TW561552B - Optical grading layer and its manufacturing method - Google Patents
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561552561552
發明領域 本發明係關於半導體微影製程,特別有關於微影製程 =抗反射層,更明破而言,係有關於—種光 其製作方法。 罈队 發明背景 、在微影製程中,為了增加解析度,曝光所需要的光源 便逐漸由G線(波長436 nm)和I線(波長365 nm)波長縮短至 小於250 nm的光源,例如深紫外光的氟化氬(ArF)雷射 (193 nm)及真空紫外光的氟(I?2)雷射(157 nm)等光源。由 於多數的基材例如高反射基材,特別是在深紫外光及真空 紫外光波段處,其反射問題都大過可見光波段,因此其導 ,光阻層發生駐波效應和凹缺(n〇tching)效應將會更加 嚴重’使得微影程序時的圖案轉移可信度大幅降低。此外 由於在此深紫外光波段,工業界生產多使用化學增幅 (Chemical Amplified)型光阻,此種光阻對於微小曝光量 的變化十分敏感,因此,在深紫外光及真空紫外光波段如 何製造高效能的光阻抗反射層是非常重要的。 為了改善特別是高反射基材在利用低波長光源進行微 影時產生如上所述缺點,便有許多方法被提出,其中之一 便是被工業界廣泛使用的底部抗反射層(BARC),它主要是 用來減小阻劑/基材界面間的反射光。 第1圖係顯示習知的一種利用底抗反射層來改善阻劑/ 基材界面間的反射光之底部抗反射結構剖面圖,其中標號 1 0為一基材’例如矽或金屬等高反射基材。為了消除此高FIELD OF THE INVENTION The present invention relates to a semiconductor lithography process, and more particularly to a lithography process = an anti-reflection layer. More specifically, it relates to a kind of light and a method for making the same. Background of the altar team. In the lithography process, in order to increase the resolution, the light source required for exposure is gradually reduced from G-line (wavelength 436 nm) and I-line (wavelength 365 nm) to less than 250 nm, such as deep Ultraviolet light argon fluoride (ArF) laser (193 nm) and vacuum ultraviolet light fluorine (I? 2) laser (157 nm). Since most substrates, such as highly reflective substrates, especially in the deep ultraviolet and vacuum ultraviolet light bands, have reflection problems that are larger than those in the visible light band, their guiding, standing wave effects and notches in the photoresist layer (n. The "tching" effect will be more serious, which greatly reduces the reliability of pattern transfer during the lithography process. In addition, because of the use of chemically amplified photoresistors in the production of deep ultraviolet light in this industry, this type of photoresist is very sensitive to small exposure changes. Therefore, how to make it in deep ultraviolet and vacuum ultraviolet light High-efficiency optical impedance reflective layers are very important. In order to improve the disadvantages mentioned above when lithography using low-wavelength light sources, especially for highly reflective substrates, many methods have been proposed. One of them is the bottom anti-reflection layer (BARC), which is widely used in the industry. It is mainly used to reduce the reflected light at the resist / substrate interface. Figure 1 is a cross-sectional view of a conventional anti-reflection structure at the bottom using an anti-reflection layer to improve the reflected light at the resist / substrate interface, where reference numeral 10 is a substrate, such as silicon or metal, with high reflection Substrate. To eliminate this height
〇522-8457TWF(N);dwwang.ptd 第 5 頁 561552 五、發明說明(2) 反射基材在微影時產生反光,而造成如上所述之駐波效應 以及凹缺(notching)效應,乃在基材10表面覆蓋一底部 抗反射層11 ,然後再塗佈一阻劑層1 2於底部抗反射層11 上。藉此方式,在微影程序時,底部抗反射層Η的存在可 使在阻劑層1 2 /底部抗反射層11界面的反射光與底部抗反 射層11/基材10界面的反射光產生破壞性干涉,將可降低 基材10產生的反射光,避免產生會影響微影可信度之駐波 和凹缺(notching)效應。 然而,上述傳統的底部抗反射層通常僅包括單一層, 且為了使在阻劑層12/底部抗反射層11界面的反射光與底 部抗反射層11/基材10界面的反射光產生破壞性干涉,底 部抗反射層1 1的厚度必須依照入射光(未顯示於圖面)的波 長與底部抗反射層11的折射率精準控制,但是底材10常因 前製程的因素造成表面有各種凹凸的現象,而使底部抗反 射層11的厚度因在底材1〇上位置的不同而有變動而難以控 制’而使上述降低基材10產生的反射光以避免產生會影響 微影可信度之駐波和凹缺效應的效果不佳。 有鑑於此,雙層或多層結構的底部抗反射層被發展出 來,例如第2圖所示,基材20上的底部抗反射層21共有 21a、21b、21c、21d、21e等五層結構。而該雙層或多層 結構的底部抗反射層中,各層之間的光學性質差異通常係 以上層為消光係數(Extinction Coefficient)及折射率較 小的材料,愈下層的材料,則消光係數及折射率愈大,以 達到理想的消除微影製程反射光的目的。而上述雙層或多〇522-8457TWF (N); dwwang.ptd Page 5 561552 5. Description of the invention (2) The reflective substrate generates light reflection during lithography, which causes the standing wave effect and the notching effect as described above. A surface of the substrate 10 is covered with a bottom anti-reflection layer 11, and then a resist layer 12 is coated on the bottom anti-reflection layer 11. In this way, during the lithography process, the presence of the bottom antireflection layer Η can cause the reflected light at the interface of the resist layer 1 2 / bottom antireflection layer 11 and the reflected light at the bottom antireflection layer 11 / substrate 10 interface to generate. Destructive interference can reduce the reflected light generated by the substrate 10 and avoid standing wave and notching effects that can affect the reliability of lithography. However, the above-mentioned conventional bottom anti-reflection layer usually includes only a single layer, and in order to make the reflected light at the interface of the resist layer 12 / bottom anti-reflection layer 11 and the reflected light at the interface of the bottom anti-reflection layer 11 / substrate 10 destructive. Interference, the thickness of the bottom anti-reflection layer 11 must be accurately controlled according to the wavelength of the incident light (not shown in the figure) and the refractive index of the bottom anti-reflection layer 11, but the substrate 10 often has various irregularities on the surface due to the factors of the previous process Phenomenon, and the thickness of the bottom anti-reflection layer 11 is changed due to the difference in position on the substrate 10, which is difficult to control. Therefore, the above-mentioned reduction of the reflected light generated by the substrate 10 is avoided to avoid affecting the reliability of lithography. The standing wave and notch effects are not as effective. In view of this, the bottom anti-reflection layer of a double-layer or multi-layer structure has been developed. For example, as shown in FIG. 2, the bottom anti-reflection layer 21 on the substrate 20 has five layers such as 21a, 21b, 21c, 21d, and 21e. In the bottom anti-reflection layer of the double-layer or multi-layer structure, the difference in optical properties between the layers is usually that the upper layer is a material with an extinction coefficient and a lower refractive index, and the lower the material, the extinction coefficient and refraction The larger the rate, the better the purpose of eliminating the reflected light in the lithography process. And the above two layers or more
0522-8457TWF(N);dwwang.p t d 5615520522-8457TWF (N); dwwang.p t d 561552
層結構的底部抗反 薄膜光學特性不同 複雜度、與成本。 太多,通常不大於 射層必須經由製程條 的目的,如此也增加 因此實際應用上,所 五層。 件的改變,來達到 了製程時間、製程 製作的層數也不會 而本發明的特徵之一,係提供一種光學漸變層及装制 作方法,以含氧原子的氣體電漿來處理單層的底:反土 層,得到無限多層的光學漸變層,其抗:邛抗反射 从苗成—▲ 丹沉反射的效果較傳娇The anti-reflection film at the bottom of the layer structure has different optical characteristics, complexity, and cost. Too much, usually no larger than the purpose of the radiation layer must go through the process bar, so it also increases so in practical applications, all five layers. Changes in the components are achieved to achieve the process time and the number of layers produced by the process. One of the features of the present invention is to provide an optically graded layer and a method for manufacturing the same. Bottom: Anti-soil layer, get infinite multilayer optical gradient layer, its anti: 邛 anti-reflection from Miaocheng-▲ Dan Shen reflection effect is better than Chuanjiao
=底部抗反射層為㊣,且製程複雜度較 H 層結構的底部抗反射層為低,且製程時間與成本降多 低0 干 社谨ΐϊΐ利用料外光微影製程定義小於180⑽ :構時’ Α 了減少高反射底材所造成阻劑内曝光不均的現 象,通常外加的底部抗反射層為氮氧化矽為基礎的材料, 但是這些材料在微影製程中曝後烘烤(PEB)步驟時會釋 放出鹼性物質,因此會破壞化學增幅型光阻的解析度。若 是使用單層的有機底部抗反射層,則必須開發出新的適用 於深紫外光的有機材料與製程。 而本發明的特徵之二,係提供一種光學漸變層及其製 作方=,以含氧原子的氣體電漿來處理單層的底部抗反射 層’得到無限多層的光學漸變層的同時也對底部抗反射層 的表面進行改質,使上述光學漸變層在微影製程中曝後烤 步驟時’減少驗性物質的釋放,避免化學增幅型光阻的解 析度受到破壞。 發明簡述= The bottom anti-reflection layer is ㊣, and the process complexity is lower than the bottom anti-reflection layer of the H-layer structure, and the process time and cost are reduced. 0 Ganshe would like to use the out-of-light lithography process definition to be less than 180⑽ 'Α Reduces the uneven exposure in the resist caused by highly reflective substrates. Usually the bottom anti-reflection layer is a silicon oxynitride-based material, but these materials are baked after exposure in the lithography process (PEB). The alkaline substance is released during the step, which will destroy the resolution of the chemically amplified photoresist. If a single-layer organic bottom anti-reflection layer is used, new organic materials and processes for deep ultraviolet light must be developed. The second feature of the present invention is to provide an optically graded layer and its preparation method. A single-layer bottom anti-reflection layer is treated with a gas plasma containing oxygen atoms to obtain an infinite number of optically graded layers. The surface of the anti-reflection layer is modified, so that the optical gradient layer in the photolithography process is exposed during the post-baking step to 'reduce the release of diagnostic substances and avoid the resolution of the chemically amplified photoresist from being damaged. Brief description of the invention
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本發明之目的係提供一種光學漸變層及其製作方法, 以含氧原子的氣體電漿來處理單層的底部抗反射層,得到 多層的光學漸變層,其抗反射的效果較傳統的單層底 部抗反射層為佳,且製程複雜度較製備雙層或多層結構的 底部抗反射層為低,且製程時間與成本也可降低。 、本發,之另一目的係提供一種光學漸變層及其製作方 ^以含氧原子的氣體電漿來處理單層的底部抗反射層, 得到無限多層的光學漸變層的同時也對底部抗反射層的表 面進行改質,使上述光學漸變層在微影製程中曝後烤步驟 $,減少鹼性物質的釋放,避免化學增幅型光阻的解析度 為了達成本發明之上述目 光學漸變層之方法,適用於一 於上述基材上形成一介電質, 其中上述下表面係與上述基材 氣體電聚處理上述介電質,以 質漸次變化的光學漸變層。 的,本發明係提供一種形成 基材之上,包含下列步驟: 包含一上表面與一下表面, 交界,以及以一含氧原子的 形成一作為抗反射層,且材 成於另1 卜从本發明更以上述方法提供—種光學漸變層,形 成^-基材之上,包括:於上述基材上形成有— = 面與一下表面,*中上述下表面係與上述基材 = 以一含氧原子的氣艎電漿處理上述介電質所形 成的一作為抗反射層,且氧化程度由上 降低的光學漸變層。 k上表面向下逐漸 實施例The object of the present invention is to provide an optically graded layer and a method for manufacturing the same. The bottom layer of a single layer is treated with a gas plasma containing oxygen atoms to obtain a multilayered optically graded layer. The bottom anti-reflection layer is better, and the process complexity is lower than that of the bottom anti-reflection layer for preparing a double-layer or multi-layer structure, and the process time and cost can also be reduced. Another purpose of the present invention is to provide an optically graded layer and a method for making the same ^ A single-layer bottom anti-reflection layer is treated with a gas plasma containing oxygen atoms to obtain an infinite number of optically graded layers while also resisting the bottom The surface of the reflective layer is modified, so that the optical gradient layer is baked in the photolithography process after the exposure step, reducing the release of alkaline substances, and avoiding the resolution of the chemically amplified photoresist. The method is suitable for forming a dielectric on the substrate, wherein the lower surface is an optically graded layer in which the dielectric is electropolymerized with the substrate gas to change the quality gradually. The present invention provides a method for forming a substrate, including the following steps: including an upper surface and a lower surface, an interface, and an oxygen-containing atom-forming layer as an anti-reflection layer, and the material is formed in another The invention further provides the above-mentioned method—an optically graded layer formed on a substrate, including: on the substrate, a surface and a lower surface are formed, the lower surface of the above and the substrate are formed by An optically-graded layer in which an oxygen atom gas plasma is used to treat one formed by the above dielectric as an anti-reflection layer, and the degree of oxidation is reduced from above. k the upper surface gradually downwards
561552 五、發明說明(5) " " ' " ----- /第3圖所示為在本發明之較佳實施例中,光學漸變層 之形成步驟與結構。 曰 。月參考第3A圖,在基材30,可以是金屬或半導體基 材’例如碎基材上,形成有厚度為約15 nm〜100 ηπι , ί好 為約30 nm、材質可為氮化物、碳化物、氮氧化物、碳氧 化物或上述之組合,較好為氮氧化矽的單層介電質抗反射 層31。再以含氧原子的氣體電漿33,較好為使用 2〇電漿,處理單層介電質抗反射層31 ;其中將含氧原子/ 的氣體電漿33的功率設定為100〜80 0瓦,較好為1〇〇〜4〇〇 瓦’處理時間為約2〜30分鐘,較好為2〜1〇分鐘;可處理的 深度可為1 nm~100 nm,視單層介電質抗反射層31的厚度 ,製程需要而定。只須施以簡單的電漿處理步驟,就可以 得到如第3B圖所示之光學漸變層34。 卜接下來請參考第4圖,第4亂所示為在本發明之較佳實 轭例中,沿第3B圖中之線段a A, C氧原子含量變化。其中 縱座標為氧原子含量數量百分比,以線性座標標示;橫座 標為光學漸變層34之縱深,以A點原點,b點為縱深約3〇 咖處、,以線性座標標示。其中在本發明之較佳實施例中, 在縱深為3〜10 nm範圍内,氧原子含量係漸次變化,可得 到層數相當於無限多層之光學漸變層。 接下來清參考第5圖,第5圖所示為在本發明之較佳實 施例中,在不同微影光線的入射光波長下,比較底部抗反 射層在電漿處理前後的反射率;其中縱座標為反射率,以 線性座標標示;而橫座標為微影入射光波長,以線性座標561552 V. Description of the invention (5) " " '" ----- / Figure 3 shows the steps and structure of forming the optically graded layer in the preferred embodiment of the present invention. Said. Referring to FIG. 3A, the substrate 30 may be a metal or semiconductor substrate. For example, a broken substrate is formed with a thickness of about 15 nm to 100 nm, preferably about 30 nm, and the material may be nitride or carbonized. It is preferably a single-layer dielectric anti-reflection layer 31 made of silicon nitride oxide, carbon oxide, or a combination thereof. Then, a single-layer dielectric anti-reflection layer 31 is treated with a gas plasma 33 containing oxygen atoms, preferably a 20 plasma; wherein the power of the gas plasma 33 containing oxygen atoms / is set to 100 ~ 80 0 Watts, preferably 100 to 400 Watts' processing time is about 2 to 30 minutes, preferably 2 to 10 minutes; the processing depth can be 1 nm to 100 nm, depending on the single-layer dielectric The thickness of the anti-reflection layer 31 depends on the manufacturing process. By simply applying a simple plasma treatment step, the optically graded layer 34 shown in Fig. 3B can be obtained. Next, please refer to FIG. 4, which shows the change of the oxygen atom content along the line a, C in FIG. 3B in the preferred yoke example of the present invention. Among them, the vertical coordinate is the percentage of the content of oxygen atoms, which is indicated by a linear coordinate; the horizontal coordinate is the depth of the optical gradient layer 34, which is at the origin of point A, and the point b is about 30 cm in depth, and is indicated by a linear coordinate. Among them, in a preferred embodiment of the present invention, the oxygen atom content is gradually changed in a range of 3 to 10 nm in depth, and an optically graded layer with an equivalent number of layers can be obtained. Next, reference is made to FIG. 5, which shows the reflectance of the bottom anti-reflection layer before and after the plasma treatment at different wavelengths of the incident light of the lithographic light in a preferred embodiment of the present invention; The vertical coordinate is the reflectivity, which is indicated by a linear coordinate; and the horizontal coordinate is the wavelength of the lithographic incident light, which is indicated by a linear coordinate.
561552 五、發明說明(6) 禚不。其中特別在波長小於200 nm的光源下,光學漸變層 34的反射率均遠較單層介電質抗反射層31的反射率為低。 ^接下來請參考第6圖,第6圖所示為在本發明之較佳實 知例中,比較在k影製程中曝後烘烤步驟時,以單層介電 =抗反射層31作為底部抗反射層與以光學漸變層34作為底 L Ϊ f射層’在不同烘烤溫度T,底部抗反射層所釋出驗 的離子強度。其中縱座標為離子強度(Α),以線性 ^標示;烘烤溫度(。〇,以線性座標標示。其中 作為底部抗反射層時,其所釋出驗性物質的離 f、&於1X 10 1G A,特別在一般烘烤溫度90 °C〜120 的離子漸變層34作為底部抗反射層所釋出鹼性物質 的離子強度遠低於以單層介電質抗反射層31作為底 射層所釋出鹼性物質的離子強度。 ^ 本發明係以一光學漸變層形於一 述光學漸變層來作Λ外少制> # 何上符別係以上 I作為谜衫1私時,阻劑之底部抗反射層。 ^成f法為於上述基材上形成-介電質,包含一上表面 一含氧;f子的ϋί係與上述基材交界;以及以 二:原子的就體電聚處理上述介電質 變層。上述光化,相當於無限多層的光學漸 微影光4 在以波長小於2°。光源為 層,在上述同波長ίίίΐ以單層介電質作為底部抗反射 微影製程中曝源下的反射率為低。且在後續 抗反射層時,所釋出二私4以上述光學漸變層作為底部 所釋出的鹼性離子強度,遠較上述以單層介 第10頁 0522-8457TWF(N);dwwang.Ptd 561552561552 V. Description of invention (6) No. Among them, especially under a light source having a wavelength of less than 200 nm, the reflectance of the optically graded layer 34 is much lower than that of the single-layer dielectric anti-reflection layer 31. ^ Please refer to FIG. 6, which shows a comparison of the single-layer dielectric = anti-reflective layer 31 as the single-layer dielectric = anti-reflective layer 31 in the preferred practical example of the present invention. At different baking temperatures T, the bottom anti-reflection layer and the optically graded layer 34 are used as the bottom L 射 f emissive layer, the ionic strengths released by the bottom anti-reflection layer are different. The vertical coordinate is the ionic strength (Α), which is indicated by a linear ^; the baking temperature (.0, is indicated by a linear coordinate. When used as the bottom anti-reflection layer, the ion f, & 10 1G A, especially at a general baking temperature of 90 ° C ~ 120. The ion intensity of the alkaline substance released from the bottom anti-reflection layer is much lower than that of the single-layer dielectric anti-reflection layer. The ionic strength of the alkaline substance released by the layer. ^ The present invention uses an optically graded layer in the form of an optically graded layer to make Λ outside reduction > The anti-reflection layer at the bottom of the resist. The f-forming method is to form a dielectric on the above-mentioned substrate, including an upper surface containing oxygen; the fluorene of the fonium is at the boundary with the above-mentioned substrate; The above dielectric change layer is processed in bulk. The above actinization is equivalent to infinite multilayer optical gradation light 4 at a wavelength of less than 2 °. The light source is a layer, and at the same wavelength, a single-layer dielectric is used as the bottom impedance. The reflectivity under the exposure source in the reflection lithography process is low, and in the subsequent anti-reflection layer At the time, the release of Erxin 4 with the above-mentioned optical gradient layer as the bottom released the basic ionic strength, which was much higher than that of the single layer described above. Page 10 0522-8457TWF (N); dwwang.Ptd 561552
五、發明說明(7) 電貝作為底部抗反射層時’所釋出的驗性離子強度為低。 如上所述,本發明係達成一種光學漸變層及其製作方 =,以含氧原子的氣體電漿來處理單層的底部抗反射層, 知到無限多層的光學漸變層,其抗反射的效果較傳統的單 層底部抗反射層為佳,且製程複雜度較製備雙層或多層結 構的底部抗反射層為低,且製程時間與成本也可降低。 另外,本發明亦能達成一種光學漸變層及其製作方 j ’以含氧原子的氣體電漿來處理單層的底部抗反射層, 得到,限多層的光學漸變層的同時也對底部抗反射層的表 =進行改質,使上述光學漸變層在微影製程中曝後烤步驟 ,,減^鹼性物質的釋放,避免化學增幅型光阻的解析度 t然本發明以較佳實施例揭露如丨,然其並非用以限 2 r ’圍:ί何熟悉此項技藝者,在不脫離本發明之精神 ® ^ ^ ^ ^ -V ^ 一 °午更動與满飾,因此本發明之保護範 圍當視錢之巾請專利“所界定者為準。V. Description of the invention (7) When the electric shell is used as the bottom anti-reflection layer, the ionic strength released is low. As mentioned above, the present invention achieves an optical gradient layer and its preparation method. The bottom anti-reflection layer of a single layer is treated with a gas plasma containing oxygen atoms. The anti-reflection effect of an infinite number of optical gradient layers is known. It is better than the traditional single-layer bottom anti-reflection layer, and the process complexity is lower than that of the bottom anti-reflection layer of double-layer or multi-layer structure, and the process time and cost can also be reduced. In addition, the present invention can also achieve an optical gradient layer and its producer j 'using a gas plasma containing oxygen atoms to process a single layer of the bottom anti-reflection layer, to obtain that the multi-layer optical gradient layer is also anti-reflection to the bottom. The surface of the layer is modified so that the optically graded layer is exposed to light during the photolithography process and then baked, thereby reducing the release of alkaline substances and avoiding the resolution of the chemically amplified photoresist. However, the present invention is a preferred embodiment. The disclosure is like 丨, but it is not intended to limit 2 r 'Wai: ί He who is familiar with this art, does not depart from the spirit of the invention ® ^ ^ ^ ^ -V ^ Noon changes and decorations, so the invention of The scope of protection shall be subject to the definition of the "scarves of money" patent.
0522-8457TWF(Ν);dwwang.p t d 第11頁 5615520522-8457TWF (N); dwwang.p t d p. 11 561552
為了讓本發明之上述目的、特徵、及優點能更明顯易 、以下配合所附圖式,作詳細說明如下·· 圖式簡單說明 第1圖所示為習知的一單層的底層抗反射層之結構。 第2圖所示為習知的一多層的底層抗反射層之結構。 第3 A及3 B圖所示為在本發明之較佳實施例中,光學漸 變層之形成步驟與結構。 第4圖所示為在本發明之較佳實施例中,沿第3B圖中 之線段AA’之氧原子含量變化。 、,第5圖所示為在本發明之較佳實施例中,在不同微影 光線的人射光波長下,比較底部抗反射層在電裝處理前後 的反射率。 第6圖所示為在本發明之較佳實施例中,比較在微影 L程=:烤步驟時’""單層介電質抗反射層31作為底 邓柷反射層與以光學漸變層34作為底部抗反射層,在不同 烘,溫度下,底部抗反射層所釋出鹼性物質的^子強度。 10〜基材、 11〜單層底部抗反射層、 1 2〜阻劑、 20〜基材、 21〜多層底部抗反射層、 21a〜多層底部抗反射層之第一層、 21b〜多層底部抗反射層之第二層、In order to make the above-mentioned objects, features, and advantages of the present invention more obvious and easy, the following detailed description is made with the accompanying drawings as follows: The drawings are briefly explained. Figure 1 shows a conventional single-layer anti-reflection of the bottom layer. Layer structure. FIG. 2 shows a conventional structure of a multi-layered bottom anti-reflection layer. Figures 3A and 3B show the steps and structure of forming an optical gradient layer in a preferred embodiment of the present invention. Fig. 4 shows the change in the oxygen atom content along the line AA 'in Fig. 3B in the preferred embodiment of the present invention. Fig. 5 shows the reflectance of the bottom anti-reflection layer before and after the electrical processing at the wavelength of human light emitted by different lithographic rays in a preferred embodiment of the present invention. FIG. 6 shows the comparison of the single-layer dielectric anti-reflection layer 31 as the bottom Deng Ying reflection layer and the optical The graded layer 34 serves as a bottom anti-reflection layer. Under different baking and temperature conditions, the intensity of the alkaline substance released by the bottom anti-reflection layer is low. 10 ~ substrate, 11 ~ single-layer bottom anti-reflection layer, 12 ~ resist, 20 ~ substrate, 21 ~ multilayer bottom anti-reflection layer, 21a ~ first layer of multilayer bottom anti-reflection layer, 21b ~ multilayer bottom anti-reflection layer The second layer of the reflective layer,
561552 圖式簡單說明 21c . 〜多層底部抗反射層之第三層、 21d, 〜多層底部抗反射層之第四層、 21e, 〜多層底部抗反射層之第五層、 30〜 基材、 31〜 單層介電質抗反射層、 33〜 02電漿處理、 34〜 光學漸變層。 ΙΙΙϋ·! 0522-8457TWF(Ν);dwwang.ρ td 第 13 頁561552 Schematic description of 21c. ~ The third layer of the multilayer bottom antireflection layer, 21d, ~ The fourth layer of the multilayer bottom antireflection layer, 21e, ~ The fifth layer of the multilayer bottom antireflection layer, 30 ~ substrate, 31 ~ Single-layer dielectric anti-reflection layer, 33 ~ 02 plasma treatment, 34 ~ optical gradient layer. ΙΙΙϋ! 0522-8457TWF (N); dwwang.ρ td page 13
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