JPS62172699A - Magnetic field generator for plasma confinement - Google Patents
Magnetic field generator for plasma confinementInfo
- Publication number
- JPS62172699A JPS62172699A JP61013287A JP1328786A JPS62172699A JP S62172699 A JPS62172699 A JP S62172699A JP 61013287 A JP61013287 A JP 61013287A JP 1328786 A JP1328786 A JP 1328786A JP S62172699 A JPS62172699 A JP S62172699A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magnetic
- plasma confinement
- end surface
- outer end
- 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.)
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- Electron Sources, Ion Sources (AREA)
- Plasma Technology (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明はプラズマを安定して閉じ込めることのできる磁
場発生装置に関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magnetic field generator capable of stably confining plasma.
(従来の技術)
プラズマを発生して、このプラズマ中のイオンまたは電
子を利用することが今日種々の分野で広く行われている
。(Prior Art) Generating plasma and utilizing ions or electrons in the plasma is now widely practiced in various fields.
(発明が解決しようとする問題点)
しかしながら、高安定にプラズマを保持することができ
小型化に適したプラズマ閉込用磁場発生装置は従来提案
されていなかった。本発明の目的は高安定にプラズマを
保持することができ小型化に適したプラズマ閉込用磁場
発生装置を提供することにある。(Problems to be Solved by the Invention) However, a magnetic field generator for plasma confinement that is capable of retaining plasma in a highly stable manner and is suitable for miniaturization has not been proposed in the past. An object of the present invention is to provide a magnetic field generator for plasma confinement that can maintain plasma in a highly stable manner and is suitable for downsizing.
(問題点を解決するための手段)
上記目的は、外側端面と内側端面との間を結ぶ磁力線を
形成する、永久磁石から構成される一対の磁力線発生手
段からなり、この一対の磁力線発生手段のそれぞれの外
側端面と内側端面とが互いに対向しており、これら対向
した外側端面および内側端面同士の磁極が同極である本
発明のプラズマ閉込用磁場発生装置により、達成される
。本発明によると、磁力線発生手段の対向空間にカスプ
磁場が形成され、プラズマが高安定に閉じ込められる。(Means for solving the problem) The above object consists of a pair of magnetic force line generating means composed of permanent magnets that form magnetic force lines connecting an outer end surface and an inner end surface. This is achieved by the magnetic field generating device for plasma confinement of the present invention, in which the respective outer end faces and inner end faces are opposed to each other, and the magnetic poles of the opposed outer end faces and inner end faces are the same. According to the present invention, a cusp magnetic field is formed in a space facing the magnetic field line generating means, and plasma is confined in a highly stable manner.
本発明を、電子サイクロトロン共鳴によりプラズマを発
生するプラズマ発生装置として使用すると特に有効であ
る。The present invention is particularly effective when used as a plasma generator that generates plasma by electron cyclotron resonance.
(発明の効果)
本発明によると、比較的小型の装置により、人界1の強
いカスプ型プラズマ閉じ込め用磁場空間を作ることがで
きる。プラズマはこの磁場空間内に安定に閉じ込められ
、高温・高密度プラズマを掛ることができる。(Effects of the Invention) According to the present invention, a strong cusp-shaped plasma confinement magnetic field space of 1 can be created using a relatively small-sized device. Plasma is stably confined within this magnetic field space, making it possible to generate high-temperature, high-density plasma.
(実施例)
以下、本発明の実施例を図面を参照しつつ詳細に説明す
る。第1図は本発明の第1実施例の斜視図である。この
第1実施例は電子サイクロトロン共鳴型プラズマ発生装
置として用いることができる。外側端面1,1“と内側
端面2,2′との間を結ぶ磁力線3.3゛を形成する、
永久磁石4゜4“、5.5”から構成される一対の磁力
線発生手段6,6゛が示されている。この一対の磁力線
発生手段6.6”の各々の外側端面1と1′と内側端面
2と2′とが互いに垂直方向で対向しており、これら対
向した外側端面1,1“および内側端面2.2゛同士の
磁極は同極である。本実施例においては、磁力線発生手
段6,6′の外側端面1.1′と内側端面2,2゛とは
中心を輔7−7゜と一致させた円環状の形状を有してい
るので、これにともなって、磁力線3.3”は軸7−7
°に対して対称な円環状に形成されている。内側端面2
.2”は外側端面1,1°より後退しており、また磁力
線発生手段6,6゛の各々の外側端面1゜1°と各々の
内側端面2,2”との間には空隙が設けられており、こ
れによって形成された磁力線発生手段6.6′の対向空
間がプラズマ閉込用およびプラズマ発生用の空間として
使用される。外側端面1.1゛はヨーク8を介して対向
している。(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings. FIG. 1 is a perspective view of a first embodiment of the invention. This first embodiment can be used as an electron cyclotron resonance type plasma generator. Forming lines of magnetic force 3.3'' connecting the outer end surfaces 1, 1'' and the inner end surfaces 2, 2',
A pair of magnetic field line generating means 6, 6'', which are composed of permanent magnets 4.5'' and 4.5'', are shown. The outer end surfaces 1 and 1' and the inner end surfaces 2 and 2' of each of the pair of magnetic force line generating means 6.6'' are perpendicularly opposed to each other. .2's magnetic poles are the same. In this embodiment, the outer end surfaces 1.1' and the inner end surfaces 2, 2' of the magnetic force line generating means 6, 6' have an annular shape with their centers coincident with the legs 7-7°. , along with this, the magnetic field line 3.3" is the axis 7-7
It is formed in a ring shape that is symmetrical with respect to °. Inner end surface 2
.. 2" is set back from the outer end surface 1.1°, and a gap is provided between the outer end surface 1.1° of each of the magnetic force line generating means 6, 6" and the inner end surface 2, 2" of each. The space thus formed facing the magnetic force line generating means 6,6' is used as a space for plasma confinement and plasma generation. The outer end surfaces 1.1'' are opposed to each other with a yoke 8 interposed therebetween.
内側端面2,2°の中央部には外部に通じる開口10.
11が設けられており、開口10には電磁波入力用の絶
縁体の窓13とアンテナ16が挿入されており、開口1
1にはイオンビーム引出し用の電極14が挿入されてい
る。外側端面1.1゛間の外方に、外側端面1,1′の
磁極と同極の磁極が近接するようにして補極15が設置
されており、これによって、本来外方に漏れる外側端面
1゜1゛からの磁力線が内方に押し返えされ、外側端面
1,1°から磁力線をより効果的に配置するこができる
。電磁波入力用の絶縁体の窓13の周囲には、磁力線を
整磁または遮蔽する磁力線遮蔽体17が設けられており
、エネルギーを伝送の途中で損失することなく、対向空
間12の所望位置に電磁波を伝送することができる。こ
の様に構成された装置内が所定圧所望元素の雰囲気によ
って満たされた状態で、外部からアンテナ16を介して
対向空間12内に電磁波が導入されると、電子サイクロ
トロン共鳴現象によってプラズマが発生する。このよう
にして発生されたプラズマはイオン引出し電極14によ
って外部に引き出される。なお、磁石4,4′と磁石5
,5°との間に設けられた磁石18.18°は、装置の
内壁周辺部分の磁場の強度を高める補極である。本実施
例においては、真空容器22が対向空間12内に設けら
れており、この内部が高真空状態にされるようになって
いるが、磁力線発生手段6.6°が真空容器22を兼ね
るようにされていてもよいことは言うまでもない。いず
れの場合においても、外部から伝播搬入された電磁波が
空洞共振するように設計されていると、電磁波エネルギ
ーが有効利用されて好ましい。At the center of the inner end surface 2.2° is an opening 10 that leads to the outside.
11 is provided, and an insulating window 13 and an antenna 16 for inputting electromagnetic waves are inserted into the opening 10.
An electrode 14 for extracting the ion beam is inserted into the electrode 1 . A commutating pole 15 is installed outwardly between the outer end surfaces 1.1' so that magnetic poles of the same polarity as those of the outer end surfaces 1 and 1' are close to each other, and this prevents the outer end surface from leaking outward. The lines of magnetic force from 1.1° are pushed back inward, allowing the lines of magnetic force to be more effectively arranged from the outer end face 1.1°. A magnetic field line shield 17 is provided around the insulator window 13 for electromagnetic wave input to demagnetize or shield the magnetic field lines, and the electromagnetic waves are transmitted to a desired position in the facing space 12 without losing energy during transmission. can be transmitted. When electromagnetic waves are introduced from the outside into the facing space 12 via the antenna 16 while the inside of the apparatus configured in this manner is filled with an atmosphere of a desired element at a predetermined pressure, plasma is generated by an electron cyclotron resonance phenomenon. . The plasma thus generated is extracted to the outside by the ion extraction electrode 14. In addition, magnets 4, 4' and magnet 5
, 5° are interpolations that increase the strength of the magnetic field around the inner wall of the device. In this embodiment, the vacuum container 22 is provided in the opposing space 12, and the inside thereof is kept in a high vacuum state. Needless to say, it is okay to be left alone. In either case, it is preferable that the cavity be designed so that the electromagnetic waves propagated in from the outside resonate in the cavity, so that the electromagnetic wave energy can be used effectively.
第2図および第3図は上述した第1実錨例におけるそれ
ぞれ磁力線配位の様子を示す図および磁束密度の等高線
図であり、第4図および第5図は第1実施例において磁
石15を取り除いた場合のそれぞれ磁力線配位の様子を
示す図および磁束密度の等高線図である。これらの図か
ら、磁極I5の有無に係わらず、対向空間12には所望
する磁場配位が形成されているが、磁極15を付加する
ことにより、内壁面近くの磁場強度がより高くなり、プ
ラズマをより効果的に閉じ込めることができることがわ
かる。2 and 3 are diagrams showing the magnetic field line arrangement and magnetic flux density contour diagram, respectively, in the first example of the actual anchor described above, and FIGS. 4 and 5 show the magnet 15 in the first example. FIG. 7 is a diagram showing the configuration of magnetic lines of force when removed, and a contour diagram of magnetic flux density. From these figures, the desired magnetic field configuration is formed in the facing space 12 regardless of the presence or absence of the magnetic pole I5, but by adding the magnetic pole 15, the magnetic field strength near the inner wall surface becomes higher, and the plasma It can be seen that it is possible to confine more effectively.
第6図は本発明の第2実施例の断面斜視図である。本実
施例においては、外側端面l、1゛を有する円筒状永久
磁石4.4′と内側端面2,2”を有する円柱状永久磁
石21,21°とから一対の磁力線発生手段6,6゛が
構成されており、対向する端面同士の磁極は第1実施例
と同様に同極である。本実施例においては、内側端面2
,2゜の中央部に、外部に通じる開口は設けられておら
ず、電磁波の搬入およびイオンビームの引き出しは軸2
3−23’に沿って対向端面間に設けられた開口24.
25を介して行われる。即ち、開口24には電磁波人力
用の絶縁体の窓13とアンテナ16とが挿入されており
、開口25にはイオン引出し用電極14が抑大されてい
る。対向空間12内には真空容器22が設けられており
、この真、空容器22の一部は開口24.25内に導か
れてれおり、開口24内に導かれた真空容器の一部は、
電磁波入力用の窓13を包囲して、アンテナ16に強い
磁場が到らない様に、周囲の磁場を遮蔽あるいは整磁す
る。FIG. 6 is a cross-sectional perspective view of a second embodiment of the invention. In this embodiment, a pair of magnetic force line generating means 6, 6' is generated from a cylindrical permanent magnet 4.4' having outer end faces l, 1' and a cylindrical permanent magnet 21, 21° having inner end faces 2, 2". The magnetic poles of the opposing end surfaces are the same as in the first embodiment.In this embodiment, the inner end surface 2
, 2° is not provided with an opening leading to the outside, and the electromagnetic waves are brought in and the ion beam is extracted from the axis 2.
3-23' between the opposing end faces 24.
This is done via 25. That is, an insulating window 13 for electromagnetic wave input and an antenna 16 are inserted into the opening 24, and an ion extraction electrode 14 is suppressed in the opening 25. A vacuum container 22 is provided in the opposing space 12, and a part of the vacuum container 22 is guided into the opening 24.25, and a part of the vacuum container guided into the opening 24 is ,
The electromagnetic wave input window 13 is surrounded to shield or demagnetize the surrounding magnetic field so that a strong magnetic field does not reach the antenna 16.
第7図は本発明の第3実施例の側面図である。FIG. 7 is a side view of a third embodiment of the present invention.
本実施例においては、一体的に形成された磁石の外側部
分と内側部分とが反対方向に磁化されており、これによ
って外方端面1,1°と内方端面2゜2゛の磁極が異な
るようにされている。In this embodiment, the outer and inner parts of the integrally formed magnet are magnetized in opposite directions, so that the magnetic poles of the outer end face 1.1° and the inner end face 2°2° are different. It is like that.
第8図は本発明の第4実施例の磁力線発生手段6の端面
を示す平面図である。この実施例においては、外方端面
1および内方端面2に突出部分1a、2aが形成されて
おり、これら端面によって形成される磁力線は軸対称と
は成らない。この突出部分に形成される磁力線はちょう
ど4電極磁場を形成し、この部分からイオンの引き出し
を行うようにすることができる。FIG. 8 is a plan view showing an end face of the magnetic force line generating means 6 according to the fourth embodiment of the present invention. In this embodiment, protruding portions 1a and 2a are formed on the outer end face 1 and the inner end face 2, and the lines of magnetic force formed by these end faces are not axially symmetrical. The lines of magnetic force formed in this protruding portion form exactly a four-electrode magnetic field, and ions can be extracted from this portion.
第9図は本発明の第5実施例の磁力線発生手段6の端面
を示す平面図である。この実施例においては、外側端面
1および内側端面2は長円形をしており、これら端面間
に形成される磁力線もこの端面に沿って長円状に空間を
囲むように形成される。FIG. 9 is a plan view showing an end face of the magnetic force line generating means 6 according to the fifth embodiment of the present invention. In this embodiment, the outer end surface 1 and the inner end surface 2 have an oval shape, and the lines of magnetic force formed between these end surfaces are also formed so as to surround a space in an oval shape along these end surfaces.
第1図は本発明の第1実施例の断面斜視図、第2図およ
び第3図は第1実施例のそれぞれ磁力線配位図および磁
束密度の等高線図、
第4図および第5図は第1実施例から補極を除いた場合
のそれぞれ磁力線配位図および磁束密度の等高線図、
第6図は本発明の第2実施例の断面斜視図、第7図は本
発明の第3実施例の平面図、・第8図は本発明の第4実
施例の平面図、第9図は本発明の第5実施例の平面図。
1.1゛・・・・・・外側端面、2.2゛・・・・・・
内側端面、3.3°・・・・・・磁力線、
4.4”、5.5’、18.18”、21.21’・・
・・・・永久磁石、
6・・・・・・磁力線発生手段、
7.7’ 、23.23′・・・・・・軸、8.9.9
’・・・・・・ヨーク、
10.11,24.25・・・・・・開口、12・・・
・・・対向空間、13・・・・・・電磁波人力用の窓、
14・・・・・・電極、15・・・・・・磁極、16・
・・・・・アンテナ、17・・・・・・磁力線遮蔽体、
18.18’・・・・・・補極、22・・・・・・真空
容器。FIG. 1 is a cross-sectional perspective view of the first embodiment of the present invention, FIGS. 2 and 3 are magnetic field line arrangement diagrams and magnetic flux density contour diagrams of the first embodiment, respectively. FIG. 6 is a cross-sectional perspective view of the second embodiment of the present invention, and FIG. 7 is a third embodiment of the present invention. FIG. 8 is a plan view of a fourth embodiment of the present invention, and FIG. 9 is a plan view of a fifth embodiment of the present invention. 1.1゛・・・・・・Outer end surface, 2.2゛・・・・・・
Inner end face, 3.3°... Lines of magnetic force, 4.4", 5.5', 18.18", 21.21'...
...Permanent magnet, 6...Magnetic field line generating means, 7.7', 23.23'...Axis, 8.9.9
'... Yoke, 10.11, 24.25... Opening, 12...
...Opposing space, 13...Window for electromagnetic wave human power,
14... Electrode, 15... Magnetic pole, 16.
...Antenna, 17...Magnetic field line shield,
18.18'...Commuting electrode, 22...Vacuum container.
Claims (11)
る、永久磁石から構成される一対の磁力線発生手段から
なり、この一対の磁力線発生手段のそれぞれの外側端面
と内側端面とが互いに対向しており、これら対向した外
側端面および内側端面同士の磁極が同極であるプラズマ
閉込用磁場発生装置。(1) Consisting of a pair of magnetic force line generating means made of permanent magnets that form lines of magnetic force connecting the outer end surface and the inner end surface, and the outer end surface and inner end surface of each of the pair of magnetic force line generating means are opposed to each other. A magnetic field generator for plasma confinement, in which the magnetic poles of the opposing outer end faces and inner end faces are the same.
範囲第(1)項記載のプラズマ閉込用磁場発生装置。(2) The plasma confinement magnetic field generating device according to claim (1), wherein the magnetic lines of force are formed axially symmetrically.
範囲第(2)項記載のプラズマ閉込用磁場発生装置。(3) The plasma confinement magnetic field generating device according to claim (2), wherein the magnetic lines of force are formed in an annular shape.
内側端面との間に空隙が設けられている特許請求の範囲
第(1)項記載のプラズマ閉込用磁場発生装置。(4) A magnetic field generating device for plasma confinement according to claim (1), wherein a gap is provided between the outer end surface and the inner end surface of each of the magnetic force line generating means.
に空隙が形成されている特許請求の範囲第(1)項記載
のプラズマ閉込用磁場発生装置。(5) The plasma confinement magnetic field generating device according to claim 1, wherein a gap is formed between the opposing end surfaces of the pair of magnetic force line generating means.
特許請求の範囲第(1)項または第(4)項記載のプラ
ズマ閉込用磁場発生装置。(6) The magnetic field generating device for plasma confinement according to claim 1 or 4, wherein the inner end surface is set back from the outer end surface.
範囲第(6)項記載のプラズマ閉込用磁場発生装置。(7) The plasma confinement magnetic field generating device according to claim (6), wherein the opposing outer end surfaces are in close contact with each other.
られている特許請求の範囲第(1)項記載のプラズマ閉
込用磁場発生装置。(8) The magnetic field generating device for plasma confinement according to claim (1), wherein an opening leading to the outside is provided in the center of the inner end surface.
磁極と同極の磁極が設けられている特許請求の範囲第(
1)項記載のプラズマ閉込用磁場発生装置。(9) A magnetic pole having the same polarity as the magnetic pole of the outer end surface is provided adjacent to the outer side between the outer end surfaces.
1) The magnetic field generator for plasma confinement as described in item 1).
振する特許請求の範囲第(1)項記載のプラズマ閉込用
磁場発生装置。 外部との連絡箇所の周囲に磁力線遮蔽体を設けた特許請
求の範囲第(1)項記載のプラズマ閉込用磁場発生装置
。(10) A magnetic field generating device for plasma confinement according to claim (1), in which electromagnetic waves propagated from the outside resonate inside a cavity. A magnetic field generating device for plasma confinement according to claim 1, wherein a magnetic field line shield is provided around a communication point with the outside.
石の端面であり、それぞれの磁石の間に空隙が形成され
ており、前記磁石の前記端面とは反対側に磁路に沿って
磁化された永久磁石が設置されている特許請求の範囲第
(1)項記載のプラズマ閉込用磁場発生装置。(11) The outer end face and the inner end face are end faces of separate permanent magnets, a gap is formed between each magnet, and a gap is formed between the magnets along a magnetic path on the opposite side from the end face of the magnet. A magnetic field generating device for plasma confinement according to claim (1), wherein a magnetized permanent magnet is installed.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61013287A JPS62172699A (en) | 1986-01-24 | 1986-01-24 | Magnetic field generator for plasma confinement |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61013287A JPS62172699A (en) | 1986-01-24 | 1986-01-24 | Magnetic field generator for plasma confinement |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62172699A true JPS62172699A (en) | 1987-07-29 |
Family
ID=11828983
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61013287A Pending JPS62172699A (en) | 1986-01-24 | 1986-01-24 | Magnetic field generator for plasma confinement |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62172699A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6351098A (en) * | 1986-08-20 | 1988-03-04 | 理化学研究所 | Plasma generator |
JPH01302645A (en) * | 1988-02-08 | 1989-12-06 | Anelva Corp | Discharging device |
JPH02123640A (en) * | 1988-11-01 | 1990-05-11 | Anelva Corp | discharge device |
JP2007212294A (en) * | 2006-02-09 | 2007-08-23 | Kyoto Univ | Electron beam generation method and apparatus |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5987798A (en) * | 1982-11-12 | 1984-05-21 | 株式会社東芝 | Plasma unit |
JPS60103626A (en) * | 1983-11-11 | 1985-06-07 | Hitachi Ltd | plasma anodization equipment |
-
1986
- 1986-01-24 JP JP61013287A patent/JPS62172699A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5987798A (en) * | 1982-11-12 | 1984-05-21 | 株式会社東芝 | Plasma unit |
JPS60103626A (en) * | 1983-11-11 | 1985-06-07 | Hitachi Ltd | plasma anodization equipment |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6351098A (en) * | 1986-08-20 | 1988-03-04 | 理化学研究所 | Plasma generator |
JPH01302645A (en) * | 1988-02-08 | 1989-12-06 | Anelva Corp | Discharging device |
JPH02123640A (en) * | 1988-11-01 | 1990-05-11 | Anelva Corp | discharge device |
JP2007212294A (en) * | 2006-02-09 | 2007-08-23 | Kyoto Univ | Electron beam generation method and apparatus |
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