JPH0329300A - Strong focussing type charged particle acceleration/ deceleration tube - Google Patents

Strong focussing type charged particle acceleration/ deceleration tube

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Publication number
JPH0329300A
JPH0329300A JP19737189A JP19737189A JPH0329300A JP H0329300 A JPH0329300 A JP H0329300A JP 19737189 A JP19737189 A JP 19737189A JP 19737189 A JP19737189 A JP 19737189A JP H0329300 A JPH0329300 A JP H0329300A
Authority
JP
Japan
Prior art keywords
electrode
along
electrode couples
ion
acceleration
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
Application number
JP19737189A
Other languages
Japanese (ja)
Other versions
JP2797490B2 (en
Inventor
Yoshio Takami
芳夫 高見
Shinji Nagamachi
信治 長町
Masakatsu Kosaka
向坂 正勝
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP19737189A priority Critical patent/JP2797490B2/en
Priority to EP19900114384 priority patent/EP0410460A3/en
Priority to US07/558,320 priority patent/US5105161A/en
Publication of JPH0329300A publication Critical patent/JPH0329300A/en
Application granted granted Critical
Publication of JP2797490B2 publication Critical patent/JP2797490B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Particle Accelerators (AREA)
  • Casings For Electric Apparatus (AREA)
  • Electron Sources, Ion Sources (AREA)

Abstract

PURPOSE:To accelerate and decelerate ion beams at high efficiency arranging a plurality of electrode couples comprising opposed paired electrodes to overlap each other along the common axis, and applying differential DC voltages to the respective electrode couples in arranged order while arranging the electrode couples orthogonally alternately in the counter direction. CONSTITUTION:A positive ion generated at an ion source 1 is induced by the potential difference between the ion source 1 and an inducing electrode 2 and formed an ion beam B which is led to an acceleration tube A and gradually accelerated along the direction of the common axis (z) through the inside of electrode couples 3, 4... which act as the acceleration electrode. When the positive ion arrives at the overlapped section of the electrode couples 3, 4, the potential of the positive ion becomes the mean between ones of the electrode couples 3,4, and further, when the positive ion arrives at the overlapped section of the electrode couples 4, 5, the potential of the positive ion becomes the means between ones of the electrode couples 4, 5. The beam B in the acceleration tube A is accelerated along the direction of the (z) axis while being focused forcedly along the direction of (x) and (y) axes alternately.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は直流電圧によってイオンや電子などのような荷
電粒子を加速もしくは減速するための強集束型荷電粒子
加減速管に関し、特に、大電流のイオンビーム発生装置
などを横戊するのに適した加減速管に関する. く従来の技術〉 従来から、直流電圧を用いてイオンビームなどの荷電粒
子ビームを加速もしくは減速するには、第3図で示すよ
うな中空円筒状もしくは円孔板状の電極を有する加減速
管が用いられている.なお、第3図はこの加減速管をイ
オンビームを加速するための加速管として用いたイオン
ビーム発生装置の構成例を示しており、第3図(a)は
各構成部材の配置状態を示す概略構戒図、同図(b)は
その共通軸線であるz軸方向から見た電極33(34.
35)の形状を示す説明図である。
[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to a highly focused charged particle acceleration/deceleration tube for accelerating or decelerating charged particles such as ions and electrons using a direct current voltage. This article relates to an acceleration/deceleration tube suitable for horizontally moving ion beam generators, etc. Conventional technology> Conventionally, in order to accelerate or decelerate a charged particle beam such as an ion beam using a DC voltage, an acceleration/deceleration tube having a hollow cylindrical or circular plate-shaped electrode as shown in Fig. 3 has been used. is used. Note that FIG. 3 shows an example of the configuration of an ion beam generator using this acceleration/deceleration tube as an acceleration tube for accelerating an ion beam, and FIG. 3(a) shows the arrangement of each component. The schematic diagram (b) shows the electrodes 33 (34.
FIG. 35) is an explanatory diagram showing the shape of FIG.

そして、この構成例においては、イオンa31、引き出
し電極32および加速管30が2軸方向に沿って並べら
れており、この加速管30は3個の中空円筒状とされた
電極33,34.35によって構威されている.さらに
、イオンag3lおよび引き出し電極32には図示して
いない高圧電源からの直流電圧が印加される一方、電極
33,34.35には高圧電源36からの直流電圧が直
列抵抗によって分圧されたうえで印加されている。また
、このとき、電極33,34.35に対する印加電圧は
引き出し電極32側に位置する電極33から最終段側の
電極35へいくほど一般に低くなるように設定されてお
り、これらの電極33,34.35は加速電極として機
能するようになっている。
In this configuration example, the ion a31, the extraction electrode 32, and the acceleration tube 30 are arranged along two axial directions, and the acceleration tube 30 has three hollow cylindrical electrodes 33, 34, 35. It is structured by Further, a DC voltage from a high-voltage power supply (not shown) is applied to the ion ag3l and the extraction electrode 32, while a DC voltage from a high-voltage power supply 36 is applied to the electrodes 33, 34, 35 by a series resistor. is applied. Further, at this time, the voltage applied to the electrodes 33, 34, 35 is generally set to become lower as it goes from the electrode 33 located on the extraction electrode 32 side to the electrode 35 on the final stage side. .35 is designed to function as an accelerating electrode.

そこで、イオン源31で発生したイオンは、このイオン
′a31と引き出し電極32との電位差によってビーム
状で引き出された後、加速電極として機能する電極33
,34.35の内部を通ることによって順次z軸方向に
沿って加速されることになる. 一方、イオンビームを減速する必要がある場合は、第3
図で示すイオンビーム発生装置の構成例における高圧電
源36の正負極を互いに逆転することにより、引き出し
電極32側に位置する電極33から最終段側の電極35
へいくほど一般に高い直流電圧が印加されるように設定
する.すると、このことによって電極33.34.35
が減速電極として機能することになり、イオン′a3l
で発生して引き出し電極32でビーム状に引き出された
イオンは、減速電極として機能する電極33,34.3
5の内部を通ることによって2軸方向に沿って減速され
ることになる。
Therefore, the ions generated in the ion source 31 are extracted in a beam shape by the potential difference between the ions 'a31 and the extraction electrode 32, and then the ions are extracted from the electrode 32 which functions as an accelerating electrode.
, 34.35, it is sequentially accelerated along the z-axis direction. On the other hand, if it is necessary to decelerate the ion beam, the third
By reversing the positive and negative poles of the high-voltage power supply 36 in the configuration example of the ion beam generator shown in the figure, the electrode 33 located on the extraction electrode 32 side is moved from the electrode 35 on the final stage side.
Generally, the higher the DC voltage is applied, the higher the setting is. Then, due to this, the electrodes 33, 34, 35
will function as a deceleration electrode, and the ion 'a3l
The ions generated in the extraction electrode 32 are extracted in a beam shape by the electrodes 33, 34.3, which function as deceleration electrodes.
5, the speed is reduced along two axes.

〈発明が解決しようとする課題〉 ところで、前記構成の加減速管においては、大1!流の
イオンビームを高い効率で加速もしくは減速することが
できないという不都合が生していた。
<Problems to be Solved by the Invention> By the way, in the acceleration/deceleration tube having the above configuration, the major problem is 1! This method has the disadvantage that it is not possible to accelerate or decelerate a flowing ion beam with high efficiency.

そして、このような不都合が生しるのは、中空円筒状と
されたffipi33.34.35の集束力が弱く、し
かも、大電流のイオンビームを加速もしくは減速する場
合には、ビーム内の各イオン間に働くクーロン力によっ
てビームがX軸およびy軸方向に沿って発散してしまう
ためと考えられる.本発明はかかる不都合に鑑みて創案
されたものであって、直流電圧によって荷電粒子を加滅
速する過程で大きな集束力を持ち、かつ、大電流の荷電
粒子ビームを高効率で加減速することができるijA!
!束型荷電粒子加減速管を提供することを目的としてい
る。
The reason for this inconvenience is that the focusing power of the hollow cylindrical ffipi33, 34, 35 is weak, and when accelerating or decelerating a large current ion beam, each part of the beam This is thought to be because the beam diverges along the X-axis and y-axis directions due to the Coulomb force acting between ions. The present invention has been devised in view of these disadvantages, and has a method of accelerating and decelerating a charged particle beam with high efficiency, which has a large focusing power in the process of accelerating and accelerating charged particles using a DC voltage, and which has a large current. IjA can do it!
! The purpose is to provide a bundled charged particle acceleration/deceleration tube.

く課題を解決するための手段〉 本発明は、このような目的を達成するため、実施例に対
応する第1図で示すように、それぞれが対向する2個の
電極3aと3b,4aと4b,・・・からなる複数の電
極対3,4,・・・を交互に対向方向で直交させつつ、
相互に重複させて互いの共通軸線であるz軸に沿って配
列するとともに、各電極対3.4.・・・にその配列順
序に従って所定の向きの電位差を付した直流電圧を印加
する直流電源回路を設けたことを特徴とするものである
Means for Solving the Problems> In order to achieve the above objects, the present invention provides two electrodes 3a and 3b, 4a and 4b facing each other, as shown in FIG. 1 corresponding to the embodiment. , . . . while alternately orthogonally intersecting the plurality of electrode pairs 3, 4, .
Each pair of electrodes 3.4. ... is provided with a DC power supply circuit that applies a DC voltage with a potential difference in a predetermined direction according to the arrangement order.

〈作用〉 上記横戒によれば、各電極対3.4.・・・に対してz
軸上での配列順序に従う電位の直流電圧を印加すること
により、荷電粒子はz軸方向に沿って加速もしくは減速
されることになる。そして、このとき、各電極対3.4
,・・・の重複部分における荷電粒子の電位は両Ti極
対の電位の中間となり、この部分では実質的に四重極構
造の電極が構成されるので、例えば、第2図の断面b−
b位置ではX軸方向、また、その断面c−c位置ではy
軸方向に沿って荷電粒子ビームを強く集束する力が働く
ことになる.その結果、この荷電粒子ビームは全体とし
てz軸方向に沿って加速もしくは減速されつつ、各電極
対3.4.・・・の重腹部分ではX軸もしくはy軸方向
に沿って集束されることになる。
<Function> According to the above precept, each electrode pair 3.4. ... against
By applying a DC voltage with a potential according to the arrangement order on the axis, the charged particles will be accelerated or decelerated along the z-axis direction. At this time, each electrode pair is 3.4
The potential of the charged particles at the overlapping portion of , .
At the b position, the X-axis direction, and at the cross-section c-c position, the y
A force acts to strongly focus the charged particle beam along the axial direction. As a result, this charged particle beam as a whole is accelerated or decelerated along the z-axis direction while each electrode pair 3.4. ... will be focused along the X-axis or y-axis direction.

〈実施例〉 以下、本発明の実施例を図面に基づいて説明する. 第1図は本発明にかかる加減速管を正のイオンビームを
加速するための加速管として用いる場合におけるイオン
ビ一ム発生装置の構成を示しており、第1図(a)は各
横或部材の配置状態を示す概略構戊図、第1図(b)〜
(d)は第1図(a)におけるb−b線,c−c線,d
−d線のそれぞれに沿う断面図である. 本実施例におけるイオンビーム発生装置は、イオン#l
と、これの引き出し口に隣接して配置された引き出し電
極2とを備えており、この引き出し電極2の後段側には
加速管Aが設けられている。
<Example> Hereinafter, an example of the present invention will be described based on the drawings. Figure 1 shows the configuration of an ion beam generator when the acceleration/deceleration tube according to the present invention is used as an acceleration tube for accelerating a positive ion beam. Schematic structural diagram showing the arrangement state of, Fig. 1(b) ~
(d) is line bb, line cc, and d in Figure 1(a).
- It is a cross-sectional view along the d line. The ion beam generator in this embodiment has ions #l
and an extraction electrode 2 disposed adjacent to the extraction port thereof, and an acceleration tube A is provided on the downstream side of the extraction electrode 2.

そして、イオン源1および引き出し電極2には図示して
いない高圧電源が接続されており、この高圧電源から直
流電圧が印加されるようになっている. 加速管Aは、それぞれが対向する2個の電極(後述する
)からなる?!敗の電極対、例えば、5対の電極対3.
  4.  5.  6および7をイオンビームBの加
速方向、すなわち、互いの共通軸心であるz軸方向に沿
って配列したものであり、各電極対3.4,・・・は交
互にその電極の対向方向で直交させられている。
A high voltage power source (not shown) is connected to the ion source 1 and the extraction electrode 2, and a DC voltage is applied from this high voltage power source. Accelerator tube A consists of two electrodes (described later) that each face each other. ! Defective electrode pairs, for example, 5 electrode pairs3.
4. 5. 6 and 7 are arranged along the acceleration direction of the ion beam B, that is, along the z-axis direction which is the mutual axis, and each electrode pair 3.4, . . . are perpendicular to each other.

そして、電極対3,4,・・・のそれぞれは、同一の長
さとされた2個の電極3aと3b,4aと4b,5aと
5b.6aと6bおよび7aと7bを2軸を中心として
対向配置させることによって構威したものであり、z軸
に垂直な平面上で互いに直交する軸をX軸およびy軸と
すると、電極3aと3b,5aと5bおよび7aと7b
はX軸方向に沿って対向し、電lJi4aと4bおよび
6aと6bはy軸方向に沿って対向している。また、こ
のとき、z軸方向に沿って互いに隣接する電極対3と4
,4と5,5と6および6と7のそれぞれは、相互に重
複させられている。
Each of the electrode pairs 3, 4, . . . includes two electrodes 3a and 3b, 4a and 4b, 5a and 5b, . It is constructed by arranging electrodes 6a and 6b and 7a and 7b facing each other around two axes.If the axes that are orthogonal to each other on a plane perpendicular to the z-axis are the X-axis and the y-axis, then the electrodes 3a and 3b , 5a and 5b and 7a and 7b
are opposed along the X-axis direction, and electric currents 4a and 4b and 6a and 6b are opposed along the y-axis direction. Also, at this time, electrode pairs 3 and 4 adjacent to each other along the z-axis direction
, 4 and 5, 5 and 6, and 6 and 7 are overlapped with each other.

さらに、このようにして配置された電極対3,4,・・
・にCよその配列順序に従って所定の向きの電位差を付
した直流電圧を印加する直流電源回路Sが接続されてお
り、この直流電源回路Sは、高圧電源8と、これからの
直流電圧を抵抗R5・・・で分圧したうえで各電極対3
,4,・・・に印加する分圧回路とを備えている.そし
て、電極3,4.・・・のそれぞれに対する印加電圧は
引き出し電極2側に位置する電極対3から最終段例の電
極対7へいくほど低くなるように設定されており、これ
らの電極対3.4,・・・は加速電極として機能するよ
うになっている.なお、このとき、各電極対3,4,・
・・をそれぞれ構成する2個の電極3aと3b.4aと
4b, ・・・は電気的に接続されており、互いに同電
位となっている. つぎに、本発明にかかる加減速管を加速管Aとして用い
た場合におけるイオンビーム発生装置の作用および動作
について説明する. イオン源1で発生した正のイオンは、このイオンStと
引き出し電極2との電位差によって引き出され、イオン
ビームBとなって加速管Aに導かれることにより、加速
電極として機能する電極対3,4,・・・の内部を通る
ことによって順次z軸方向に沿って加速される。
Furthermore, the electrode pairs 3, 4,... arranged in this way
A DC power supply circuit S that applies a DC voltage with a potential difference in a predetermined direction according to the arrangement order around C is connected to the high voltage power supply 8 and a resistor R5. After dividing the pressure by ..., each electrode pair 3
, 4,... And electrodes 3, 4 . The voltage applied to each of the electrode pairs 3, 4, . is designed to function as an accelerating electrode. In addition, at this time, each electrode pair 3, 4, .
Two electrodes 3a and 3b . 4a and 4b, . . . are electrically connected and have the same potential. Next, the function and operation of the ion beam generator when the acceleration/deceleration tube according to the present invention is used as the acceleration tube A will be explained. The positive ions generated in the ion source 1 are extracted by the potential difference between the ions St and the extraction electrode 2, and are guided to the acceleration tube A as an ion beam B, thereby forming an electrode pair 3, 4 that functions as an acceleration electrode. , ... are sequentially accelerated along the z-axis direction.

そして、正イオンが電極対3.4の重複部分に到達する
と、この正イオンの電位は電極対3および4の電位の中
間となる。そこで、この重複部分においては、第2図(
a)で示すように、X軸一y軸平面での電位がイオンビ
ームBから見て電極対3を横戒する電極3a,3bが正
、また、電極対4を溝威する電極4a,4bが負となる
ので、四重極横造の電極が構威されることになる.従っ
て、これらの重複部分に到達したイオンビームBは、X
軸方向に沿って強く集束されることになる。なお、この
とき、y軸方向に沿っては強発散することになるが、こ
の発散力よりも集束力の方が大きいので、合成すると強
集束されることになる。
When the positive ions reach the overlapping portion of the electrode pairs 3.4, the potential of the positive ions becomes intermediate between the potentials of the electrode pairs 3 and 4. Therefore, in this overlapping part, see Figure 2 (
As shown in a), when viewed from the ion beam B, the electrodes 3a and 3b that cross the electrode pair 3 are positive, and the electrodes 4a and 4b that cross the electrode pair 4 have a positive potential on the X-axis and y-axis plane. is negative, so a quadrupole horizontal electrode is constructed. Therefore, the ion beam B that has reached these overlapping parts is
It will be strongly focused along the axial direction. Note that at this time, there will be strong divergence along the y-axis direction, but since the focusing force is greater than this divergent force, the combination will result in strong focusing.

さらに、正イオンが電極対4,5の重復部分にまで到達
すると、この正イオンの電位は1!極対4および5の電
位の中間となる.そして、この重複部分におけるX軸−
y軸平面での電位は、第2図(b)で示すように、イオ
ンビームBから見て電極対4を構成する電極4a,4b
が正、また、TF1極対5をFjl成する電極5a,5
bが負となる結果、この重複部分に到達したイオンビー
ムBはy軸方向に沿って強く集束されることになる。こ
のようにして、イオンビームBは加速管A内においてX
軸方向およびy軸方向に沿って交互に強集束されつつ、
z軸方向に沿って加速されることになる。
Furthermore, when the positive ions reach the overlapping part of the electrode pair 4 and 5, the potential of these positive ions is 1! The potential is midway between the potentials of pole pairs 4 and 5. Then, the X-axis in this overlapping part -
As shown in FIG. 2(b), the potential on the y-axis plane is determined by the potential of the electrodes 4a and 4b forming the electrode pair 4 when viewed from the ion beam B.
is positive, and the electrodes 5a, 5 forming the TF1 pole pair 5
As a result of b becoming negative, the ion beam B that reaches this overlapping portion is strongly focused along the y-axis direction. In this way, the ion beam B is
While being strongly focused alternately along the axial direction and the y-axis direction,
It will be accelerated along the z-axis direction.

なお、以上の説明においては、加速管Aによって正のイ
オンビームを加速するものとしているが、これに限定さ
れるものではなく、加速管八を構威する電極対3.4,
・・・に印加する電位差の向きを逆転することによって
負のイオンビームを加速することも可能であり、また、
電子ビームなどのような荷電粒子ビームを同様にして加
速することもできることはいうまでもない。
In the above description, it is assumed that the positive ion beam is accelerated by the acceleration tube A, but the present invention is not limited to this.
It is also possible to accelerate a negative ion beam by reversing the direction of the potential difference applied to...
It goes without saying that charged particle beams such as electron beams can also be accelerated in a similar manner.

さらにまた、イオンビームを減速する必要がある場合は
、第1図で示すイオンビーム発生装置の構威例における
高圧電源8の正負極を互いに逆転することにより、引き
出し電極2側に位置する電極対3から最終段例の電極対
7へいくほど高い直流電圧が印加されるように設定すれ
ばよい。すなわち、このことによって電極対3,4,5
.6および7が減速電極として機能することになる結果
、イオン源1で発生して引き出し電極2でビーム状に引
き出されたイオンは、減速電極として機能する電極対3
,4,5.6および7の内部を通ることによって2軸方
向に沿って減速されることになる。
Furthermore, when it is necessary to decelerate the ion beam, the positive and negative poles of the high voltage power supply 8 in the configuration example of the ion beam generator shown in FIG. The setting may be such that a higher DC voltage is applied from electrode pair 3 to electrode pair 7 in the final stage example. That is, by this, electrode pairs 3, 4, 5
.. As a result, the ions generated in the ion source 1 and extracted in the form of a beam by the extraction electrode 2 are transferred to the electrode pair 3 which functions as the deceleration electrode.
, 4, 5.6, and 7, the speed is reduced along two axes.

く発明の効果〉 以上説明したように、本発明によれば、各電極対の重複
部分で荷電粒子をX軸方向もしくはy軸方向に沿って集
束しつつ、荷電粒子を全体としてz軸方向に沿って加速
もしくは減速することになる結果、大電流の荷電粒子ビ
ームであっても高効率で加速もしくは減速することがで
きるという優れた効果が得られることになる.
Effects of the Invention> As explained above, according to the present invention, charged particles are focused along the X-axis direction or y-axis direction at the overlapping portion of each electrode pair, and the charged particles are focused in the z-axis direction as a whole. As a result, even charged particle beams with large currents can be accelerated or decelerated with high efficiency, which is an excellent effect.

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

第1図および第2図は本発明にかかる加減速管を正のイ
オンピームを加速するための加速管として用いる場合に
おけるイオンビーム発生装置の構戒を示しており、第1
図(a)は各構成部材の配置状態を示す概略構威図、第
1図(b)〜(d)のそれぞれは第l図(a)における
b−b線,c−c線.d−d線に沿う断面図であり、第
2図はその作用を説明するための断面図である。また、
第3図は従来例にかかる加減速管を加速管として用いた
イオンビーム発生装置の横威例を示しており、第3図(
a)は各構成部材の配置状態を示す概略構成図、同図(
b)はその共通軸線であるz軸方向から見た電極の形状
を示す説明図である。 図における符号1はイオン源、2は引き出し電極、3.
4,5,6.7は電極対、3a,3b,4a,4b,5
a,5b,6a,6b,7a,7bは電極、8は高圧電
源、Aは加速管(加滅速管)、Bはイオンビーム、Rは
抵抗、Sは直流電源回路である。
FIG. 1 and FIG. 2 show the configuration of the ion beam generator when the acceleration/deceleration tube according to the present invention is used as an acceleration tube for accelerating a positive ion beam.
FIG. 1(a) is a schematic structural diagram showing the arrangement of each component, and FIGS. 1(b) to 1(d) are lines bb and cc in FIG. 1(a), respectively. It is a cross-sectional view taken along the line dd, and FIG. 2 is a cross-sectional view for explaining the action. Also,
Figure 3 shows an example of the performance of an ion beam generator using a conventional acceleration/deceleration tube as an acceleration tube.
a) is a schematic configuration diagram showing the arrangement of each component;
b) is an explanatory diagram showing the shape of the electrode viewed from the z-axis direction, which is the common axis. In the figure, numeral 1 is an ion source, 2 is an extraction electrode, and 3.
4, 5, 6.7 are electrode pairs, 3a, 3b, 4a, 4b, 5
a, 5b, 6a, 6b, 7a, and 7b are electrodes, 8 is a high-voltage power supply, A is an acceleration tube (acceleration tube), B is an ion beam, R is a resistor, and S is a DC power supply circuit.

Claims (1)

【特許請求の範囲】[Claims] (1)それぞれが対向する2個の電極からなる複数の電
極対を交互に対向方向で直交させつつ、相互に重複させ
て共通軸線に沿って配列するとともに、各電極対にその
配列順序に従って所定の向きの電位差を付した直流電圧
を印加する直流電源回路を設けたことを特徴とする強集
束型荷電粒子加減速管。
(1) A plurality of electrode pairs, each consisting of two electrodes facing each other, are alternately orthogonally crossed in opposite directions, overlapped with each other, and arranged along a common axis, and each electrode pair is arranged in a predetermined manner according to the arrangement order. A strongly focused charged particle acceleration/deceleration tube characterized in that it is provided with a DC power supply circuit that applies a DC voltage with a potential difference in the direction of .
JP19737189A 1989-03-31 1989-07-28 Strongly focused charged particle acceleration / deceleration tube Expired - Lifetime JP2797490B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP19737189A JP2797490B2 (en) 1989-03-31 1989-07-28 Strongly focused charged particle acceleration / deceleration tube
EP19900114384 EP0410460A3 (en) 1989-07-28 1990-07-26 Strong-convergent type charged particle acceleration/deceleration tube
US07/558,320 US5105161A (en) 1989-07-28 1990-07-26 Strong-convergent type charged particle acceleration/deceleration tube

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP8229689 1989-03-31
JP1-82296 1989-03-31
JP19737189A JP2797490B2 (en) 1989-03-31 1989-07-28 Strongly focused charged particle acceleration / deceleration tube

Publications (2)

Publication Number Publication Date
JPH0329300A true JPH0329300A (en) 1991-02-07
JP2797490B2 JP2797490B2 (en) 1998-09-17

Family

ID=26423315

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19737189A Expired - Lifetime JP2797490B2 (en) 1989-03-31 1989-07-28 Strongly focused charged particle acceleration / deceleration tube

Country Status (1)

Country Link
JP (1) JP2797490B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008178299A (en) * 2007-01-23 2008-08-07 Sanyo Super Stand Co Ltd Case for storing and exhibiting pet

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008178299A (en) * 2007-01-23 2008-08-07 Sanyo Super Stand Co Ltd Case for storing and exhibiting pet

Also Published As

Publication number Publication date
JP2797490B2 (en) 1998-09-17

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