JPH0463019B2 - - Google Patents
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- Publication number
- JPH0463019B2 JPH0463019B2 JP62323882A JP32388287A JPH0463019B2 JP H0463019 B2 JPH0463019 B2 JP H0463019B2 JP 62323882 A JP62323882 A JP 62323882A JP 32388287 A JP32388287 A JP 32388287A JP H0463019 B2 JPH0463019 B2 JP H0463019B2
- Authority
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- Prior art keywords
- laser
- optical system
- refractive index
- quartz glass
- purity
- Prior art date
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
- H01S3/03—Constructional details of gas laser discharge tubes
- H01S3/0305—Selection of materials for the tube or the coatings thereon
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- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Glass Compositions (AREA)
- Lasers (AREA)
Description
「産業上の利用分野」
本発明は、レーザステツパ装置、レーザ発振装
置、レーザ核融合装置等に用いるレンズ、窓部
材、ミラー、プリズム、フイルター等の製造に好
適なレーザ光学系素体に係り、特に高出力の且つ
短波長域のレーザ光に対し耐久性と高品質性を保
証し得るレーザ光学系素体に関する。
「従来の技術」
近年におけるLSIの微細化、高集積化の進展は
極めて著しく既にチツプ当たりの素子数が100000
以上のVLSIの時代に突入しつつあり、これに伴
ないウエハ上に集積回路パターンを描画するリソ
グラフイ技術においてもその開発が急速に進み、
例えば1MビツトDRAMに対応するパターン線巾
1μm、更には4MビツトDRAMに対応するパター
ン線巾0.8μmと、より微細な線幅が描画可能な技
術が開発されつつあり、これらの微細な線幅描画
技術はいずれも光リソグラフイー技術により行わ
れている。
更にリソグラフイ技術分野においては、近い将
来において実現し得る16MビツトDRAMに対応
するパターン線巾0.5μmというサブミクロン単位
の描画技術の開発も急がねばならないが、このよ
うな超微細な線幅描画技術においても最近の光学
系、光源、フオトレジスト等の着実な進歩からみ
てやはり光リソグラフイーが主流になるものと推
定される。
確かに光リソグラフイーは、比較的高輝度の光
源、高感度レジスト、安定した光学材料がそろつ
ている等超微細な線幅描画を行う上で必要な種々
の条件を備えているが、欠点として露光波長が大
きいため、回折により解像力が制限されるという
問題がある。
その解決策は、光学系の高NA(開口数)化と
光の短波長化である。
光学系の高NA化は、NA(開口数)0.4を超え
る時代に入つており、試作品としてNA0.6のレン
ズも開発されているが、高NA化に伴い焦点深度
が浅くなる為にその解像度の向上を図る為の高
NA化は限界に来ている。
例えば、NA0.43、波長g線(436nm)にて、
露光した場合、焦点深度=±0.5λ/(NA)2の経
験則を適用すると約±1.2μmとなり、レジストの
厚さ、段差、焦点合せ精度の現状を考えると許容
限界に近い。
そこで、次に光の短波長化が検討されることに
なる。
しかしながら光の短波長化を図る為に、400nm
以下の紫外線を用いた場合は、従来の光学ガラス
を用いたレンズでは使用波長が365nm(i線)付
近より光透過率が急激に低下して、言い変えれば
光吸収と該光吸収による発熱が生じ、該レンズの
焦点位置やその他の特性を狂わせることになる。
かかる欠点を解消する為に、レンズ材料を従来
の光学ガラスから石英ガラス又は蛍石に代える事
が提案されているが、これらの材料に通常の紫外
線を透過した場合光スペクトル巾が広いために色
収差が発生してしまう。
そこで前記光リソグラフイー用の光源としてス
ペクトル巾の狭いレーザ光を使うことが考えら
れ、特に光リソグラフイー用のレーザの中で最も
完成度の高いものがエキシマレーザである。
エキシマレーザは短波長域、主として紫外域で
発振する高出力パルスレーザであり、エキシマレ
ーザの種類としては、Xe2(172nm)、Kr2
(146nm)、Ar2(126nm)、等の希ガスエキシマ、
XeO(538,546nm)、KrO(558nm)、等の希ガス
酸素エキシマ、HgI(443nm)等の水銀ハライド
エキシマ、KrF(248nm)、XeCl(308nm)、ArF
(193nm)、等の希ガスハライドエキシマなど、合
計、数10種類におよぶが、発振効率とガス寿命の
点から、KrF(248nm)、XeCl(308nm)、ArF
(193nm)等が有利である。
そしてかかるレーザ光はいずれも波長が350nm
以下と、従来の水銀灯の紫外線使用波長であるg
線(436nm)或いはi線(365nm)の場合に比較
して極めて短波長であるが故にこれらの光学材料
の屈折率の均一性は前記g線或いはi線の場合に
比較して1桁以上高い(△n≒1×10-7〜1×
10-6、△n:屈折率変動幅)ものが要求される事
となるが、前記短波長レーザ光を光源とする場合
のレンズ材料の内、蛍石については屈折率の均一
性と最大寸法、加工時の吸湿性と機械的強度に問
題が多く残されており、この為短波長域のレーザ
光に対し耐久性と高品質性を保証し得るレーザ光
学系素体としては石英ガラス以外には見出せな
い。
「発明が解決しようとする問題点」
しかしながら、例え石英ガラスを用いてレーザ
光学系を製作したとしても、該光学系に高出力パ
ルス光である短波長のエキシマレーザ光が長時間
照射されると時間経過とともに、石英ガラス(レ
ンズ等)がダメージを受け、歪が入り複屈折が起
こるのみならず、前記短波長レーザ光の長時間照
射により、透過率の低下、絶対屈折率の上昇、屈
折率分布の変動が起こり、最終的にクラツクが発
生するという問題が派生する。
特に短波長化エキシマレーザ用の石英ガラスレ
ンズに対しては、前述したように、屈折率分布の
△nが1×10-6以下という要求があり、前記のよ
うな石英ガラスの光学的物性変化が起こると、レ
ンズの光軸、焦点位置が変動し、微細かつ鮮明パ
ターンの形成が極めて困難となる。
又、300nm以下の短波長レーザ光が照射される
と、例え従来の光学ガラスより光学的安定性の高
い石英ガラスにおいても蛍光を発生し、特にエキ
シマレーザステツパのように投影型露光装置にお
いては、レンズその他の光学系から発生した蛍光
がレーザ光とともにウエハ上のフオトレジストに
感応してしまい、鮮明パターンの形成が困難とな
る。
本発明はかかる従来技術の欠点に鑑み、前述し
た石英ガラスに新たな別異の要素を加味する事に
より、長時間にわたる屈折率、透過率等の安定性
を確保するとともに、蛍光の低減をはかり、特に
エキシマレーザ用の光学系材料として極めて好適
なレーザ光学系素体を提供する事を目的とする。
「問題点を解決する為の手段」
さて、石英ガラスを用いてレーザ光学系を形成
した場合においても、短波長域のエキシマレーザ
光を石英ガラスに照射すると照射線量を増大させ
るに従つて石英ガラスの屈折率は徐々に高くな
り、透過率は徐々に低下していく事は前述した通
りである。
又石英ガラスにおいてもレーザ光を短波長化す
るに連れ蛍光が発生し、特に略300nm以下の波長
域においては蛍光発生度合が強くなることも先に
説明した通りである。
一方前記蛍光特性、屈折率、透過率等、光学特
性変化の程度は、レーザ光学系に照射されるエキ
シマレーザ光のパルス当りエネルギー密度(J/
cm2・pules)、発振周波数(Hz)、総照射パルス数
(pules)に依存する事も公知である。
そこで本発明者らは不純物濃度レベルの異なる
二種類の合成石英ガラス、すなわち普通純度合成
石英ガラスと高純度合成石英ガラスを用いて、該
ガラス組織中に含まれるOH基含有量を種々変化
させて形成した試験片を複数個用意し、該試験片
に、パルス当りエネルギー密度(J/cm2・pules)
と、総照射パルス数(pules)を変化させた同一
波長域(248nm)の短波長エキシマレーザ光を照
射させ、その蛍光特性、透過率、屈折率変化、及
びクラツク発生の有無について調査してみた。
この結果、蛍光特性、屈折率、透過率等の光学
特性の劣化等を引き起こす主原因の一つとして不
純物元素である事が確認出来たが、これのみなら
ず、不純物元素濃度低減に加えて、特に不純物濃
度を一定にした場合、透過率と屈折率等の変化は
OH基含有量にも依存し、具体的にはOH基含有
量を増大させる事により、前記蛍光特性、屈折
率、透過率等の光学特性が向上する事が知見出来
た。
このように、不純物濃度の低減と相まつてOH
基含有量の増大が、短波長域レーザ光に使用され
るレーザ光学系の蛍光を低減させ、透過率、屈折
率等の安定性が向上し得る事は本発明者達が始め
て知見した事実であり、従つて石英ガラスの高純
度化とともに、前記OH基含有量を規定する事に
より、前記した本発明の目的を達成し得る。
尚、OH基含有量が何故前述した光学特性に影
響するのかはさだかではないが、以下のように考
えられる。
石英ガラスに強力なレーザ光を照射すると、ガ
ラス網目構造を構成する元素間の結合が切断さ
れ、その結果透過率が低下し、吸収バンドが現わ
れる。又、蛍光強度も増加する。
しかし、これらの元素間の切断も、石英ガラス
中に含まれるOH基そのものや、OH基の水素元
素の存在や移動により大部分が修復されるものと
推定している。
クラツクの発生は、OH基が多量に含まれると
上記理由により吸収バンドの発生が小さくなり、
その結果として光吸収が少なくなり、クラツクが
少なくなると考えている。
本発明は上述した知見と実験結果に基づいてな
されたものであり、その特徴とする所は、略
400nm以下、より限定的には350nm以下の特定波
長域のレーザ光に使用されるレーザ光学系素体を
高純度の石英ガラス材で形成するとともに、該ガ
ラス材組織中のOH基含有量を少なくとも
300ppm以上に設定した点にある。
これにより、短波長域レーザ光に使用されるレ
ーザ光学系の蛍光発生を低減させ、屈折率、透過
率等の安定性を向上させることが出来る。
尚、短波長域で且つより高出力のレーザ光を用
いる場合には前記設定値を更に引き上げ、前記素
体を高純度の合成石英ガラス材で形成するととも
に、該ガラス材組織中のOH基含有量を700ppm
以上に設定する事により、350nm以下の高出力レ
ーザ光学系素体として特に好適なものを提供し得
る。
この場合前記高純度石英ガラス材とは、少なく
とも金属元素の含有量が原子吸光分析法に基づい
て測定した場合に検出限度以下、具体的には原子
の種類にもよるが略0.1〜0.01ppm以下であるも
の、例えばLi、Na、Kのアルカリ金属元素及び
Mg、Caのアルカリ土類金属元素が、夫々
0.1ppm以下であり、且つTi、Cr、Fe、Cuの遷移
金属元素及びAl元素が、夫々0.01ppm以下である
高純度石英ガラス材をいう。
尚、前記合成石英の高純度化とOH基含有量の
制御は下記のように処理する事により容易に調整
する事が出来る。
即ち合成石英ガラスは、例えば四塩化ケイ素
(SiCl4)ガスを酸水素炎中で加水分解して合成さ
れ、そして特に高純度化については例えば、不純
物濃度が所定値以下の純度のよい四塩化ケイ素原
料を蒸留処理することにより前記原料中に残留し
ている不純物を更に除去させ、これをテフロンラ
イニング材のステンレス製容器に貯溜し、更にテ
フロンライニング材パイプを通して合成バーナー
に導入し、これを酸水素炎中で加水分解して合成
することにより、金属不純物元素が略0.1ppm以
下の高純度石英ガラス材を製造することが出来
る。
そしてOH基含有量は、前記石英ガラス合成時
における、四塩化ケイ素ガスと酸素水素ガスとの
混合比を変化させることにより、OH基含有量を
増減させることが出来る。尚、合成に使用するバ
ーナーの形状によつてもOH基含有量を制御する
ことが可能である。
「実施例」
先ず本発明の効果を確認する為に、下記のよう
な製造法でエキシマレーザ照射実験用試験片夫々
複数個用意する。
先ず、不純物濃度の低い原料四塩化ケイ素を蒸
留処理した後、これをテフロンライニング付のス
テンレス製容器に貯溜した高純度の四塩化ケイ素
と、前記蒸留処理を行わない普通純度の四塩化ケ
イ素とを用意し、これらを夫々テフロンライニン
グ付パイプを通して合成バーナーに導入し、これ
を酸水素炎中で反応させる際に、該四塩化ケイ素
ガスと酸素水素ガスとの混合比を変化させて、
OH基の含有量の異なる石英ガラスインゴツトを
複数種類製造する。
そしてかかる石英ガラスインゴツトの不純物濃
度を測定してみるに、普通純度の四塩化ケイ素を
用いたインゴツトにおいては、Mgが430ppb、Fe
が100ppb、Alが90ppb、Cuが10ppbで、他の金属
元素は検出限界以下すなわちLi、Na、K、Caは
100ppb以下、Ti、Crは10ppb以下であつた。次
にかかるインゴツトのOH基の含有量を調べてみ
ると概算300、500、700、900、1100ppm有してい
た。
一方高純度の四塩化ケイ素を用いたインゴツト
においては、Clの含有量は25ppmである点を除い
て他の不純物元素はいずれも検出限界以下であつ
た。次にかかるインゴツトのOH基の含有量を調
べてみると前記と同様に概算300、500、700、
900、1100ppm有していた。
更に、上記普通純度の四塩化ケイ素と高純度の
四塩化ケイ素を各々プラズマ発生装置に導入し、
プラズマ雰囲気で石英ガラスに変化させ、インゴ
ツトを合成した。
このプラズマ法で合成した石英ガラスインゴツ
トのOH基含有量は、5ppm以下であつた。
このようにして形成した各種合成石英ガラスイ
ンゴツトを30×20×10mmの寸法に切断し且つ両面
鏡面仕げを行つてエキシマレーザ照射実験用試験
片を夫々9個作成する。
次にこれらの各9個の試験片に対して、248nm
(KrF)の波長域を有するレーザ光についてパル
ス当りエネルギー密度200,400,600(mJ/cm2・
pules)、及び照射パルス数1×104、1×105、1
×106(pules)の組合わせから成る照射条件にて
照射を行つた。
そして前記照射終了後の各試験片について干渉
計にて屈折率分布変化、透過率計にてソーラリゼ
ーシヨン、蛍光測定器にて蛍光強度測定、及び目
視にてクラツクの有無の判定を行つた。
その結果を下記の実験結果条件一覧表に示す。
この結果、蛍光特性、透過率、屈折率変化等に
よつては普通純度の試験片と高純度の試験片とで
は、明らかに有為差がみられ、その主要原因が石
英ガラスに含まれる不純物元素である事が確認出
来たが、これのみならず、前記不純物元素の高純
度化に加えてOH基含有量にも依存する事が知見
出来た。(実験例1)〜6)、7)〜12)参照)
更に不純物濃度が普通純度の試験片では、OH
基含有量を多くする程透過率、屈折率等の安定性
が向上する事は理解出来るが、OH基含有量が
1100ppmの場合でも尚蛍光特性が強く実用上問題
がある。(実験例1)〜6)参照)
次に高純度の試験片同士を比較すると、OH基
含有量が5ppmでは蛍光強度、透過率低下、屈折
率変化、クラツクの発生がいずれも問題がある
が、OH基含有量が300ppmであれば、透過率と
屈折率が実用化に耐える程度に安定し、且つ蛍光
強度とクラツクの発生を低減させる事が出来る。
(実験例8)参照)
更に前記実験例10)より理解される如く、OH
基含有量が少なくとも700ppm以上に設定する事
により、レーザ光学系の蛍光特性、透過率、屈折
率等を更に改善するとともに、クラツクの発生を
解消させる事が出来、これにより短波長域で且つ
高出力のレーザ光の光学系として好適な素体の提
供が可能となる。
"Industrial Application Field" The present invention relates to a laser optical system element body suitable for manufacturing lenses, window members, mirrors, prisms, filters, etc. used in laser stepper devices, laser oscillation devices, laser fusion devices, etc. The present invention relates to a laser optical system element that can guarantee durability and high quality for high-output laser light in a short wavelength range. "Conventional technology" The progress in miniaturization and high integration of LSIs in recent years has been extremely remarkable, with the number of elements per chip already reaching 100,000.
We are entering the era of VLSI as described above, and along with this, the development of lithography technology for drawing integrated circuit patterns on wafers is progressing rapidly.
For example, pattern line width corresponding to 1M bit DRAM
Technologies that can draw finer line widths of 1 μm and even finer line widths of 0.8 μm, which corresponds to 4M-bit DRAM, are being developed, and all of these fine line width writing techniques can be performed using optical lithography technology. It is being said. Furthermore, in the field of lithography technology, there is an urgent need to develop submicron pattern writing technology with a pattern line width of 0.5 μm, which is compatible with 16M-bit DRAM, which will be realized in the near future. In terms of technology, it is estimated that optical lithography will become the mainstream, considering recent steady progress in optical systems, light sources, photoresists, etc. It is true that optical lithography has various conditions necessary for drawing ultra-fine line widths, such as a relatively high-intensity light source, high-sensitivity resist, and stable optical materials, but there are drawbacks. Since the exposure wavelength is large, there is a problem in that the resolution is limited by diffraction. The solution is to increase the NA (numerical aperture) of the optical system and shorten the wavelength of light. We have entered the era of high NA (numerical aperture) in optical systems, exceeding NA (numerical aperture) of 0.4, and a prototype lens with NA of 0.6 has been developed, but the depth of focus becomes shallower as the NA increases. High resolution to improve resolution
NA has reached its limit. For example, at NA0.43 and wavelength g-line (436nm),
When exposed, applying the empirical rule of depth of focus = ±0.5λ/(NA) 2 , the depth of focus is approximately ±1.2 μm, which is close to the allowable limit considering the current state of resist thickness, steps, and focusing accuracy. Therefore, the next step is to consider shortening the wavelength of light. However, in order to shorten the wavelength of light, 400nm
When the following ultraviolet rays are used, the light transmittance of lenses using conventional optical glass decreases rapidly when the wavelength used is around 365 nm (i-line), in other words, light absorption and heat generation due to the light absorption occur. This causes the focal position and other characteristics of the lens to be disturbed. In order to eliminate this drawback, it has been proposed to replace the conventional optical glass with silica glass or fluorite as the lens material, but when normal ultraviolet light is transmitted through these materials, chromatic aberration occurs due to the wide light spectrum width. will occur. Therefore, it has been considered to use a laser beam with a narrow spectral width as a light source for the optical lithography, and in particular, the excimer laser is the most sophisticated laser for optical lithography. Excimer laser is a high-power pulsed laser that oscillates in a short wavelength region, mainly in the ultraviolet region. Types of excimer laser include Xe 2 (172 nm), Kr 2
(146nm), Ar2 (126nm), etc., noble gas excimers,
Noble gas oxygen excimers such as XeO (538, 546nm), KrO (558nm), mercury halide excimers such as HgI (443nm), KrF (248nm), XeCl (308nm), ArF
(193nm), etc., but in terms of oscillation efficiency and gas life, KrF (248nm), XeCl (308nm), ArF
(193nm) etc. are advantageous. The wavelength of all such laser beams is 350nm.
The following is the wavelength of ultraviolet light used in conventional mercury lamps: g
Because the wavelength is extremely short compared to the case of the g-line (436 nm) or the i-line (365 nm), the uniformity of the refractive index of these optical materials is more than one order of magnitude higher than that of the g-line or i-line. (△n≒1×10 -7 ~1×
10 -6 , △n: refractive index variation width), but among the lens materials when the short wavelength laser beam is used as a light source, for fluorite, the uniformity of the refractive index and the maximum dimension are required. However, there are still many problems with hygroscopicity and mechanical strength during processing, and for this reason, quartz glass is the only material that can be used as a laser optical system element that can guarantee durability and high quality for laser light in the short wavelength range. I can't find it. "Problems to be Solved by the Invention" However, even if a laser optical system is manufactured using quartz glass, if the optical system is irradiated with short wavelength excimer laser light, which is high-power pulsed light, for a long time. Over time, silica glass (lenses, etc.) is damaged and distorted, causing birefringence. In addition, long-term irradiation with the short wavelength laser light causes a decrease in transmittance, an increase in the absolute refractive index, and a decrease in the refractive index. A problem arises in that the distribution changes and eventually cracks occur. In particular, for silica glass lenses for short wavelength excimer lasers, as mentioned above, there is a requirement that Δn of the refractive index distribution be 1×10 -6 or less, and the above-mentioned changes in the optical properties of silica glass are required. When this occurs, the optical axis and focal position of the lens fluctuate, making it extremely difficult to form fine and clear patterns. Furthermore, when irradiated with short wavelength laser light of 300 nm or less, even silica glass, which has higher optical stability than conventional optical glass, will generate fluorescence, especially in projection exposure equipment such as excimer laser steppers. Fluorescence generated from lenses and other optical systems is sensitive to the photoresist on the wafer together with the laser light, making it difficult to form a clear pattern. In view of the shortcomings of the prior art, the present invention adds new and different elements to the quartz glass described above, thereby ensuring long-term stability in refractive index, transmittance, etc., and reducing fluorescence. The object of the present invention is to provide a laser optical system element body which is particularly suitable as an optical system material for excimer lasers. "Means for solving the problem" Now, even when a laser optical system is formed using quartz glass, when the quartz glass is irradiated with excimer laser light in the short wavelength range, as the irradiation dose increases, the quartz glass As mentioned above, the refractive index of the material gradually increases and the transmittance gradually decreases. Furthermore, as explained above, fluorescence is generated in silica glass as the wavelength of the laser beam is shortened, and the degree of fluorescence generation becomes particularly strong in the wavelength range of about 300 nm or less. On the other hand, the degree of change in optical properties such as fluorescence properties, refractive index, and transmittance is determined by the energy density per pulse (J/
It is also known that it depends on the oscillation frequency (Hz), oscillation frequency (Hz), and total number of irradiation pulses (pules). Therefore, the present inventors used two types of synthetic quartz glass with different impurity concentration levels, namely, ordinary purity synthetic quartz glass and high purity synthetic quartz glass, and variously changed the OH group content contained in the glass structure. Prepare a plurality of formed test pieces, and apply energy density per pulse (J/cm 2 ·pules) to the test pieces.
Then, we irradiated it with short-wavelength excimer laser light in the same wavelength range (248 nm) by varying the total number of irradiation pulses (pules), and investigated its fluorescence characteristics, transmittance, refractive index changes, and the presence or absence of cracks. . As a result, it was confirmed that impurity elements are one of the main causes of deterioration of optical properties such as fluorescence characteristics, refractive index, and transmittance. Especially when the impurity concentration is kept constant, changes in transmittance, refractive index, etc.
It was found that it depends on the OH group content, and specifically, by increasing the OH group content, the optical properties such as the fluorescence properties, refractive index, and transmittance can be improved. In this way, the reduction in impurity concentration and the reduction in OH
The present inventors discovered for the first time that an increase in the group content can reduce the fluorescence of laser optical systems used for short wavelength laser beams and improve the stability of transmittance, refractive index, etc. Therefore, by increasing the purity of quartz glass and regulating the OH group content, the above-mentioned object of the present invention can be achieved. Although it is not entirely clear why the OH group content affects the above-mentioned optical properties, it is thought to be as follows. When quartz glass is irradiated with a strong laser beam, the bonds between the elements that make up the glass network structure are broken, resulting in a decrease in transmittance and the appearance of absorption bands. Furthermore, the fluorescence intensity also increases. However, it is estimated that most of the breaks between these elements are repaired by the presence and movement of the OH groups themselves contained in the quartz glass or the hydrogen elements of the OH groups. The generation of cracks occurs because when a large amount of OH groups are included, the generation of absorption bands becomes smaller due to the above reasons.
We believe that this will result in less light absorption and fewer cracks. The present invention was made based on the above-mentioned knowledge and experimental results, and its characteristics are as follows:
The laser optical system element used for laser light in a specific wavelength range of 400 nm or less, more specifically 350 nm or less, is made of a high-purity quartz glass material, and the OH group content in the structure of the glass material is reduced to at least
The point is that it is set at 300ppm or more. This makes it possible to reduce fluorescence generation in a laser optical system used for short-wavelength laser beams and improve stability of refractive index, transmittance, and the like. In addition, when using a laser beam with a shorter wavelength range and higher power, the setting value is further increased, and the element body is formed of a high-purity synthetic quartz glass material, and the OH group content in the structure of the glass material is increased. amount 700ppm
With the above settings, it is possible to provide a particularly suitable element for a high-output laser optical system of 350 nm or less. In this case, the high-purity quartz glass material means that the content of at least metal elements is below the detection limit when measured based on atomic absorption spectrometry, specifically about 0.1 to 0.01 ppm or less, depending on the type of atoms. , such as alkali metal elements such as Li, Na, K, and
The alkaline earth metal elements Mg and Ca are
It refers to a high-purity silica glass material in which the transition metal elements of Ti, Cr, Fe, and Cu and the Al element are each 0.01 ppm or less. In addition, the high purity of the synthetic quartz and the control of the OH group content can be easily adjusted by the following treatment. That is, synthetic quartz glass is synthesized, for example, by hydrolyzing silicon tetrachloride (SiCl 4 ) gas in an oxyhydrogen flame, and especially for high purity, for example, silicon tetrachloride of high purity with an impurity concentration below a predetermined value is used. Impurities remaining in the raw material are further removed by distilling the raw material, stored in a stainless steel container lined with Teflon, and introduced into a synthesis burner through a Teflon-lined pipe, where it is converted into oxyhydrogen. By hydrolyzing and synthesizing in a flame, it is possible to produce a high-purity quartz glass material containing approximately 0.1 ppm or less of metal impurity elements. The OH group content can be increased or decreased by changing the mixing ratio of silicon tetrachloride gas and oxygen hydrogen gas during the silica glass synthesis. Note that the OH group content can also be controlled by the shape of the burner used for synthesis. "Example" First, in order to confirm the effects of the present invention, a plurality of test pieces for excimer laser irradiation experiments were prepared by the following manufacturing method. First, silicon tetrachloride, a raw material with a low concentration of impurities, is distilled, and then high-purity silicon tetrachloride, which is stored in a stainless steel container with a Teflon lining, and silicon tetrachloride of normal purity, which is not subjected to the distillation process, are separated. Each of these is introduced into a synthesis burner through a Teflon-lined pipe, and when reacting in an oxyhydrogen flame, the mixing ratio of the silicon tetrachloride gas and oxygen hydrogen gas is changed,
Multiple types of quartz glass ingots with different OH group contents are manufactured. When we measured the impurity concentration of such silica glass ingots, we found that in ingots using silicon tetrachloride of normal purity, Mg was 430 ppb and Fe was 430 ppb.
is 100ppb, Al is 90ppb, Cu is 10ppb, and other metal elements are below the detection limit, namely Li, Na, K, and Ca.
Ti and Cr were below 100ppb. Next, the content of OH groups in such ingots was investigated and was estimated to be 300, 500, 700, 900, and 1100 ppm. On the other hand, in the ingot using high-purity silicon tetrachloride, except for the Cl content of 25 ppm, all other impurity elements were below the detection limit. Next, when we investigated the OH group content of such ingots, we found that they were approximately 300, 500, 700,
It had 900 and 1100ppm. Furthermore, the above-mentioned normal purity silicon tetrachloride and high purity silicon tetrachloride are respectively introduced into the plasma generator,
It was transformed into quartz glass in a plasma atmosphere and an ingot was synthesized. The OH group content of the quartz glass ingot synthesized by this plasma method was 5 ppm or less. The various synthetic quartz glass ingots thus formed were cut into dimensions of 30 x 20 x 10 mm, and both sides were polished to a mirror finish to prepare nine test pieces for excimer laser irradiation experiments. Next, for each of these nine test pieces, 248 nm
(KrF) energy density per pulse is 200, 400, 600 (mJ/cm 2
pulses), and the number of irradiation pulses 1×10 4 , 1×10 5 , 1
Irradiation was performed under irradiation conditions consisting of a combination of ×10 6 (pules). After the irradiation, each test piece was examined for changes in refractive index distribution using an interferometer, solarization using a transmittance meter, fluorescence intensity measurement using a fluorometer, and visually determining the presence or absence of cracks. . The results are shown in the table of experimental results and conditions below. As a result, there were clearly significant differences between the normal purity test piece and the high purity test piece in terms of fluorescence properties, transmittance, refractive index changes, etc., and the main cause of this was impurities contained in the silica glass. Although it was confirmed that it was an element, it was also found that it depends not only on this, but also on the OH group content in addition to the high purity of the impurity element. (Refer to Experimental Examples 1) to 6), 7) to 12)) Furthermore, in test pieces with normal purity impurity concentrations, OH
It is understandable that the stability of transmittance, refractive index, etc. improves as the group content increases, but
Even at 1100 ppm, the fluorescent properties are still strong and pose a practical problem. (See Experimental Examples 1) to 6)) Next, when comparing high-purity test pieces, it is found that when the OH group content is 5 ppm, there are problems with fluorescence intensity, transmittance decrease, refractive index change, and crack generation. If the OH group content is 300 ppm, the transmittance and refractive index are stable enough for practical use, and the fluorescence intensity and occurrence of cracks can be reduced.
(See Experimental Example 8) Furthermore, as understood from Experimental Example 10), OH
By setting the group content to at least 700 ppm, it is possible to further improve the fluorescence characteristics, transmittance, refractive index, etc. of the laser optical system, and also eliminate the occurrence of cracks. It becomes possible to provide an element suitable as an optical system for output laser light.
【表】
前頁の「実験結果一覧表」の「耐エキシマレー
ザ性」の欄の内、「透過、屈折率」の小欄におい
て“悪”とは、相対的にEプライムセンタが生成
することにより透過率が低下しやすく、屈折率が
上昇しやすいことを示し、“良い”とは、透過率
が低下しにくく、屈折率も変動しにくいことを示
す。
又、「耐エキシマレーザ性」の欄の内、「蛍光」
の小欄において“強い”とは、略650nmにピーク
を示す赤い蛍光が相対的に強いことを示し、“弱
い”とは相対的に弱いことを示す。
更に、「耐エキシマレーザ性」の欄の内、「クラ
ツク」の小欄において“多い”とは、パルス当り
のエネルギー密度(mJ/cm2・pulse)を高くして
照射した場合、クラツクの発生する頻度が高いこ
とを示し、“少ない”とは、クラツクの発生がほ
とんど起こらないことを示す。
「発明の効果」
以上記載の如く本発明によれば、石英ガラスの
高純度化とともにOH基という別異の要素を加味
する事により、前記光学特性や耐クラツク性等の
向上を図るとともに、長時間にわたる屈折率、透
過率等の安定性を確保し、高出力レーザ用の光学
系材料として極めて好適な素体を得る事が出来
る。
又本発明はリソグラフイー装置その他の高集積
回路製造装置のみならず、レーザ核融合装置その
他の高出力レーザに使用される光学系素体にも十
分適用可能である。[Table] "Bad" in the "Transmission, refractive index" column of the "Excimer laser resistance" column in the "Experiment results list" on the previous page means that the E-prime center is relatively generated. "Good" indicates that the transmittance tends to decrease and the refractive index tends to increase, and "good" indicates that the transmittance does not easily decrease and the refractive index does not easily fluctuate. Also, in the "Excimer laser resistance" column, "Fluorescence"
In the sub-column, "strong" indicates that the red fluorescence having a peak at about 650 nm is relatively strong, and "weak" indicates that it is relatively weak. Furthermore, in the "Excimer laser resistance" column, "a lot" in the "Cracks" column means that cracks occur when irradiation is performed at a high energy density per pulse (mJ/cm 2・pulse). "Rare" means that cracks rarely occur. "Effects of the Invention" As described above, according to the present invention, by increasing the purity of quartz glass and adding a different element called OH group, it is possible to improve the optical properties and crack resistance, etc. The stability of refractive index, transmittance, etc. over time can be ensured, and an element body that is extremely suitable as an optical system material for high-power lasers can be obtained. Furthermore, the present invention is fully applicable not only to lithography equipment and other highly integrated circuit manufacturing equipment, but also to optical system elements used in laser fusion equipment and other high-power lasers.
Claims (1)
されるレーザ光学系素体において、該素体を高純
度の石英ガラス材で形成するとともに、該ガラス
材組織中のOH基含有量を少なくとも300ppm以
上に設定した事を特徴とするレーザ光学系素体。 2 特許請求の範囲第1項記載のレーザ光学系素
体において、該素体を高純度の合成石英ガラス材
で形成するとともに、OH基含有量を少なくとも
700ppm以上に設定したレーザ光学系素体。 3 前記レーザ光がエキシマレーザである特許請
求の範囲第1項記載のレーザ光学系素体。[Claims] 1. In a laser optical system element used for laser light in a specific wavelength range of about 400 nm or less, the element is formed of a high-purity quartz glass material, and the OH in the structure of the glass material is A laser optical system element characterized by having a group content of at least 300 ppm or more. 2. In the laser optical system element according to claim 1, the element is formed of a high-purity synthetic quartz glass material, and the OH group content is at least
Laser optical system element set to 700ppm or higher. 3. The laser optical system element according to claim 1, wherein the laser beam is an excimer laser.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32388287A JPH01167258A (en) | 1987-12-23 | 1987-12-23 | Element assembly of laser optical system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32388287A JPH01167258A (en) | 1987-12-23 | 1987-12-23 | Element assembly of laser optical system |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5323264A Division JP2558217B2 (en) | 1993-11-29 | 1993-11-29 | Optical lithography equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01167258A JPH01167258A (en) | 1989-06-30 |
| JPH0463019B2 true JPH0463019B2 (en) | 1992-10-08 |
Family
ID=18159654
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP32388287A Granted JPH01167258A (en) | 1987-12-23 | 1987-12-23 | Element assembly of laser optical system |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01167258A (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8048169B2 (en) * | 2003-07-28 | 2011-11-01 | Baronova, Inc. | Pyloric valve obstructing devices and methods |
| CN103435260B (en) * | 2013-08-30 | 2015-08-05 | 连云港市弘扬石英制品有限公司 | A kind of ozone free quartz glass plate and preparation method thereof |
| JP7409636B2 (en) | 2019-11-27 | 2024-01-09 | 株式会社住田光学ガラス | Multi-component oxide glass, optical element, optical fiber, and method for producing multi-component oxide glass |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58125635A (en) * | 1982-01-22 | 1983-07-26 | Furukawa Electric Co Ltd:The | Radiation-resistant optical fiber |
| JP2542356B2 (en) * | 1983-10-22 | 1996-10-09 | 古河電気工業 株式会社 | Radiation resistant method for silica optical fiber glass |
| JPS611380A (en) * | 1984-06-14 | 1986-01-07 | Ishihara Sangyo Kaisha Ltd | Novel microorganism and production of optically active compound with the same |
| JPS61251538A (en) * | 1985-04-26 | 1986-11-08 | Chiyoe Yamanaka | Optical fiber |
| JPS6238291A (en) * | 1985-08-13 | 1987-02-19 | Nippon Steel Chem Co Ltd | Dephosphorization treatment method |
| JPS6280606A (en) * | 1985-10-04 | 1987-04-14 | Furukawa Electric Co Ltd:The | Single mode optical fiber |
| JPH0737336B2 (en) * | 1986-05-19 | 1995-04-26 | 古河電気工業株式会社 | Optical transmitter |
| JP2572410B2 (en) * | 1988-01-30 | 1997-01-16 | 大日本印刷株式会社 | Quartz glass inspection method |
-
1987
- 1987-12-23 JP JP32388287A patent/JPH01167258A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01167258A (en) | 1989-06-30 |
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