JP2754657B2 - High light-transmitting dust-proof coating with anti-reflection layer - Google Patents
High light-transmitting dust-proof coating with anti-reflection layerInfo
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- JP2754657B2 JP2754657B2 JP2452289A JP2452289A JP2754657B2 JP 2754657 B2 JP2754657 B2 JP 2754657B2 JP 2452289 A JP2452289 A JP 2452289A JP 2452289 A JP2452289 A JP 2452289A JP 2754657 B2 JP2754657 B2 JP 2754657B2
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- thickness
- transmittance
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、半導体の製造工程において、フォトマスク
やレクチルに塵埃等の異物が付着することを防止するた
めの反射防止層を有する高光線透過性防塵膜、特に2種
の照射光に共用できる防塵膜に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a high light transmission having an antireflection layer for preventing foreign matter such as dust from adhering to a photomask or a reticle in a semiconductor manufacturing process. The present invention relates to a dustproof film, particularly a dustproof film that can be used for two types of irradiation light.
LSIなどの半導体の製造において、フォトマスクのマ
スクパターンをフォトレジストに転写するリソグラフィ
ー工程では、フォトマスクやレチクルに異物が付着する
のを防止する必要があり、そのためにフォトマスクやレ
クチルをペリクルと呼ばれる防塵膜で保護している。In the manufacture of semiconductors such as LSIs, in the lithography process of transferring the mask pattern of a photomask to a photoresist, it is necessary to prevent foreign substances from adhering to the photomask or reticle. For this reason, the photomask or reticle is called a pellicle. Protected with a dustproof film.
フォトリソグラフィーにおいて用いる露光装置(ステ
ッパー)には、照射光の波長が365nm(i線)のもの
(i線ステッパー)と436nm(g線)のもの(g線ステ
ッパー)とがあり、必要に応じて両者を使い分けてい
る。この場合、防塵膜にはi線に対しては高透光性を示
すがg線に対しては高透光性を示さないものや、逆にg
線に対しては高透光性を示すがi線に対しては高透光性
を示さないものがあり、i線ステッパーとg線ステッパ
ーとでそれぞれに適した防塵膜を用意して使い分けなけ
ればならないという繁雑さがある。Exposure apparatuses (steppers) used in photolithography include those having an irradiation light wavelength of 365 nm (i-line) (i-line stepper) and those of 436 nm (g-line) (g-line stepper). We use both. In this case, the dustproof film has high translucency with respect to i-line but does not have high translucency with respect to g-line.
Some have high translucency for lines but not high for i-lines. For each i-line stepper and g-line stepper, a suitable dustproof film must be prepared and used. There is complexity that must be done.
このような繁雑さを解決するため、一つの防塵膜でi
線およびg線のいずれの光にも高い透過性を有する防塵
膜が提案されている(特願昭62−290882号)。この防塵
膜は、膜厚に対する光の透過率曲線がサインカーブを描
くことを利用して、365nmの光の透過率と436nmの光の透
過率がともに高くなるような膜厚、例えば1.45〜1.48μ
mを選択するものである。In order to solve such complexity, one dustproof film can
A dust-proof film having high transmittance to both light of the g-line and the g-line has been proposed (Japanese Patent Application No. 62-290882). This dust-proof film, using the fact that the light transmittance curve with respect to the film thickness draws a sine curve, a film thickness such that both the transmittance of 365 nm light and the transmittance of 436 nm light increase, for example, 1.45 to 1.48 μ
m is selected.
しかし、上記のような従来の防塵膜では、i線とg線
に対してともに高い透過率を示す膜厚の範囲が狭いた
め、膜厚のわずかの変化で透過率が大幅に変動する。ま
た膜厚を狭い範囲に制御することは困難であり、i線と
g線に対してともに透過率の高い防塵膜を得ることは事
実上難しいという欠点がある。However, in the above-described conventional dustproof film, since the range of the film thickness showing a high transmittance for both the i-line and the g-line is narrow, the transmittance greatly varies with a slight change in the film thickness. Further, it is difficult to control the film thickness in a narrow range, and it is practically difficult to obtain a dustproof film having a high transmittance for both the i-line and the g-line.
一方、防塵膜の透過率の高い領域を拡大する手段とし
て、防塵膜の片面または両面に反射防止層を形成するこ
とが行われている。しかしながら、上記のようなi線と
g線に対してともに高い透過率を示す防塵膜に反射防止
層を形成すると、逆にi線とg線に対してともに高い透
過率を示す領域が狭くなるという問題点がある。On the other hand, as a means for enlarging a region of the dustproof film having a high transmittance, an antireflection layer is formed on one or both surfaces of the dustproof film. However, when the antireflection layer is formed on the dust-proof film that exhibits high transmittance for both the i-line and the g-line as described above, the region that exhibits high transmittance for both the i-line and the g-line is narrowed. There is a problem.
本発明の目的は、上記のような問題点を解決するため
の、2種の照射光のいずれにも高い透過率を示し、かつ
高い透過率を示す膜厚の範囲が広い反射防止層を有する
高光線透過性防塵膜を提供することである。An object of the present invention is to provide an anti-reflection layer having a high transmittance for both of the two types of irradiation light and a wide range of film thickness showing a high transmittance in order to solve the above-described problems. An object of the present invention is to provide a high light-transmitting dustproof film.
本発明は、次の反射防止層を有する高光線透過性防塵
膜である。The present invention is a highly light-transmitting dustproof film having the following antireflection layer.
(1)セルロース誘導体からなる基層の両面に反射防止
層を積層し、2種の照射光に共用する防塵膜であって、
基層の膜厚をd1(μm)、上記2種の照射光に対する基
層の屈折率の平均値をn1、それぞれの反射防止層の膜厚
をd2(nm)、上記2種の照射光に対する反射防止層の屈
折率の平均値をn2とした場合、d1、d2が 7.909n1 2−22.92n1+18.14≧d1≧ −1.935n1 3+13.08n1 2−27.04n1+18.82 …〔I〕 および −105.2n2+281.9≧d2≧−441.4n2 2+1184n2−731.8 …〔II〕 の範囲にあって、上記2種の照射光を98%以上透過する
ことを特徴とする高光線透過性防塵膜。(1) A dustproof film which is formed by laminating antireflection layers on both sides of a base layer made of a cellulose derivative and is shared by two types of irradiation light,
The thickness of the base layer is d 1 (μm), the average value of the refractive index of the base layer with respect to the above two types of irradiation light is n 1 , the thickness of each antireflection layer is d 2 (nm), and the above two types of irradiation light If the average value of the refractive index of the antireflection layer was n 2 with respect to, d 1, d 2 is 7.909n 1 2 -22.92n 1 + 18.14 ≧ d 1 ≧ -1.935n 1 3 + 13.08n 1 2 -27.04 n 1 +18.82 ... in the range of [I] and -105.2n 2 + 281.9 ≧ d 2 ≧ -441.4n 2 2 + 1184n 2 -731.8 ... [II], the two irradiation light 98% Highly light-transmitting dustproof film characterized by transmission.
(2)セルロース誘導体がプロピオン酸セルロースであ
る上記(1)記載の高光線透過性防塵膜。(2) The highly light-permeable dustproof film according to the above (1), wherein the cellulose derivative is cellulose propionate.
(3)基層の厚さが1.29〜1.34μm、反射防止層の厚さ
が62〜99nmで、365nmおよび436nmの波長の照射光を98%
以上透過する上記(2)記載の高光線透過性防塵膜。(3) The thickness of the base layer is 1.29 to 1.34 μm, the thickness of the anti-reflection layer is 62 to 99 nm, and the irradiation light having wavelengths of 365 nm and 436 nm is 98%.
The highly light-transmitting dustproof film according to the above (2), which transmits the above.
以下、本発明を図面により説明する。第1図は防塵膜
の例を示す断面図である。図において、1は防塵膜で、
基層2の両面に反射防止層3が形成されている。Hereinafter, the present invention will be described with reference to the drawings. FIG. 1 is a sectional view showing an example of a dustproof film. In the figure, 1 is a dustproof film,
Antireflection layers 3 are formed on both sides of the base layer 2.
本発明において、基層2として使用するセルロース誘
導体としては、例えばエチルセルロース、酢酸セルロー
ス、硫酸セルロース、リン酸セルロース、あるいはプロ
ピオン酸セルロースのような脂肪酸セルロース等がある
が、i線等の短波長の照射光に対する強度、製膜の容易
さの点からプロピオン酸セルロースが好ましい。In the present invention, examples of the cellulose derivative used as the base layer 2 include ethyl cellulose, cellulose acetate, cellulose sulfate, cellulose phosphate, and fatty acid cellulose such as cellulose propionate. Cellulose propionate is preferred from the viewpoints of strength and ease of film formation.
基層2の膜厚d1は前記〔I〕式で示される範囲、好ま
しくは −0.9136n1+2.720≧d1≧−1.036n1+2.854…〔III〕 で示される範囲とし、共用する照射光がi線およびg線
の場合は1.29〜1.34μmの範囲のものを使用する。上記
〔III〕式で示される範囲の膜厚は、通常の方法で容易
に製造できるので好ましい。プロピオン酸セルロース単
層膜の場合、i線およびg線の両方に高い透過率を示す
膜厚は、後述のように1.45〜1.48μmであり、1.29〜1.
34μmの膜厚のものはi線およびg線の両方に対して高
い透過率を示さないが、この範囲の膜厚を選択すること
により、反射防止層3を形成したときに98%以上の透過
率を得ることができる。Range thickness d 1 of the base layer 2 is represented by the formula [I] wherein preferably the range indicated by -0.9136n 1 + 2.720 ≧ d 1 ≧ -1.036n 1 + 2.854 ... (III), shared When the irradiation light is i-line and g-line, those having a range of 1.29 to 1.34 μm are used. The film thickness in the range represented by the above formula [III] is preferable because it can be easily produced by a usual method. In the case of the cellulose propionate monolayer film, the film thickness showing a high transmittance for both the i-line and the g-line is 1.45 to 1.48 μm as described later, and 1.29 to 1.
A film having a thickness of 34 μm does not show a high transmittance for both the i-line and the g-line, but by selecting a film thickness in this range, when the antireflection layer 3 is formed, a transmittance of 98% or more is obtained. Rate can be obtained.
第1図の反射防止層3には、2種の照射光に対する基
層2の屈折率の平均値n1より小さい屈折率の平均値n2の
ものを使用する。例えば基層2にプロピオン酸セルロー
スの薄膜を使用した場合、基層2のi線とg線に対する
屈折率の平均値n1は1.51となるので、反射防止層3には
屈折率の平均値n2が1.51より小さいもの、好ましくは1.
37以下の低屈折率のものを使用するのが好ましい。一般
的に使用可能な低屈折率のものとして、例えばテトラフ
ルオロエチレン/ビニリデンフルオライドコポリマー、
テトラフルオロエチレン/ビニリデンフルオライド/ヘ
キサフルオロプロピレンコポリマー、またはアクリル系
フッ素ポリマー、例えばCH2=CHCOOR1あるいはCH2=C
(CH3)COOR2〔ただしR1、R2は間にエーテル酸素原子を
含んでいてもよいフルオロアルキル基〕から選ばれるモ
ノマーの少なくとも1種からなるポリフルオロ(メタ)
アクリレート等のフッ素系ポリマーをあげることができ
る。The antireflection layer 3 of FIG. 1, to use a mean value n 2 of the average value n 1 is smaller than the refractive index of the refractive index of the base layer 2 with respect to two irradiation light. For example, when a thin film of cellulose propionate is used for the base layer 2, the average value n 1 of the refractive index for the i-line and the g-line of the base layer 2 is 1.51, and the average value n 2 of the refractive index for the antireflection layer 3 is Those smaller than 1.51, preferably 1.
It is preferable to use one having a low refractive index of 37 or less. Commonly used low refractive index materials include, for example, tetrafluoroethylene / vinylidene fluoride copolymer,
Tetrafluoroethylene / vinylidene fluoride / hexafluoropropylene copolymer or acrylic fluoropolymer such as CH 2 CHCOOR 1 or CH 2 CC
(CH 3 ) COOR 2 [where R 1 and R 2 are fluoroalkyl groups which may contain an ether oxygen atom therebetween] Polyfluoro (meth) comprising at least one monomer selected from
Fluorine-based polymers such as acrylates can be used.
それぞれの反射防止層3の膜厚d2は前記〔II〕式で示
される範囲、好ましくは −20.03n2+126.7≧d2≧−441.4n2 2+1184n2−731.8 …〔IV〕 で示される範囲とし、共用する照射光がi線およびg線
の場合は62〜99nmの範囲のものを使用する。上記〔IV〕
式で示される範囲の膜厚は、通常の方法で容易に製造で
きるので好ましい。Range thickness d 2 of each of the antireflection layer 3 is represented by [II] wherein preferably -20.03n 2 + 126.7 ≧ d 2 ≧ -441.4n 2 2 + 1184n 2 -731.8 ... shown in (IV) In the case where the shared irradiation light is i-line and g-line, the light having a range of 62 to 99 nm is used. Above [IV]
The film thickness in the range shown by the formula is preferable because it can be easily produced by a usual method.
特定の波長の光の透過率は膜厚によって変動し、膜厚
に対する透過率曲線はサインカーブを描く。そこで共用
する2種の照射光、例えばi線とg線について透過率曲
線を描くと、異なるサインカーブが得られる。2種の照
射光、例えばi線、g線共用防塵膜は、両方の透過率曲
線のピークが一致する膜厚、すなわち2種の照射光、例
えばi線、g線の両方に対して高い透過率を示す膜厚の
光線透過性膜を使用するが、このような光線透過性膜を
基層2として、その上に反射防止層3を形成すると、2
種の照射光、例えばi線およびg線の両方に対して高い
透過性を示す膜厚の範囲は逆に狭くなる。The transmittance of light of a specific wavelength varies depending on the film thickness, and the transmittance curve for the film thickness draws a sine curve. Therefore, when a transmittance curve is drawn for two types of shared irradiation light, for example, i-line and g-line, different sine curves are obtained. The two types of irradiation light, for example, the i-line and g-line shared dustproof film have a film thickness at which the peaks of both transmittance curves coincide with each other, that is, a high transmission for the two types of irradiation light, for example, both the i-line and the g-line. A light-transmitting film having a film thickness exhibiting a specific ratio is used. When such a light-transmitting film is used as a base layer 2 and an anti-reflection layer 3 is formed thereon,
On the contrary, the range of the film thickness that shows high transparency to various kinds of irradiation light, for example, both the i-line and the g-line is narrowed.
第2図(b)は反射防止層3を積層していないプロピ
オン酸セルロース膜の膜厚に対するi線(365nm)およ
びg線(436nm)の透過率曲線図であり、ピークAすな
わち1.45〜1.48μmの膜厚での範囲でi線およびg線の
両方に対する透過率が高いことがわかる。FIG. 2 (b) is a transmittance curve diagram of the i-line (365 nm) and the g-line (436 nm) with respect to the film thickness of the cellulose propionate film on which the antireflection layer 3 is not laminated, and shows the peak A, ie, 1.45 to 1.48 μm. It can be seen that the transmittance for both the i-line and the g-line is high in the range of the film thickness.
第2図(a)はプロピオン酸セルロース膜(基層)の
両面に厚さ79nmのフッ素ポリマーの反射防止層3(i線
とg線に対する屈折率の平均値1.37)を積層した高光線
透過性防塵膜について、基層2の膜厚の変化(反射防止
層の厚さは一定)に対するi線(365nm)およびg線(4
36nm)の透過率曲線図であり、第2図(b)におけるピ
ークAは、(a)ではピークBに示すように2つのピー
クに別れ、i線、g線の両方に高い透過率を示す範囲は
狭くなっている。一方、第2図(b)において2つに分
離していたピークC、すなわち基層2の膜厚が1.29〜1.
34μmの範囲では、(a)におけるピークDに示すよう
に一致したピークになり、i線およびg線の両方に高い
透過率を示し、かつ透過率98%以上の膜厚の範囲も広く
なっている。FIG. 2 (a) shows a high-light-transmitting dustproof layer in which a 79 nm-thick fluoropolymer antireflection layer 3 (average refractive index for i-line and g-line 1.37) is laminated on both surfaces of a cellulose propionate film (base layer). For the film, i-line (365 nm) and g-line (4 nm) with respect to a change in the thickness of the base layer 2 (the thickness of the antireflection layer is constant).
FIG. 2 (b) shows a peak curve A in FIG. 2 (b), which is divided into two peaks as shown by a peak B in FIG. 2 (a), and shows high transmittance in both i-line and g-line. The range is narrow. On the other hand, the peak C, which was separated into two in FIG. 2B, that is, the film thickness of the base layer 2 is 1.29 to 1.
In the range of 34 μm, the peak coincides as shown by the peak D in (a), shows a high transmittance for both the i-line and the g-line, and the range of the film thickness having a transmittance of 98% or more is widened. I have.
このように反射防止層3を積層しない状態で、i線お
よびg線の透過率がともに高くない膜厚1.29〜1.34μm
の範囲の基層2に前記のような反射防止層3を形成する
ことにより、i線、g線ともに高い透過率を示し、かつ
高透過率の範囲が広い反射防止層3を有する高光線透過
性防塵膜が得られる。In the state where the antireflection layer 3 is not laminated as described above, the film thickness of 1.29 to 1.34 μm in which the transmittance of both the i-line and the g-line is not high.
By forming the above-described anti-reflection layer 3 on the base layer 2 in the range of, high light transmittance having both the i-line and the g-line and high transmittance and having a wide range of high transmittance is obtained. A dustproof film is obtained.
以下、前記〔I〕〜〔IV〕式が導かれる過程について
説明する。Hereinafter, the process of deriving the formulas [I] to [IV] will be described.
一般に薄膜の透過率Tは、薄膜の膜厚をd、薄膜の屈
折率をn、入射側の相の屈折率をn11、透過側の相の屈
折率をn12、透過光の波長をλ、入射角を0(垂直入
射)とした場合、次の〔V〕式で表される(例えばフジ
テクノシステム(株)1984年発行、楯田俊一監修、「評
価とその応用技術ハンドブック」第134〜146頁「薄膜の
作製」吉田貞央著)。In general, the transmittance T of the thin film is d, the thickness of the thin film is n, the refractive index of the thin film is n, the refractive index of the incident side phase is n 11 , the refractive index of the transmission side phase is n 12 , and the wavelength of the transmitted light is λ. When the incident angle is 0 (normal incidence), it is expressed by the following equation [V] (for example, published by Fuji Techno System Co., Ltd., 1984, supervised by Shunichi Tateda, "Evaluation and Application Technology Handbook", No. 134 Pp. 146, "Preparation of thin film", written by Sadao Yoshida.
T=8n11n2n12{(n11 2+n2)(n2+n12 2)+4n11n2n
12 +(n11 2−n2)(n2−n12 2)cos(4πnd/λ)} …〔V〕 上記〔V〕式は単層の薄膜の透過率の計算式である
が、3層の場合は各層について〔V〕式の計算を繰り返
すと全体の透過率が得られることになる。すなわち第1
図の場合、入射光を1として上側の反射防止層3の透過
率を計算し、これにより得られた透過率を乗じた入射光
について基層2の透過率を計算し、これにより得られた
透過率を乗じた入射光についてさらに下側の反射防止層
の透過率を計算すれば、全体の透過率が得られる。この
場合、上側の反射防止層3の透過率は空気の屈折率をn
11とし、基層2の屈折率をn12として計算を行う。基層
2の透過率は上側の反射防止層3の屈折率をn11とし、
下側の反射防止層3の屈折率をn12として計算を行う。
下側の反射防止層3の屈折率は基層2の屈折率をn11と
し、空気の屈折率をn12として計算を行う。このような
全体の透過率の計算を基層2および各反射防止層3の屈
折率および膜厚を変えてi線およびg線の波長について
以下の計算を行い、透過率98%以上になる組合せを求め
る。T = 8n 11 n 2 n 12 {(n 11 2 + n 2 ) (n 2 + n 12 2 ) + 4n 11 n 2 n
12 + While (n 11 2 -n 2) ( n 2 -n 12 2) cos (4πnd / λ)} ... (V) above [V] formula is the calculation formula of the transmittance of the thin film of single-layer, 3 In the case of a layer, the total transmittance can be obtained by repeating the calculation of the equation [V] for each layer. That is, the first
In the case of the figure, the transmittance of the upper antireflection layer 3 is calculated with the incident light as 1, and the transmittance of the base layer 2 is calculated for the incident light multiplied by the transmittance thus obtained, and the transmittance obtained by this is calculated. By calculating the transmittance of the lower antireflection layer with respect to the incident light multiplied by the ratio, the overall transmittance can be obtained. In this case, the transmittance of the upper antireflection layer 3 is n
And 11, performs the calculation of the refractive index of the base layer 2 as n 12. The transmittance of the substrate 2 is the refractive index of the antireflection layer 3 of the upper and n 11,
Performing the calculation of the refractive index of the antireflection layer 3 of the lower as n 12.
Refractive index of the antireflection layer 3 on the lower side and the refractive index of the base layer 2 and n 11, performs calculation of the refractive index of air as n 12. The following calculation is performed for the wavelengths of the i-line and the g-line by changing the refractive index and the film thickness of the base layer 2 and each antireflection layer 3 based on the calculation of the entire transmittance. Ask.
初期設定として、基層2の膜厚を1200nm、屈折率は
波長365nmの時1.494、波長436nmの時は1.484に固定し、
入射角は0度(垂直入射)とし、各反射防止層3の膜厚
を60nm、屈折率を1.34として計算を行い、波長365nm、
波長436nmの透過率が共に、98%以上となる基材膜厚を
プロットする。As an initial setting, the thickness of the base layer 2 is fixed at 1200 nm, the refractive index is fixed at 1.494 at a wavelength of 365 nm, and 1.484 at a wavelength of 436 nm.
The incident angle was set to 0 degree (normal incidence), the thickness of each antireflection layer 3 was set to 60 nm, and the refractive index was set to 1.34.
The substrate film thickness at which the transmittance at a wavelength of 436 nm is both 98% or more is plotted.
反射防止層3の膜厚を2nmプラスしての計算を行
い、反射防止層3の膜厚が150nmになるまで繰り返し
た。The calculation was performed by adding the thickness of the antireflection layer 3 to 2 nm, and the calculation was repeated until the thickness of the antireflection layer 3 became 150 nm.
反射防止層3の屈折率を0.5プラスしての計算
を行い、反射防止層3の屈折率が1.40となるまで繰り返
す。The calculation is performed by adding the refractive index of the anti-reflection layer 3 to 0.5, and the calculation is repeated until the refractive index of the anti-reflection layer 3 becomes 1.40.
基層2の膜厚を5nmプラスしての計算を行
い、基層2の膜厚が1800nmとなるまで繰り返す。The calculation is performed by adding the thickness of the base layer 2 to 5 nm, and the calculation is repeated until the thickness of the base layer 2 becomes 1800 nm.
上記〜で得られる透過率98%以上のプロット
を、横軸が基層屈折率、縦軸が基層膜厚の座標上に表わ
すと、右方向に末広がり状のほぼ横方向に伸びる帯状の
領域に分散するので、その最も膜厚が広がった部分の上
側の輪郭線を最小二乗法によって関数を求めることによ
り、基層2の上限値の式として〔I〕式の不等号の左側
の式が得られた。この場合、基層および反射防止層の屈
折率は2種の照射光に対する屈折率の平均値として表し
た。同じく最も膜厚が広がった下側の輪郭線の関数を求
めることにより、基層2の下限値の式として〔I〕式の
不等号の右側の式が得られた。When the plot of the transmittance of 98% or more obtained in the above is represented on the coordinates of the base layer refractive index on the horizontal axis and the base layer thickness on the vertical axis, the plot is dispersed in a band-like region extending to the right and diverging almost horizontally. Therefore, by obtaining a function by the least squares method on the upper contour line of the portion where the film thickness is widened, the expression on the left side of the inequality sign of the expression [I] was obtained as the upper limit value of the base layer 2. In this case, the refractive indices of the base layer and the antireflection layer were represented as the average of the refractive indices for two types of irradiation light. Similarly, by calculating the function of the lower contour line where the film thickness is the largest, the equation on the right side of the inequality sign of the equation [I] was obtained as the equation of the lower limit value of the base layer 2.
上記〜で得られる透過率98%以上のプロットを
横軸が反射防止層屈折率、縦軸が反射防止層膜厚の座標
に表すと、右方向に末広がり状のほぼ横方向に伸びる帯
状の領域に分散するので、その最も膜厚が広がった部分
の上側の輪郭線をと同様にして最小二乗法によって関
数を求めることにより、反射防止層の上限の式として
〔II〕式の不等号の左側の式が得られた。同じく最も膜
厚が広がった下側の輪郭線の関数を求めることにより、
反射防止層の下限値の式として〔II〕式の不等号の右側
の式が得られた。If the horizontal axis represents the refractive index of the antireflection layer and the vertical axis represents the coordinates of the thickness of the antireflection layer, and the plot of the transmittance of 98% or more obtained in the above is represented by the coordinates of the antireflection layer thickness, the belt-shaped region extends to the right and extends substantially in the horizontal direction. As the upper limit of the antireflection layer is obtained by calculating the function by the least square method in the same manner as the upper contour line of the portion where the film thickness is widened, The formula was obtained. Similarly, by calculating the function of the lower contour line where the film thickness is the widest,
The expression on the right side of the inequality sign of the expression [II] was obtained as the expression of the lower limit value of the antireflection layer.
上記において、膜形成が容易な反射防止層の膜厚
が60〜100nmのプロットを同様に基層の座標に表わす
と、ほぼ横方向に伸びる帯状の領域に分散するので、そ
の最も膜厚が広がった上側の輪郭線の関数を求めること
により、好ましい範囲の上限値の式として〔III〕式の
不等号の左側の式を得た。同様に最も膜厚が広がった下
側の輪郭線の関数を求めることにより、好ましい範囲の
下限値の式として〔III〕式の不等号の右側の式を得
た。In the above description, if the thickness of the anti-reflection layer in which the film is easily formed is plotted in the range of 60 to 100 nm similarly to the coordinates of the base layer, it is dispersed in a band-like region extending substantially in the horizontal direction, so that the film thickness is the widest. By calculating the function of the upper contour line, the equation on the left side of the inequality sign of the equation [III] was obtained as the equation of the upper limit of the preferable range. Similarly, by calculating the function of the lower contour line where the film thickness is the widest, the equation on the right side of the inequality sign of the equation [III] was obtained as the equation of the lower limit of the preferable range.
上記において、膜形成が容易な反射防止層の膜厚
が60〜100nmのプロットを同様に反射防止層の座標に表
わすと、ほぼ横方向に伸びる帯状の領域に分散するの
で、その最も膜厚が広がった上側の輪郭線の関数を求め
ることにより、好ましい範囲の上限値の式として〔IV〕
式の不等号の左側の式が得られた。下側の輪郭線はと
同じであり、〔IV〕式の不等号の右側の式は〔II〕式の
それと同じ式である。In the above, if the plot of the film thickness of the anti-reflection layer for which the film formation is easy is 60 to 100 nm is similarly represented in the coordinates of the anti-reflection layer, it is dispersed in a band-like region extending substantially in the lateral direction, and the most film thickness is obtained. By calculating the function of the expanded upper contour line, the formula of the upper limit of the preferred range [IV]
The expression to the left of the expression inequality was obtained. The contour on the lower side is the same as that of [IV], and the equation on the right side of the inequality sign of equation [IV] is the same as that of equation [II].
本発明の反射防止層3を有する高光線透過性防塵膜の
製造方法は、スピンナーを用いて回転製膜法により形成
した基層2の両面に、低屈折率ポリマーの溶液を供給し
て回転製膜法により積層製膜して反射防止層3を形成す
る。The method for producing a highly light-transmitting dustproof film having the antireflection layer 3 according to the present invention comprises the steps of: supplying a low-refractive-index polymer solution to both surfaces of the base layer 2 formed by a spinning method using a spinner; The antireflection layer 3 is formed by laminating a film by a method.
具体的には、まずスピンナーに取付けたガラス等の平
滑な基板上にセルロース誘導体溶液を供給し、スピンナ
ーを回転させて回転製膜法によりセルロース誘導体の透
明薄膜からなる基層2を形成する。セルロース誘導体は
溶媒に溶解し、濾過等の精製を行った溶液を使用する。
溶媒としてはメチルエチルケトン、メチルイソブチルケ
トン、アセトン等のケトン類、酢酸ブチル、酢酸イソブ
チル等の低級脂肪酸エステル類、および前述のケトンま
たはエステルとイソプロピルアルコール等との混合溶媒
が使用される。形成される基層2の厚さ、溶液粘度や基
板の回転速度を変化させることにより前記範囲内の厚さ
にする。Specifically, first, a cellulose derivative solution is supplied onto a smooth substrate such as glass attached to a spinner, and the spinner is rotated to form a base layer 2 made of a transparent thin film of the cellulose derivative by a rotary film forming method. The cellulose derivative is dissolved in a solvent, and a purified solution such as filtration is used.
As the solvent, ketones such as methyl ethyl ketone, methyl isobutyl ketone and acetone, lower fatty acid esters such as butyl acetate and isobutyl acetate, and a mixed solvent of the aforementioned ketone or ester and isopropyl alcohol are used. The thickness within the above range is obtained by changing the thickness of the base layer 2 to be formed, the viscosity of the solution, and the rotation speed of the substrate.
基板上に形成されたセルロース誘導体透明薄膜からな
る基層2は、熱風や赤外線ランプ照射等の手段によって
乾燥させ、残存溶媒を除去する。The base layer 2 formed of a transparent thin film of cellulose derivative formed on the substrate is dried by means of hot air or irradiation with an infrared lamp to remove the residual solvent.
次いで、乾燥された基層2上に、低屈折率ポリマーの
溶液を供給し、回転製膜法により、前記の厚さの範囲内
になるように反射防止層3を形成する。低屈折率ポリマ
ーを溶解する溶媒は、低屈折率ポリマーを溶解でき、基
層2を溶解または膨潤させない溶媒で、沸点40〜220
℃、好ましくは60〜150℃の範囲のものが好ましく、例
えばキシレンヘキサフルオライド、ベンゾトリフルオラ
イド、五フッ化プロパノール等が使用できる。低屈折率
ポリマー溶液の濃度は0.3〜3重量%が好ましい。Next, a solution of a low-refractive-index polymer is supplied onto the dried base layer 2, and the antireflection layer 3 is formed so as to have a thickness within the above-described range by a rotary film forming method. The solvent that dissolves the low refractive index polymer is a solvent that can dissolve the low refractive index polymer and does not dissolve or swell the base layer 2 and has a boiling point of 40 to 220.
C, preferably in the range of 60 to 150C. For example, xylene hexafluoride, benzotrifluoride, propanol pentafluoride, etc. can be used. The concentration of the low refractive index polymer solution is preferably from 0.3 to 3% by weight.
次いで、上記によって得られた防塵膜1を反転してス
ピンナーに取付け、前記と同様の操作により、基層2の
もう一方の側に反射防止層3を積層する。Next, the dustproof film 1 obtained above is turned upside down and attached to a spinner, and the antireflection layer 3 is laminated on the other side of the base layer 2 by the same operation as described above.
以上のようにして製造された高光線透過性防塵膜は、
従来の防塵膜と同様に枠に取付け、マスクまたはレクチ
ル等の防塵体として用いられ、2種の照射光、例えばi
線およびg線の両方に対して高い透過率を示す。そして
2種の照射光、例えばi線およびg線のいずれも98%以
上透過する膜厚の幅が広いため、膜厚に多少の変動があ
っても高い透過率が得られ、膜の製造も容易になる。The high light-transmitting dustproof film manufactured as described above is
Attached to a frame in the same manner as a conventional dustproof film, used as a dustproof body such as a mask or a reticle, and used with two types of irradiation light, for example, i.
It shows high transmission for both the g-line and the g-line. Further, since the width of the film thickness through which the two types of irradiation light, for example, both the i-line and the g-line, transmit at least 98% is wide, a high transmittance can be obtained even if there is a slight variation in the film thickness. It will be easier.
以上の通り、本発明によれば、特定の厚さの基層に、
特定の反射防止層を積層するようにしたので、2種の照
射光のいずれの光にも高い透過率を示し、かつ高い透過
率を示す膜厚の範囲が広い高光線透過性防塵膜を得るこ
とができる。As described above, according to the present invention, in the base layer having a specific thickness,
Since a specific anti-reflection layer is laminated, a high light-transmitting dust-proof film having a high transmittance for both of the two types of irradiation light and a wide range of film thickness showing a high transmittance is obtained. be able to.
次に、本発明の実施例について説明する。 Next, examples of the present invention will be described.
実施例1 回転製膜法により製膜したプロピオン酸セルロース膜
からなる膜厚1.25〜1.4μmの基層に、回転製膜法によ
り79nmのフッ素ポリマー(ポリトリフルオロオクチルア
クリレート)の反射防止層(屈折率の平均値1.37)を積
層した防塵膜について、i線(365nm)およびg線(436
nm)の透過率を測定した。結果を第3図(a)に示す。Example 1 An antireflection layer (refractive index) of 79 nm fluoropolymer (polytrifluorooctyl acrylate) was formed on a base layer having a thickness of 1.25 to 1.4 μm comprising a cellulose propionate film formed by a rotary film forming method. The average value of 1.37) of the dustproof film was measured for the i-line (365 nm) and the g-line (436
nm) was measured. The results are shown in FIG.
第3図(a)からわかるように、基層に反射防止層を
積層することにより、i線およびg線の透過率100%の
ピークがほぼ重なり、かつ透過率の変動の幅も94〜100
%と小さく、i線およびg線の両方が98%以上の透過率
となる膜厚の範囲は約43nmであり、この時の基層の膜厚
は、1.29〜1.34μmである。As can be seen from FIG. 3 (a), by laminating the antireflection layer on the base layer, the peaks of the transmittance of 100% for the i-line and the g-line almost overlap, and the variation range of the transmittance is 94 to 100.
%, And the range of the film thickness at which both the i-line and the g-line have a transmittance of 98% or more is about 43 nm, and the film thickness of the base layer at this time is 1.29 to 1.34 μm.
比較例1 実施例1の基層(反射防止層を有しない膜厚1.25〜1.
4μmのプロピオン酸セルロースの薄膜)について、実
施例1と同様にして透過率を測定した。結果を第3図
(b)に示す。Comparative Example 1 The base layer of Example 1 (film thickness 1.25 to 1.
The transmittance was measured in the same manner as in Example 1 for a 4 μm thin film of cellulose propionate). The results are shown in FIG.
第3図(b)では、i線およびg線の透過率100%の
ピークが約21nmずれており、i線およびg線のいずれも
98%以上透過する膜厚の範囲は約15nmである。In FIG. 3 (b), the peaks of the transmittance of 100% for the i-line and the g-line are shifted by about 21 nm.
The range of the film thickness transmitting 98% or more is about 15 nm.
比較例2 第4図(b)に示すような透過率曲線を有する膜厚1.
4〜1.55μmのプロピオン酸セルロースからなる基層
に、実施例1と同様にして反射防止層を形成した防塵膜
について、i線およびg線の透過率を測定した。結果を
第4図(a)に示す。Comparative Example 2 Film thickness having a transmittance curve as shown in FIG.
The transmittance of i-line and g-line was measured for the dustproof film having an antireflection layer formed on a base layer of cellulose propionate having a thickness of 4 to 1.55 μm in the same manner as in Example 1. The results are shown in FIG.
第4図(b)では、i線およびg線の透過率100%の
ピークが膜厚1.46μm付近でほぼ一致しており、i線お
よびg線のいずれも98%以上透過する膜厚の範囲は約28
nmであるが、これに反射防止層を積層すると、第4図
(a)のように、透過率の変動幅は小さくなるものの、
i線およびg線の透過率100%のピークが約35nmずれる
ためi線およびg線のいずれも98%以上透過する膜厚の
範囲は約28nmから約19nmに狭くなる。In FIG. 4 (b), the peaks of the transmittance of 100% for the i-line and the g-line almost coincide with each other near the film thickness of 1.46 μm. Is about 28
When an anti-reflection layer is laminated on this, as shown in FIG. 4 (a), although the fluctuation width of the transmittance becomes small,
Since the peak of the transmittance of 100% for the i-line and the g-line is shifted by about 35 nm, the range of the film thickness for transmitting the 98% or more of the i-line and the g-line narrows from about 28 nm to about 19 nm.
実施例1および比較例1〜2の結果から、1.29〜1.34
μmの厚さの基層に特定の反射防止層を積層した場合
に、最も広い幅の範囲でi線およびg線をいずれも98%
以上透過する防塵膜を得ることができることがわかる。From the results of Example 1 and Comparative Examples 1-2, 1.29-1.34
When a specific antireflection layer is laminated on a base layer having a thickness of μm, both the i-line and the g-line are 98% in the widest range.
It can be seen that a transparent dustproof film can be obtained.
また、i線およびg線の透過率が重なった付近の膜厚
の膜に反射防止層を積層しても、i線およびg線の透過
率をさらに改善することはできないことがわかる。Further, it can be seen that even if an antireflection layer is laminated on a film having a thickness near the overlap of the transmittances of the i-line and the g-line, the transmittances of the i-line and the g-line cannot be further improved.
実施例2および3 実施例1において、基層の膜厚を1.29μm(実施例
2)または1.34μm(実施例3)とし、これらの基層に
50〜100nmの反射防止層を積層した防塵膜について、実
施例1と同様にして透過率を測定した。結果を第5図
(a)(実施例2)および第5図(b)(実施例3)に
示す。Examples 2 and 3 In Example 1, the thickness of the base layer was set to 1.29 μm (Example 2) or 1.34 μm (Example 3).
The transmittance of the dustproof film having the 50 to 100 nm antireflection layer laminated thereon was measured in the same manner as in Example 1. The results are shown in FIG. 5 (a) (Example 2) and FIG. 5 (b) (Example 3).
以上の結果から、1.29〜1.34μmの膜厚のプロピオン
酸セルロースの基層に62〜99nmの厚さの反射防止層を積
層した時、i線およびg線をどちらも98%以上透過する
防塵膜が得られることがわかる。From the above results, when an antireflection layer having a thickness of 62 to 99 nm is laminated on a base layer of cellulose propionate having a thickness of 1.29 to 1.34 μm, a dustproof film that transmits 98% or more of both i-line and g-line is obtained. It can be seen that it can be obtained.
第1図は防塵膜の断面図、第2図(a)、(b)は防塵
膜の膜厚に対する透過率曲線図、第3図(a)、
(b)、第4図(a)、(b)および第5図(a)、
(b)はそれぞれ実施例における透過率曲線図である。 1:防塵膜、2:基層、3:反射防止層FIG. 1 is a cross-sectional view of the dust-proof film, FIGS. 2 (a) and (b) are transmittance curve diagrams with respect to the thickness of the dust-proof film, FIG.
(B), FIGS. 4 (a), (b) and 5 (a),
(B) is a transmittance curve diagram in each Example. 1: dustproof film, 2: base layer, 3: anti-reflective layer
Claims (3)
射防止層を積層し、2種の照射光に共用する防塵膜であ
って、基層の膜厚をd1(μm)、上記2種の照射光に対
する基層の屈折率の平均値をn1、それぞれの反射防止層
の膜厚をd2(nm)、上記2種の照射光に対する反射防止
層の屈折率の平均値をn2とした場合、d1、d2が 7.909n1 2−22.92n1+18.14≧d1≧ −1.935n1 3+13.08n1 2−27.04n1+18.82 …〔I〕 および −105.2n2+281.9≧d2≧−441.4n2 2+1184n2−731.8 …〔II〕 の範囲にあって、上記2種の照射光を98%以上透過する
ことを特徴とする高光線透過性防塵膜。An antireflection layer laminated on both sides of a base layer made of a cellulose derivative and used for two types of irradiation light, wherein the base layer has a thickness of d 1 (μm), When the average value of the refractive index of the base layer with respect to light is n 1 , the thickness of each antireflection layer is d 2 (nm), and the average value of the refractive index of the antireflection layer with respect to the above two types of irradiation light is n 2 , d 1, d 2 is 7.909n 1 2 -22.92n 1 + 18.14 ≧ d 1 ≧ -1.935n 1 3 + 13.08n 1 2 -27.04n 1 +18.82 ... [I] and -105.2n 2 +281. 9 ≧ d 2 ≧ −441.4n 2 2 + 1184n 2 −731.8 A highly light-transmitting dustproof film which is in the range of [II] and transmits 98% or more of the above two types of irradiation light.
スである請求項(1)記載の高光線透過性防塵膜。2. The highly light-permeable dustproof film according to claim 1, wherein the cellulose derivative is cellulose propionate.
の厚さが62〜99nmで、365nmおよび436nmの波長の照射光
を98%以上透過する請求項(2)記載の高光線透過性防
塵膜。3. The high light beam according to claim 2, wherein the base layer has a thickness of 1.29 to 1.34 μm and the antireflection layer has a thickness of 62 to 99 nm, and transmits at least 98% of irradiation light having wavelengths of 365 nm and 436 nm. Permeable dustproof membrane.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2452289A JP2754657B2 (en) | 1989-02-02 | 1989-02-02 | High light-transmitting dust-proof coating with anti-reflection layer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2452289A JP2754657B2 (en) | 1989-02-02 | 1989-02-02 | High light-transmitting dust-proof coating with anti-reflection layer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02204747A JPH02204747A (en) | 1990-08-14 |
| JP2754657B2 true JP2754657B2 (en) | 1998-05-20 |
Family
ID=12140496
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2452289A Expired - Lifetime JP2754657B2 (en) | 1989-02-02 | 1989-02-02 | High light-transmitting dust-proof coating with anti-reflection layer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2754657B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7128007B2 (en) * | 2018-03-29 | 2022-08-30 | パイオニア株式会社 | Gas component detection flow cell and detector |
| KR20210146491A (en) * | 2020-05-26 | 2021-12-06 | 삼성디스플레이 주식회사 | Transport complex and transport module including the same |
-
1989
- 1989-02-02 JP JP2452289A patent/JP2754657B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02204747A (en) | 1990-08-14 |
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