TW424263B - The polarizing mask for printing the narrow-pitch holes - Google Patents
The polarizing mask for printing the narrow-pitch holes Download PDFInfo
- Publication number
- TW424263B TW424263B TW88120656A TW88120656A TW424263B TW 424263 B TW424263 B TW 424263B TW 88120656 A TW88120656 A TW 88120656A TW 88120656 A TW88120656 A TW 88120656A TW 424263 B TW424263 B TW 424263B
- Authority
- TW
- Taiwan
- Prior art keywords
- regions
- polarized
- patent application
- item
- scope
- Prior art date
Links
Landscapes
- Preparing Plates And Mask In Photomechanical Process (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
Abstract
Description
424:2:6; 3, 五、發明說明(l) ---- 5 -1發明領域: i ί t = Ϊ有關於積體電路設計,其特別是關係到—種 在先于U影成像製程中,用來印刷窄間距洞( narr〇w-Pltch h〇les)之分極光罩(p〇iarizing 。 5-2發明背景.· —電路領域内的製造商一直在盡力縮小積體電路上 的元4例如,電晶體或複晶閘極)之幾何尺寸 在缩小 元件尺寸方面所獲得的好處包括有更佳。J更二構 ^尺=然而,如當製造商試圖達到小及更小的元件尺寸 恰,許夕局限性的問題漸漸地浮現出來。其中,製造商必 須面對的-個首要問題是當要尋找更小的元件,用來 製造積體電路元件之工具所需的精密度也會隨著增高。 光學微影成像製程是用來轉移圖案於一個工件表面上 的-個著j的技術,如同對一個半導體晶片或者晶圓的一 個電路圖帛’並且也能夠為許多其他應用產生極小及錯綜 複雜㈣帛。傳統光學微影成冑製程涉及才巴電磁輻射( eleCtr〇magnetlc radiati〇n)應用於光罩(mask),而此 2罩具有開口處形成於其中,如此的設計可以把經過開口 處的光線或㈣線作m表面上的m域。一般 上’典型的光罩包含有—個透明的底#,底材上佈署著由424: 2: 6; 3, V. Description of the invention (l) ---- 5 -1 Field of invention: i ί t = Ϊ is related to integrated circuit design, which is particularly related to-a kind of imaging before U shadow In the manufacturing process, a narrow polar hole (narr0w-Pltch h0les) is used to print a polarizing mask (p0iarizing). 5-2 Background of the Invention ...-Manufacturers in the field of circuits have been trying to reduce the size of integrated circuits Element 4 (e.g. transistors or complex gates) has the following advantages in reducing component size: J is more structured. However, when manufacturers try to achieve small and smaller component sizes, the problem of Xu Xi's limitations gradually emerges. Among them, one of the first problems that manufacturers must face is that when looking for smaller components, the precision required for tools used to manufacture integrated circuit components will also increase. Optical lithography is a technique used to transfer patterns onto the surface of a workpiece, just like a semiconductor wafer or a circuit diagram of a wafer, and it can also produce very small and intricate complexities for many other applications. The traditional optical lithography process involves applying electromagnetic radiation (eleCtr〇magnetlc radiati〇n) to a mask, and the 2 masks have openings formed in them. Such a design can make light passing through the openings or The squall line is the m domain on the m surface. Generally, a typical photomask contains a transparent bottom #, and the substrate is
第4頁 212^2&3 五、發明說明(2) 電腦輔助設計系統(CAD)制定之各種不同 :"二路二轉移至,晶圓的表面上=罩 = = :完成是藉由可見的、紫外線的,或甚 因為女透過光罩傳遞至含有光阻材質的石夕底材 上。因為先罩含有由固體線和透光的空間组成的一個圖案 ,僅僅由透光空間編寫的那些範圍將允許輻射線透過。矽 底材上的元件便是由上述之過程創造出來的。 板1 〇組成 )上移除 在晶圓上 曝光在適 修正與改 除光阻上 的光阻顯 個獨立的 區域覆蓋 第一 Α圖顯示一傳 的光軍(mask) 鉻的地方。特 的光阻,將光 當的波長之下 變,光阻聚合 曝光的區域。 影並移除。) ,無限小的光 的點)或是被 統由鉻(c h 之剖面圖, 定波長的光 罩上洞圖案 將會造成光 物讓顯影劑 (相反地, 光罩被照射 源,其中光 關上(被鉻 rom 1 uni ) 其讓光通 經由.一光 曝光在光 阻聚合物 以化學的 負光阻系 過後,可 源可以被 覆蓋的點 圖案1 1 過光罩 罩投射 阻上。 上分子 方式分 統讓未 以被想 打開( 與石英 (mask 在塗佈 將光阻 結構的 解並移 被曝光 像成各 被乾淨 © 上述之傳統的光罩一般被稱作為玻璃上的鉻(Chr〇me on Glass; COG)或是一元(binary)光罩。完美的方型步 進函數只存在精確的光罩平面的理論極限。在與光罩的任 何距離上,比如晶圓平面,散射效應會造成影像呈現一有 限的影像傾斜。在較小的尺寸上,即影像的大小與距離印Page 4 212 ^ 2 & 3 V. Description of the invention (2) Computer aided design system (CAD) formulation of various differences: " Two-way two-to-two transfer to, the surface of the wafer = cover = =: completion is visible by , Ultraviolet, or even because the woman transmitted through the photomask to the stone Xi substrate containing a photoresist material. Because the mask first contains a pattern composed of solid lines and light-transmitting spaces, those ranges written only by light-transmitting spaces will allow radiation to pass through. The components on the silicon substrate are created by the above process. The composition of the board is removed on the wafer. The photoresist on the wafer is exposed to appropriate correction and removal. The photoresist is displayed in a separate area. The first Α image shows the area of a mask of chromium. The special photoresist changes the light below the current wavelength, and the photoresist polymerizes the exposed area. Shadow and remove. ), Infinitely small points of light) or chrome (cross-section view of ch, a pattern of holes on a mask with a fixed wavelength will cause a light object to allow the developer (in contrast, the mask is illuminated by the source, where the light is turned off (By chrome rom 1 uni) It allows light to pass through. After a light is exposed to the photoresist polymer with a chemical negative photoresist system, the dot pattern that can be covered by the source 1 1 passes through the photomask to project the resist. The method is divided so that the photoresist structure that is not opened with the mask (with quartz (mask in the coating) is exposed to be cleaned. Each of the traditional photomasks mentioned above is generally referred to as chromium on glass (Chr. me on Glass; COG) or binary mask. The perfect square step function only has the theoretical limit of the exact mask plane. At any distance from the mask, such as the wafer plane, the scattering effect will Causes the image to show a limited image tilt. At a smaller size, that is, the size and distance of the image
第5頁 424263 五、發明說明(3) 刷在相對λ /NA小的時候’附近影像的電場向量會相互作 用並且建設性的相加。產生的光強度曲線在特徵之間並不 完全是黑暗的’而是呈現了藉由鄰近特徵的交互作用所產 生的光強度。曝光系統的解析度是限制在投射光影像的對 比,即在鄰近的亮案特徵的之間的強度差。光強度在正常 為黑暗區的增加最後會造成鄰近特徵印刷成一級合的結構 而並非分離的影像。第一 Β圖顯示形成於光罩上的電場圖 。第一C圖顯示形成於晶圓上的電場圖。第一D圖顯示在晶 圓的光阻薄膜上光強度圖。 1私教程座生 常會提供改 輻射作用在 良通常包含 些開口或是 把相偏移光 設計的一個 的困難以自 減性相偏移 稱的半§周相 ,在使用上 在半導體製程中’電路中藉由光學微影成 的最小尺寸通常會縮減。改善微影成像技術通 良的解析度’這產生縮減最小的尺寸以及電磁 光罩區域之間的空間。最近在微影光罩上的改 相偏移(phase shift)技術,其中光罩上的某 某些部分是經過相偏移的。到目前為止,妨礙 罩(Phase shift mask)引進至實體大的微電路 問題是’就電路設計者而言,產生設計工具上 動地有利於光罩版面設計。由於這一原因,衰 ^ 罩(attenuated phase shifting mask)或 ,光罩(half-tone phase shifting mask) 已成為另一焦點。 在农減性相偏移光罩中,通常是以與半波長相偏移結Page 5 424263 V. Explanation of the invention (3) The electric field vector of the image near the brush when the relative λ / NA is small will interact with each other and add constructively. The resulting light intensity curve is not completely dark between features' but presents the light intensity generated by the interaction of neighboring features. The resolution of the exposure system is limited to the contrast of the projected light image, that is, the intensity difference between the adjacent bright case features. Increasing the light intensity in the normally dark area will eventually cause adjacent features to print into a superimposed structure rather than a separate image. The first B picture shows the electric field map formed on the photomask. The first C diagram shows an electric field pattern formed on a wafer. The first D picture shows a light intensity map on a circular photoresist film. 1Private course students will often provide a semi-§peripheral phase called the self-decreasing phase shift, which is a difficulty in designing radiation, which usually contains some openings or a phase shift light design. It is used in semiconductor processes. The minimum size of a circuit by optical lithography is usually reduced. Improving the lithographic imaging technology's good resolution 'This results in a reduction in the size and space between the areas of the electromagnetic mask. Recently, a phase shift technique on a lithographic mask, in which a certain part of the mask is phase shifted. Until now, the problem of preventing the introduction of phase shift masks to physically large microcircuits has been that 'for circuit designers, generating a design tool that facilitates the layout of a photomask. For this reason, attenuated phase shifting masks or half-tone phase shifting masks have become another focus. In agricultural subtractive phase shift masks, the
五、發明說明(4) 合的一輕微透明層來代替上述之鉻層。此光罩有就二元光 罩來說只有一個圖案步驟(patterning step)的性質。光 罩上的黑暗區域可以相偏移到1 8 〇度,且具有一衰減的振 幅(amplitude)以防止在這些區域内產生太多的光。第二A 圖顯示上述之技術的反射性範例。反射元件2 〇和反射相偏 移元件21的結合產生了負振幅,其提供圖像邊緣對比的改 進’而衰減則防止負振幅成為一個問題。第二B圖顯示形 成於光罩上的電場圖。第二C圖顯示形成於晶圓上的電場 圖。第二D圖顯示在晶圓的光阻薄膜上光強度圖。 雖然衰減性相偏移光罩已被廣泛用於印刷具有比傳統 一元光罩更大的製程視窗和圖像對比的洞圖案,但它仍然 有它的缺陷。尤其是,由於光或是適用於光學微影成像製 程之其他形式的輻射具有波浪般的性質,衍射( diffraction)和其他的干擾影響在光罩不透光區域的邊緣 出現’可能在曝光的圖案中產生尺度變化(或者產生錯置 圖案)。此一現象清楚地顯示於第二E圖中,一錯置圖案( ghost pattern)22形成於光阻層中。 5-3發明目的及概述: 鑒於上述之發明背景中’傳統的光罩所產生的諸多缺 點。本發明提供一種在光學微影成像製程中,甩來印刷窄 間距洞(narrow-pitch holes)之分極光罩(p〇iarizing5. Description of the invention (4) A slightly transparent layer is used instead of the chromium layer described above. This mask has the property that there is only one patterning step in the case of a binary mask. The dark areas on the reticle can be phase shifted to 180 degrees and have an attenuating amplitude to prevent too much light from being generated in these areas. Figure A shows a reflective example of the above technique. The combination of the reflective element 20 and the reflective phase shifting element 21 produces a negative amplitude, which provides an improvement in the contrast of the image edges' while attenuation prevents a negative amplitude from becoming a problem. The second diagram B shows the electric field pattern formed on the photomask. The second C diagram shows the electric field pattern formed on the wafer. The second D image shows a light intensity map on the photoresist film of the wafer. Although the attenuating phase shift mask has been widely used to print hole patterns with a larger process window and image contrast than traditional unitary masks, it still has its shortcomings. In particular, due to the wave-like nature of light or other forms of radiation suitable for optical lithography imaging processes, diffraction and other interference influences appear at the edges of the opaque areas of the reticle, which may be in the exposed pattern Changes in scale (or produces misaligned patterns). This phenomenon is clearly shown in the second E diagram, and a ghost pattern 22 is formed in the photoresist layer. 5-3 Objects and Summary of the Invention: In view of the above-mentioned background of the invention, there are many shortcomings caused by the traditional photomask. The invention provides a polarizing mask for printing narrow-pitch holes in optical lithography imaging processes.
42426 3 五、發明說明(5) mask),其藉由分極化的投射光源來增大製程視窗 (process window),且不會有側部突出現象(side lobe effect)的產生。 本發明的另一目的在借用於偏光器的優點,來調整光 源的分極方向。隨著這個操作,能夠改進精密圖案圖像的 對比,並且因此能夠縮小積體電路的尺寸。關於除了精密 的一維圖案以外的圖案,微圖案(micropatterning)程度 的需求相對地低。因此,即使光源分極就圖案來說沒有精 確地充分運用’對比的最終衰退仍很小。 根據以上所述之目的,本發明提供了一種在光學微影 成像製程中,用來印刷窄間距洞(narrow-pitch holes)之 分極光罩(polarizing mask)。此分極光罩包括一透明底 材’複數個第一分極區域和複數個第二分極區域。上述之 複數個第一分極區域係形成於透明底材上,且以等間隔放 置’再者’此複數個第一分極區域係用來指定一光源的— 第一分極方向。上述之複數個第二分極區域係形成於第— 分極區域上方,且每一個分極區域具有一部份與第一分極 區域位置重疊。此外,第二分極區域係設置於第一分極區 域的間隔處,再者’此複數個第二分極區域係用來指定光 源的一第二分極方向。而第一分極方向與第二分極方向的 相隔角度在設計上係用來控制光源穿越光罩的數量。42426 3 V. Description of the invention (5) mask), which uses a polarized projection light source to increase the process window, and does not have a side lobe effect. Another object of the present invention is to adjust the polarization direction of a light source by taking advantage of a polarizer. With this operation, the contrast of the precise pattern image can be improved, and therefore the size of the integrated circuit can be reduced. Regarding patterns other than precise one-dimensional patterns, the demand for the degree of micropatterning is relatively low. Therefore, even if the light source polarization is not accurately used in terms of the pattern, the final decay of the contrast is still small. According to the above purpose, the present invention provides a polarizing mask for printing narrow-pitch holes in an optical lithography imaging process. The polarizing mask includes a transparent substrate 'a plurality of first polarizing regions and a plurality of second polarizing regions. The plurality of first polarizing regions described above are formed on a transparent substrate, and 'more' are placed at equal intervals. The plurality of first polarizing regions are used to designate a first polarizing direction of a light source. The plurality of second polarized regions are formed above the first polarized region, and each of the polarized regions has a portion overlapping the position of the first polarized region. In addition, the second polarizing region is disposed at an interval of the first polarizing region, and further, the plurality of second polarizing regions are used to designate a second polarizing direction of the light source. The separation angle between the first polarization direction and the second polarization direction is designed to control the number of light sources passing through the mask.
第8頁 4242.6 3 五、發明說明(6) 5-4圓式簡單說明: ί - 5 Ξ :: 一傳統光罩的剖面圖; :一成於傳統光罩上的電場固. 第〇圖顯示形成你曰 致圖, 使用時; ;曰曰圓上的電場圖’當傳統光罩被 光罩IS:顯示在晶圓的光阻薄膜上光強度圖,當傳統 第二Β圖顯示ί::ί =移光罩的剖面圖; 第二。圖顯示形成於移光罩上的電場圖; 移光,被使用時; 、3曰 、電場圖,當衰減性相偏 性相: = = 圓的光阻薄膜上光強度圖,當衰減 第二Ε圆顯示—錯 第三Α圖顯示本圖於光阻層中; 第三B圖顯示—圖的剖面圖; 施例被使用時;以及” ^ '光阻層,當本發明之實 第四圖顯示本發明實 貝匕仍尸/r才未用的分極角度。 主要部分之代表符號: 3 0 0分極相偏移光單; 〗石英底材; 302第一分極區域; 第9頁 ^ 42426 五、發明說明(乃 303第二分極區域 304相偏移區域; 3 1 ◦光阻圖案層; 3 1 1 光阻;以及 3 1 2光阻。 5-5發明鮮細說明 &文,藉由第三A、第三B和第四圖來更詳細描述本 ^ ^ ^佳貫施例。請參照上述圖式,特別是第三Α圖, 士庶制Γ 了為依據本發明之較佳實施例的—種在光學微影 二王中’用來印刷窄間距洞(narrow-pi tch holes)之 么極农減性相偏移光罩(P〇Urizing attenuated phase shifting mask)。 在進入本發明之較佳實施例的細節前,首先介紹為配 合本發明所使用之習知的光學微影成像裝置。光學微影成 像裝置包含有一散發部分耦合之電磁輻射的光源(例如, 紫外線)。此電磁輻射係應用於本發明之分極光罩( polarizing mask)。而上述之分極光罩的構成是為了套用 電磁輻射的一個預期的圖案,透過一個適當地光學系統, 轉移到一個工件或晶圓的表面上。光學微影成像術在用於 半導體元件的圊案轉移時早已成為一個尤其合適的技術, 因此它將理解這個描述將在那環境條件中。在光阻製程中Page 8 4242.6 3 V. Description of the invention (6) 5-4 Circular simple description: ί-5 Ξ :: a cross-sectional view of a traditional photomask;: a solid electric field on the traditional photomask. Figure 0 shows Form your own picture, when used; The electric field diagram on the circle 'when the traditional photomask is covered by the photomask IS: the light intensity map displayed on the photoresist film of the wafer, when the traditional second B chart shows ί :: ί = sectional view of the shift mask; second. The figure shows the electric field pattern formed on the light shifting mask; when light is shifted, when it is used; 3, the electric field pattern, when the attenuation phase is biased: = = the light intensity diagram on the circular photoresist film, when the attenuation is second Ε circle display-wrong third A picture shows this picture in the photoresist layer; third B picture shows-sectional view of the picture; when the embodiment is used; and "^" photoresist layer, when the fourth embodiment of the invention The figure shows the polarizing angle of the real shell dagger of the present invention, which is not used yet. The representative symbols of the main part: 300 polarizing phase shift light sheet; Quartz substrate; 302 first polarizing region; page 9 ^ 42426 V. Description of the invention (the 303 phase shift region of the 303 second polarized region; 3 1 ◦ photoresist pattern layer; 3 1 1 photoresist; and 3 1 2 photoresist. 5-5 invention detailed description & text, borrow The third A, the third B, and the fourth diagram are used to describe this embodiment in more detail. Please refer to the above-mentioned drawings, especially the third diagram A, which is made according to the present invention. Example of the "Second King of Optical Lithography" used to print narrow-pi tch holes. zing attenuated phase shifting mask). Before entering the details of the preferred embodiment of the present invention, the conventional optical lithography imaging device used in conjunction with the present invention is first introduced. The optical lithography imaging device includes an electromagnetic coupling that emits a partial coupling. A light source of radiation (for example, ultraviolet light). This electromagnetic radiation is applied to the polarizing mask of the present invention. The polarizing mask described above is configured to apply an expected pattern of electromagnetic radiation and transmit through an appropriate optical System, transferred to the surface of a workpiece or wafer. Optical lithography has long been a particularly suitable technology for the transfer of semiconductor components, so it will understand that description will be in that environmental condition. Photoresist
第10頁 4242^3 五、發明說明(8) ’工件或晶圓的表面上覆蓋有一正或負光阻層。合適的光 阻質在技藝中眾所周知,因此其細節在此不做進—步的探 討。隨後’由或缺少電磁輻射的應用下’選擇性地圖銮 刻上述之光阻層。 、 電磁輪射所衝擊到的選擇性區域表面,被稱作為電磁 轄射應用區域(electromagneic radiation appiicati〇n region,EAR)。電磁輻射應用區域的定義為已經暴露在有 影響的光源之足夠的電磁輻射中的表面區域。而任何不在 電磁輪射應用區域内的表面區域則定義為不受影響的空間 本發明之分極相偏移光罩(P〇larizing phase shifting mask)300包含有一透明底材3〇1,此透明底材以 含石英尤佳,複數個第一分極區域3 〇 2,複數個第二分極 區域3 0 3以及一非強制性(可有或可無)的相偏移區域3〇4 上述之複數個第一分極區域3〇2係形成於石英底材3〇1 上,且以等間隔放置。再者,此複數個第一分極區域係用 來指定一光源的一第一分極方向。而上述之複數個第二分 極區域303則形成於複數個第一分極區域3〇2上方,且複數 個第一分極區域的每一個分極區域具有一部份與複數個第 一分極區域位置重璺。再者,此複數個第二分極區域係設Page 10 4242 ^ 3 V. Description of the invention (8) ’The surface of the workpiece or wafer is covered with a positive or negative photoresist layer. Appropriate photoresistors are well known in the art, so the details are not discussed further here. Subsequently, the aforementioned photoresist layer is selectively engraved "with or without the application of electromagnetic radiation". The surface of the selective area that the electromagnetic wheel strikes is called the electromagnetic radiation appiication region (EAR). An electromagnetic radiation application area is defined as a surface area that has been exposed to sufficient electromagnetic radiation from an influential light source. And any surface area that is not within the application area of the electromagnetic wheel is defined as an unaffected space. The polarizing phase shifting mask 300 of the present invention includes a transparent substrate 30, which is a transparent substrate. Quartz material is particularly preferred, a plurality of first subpolar regions 3 002, a plurality of second subpolar regions 3 303, and a non-mandatory (optional or optional) phase offset region 304. The first polarizing region 302 is formed on the quartz substrate 301 and is placed at equal intervals. Furthermore, the plurality of first polarization regions are used to designate a first polarization direction of a light source. The plurality of second polarized regions 303 are formed above the plurality of first polarized regions 302, and each of the plurality of first polarized regions has a portion and the positions of the plurality of first polarized regions are repeated . Furthermore, the plurality of second polar regions are designed
五、發明說明(9) 置於複數個第一分極區域中的間隔處,其主要是用來指定 光源的一第二分極方向。上述之可有或可無的相偏移區域 304係被部屬在第一分極區域與第二分極區域的重疊位置 ’且介於第一分極區域與第·一分極區域之間。V. Description of the invention (9) It is placed at intervals in a plurality of first polarization regions, and is mainly used to specify a second polarization direction of the light source. The above-mentioned optional phase shift region 304 is subordinated to the overlapping position of the first polar region and the second polar region, and is between the first polar region and the first polar region.
除此之外,複數個第二分極區域3 0 3的每一個分極區 域係以一 T型結構形成’且同樣以等間隔放置,並具有一 第一厚度於重疊位置,以及一第二厚度於複數個第一分極 區域302中的間隔處。第一分極區域的厚度大概與第二分 極區域的第一厚度相等,而複數個第二分極區域中的間隔 寬度則與複數個第一分極區域中的間隔寬度相等。雖然如 此,第一和第二分極區域的等間隔寬度與第一或第二分極 區域的等間隔是特別為固定間距(f i X e d p i t c h )之洞圖案 (hole pattern )設計的。而這些限制情況可以隨著不同 圖案而更改或再設計。In addition, each of the plurality of second polarized regions 3 0 3 is formed in a T-shaped structure and is also placed at equal intervals, and has a first thickness at the overlapping position, and a second thickness at At intervals in the plurality of first polarization regions 302. The thickness of the first polarized region is approximately the same as the thickness of the second polarized region, and the width of the interval in the plurality of second polarized regions is equal to the width of the interval in the plurality of first polarized regions. Nonetheless, the equal interval width of the first and second polarized regions and the equal interval of the first or second polarized regions are specifically designed for hole patterns of a fixed pitch (f i X e d p i t c h). These restrictions can be changed or redesigned with different patterns.
無論如何,本發明用來设计分極相偏移光罩3 0 0之上 述限制情況最終產生如第三B圖所示之圖案钱刻後的光阻 層310。在此,光阻圖案310所需之解析度由傳統之間距1 (不同分極區域所產生之光阻311與312之間的距離)降至 本發明之間距2 (相同分極區域所產生之光阻3 11間的距離 )。換句話說,製造高密度的元件,本發明僅需較一般低 的解析度。In any case, the present invention is used to design the above-mentioned limitation of the phase-shifting phase shift mask 300, and finally the patterned photoresist layer 310 shown in FIG. 3B is generated. Here, the required resolution of the photoresist pattern 310 is reduced from the conventional distance 1 (the distance between the photoresist 311 and 312 generated in different polarized regions) to the distance 2 in the present invention (the photoresist generated in the same polarized region). Distance between 3 and 11). In other words, to make high-density components, the present invention only requires a lower resolution than in general.
第12頁 4-24263 五、發明說明(ίο) 最後,.第一分極區域之第一分極方向與第二分極區域 之第二分極方向在相隔角度的設計上是小於9 0度。此相隔 角度在設計上係用來控制光源穿越分極光罩的數量。第四 圖顯示本發明之實施例所採用的分極角度。 以上所述僅為本發明之較佳實施例而已,並非用以限 定本發明之申請專利範圍;凡其它未脫離本發明所揭示2 精神下所完成之等效改變或修飾,均應包含在下述之 專利範圍内。 请Page 12 4-24263 V. Description of the Invention Finally, the first polarizing direction of the first polarizing region and the second polarizing direction of the second polarizing region are less than 90 degrees in the design of the separation angle. This separation angle is designed to control the number of light sources passing through the polarizing mask. The fourth figure shows the polarization angle used in the embodiment of the present invention. The above is only a preferred embodiment of the present invention, and is not intended to limit the scope of the patent application for the present invention; all other equivalent changes or modifications made without departing from the spirit disclosed in the present invention 2 should be included in the following Within the scope of patents. please
第13頁Page 13
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW88120656A TW424263B (en) | 1999-11-26 | 1999-11-26 | The polarizing mask for printing the narrow-pitch holes |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW88120656A TW424263B (en) | 1999-11-26 | 1999-11-26 | The polarizing mask for printing the narrow-pitch holes |
Publications (1)
Publication Number | Publication Date |
---|---|
TW424263B true TW424263B (en) | 2001-03-01 |
Family
ID=21643151
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW88120656A TW424263B (en) | 1999-11-26 | 1999-11-26 | The polarizing mask for printing the narrow-pitch holes |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW424263B (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7150945B2 (en) | 2003-11-18 | 2006-12-19 | Micron Technology, Inc. | Polarized reticle, photolithography system, and method of forming a pattern using a polarized reticle in conjunction with polarized light |
TWI798485B (en) * | 2019-09-06 | 2023-04-11 | 聯華電子股份有限公司 | Method for transferring mask pattern, polarizing mask and polarized exposure apparatus |
-
1999
- 1999-11-26 TW TW88120656A patent/TW424263B/en not_active IP Right Cessation
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7150945B2 (en) | 2003-11-18 | 2006-12-19 | Micron Technology, Inc. | Polarized reticle, photolithography system, and method of forming a pattern using a polarized reticle in conjunction with polarized light |
US7569311B2 (en) | 2003-11-18 | 2009-08-04 | Micron Technology, Inc. | Method of forming a pattern using a polarized reticle in conjunction with polarized light |
US7592107B2 (en) | 2003-11-18 | 2009-09-22 | Micron Technology, Inc. | Polarized reticle, photolithography system, and method of fabricating a polarized reticle |
TWI798485B (en) * | 2019-09-06 | 2023-04-11 | 聯華電子股份有限公司 | Method for transferring mask pattern, polarizing mask and polarized exposure apparatus |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US6934007B2 (en) | Method for photolithography using multiple illuminations and a single fine feature mask | |
US20050123841A1 (en) | Full phase shifting mask in damascene process | |
JP7384695B2 (en) | Photomask, photomask manufacturing method, and display device manufacturing method | |
US20020177078A1 (en) | Proximity correction using shape engineering | |
US20090258302A1 (en) | Sub-resolution assist feature of a photomask | |
JPH03141354A (en) | Exposing mask | |
EP1488284B1 (en) | Photomask and method for photolithographic patterning of a substrate by use of phase shifted assist features | |
TW407302B (en) | Photomask for use in manufacturing semiconductor and method of forming resist pattern | |
TW424263B (en) | The polarizing mask for printing the narrow-pitch holes | |
JPH06301192A (en) | Photo-mask | |
US7579121B2 (en) | Optical proximity correction photomasks | |
JP4784220B2 (en) | Phase shift mask | |
KR100207528B1 (en) | Half torn phase shift mask and its manufacturing method | |
JPH03156459A (en) | Memory semiconductor structure and phase shifting mask | |
JP3462650B2 (en) | Resist exposure method and method of manufacturing semiconductor integrated circuit device | |
JPH09204035A (en) | Phase shift mask and its production | |
JP7507100B2 (en) | Photomask, photomask manufacturing method, and display device manufacturing method | |
JPH0345951A (en) | Exposure mask, production of exposure mask, and exposing method using it | |
TW472172B (en) | Method to repair the attenuated phase shift mask by optical proximity effect correction technology | |
US20040013948A1 (en) | Chromeless PSM with chrome assistant feature | |
KR0151228B1 (en) | Photomask for preparing resist pattern | |
JPH0511433A (en) | Production of photomask and photomask | |
JPH04268556A (en) | Formation of resist pattern | |
JPH0829963A (en) | Half tone type phase shift mask and resist light exposure method | |
JP2624335B2 (en) | Resist exposure method |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MM4A | Annulment or lapse of patent due to non-payment of fees |