JPH0470760B2 - - Google Patents
Info
- Publication number
- JPH0470760B2 JPH0470760B2 JP9108084A JP9108084A JPH0470760B2 JP H0470760 B2 JPH0470760 B2 JP H0470760B2 JP 9108084 A JP9108084 A JP 9108084A JP 9108084 A JP9108084 A JP 9108084A JP H0470760 B2 JPH0470760 B2 JP H0470760B2
- Authority
- JP
- Japan
- Prior art keywords
- tube
- exhaust
- accelerator
- acceleration
- microwaves
- 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
- 230000001133 acceleration Effects 0.000 claims description 19
- 239000002245 particle Substances 0.000 claims description 8
- 230000005684 electric field Effects 0.000 claims description 6
- 230000007423 decrease Effects 0.000 description 3
- 230000005672 electromagnetic field Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000005192 partition Methods 0.000 description 2
- 230000002411 adverse Effects 0.000 description 1
- 230000004323 axial length Effects 0.000 description 1
Landscapes
- Particle Accelerators (AREA)
Description
【発明の詳細な説明】 本発明は線型加速器用加速管に関する。[Detailed description of the invention] The present invention relates to an acceleration tube for a linear accelerator.
荷電粒子をマイクロ波で形成した電界により加
速する線型加速器は、超高真空下で運転しなけれ
ばならない。 Linear accelerators, which accelerate charged particles using electric fields created by microwaves, must operate under ultrahigh vacuum conditions.
しかしながら、前記加速管は荷電粒子を加速す
るためにその管内に互に連通する軸方向に沿つた
多数個の空洞共振器により形成されており、しか
も長いので、その両端から真空ポンプで排気した
場合、加速管内壁からの放出ガスによる管の中央
部の圧力は両端部のように低くならず、また管壁
から急激なガス放出があつた場合、管内の圧力が
低下するのに要する時間が長い。 However, since the accelerator tube is formed of a large number of cavity resonators along the axial direction that communicate with each other in the tube in order to accelerate charged particles, and is long, it is necessary to exhaust the gas from both ends with a vacuum pump. , the pressure in the center of the tube due to gas released from the inner wall of the accelerator tube does not drop as low as at both ends, and when there is sudden gas release from the tube wall, it takes a long time for the pressure inside the tube to decrease. .
本発明は加速管内壁からの放出ガスに基づく加
速管内の圧力がビーム加速運転できる値まで低下
するのに要する時間を短かくし、また運転時の加
速管内圧力を低くすることをその目的としたもの
で、多数個の直列につながる空洞共振器から成る
長尺の加速管内をその端部から真空ポンプで排気
し、超高真空下の該加速管内で荷電粒子をマイク
ロ波で形成した電界により加速する線型加速器に
おいて、各空洞共振器の管壁に縦横比の大きい軸
方向に長尺の排気孔を複数個軸対称に設け、該排
気孔を通して該加速管を抱く排気管による排気を
付加したことを特徴とする。 The purpose of the present invention is to shorten the time required for the pressure inside the acceleration tube, which is based on the gas released from the inner wall of the acceleration tube, to drop to a value that allows beam acceleration operation, and to lower the pressure inside the acceleration tube during operation. Then, a long acceleration tube consisting of a large number of cavity resonators connected in series is evacuated from its end using a vacuum pump, and charged particles are accelerated in the acceleration tube under an ultra-high vacuum using an electric field created by microwaves. In a linear accelerator, a plurality of elongated exhaust holes with a large aspect ratio are provided in the tube wall of each cavity resonator in an axially symmetrical manner, and exhaust air is added by an exhaust pipe that holds the acceleration tube through the exhaust holes. Features.
以下本発明の実施例を図面につき説明する。 Embodiments of the present invention will be described below with reference to the drawings.
図面において、1は長尺の加速管で、該加速管
1は内壁に軸方向に沿つて所定間隔毎に中心に孔
2を有する隔壁板3が一体に形成されて複数個の
空洞4が形成され、適宜個所から導入されたマイ
クロ波に対し各空洞4を共振器として作用させて
荷電粒子を加速するようにしたものである。5は
加速管1の管壁に軸方向に長尺の排気孔で、該排
気孔5は例えば4個を軸対称に設けた。6は該排
気孔5に連なり適所から図示しない真空ポンプで
排気される排気管である。 In the drawings, reference numeral 1 denotes a long acceleration tube, and the acceleration tube 1 is integrally formed with partition plates 3 having holes 2 in the center at predetermined intervals along the axial direction on the inner wall, thereby forming a plurality of cavities 4. Each cavity 4 acts as a resonator for microwaves introduced from appropriate locations to accelerate charged particles. Reference numeral 5 denotes an axially elongated exhaust hole in the tube wall of the acceleration tube 1, and for example, four exhaust holes 5 are provided axially symmetrically. Reference numeral 6 denotes an exhaust pipe which is connected to the exhaust hole 5 and is exhausted from a suitable position by a vacuum pump (not shown).
前記排気孔5は、その管の周方向の幅を管内の
マイクロ波による軸対象電磁場に悪影響を及ぼさ
ない程度の大きさとし、管の軸方向の長さをその
孔5の数と関連するが、必要なガス排出性能が得
られる大きさとし、また適所から導入されたマイ
クロ波が外部に対して遮断される大きさ以下とし
た。 The exhaust holes 5 have a width in the circumferential direction of the tube such that it does not adversely affect the axially symmetric electromagnetic field due to microwaves in the tube, and the length in the axial direction of the tube is related to the number of holes 5, The size was chosen so that the necessary gas exhaust performance could be obtained, and the size was chosen so that microwaves introduced from a suitable location would be blocked from the outside.
次にその作動について説明する。 Next, its operation will be explained.
加速管1は、図示しない真空ポンプにより両端
から排気され、同時にその軸に沿つて穿設された
軸方向に長尺の排気孔5から排気管6を介して排
気されているので、管内の中央部及び両端部は一
様に排気されて圧力が低下し、また何等かの原因
で管壁等から急激なガス放出があつて管内圧力が
上昇しても速やかに圧力が低下する。かくてこの
管内に図示しない荷電粒子源から荷電粒子例えば
電子が入射すると、該電子は管内に導入されたマ
イクロ波で形成された軸方向の電界によつて超高
真空下を軸7に沿つて支障なく加速される。 The acceleration tube 1 is evacuated from both ends by a vacuum pump (not shown), and at the same time is exhausted from an axially long exhaust hole 5 drilled along its axis via an exhaust pipe 6, so that the center of the tube The tube and both ends are uniformly evacuated and the pressure decreases, and even if the pressure inside the tube increases due to sudden gas release from the tube wall or the like for some reason, the pressure quickly decreases. Thus, when charged particles, such as electrons, enter the tube from a charged particle source (not shown), the electrons are moved along the axis 7 under ultra-high vacuum by the axial electric field formed by the microwave introduced into the tube. Accelerates without any problem.
前記排気孔5は管の周方向の長さが短いので、
マイクロ波による軸対称電磁場に与える影響が少
なく、また管の軸方向の長さが長いので、管の周
方向に電流が流れるのを妨げるように作用し、そ
の結果、ビームの管軸からの発散の原因となりう
る非軸対称電磁場が発生しにくくなる。したがつ
て、軸方向に長尺の排気孔5はその周方向の長さ
に等しい丸孔に比べて電子の加速性能が高い。更
にまた、該丸孔に比べて(排気孔5の軸方向の長
さr)/(周方向の長さr′)倍の排気性能が得ら
れる。 Since the exhaust hole 5 has a short length in the circumferential direction of the pipe,
The microwave has little effect on the axially symmetrical electromagnetic field, and the length of the tube in the axial direction is long, so it acts to prevent the current from flowing in the circumferential direction of the tube, and as a result, the beam diverges from the tube axis. Non-axisymmetric electromagnetic fields that can cause problems are less likely to occur. Therefore, the axially long exhaust hole 5 has a higher electron acceleration performance than a round hole whose length in the circumferential direction is equal to that of the exhaust hole 5. Furthermore, compared to the round hole, an exhaust performance that is (axial length r of the exhaust hole 5)/(circumferential length r') can be obtained.
このように本発明によるときは、多数の空洞共
振器からなる長尺の加速管内をその端部から真空
ポンプで排気し、超高速真空下の加速管内で荷電
粒子をマイクロ波で形成した電界により加速する
線型加速器において、前記各空洞共振器の管壁に
軸方向に長尺の排気孔を軸対称に設けることによ
り、加速管内の中央部及び端部を一様に排気する
ことができ、このため加速管内壁からの放出ガス
による圧力を短時間のうちに低下させ装置の運転
を始めることができる。また加速管内において急
激なガスの放出があつた場合でも速やかに圧力を
低下させることができる。このときマイクロ波で
形成される電界を悪化することがないため電子の
加速に支障を生じない効果を有する。 As described above, according to the present invention, the inside of a long acceleration tube consisting of a large number of cavity resonators is evacuated from its end with a vacuum pump, and charged particles are generated by an electric field generated by microwaves inside the acceleration tube under an ultrahigh-speed vacuum. In an accelerating linear accelerator, by axially symmetrically providing elongated exhaust holes in the tube wall of each cavity resonator, the center and ends of the acceleration tube can be uniformly exhausted. Therefore, the pressure due to the gas released from the inner wall of the accelerator tube can be reduced in a short time, and the device can be started operating. Furthermore, even if there is a sudden release of gas within the accelerator tube, the pressure can be quickly reduced. At this time, since the electric field formed by the microwave is not deteriorated, there is an effect that acceleration of electrons is not hindered.
第1図は本発明の一実施例の要部の断面図、第
2図は第1図のA−A線断面図を示す。
1……加速管、2……孔、3……隔壁板、4…
…空洞、5……排気孔、6……排気管、7……
軸。
FIG. 1 is a sectional view of a main part of an embodiment of the present invention, and FIG. 2 is a sectional view taken along the line A--A in FIG. 1... Accelerator tube, 2... Hole, 3... Partition plate, 4...
...Cavity, 5...Exhaust hole, 6...Exhaust pipe, 7...
shaft.
Claims (1)
長尺の加速管内をその端部から真空ポンプで排気
し、超高真空下の該加速管内で荷電粒子をマイク
ロ波で形成した電界により加速する線型加速器に
おいて、各空洞共振器の管壁に縦横比の大きい軸
方向に長尺の排気孔を複数個軸対称に設け、該排
気孔を通して該加速管を抱く排気管による排気を
付加したことを特徴とする線型加速器用加速管。1 A linear type in which a long acceleration tube consisting of a large number of cavity resonators connected in series is evacuated from the end with a vacuum pump, and charged particles are accelerated in the tube under ultra-high vacuum by an electric field created by microwaves. In the accelerator, a plurality of elongated exhaust holes having a large aspect ratio in the axial direction are provided in the tube wall of each cavity resonator in an axially symmetrical manner, and exhaust is added by an exhaust pipe that hugs the acceleration tube through the exhaust holes. Accelerator tube for linear accelerator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9108084A JPS60236499A (en) | 1984-05-09 | 1984-05-09 | Accelerating tube for linear accelerator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9108084A JPS60236499A (en) | 1984-05-09 | 1984-05-09 | Accelerating tube for linear accelerator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS60236499A JPS60236499A (en) | 1985-11-25 |
JPH0470760B2 true JPH0470760B2 (en) | 1992-11-11 |
Family
ID=14016531
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9108084A Granted JPS60236499A (en) | 1984-05-09 | 1984-05-09 | Accelerating tube for linear accelerator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60236499A (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5812969B2 (en) | 2012-11-07 | 2015-11-17 | 三菱重工業株式会社 | Accelerating tube |
-
1984
- 1984-05-09 JP JP9108084A patent/JPS60236499A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS60236499A (en) | 1985-11-25 |
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