JPH0458445A - Electron beam source - Google Patents

Electron beam source

Info

Publication number
JPH0458445A
JPH0458445A JP2166253A JP16625390A JPH0458445A JP H0458445 A JPH0458445 A JP H0458445A JP 2166253 A JP2166253 A JP 2166253A JP 16625390 A JP16625390 A JP 16625390A JP H0458445 A JPH0458445 A JP H0458445A
Authority
JP
Japan
Prior art keywords
acceleration
region
cathode
insulator
ions
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
JP2166253A
Other languages
Japanese (ja)
Other versions
JP2538804B2 (en
Inventor
Tamio Hara
民夫 原
Manabu Hamagaki
浜垣 学
Katsunobu Aoyanagi
克信 青柳
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.)
RIKEN
Original Assignee
RIKEN
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 RIKEN filed Critical RIKEN
Priority to JP2166253A priority Critical patent/JP2538804B2/en
Publication of JPH0458445A publication Critical patent/JPH0458445A/en
Application granted granted Critical
Publication of JP2538804B2 publication Critical patent/JP2538804B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Drying Of Semiconductors (AREA)
  • Electron Sources, Ion Sources (AREA)

Abstract

PURPOSE:To prevent sputtering due to ions of acceleration electrode for evading metal contamination in an acceleration region and an ion generation region by covering a surface of an acceleration cathode opposing to an acceleration anode with an insulator. CONSTITUTION:A surface of an acceleration cathode 2 facing to an acceleration cathode 4 is covered with an insulator 3. For the insulator 3, ceramics can be used in addition to a glass plate. Ions accelerated inside an acceleration region reach the whole surface of the acceleration cathode 2 so as to extinguish space charge due to electrons near the hole of an acceleration cathode 2 while in the other area, ions come to strike the insulator surface, however, ions have no such energy as to sputter an insulator. Accordingly, contamination of a plasma region due to sputtering and metal contamination of a semiconductor wafer can be avoided.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、再結晶化による半導体ウェハの表面処理、半
導体ウェハのエツチング、成膜に利用できる電子ビーム
源に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an electron beam source that can be used for surface treatment of semiconductor wafers by recrystallization, etching of semiconductor wafers, and film formation.

(従来の技術) 第2図にこの従来の電子ビーム源を示す。第2図におい
て、5はプラズマ領域、2は加速陰極、6は電子ビーム
加速領域、4は加速陽極そして7はイオン生成領域を示
す。この従来の電子ビーム源を半導体ウェハのエツチン
グに利用するときの動作を説明する。アルゴンガスを導
入口11aから供給し、排気口12a、12bから排出
して、プラズマ領域5にほぼ10−’)−ル程度のアル
ゴン雰囲気をつくり、そして電子ビーム加速領域6にほ
ぼ10−’トール程度のアルゴン雰囲気をつくる。又、
導入口11bから塩素ガスを供給し、排気口12cから
排出して、イオン生成領域7にはN’l0−3)−ル程
度の塩素雰囲気をつくる。
(Prior Art) FIG. 2 shows this conventional electron beam source. In FIG. 2, 5 is a plasma region, 2 is an accelerating cathode, 6 is an electron beam accelerating region, 4 is an accelerating anode, and 7 is an ion generating region. The operation of this conventional electron beam source when used for etching a semiconductor wafer will be explained. Argon gas is supplied from the inlet 11a and exhausted from the exhaust ports 12a and 12b to create an argon atmosphere of approximately 10-' Torr in the plasma region 5, and approximately 10-' Torr in the electron beam acceleration region 6. Create a moderate argon atmosphere. or,
Chlorine gas is supplied from the inlet 11b and discharged from the exhaust port 12c to create a chlorine atmosphere of approximately N'l0-3) in the ion generation region 7.

放電用電源8によってプラズマ領域5内につくった電界
によりカソードからの電子をアルゴン雰囲気内で加速し
て、プラズマを生成する。加速用電源9は加速電極4に
向う電位勾配を電子ビーム加速領域6に確立し、プラズ
マ領域から加速陰極2の孔を通して拡散してくる電子を
加速する。この加速電子による塩素原子の電離断面積を
最大とするエネルギーを電子に与えるよう加速用電源の
電位は100v程度とする。この加速電子は加速陽極4
の孔を通ってイオン生成領域7に入り、塩素プラズマを
生成する。電子ビームコレクタ13を加速陽極4に対し
て負電位としてコレクタ13に配置した半導体ウェハ(
図示せず)をエツチングする。
An electric field created in the plasma region 5 by the discharge power source 8 accelerates electrons from the cathode in an argon atmosphere to generate plasma. The acceleration power source 9 establishes a potential gradient in the electron beam acceleration region 6 toward the acceleration electrode 4 and accelerates electrons diffusing from the plasma region through the holes in the acceleration cathode 2 . The potential of the acceleration power source is set to about 100 V so as to give the electrons energy that maximizes the ionization cross section of the chlorine atoms by the accelerated electrons. These accelerated electrons are transferred to the accelerated anode 4
It enters the ion generation region 7 through the hole and generates chlorine plasma. A semiconductor wafer (
(not shown).

この従来装置の特徴は、低エネルギーで大電流を供給す
ることができる、すなわち電子ビーム加速領域の加速電
圧が低いにもか〜わらず、加速陽極を通る電流はIOA
程度の大きな電流とすることができる。イオン生成領域
7のプラズマからのイオンが加速陽極4の孔を通って電
子ビーム加速領域6内に浸出してくると、このイオンは
電子とは逆方向に加速されて加速陰極の孔付近に到達し
て、この孔付近の電子による空間電荷を中和して、プラ
ズマ領域5からの電子の浸出の空間電荷による抑制を排
除するからである。
The feature of this conventional device is that it can supply a large current with low energy, that is, even though the accelerating voltage in the electron beam accelerating region is low, the current passing through the accelerating anode is IOA
It is possible to generate a relatively large current. When ions from the plasma in the ion generation region 7 pass through the holes in the acceleration anode 4 and leak into the electron beam acceleration region 6, these ions are accelerated in the opposite direction to the electrons and reach the vicinity of the holes in the acceleration cathode. This is because the space charge caused by electrons near this hole is neutralized, and the suppression of the leakage of electrons from the plasma region 5 by the space charge is eliminated.

(発明が解決しようとする問題点) 加速領域6内で加速陰極2に向かってイオンが加速され
るとき、イオンは加速陰極2全体を叩いてスパッタリン
グを生じさせてしまう。この結果、加速領域6の壁面を
汚染するばかりでなく、加速陽極4の孔を通ってイオン
生成領域7に侵入して、半導体ウェハを汚染するという
問題があった。
(Problems to be Solved by the Invention) When ions are accelerated toward the acceleration cathode 2 within the acceleration region 6, the ions hit the entire acceleration cathode 2, causing sputtering. As a result, there was a problem that not only the wall surface of the acceleration region 6 was contaminated, but also the ions entered the ion generation region 7 through the holes of the acceleration anode 4 and contaminated the semiconductor wafer.

(問題を解決するための手段) 本発明の目的は、加速電極のイオンによるスパッタリン
グを防止して加速領域とイオン生成領域における金属汚
染を回避した低エネルギー大電流電子ビーム源を提供す
ることである。
(Means for Solving the Problem) An object of the present invention is to provide a low-energy, high-current electron beam source that prevents sputtering of accelerating electrodes by ions and avoids metal contamination in the accelerating region and ion generation region. .

この目的は本発明に従って加速陰極の加速陽極に対向す
る面を絶縁物で覆うことによって達成される。
This object is achieved according to the invention by covering the surface of the accelerating cathode facing the accelerating anode with an insulating material.

(作 用) 加速領域内で加速されたイオンは加速陰極2の全面に到
達し、加速陰極2の孔付近では電子による空間電荷を消
滅させ、その他の区域では絶縁物表面をイオンは叩くこ
とになるが、イオンは絶縁物をスパッタする程のエネル
ギーは持たない。
(Function) The ions accelerated in the acceleration region reach the entire surface of the acceleration cathode 2, and near the holes of the acceleration cathode 2, the space charge caused by electrons disappears, and in other areas, the ions hit the surface of the insulator. However, ions do not have enough energy to sputter an insulator.

(実施例) 本発明の低エネルギー大電流電子ビーム源の実施例を第
1図に示す。第1図で第2図と同じ部分は同じ参照数字
で示し、その説明は省略する。
(Embodiment) An embodiment of the low-energy, high-current electron beam source of the present invention is shown in FIG. The same parts in FIG. 1 as in FIG. 2 are designated by the same reference numerals, and their explanation will be omitted.

第1図に示すように、加速陰極2の加速陰極4に対向す
る面を絶縁物3で覆っている。絶縁物3はこの実施例で
はガラス板であるが、セラミックス等でもよい。プラズ
マ領域5のプラズマ、電子ビーム加速領域の電子ビーム
そしてイオン生成領域7のプラズマを径方向に拘束する
ため軸方向に磁界をかけることがある。半導体ウェハ表
面層の再結晶化処理に本発明の電子ビーム源を使用する
ときは、プラズマ領域5と加速領域6とにそれぞれ10
−’)−ルと10−’)−ル程度のアルゴンガス雰囲気
をつくる。イオン生成領域7に1.0−3)−ル程度の
アルゴンガス雰囲気をつくる。コレクタ電極13に半導
体ウェハ(図示せず)をのせ、電子ビームを照射して高
温加熱して、ウエノ\の表面層を溶かして再結晶化を促
す。
As shown in FIG. 1, the surface of the accelerating cathode 2 facing the accelerating cathode 4 is covered with an insulator 3. Although the insulator 3 is a glass plate in this embodiment, it may also be made of ceramics or the like. A magnetic field may be applied in the axial direction to restrain the plasma in the plasma region 5, the electron beam in the electron beam acceleration region, and the plasma in the ion generation region 7 in the radial direction. When using the electron beam source of the present invention for recrystallization treatment of the surface layer of a semiconductor wafer, the plasma region 5 and the acceleration region 6 each have a beam of 10
-')-L and 10-')-L to create an argon gas atmosphere. An argon gas atmosphere of about 1.0-3) is created in the ion generation region 7. A semiconductor wafer (not shown) is placed on the collector electrode 13 and heated to a high temperature by irradiating it with an electron beam to melt the surface layer of the wafer and promote recrystallization.

半導体ウェハのエツチングに本発明の電子ビーム源を使
用するときは、プラズマ領域と加速領域とに再結晶化処
理の場合と同じアルゴン雰囲気をつくる。イオン生成領
域7に1O−3)−ル程度の塩素雰囲気をつくる。この
塩素雰囲気に電子を打ち込んでプラズマを発生させ、そ
のプラズマのイオンをコレクタ13上の半導体ウェハに
照射してエツチングする。スパッタリングによる汚染が
ないので、64メガD RAM程度の太きフヨ集積度を
持つ半導体ウェハのエツチングを実現できる。
When using the electron beam source of the present invention for etching semiconductor wafers, the same argon atmosphere as in the recrystallization process is created in the plasma region and acceleration region. A chlorine atmosphere of approximately 1O-3) is created in the ion generation region 7. Electrons are injected into this chlorine atmosphere to generate plasma, and the ions of the plasma are irradiated onto the semiconductor wafer on the collector 13 for etching. Since there is no contamination due to sputtering, it is possible to etch a semiconductor wafer with a thick wafer density of about 64 mega DRAM.

(効 果) 以上から明らかなように、本発明によってスパッタリン
グによるプラズマ領域の汚染と半導体ウェハの金属汚染
を回避できる。更に、加速陰極のスパッタリングによる
損耗をなくすことができる。
(Effects) As is clear from the above, according to the present invention, contamination of the plasma region and metal contamination of the semiconductor wafer due to sputtering can be avoided. Furthermore, wear and tear of the accelerating cathode due to sputtering can be eliminated.

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

第1図は本発明の実施例の縦断面図である。 第2図は従来の電子ビーム源の縦断面図である。 図中:2は加速陰極、3は絶縁物、4は加速陽極、5は
プラズマ領域、6は電子ビーム加速領域、7はイオン生
成領域そして13は電子ビームコレクタ。 第1図
FIG. 1 is a longitudinal sectional view of an embodiment of the invention. FIG. 2 is a longitudinal sectional view of a conventional electron beam source. In the figure: 2 is an accelerating cathode, 3 is an insulator, 4 is an accelerating anode, 5 is a plasma region, 6 is an electron beam acceleration region, 7 is an ion generation region, and 13 is an electron beam collector. Figure 1

Claims (1)

【特許請求の範囲】[Claims]  プラズマ領域、加速陰極、電子ビーム加速領域、加速
陽極及びイオン生成領域がこの順で設けられている電子
ビーム源において、加速陰極の加速陽極に対向する面を
絶縁物で覆うことを特徴とする電子ビーム源。
An electron beam source in which a plasma region, an accelerating cathode, an electron beam accelerating region, an accelerating anode, and an ion generation region are provided in this order, characterized in that a surface of the accelerating cathode facing the accelerating anode is covered with an insulator. Beam source.
JP2166253A 1990-06-25 1990-06-25 E-beam source Expired - Lifetime JP2538804B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2166253A JP2538804B2 (en) 1990-06-25 1990-06-25 E-beam source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2166253A JP2538804B2 (en) 1990-06-25 1990-06-25 E-beam source

Publications (2)

Publication Number Publication Date
JPH0458445A true JPH0458445A (en) 1992-02-25
JP2538804B2 JP2538804B2 (en) 1996-10-02

Family

ID=15827957

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2166253A Expired - Lifetime JP2538804B2 (en) 1990-06-25 1990-06-25 E-beam source

Country Status (1)

Country Link
JP (1) JP2538804B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005146363A (en) * 2003-11-17 2005-06-09 Toshio Goto Apparatus for supplying metal ions and method therefor

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63138634A (en) * 1986-11-28 1988-06-10 Rikagaku Kenkyusho Electron beam excited ion irradiator
JPH01155251U (en) * 1988-04-15 1989-10-25
JPH03210743A (en) * 1990-01-11 1991-09-13 Tokyo Electron Ltd Ion source

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63138634A (en) * 1986-11-28 1988-06-10 Rikagaku Kenkyusho Electron beam excited ion irradiator
JPH01155251U (en) * 1988-04-15 1989-10-25
JPH03210743A (en) * 1990-01-11 1991-09-13 Tokyo Electron Ltd Ion source

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005146363A (en) * 2003-11-17 2005-06-09 Toshio Goto Apparatus for supplying metal ions and method therefor

Also Published As

Publication number Publication date
JP2538804B2 (en) 1996-10-02

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