JPS6410058B2 - - Google Patents
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- Publication number
- JPS6410058B2 JPS6410058B2 JP56035227A JP3522781A JPS6410058B2 JP S6410058 B2 JPS6410058 B2 JP S6410058B2 JP 56035227 A JP56035227 A JP 56035227A JP 3522781 A JP3522781 A JP 3522781A JP S6410058 B2 JPS6410058 B2 JP S6410058B2
- Authority
- JP
- Japan
- Prior art keywords
- resist
- resist material
- ultraviolet rays
- sensitivity
- present
- 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
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Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/004—Photosensitive materials
- G03F7/038—Macromolecular compounds which are rendered insoluble or differentially wettable
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- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Photosensitive Polymer And Photoresist Processing (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
Description
本発明は、例えば高密度集積回路素子の製造の
際にリソグラフイ工程で微細レジストパターンを
形成するために用いる遠紫外線用ネガ型レジスト
材料およびこの材料によるレジストパターン形成
方法に関するものである。
近年、半導体集積回路素子等の高性能化、高集
積度化の要求は非常に高く、リソグラフイ技術の
分野では、従来の紫外線のような光を用いたホト
リソグラフイに代つて、より波長の短い電子線、
X線、遠紫外線等の高エネルギービームを照射す
るリソグラフイ技術により、ホトリソグラフイで
得られる加工寸法よりさらに微細な加工寸法が得
られる微細加工技術を確立する努力が払われてい
る。これらの高エネルギービームを用いるリソグ
ラフイで使用されるレジスト材料は、微細加工の
加工寸法精度や能率に大きな影響を与えるためき
わめて重要である。
従来から、前述の重要さによつて、高エネルギ
ービーム用のレジスト材料の開発が多く試みられ
ているが、一般にポジ型レジスト材料は解像性は
すぐれているが感度が低く、またネガ型レジスト
材料は高感度ではあるがパターンの断面形状を制
御できるほど高い解像性を有しておらず、感度と
解像性が共にすぐれたレジスト材料の開発が強く
望まれている。
従来、電子線用のレジスト材料としては、いく
つかの高感度レジスト材料が知られており、X線
に対するレジスト材料の感度は電子線に対する感
度とほぼ平行関係にあることが知られている。し
かし、遠紫外線に対するレジスト材料の感度は電
子線に対する感度と平行関係にないため、高感度
電子線用レジスト材料が必ずしも高感度遠紫外線
用レジスト材料とはならない。したがつて遠紫外
線リソグラフイには、これに適したレジスト材料
の開発が必要である。とくに、近年開発された遠
紫外線を用いるマスクからウエハへのパターンの
一括転写法(遠紫外線反射投影露光方法)は、マ
スクとウエハが完全に分離しているために、マス
クおよびウエハの損傷がなく、低欠陥性等の利点
を有しているが、転写に有効な光量が少なく、こ
のためレジスト材料の高感度化が要求されてお
り、現在前記一括転写法の装置に適用可能な感度
をもつレジスト材料はほとんど知られていない。
これまで、遠紫外線用の高感度レジストとして
は、ホトレジストのAZ−2400およびホワイトレ
ジストが知られている。しかし、前者は現像液に
アルカリ溶液を用いるため、アルカリ金属による
汚染により、IC素子等の電気特性に悪影響を及
ぼし、また遠紫外線の吸収係数が大きい(吸収係
数;1.73μm-1at250mm)ため、レジスト膜厚が厚
いと遠紫外線が下部まで到達せず、充分な解像性
が得られない欠点があつた。後者のホワイトレジ
ストは、現像後の膜減りが30%〜40%と大きいた
めに、充分な加工精度が得られない欠点があつ
た。
本発明の発明者等は、前述の欠点を解消して高
感度でかつ高解像度の新規な遠紫外線用ネガ型レ
ジストの材料を得るために多くの試験研究を重ね
た結果、本発明に至つたものである。
すなわち、本発明の第1の発明は、繰返し単位
の重合体からなることを特徴とする遠紫外線用ネ
ガ型レジスト材料である。
また、本発明の第2の発明は、前記第1の発明
による遠紫外線用ネガ型レジスト材料を用いて基
材上に被膜を形成し、遠紫外線を照射した後、四
塩化炭素からなる現像液で現像し、ネガ型のレジ
ストパターンを得ることを特徴とする遠紫外線用
ネガ型レジスト材料によるレジストパターン形成
方法である。
本発明の前記式による繰返し単位からなる重合
体、すなわち、ポリノルマルプロピルα−クロロ
アクリレート(以下PnPCAと略称する)は後述
するようにレジスト材料として著しく高い感度お
よび解像性を有するものである。そして、レジス
ト材料としてこのPnPCAを使用し、現像液とし
て四塩化炭素を使用することにより前述の目的が
充分に達成されることが認められた。これを具体
的に説明すると、PnPCAを適当な溶剤に溶解し
てレジスト溶液を調製し、これを例えば回転法に
より基板上に塗布して乾燥した後、所定のパター
ンに従つて遠紫外線を照射し、次いで現像液とし
て四塩化炭素を用いて現像し、ネガ型のレジスト
パターンを得る。このようにして、本発明による
と遠紫外線に対してコントラストを示すγ値が
1.65であり、ネガ型レジスト材料として高いコン
トラストを示し、1.0μmのレジストパターンが断
面矩形形状を保つて解像でき、さらに現在最もよ
く用いられているレジスト材料であるポリメチル
メタクリレート(以下PMMAと略称する)に比
べ75倍の高感度を示した。
本発明によるレジスト材料は、高エネルギービ
ームに対し感応性の高いハロゲン元素を含んでい
るために、前述のような高感度を示すものと推定
されるが、反応のし易さは構造式から通常予想さ
れる値をはるかに超えるものであり、この特性は
本発明者等によつて初めて明らかにされたもので
ある。
また、本発明によるレジスト材料は遠紫外線の
波長域で感光性を有する。第1図は本発明のレジ
スト材料の吸光係数を示すものであり、第1図中
は100℃で30分間の熱処理をした本発明のレジ
スト材料の吸光係数であり、は対照としての
PMMAの吸光係数である。第1図から明らかな
ように、本発明のレジスト材料は180〜260nmに
吸収をもち、これらの波長域での吸収ピークにお
ける吸光係数は、本発明のレジスト材料では
0.34μm-1であり、PMMAの0.44μm-1に比べて小
さい。このことは充分に厚いレジスト層の下部ま
でエネルギ供給が行われ、したがつて高い形状比
の加工が可能となり、さらにピンホールの減少に
よる歩留りの向上が期待できる。
さらに、本発明のレジスト材料は、可視光、紫
外光(波長260nm以上)に感光性がないため、
通常光下で取扱うことができ、生産工程および管
理上取扱い易いという効果がある。
また、本発明によるレジストパターン形成方法
は、レジスト材料の現像処理工程で用いる現像液
が有機溶剤であるため、AZ−2400を使用した場
合のようなアルカリ金属による汚染並びにこれに
伴うIC素子等の電気特性への悪影響を生ずるこ
とがないという効果がある。
そして、本発明のレジスト材料は、一般のネガ
型レジスト材料と同様に、より高分子量のレジス
ト材料ではより高感度を示すことはいうまでもな
い。
本発明に用いるPnPCAの単量体は、公知の化
合物であり、例えばノルマルプロピルα−クロロ
アクリレート単量体は英国特許第514619号(1939
年)に記載されている方法に従つて製造すること
ができる。また、PnPCA重合体は溶液重合、懸
濁重合、塊状重合、乳化重合のような一般的な方
法で製造することができる。
以下、本発明の実施例について説明する。
単量体合成例
温度計、撹拌機および還流器を付けた容器に、
撹拌しながらトリクロロエチレン180.2g、98%
濃硫酸379.7g、ハイドロキノン0.2716gを入れ
液温を70℃に昇温した。液温を70℃に保持しなが
ら35%ホルマリン112gを1.5時間〜2.0時間かけ
て徐々に滴下した。ホルマリンの添加後に、徐々
に100〜110℃に昇温し、この温度をトリクレンの
還流が止まるまで保持した。続いて急激に140℃
に昇温させ、この温度を30分間保持した後、100
℃に冷却した。次に100℃を保持したまま、精製
したノルマルプロピルアルコール159.2gと水
60.6gの混合液を徐々に滴下し、液温を100℃で
1時間保持した後、撹拌を止めて水蒸気蒸留を行
い、106〜120℃の留分(2層に分離)を採集し
た。前記留分のうち下層の成分を5〜10wt%の炭
酸ソーダ水溶液で洗浄液が中性になるまで洗浄し
た後に、モレキユラーシーブを添加して脱水し
た。その後、ハイドロキノンを少量添加して減圧
蒸留を行い、10mmHgで46〜48℃の留分すなわち
精製nプロピルα−クロロアクリレート単量体
(以下これをnPCAという)41.58gを得た。
重合体合成例
前述のようにして得たnPCA29.7g、ジメチル
ホルムアミド118.7gおよびアゾビスイソブチロ
ニトリル0.297gを混合し、窒素気流中で撹拌し
ながら温度50℃で17時間重合した。重合の終了後
に、溶液を2のメタノール中に注ぎ、生成した
沈澱を真空乾燥した。次に、クロロホルムに溶解
し、メタノールで再沈澱させて精製した後に、真
空乾燥して約20.7gの目的とするPnPCA重合体
を得た。
この重合体について、ゲルパーミエーシヨンク
ロマトグラフイ(GPC)により求めた分子量は
重量平均分子量(w)で21.5万であり、多分散
度(d)は1.84であつた。また、デイフアレンシヤル
スキヤニングカロリメトリツク分析(DSC)お
よび熱重量分析(TG)の結果、ガラス転移温度
(Tg)は86〜87℃、分解温度(Td)は216〜217
℃であつた。
次に、レジストパターンの形成方法の実施例に
ついて説明する。
実施例 1
PnPCA1.4gをメチルセロソルブアセテート10
mlに溶解した後、0.45μmのフイルターで濾過し
てレジスト溶液を調製した。このレジスト溶液を
Si基板上に滴下し、2000rpmで回転塗布し、これ
を空気中において100℃で30分間熱処理した。熱
処理後のレジストの膜厚は約1.0μmであつた。次
いで、レジスト層に200W重水素ランプから発生
する遠紫外線を露光量を変えて照射した。照射後
に、基板を液温26.2℃の四塩化炭素からなる現像
液に2分間浸漬した後、乾燥窒素を吹きつけて乾
燥した。このとき、遠紫外線に照射された部分の
レジストは残る。その後、空気中において100℃
で30分間熱処理した後、各露光量での残存膜厚を
薄膜段差測定器(タリステツプ)で測定した。前
述のようにして得た遠紫外線露光における特性曲
線を第2図に示し、また感度およびコントラスト
(γ値)を後記表1に示す。第2図について説明
すると、縦軸は現像後の照射部の膜厚を、照射前
の膜厚を1とした場合の相対値(規格化残存膜
厚)で示したものであり、横軸は遠紫外線照射量
(mJ/cm2)の常用対数である。そして、ここでγ
値とは第2図に示した規格化残存膜厚と照射量の
関係において、規格化残存膜厚0.5における接線
の勾配をいい、この値がレジストの解像度を示す
1つの目安となる。一般に、前記勾配が大きいほ
どレジストの解像度がよい。感度は常法により、
規格化残存膜厚が0.5における照射量とした。
The present invention relates to a far-ultraviolet negative resist material used to form a fine resist pattern in a lithography process, for example, in the production of high-density integrated circuit devices, and a method for forming a resist pattern using this material. In recent years, demands for higher performance and higher integration of semiconductor integrated circuit elements have become extremely high. short electron beam,
Efforts are being made to establish microfabrication techniques that can obtain finer processing dimensions than those obtained by photolithography, using lithography techniques that irradiate high-energy beams such as X-rays and deep ultraviolet rays. Resist materials used in lithography using these high-energy beams are extremely important because they have a significant impact on the dimensional accuracy and efficiency of microfabrication. Due to the above-mentioned importance, many attempts have been made to develop resist materials for high-energy beams, but in general, positive resist materials have excellent resolution but low sensitivity, and negative resist materials Although the resist material has high sensitivity, it does not have high enough resolution to control the cross-sectional shape of the pattern, and there is a strong desire to develop a resist material that has both excellent sensitivity and resolution. Conventionally, several high-sensitivity resist materials have been known as resist materials for electron beams, and it is known that the sensitivity of a resist material to X-rays is approximately parallel to the sensitivity to electron beams. However, since the sensitivity of a resist material to far ultraviolet rays is not in a parallel relationship with the sensitivity to electron beams, a highly sensitive resist material for electron beams does not necessarily become a highly sensitive resist material for far ultraviolet rays. Therefore, it is necessary to develop resist materials suitable for deep ultraviolet lithography. In particular, the recently developed method of batch transfer of patterns from a mask to a wafer using deep ultraviolet light (deep ultraviolet reflection projection exposure method) eliminates damage to the mask and wafer because the mask and wafer are completely separated. , has advantages such as low defectivity, but the amount of light effective for transfer is small, and for this reason, there is a demand for higher sensitivity of resist materials. Resist materials are largely unknown.
Until now, photoresist AZ-2400 and white resist have been known as highly sensitive resists for deep ultraviolet rays. However, since the former uses an alkaline solution as a developer, contamination with alkali metals adversely affects the electrical characteristics of IC elements, etc., and the absorption coefficient of far ultraviolet rays is large (absorption coefficient: 1.73 μm -1 at 250 mm). If the resist film was too thick, far ultraviolet rays would not reach the bottom, resulting in a disadvantage that sufficient resolution could not be obtained. The latter white resist had the disadvantage that sufficient processing accuracy could not be obtained because the film loss after development was as large as 30% to 40%. The inventors of the present invention have conducted numerous experiments and researches in order to solve the above-mentioned drawbacks and obtain a new negative resist material for deep ultraviolet rays with high sensitivity and high resolution, and as a result, they have arrived at the present invention. It is something. That is, the first invention of the present invention is a repeating unit This is a negative resist material for deep ultraviolet rays, characterized by being made of a polymer of Further, the second invention of the present invention is to form a film on a base material using the negative resist material for far ultraviolet rays according to the first invention, and after irradiating it with far ultraviolet rays, a developer made of carbon tetrachloride is applied. This is a method for forming a resist pattern using a negative type resist material for deep ultraviolet rays, which is characterized by developing with a negative type resist material to obtain a negative type resist pattern. The polymer of the present invention comprising repeating units according to the above formula, ie, polynormal propyl α-chloroacrylate (hereinafter abbreviated as PnPCA), has extremely high sensitivity and resolution as a resist material, as described below. It has been found that the above object can be fully achieved by using this PnPCA as a resist material and using carbon tetrachloride as a developer. To explain this in detail, PnPCA is dissolved in a suitable solvent to prepare a resist solution, which is applied onto a substrate by a rotation method, dried, and then irradiated with far ultraviolet rays according to a predetermined pattern. Then, development is performed using carbon tetrachloride as a developer to obtain a negative resist pattern. In this way, according to the present invention, the γ value that shows contrast to far ultraviolet rays is
1.65, it shows high contrast as a negative resist material, and can resolve a 1.0 μm resist pattern while maintaining a rectangular cross-sectional shape. The sensitivity was 75 times higher than that of Since the resist material according to the present invention contains a halogen element that is highly sensitive to high-energy beams, it is presumed to exhibit high sensitivity as described above, but the ease of reaction is generally determined from the structural formula. This value far exceeds the expected value, and this characteristic was revealed for the first time by the present inventors. Further, the resist material according to the present invention has photosensitivity in the deep ultraviolet wavelength range. FIG. 1 shows the extinction coefficient of the resist material of the present invention. In FIG.
This is the extinction coefficient of PMMA. As is clear from FIG. 1, the resist material of the present invention has absorption in the wavelength range of 180 to 260 nm, and the extinction coefficient at the absorption peak in these wavelength ranges is
It is 0.34 μm -1 , which is smaller than PMMA's 0.44 μm -1 . This means that energy is supplied to the bottom of a sufficiently thick resist layer, thus making it possible to process a high shape ratio, and further improving the yield due to the reduction of pinholes. Furthermore, since the resist material of the present invention is not sensitive to visible light and ultraviolet light (wavelength of 260 nm or more),
It can be handled under normal light and has the advantage of being easy to handle in terms of production process and management. In addition, since the resist pattern forming method according to the present invention uses an organic solvent as the developer used in the development process of the resist material, contamination by alkali metals such as when AZ-2400 is used, and contamination of IC elements etc. due to this, can be avoided. This has the effect of not causing any adverse effects on electrical characteristics. It goes without saying that the resist material of the present invention exhibits higher sensitivity with higher molecular weight resist materials, similar to general negative resist materials. The PnPCA monomer used in the present invention is a known compound. For example, normal propyl α-chloroacrylate monomer is disclosed in British Patent No. 514619 (1939
It can be manufactured according to the method described in 2010). In addition, the PnPCA polymer can be manufactured by common methods such as solution polymerization, suspension polymerization, bulk polymerization, and emulsion polymerization. Examples of the present invention will be described below. Monomer synthesis example: In a container equipped with a thermometer, stirrer and reflux device,
Trichlorethylene 180.2g, 98% while stirring
379.7 g of concentrated sulfuric acid and 0.2716 g of hydroquinone were added, and the liquid temperature was raised to 70°C. While maintaining the liquid temperature at 70°C, 112 g of 35% formalin was gradually added dropwise over 1.5 to 2.0 hours. After addition of formalin, the temperature was gradually raised to 100-110°C, and this temperature was maintained until the reflux of trichlene stopped. Then, the temperature suddenly increased to 140℃.
After raising the temperature to 100 and holding this temperature for 30 minutes,
Cooled to ℃. Next, while maintaining the temperature at 100℃, add 159.2g of purified normal propyl alcohol and water.
After gradually dropping 60.6 g of the mixed solution and maintaining the liquid temperature at 100° C. for 1 hour, stirring was stopped and steam distillation was performed to collect a fraction at 106 to 120° C. (separated into two layers). The lower layer of the fraction was washed with a 5 to 10 wt % aqueous solution of sodium carbonate until the washing liquid became neutral, and then a molecular sieve was added to dehydrate it. Thereafter, a small amount of hydroquinone was added and vacuum distillation was performed to obtain 41.58 g of a fraction having a temperature of 46 to 48° C. at 10 mmHg, that is, purified n-propyl α-chloroacrylate monomer (hereinafter referred to as nPCA). Polymer Synthesis Example 29.7 g of nPCA obtained as described above, 118.7 g of dimethylformamide and 0.297 g of azobisisobutyronitrile were mixed and polymerized at a temperature of 50° C. for 17 hours with stirring in a nitrogen stream. After the polymerization was completed, the solution was poured into 2 methanol, and the resulting precipitate was dried under vacuum. Next, the product was purified by dissolving it in chloroform, reprecipitating with methanol, and then vacuum drying to obtain about 20.7 g of the desired PnPCA polymer. The weight average molecular weight (w) of this polymer was determined by gel permeation chromatography (GPC) to be 215,000, and the polydispersity (d) was 1.84. Additionally, as a result of differential scanning calorimetric analysis (DSC) and thermogravimetric analysis (TG), the glass transition temperature (Tg) was 86-87℃, and the decomposition temperature (Td) was 216-217℃.
It was warm at ℃. Next, an example of a method for forming a resist pattern will be described. Example 1 1.4 g of PnPCA was added to methyl cellosolve acetate 10
ml and filtered through a 0.45 μm filter to prepare a resist solution. This resist solution
It was dropped onto a Si substrate, spin-coated at 2000 rpm, and heat-treated at 100°C for 30 minutes in air. The film thickness of the resist after heat treatment was approximately 1.0 μm. Next, the resist layer was irradiated with far ultraviolet light generated from a 200W deuterium lamp at varying exposure doses. After the irradiation, the substrate was immersed for 2 minutes in a developer made of carbon tetrachloride at a temperature of 26.2° C., and then dried by blowing dry nitrogen. At this time, the portions of the resist that were irradiated with deep ultraviolet light remain. After that, it was heated to 100℃ in the air.
After heat treatment for 30 minutes, the remaining film thickness at each exposure dose was measured using a thin film step measuring device (Talystep). The characteristic curve obtained as described above upon exposure to deep ultraviolet rays is shown in FIG. 2, and the sensitivity and contrast (γ value) are shown in Table 1 below. To explain Figure 2, the vertical axis shows the film thickness of the irradiated area after development as a relative value (normalized residual film thickness) when the film thickness before irradiation is set to 1, and the horizontal axis shows the film thickness of the irradiated area after development as a relative value (normalized residual film thickness). It is the common logarithm of the far ultraviolet irradiation amount (m J /cm 2 ). And here γ
The value refers to the slope of the tangent line at the normalized residual film thickness of 0.5 in the relationship between the normalized residual film thickness and the irradiation dose shown in FIG. 2, and this value is a measure of the resolution of the resist. Generally, the larger the gradient, the better the resolution of the resist. Sensitivity is determined by the usual method.
The irradiation dose was taken as the normalized residual film thickness of 0.5.
【表】
前述したように、本実施例の場合に本発明のレ
ジスト材料のγ値は1.65で、遠紫外線用ネガ型レ
ジスト材料としては高いコントラストを示すこと
がわかる。また、感度は8.0mJ/cm2でPMMAの
600mJ/cm2に比べて約75倍の高い感度を示すも
のであつた。さらに、本発明のレジスト材料は、
一般のネガ型レジスト材料と同様により高分子量
のレジスト材料を用いれば、より高感度であるこ
とはいうまでもない。
実施例 2
実施例1と全く同様な方法で、Si基板上にレジ
スト膜を膜厚が約0.8μmになるように形成した。
次いで、レジスト層に最小線幅0.5μmのラインア
ンドスペースをもつマスクを通して200W重水素
ランプから発生する遠紫外光を照射した。その照
射量は特性曲線において、残膜率100%における
最少露光量を39mJ/cm2とした。照射後は実施例
1と全く同様な方法で現像および乾燥を行なつ
た。
前述のようにして得られたレジストパターン
は、1.0μmのラインアンドスペースがきれいに解
像されており、レジストパターン断面をSEMで
観察した結果、立上がりのよい矩形形状を示して
いた。なお、この際照射部の膜厚の減少はほとん
ど零であつた。
以上説明したように、本発明によるレジスト材
料は遠紫外線に対してPMMAの75倍の感度を有
し、かつ高いコントラストを有しているので、短
い露光時間で解像性の高い微細加工が可能である
という効果が得られる。また、本発明によるレジ
ストパターンの形成方法は、四塩化炭素からなる
現像液を用いるものであるため、アルカリ金属に
よる汚染やこれに伴なうIC等の電気特性への悪
影響がないという効果が得られる。そして本発明
は、半導体集積回路装置の他に光応用部品や磁気
バブル素子や表面弾性波素子等の微細パターン形
成用に適用して有効である。[Table] As described above, in the case of this example, the γ value of the resist material of the present invention is 1.65, which indicates that it exhibits high contrast as a negative type resist material for deep ultraviolet rays. In addition, the sensitivity is 8.0 mJ/cm 2 for PMMA.
The sensitivity was approximately 75 times higher than that of 600 mJ/cm 2 . Furthermore, the resist material of the present invention has
It goes without saying that if a resist material with a higher molecular weight is used like a general negative resist material, the sensitivity will be higher. Example 2 In exactly the same manner as in Example 1, a resist film was formed on a Si substrate to a thickness of about 0.8 μm.
Next, the resist layer was irradiated with far-ultraviolet light generated from a 200W deuterium lamp through a mask having lines and spaces with a minimum line width of 0.5 μm. Regarding the irradiation amount, the minimum exposure amount at a residual film rate of 100% was set as 39 mJ/cm 2 in the characteristic curve. After irradiation, development and drying were carried out in exactly the same manner as in Example 1. In the resist pattern obtained as described above, lines and spaces of 1.0 μm were clearly resolved, and when the cross section of the resist pattern was observed by SEM, it had a rectangular shape with good rise. At this time, the decrease in film thickness in the irradiated area was almost zero. As explained above, the resist material according to the present invention is 75 times more sensitive than PMMA to deep ultraviolet rays and has high contrast, making it possible to perform microfabrication with high resolution in a short exposure time. The effect is obtained. Furthermore, since the method for forming a resist pattern according to the present invention uses a developer made of carbon tetrachloride, it has the advantage that there is no contamination by alkali metals and the accompanying adverse effects on the electrical characteristics of ICs, etc. It will be done. In addition to semiconductor integrated circuit devices, the present invention is also effective when applied to the formation of fine patterns for optical application components, magnetic bubble devices, surface acoustic wave devices, and the like.
第1図は、本発明によるレジスト材料と
PMMAの吸光係数とを示す図、第2図は、本発
明のレジスト材料の遠紫外線に対する露光特性曲
線を示す図である。
FIG. 1 shows resist materials according to the present invention and
FIG. 2 is a diagram showing the exposure characteristic curve of the resist material of the present invention to deep ultraviolet rays.
Claims (1)
ガ型レジスト材料。 2 繰返し単位 の重合体からなる遠紫外線用ネガ型レジスト材料
を用いて基材上に被膜を形成し、遠紫外線を照射
した後、四塩化炭素からなる現像液で現像し、ネ
ガ型のレジストパターンを得ることを特徴とする
遠紫外線用ネガ型レジスト材料によるレジストパ
ターン形成方法。[Claims] 1. Repeating unit A negative-tone resist material for deep ultraviolet rays, characterized by consisting of a polymer of 2 Repeat unit Forming a film on a base material using a negative resist material for deep ultraviolet rays made of a polymer of A method for forming a resist pattern using a negative resist material for deep ultraviolet rays, characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56035227A JPS57150843A (en) | 1981-03-13 | 1981-03-13 | Negative type resist material for far ultraviolet ray and formation of resist pattern by this material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56035227A JPS57150843A (en) | 1981-03-13 | 1981-03-13 | Negative type resist material for far ultraviolet ray and formation of resist pattern by this material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57150843A JPS57150843A (en) | 1982-09-17 |
| JPS6410058B2 true JPS6410058B2 (en) | 1989-02-21 |
Family
ID=12435946
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56035227A Granted JPS57150843A (en) | 1981-03-13 | 1981-03-13 | Negative type resist material for far ultraviolet ray and formation of resist pattern by this material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57150843A (en) |
-
1981
- 1981-03-13 JP JP56035227A patent/JPS57150843A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57150843A (en) | 1982-09-17 |
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