JPH0542099B2 - - Google Patents

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Publication number
JPH0542099B2
JPH0542099B2 JP62091973A JP9197387A JPH0542099B2 JP H0542099 B2 JPH0542099 B2 JP H0542099B2 JP 62091973 A JP62091973 A JP 62091973A JP 9197387 A JP9197387 A JP 9197387A JP H0542099 B2 JPH0542099 B2 JP H0542099B2
Authority
JP
Japan
Prior art keywords
electron beam
sample
mask
linear
area
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
Application number
JP62091973A
Other languages
Japanese (ja)
Other versions
JPS63259947A (en
Inventor
Tsuyoshi Nakamura
Hiromitsu Namita
Hidekazu Okabayashi
Yutaka Kawase
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP62091973A priority Critical patent/JPS63259947A/en
Publication of JPS63259947A publication Critical patent/JPS63259947A/en
Publication of JPH0542099B2 publication Critical patent/JPH0542099B2/ja
Granted legal-status Critical Current

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  • Electron Sources, Ion Sources (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は線状電子ビーム装置に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to a linear electron beam device.

(従来の技術) 従来、半導体基板等を熱処理する一つの方法と
して断面形状がほぼ矩形(線状)である線状電子
ビームを、固定された基板上に照射し走査させる
方法が行われてきた。(「エネルギビーム加工」精
機学会エネルギビーム分析会編、リアライズ社、
1985年、268頁。「第5回新機能素子技術シンポジ
ウム予稿集」新機能素子開発協会、1986年、145
頁〜152頁)。従来の電子ビーム装置では、第5図
の概略構成図に示したように、試料9上に線状電
子ビームを収束させ、偏向器6で電子ビームを偏
向させることにより試料上を広範囲に走査させ、
試料9を熱処理してきた。
(Prior art) Conventionally, one method of heat treating semiconductor substrates, etc. has been to irradiate and scan a fixed substrate with a linear electron beam whose cross section is approximately rectangular (linear). . (“Energy Beam Processing” Edited by Energy Beam Analysis Society, Japan Society of Precision Machinery Engineers, Realize Inc.,
1985, 268 pages. "Proceedings of the 5th New Functional Device Technology Symposium" New Functional Device Development Association, 1986, 145
p.-152). In a conventional electron beam device, as shown in the schematic diagram of FIG. 5, a linear electron beam is focused on a sample 9 and the electron beam is deflected by a deflector 6 to scan over a wide range of the sample. ,
Sample 9 has been heat treated.

(発明が解決しようとする問題点) しかしながら、線状電子ビーム4の収束状態
は、線状カソード1とウエーネルト電極2とアノ
ード3の電子銃やレンズ5と偏向器6の電子光学
系によつて調整されるが、線状電子ビームが非軸
対称であることや、偏向幅が大きいことなどのた
めに、良好なビーム電流密度を持つた線状電子ビ
ームを広範囲で得るように制御することは困難で
あつた。そのため、例えば、電子ビームアニール
法をSOI(Silicon−On−Insulator)形成技術に使
用する場合、2インチあるいは4インチ以上のウ
エハ全面を均一にアニールするとき広範囲のアニ
ールが難しく実用化の大きな障害となつていた。
(Problem to be Solved by the Invention) However, the convergence state of the linear electron beam 4 is determined by the electron gun of the linear cathode 1, the Wehnelt electrode 2, and the anode 3, and the electron optical system of the lens 5 and the deflector 6. However, because the linear electron beam is non-axisymmetric and the deflection width is large, it is difficult to control the linear electron beam to obtain a linear electron beam with good beam current density over a wide range. It was difficult. For this reason, for example, when electron beam annealing is used in SOI (Silicon-On-Insulator) formation technology, it is difficult to anneal a wide area uniformly over the entire surface of a 2-inch or 4-inch wafer, which is a major obstacle to practical application. I was getting used to it.

本発明の目的は、この様な問題を解決し、大面
積領域をむらなく均一に電子ビーム照射による熱
処理ができる線状電子ビーム装置を提供すること
にある。
SUMMARY OF THE INVENTION An object of the present invention is to solve these problems and provide a linear electron beam device that can evenly and uniformly heat-treat a large area by electron beam irradiation.

(問題を解決するための手段) 本発明の線状電子ビーム装置は、試料の線状電
子ビーム照射面直近に配置され、略鼓形の開口部
を有し該開口部のみ電子ビームを通過させ開口部
以外は電子ビームを遮断する手段としてのマスク
を備えたことを特徴とする構成を取る。
(Means for Solving the Problem) The linear electron beam device of the present invention is disposed in close proximity to the linear electron beam irradiation surface of a sample, has a substantially drum-shaped opening, and only allows the electron beam to pass through the opening. The structure is characterized in that a mask is provided as a means for blocking the electron beam except for the opening.

(作用) 本発明の電子ビーム装置によれば、マスクの開
口幅を収差等の極めて少ない安定したビーム得ら
れる最大偏向幅以下にし、試料をマスク開口部を
通過した電子ビームの照射位置に合わせた後、該
マスクの開口幅よりも大きく線状電子ビームを走
査することにより、電子ビーム照射による熱処理
領域を電子ビームの収差等の極めて少ない良好な
状態であるマスク開口部を通過した電子ビームの
照射領域に限定することが出来る。電子ビームは
試料に照射された極電子の持つ運動エネルギによ
つて試料を加熱し、温度が融点以上になると試料
が溶融するが、熱は試料の温度に低い方に逃げ
る。この熱の逃げを考慮すると、第4図に示すよ
うにマスク20のマスク開口21が矩形の場合、
電子ビームが試料に照射されアニールが開始及び
終了するところでは線状電子ビームが照射される
両端(第4図A部)からの熱の逃げ22が中央部
(第4図C部)よりも多いため中央部から溶融し
アニール形状が走査方向前後端で凸型になり、ま
た走査方向両側(第4図B部)に関しては熱の逃
げは一定と考えられるため全体のアニール形状は
電子ビーム照射領域20が矩形であるにもかかわ
らず試料溶融領域21に示すようになると考えら
れる。そこで、第2図に示すようにマスク開口1
6を線状電子ビームが走査時に横切る2辺を開口
内側に凹状にし、試料への電子ビーム照射を線状
長手方向両端から先に行うことによりアニール形
状を第2図の試料溶融領域17に示すように矩形
に整えることが出来る。この作用はマスクの線状
電子ビーム長辺のカツトの有無によらず同じもの
であるのでマスクで線状電子ビームの長辺両端を
カツトして電子ビームの長さを整えても良い。
(Function) According to the electron beam device of the present invention, the aperture width of the mask is set to be equal to or less than the maximum deflection width that can obtain a stable beam with extremely few aberrations, and the sample is aligned with the irradiation position of the electron beam that has passed through the mask aperture. After that, by scanning a linear electron beam wider than the aperture width of the mask, the heat-treated area by electron beam irradiation is irradiated with the electron beam that has passed through the mask aperture, which is in a good condition with very little electron beam aberration. It can be limited to an area. The electron beam heats the sample using the kinetic energy of the polar electrons irradiated onto the sample, and when the temperature rises above the melting point, the sample melts, but the heat escapes to the lower sample temperature. Considering this heat escape, if the mask opening 21 of the mask 20 is rectangular as shown in FIG.
Where the sample is irradiated with the electron beam and annealing begins and ends, more heat escapes 22 from both ends (section A in FIG. 4) where the linear electron beam is irradiated than from the center (section C in FIG. 4). Therefore, melting starts from the center and the annealed shape becomes convex at the front and rear ends in the scanning direction, and since the heat escape is considered to be constant on both sides in the scanning direction (section B in Figure 4), the overall annealed shape is similar to the electron beam irradiation area. Although 20 is rectangular, it is considered that the sample melting region 21 becomes as shown. Therefore, as shown in FIG.
6, the two sides crossed by the linear electron beam during scanning are made concave inside the opening, and the sample is irradiated with the electron beam from both ends in the longitudinal direction of the line first, resulting in an annealed shape as shown in the sample melting region 17 in Fig. 2. You can arrange it into a rectangle like this. Since this effect is the same whether or not the long side of the linear electron beam is cut by the mask, the length of the electron beam may be adjusted by cutting both ends of the long side of the linear electron beam using the mask.

(実施例) 第1図は本発明の一実施例の主要な構成図を示
したものである。
(Embodiment) FIG. 1 shows a main configuration diagram of an embodiment of the present invention.

真空容器14内の線状カソード1とウエーネル
ト電極2と陽極3から構成される電子銃から出射
された線状電子ビーム4は、レンズ5によつて試
料9上に線状電子ビームとして結像される。結像
された線状電子ビームは偏向器6によつて試料9
上を走査するがマスク8によつて線状電子ビーム
は遮断されマスク開口7部分のみ線状電子ビーム
は通過し、マスク開口7を通過した電子ビームの
照射領域の試料9上のみ電子ビームにより熱処理
がされる。試料9は試料ホルダ10にセツトさ
れ、試料加熱ヒータ13等の手段によつて例えば
約600℃に予備加熱される。さらに試料を移動す
る機構を設けてもよく、例えば、試料ホルダ10
をXYテーブル12上にセツトし、XYテーブル
駆動系11によつて電子ビーム照射により熱処理
したい試料範囲がマスク開口7を通過した電子ビ
ームの照射領域内に位置するように試料9を移動
し、線状電子ビームを照射し熱処理する。電子ビ
ーム照射による熱処理後次に熱処理したい試料範
囲がマスク開口7を通した電子ビームの照射領域
内にくるように試料を移動し電子ビーム照射によ
る熱処理をする。この繰り返しにより、試料の所
定の領域をむら無く均一に広範囲に電子ビームに
よる熱処理をすることが出来る。
A linear electron beam 4 emitted from an electron gun consisting of a linear cathode 1, a Wehnelt electrode 2, and an anode 3 in a vacuum vessel 14 is imaged by a lens 5 onto a sample 9 as a linear electron beam. Ru. The focused linear electron beam is directed to the sample 9 by the deflector 6.
However, the linear electron beam is blocked by the mask 8 and passes only through the mask opening 7, and only the sample 9 in the irradiation area of the electron beam that has passed through the mask opening 7 is heat-treated by the electron beam. is done. The sample 9 is set in the sample holder 10 and preheated to, for example, about 600° C. by a sample heater 13 or the like. Furthermore, a mechanism for moving the sample may be provided, for example, the sample holder 10.
is set on the XY table 12, and the sample 9 is moved by the XY table drive system 11 so that the sample area to be heat treated by electron beam irradiation is located within the irradiation area of the electron beam that has passed through the mask opening 7, and the line Heat treatment is performed by irradiating a shaped electron beam. After the heat treatment by electron beam irradiation, the sample is moved so that the area of the sample to be heat treated is within the irradiation area of the electron beam through the mask opening 7, and heat treatment is performed by electron beam irradiation. By repeating this process, a predetermined region of the sample can be evenly and uniformly heat-treated over a wide range with the electron beam.

第2図は第1図のマスクと電子ビーム走査と試
料への照射状態とアニール状態を示したものであ
る。
FIG. 2 shows the mask shown in FIG. 1, electron beam scanning, sample irradiation state, and annealing state.

線状電子ビーム4はマスク8に設けられたマス
ク開口7の内側に凹状になつた辺を横切り走査さ
れる。電子ビーム走査範囲15はマスク開口幅よ
り大きく設定され、走査された電子ビームはマス
ク開口7を通過し試料上に電子ビーム照射領域1
6のように照射され、熱の逃げなどによりアニー
ルされる領域は試料溶融領域17となる。マスク
開口形状は各種考えられ、例えば第3図に示すよ
うに線状電子ビームが横切る辺を(a)のように曲線
としても、(b)のように三角形としても、(c)のよう
に多角形としても良い。また、マスク開口凹部は
対称である必要はなく、熱の逃げ具合で適時変形
させるのが良い。
The linear electron beam 4 is scanned across the concave side of the mask opening 7 provided in the mask 8 . The electron beam scanning range 15 is set larger than the mask aperture width, and the scanned electron beam passes through the mask aperture 7 and forms an electron beam irradiation area 1 on the sample.
The area irradiated as shown in 6 and annealed by heat escape becomes a sample melting area 17. Various mask aperture shapes are possible; for example, as shown in Figure 3, the side that the linear electron beam crosses can be curved as in (a), triangular as in (b), or triangular as in (c). It may also be a polygon. Further, the mask opening recess does not need to be symmetrical, and may be deformed as appropriate depending on the condition of heat escape.

(発明の効果) 以上述べたとおり、本発明によれば、電子ビー
ム照射により熱処理される領域をマスクによつて
線状電子ビームが良好な状態の部分のみに限定し
電子ビームの収差等の不安定な要素を減らすこと
が出来る。また、アニール形状を矩形に整えるこ
とができるためアニール形状をチツプサイズに合
わせることが容易になる。さらに必要に応じ、試
料を順次、例えば間欠方式で、移動させた広範囲
に均一な電子ビーム照射による熱処理を行うこと
が出来る。このような諸効果により大口径ウエハ
等の電子ビーム照射による大面積熱処理の歩留ま
りを飛躍的に向上させることが出来る。
(Effects of the Invention) As described above, according to the present invention, the area to be heat-treated by electron beam irradiation is limited to only the area where the linear electron beam is in a good condition by using a mask, thereby preventing electron beam aberrations and other problems. Stable elements can be reduced. Furthermore, since the annealed shape can be arranged into a rectangular shape, it becomes easy to match the annealed shape to the chip size. Furthermore, if necessary, heat treatment can be performed by uniformly irradiating the sample with an electron beam over a wide range while moving the sample sequentially, for example, in an intermittent manner. These effects can dramatically improve the yield of large-area heat treatment by electron beam irradiation of large-diameter wafers and the like.

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

第1図は本発明による装置の一実施例の全体概
略構成図、第2図は第1図のマスクと電子ビーム
走査と照射状態とアニール状態の概念図、第3図
は本発明によるマスク開口形状の一部の例を示し
た図、第4図はマスク開口形状が矩形の場合のマ
スクと電子ビーム走査と照射状態とアニール状態
の概念図、第5図は従来装置の全体概略構成図を
示したものである。 図に於て、1は線状カソード、2はウエーネル
ト電極、3は陽極、4は線状電子ビーム、5はレ
ンズ、6は偏向器、7はマスク開口、8はマス
ク、9は試料、10は試料ホルダ、11はXYテ
ーブル駆動系、12はXYテーブル、13は試料
加熱ヒータ、14は真空容器、15は電子ビーム
走査範囲、16は電子ビーム照射領域、17は試
料溶融領域、18はマスク、19はマスク開口、
20は電子ビーム照射領域、21は試料溶融領
域、22は熱の逃げをそれぞれ示す。
FIG. 1 is an overall schematic configuration diagram of an embodiment of the apparatus according to the present invention, FIG. 2 is a conceptual diagram of the mask in FIG. 1, electron beam scanning, irradiation state, and annealing state, and FIG. 3 is a mask opening according to the present invention. Figure 4 is a conceptual diagram of the mask, electron beam scanning, irradiation state, and annealing state when the mask opening shape is rectangular, and Figure 5 is a schematic diagram of the overall configuration of the conventional device. This is what is shown. In the figure, 1 is a linear cathode, 2 is a Wehnelt electrode, 3 is an anode, 4 is a linear electron beam, 5 is a lens, 6 is a deflector, 7 is a mask aperture, 8 is a mask, 9 is a sample, 10 11 is a sample holder, 11 is an XY table drive system, 12 is an XY table, 13 is a sample heater, 14 is a vacuum container, 15 is an electron beam scanning range, 16 is an electron beam irradiation area, 17 is a sample melting area, and 18 is a mask , 19 is a mask opening,
Reference numeral 20 indicates an electron beam irradiation region, 21 indicates a sample melting region, and 22 indicates a heat escape region.

Claims (1)

【特許請求の範囲】[Claims] 1 線状電子ビーム装置に於て、試料の線状電子
ビーム照射面直近に配置され、略鼓形の開口部を
有し、該開口部のみ電子ビームを通過させ、開口
部以外は電子ビームを遮断する手段としてのマス
クを備えたことを特徴とする線状電子ビーム装
置。
1. In a linear electron beam device, it is placed in close proximity to the linear electron beam irradiation surface of the sample and has an approximately drum-shaped opening, and only this opening allows the electron beam to pass through, while other parts other than the opening do not pass the electron beam. A linear electron beam device characterized by being equipped with a mask as a blocking means.
JP62091973A 1987-04-16 1987-04-16 Linear electron beam device Granted JPS63259947A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62091973A JPS63259947A (en) 1987-04-16 1987-04-16 Linear electron beam device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62091973A JPS63259947A (en) 1987-04-16 1987-04-16 Linear electron beam device

Publications (2)

Publication Number Publication Date
JPS63259947A JPS63259947A (en) 1988-10-27
JPH0542099B2 true JPH0542099B2 (en) 1993-06-25

Family

ID=14041469

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62091973A Granted JPS63259947A (en) 1987-04-16 1987-04-16 Linear electron beam device

Country Status (1)

Country Link
JP (1) JPS63259947A (en)

Also Published As

Publication number Publication date
JPS63259947A (en) 1988-10-27

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