JPS6355775B2 - - Google Patents
Info
- Publication number
- JPS6355775B2 JPS6355775B2 JP57013003A JP1300382A JPS6355775B2 JP S6355775 B2 JPS6355775 B2 JP S6355775B2 JP 57013003 A JP57013003 A JP 57013003A JP 1300382 A JP1300382 A JP 1300382A JP S6355775 B2 JPS6355775 B2 JP S6355775B2
- Authority
- JP
- Japan
- Prior art keywords
- wafer
- irradiated
- plasma
- electron beam
- insulating film
- 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
Links
Classifications
-
- 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
- H01J37/02—Details
- H01J37/026—Means for avoiding or neutralising unwanted electrical charges on tube components
Landscapes
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Electron Beam Exposure (AREA)
- Recrystallisation Techniques (AREA)
Description
【発明の詳細な説明】
(a) 発明の技術分野
本発明は絶縁体表面を電子ビームや紫外線等の
エネルギー線で照射した場合の帯電防止技術に関
するものである。DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field of the Invention The present invention relates to antistatic technology when the surface of an insulator is irradiated with energy rays such as electron beams and ultraviolet rays.
(b) 技術の背景及び問題点
半導体装置の製造に於て、イオン注入層のアニ
ール、アモルフアス層の熱処理などの目的で電子
ビームを半導体基板表面に照射することが行われ
る。(b) Technical Background and Problems In the manufacture of semiconductor devices, the surface of a semiconductor substrate is irradiated with an electron beam for purposes such as annealing an ion-implanted layer and heat treating an amorphous layer.
これは、通常X−Yステージに載せた半導体基
板をX方向およびY方向に移動させながら、基板
全面に電子ビームを照射して行うため、基板表面
に絶縁物皮膜が存在する領域も同時に電子ビーム
の照射をうける。 This is usually done by irradiating the entire surface of the substrate with an electron beam while moving the semiconductor substrate placed on an be irradiated with.
絶縁物皮膜が電子ビームの照射をうけると、そ
の表面に電荷が蓄積し、それが増加すると、遂に
は絶縁物皮膜が絶縁破壊を起すに至る。電子ビー
ムのような荷電粒子線に限らず、紫外線のような
放射線の照射を受けた場合にも、叩き出された電
子が蓄積し、同様の事態が発生する。特にエキシ
マレーザのような強力な紫外光源を使用する場
合、この問題が顕著になる。 When an insulating film is irradiated with an electron beam, charge accumulates on its surface, and as this increases, the insulating film eventually undergoes dielectric breakdown. A similar situation occurs not only when irradiated with charged particle beams such as electron beams, but also when irradiated with radiation such as ultraviolet rays, as ejected electrons accumulate. This problem becomes particularly noticeable when using a powerful ultraviolet light source such as an excimer laser.
半導体装置の製造工程に於ては、表面の平坦化
或いは汚染防止などの目的で、基板表面には二酸
化珪素などの絶縁皮膜が存在するのが通常である
から、このような半導体基板に放射線を照射する
場合には、絶縁破壊にたいする配慮が必要であ
る。 In the manufacturing process of semiconductor devices, an insulating film such as silicon dioxide is usually present on the surface of the substrate for the purpose of flattening the surface or preventing contamination. When irradiating, consideration must be given to dielectric breakdown.
イオン注入に於ても類似の問題が生ずるが、イ
オン注入の場合は正電荷の蓄積であり、電子シヤ
ワーや紫外線照射による負電荷の発生を併用する
ことにより、蓄積電荷を中和することが可能であ
つたのに対し、負電荷の蓄積に対しては、従来適
切な対策が知られていなかつた。 A similar problem occurs with ion implantation, but in the case of ion implantation, positive charges are accumulated, and it is possible to neutralize the accumulated charges by using electronic shower or ultraviolet irradiation to generate negative charges. On the other hand, no suitable countermeasures against the accumulation of negative charges have been known so far.
(c) 発明の目的
本発明は上記の点に鑑み、絶縁皮膜上の負電荷
帯電を防止しながらエネルギー線の照射を行う方
法を提供するものである。(c) Object of the Invention In view of the above points, the present invention provides a method of irradiating energy rays while preventing negative charge build-up on an insulating film.
(d) 発明の構成
上記目的を達成するため本発明は負電荷の生ず
るエネルギー線照射を、少なくもその一部が絶縁
物から成る被照射体表面をプラズマガスに接触さ
せた状態で行う事を特徴とする。(d) Structure of the Invention In order to achieve the above object, the present invention involves irradiating energy rays that generate negative charges with the surface of an irradiated object, at least a part of which is an insulator, in contact with plasma gas. Features.
(e) 発明の実施例 第1図に本発明の一実施例を示す。(e) Examples of the invention FIG. 1 shows an embodiment of the present invention.
X−Yステージ1に載せられた半導体基板2
(以下ウエフアーと記す)は既述したように、X
方向およびY方向に移動しながら、全面に電子ビ
ームの照射を受ける。3は電子銃であり、4は電
子ビームをウエフアー上にフオーカスさせるため
の電子レンズである。 Semiconductor substrate 2 placed on X-Y stage 1
(hereinafter referred to as wafer) is X
While moving in the direction and the Y direction, the entire surface is irradiated with the electron beam. 3 is an electron gun, and 4 is an electron lens for focusing the electron beam onto the wafer.
以上は従来技術と同様であるが、本発明に使用
される装置では更に電極5が設けられ、該電極と
X−Yステージとの間には高周波電界が印加され
て、ウエフアー上方の空間領域にプラズマが発生
するように構成されている。電極5には電子ビー
ムを通過させる為の開口6が設けられている。プ
ラズマ発生の為に前記空間は10Torr.のArガス雰
囲気となつており、印加される13.56MHzの高周
波電力はウエフアー1枚当り100W程度である。
更に、プラズマ中の正イオンが効率よくウエフア
ー表面に到達するように、ウエフアー側の電極が
負電位になるような直流電圧を、電極間に重ねて
印加してもよい。 The above is the same as the conventional technology, but the apparatus used in the present invention is further provided with an electrode 5, and a high frequency electric field is applied between the electrode and the X-Y stage to apply it to the spatial region above the wafer. It is configured to generate plasma. The electrode 5 is provided with an opening 6 for passing the electron beam. In order to generate plasma, the space has an Ar gas atmosphere of 10 Torr, and the applied high frequency power of 13.56 MHz is about 100 W per wafer.
Furthermore, a DC voltage may be applied between the electrodes such that the electrode on the wafer side has a negative potential so that positive ions in the plasma efficiently reach the wafer surface.
このような条件の下にプラズマを発生させなが
ら電子ビームの照射を行うと、ウエフアー表面に
生じた電荷はプラズマイオンによつて中和される
為、絶縁膜上に蓄積されることが無く、従つて絶
縁破壊の生ずることが無い。 When electron beam irradiation is performed while generating plasma under these conditions, the charges generated on the wafer surface are neutralized by the plasma ions, so they are not accumulated on the insulating film and are Therefore, no dielectric breakdown occurs.
本発明が実施される対象は主としてシリコンウ
エフアーであるが、上記の実施条件では発生した
プラズマガスによつてシリコン或いは二酸化珪素
が強くエツチングされることは無く、素子形成上
の障害とはならない。なお、新たに電極5が設け
られ、電圧が印加されることから、電子銃3に印
加される電圧或いは電子レンズ4のフオーカス条
件には、若干の修正が必要な場合がある。 Although the present invention is mainly applied to silicon wafers, under the above-mentioned conditions, silicon or silicon dioxide will not be strongly etched by the generated plasma gas, and will not pose an obstacle to device formation. Note that since the electrode 5 is newly provided and a voltage is applied, the voltage applied to the electron gun 3 or the focus condition of the electron lens 4 may need to be slightly modified.
本発明は復、第2図に示すように実施すること
も出来る。 The present invention can also be implemented as shown in FIG.
この実施例ではプラズマ発生の為のチエンバー
7が、電子ビーム照射空間から分離されて設けら
れており、発生したプラズマガスはウエフアー2
の表面に到達して、絶縁膜上に生じた電荷を中和
する。プラズマ発生の条件は第1図の実施例と同
様か、或いは若干強いものとする。 In this embodiment, a chamber 7 for plasma generation is provided separately from the electron beam irradiation space, and the generated plasma gas is transferred to the wafer 2.
reaches the surface of the insulating film and neutralizes the charges generated on the insulating film. The conditions for plasma generation are the same as those in the embodiment shown in FIG. 1, or slightly stronger.
このように構成した装置を使用すれば、電子ビ
ーム照射空間に余分の電極(第1図の5に相当)
が無いので、照射条件の設定は従来と同じになる
ばかりでなく、ウエフアーに対するエツチングそ
の他の悪影響を小とすることができる。 If you use a device configured in this way, an extra electrode (corresponding to 5 in Figure 1) can be placed in the electron beam irradiation space.
Since there is no irradiation condition, the setting of irradiation conditions is not only the same as in the conventional method, but also etching and other adverse effects on the wafer can be reduced.
(f) 発明の効果
以上説明したような本発明の方法によれば、絶
縁皮膜上に生じる負電荷は遂次中和されるので、
電荷の蓄積が起らず、絶縁破壊を防止することが
出来る。(f) Effects of the invention According to the method of the invention as explained above, the negative charges generated on the insulating film are successively neutralized.
No charge accumulation occurs, and dielectric breakdown can be prevented.
第1図及び第2図は本発明の実施例を示す図で
あつて、図に於て1はX−Yステージ、2はウエ
フアー、3は電子銃、4は電子レンズ、5はプラ
ズマ発生用電極、7はプラズマ発生の為のチエン
バーである。
1 and 2 are diagrams showing an embodiment of the present invention, in which 1 is an X-Y stage, 2 is a wafer, 3 is an electron gun, 4 is an electron lens, and 5 is for plasma generation. The electrode 7 is a chamber for plasma generation.
Claims (1)
射に於て、少なくもその一部が絶縁物から成る被
照射体表面をプラズマガスに接触させた状態で行
う事を特徴とするエネルギー線照射方法。 2 前記プラズマガスを発生させるための空間
を、前記被照射体表面をプラズマガスに接触させ
る空間とは別に設けることを特徴とする特許請求
の範囲第1項記載のエネルギー線照射方法。[Claims] 1. A radiation irradiation that generates a negative charge on the surface of an insulator is characterized in that the surface of the irradiated object, at least a part of which is made of an insulator, is in contact with plasma gas. Energy ray irradiation method. 2. The energy ray irradiation method according to claim 1, wherein a space for generating the plasma gas is provided separately from a space for bringing the surface of the irradiated object into contact with the plasma gas.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57013003A JPS58131731A (en) | 1982-01-29 | 1982-01-29 | Irradiation of energy rays |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57013003A JPS58131731A (en) | 1982-01-29 | 1982-01-29 | Irradiation of energy rays |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS58131731A JPS58131731A (en) | 1983-08-05 |
| JPS6355775B2 true JPS6355775B2 (en) | 1988-11-04 |
Family
ID=11820998
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57013003A Granted JPS58131731A (en) | 1982-01-29 | 1982-01-29 | Irradiation of energy rays |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58131731A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2602051B1 (en) * | 1986-07-23 | 1988-09-16 | Cameca | METHOD AND DEVICE FOR DISCHARGE OF INSULATING SAMPLES DURING ION ANALYSIS |
| JPH0745227A (en) * | 1993-06-11 | 1995-02-14 | Mitsubishi Electric Corp | Charged particle applied analysis device and charged particle applied drawing device |
-
1982
- 1982-01-29 JP JP57013003A patent/JPS58131731A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS58131731A (en) | 1983-08-05 |
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