JPH0612660B2 - High voltage ion implanter - Google Patents
High voltage ion implanterInfo
- Publication number
- JPH0612660B2 JPH0612660B2 JP58226860A JP22686083A JPH0612660B2 JP H0612660 B2 JPH0612660 B2 JP H0612660B2 JP 58226860 A JP58226860 A JP 58226860A JP 22686083 A JP22686083 A JP 22686083A JP H0612660 B2 JPH0612660 B2 JP H0612660B2
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- ion
- voltage
- accelerator
- quadrupole accelerator
- 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 - Lifetime
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Classifications
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H9/00—Linear accelerators
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/30—Electron-beam or ion-beam tubes for localised treatment of objects
- H01J37/3002—Details
- H01J37/3007—Electron or ion-optical systems
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/30—Electron-beam or ion-beam tubes for localised treatment of objects
- H01J37/317—Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation
- H01J37/3171—Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation for ion implantation
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H7/00—Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
- H05H7/02—Circuits or systems for supplying or feeding radio-frequency energy
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H7/00—Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
- H05H7/14—Vacuum chambers
- H05H7/18—Cavities; Resonators
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- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Particle Accelerators (AREA)
- Electron Sources, Ion Sources (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明はイオン打込み装置に係り、特に数100keV〜
数MeVのエネルギーの大電流ビーム打込みに好適な高
電圧イオン打込み装置に関する。Description: FIELD OF THE INVENTION The present invention relates to an ion implanting device, and particularly to several 100 keV.
The present invention relates to a high-voltage ion implantation apparatus suitable for high-current beam implantation with energy of several MeV.
従来の工業的に使われているイオン打込み装置で高エネ
ルギイオンを得てこれを基板に打込む場合、イオン源か
ら引出したビームを質量分離器により一旦目的としたイ
オン種に選別した後、これを加速電極リング等を並べた
加速管を使い高エネルギにしていた。この場合、高電圧
印加に伴い、加速電極間の放電やいわゆるコロナ放電が
発生し、実用上達成しうるエネルギーは高々、数100
keV程度であった。(例えばSpringer Series in Ele
ctrophsics 10巻,“Ion Implantation Techvique
s”,Springer-Verlog社出版,1982年,351頁参照)
また、数100keVの桁の加速を行うための加速管の
長さは数mにも及び、巨大なイオン打込み装置となって
いた。さらに、従来の加速リングを並べた後段加速管で
は、ビームを中心軸上に集める集束作用がないため、一
般にビームは広がり、ビーム損失や試料基板で小口径ビ
ームが得られなかった。又、質量分離器としては一般に
磁場形質量分離器が使われているが、ビームを中心軸に
集めるには特殊な入出射角度の設定や別の収束レンズ等
を使わなければ、効率より強い収束効果は得られなかっ
た。When obtaining high-energy ions with a conventional ion implanter used industrially and implanting them on a substrate, the beam extracted from the ion source is once sorted by the mass separator into the desired ion species, and then this A high energy was used by using an accelerating tube with an accelerating electrode ring and the like. In this case, the high voltage application causes discharge between the acceleration electrodes and so-called corona discharge, and the energy that can be practically achieved is several hundreds at most.
It was about keV. (For example Springer Series in Ele
ctrophsics Volume 10, "Ion Implantation Techvique
s ”, Springer-Verlog Publishing, 1982, p.351)
In addition, the length of the accelerating tube for accelerating to the order of several hundred keV is several meters, which is a huge ion implanter. Further, in the latter-stage accelerating tube in which the conventional accelerating rings are arranged, there is no focusing action for concentrating the beam on the central axis, so that the beam generally spreads, and beam loss and a small-diameter beam cannot be obtained due to the sample substrate. In addition, a magnetic field type mass separator is generally used as a mass separator, but in order to focus the beam on the central axis, unless a special entrance / exit angle setting or another converging lens is used, the convergence is stronger than the efficiency. No effect was obtained.
本発明の目的は、イオン源から引出されたビームをRF
Qなる加速装置を使い、質量分離,加速,収束を同時に
効率良く行い、数100keV〜数MeVのイオンビー
ムを使った高電圧イオン打込み装置を提供することにあ
る。It is an object of the invention to RF the beam extracted from the ion source.
An object is to provide a high-voltage ion implanter using an ion beam of several hundred keV to several MeV, which efficiently performs mass separation, acceleration, and convergence simultaneously by using an accelerator Q.
本発明は、イオン源と試料基板との間に高周波四重極加
速器を設け、この高周波四重極加速器で質量分離とイオ
ンの加速を同時に行い、以って数100keV〜数Me
Vの高エネルギーイオン打込みを実現させるものであ
る。According to the present invention, a high frequency quadrupole accelerator is provided between an ion source and a sample substrate, and mass separation and ion acceleration are performed simultaneously by this high frequency quadrupole accelerator, whereby several hundred keV to several Me.
This is to realize high-energy ion implantation of V.
以下、本発明の一実施例を第1図により説明する。第1
図において、本発明の打込み装置は、イオン源1、高周
波四重極加速器(RFQ)を内蔵したRFQタンク2、
及び試料基板5を内蔵した打込み室3とからなる。高周
波四重極加速器の構造を第2図に示す。第2図におい
て、RFQタンク2は波うった形状を持つ四つの電極2
a,2b,2c,2dからなり、相対する2ケの電極の
出っぱった部分では、残りの2組の電極がへこむよう周
期的な波うった形状になっている。このRFQタンク2
は1種の空洞共振器を構成しており、これに数10〜数
100MHZの周波数をもつ高周波電圧を印加すると、中
心軌道部分に軸方向の加速電界が生じイオンは効率良く
数MeVまで加速される。第1図において、イオン源か
ら引出されたイオンビームは一般に種々のイオン種を含
むが、RFQタンク2の波うたせた周期、印加高周波電
圧に応じ、RFQタンク2内で加速されるものは一種類
のイオンだけであり、他のイオン種は発散して透過でき
ない。又、RFQは一種の収束レンズを構成しているの
で透過可能なビームは中心軸上に集まる収束作用をうけ
る。即ちRFQタンク2の使用により、質量分離と加
速,収束が同時に可能となる。またイオン源1から出る
ビームは高高数10keVでよいため、イオン源1の直
流高圧電源の負担が軽く済み、また装置も小形化でき
た。第1図の実施例では、イオン種ごとに形状及び高周
波電圧の異なったRFQタンク2をつかい、数MeVの
B+,N+,O+,As+,P+,He+等のイオンビームを
パルス状に得ることができた。イオン源には、特公昭57
−4056号公報、同57−11094号公報,同57−11093号公
報、及び同57−41059号公報に記載されたマイクロ波イ
オン源を使用した。ビーム電流としては直流換算で数m
Aの桁のMeVイオンが得られた。An embodiment of the present invention will be described below with reference to FIG. First
In the figure, the implanting apparatus of the present invention is composed of an ion source 1, an RFQ tank 2 containing a high-frequency quadrupole accelerator (RFQ),
And the implantation chamber 3 containing the sample substrate 5. The structure of the high frequency quadrupole accelerator is shown in FIG. In FIG. 2, the RFQ tank 2 has four electrodes 2 having a wavy shape.
a, 2b, 2c, and 2d, and in a portion where two opposing electrodes protrude, the remaining two sets of electrodes have a periodic wavy shape so as to be dented. This RFQ tank 2
Consists of one type of cavity resonator, and when a high-frequency voltage having a frequency of several tens to several hundreds MHZ is applied to this, an accelerating electric field in the axial direction is generated in the central orbital portion, and ions are efficiently accelerated to several MeV. It In FIG. 1, the ion beam extracted from the ion source generally contains various ion species, but one that is accelerated in the RFQ tank 2 depends on the waved period of the RFQ tank 2 and the applied high frequency voltage. It is only one kind of ion, and other ion species diverge and cannot penetrate. Further, since the RFQ constitutes a kind of converging lens, the beams that can be transmitted are subjected to a converging action of concentrating on the central axis. That is, the use of the RFQ tank 2 enables mass separation, acceleration, and convergence at the same time. Further, since the beam emitted from the ion source 1 may have a height of several 10 keV, the burden on the DC high-voltage power source of the ion source 1 can be lightened and the apparatus can be downsized. In the embodiment shown in FIG. 1, an RFQ tank 2 having different shapes and high-frequency voltages for each ion species is used to generate an ion beam of several MeV such as B + , N + , O + , As + , P + , He +. It was possible to obtain in pulse form. As the ion source, Japanese Patent Sho 57
The microwave ion sources described in JP-A-4056, JP-A-57-11094, JP-A-57-11093 and JP-A-57-41059 were used. Beam current is several meters in DC conversion
MeV ions in the order of A were obtained.
次に第1図では、イオン種及び最終エネルギを変えるた
びにRFQタンク2の構造を変える必要があった。この
ためRFQタンク2として外部共振形RFQを使ったと
ころ、1つのRFQで種々のイオン種を加速し、基板に
イオン打込みできた。Next, in FIG. 1, it was necessary to change the structure of the RFQ tank 2 each time the ion species and the final energy were changed. For this reason, when an external resonance type RFQ was used as the RFQ tank 2, it was possible to accelerate various ion species with one RFQ and implant ions into the substrate.
次に別の実施例を第3図により説明する。第1図の打込
み装置では、ビーム最終エネルギーはイオン種とRFQ
の構造により決まる。このため任意のエネルギーを簡単
に得ることは困難である。第3図ではRFQから出たビ
ーム1′を、これも一種の空洞共振器であるシングルギ
ャップ共振器6に入れ、その印加高周波電圧に応じて発
生する減速電界を使い、打込みエネルギーを可変とした
ものである。これにより、同一のRFQタンク2を使
い、一種類のイオン種については、任意のエネルギーで
イオン打込みが可能となった。Next, another embodiment will be described with reference to FIG. In the implanter of FIG. 1, the final energy of the beam is the ion species and the RFQ.
It depends on the structure of. Therefore, it is difficult to easily obtain arbitrary energy. In FIG. 3, the beam 1 ′ emitted from RFQ is put into a single-gap resonator 6 which is also a kind of cavity resonator, and the deceleration electric field generated according to the applied high-frequency voltage is used to make the implantation energy variable. It is a thing. As a result, using the same RFQ tank 2, it is possible to implant ions of one kind with arbitrary energy.
なお、減速のため,シングルギャップの代りに、従来か
ら使われている、円筒リング電極や平板リング電極6′
を複数個並べ、RFQ側の初段の電極を接地電位とし、
試料側にいくにつれ正の電圧を電極に印加した減速電極
系でも同様な効果が得られた。この実施例を第4図に示
す。For deceleration, instead of the single gap, the cylindrical ring electrode or the flat plate ring electrode 6'used conventionally is used.
A plurality of electrodes, the first electrode on the RFQ side is set to the ground potential,
Similar effects were obtained with a deceleration electrode system in which a positive voltage was applied to the electrodes as it went to the sample side. This embodiment is shown in FIG.
次に本発明に基づく別の実施例を第5図に示す。一般に
イオン打込みではシリコンウェーハを初めとして各種基
板の全面に所定の量だけ一様にイオン打込みすることが
要求される。第5図では、このため、試料基板5を回転
する円板13表面に多数枚取付け、ビーム1′に対し半
径方向にも円板13自身を機械的に移動させ、基板5へ
の均一打込みを行っている。この場合、RFQを使って
いることに起因する特有な問題がある。即ち、RFQでは
イオン源1から出たビーム1′が直流的であっても、R
FQ2通過に伴い、塊りとなったパルス状のビームとな
り、そのパルス周期はRFQ2に印加する高周波電圧の
周期に同期する。従って、円板13回転周波数1とR
FQ2印加高周波の周波数2の比が有里数であると、
その値に応じて、照射される場所は回転円板13上でと
びとびの場所となる。したがって本発明では、回転周波
数1については、とびとびの点群のうち、最近接した
2点間の距離がビーム直径より小さくなるようにし、円
周方向に沿って均一なイオン打込みが行えるようにし
た。第5図の一実施例で、10は無理数の有限個の桁の
数を発生させる数値発生器であり、エンコーダ8からの
出力と共に、差動増幅器9に入力させる。差動増幅器9
は両者の値の差な応じて電気出力を出し、円板回転モー
タ7の回転数を制御し、両者の差がゼロになるように工
夫されている。Next, another embodiment according to the present invention is shown in FIG. Generally, in ion implantation, it is required to uniformly implant a prescribed amount of ions onto the entire surface of various substrates including silicon wafers. In FIG. 5, for this reason, a large number of sample substrates 5 are attached to the surface of the rotating disc 13 and the discs 13 themselves are mechanically moved in the radial direction with respect to the beam 1 ′ so that the substrate 5 can be uniformly driven. Is going. In this case, there is a particular problem due to the use of RFQ. That is, in RFQ, even if the beam 1 ′ emitted from the ion source 1 is direct current,
Along with the passage of the FQ2, a pulsed beam becomes a lump, and the pulse cycle is synchronized with the cycle of the high frequency voltage applied to the RFQ2. Therefore, disk 13 rotation frequency 1 and R
If the ratio of the frequency 2 of the high frequency applied to FQ2 is the number of Risato,
Depending on the value, the irradiation location is a discrete location on the rotating disk 13. Therefore, in the present invention, for the rotation frequency 1 , the distance between the two closest points of the discrete point group is smaller than the beam diameter, and uniform ion implantation can be performed along the circumferential direction. . In one embodiment of FIG. 5, numeral 10 is a numerical value generator for generating a finite number of irrational numbers, which is input to the differential amplifier 9 together with the output from the encoder 8. Differential amplifier 9
Is designed to output an electric output in accordance with the difference between the two values, control the rotation speed of the disk rotation motor 7, and make the difference between the two zero.
本発明に基づく別の実施例を第6図に示す。第6図では
RFQ2と打込み基板5の間にビームをXY方向に走査
させるビーム走査電極系11を設け、基板5での均一打
込みを行った。この場合、第5図で示したようにX,Y
方向の走査周波数はRFQ周波数より小さくした。この
場合、基板5上でとびとびの照射点群の二点間の距離は
X,Y電極電圧及びその周波数に依存する。本実施例で
は、最近接する二点間の照射位置がビーム直径より小さ
くなるようにした。図では電場を使った実施例を示した
が、磁場コイルを使ったXY走査系でも、同様な均一打
込みが実現できた。Another embodiment according to the present invention is shown in FIG. In FIG. 6, a beam scanning electrode system 11 for scanning a beam in the XY directions is provided between the RFQ 2 and the implantation substrate 5, and uniform implantation is performed on the substrate 5. In this case, as shown in FIG. 5, X, Y
The scanning frequency in the direction was smaller than the RFQ frequency. In this case, the distance between the two irradiation spots on the substrate 5 depends on the X and Y electrode voltages and their frequencies. In this embodiment, the irradiation position between the two closest points is smaller than the beam diameter. Although an example using an electric field is shown in the figure, the same uniform implantation can be realized by an XY scanning system using a magnetic field coil.
次に、本発明に基づく別の実施例を第7図に示す。第7
図ではイオン源1とRFQタンク2の間にビーム収束用
の二段の磁気四重極レンズ12a,12bをとりつけて
いる。一般に大電流イオン源のビーム断面は長方形断面
である。これに対し、RFQのビーム通過部は数mm〜数
cmの半径をもつ円形部分である。従って、イオン源から
引出されたビームをビーム損失なく有効に加速するには
ビーム断面をRFQ入射部に合った形状に変換する必要
がある。本実施例では二段の磁気四重極レンズを使い、
大電流ビームが有効にRFQ2に導入され、打込み電流
も1mA以上に改善された。Next, another embodiment based on the present invention is shown in FIG. 7th
In the figure, two-stage magnetic quadrupole lenses 12a and 12b for focusing the beam are mounted between the ion source 1 and the RFQ tank 2. Generally, the beam cross section of a high current ion source is a rectangular cross section. On the other hand, the beam passing part of RFQ is several mm to several mm.
A circular part with a radius of cm. Therefore, in order to effectively accelerate the beam extracted from the ion source without beam loss, it is necessary to convert the beam cross section into a shape suitable for the RFQ incident part. In this embodiment, a two-stage magnetic quadrupole lens is used,
A high current beam was effectively introduced into RFQ2, and the driving current was also improved to 1 mA or more.
以上説明した本発明の高電圧イオン打込み装置によれ
ば、イオン源と試料基板との間に高周波四重極加速器を
設け、この高周波四重極加速器で質量分離とイオンの加
速を同時に行うようにしたものであるから、数100K
eV〜数MeV領域の種々の大電流イオンビームを効率
良く打込みすることが可能となり、実用に供し、その効
果は著しく大である。According to the high-voltage ion implantation apparatus of the present invention described above, a high-frequency quadrupole accelerator is provided between the ion source and the sample substrate, and mass separation and ion acceleration are performed simultaneously with this high-frequency quadrupole accelerator. Because it was done, several hundred K
It becomes possible to efficiently implant various high-current ion beams in the eV to several MeV range, which is put to practical use, and the effect is extremely large.
第1図は本発明の高電圧イオン打込み装置の一実施例を
示す図、第2図は第1図中に用いられたRFQタンクの詳
細を一部破断して示す斜視図、第3図ないし第7図は本
発明の高電圧イオン打込み装置のそれぞれ別の実施例を
示す図である。 1…イオン源、1′…イオンビーム、2…高周波四重極
加速器、3…打込み室、4…電流測定のためのファラデ
ーカップ、5…打込み試料基板、6…シングルギャップ
共振器、7…回転用モータ、8…エンコーダ、9…差動
増幅器、10…数値発生器、11…ビーム走査電極系、
12…磁気四重極レンズ、6″…減速用電極。FIG. 1 is a diagram showing an embodiment of the high voltage ion implantation apparatus of the present invention, and FIG. 2 is a perspective view showing the details of the RFQ tank used in FIG. FIG. 7 is a diagram showing different embodiments of the high voltage ion implantation apparatus of the present invention. DESCRIPTION OF SYMBOLS 1 ... Ion source, 1 '... Ion beam, 2 ... High frequency quadrupole accelerator, 3 ... Implanting chamber, 4 ... Faraday cup for current measurement, 5 ... Implanted sample substrate, 6 ... Single gap resonator, 7 ... Rotation Motor, 8 ... Encoder, 9 ... Differential amplifier, 10 ... Numerical value generator, 11 ... Beam scanning electrode system,
12 ... Magnetic quadrupole lens, 6 ″ ... deceleration electrode.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 小池 英巳 東京都国分寺市東恋ヶ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 斉藤 徳郎 東京都国分寺市東恋ヶ窪1丁目280番地 株式会社日立製作所中央研究所内 (72)発明者 小笹 進 東京都国分寺市東恋ヶ窪1丁目280番地 株式会社日立製作所中央研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hidemi Koike 1-280 Higashi Koigakubo, Kokubunji, Tokyo Inside Hitachi Central Research Laboratory (72) Inventor Tokuro Saito 1-280 Higashi Koigakubo, Kokubunji, Tokyo Hitachi Ltd. Central Research Laboratory (72) Inventor Susumu Kosasa 1-280, Higashikoigakubo, Kokubunji, Tokyo Hitachi Research Laboratory, Hitachi Ltd.
Claims (5)
質量分離し、目的とするイオン試料基板に所定の量だけ
混入させるイオン打込み装置において、 前記イオン源と試料基板との間に高周波四重極加速器を
設け、該高周波四重極加速器で質量分離とイオンの加速
を同時に行うことを特徴とする高電圧イオン打込み装
置。1. An ion implanting apparatus for mass-separating a beam of ions extracted from an ion source and mixing the beam into a target ion sample substrate by a predetermined amount, wherein a high frequency quadruple is provided between the ion source and the sample substrate. A high-voltage ion implanting device, which is provided with a polar accelerator, and performs mass separation and ion acceleration at the same time by the high-frequency quadrupole accelerator.
にイオンの減速を行うシングルギャップ形減速器、もし
くは平板,円筒状の減速用電極系を設け、該シングルギ
ャップ形減速器、もしくは減速用電極系で打込みイオン
のエネルギーを可変としたことを特徴とする特許請求の
範囲第1項記載の高電圧イオン打込み装置。2. A single gap type speed reducer for decelerating ions between the high frequency quadrupole accelerator and the sample substrate, or a flat plate or cylindrical electrode system for speed reduction, wherein the single gap type speed reducer, or The high-voltage ion implantation apparatus according to claim 1, wherein the energy of the implanted ions is variable by the deceleration electrode system.
取付け、かつ、ビームに対し半径方向に円板自身を駆動
せしめ、試料基板全体に均一にイオン打込みを可能とし
た打込み室を設け、前記円板の回転周波数を前記高周波
四重極加速器に印加する高周波電圧の周波数より小さく
し、かつ、その回転周波数については、回転円周方向に
沿って規則的に飛び飛びにビーム照射をうける点群のう
ち、もっとも近接した2点間の距離がビーム直径より小
さくなるように周波数値を選び、以って基板への均一打
込みをできるようにしたことを特徴とする特許請求の範
囲第1項、又は第2項記載の高電圧イオン打込み装置。3. A plurality of said sample substrates are mounted on the surface of a rotating disk, and the disk itself is driven in the radial direction with respect to the beam to provide an implantation chamber capable of uniformly implanting ions on the entire sample substrate. The rotation frequency of the disk is made smaller than the frequency of the high-frequency voltage applied to the high-frequency quadrupole accelerator, and the rotation frequency is such that the beam is regularly and intermittently irradiated along the rotation circumferential direction. The frequency value is selected so that the distance between the two points closest to each other in the group is smaller than the beam diameter, so that uniform implantation can be performed on the substrate. Alternatively, the high-voltage ion implantation apparatus according to item 2.
に電場、あるいは磁場、あるいはこれらを組合せたビー
ム走査手段を設けると共に、ビーム走査周波数を高周波
四重極加速器に印加する周波数より小さくし、かつ、走
査電圧、及び周波数については、基板上で規則的に飛び
飛びにビーム照射をうける点群のうち、X,Y方向のも
っとも近接した2点間の距離がビーム直径より小さくな
るように電圧値、及び周波数値を選んだことを特徴とす
る特許請求の範囲第1項、又は第2項記載の高電圧イオ
ン打込み装置。4. An electric field, a magnetic field, or a beam scanning means combining them is provided between the high frequency quadrupole accelerator and the sample substrate, and the beam scanning frequency is smaller than the frequency applied to the high frequency quadrupole accelerator. As for the scanning voltage and the frequency, the distance between the two closest points in the X and Y directions of the point group that receives the beam irradiation regularly on the substrate is smaller than the beam diameter. The high-voltage ion implantation device according to claim 1 or 2, wherein a voltage value and a frequency value are selected.
に、該イオン源から出たイオンビームを効率良く高周波
四重極加速器内に導入せしめる多段の磁気四重極レンズ
を設けたことを特徴とする特許請求の範囲第1項、又は
第2項記載の高電圧イオン打込み装置。5. A multi-stage magnetic quadrupole lens is provided between the ion source and the high frequency quadrupole accelerator to efficiently introduce an ion beam emitted from the ion source into the high frequency quadrupole accelerator. The high-voltage ion implantation apparatus according to claim 1 or 2, characterized in that.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58226860A JPH0612660B2 (en) | 1983-12-02 | 1983-12-02 | High voltage ion implanter |
| PCT/JP1984/000557 WO1985002489A1 (en) | 1983-11-28 | 1984-11-22 | Quadrupole particle accelerator |
| DE8484904176T DE3477528D1 (en) | 1983-11-28 | 1984-11-22 | Quadrupole particle accelerator |
| US06/763,133 US4801847A (en) | 1983-11-28 | 1984-11-22 | Charged particle accelerator using quadrupole electrodes |
| EP84904176A EP0163745B1 (en) | 1983-11-28 | 1984-11-22 | Quadrupole particle accelerator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58226860A JPH0612660B2 (en) | 1983-12-02 | 1983-12-02 | High voltage ion implanter |
Related Child Applications (2)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8209591A Division JP2723106B2 (en) | 1996-08-08 | 1996-08-08 | High voltage ion implanter |
| JP8209592A Division JP2954536B2 (en) | 1996-08-08 | 1996-08-08 | High voltage ion implanter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60121655A JPS60121655A (en) | 1985-06-29 |
| JPH0612660B2 true JPH0612660B2 (en) | 1994-02-16 |
Family
ID=16851700
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58226860A Expired - Lifetime JPH0612660B2 (en) | 1983-11-28 | 1983-12-02 | High voltage ion implanter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0612660B2 (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4667111C1 (en) * | 1985-05-17 | 2001-04-10 | Eaton Corp Cleveland | Accelerator for ion implantation |
| JP2569812B2 (en) * | 1989-06-30 | 1997-01-08 | 株式会社島津製作所 | High energy ion implanter |
| JPH0821355B2 (en) * | 1992-12-24 | 1996-03-04 | 株式会社日立製作所 | High energy ion implanter |
| JPH0773041B2 (en) * | 1993-03-02 | 1995-08-02 | 株式会社日立製作所 | Ion implanter |
| JP2613351B2 (en) * | 1993-04-02 | 1997-05-28 | 株式会社日立製作所 | Ion implantation equipment |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5834600A (en) * | 1981-08-25 | 1983-03-01 | 株式会社東芝 | High frequency quadruple pole accelerator |
-
1983
- 1983-12-02 JP JP58226860A patent/JPH0612660B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60121655A (en) | 1985-06-29 |
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