JPH0362924A - Laser annealing apparatus - Google Patents

Laser annealing apparatus

Info

Publication number
JPH0362924A
JPH0362924A JP1198970A JP19897089A JPH0362924A JP H0362924 A JPH0362924 A JP H0362924A JP 1198970 A JP1198970 A JP 1198970A JP 19897089 A JP19897089 A JP 19897089A JP H0362924 A JPH0362924 A JP H0362924A
Authority
JP
Japan
Prior art keywords
laser
laser annealing
reflection film
laser beam
annealing apparatus
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
JP1198970A
Other languages
Japanese (ja)
Other versions
JPH0734432B2 (en
Inventor
Genichi Yamazaki
山崎 弦一
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP1198970A priority Critical patent/JPH0734432B2/en
Publication of JPH0362924A publication Critical patent/JPH0362924A/en
Publication of JPH0734432B2 publication Critical patent/JPH0734432B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Recrystallisation Techniques (AREA)
  • Lasers (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は 半導体装置特に高集塊 高速の高性能な完全
絶縁分離された半導体集積回路 即ちS○■デバイス用
基体製造の為のレーザアニール装置に関するものであも 従来の技術 社風 半導体集積回路はますます高密度化 高速化され
る傾向にあり、絶縁分離の半導体集積回路に対する要望
が高まっている。従来 絶縁分離の半導体集積回路の形
成に(よ 例えば 絶縁物基板たとえば表面に絶縁膜が
形成されたシリコン(Si)ウェハ上に堆積したポリS
iにレーザビームを照射することによりポリSiの単結
晶化を行(\ このSiウェーハに回路素子を形成する
という方法で行なわれている。以下に従来のレーザアニ
ール装置について第3図とともに説明する。第3図は最
も一般的なレーザアニール装置のブロック図である。
[Detailed Description of the Invention] Industrial Application Field The present invention relates to a laser annealing apparatus for manufacturing substrates for semiconductor devices, particularly highly agglomerated, high-speed, high-performance, fully insulated semiconductor integrated circuits, that is, S○■ devices. However, traditional technology company culture Semiconductor integrated circuits are becoming increasingly denser and faster, and the demand for semiconductor integrated circuits with insulation isolation is increasing. Conventionally, in the formation of semiconductor integrated circuits with insulation isolation (for example, polysilicon deposited on an insulator substrate, such as a silicon (Si) wafer with an insulating film formed on the surface),
Poly-Si is single-crystalized by irradiating a laser beam onto the Si wafer (This is done by forming circuit elements on this Si wafer.The conventional laser annealing apparatus will be explained below with reference to Fig. 3). 3 is a block diagram of the most common laser annealing device.

レーザ光源1から出たレーザビームL(よ 全反射ミラ
ー3によって収光レンズ4に垂直に入射するように光路
変換され 収光レンズ4によってシリコンウェハ5上で
のレーザビーム径を調整された眞 シリコンウェハ5に
照射さh  x−yステージ6を走査することによって
シリコンウェハ5全面をレーザ照射していt4 発明が解決しようとする課題 第3図に示したレーザアニール装置において、全反射ミ
ラー3や収光レンズ4には レーザビームLの反射によ
るエネルギー損失を防ぐ為に 反射防止膜が塗布されて
いる為に レーザビームLのシリコンウェハ5からの反
射光 いわゆるもどり光がレーザビームLの光路と全く
同じ光路を何ら減衰することなく逆進し レーザ光源1
の光共振器内に入り、レーザ光源lの出力が不安定にな
り、単結晶化状態が不安定になるという問題があった 
本発明はかかる点に鑑ム レーザ出力がもどり光の影響
を受けないレーザアニール装置を提供することを目的と
すも 課題を解決するための手段 本発明(よ 上述の課題を解決するた△ 半導体基板の
レーザアニールを行うに際し レーザ光源から前記半導
体基板へ到る光路中に 一方の主面には反射防止膜が塗
布されている力交 反対側の主面には前記反射防止膜が
塗布されていないガラス基板を前記反射防止膜塗布面が
レーザ光入射側になるように設置したレーザアニール装
置である。
The laser beam L emitted from the laser light source 1 (the optical path of the laser beam L is changed by the total reflection mirror 3 so that it enters the converging lens 4 perpendicularly, and the diameter of the laser beam on the silicon wafer 5 is adjusted by the converging lens 4.) By scanning the x-y stage 6, the entire surface of the silicon wafer 5 is irradiated with laser beam. Since the optical lens 4 is coated with an anti-reflection film to prevent energy loss due to reflection of the laser beam L, the reflected light from the silicon wafer 5 of the laser beam L, so-called return light, is exactly the same as the optical path of the laser beam L. Reverse the optical path without any attenuation Laser light source 1
There was a problem that the laser beam enters the optical resonator and the output of the laser light source becomes unstable, making the single crystallization state unstable.
In view of these points, the present invention aims to provide a laser annealing apparatus in which the laser output is restored and is not affected by light. When laser annealing a substrate, there is an optical path from the laser light source to the semiconductor substrate in which an anti-reflection film is coated on one main surface, and the anti-reflection film is coated on the opposite main surface. This is a laser annealing apparatus in which a glass substrate without any antireflection film is installed so that the surface coated with the antireflection film is on the laser beam incident side.

作用 本発明は上述の構成により、 レーザ光源から出たレー
ザビームは ガラス基板の反射防止膜コート面側から入
射するた△ はとんど減衰することなく半導体基板に到
達すも 一方半導体基板からのもどり光(九 反射防止
膜無面側から入射することになり、もどり光の一部は反
射防止膜焦面への入射角に応じて反射さも 従って、も
どり光のガラス基板への入射角を調整することにより、
所望の量だけもどり光を反射させることができ、もどり
光がレーザ光源の光共振器へ入ることによってレーザ出
力が不安定になるという問題を解消することが可能とな
ん 実施例 以下に 本発明の実施例を図面に基づき説明すも 第1
図は 本発明に係るレーザアニール装置のブロック図で
あも レーザ光源1と全反射ミラー3の間に(よ 一方
の主面がそれぞれ反射防止膜コート面7A、7Bであり
、反対側の主面が反射防止膜焦面8A、8Bであるガラ
ス基板2A、2Bがいずれも反対防止膜焦面8A、8B
に対してもどり光の入射角がθiとなるように設置され
ている。従って、レーザ光源1から出たレーザ光は ガ
ラス基板2A、2B、  全反射ミラー3、収光レンズ
4を、はとんどエネルギー損失なく通過し半導体基板例
えばシリコンウェハ5上に照射される。一方、もどり光
(よ まずガラス基板2Bの反射防止膜焦面8Bで入射
角θiに対応した反射率R(%)でその一部力交 反射
され さらにガラス基板2Aの反射防止膜焦面8Aでも
入射角θiに対応した反射率R(%)でその一部が反射
され 最終的にはもどり光のR(2−R/100)%が
反射される本実施例で用いたガラス基板の入射角θiに
対する反射率の測定結果を第2図に示す。例えばR=2
0%となるようにガラス基板2A、2Bを設置し レー
ザ光源1の出力3Wでシリコンウェハ5にレーザビーム
Lを照射した場合、もどり光の36%がガラス基板2A
、2Bで反射され レーザ光源1の出力に不安定性は認
められ衣 レーザ照射中のレーザ出力を安定化すること
が可能となっf。
Effect of the present invention With the above-described configuration, the laser beam emitted from the laser light source is incident on the anti-reflection film coated side of the glass substrate, so that it reaches the semiconductor substrate without being attenuated. Return light (9) The return light enters from the non-surface side of the anti-reflection film, and a portion of the return light is reflected depending on the angle of incidence on the focal plane of the anti-reflection film. Therefore, the angle of incidence of the return light on the glass substrate is adjusted. By doing so,
The following embodiments show that it is possible to reflect the returning light by a desired amount and to solve the problem that the laser output becomes unstable due to the returning light entering the optical resonator of the laser light source. The embodiment will be explained based on the drawings.
The figure is a block diagram of a laser annealing apparatus according to the present invention. are anti-reflection film focal planes 8A and 8B, and glass substrates 2A and 2B are opposite anti-reflection film focal planes 8A and 8B.
It is installed so that the incident angle of the returning light is θi. Therefore, the laser light emitted from the laser light source 1 passes through the glass substrates 2A, 2B, the total reflection mirror 3, and the condensing lens 4 with almost no energy loss, and is irradiated onto a semiconductor substrate, such as a silicon wafer 5. On the other hand, the returning light (firstly, at the focal plane 8B of the anti-reflection film of the glass substrate 2B, a part of it is reflected by the reflectance R (%) corresponding to the incident angle θi, and then also at the focal plane 8A of the anti-reflection film of the glass substrate 2A). The incident angle of the glass substrate used in this example is that part of it is reflected by the reflectance R (%) corresponding to the incident angle θi, and finally R (2-R/100)% of the returned light is reflected. Figure 2 shows the measurement results of reflectance versus θi.For example, R=2
When the glass substrates 2A and 2B are installed so that the laser beam L is 0% and the silicon wafer 5 is irradiated with the laser beam L with an output of 3W from the laser light source 1, 36% of the returned light is on the glass substrate 2A.
, 2B, it is possible to stabilize the laser output during laser irradiation.

発明の詳細 な説明したように 本発明によれば 半導体基板のレー
ザアニールを行うに際し レーザ照射中ももどり光に起
因するレーザ出力のゆらぎは発生せ哄 常に安定した単
結晶化が可能なレーザアニール装置が実現され 単結晶
化の量産工程にとってその実用的効果は極めて大なるも
のである。
As described in detail, according to the present invention, when laser annealing a semiconductor substrate, fluctuations in laser output due to returning light do not occur during laser irradiation, and a laser annealing device that can always produce stable single crystals. has been realized, and its practical effects are extremely significant for the mass production process of single crystallization.

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

第1図は本発明における一実施例のレーザアニール装置
のブロック阻 第2図は゛もどり光の入射角θiと反射
率Rの関係を示すが 第3図は従来のレーザアニール装
置のブロック図である。 1・・・・レーザ光風 2A、2B・・・・ガラス基板
3・・・・全反射ミラコ 4・・・・収光レンX 5・
・・・シリコンウニI\ 6・・・・X−Yステージ、
 ?A、7B・・・・反射防止膜コートffi  8A
、8B・・・・反射防止膜無胤
Fig. 1 shows the block diagram of a laser annealing apparatus according to an embodiment of the present invention. Fig. 2 shows the relationship between the incident angle θi of the returning light and the reflectance R. Fig. 3 is a block diagram of a conventional laser annealing apparatus. . 1...Laser light wind 2A, 2B...Glass substrate 3...Total reflection Miraco 4...Convergent lens X 5.
...Silicon sea urchin I\6...X-Y stage,
? A, 7B...Anti-reflection film coat ffi 8A
, 8B...No anti-reflection film

Claims (1)

【特許請求の範囲】[Claims] 半導体基板のレーザアニールを行うに際し、レーザ光源
から前記半導体基板へ到る光路中に、一方の主面には反
射防止膜が塗布されているが、反対側の主面には前記反
射防止膜が塗布されていないガラス基板を前記反射防止
膜塗布面がレーザ光入射側になるように設置したレーザ
アニール装置。
When laser annealing a semiconductor substrate, an anti-reflection film is coated on one main surface in the optical path from the laser light source to the semiconductor substrate, and the anti-reflection film is coated on the opposite main surface. A laser annealing device in which an uncoated glass substrate is installed so that the surface coated with the antireflection film is on the laser beam incident side.
JP1198970A 1989-07-31 1989-07-31 Laser annealing equipment Expired - Fee Related JPH0734432B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1198970A JPH0734432B2 (en) 1989-07-31 1989-07-31 Laser annealing equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1198970A JPH0734432B2 (en) 1989-07-31 1989-07-31 Laser annealing equipment

Publications (2)

Publication Number Publication Date
JPH0362924A true JPH0362924A (en) 1991-03-19
JPH0734432B2 JPH0734432B2 (en) 1995-04-12

Family

ID=16399956

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1198970A Expired - Fee Related JPH0734432B2 (en) 1989-07-31 1989-07-31 Laser annealing equipment

Country Status (1)

Country Link
JP (1) JPH0734432B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5930606A (en) * 1996-01-04 1999-07-27 U.S. Philips Corporation Electronic device manufacture with a laser beam

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5930606A (en) * 1996-01-04 1999-07-27 U.S. Philips Corporation Electronic device manufacture with a laser beam

Also Published As

Publication number Publication date
JPH0734432B2 (en) 1995-04-12

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