positioned that the quartz slab 4 is in the path of the ion beam 2 which is travelling from right to left in FIG. 1 so that the beam strikes the quartz slab before striking any portion of the Faraday cage 3.
- the effect of the impingement of a charged-particle beam on a quartz sl-ab is to cause the latter to glow visibly at the spot where the quartz is being bombarded.
- the wall of the tube extension is equipped with a viewing part comprising transparent area 7 through which the position of the glow on the quartz slab may be observed, and in this way the position of the charged-particle beam 2 in the tube extension 1 may be determined optically.
- the Fara-day cage 3 is connected by a wire 8 to an appropriate terminal 9 which in turn can be connected to an appropriate current indicating means such as microammeter 10.
- the fiuorescible target 4 may be covered by wire mesh 11 or a conducting coat as might be desirable.
- the wire mesh or conducting coat would be electrically connected to the shaft 5 and hence would be grounded. In this way unwanted charging effects can be eliminated, such as accumulation of charge on the quartz slab 4 which might deflect the beam of charged particles.
- apparatus for selectively indicating the position and measuring the current of a charged particle beam generated thereby comprising a housing member having a viewing port therein and being adapted to effect a longitudinal extension to the output end of said particle accelerator, a Faraday cage disposed within said housing member, said Faraday cage being electrically connected to current indicating means, a beam position indicator disposed within said housing member, said beam position indicator consisting of a quartz plate and having a grounded wire mesh on the beam intercepting surface thereof, a rotatable shaft disposed transversely through said housing member, said Faraday cage and said beam position indicator being mounted on said shaft in mutually fixed relationship, and means for rotating said shaft, said Faraday cage and said beam position indicator being mutually spaced so that rotation of said shaft effects successive interception of the charged particle beam by said Faraday cage, said beam position indicator, and neither.
Description
June 18, 1963 P. H. ROSE CHARGED PARTICLE BEAM-VIEWING ARRANGEMENT Filed Aug. 24, 1959 United States Patent 94,615 CHARGED PARTICLE BEAM-VIEWING ARRANGEMENT Peter H. Rose, Bedford, Mass., assignor to High Voltage Engineering Corporation, Burlington, Mass., a corporation of Massachusetts Filed Aug. 24, 1959, Ser. No. 835,528 1 Claim. (Cl. 250-495) This invention relates to apparatus for the acceleration of charged particles to high energy and in particular to a device for viewing and measuring the beam of charged particles produced by such apparatus. Particle accelerators are used to produce ion beams which then may be employed to bombard specific targets for the production of nuclear reactions useful in physical research. Usually experiments of this nature require a high degree of precision so that it becomes important that such a particle accelerator be equipped with an appropriate device for determining the location of the ion beam and for measuring the electrical current in the ion beam. The invention comprehends a simple device for accomplishing this purpose. Although the invention is particularly useful with ion .accelerators, it may also be used with other particle accelerators, such as electron accelerators. In accordance with the invention a fiuorescible target capable of emitting visible light upon bombardment by the charged-particle beam, and a Faraday cage are mounted in the vicinity of the beam so as to be in fixed position relative to each other but rotatable with respect to the rest of the particle accelerator. When properly mounted in the particle accelerator such a device may be rotated about its axis so as to bring either the fiuorescible target or the Faraday cage or neither in the path of the beam.
The invention may best be understood from the following detailed description thereof having reference to the accompanying drawing in which:
FIG. 1 is a sectional view of a device through which the charged-particle beam to be measured travels and which device is equipped with a beam-viewing arrangement constructed in accordance with the invention and so positioned that the fiuorescible target is in the path of the charged-particle beam;
FIG. 2 is a sectional view along the line 22 of FIG. 1;
FIG. 3 is a view similar to a portion of that of FIG. 1 but showing the device adjusted so that the Faraday cage is in the path of the charged-particle beam; and
FIG. 4 is a view similiar to that of FIG. 3 but showing the device positioned so that neither the fiuorescible target nor the Faraday cage is in the path of the chargedparticle beam.
Referring to the drawing and first to FIGS. 1 and 2 thereof, therein is shown a portion of the tube extension 1 of a charged particle accelerator. The particle accelerator is not shown in any greater detail since the construction thereof has no bearing on the invention which is concerned merely with a measurement and detection of a charged-particle beam however created. The location of the charged-particle beam is indicated by the line 2. A Faraday cage 3 and a current indicating means such as fiuorescible target 4 which may comprise, for example, a quartz slab are mounted upon a shaft 5 which extends through the wall of the tube extension 1 and which is rotatable by means of the handle or lever 6. The Faraday cage 3 and quartz slab 4 are mounted substantially Patented June 18, 1963 ice parallel to each other and in FIGS. 1 and 2 the lever 6 is so positioned that the quartz slab 4 is in the path of the ion beam 2 which is travelling from right to left in FIG. 1 so that the beam strikes the quartz slab before striking any portion of the Faraday cage 3. As is well known, the effect of the impingement of a charged-particle beam on a quartz sl-ab is to cause the latter to glow visibly at the spot where the quartz is being bombarded. The wall of the tube extension is equipped with a viewing part comprising transparent area 7 through which the position of the glow on the quartz slab may be observed, and in this way the position of the charged-particle beam 2 in the tube extension 1 may be determined optically.
Rotation of the lever 6 through Will bring the Faraday cage 3 into the position shown in FIG. 3, namely in the path of the charged-particle beam 2, so that the cup-shaped Faraday cage 3 collects all the beam current. As shown in FIG. 2 the Fara-day cage 3 is connected by a wire 8 to an appropriate terminal 9 which in turn can be connected to an appropriate current indicating means such as microammeter 10.
If the lever is rotated through 90 in the opposite direction from the position shown in FIGS. 1 and 2, both the Faraday cage 3 and the quartz slab 4 are removed from the path of the beam 2 as is shown in FIG. 4.
The fiuorescible target 4 may be covered by wire mesh 11 or a conducting coat as might be desirable. The wire mesh or conducting coat would be electrically connected to the shaft 5 and hence would be grounded. In this way unwanted charging effects can be eliminated, such as accumulation of charge on the quartz slab 4 which might deflect the beam of charged particles.
Having thus described the principles of the apparatus together with several illustrative embodiments thereof, it is to be understood that although specific terms are em.- ployed they are used in a generic and descriptive sense and not for purposes of limitation, the scope of the invention being set forth in the following claim.
I claim:
In combination with a particle accelerator, apparatus for selectively indicating the position and measuring the current of a charged particle beam generated thereby comprising a housing member having a viewing port therein and being adapted to effect a longitudinal extension to the output end of said particle accelerator, a Faraday cage disposed within said housing member, said Faraday cage being electrically connected to current indicating means, a beam position indicator disposed within said housing member, said beam position indicator consisting of a quartz plate and having a grounded wire mesh on the beam intercepting surface thereof, a rotatable shaft disposed transversely through said housing member, said Faraday cage and said beam position indicator being mounted on said shaft in mutually fixed relationship, and means for rotating said shaft, said Faraday cage and said beam position indicator being mutually spaced so that rotation of said shaft effects successive interception of the charged particle beam by said Faraday cage, said beam position indicator, and neither.
References Cited in the file of this patent UNITED STATES PATENTS 2,356,963 Young Aug. 29, 1944 2,360,872 Hillier Oct. 24, 1944 2,626,359 Weber Jan. 20, 1953
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US835528A US3094615A (en) | 1959-08-24 | 1959-08-24 | Charged particle beam-viewing arrangement |
Applications Claiming Priority (1)
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US835528A US3094615A (en) | 1959-08-24 | 1959-08-24 | Charged particle beam-viewing arrangement |
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US835528A Expired - Lifetime US3094615A (en) | 1959-08-24 | 1959-08-24 | Charged particle beam-viewing arrangement |
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3179804A (en) * | 1962-01-15 | 1965-04-20 | Ethicon Inc | Accelerator beam energy monitor |
US3360663A (en) * | 1965-05-14 | 1967-12-26 | Albert V Crewe | High-voltage generator |
US3446960A (en) * | 1965-08-30 | 1969-05-27 | Nasa | Device for measuring electron-beam intensities and for subjecting materials to electron irradiation in an electron microscope |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2356963A (en) * | 1942-08-29 | 1944-08-29 | Rca Corp | Electron microscope viewing chamber |
US2360872A (en) * | 1943-09-25 | 1944-10-24 | Rca Corp | Electron optical instrument |
US2626359A (en) * | 1951-10-16 | 1953-01-20 | Jr Frank R Weber | Target for particle accelerators |
-
1959
- 1959-08-24 US US835528A patent/US3094615A/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2356963A (en) * | 1942-08-29 | 1944-08-29 | Rca Corp | Electron microscope viewing chamber |
US2360872A (en) * | 1943-09-25 | 1944-10-24 | Rca Corp | Electron optical instrument |
US2626359A (en) * | 1951-10-16 | 1953-01-20 | Jr Frank R Weber | Target for particle accelerators |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3179804A (en) * | 1962-01-15 | 1965-04-20 | Ethicon Inc | Accelerator beam energy monitor |
US3360663A (en) * | 1965-05-14 | 1967-12-26 | Albert V Crewe | High-voltage generator |
US3446960A (en) * | 1965-08-30 | 1969-05-27 | Nasa | Device for measuring electron-beam intensities and for subjecting materials to electron irradiation in an electron microscope |
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