JPS58167987A - Particle beam position detector - Google Patents

Particle beam position detector

Info

Publication number
JPS58167987A
JPS58167987A JP5081882A JP5081882A JPS58167987A JP S58167987 A JPS58167987 A JP S58167987A JP 5081882 A JP5081882 A JP 5081882A JP 5081882 A JP5081882 A JP 5081882A JP S58167987 A JPS58167987 A JP S58167987A
Authority
JP
Japan
Prior art keywords
particle beam
grid electrode
collector
particle
intensity distribution
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
JP5081882A
Other languages
Japanese (ja)
Inventor
Hironobu Kimura
博信 木村
Chikara Konagai
主税 小長井
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura Electric Co 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP5081882A priority Critical patent/JPS58167987A/en
Publication of JPS58167987A publication Critical patent/JPS58167987A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/29Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Measurement Of Radiation (AREA)

Abstract

PURPOSE:To enable a highly accurate detection of the beam position and the intensity by arranging a flat grid electrode on the incidence surface like a metal screen. CONSTITUTION:When a particle beam 11 irradiates the surface of a grid electrode 13, it 13 is incident in a two-directional expanse because of the flat shape of the grid electrode 13. The particle beam 11 enters an anode 19 passing through cylindrical collectors 17. The intensity distribution of the particle beam 11 within the incident surface is converted with the anode 19 into an intensity distribution of current and sent to a signal processing circuit 22. Then, it is memorized in a two dimentional memory in the signal processing circuit 22 corresponding to a two-dimensional expanse of the particle beam 11 as image signal while inputted into a display 23 for two-dimensional indication.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、例えば被融合装置のプラズマ温度を上昇する
丸めの中性粒子入射装置等に使用される能動粒子源(N
Jil )の粒子ビームの入射位置を検出する装置に関
する。
Detailed Description of the Invention [Technical Field of the Invention] The present invention relates to an active particle source (N
Jil) relates to a device for detecting the incident position of a particle beam.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

核融合装置に使用畜れる能動粒子源の粒子ビームの入射
位置の検出は、第1図に示すように大径のファラデーカ
ッグ1に粒子ビーム2を入射させ、そのビーム強度を電
流値に変換してビーム位置を検出するようkしてい丸。
To detect the incident position of the particle beam of an active particle source used in a nuclear fusion device, as shown in Figure 1, the particle beam 2 is incident on a large-diameter Faraday cag 1, and the beam intensity is converted into a current value. mark to detect the beam position.

ところがこのような鉄酸では、能動粒子源の粒子ビーム
が一般に2次元的な広が)をもって照射されるため、粒
子ビーム2の中心と7ァラデ一カ、グ1の中心とが一致
しているかどうかを正確に判定することが困難であシ、
粒子ビーム20入射位置・及びその入射面内における強
度分布を高精度に検出する°ことがで龜なかり゛た。
However, with such ferric acid, the particle beam from the active particle source is generally irradiated with a two-dimensional spread, so the center of particle beam 2 and the center of particle beam 1 coincide with each other. It is difficult to accurately determine whether
It was not possible to detect the incident position of the particle beam 20 and the intensity distribution within the incident plane with high accuracy.

〔発明の目的〕[Purpose of the invention]

本発明は、2次元的な広がシをもって照射される粒子ビ
ームの位置及びその入射面内における強度分布を高精度
に検出し、かつ画像表示することができる粒子ビーム位
置検出装置を提供することを目的とする。
An object of the present invention is to provide a particle beam position detection device capable of highly accurately detecting the position of a particle beam irradiated with a two-dimensional spread and the intensity distribution within its incident plane, and displaying the image. With the goal.

〔発明の概費〕[Outline of invention cost]

本発明に係る粒子ビーム位置検出装置は、金網状をなし
2次元的な広がシを奄りた粒子ビームを表1iii肯よ
シ裏面側へ挿通させる平面的なグリッド電極と、このグ
リ、ド電極の裏面側に軸方向をグリッド電極に直交させ
てマトリックス状に配列され九複数の円筒形コレクタと
、各コレクタの前記グリッド電極と反対肯の端面に接触
して配設され各コレクタを一通過した前記粒子ビームを
入射させそのビーム強度に応じた電気信号を出力する複
数のアノードと、これらのアノードよ少入力され良電気
信号を画像信号に変換する信号処理回路と、この信号処
理回路よ少入力された画像信号にもとづいて前記粒子ビ
ームの強度分布を表示する表示装置とを具備してなるも
のである拳 〔発明の実施例〕 第2図は本発明の一実施例を示すもので、図中11は2
次元的な広がシをもって照射される粒子ビームである。
The particle beam position detection device according to the present invention includes a flat grid electrode through which a particle beam having a wire mesh shape and a two-dimensional spread is passed from the front side to the back side, and the grid electrode and the grid electrode. A plurality of nine cylindrical collectors arranged in a matrix with the axial direction perpendicular to the grid electrode on the back surface side of the electrode, and a plurality of cylindrical collectors disposed in contact with the end face opposite to the grid electrode of each collector and passing through each collector once. a plurality of anodes that input the particle beam and output electrical signals corresponding to the beam intensity; a signal processing circuit that receives a small number of input signals from these anodes and converts the electrical signals into image signals; A fist comprising a display device that displays the intensity distribution of the particle beam based on an input image signal [Embodiment of the Invention] FIG. 2 shows an embodiment of the present invention. 11 in the diagram is 2
This is a particle beam that is irradiated with a dimensional spread.

t*、−中12はこの粒子ビーム11の入射位置及びそ
の強度分布を検出し、かつ表示する粒子ビーム位置検出
装置であって、この装置120粒子ビーム入射面には、
粒子ビーム11を十分挿通させうる粗目の金網状をなす
グリ、ド電@JJが平面的に配設されている。
t*, - 12 is a particle beam position detection device that detects and displays the incident position of the particle beam 11 and its intensity distribution, and the particle beam entrance surface of this device 120 has:
A wire mesh-like grid, which allows the particle beam 11 to penetrate sufficiently, is arranged in a plane.

このグリ、ド電極11は電#14に接続され負のバイア
ス電圧が勾加されている。を九前記グリ、ド電極13の
裏面側には耐熱性e(優れたセラミ、り勢による絶縁性
のコレクタ保持板15が配設されている。このコレクタ
保持板16は第3図に示すようにマトリックス状に配列
して穿設された多数の孔16・・・を有するもので、そ
This grid electrode 11 is connected to voltage #14 and a negative bias voltage is applied thereto. On the back side of the negative electrode 13, there is provided a collector holding plate 15 made of heat-resistant ceramic (made of excellent ceramic material), which is insulated by tension. It has a large number of holes 16 arranged in a matrix.

れらの合孔16′・・・には第4図に示すように4II
L金属@C)円筒形マルテテ°ヤンネル2次元コレクタ
11・・・が嵌合されている拳これらのコレクタ17・
・・の材質としては、対高温特性の嵐い例えばタングス
テン又はモリブデン等が使用される。
These matching holes 16'... have 4II holes as shown in FIG.
L metal @ C) Cylindrical maltete ° Jannel two-dimensional collector 11... is fitted into these collectors 17.
As for the material, a material having high temperature resistance properties such as tungsten or molybdenum is used.

そして前記コレクタ保持板11の裏thiIIKはセラ
ミ、りでで龜た多層のプリント配線基板18が配設され
ておシ、この基板18のiI面には前記各;レクタ11
・・・の下端に直接接触して各コレクタ11・・・K!
I続されかつ相互に絶縁された円形平板状の多数のアノ
ード19・・・と、各アノード1g・・・に接続され良
信号゛引出し用の配線ノlターン20・・・とが設けら
れている。そして前記各アノード19・・・には配線基
板18の11面に引出された配置I/fターン20・・
・を介してマルチチャンネルアン7”JJ・・・が接a
され、さらにそのアyfxz・・・を介して行方向と列
方向とに分かれて2つの信号処理回路22°゛、22が
接続されている。まえ、両信号処理回路x2.;12に
は表示装置21が接続され、さらにこの表示装置2Jを
介して計算機24が接続されている。
A multilayer printed wiring board 18 made of ceramic or resin is disposed on the back side of the collector holding plate 11, and on the iI side of this board 18, each of the collectors 11
Each collector 11...K!
A large number of circular plate-shaped anodes 19 connected to each other and insulated from each other are provided, and a wiring turn 20 connected to each anode 1g for extracting a good signal is provided. There is. Each of the anodes 19... has I/F turns 20 drawn out on the 11th surface of the wiring board 18.
・Multi-channel antenna 7”JJ... is connected via
Further, two signal processing circuits 22° and 22 are connected in the row direction and column direction via the eyes yfxz, . . . . In front, both signal processing circuits x2. 12 is connected to a display device 21, and further connected to a computer 24 via this display device 2J.

次に、以上の如く構成され九粒子ビーム位置検出装置1
20作用を説明する。まずグリッド電極JJK例えば−
50〜−100Vii度の負電圧を印加する。tた各コ
レクタ17・・・内を高真空状1iK排気してお龜、グ
リッド電極JJの表面に、正電位に帯電された、例えば
プロトン(H”)ビーム、重水素(P+)ビーム、ヘリ
ウム()i@”)ビーム等の粒子ビーム11を照射する
と、このグリッド電極IJは平面的な形状をもつもの゛
であるから、2次元的な広がシをもつ粒子ビーム11の
入射を確実に受けることがで龜る・まだ粒子ビーム11
″が高速でコレクタ11に入射すると自コレクタ11か
ら電子を放出するが、グリッド電極13は負電位に保た
れているので放出された電子をコレクタ11へ押戻す作
用を果している。また各円筒形コレクタ17・・・は1
個1個がファラデーカ、グの役目を果し、粒子ビーム1
1は各円筒形コレクタ11・・・を通してアノード19
・・・K入射する。そこで、各アノード1#・・・は、
個々に入射し九粒子ビームの強度に比例し走電流をアン
プ21・・・へ流す。
Next, the nine-particle beam position detection device 1 configured as described above will be described.
20.Explain the action. First, grid electrode JJK for example -
A negative voltage of 50 to -100 Vii degrees is applied. The interior of each collector 17 is evacuated to a high vacuum state of 1iK, and a positively charged beam, such as a proton (H'') beam, deuterium (P+) beam, or helium, is applied to the surface of the grid electrode JJ. When a particle beam 11 such as a ()i@”) beam is irradiated, since this grid electrode IJ has a planar shape, it ensures that the particle beam 11 with a two-dimensional spread is incident. Particle beam 11 still slows down due to receiving
'' enters the collector 11 at high speed, it emits electrons from its own collector 11, but since the grid electrode 13 is kept at a negative potential, it functions to push the emitted electrons back to the collector 11.In addition, each cylindrical Collector 17...is 1
Each particle plays the role of Faradeka, and the particle beam 1
1 is an anode 19 through each cylindrical collector 11...
...K is incident. Therefore, each anode 1#...
A traveling current proportional to the intensity of the nine particle beams incident on each beam is sent to the amplifier 21 .

このと素粒子ビーム11の、入射面(すなわちグリ、ド
電@Pi13の表面)内における強度分布は、アノード
19・・・において電流の強−分布に変換され、さらに
アン7’JJ・・・で増幅されて信号処理回路i:tt
、xzに送出されることになる。そして信号処理回路i
s 、 27においてサングルホールドされ九後A/D
変供され、粒子ビーム1102次元釣人がシに対、応し
た信号処理、回路32.22内の2次元メモリに画像信
号として記憶される。そこで、このi!i儂信号は表示
装置23へ入力されて2次元表示されるとともに、計算
機24へ入力される。そしてこの計算機24では電流の
ピーク値を検出し、そのピーク値に対応するコレクタ1
1から粒子ビーム11の中心位置が算出されるので、粒
子ビーム11の位置及びその入射面内における強度分布
をll1ib棺度に検出することができる。
At this time, the intensity distribution of the elementary particle beam 11 within the incident plane (i.e., the surface of the doped electric @Pi 13) is converted into an intensity distribution of current at the anodes 19... and further anodes 19... signal processing circuit i:tt
, xz. and signal processing circuit i
s, Sangle hold at 27 and 9th A/D
The particle beam 110 is converted into a two-dimensional beam, and corresponding signal processing is performed and stored as an image signal in the two-dimensional memory in the circuit 32.22. So this i! The i-signal is input to the display device 23 for two-dimensional display, and is also input to the computer 24. Then, this calculator 24 detects the peak value of the current, and selects the collector 1 corresponding to the peak value.
Since the center position of the particle beam 11 is calculated from 1, the position of the particle beam 11 and its intensity distribution within the plane of incidence can be detected accurately.

〔発明の効果〕〔Effect of the invention〕

以上詳述し九ように、本発明に係る粒子ビーム位置検出
装置によれば、入射面に、金網状をなす平面的なグリ、
ド電也が配置されているので、2次元的な広がシをもつ
粒子ビーム11の照射をその表tJK@夷に受けること
ができる。
As described in detail above, according to the particle beam position detection device according to the present invention, the plane grid having a wire mesh shape is provided on the incident surface.
Since the electron beams are arranged, the surface thereof can be irradiated with the particle beam 11 having a two-dimensional spread.

また、グリッド電極の皇面肯には複数の円筒形コレクタ
を、それらの軸方向をグリッド電極に直交させてマトリ
ックス状に配列し、かつlレクタの、前記グリッド電極
と反対側の図面にはアノードを接触させているので、グ
リッド電極を通過した粒子ビームを、各コレクタを通し
て各アノードへ確実に入射させることかで龜る。
Further, on the opposite side of the grid electrode, a plurality of cylindrical collectors are arranged in a matrix with their axial directions perpendicular to the grid electrode, and on the opposite side of the collector from the grid electrode, an anode is arranged. Since the grid electrodes are in contact with each other, it is difficult to ensure that the particle beam that has passed through the grid electrode is incident on each anode through each collector.

そして各アノードよ)、その粒子ビームのビーム強度に
応じた電気信号を出力させ、その電気信号にもとづき、
信号処理回路よシ画像信号を表示装置へ入力させ−〔、
粒子ビームの位置及びその入射面内における強度分布を
2次元表示することができる。従ってビーム位置及び強
度分布1を高精度に検出することができ、目動粒子―の
粒子ビーム軸合せも容易となる。
Then, each anode) outputs an electrical signal corresponding to the beam intensity of the particle beam, and based on that electrical signal,
The signal processing circuit inputs the image signal to the display device.
The position of the particle beam and its intensity distribution within the plane of incidence can be displayed two-dimensionally. Therefore, the beam position and intensity distribution 1 can be detected with high precision, and particle beam axis alignment of the moving particles is also facilitated.

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

第1図は背景技術の説明図、第2図は本発明の一実施例
を示す粒子ビーム位置検出輌皺の概略構成図、第3図は
同実施例の一部を取出して示す平面図、#g4図は同冥
施例の部分斜視−である。 11・・・粒子ビーム、12・・・粒子ビーム位置検−
出装置、13・・・グリ、ド電極、11・・・円筒形コ
レクタ、19・・・アノード、22・・・信号処111
1g回路、21・・・表示装置。 出願人代理人  弁理士 鈴 江 武 彦牙1図
FIG. 1 is an explanatory diagram of the background art, FIG. 2 is a schematic configuration diagram of a particle beam position detection vehicle wrinkle showing an embodiment of the present invention, and FIG. 3 is a plan view showing a part of the embodiment. Figure #g4 is a partial perspective view of the same example. 11...Particle beam, 12...Particle beam position detection-
Output device, 13... Grid, electrode, 11... Cylindrical collector, 19... Anode, 22... Signal processing 111
1g circuit, 21...display device. Applicant's agent Patent attorney Takeshi Suzue Hikoga 1

Claims (3)

【特許請求の範囲】[Claims] (1)  金網状をなし2次元的な広が9をもつ九粒子
ビームを表面匈よ〕裏面側へ挿通させる平  3゜面的
なグリッド電極と、このグリッド電極の裏面側に軸方向
をグリッド電極に直交させてマトリッタス状に配ダ1j
され九複数の円筒形;レクタと、各コレクタの前記グリ
、t/電極と反対側の端面KI[+触して配設され各コ
レクタを通過した一紀粒子e−ムを入射させそのビーム
強度に応じ良電気信号を出力する複数のアノードと、こ
れらのアノードより入力された電気信号を画像信号に変
換する信号処理回路と、この信号処理回路よシ入力され
た画像信号にもとづいて紡紀粒子ビームの強度分布を表
示する表示装置とを具備し九ことを%黴とする粒子゛ビ
ーム位置検出装置―
(1) A flat 3° grid electrode that has a wire mesh shape and a nine-particle beam with a two-dimensional spread 9 is passed from the surface to the back side, and a grid that runs in the axial direction on the back side of this grid electrode. Arranged in a matrittas shape perpendicular to the electrode 1j
A plurality of cylindrical collectors; each collector has an end surface KI on the opposite side to the electrode; A plurality of anodes that output electrical signals, a signal processing circuit that converts the electrical signals input from these anodes into image signals, and a spin particle beam based on the input image signals from this signal processing circuit. and a display device for displaying the intensity distribution of the particle beam, the particle beam position detection device being equipped with a display device that displays the intensity distribution of the particle.
(2)  前記円筒形コレクタをタングステンにて形成
したことを特徴とする特許請求の範囲第(1)項記載の
粒子ビー五位置検出装置。
(2) The particle bee five-position detection device according to claim (1), wherein the cylindrical collector is made of tungsten.
(3)  前記円筒形コレクタをモリブデンにて形成し
九ことを特徴とする特許請求の範囲鮪(1)項記載の粒
子ビーム位置検出装置・
(3) The particle beam position detection device according to claim (1), wherein the cylindrical collector is made of molybdenum.
JP5081882A 1982-03-29 1982-03-29 Particle beam position detector Pending JPS58167987A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5081882A JPS58167987A (en) 1982-03-29 1982-03-29 Particle beam position detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5081882A JPS58167987A (en) 1982-03-29 1982-03-29 Particle beam position detector

Publications (1)

Publication Number Publication Date
JPS58167987A true JPS58167987A (en) 1983-10-04

Family

ID=12869337

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5081882A Pending JPS58167987A (en) 1982-03-29 1982-03-29 Particle beam position detector

Country Status (1)

Country Link
JP (1) JPS58167987A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60167248A (en) * 1984-02-10 1985-08-30 Jeol Ltd Electron microscope

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5148975A (en) * 1974-10-25 1976-04-27 Tokyo Shibaura Electric Co SOSAKADENRYUSHIBIIMUNO BUNPUSOKUTE ISOCHI
JPS5571970A (en) * 1978-11-07 1980-05-30 Thomson Csf Divice for visualizing current density distribution in electric charge particle beam

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5148975A (en) * 1974-10-25 1976-04-27 Tokyo Shibaura Electric Co SOSAKADENRYUSHIBIIMUNO BUNPUSOKUTE ISOCHI
JPS5571970A (en) * 1978-11-07 1980-05-30 Thomson Csf Divice for visualizing current density distribution in electric charge particle beam

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60167248A (en) * 1984-02-10 1985-08-30 Jeol Ltd Electron microscope
JPH0339378B2 (en) * 1984-02-10 1991-06-13 Nippon Electron Optics Lab

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