EP2909840A1 - Band-shaped chopper for a particle beam - Google Patents
Band-shaped chopper for a particle beamInfo
- Publication number
- EP2909840A1 EP2909840A1 EP13801464.2A EP13801464A EP2909840A1 EP 2909840 A1 EP2909840 A1 EP 2909840A1 EP 13801464 A EP13801464 A EP 13801464A EP 2909840 A1 EP2909840 A1 EP 2909840A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- particle beam
- control
- chopper
- drive source
- band
- 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.)
- Granted
Links
- 239000002245 particle Substances 0.000 title claims abstract description 51
- 238000013016 damping Methods 0.000 claims description 4
- 238000000034 method Methods 0.000 claims description 3
- 230000033001 locomotion Effects 0.000 description 7
- 239000011248 coating agent Substances 0.000 description 5
- 238000000576 coating method Methods 0.000 description 5
- 239000000463 material Substances 0.000 description 5
- 229920000049 Carbon (fiber) Polymers 0.000 description 3
- 239000011358 absorbing material Substances 0.000 description 3
- 239000004917 carbon fiber Substances 0.000 description 3
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 3
- 230000005855 radiation Effects 0.000 description 3
- 239000006096 absorbing agent Substances 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 229920000642 polymer Polymers 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 230000004936 stimulating effect Effects 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 230000001360 synchronised effect Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- 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
- G21K1/02—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators
- G21K1/04—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators using variable diaphragms, shutters, choppers
- G21K1/043—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating using diaphragms, collimators using variable diaphragms, shutters, choppers changing time structure of beams by mechanical means, e.g. choppers, spinning filter wheels
Definitions
- the invention relates to a chopper for a particle beam.
- choppers are used with a control that have areas with different particle beam transmission. By moving the control through the particle beam, the particle beam alternately strikes higher and lower transmission regions and is modulated in this way.
- choppers designed as wheels are known, which are rotated by the particle beam.
- the peripheral speed at the edge of the chopper wheel specifies the frequency with which the particle beam can be modulated.
- the disadvantage is a lot of space needed for the Chopperrad or for the guide element.
- this space is tight enough to allow as many users as possible to get involved.
- there is a great interest in modulating the beam as close as possible to this place of origin in particular at spallation sources or research reactors, which initially emit neutrons starting from their place of origin analogously to a point source in order to be able to use as many neutrons as possible during a given pulse duration ,
- spallation sources or research reactors which initially emit neutrons starting from their place of origin analogously to a point source in order to be able to use as many neutrons as possible during a given pulse duration .
- the closer the chopper is to the place of origin of the neutrons the less space is available.
- a chopper for a particle beam comprises at least one flexible control element which is subdivided into at least two regions A and B, the region B having a smaller, in particular no, transparency for the particle beam than the region A, and at least one drive source for conveying the control element through the latter Particle beam that this time alternately hits the areas A and B.
- control element is strip-shaped and frictionally abuts the outer circumference of at least one element displaceable by the drive source in rotation.
- the formation of the control element as a band-shaped element of the chopper can be made substantially more space-saving than wheel or annular choppers according to the prior art.
- the voluminous in comparison to the control drive source can be arranged spatially separated from the beam path by the tape itself transmits the power of the drive source.
- the belt can be deflected by one or more rollers and the drive source can be placed far away from the beam path in a place where space is no longer scarce.
- the tape can also be passed through a narrow opening in a wall in another room by the drive source is located. The rate at which the control is promoted by the particle beam can then be increased by increasing the circumference of the rotatable element.
- the space savings entail that the user gains additional freedom in which direction the control element is conveyed by the particle beam. For example, if the particle beam does not have a square, but a rectangular transverse cut, so at the same linear conveying speed, the minimum achievable pulse duration can be shortened by the control element along the short side of the rectangular cross section is promoted by the particle beam. For this purpose, it is particularly advantageous if the control is flexible in itself (twistable), because it can then be promoted along a bent course.
- the drive source is advantageously protected from potential radiation damage, which improves the durability of the chopper.
- a neutron beam is modulated as a particle beam with the chopper, many materials that can serve to capture the neutron beam in region B are activated by the incident neutrons and in turn emit strong gamma radiation. This attacks organic molecules by breaking chemical bonds and stimulating the formation of free radicals.
- the insulation of the windings in electric motors, which are often used as a driving source, contains organic molecules and is therefore permanently attacked by the gamma radiation, so that the motor finally fails due to a short circuit.
- the control has only a very small mass in comparison to solid Chopperrä- ners and that by the non-positive engagement on the displaceable by the drive source in rotation element, a change or even reversal of the rotational speed of this element immediately passes through the control without having to overcome a large moment of inertia. Therefore, the conveying speed at which the control is moved by the particle beam can be varied.
- the drive source may be operated at a different conveying speed than in the configuration of the control in which the particle beam fully strikes an area B.
- the former conveying speed is then decisive for the pulse duration, within which the chopper is more permeable to the particle beam.
- the latter conveying speed is decisive for the repetition rate, ie the duration between the pulses.
- Both speeds can be selected independently of one another according to the needs arising from the specific application.
- the rotational frequency of the control element could be varied in the prior art, it was not possible to change the revolution speed during a single revolution.
- the chopper according to the invention can at least achieve the performance of the previous Radchopper, because of the lower moving mass tends to rather a better performance.
- the chopper according to the invention it is also possible to respond more flexibly to a change in the beam cross section, in particular the beam height, than with conventional wheel choppers.
- the beam height changes perpendicular to the conveying direction of the control element
- the areas A and B would have to be redesigned in the same situation with regard to the peripheral speed dependent on the radial distance from the axis of rotation, so that the jet is closed or opened over its entire cross-sectional area for the same time.
- the control is stretchable in the conveying direction. As a result, it can be kept constantly on mechanical tension, which improves the adhesion to the rotatable element.
- the control need not be externally pressed against the rotatable element.
- a coating which forms the areas B with a lower permeability to the particle beam can be applied to the outside of the control, which is not frictionally engaged, in partial areas. Both a pressing mechanism and the coating itself wear out quickly when the coating is repeatedly rolled between the Andrückmechanik and the rotatable element.
- the stretchable control also has damping characteristics such that vibrations from the drive source are largely unable to propagate to the location where the beam is modulated.
- Radchoppers are rigid systems and susceptible to vibrations.
- a damping element is arranged in the frictional connection between the drive source and the control element, for example a torsion spring.
- the damping element dissipates the energy of the vibrations originating from the drive source.
- the torque at which the drive source via the rotatable element promotes the control, and the mass density of the control should be coordinated so that the running of the drive source is not affected.
- the control has a mean mass density of less than 50 g per meter in length. The lighter the material, the lower the forces required to drive and change any direction of rapid movement. For example, if the tape is closed, there are inevitably reversal points along its length, at which even a uniform speed motion becomes an accelerated motion. As a result, both the control itself and the mechanics are claimed for their deflection at the turning point with forces.
- a carbon fiber ribbon or a band made of a fiber composite material having a thickness of between 0.025 mm and 0.5 mm, preferably with a thickness of 0.1 mm or less, is suitable as a control element.
- These materials are both light and stretchable in the conveying direction. They are very well transparent to a neutron beam as a particle beam, thus forming the area A.
- Areas B are formed on the belt by applying a neutron absorbing material either as a layer on one or both sides of the belt or integrated into the belt.
- Suitable neutron-absorbing materials are, for example, 10 B or Gd, which can be applied to the tape, for example embedded in a polymer, with a layer thickness of between 0.1 and 0.5 mm.
- the control may also be a metallic band with openings through which particles can pass. The openings then form the areas A, while the metallic band itself forms the impermeable area B.
- the control consists essentially (95%) of areas B which are neutron-impermeable and has only a few neutron windows (areas A) that are permeable to neutrons.
- the range A for the particle beam is advantageously at least 75%, preferably at least 90%, very particularly preferably at least 95%, and ideally completely permeable.
- the area B for the particle beam is advantageously at most 10%, preferably at most 1%, very particularly preferably at most 0.1% permeable and ideally completely impermeable.
- control is a closed band. Then, the drive source can be operated uniformly and the particle beam can nevertheless be periodically modulated. In particular, it is not necessary to stop and reverse the movement again and again under high acceleration forces.
- the control can be performed on a path (in a position) through the beam path and be guided on the way back around the beam path around.
- the control is guided at least in two layers through the beam path of the particle beam and has in each case at least two areas A and two areas B. These regions are arranged relative to one another in such a way that at least part of the particle beam in at least one configuration of the control element that can be moved by the drive source passes through an area A in both layers. Then it is not necessary to guide the control on the way back around the beam path around. Rather, both paths can be kept in one plane. so that the tape does not have to be twisted. In this configuration, the entire particle beam advantageously passes through an area A in both layers.
- the distance between the two layers in the beam direction is variable. This can be achieved, for example, by guiding both layers over separate pairs of rollers. By guiding the rollers of the second pair, over which the second layer is guided, closer together and at the same time away from the first layer in the beam direction, the distance between the two layers can be increased while the length of the control element remains the same. This can be used to allow only particles with a speed within a certain range to pass through the time of flight (speed filter).
- the particle beam strikes a region B in the second position then it helps to form a permeable window for the particle beam only for the shortest possible time.
- this configuration one-half of the beam cross-section is blocked by a region B in the first layer.
- the second half of the beam cross section, which passes through a region A in the first layer, is blocked by a region B in the second layer. Then the pulse duration can be halved. This effect can be achieved not only with two layers of one and the same closed band, but also with two non-contiguous bands which are only synchronized in their movement.
- the invention also relates to a method for operating a chopper according to the invention.
- the drive source in the configuration of the control element in which at least part of the particle beam passes exclusively through regions A of the control, the drive source is operated at a different conveying speed than in the configuration of the control element in which the particle beam completely strikes a region B. This has the effect that the pulse duration and the repetition rate can be adjusted independently of each other.
- Figure 1 embodiment of the chopper invention.
- FIG. 2 generation of a neutron pulse with the chopper shown in FIG.
- Figure 3 modulation of the feed rate of the control.
- FIG. 1a shows an exemplary embodiment of a chopper according to the invention, in which the drive source and the element which can be set into rotation by rotation thereof are not shown for the sake of clarity, in a perspective schematic drawing.
- the control element 1 is a closed, 0.1 mm thick band of carbon fiber, which is coated in the areas B1, B2 with 10 B as neutron-absorbing material. In areas A1, A2 it is uncoated; these areas serve as neutron windows.
- the band runs in a plane and is thus guided in two layers through the beam path 2 of the neutron beam. The two layers move in different directions, which are indicated by arrows.
- the regions A1, A2 are arranged relative to one another in such a way that there is a position of the band in which an area A1 and simultaneously in the second position an area A2 in the line of the beam path are in the first position. In this position, the chopper for the neutron beam 2 is permeable. If, on the other hand, all neutrons are absorbed either by a region B1 of the first layer or by a region B2 of the second layer of the strip, the chopper is impermeable to the neutron beam as a whole (closed).
- the designation in which position an area is (A1 or A2 or B1 or B2) refers to the instantaneous state shown in FIG. 1a. Of course, the areas wander from one layer to another as the tape rotates.
- Figure 1 b shows this embodiment in a further schematic drawing in plan view.
- the control element 1 is stretched between two rollers 3 and 4, on the outer circumference of which it rests in each case in a force-fitting manner.
- the roller 3 can be rotated by the drive source, which causes the belt to rotate.
- the drive source is a DC motor that can drive the roller 3 in both directions of rotation.
- the tape (control) is guided by further non-driven rollers 5 so that the two layers in which it is guided by the neutron beam 2, parallel to each other and are close to each other. If the neutrons are guided in evacuated neutron guides, then only a minimal gap between two neutron conductors is necessary for the installation of the chopper, which must pass through the neutron in air. In addition, the closer the two layers are to each other, the sharper the pulse width.
- FIG. 1 c shows a further snapshot.
- the roller 3 has rotated clockwise. Accordingly, the area A1 has moved to the right, while at the same time the area A2 has moved to the left.
- the neutron beam 2 is still incident on the belt 1 at the same location with the same beam width w. He is already there in the first position on an impermeable area B1 and is absorbed, so that he no longer reaches the second position and certainly can not pass the chopper as a whole.
- Figure 1 c shows the closed state of the chopper.
- FIG. 2 shows schematically the generation of a neutron pulse with the chopper sketched in FIG.
- the first layer of the tape has areas A1 which are transparent to the neutron beam and areas B1 which are opaque to the neutron beam.
- the second layer of tape has areas A2 which are permeable to the neutron beam and areas B2 which are opaque to the neutron beam.
- the beam hits entirely on an impermeable area B1 in the first layer of the strip and is therefore shaded (FIG. 2a).
- the two layers of the tape move in opposite directions in the directions indicated by arrows.
- any further movement of the band in the same direction will mean that the beam will no longer be completely shadowed, but a gap will be created between areas B1 and B2.
- the part of the neutron beam which has been transmitted in the first position through an area A1 is not completely shaded by a region B2 in the second position, but also encounters a transmissive area A2 there (FIG. 2c).
- the part of the neutron beam that has not been shaded in either of the two layers of the tape is allowed to pass through the chopper as a whole.
- the neutron beam After a time w / (2 * v), where w is the beam width and v is the linear velocity of the belt, the neutron beam passes completely through first the transmissive region A1 in the first layer and then through the transmissive region A2 in the second layer therethrough. He is thus passed through the chopper in total undiminished. At this moment, the neutron pulse reaches its maximum intensity (FIG. 2d).
- a pulse duration of about 3 ms can be realized at a repetition rate of 14 Hz.
- T can be varied during operation by operating the drive source at a different speed in the closed state of the chopper than during a pulse. Typically, the shortest possible pulses are desired, so that the band runs much faster during a pulse than between the pulses. With wheel choppers or even Fermi choppers, pulse duration and repetition time T can not be set independently of each other to the same extent.
- FIG. 3 shows a possible course of the linear velocity v of the band over time t.
- the feed of the tape is between two different working speeds V! and v 2 alternates.
- the belt moves at the speed Vi.
- the band is accelerated in time before the start of a pulse at the maximum possible rate that it runs for the duration ⁇ of the pulse at the much higher speed v 2 .
- ⁇ is defined either over the half-width (FWHM) or over the time span during which a nonzero number of neutrons passes the chopper.
- FWHM half-width
- the tape is decelerated with the maximum possible delay until it again runs at the speed Vi.
- the carbon fiber ribbon may not only be coated with 10 B or Gd as a neutron absorber, but also be impregnated with these materials in conjunction with a binder.
- the neutron absorber (region B) is then less susceptible to damage than a coating that can flake off in the course of bending the belt, such as when passing through rollers. Should the band break or lose its coating, it is advantageously much easier to replace than a voluminous and heavy wheel chopper, so that less of the precious measuring time is required for the repair.
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Particle Accelerators (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE102012020636.4A DE102012020636A1 (en) | 2012-10-20 | 2012-10-20 | Band-shaped chopper for a particle beam |
PCT/DE2013/000533 WO2014075649A1 (en) | 2012-10-20 | 2013-09-19 | Band-shaped chopper for a particle beam |
Publications (2)
Publication Number | Publication Date |
---|---|
EP2909840A1 true EP2909840A1 (en) | 2015-08-26 |
EP2909840B1 EP2909840B1 (en) | 2021-03-31 |
Family
ID=49724428
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP13801464.2A Active EP2909840B1 (en) | 2012-10-20 | 2013-09-19 | Band-shaped chopper for a particle beam |
Country Status (5)
Country | Link |
---|---|
US (1) | US9330802B2 (en) |
EP (1) | EP2909840B1 (en) |
JP (1) | JP6261597B2 (en) |
DE (2) | DE102012020636A1 (en) |
WO (1) | WO2014075649A1 (en) |
Family Cites Families (22)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2673297A (en) * | 1949-06-13 | 1954-03-23 | Phillips Petroleum Co | Analyzing and control device |
US2926253A (en) * | 1954-12-22 | 1960-02-23 | Distillers Co Yeast Ltd | Radiation analysis |
US3184679A (en) * | 1961-10-17 | 1965-05-18 | Texas Instruments Inc | Multi-phase signal processor for light line optical correlator |
JPS4527652Y1 (en) * | 1966-12-29 | 1970-10-26 | ||
JPS545199A (en) * | 1977-06-15 | 1979-01-16 | Mitsubishi Heavy Ind Ltd | High speed opening and clothing valve |
US5533692A (en) * | 1979-01-30 | 1996-07-09 | Oerlikon-Contraves Ag | Beamrider guidance system using digital phase modulation encoding |
DE8436281U1 (en) * | 1984-12-11 | 1986-04-10 | Siemens AG, 1000 Berlin und 8000 München | Primary radiation diaphragm for X-ray examination equipment |
JP2744245B2 (en) * | 1988-03-25 | 1998-04-28 | キヤノン株式会社 | Exposure apparatus and exposure method |
US5365561A (en) * | 1988-03-25 | 1994-11-15 | Canon Kabushiki Kaisha | Exposure control in an X-ray exposure apparatus |
JPH0747095B2 (en) * | 1989-02-08 | 1995-05-24 | 富士電機株式会社 | Electro-osmotic dehydrator |
US4969174A (en) * | 1989-09-06 | 1990-11-06 | General Electric Company | Scanning mammography system with reduced scatter radiation |
JPH0562885A (en) * | 1991-09-03 | 1993-03-12 | Canon Inc | Sor exposure system |
JPH0743498A (en) * | 1993-07-30 | 1995-02-14 | Seiko Seiki Co Ltd | Collimator of neutron chopper and manufacture thereof |
US5686722A (en) * | 1996-02-28 | 1997-11-11 | Her Majesty The Queen In Right Of Canada, As Represented By The Minister Of National Defence Of Her Majesty's Canadian Government | Selective wavelength identification friend or foe (SWIFF) |
JP4346320B2 (en) * | 2003-02-05 | 2009-10-21 | 大日本印刷株式会社 | Exposure method and exposure apparatus |
DE102004002326A1 (en) | 2004-01-16 | 2005-08-04 | Forschungszentrum Jülich GmbH | rotor |
JP4227065B2 (en) * | 2004-04-16 | 2009-02-18 | 株式会社神戸製鋼所 | Neutron disc chopper |
DE202004011832U1 (en) * | 2004-07-28 | 2004-11-04 | Lambda Physik Ag | Light beam blocking system for machining laser with synchronized triggering uses chopper disk with opaque sectors and laser trigger pulses may be synchronized with rotation of disk |
JP2006264329A (en) * | 2005-02-28 | 2006-10-05 | Toray Ind Inc | Fiber-reinforced plastic long sheet and its manufacturing method |
DE102007046739A1 (en) * | 2007-09-28 | 2009-07-23 | Forschungszentrum Jülich GmbH | Chopper for a particle beam |
US7593510B2 (en) | 2007-10-23 | 2009-09-22 | American Science And Engineering, Inc. | X-ray imaging with continuously variable zoom and lateral relative displacement of the source |
EP2548207B1 (en) | 2010-03-14 | 2020-02-12 | Rapiscan Systems, Inc. | Beam forming apparatus |
-
2012
- 2012-10-20 DE DE102012020636.4A patent/DE102012020636A1/en not_active Withdrawn
-
2013
- 2013-09-19 JP JP2015537141A patent/JP6261597B2/en not_active Expired - Fee Related
- 2013-09-19 US US14/434,612 patent/US9330802B2/en not_active Expired - Fee Related
- 2013-09-19 EP EP13801464.2A patent/EP2909840B1/en active Active
- 2013-09-19 DE DE112013005055.2T patent/DE112013005055A5/en not_active Withdrawn
- 2013-09-19 WO PCT/DE2013/000533 patent/WO2014075649A1/en active Application Filing
Non-Patent Citations (1)
Title |
---|
See references of WO2014075649A1 * |
Also Published As
Publication number | Publication date |
---|---|
EP2909840B1 (en) | 2021-03-31 |
US20150279494A1 (en) | 2015-10-01 |
JP6261597B2 (en) | 2018-01-17 |
DE112013005055A5 (en) | 2015-07-02 |
WO2014075649A1 (en) | 2014-05-22 |
JP2015533414A (en) | 2015-11-24 |
US9330802B2 (en) | 2016-05-03 |
DE102012020636A1 (en) | 2014-04-24 |
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