JPH063496A - Device for generating radial beams - Google Patents

Device for generating radial beams

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Publication number
JPH063496A
JPH063496A JP16455792A JP16455792A JPH063496A JP H063496 A JPH063496 A JP H063496A JP 16455792 A JP16455792 A JP 16455792A JP 16455792 A JP16455792 A JP 16455792A JP H063496 A JPH063496 A JP H063496A
Authority
JP
Japan
Prior art keywords
electron beam
magnetic field
synchrotron radiation
deflected
deflection electromagnet
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.)
Pending
Application number
JP16455792A
Other languages
Japanese (ja)
Inventor
Yoshibumi Hojo
義文 北條
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP16455792A priority Critical patent/JPH063496A/en
Publication of JPH063496A publication Critical patent/JPH063496A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【構成】放射光発生装置は、部分的に磁場強度の異なる
偏向電磁石2、偏向電磁石の2極間に位置し電子ビーム
を入出射するためのビームダクト5,6と複数の放射光
取り出し口7を有する真空容器3から構成される。本発
明の放射光発生装置に入射した電子ビームは磁場強度分
布の影響で軌道半径を変えながら360°またはその整
数倍に近い偏向を受けた後に出射する。 【効果】放射光発生装置に入射した電子ビームはほぼ3
60°の整数倍の偏向を受けて出射するため、放射光発
生部である偏向部を増すために追加しなければならない
磁石の台数は最小限になる。
(57) [Summary] [Structure] A synchrotron radiation generator comprises a deflecting electromagnet 2 having partially different magnetic field strengths, a plurality of beam ducts 5 and 6 located between two poles of the deflecting electromagnet for entering and exiting an electron beam. It is composed of a vacuum container 3 having a radiant light extraction port 7. The electron beam incident on the synchrotron radiation generator of the present invention is deflected by 360 ° or an integer multiple thereof while changing the orbital radius under the influence of the magnetic field intensity distribution, and then is emitted. [Effect] The electron beam incident on the synchrotron radiation generator is almost 3
Since the light is output after being deflected by an integral multiple of 60 °, the number of magnets that must be added in order to increase the deflection unit that is the radiation light generation unit is minimized.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、工業用の放射光発生装
置に係り、特に、多数の放射光光源が必要な放射光発生
施設に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an industrial radiation light generator, and more particularly to a radiation light generation facility that requires a large number of radiation light sources.

【0002】[0002]

【従来の技術】従来の放射光発生施設では電子蓄積リン
グの偏向部から放射光を取り出すので、放射光光源とな
る偏向部の角度の総和は360°であり、偏向部を増す
ための装置は特開平1−186798 号公報に示されるよう
に、複数台の偏向電磁石を追加する。
2. Description of the Related Art In a conventional synchrotron radiation generating facility, radiant light is extracted from a deflector of an electron storage ring. Therefore, the total angle of the deflector serving as a radiant light source is 360 °, and a device for increasing the deflector is As shown in JP-A-1-186798, a plurality of bending electromagnets are added.

【0003】[0003]

【発明が解決しようとする課題】従来の放射光発生施設
では放射光光源となる偏向部は軌道半径が一定の偏向電
磁石を用いており、各偏向部での偏向角は360°より
も小さくなければならない。従って、一平面内で偏向部
の総偏向角を360°よりも大きくするには最低二台の
極性の異なる偏向電磁石を追加しなければならなかっ
た。
In the conventional synchrotron radiation generating facility, the deflector serving as the radiant light source uses a deflecting electromagnet having a constant orbit radius, and the deflecting angle of each deflector must be smaller than 360 °. I have to. Therefore, at least two deflection electromagnets having different polarities had to be added in order to make the total deflection angle of the deflection section larger than 360 ° in one plane.

【0004】本発明の目的は、放射光発生部を増すため
に追加する偏向電磁石の台数を最低限にすることができ
る放射光発生装置を提供することにある。
An object of the present invention is to provide a radiant light generating device capable of minimizing the number of deflection electromagnets added to increase the radiant light generating portion.

【0005】[0005]

【課題を解決するための手段】本発明の特徴は、磁場強
度を部分的に変えた偏向電磁石、及び、入射した電子ビ
ームが偏向電磁石中で軌道半径を変えながら360°ま
たはその整数倍に近い偏向を受けて出射するように入出
射部を設けることにある。本発明の目的は、最小の台数
の電磁石の追加で放射光発生部を増すことができる放射
光発生装置を提供することにある。
The features of the present invention are a deflection electromagnet in which the magnetic field strength is partially changed, and an incident electron beam is approximately 360 ° or an integral multiple thereof while changing the orbital radius in the deflection electromagnet. An input / output unit is provided so as to be output by being deflected. An object of the present invention is to provide a radiant light generation device capable of increasing the radiant light generation unit by adding a minimum number of electromagnets.

【0006】[0006]

【作用】本発明の放射光発生装置で用いる偏向電磁石に
入射した電子ビームは、部分的に変化する磁場強度分布
によって偏向電磁石中で軌道半径を変えながら旋回す
る。この電子ビームが360°またはその整数倍に近い
偏向を受けたところで出射するように出射部を設けるこ
とによって最低一台の電磁石の追加で放射光発生部を増
すことができる。
The electron beam incident on the deflection electromagnet used in the synchrotron radiation generator of the present invention turns while changing the orbital radius in the deflection electromagnet due to the partially changing magnetic field intensity distribution. By providing the emitting portion so that the electron beam is emitted when it is deflected by 360 ° or an integral multiple thereof, it is possible to increase the emitted light generating portion by adding at least one electromagnet.

【0007】[0007]

【実施例】以下、本発明の実施例を図面を用いて説明す
る。図1は本発明の放射光発生装置の真空容器3を上か
ら見た断面図であり、電子ビーム軌道1も併わせて示し
てある。図2は本発明の放射光発生装置に用いる偏向電
磁石の単磁極形状の例である。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a cross-sectional view of the vacuum container 3 of the synchrotron radiation generating apparatus of the present invention seen from above, and also shows an electron beam trajectory 1. FIG. 2 shows an example of a single pole shape of a deflecting electromagnet used in the synchrotron radiation generating apparatus of the present invention.

【0008】図1に示した本発明の放射光発生装置は、
部分的に磁場強度の異なる偏向電磁石2、偏向電磁石の
2極間に位置し電子ビームを入出射するためのビームダ
クト5,6と複数の放射光取り出し口7を有する真空容
器3から構成される。また、磁極中ではあるがビーム軌
道が直線でなければならない部分には磁気シールド板4
が真空容器3の上下に取付けられている。その磁極中に
入射した電子ビーム1は磁気シールド部分4を出ると偏
向電磁石2中の磁場の影響を受けて円軌道を描く。この
実施例では電子ビーム1が進行するにつれて磁場強度が
強くなるようにしてあるので、電子ビーム1の軌道半径
は次第に小さくなり、ほぼ360°の偏向を受けて出射
用の磁気シールド部4に到達すると磁場の影響を受けな
くなって出射用ビームダクト6から出射する。このよう
にして、一つの偏向電磁石をビームラインに挿入するこ
とにより放射光発生部を増すことができる。電子ビーム
1の偏向角は360°の整数倍に近ければ何度でも良
い。
The radiation light generator of the present invention shown in FIG.
It is composed of a deflection electromagnet 2 having a partially different magnetic field strength, beam ducts 5 and 6 located between the two poles of the deflection electromagnet for entering and exiting an electron beam, and a vacuum container 3 having a plurality of radiation light extraction ports 7. . In addition, the magnetic shield plate 4 is provided in a portion of the magnetic pole where the beam trajectory must be a straight line.
Are attached above and below the vacuum container 3. When the electron beam 1 that has entered the magnetic pole exits the magnetic shield portion 4, it is affected by the magnetic field in the deflection electromagnet 2 and draws a circular orbit. In this embodiment, since the magnetic field strength is made stronger as the electron beam 1 advances, the orbital radius of the electron beam 1 becomes gradually smaller and reaches the magnetic shield portion 4 for emission after being deflected by about 360 °. Then, the beam is not affected by the magnetic field and is emitted from the emission beam duct 6. In this way, the radiation light generator can be increased by inserting one deflection electromagnet into the beam line. The deflection angle of the electron beam 1 may be any number as long as it is close to an integral multiple of 360 °.

【0009】図2,図3はこのような軌道半径変化を起
こさせるための磁場分布を磁極間隔が異なる部分を作る
ことによって実現するための偏向電磁石2の磁極形状で
ある。図2は電子ビームが180°偏向したときに強い
磁場領域に入るものであり、図3は電子ビームの進行に
ともなって磁場強度が滑らかに強くなるものである。こ
の磁場強度分布は図1に示した電子ビーム軌道と類似の
軌道を実現できる分布であれば良い。
FIGS. 2 and 3 show the magnetic pole shape of the deflection electromagnet 2 for realizing the magnetic field distribution for causing such a change in the orbital radius by making portions having different magnetic pole intervals. FIG. 2 shows that the electron beam enters a strong magnetic field region when deflected by 180 °, and FIG. 3 shows that the magnetic field intensity smoothly increases as the electron beam advances. This magnetic field intensity distribution may be any distribution that can realize a trajectory similar to the electron beam trajectory shown in FIG.

【0010】[0010]

【発明の効果】本発明によれば、最小の台数の電磁石の
追加で放射光発生部を増すことができる放射光発生装置
を提供することができる。
According to the present invention, it is possible to provide a radiant light generating device capable of increasing the radiant light generating portion by adding a minimum number of electromagnets.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の放射光発生装置の真空容器を上から見
た説明図。
FIG. 1 is an explanatory view of a vacuum container of a synchrotron radiation generating apparatus of the present invention seen from above.

【図2】本発明の放射光発生装置に用いる偏向電磁石の
斜視図。
FIG. 2 is a perspective view of a bending electromagnet used in the synchrotron radiation generating apparatus of the present invention.

【図3】本発明の放射光発生装置に用いる偏向電磁石の
斜視図。
FIG. 3 is a perspective view of a bending electromagnet used in the synchrotron radiation generating apparatus of the present invention.

【符号の説明】[Explanation of symbols]

1…電子ビーム、2…偏向電磁石、3…真空容器、4…
磁気シールド板、5…入射用ビームダクト、6…出射用
ビームダクト、7…放射光取り出し口、10…磁場強度
変更用突出部。
1 ... Electron beam, 2 ... Bending electromagnet, 3 ... Vacuum container, 4 ...
Magnetic shield plate, 5 ... Incident beam duct, 6 ... Emitting beam duct, 7 ... Radiant light extraction port, 10 ... Projection portion for changing magnetic field strength.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】電子ビームを偏向し放射光を発生させる放
射光発生装置であって、磁場強度を部分的に変えた偏向
電磁石,前記偏向電磁石の2極間に位置し複数の放射光
取り出し口を有する真空容器、前記真空容器に前記電子
ビームを入出射するためのビームダクトから構成される
装置であって、前記偏向電磁石に入射した前記電子ビー
ムが前記偏向電磁石中で部分的に異なる磁場強度の影響
で軌道半径を変えながら360°またはその整数倍に近
い偏向を受けて出射するように入出射部を設けることを
特徴とする放射光発生装置。
1. A radiation light generator for deflecting an electron beam to generate radiation light, comprising a deflection electromagnet having a partially changed magnetic field strength, and a plurality of radiation light extraction ports located between two poles of the deflection electromagnet. And a beam duct for letting the electron beam into and out of the vacuum container, wherein the electron beam incident on the deflection electromagnet partially differs in magnetic field strength in the deflection electromagnet. The radiation light generation device is characterized in that an entrance / exit portion is provided so as to be emitted while being deflected by 360 ° or an integer multiple thereof while changing the orbital radius under the influence of.
JP16455792A 1992-06-23 1992-06-23 Device for generating radial beams Pending JPH063496A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16455792A JPH063496A (en) 1992-06-23 1992-06-23 Device for generating radial beams

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16455792A JPH063496A (en) 1992-06-23 1992-06-23 Device for generating radial beams

Publications (1)

Publication Number Publication Date
JPH063496A true JPH063496A (en) 1994-01-11

Family

ID=15795432

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16455792A Pending JPH063496A (en) 1992-06-23 1992-06-23 Device for generating radial beams

Country Status (1)

Country Link
JP (1) JPH063496A (en)

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