JP2952011B2 - Charged particle device - Google Patents
Charged particle deviceInfo
- Publication number
- JP2952011B2 JP2952011B2 JP2194806A JP19480690A JP2952011B2 JP 2952011 B2 JP2952011 B2 JP 2952011B2 JP 2194806 A JP2194806 A JP 2194806A JP 19480690 A JP19480690 A JP 19480690A JP 2952011 B2 JP2952011 B2 JP 2952011B2
- Authority
- JP
- Japan
- Prior art keywords
- quadrupole electromagnet
- charged particle
- gear
- quadrupole
- particle device
- 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 - Fee Related
Links
Landscapes
- Particle Accelerators (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] この発明は、荷電粒子、例えば電子やイオンのビーム
を輸送、加速、減速および蓄積する荷電粒子装置に関す
るものである。Description: TECHNICAL FIELD The present invention relates to a charged particle device for transporting, accelerating, decelerating, and accumulating a beam of charged particles, for example, electrons and ions.
[従来の技術] 従来、この種の荷電粒子装置については、分子科学研
究所発行“UVSORストレージリングの設計"UVSOR−9(1
982年12月)に記載されたものがある。[Prior art] Conventionally, this type of charged particle device has been described in “Design of UVSOR Storage Ring” published by Institute of Molecular Science, UVSOR-9 (1
December 982).
第5図は従来の4極電磁石(1)を示す断面図、第6
図はスキュー電磁石(2)の断面図を示していて、
(3)はこれらを支える架台、(4)は荷電粒子の通過
するビームダクトである。第7図はこれらを蓄積リング
の一部に組み込んだ例を示す。FIG. 5 is a sectional view showing a conventional quadrupole electromagnet (1), and FIG.
The figure shows a cross-sectional view of the skew electromagnet (2).
(3) is a gantry for supporting them, and (4) is a beam duct through which charged particles pass. FIG. 7 shows an example in which these are incorporated in a part of the storage ring.
次に動作について説明する。ビームダクト(4)内を
通過する荷電粒子の束(ビーム)は、4極電磁石(1)
によって作られた磁場によって、x方向とy方向に収束
や発散の力を受け、ビーム光学上のレンズの働きをし、
蓄積リングにおいては、ベータトロン凾数等のパラメー
タを決定する(x方向は蓄積リングにおいてビーム偏向
面内でビーム進行方向と垂直な方向、y方向はビーム進
行方向とx方向に垂直な方向)。一方、スキュー4極電
磁石(2)は、4極電磁石(1)をビーム軸を中心に45
゜回転したものに相当し、その作る磁場によって蓄積リ
ング等においてx方向とy方向のエミッタンスという量
の結合度を調整し、結果としてビーム形状のうちX方向
とy方向の大きさの比をコントロールするために用いら
れる。Next, the operation will be described. The bundle (beam) of charged particles passing through the inside of the beam duct (4) is a quadrupole electromagnet (1)
By the magnetic field created by the convergence and divergence force in the x and y directions, acting as a lens on the beam optics,
In the storage ring, parameters such as betatron function are determined (the x direction is a direction perpendicular to the beam advancing direction in the beam deflection plane in the storage ring, and the y direction is a direction perpendicular to the beam advancing direction and the x direction). On the other hand, the skew quadrupole electromagnet (2) is constructed such that the quadrupole electromagnet (1) is
相当 It is equivalent to a rotated one and adjusts the degree of coupling in the x- and y-directions in the storage ring etc. by the magnetic field created by the magnetic field, and as a result, controls the ratio of the beam shape in the X-direction and the y-direction. Used to
[発明が解決しようとする課題] 以上のような従来の荷電粒子装置は、4極電磁石およ
びスキュー4極電磁石がビーム軸に関して固定されてい
たので、ビーム形状のうちのx方向とy方向の大きさの
比を制御するためには、4極電磁石の他にスキュー4極
電磁石を用いなければならず、電磁石やそれに必要な電
源の個数が増えるのみならず、ビーム軌道方向の空間的
取合いを苦しくするという問題があつた。[Problems to be Solved by the Invention] In the conventional charged particle device as described above, since the quadrupole electromagnet and the skew quadrupole electromagnet are fixed with respect to the beam axis, the size of the beam shape in the x and y directions is large. In order to control the height ratio, it is necessary to use a skew quadrupole electromagnet in addition to the quadrupole electromagnet, which not only increases the number of electromagnets and the necessary power supplies, but also makes the spatial arrangement in the beam orbit direction difficult. There was a problem of doing.
この発明は上記のような問題点を解消するためになさ
れたもので、磁石や電源の数を節約したシステムを構築
するとともに、わずかなスペースでビーム光学上のパラ
メータの他にビーム断面形状のx方向とy方向の大きさ
の比を任意に変えることを可能にする荷電粒子装置を得
ることを目的とする。SUMMARY OF THE INVENTION The present invention has been made to solve the above-described problems. In addition to constructing a system in which the number of magnets and power supplies is reduced, the beam cross-sectional shape and the beam optics parameters are reduced in a small space. It is an object of the present invention to obtain a charged particle device that enables the ratio of the size in the direction to the size in the y direction to be arbitrarily changed.
[課題を解決するための手段] この発明に係る荷電粒子装置は、4極電磁石にビーム
軸を中心に回転できるような駆動装置を付設し、その回
転角度を調整できるようにしたものである。[Means for Solving the Problems] In the charged particle device according to the present invention, a drive device that can rotate around a beam axis is attached to a quadrupole electromagnet so that the rotation angle can be adjusted.
[作 用] この発明においては、4極電磁石は、ビーム軸を中心
に任意の角度だけ回転できるような駆動装置により、そ
の作る4極磁場の向きをビーム軸に垂直な面内の任意の
方向にとることができる。そこでビーム軸のまわりの回
転角と、4極磁場の強さを制御することにより、ビーム
x方向、y方向の収束、発散のみならず、ビーム断面形
状のx方向、y方向の比を任意に変えることができる。[Operation] In the present invention, the quadrupole electromagnet is rotated by an arbitrary angle about the beam axis by a driving device so that the direction of the quadrupole magnetic field to be produced is changed in an arbitrary direction in a plane perpendicular to the beam axis. Can be taken. Therefore, by controlling the rotation angle around the beam axis and the strength of the quadrupole magnetic field, not only the convergence and divergence of the beam in the x and y directions but also the ratio of the beam cross-sectional shape in the x and y directions can be arbitrarily determined. Can be changed.
[実施例] 以下、この発明の一実施例を第1図、第2図について
説明する。Embodiment An embodiment of the present invention will be described below with reference to FIGS.
図において、(1)は4極電磁石、(4)はビームダ
クト、(5)はステッピングモータ、(6)はこのモー
タの軸に取付けられた歯車、(7)はビームダクト
(4)を中心軸として回転する歯車であり、4極電磁石
(1)を支持している。(8)は歯車(7)が滑らかに
回転できるようにした支持枠であり、(3)は支持枠
(8)やステッピングモータ(5)を固定する架台であ
る。歯車(6)は歯車(7)とかみ合わせてある。In the figure, (1) is a quadrupole electromagnet, (4) is a beam duct, (5) is a stepping motor, (6) is a gear mounted on a shaft of the motor, and (7) is a center of the beam duct (4). The gear rotates as a shaft, and supports the quadrupole electromagnet (1). (8) is a support frame that allows the gear (7) to rotate smoothly, and (3) is a mount that fixes the support frame (8) and the stepping motor (5). Gear (6) meshes with gear (7).
次に動作について説明する。ステッピングモータ
(5)を動かすと、歯車(6)が回転し、支持枠(8)
によって支えられた歯車(7)が回転する。歯車(7)
は4極電磁石(1)を支持しているので、4極電磁石
(1)のつくる磁場は、従ってビームダクト(4)を中
心に回転することになる。そこで、ビームのx方向,y方
向の収束、発散力、並びにx方向,y方向のエミッタンス
の結合度、つまりビーム断面形状のx方向とy方向の大
きさの比を任意の値にするために、4極磁場の回転角と
4極磁場の大きさを定める。Next, the operation will be described. When the stepping motor (5) is moved, the gear (6) rotates and the support frame (8)
The gear (7) supported by the shaft rotates. Gear (7)
Supports the quadrupole electromagnet (1), the magnetic field created by the quadrupole electromagnet (1) will therefore rotate about the beam duct (4). Therefore, in order to set the convergence and divergence of the beam in the x and y directions, and the degree of coupling of the emittance in the x and y directions, that is, the ratio of the size of the beam cross-sectional shape in the x and y directions to an arbitrary value. The rotation angle of the quadrupole magnetic field and the magnitude of the quadrupole magnetic field are determined.
第3図,第4図は他の実施例を示し、4極電磁石
(1)とステッピングモータ(5)と、その軸に取付け
られた歯車(6)を支持枠(9)に取付け、ビームダク
ト(4)に固定されている支持枠(10)に歯車(7)が
取付けられ、歯車(6)とかみ合わさって、支持枠
(9)がビームダクト(4)を中心に滑らかに回転でき
るようになっている。従って、この場合はステッピング
モータ(5)自体が4極電磁石(1)とともに回転する
ように構成されおり、また、装置全体を支持する架台も
必要がない。FIGS. 3 and 4 show another embodiment, in which a quadrupole electromagnet (1), a stepping motor (5) and a gear (6) mounted on its shaft are mounted on a support frame (9), and a beam duct is mounted. A gear (7) is attached to a support frame (10) fixed to (4), and meshes with the gear (6) so that the support frame (9) can rotate smoothly about the beam duct (4). It has become. Therefore, in this case, the stepping motor (5) itself is configured to rotate together with the quadrupole electromagnet (1), and there is no need for a stand for supporting the entire apparatus.
なお、上記実施例では、歯車のかみ合わせを用いた
が、車などを使った摩擦を利用したものや、ベルトやチ
ェーンなどの動力伝達方法でもよい。またステッピング
モータを用いているが、制御できるものなら他の駆動装
置でもよい。In the above embodiment, the meshing of the gears is used, but a method using friction using a car or the like, or a power transmission method such as a belt or a chain may be used. Although a stepping motor is used, other drive devices may be used as long as they can be controlled.
[発明の効果] 以上のように、この発明によれば、4極電磁石をビー
ム軸を中心に任意の角度に回転できるように構成したの
で、これまで4極電磁石とスキュー4極電磁石を使って
行なっていたビームパラメータの調整が、安価な構造で
達成され、またこの装置を取付けるためのビーム軌道方
向の空間も少なくてすむという効果がある。[Effects of the Invention] As described above, according to the present invention, the quadrupole electromagnet is configured to be able to rotate at an arbitrary angle about the beam axis, so that the quadrupole electromagnet and the skew quadrupole electromagnet have been used. The adjustment of the beam parameters, which has been performed, can be achieved with an inexpensive structure, and there is an effect that the space in the beam trajectory direction for mounting the device is reduced.
第1図はこの発明の一実施例の立断面図、第2図は同じ
く側面図、第3図は他の実施例の立断面図、第4図は同
じく側面図、第5図および第6図はそれぞれ従来の荷電
粒子装置の一部立断面図、第7図は同じく斜視図であ
る。 (1)……4極電磁石、(4)……ビームダクト、
(5)……ステッピングモータ、(6)……歯車、
(7)……歯車、(8)……支持枠。 なお、各図中、同一符号は同一又は相当部分を示す。FIG. 1 is an elevational sectional view of one embodiment of the present invention, FIG. 2 is a side elevational view, FIG. 3 is an elevational elevational view of another embodiment, FIG. 4 is a side elevational view, FIG. The figures are each a partial cross-sectional view of a conventional charged particle device, and FIG. 7 is a perspective view of the same. (1) ... 4-pole electromagnet, (4) ... beam duct,
(5) Stepping motor, (6) Gear,
(7) ... gear, (8) ... support frame. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (1)
軌道軸を中心とする任意の角度の回転を与える駆動装置
とを備えてなる荷電粒子装置。1. A charged particle device comprising: a quadrupole electromagnet; and a drive device for rotating the quadrupole electromagnet at an arbitrary angle about a charged particle orbit axis.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2194806A JP2952011B2 (en) | 1990-07-25 | 1990-07-25 | Charged particle device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2194806A JP2952011B2 (en) | 1990-07-25 | 1990-07-25 | Charged particle device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0481700A JPH0481700A (en) | 1992-03-16 |
| JP2952011B2 true JP2952011B2 (en) | 1999-09-20 |
Family
ID=16330569
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2194806A Expired - Fee Related JP2952011B2 (en) | 1990-07-25 | 1990-07-25 | Charged particle device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2952011B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7166214B2 (en) | 2004-09-29 | 2007-01-23 | 3Ma Solutions Incorporated | Dental amalgam separator |
-
1990
- 1990-07-25 JP JP2194806A patent/JP2952011B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0481700A (en) | 1992-03-16 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |