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TW200414183A - Method of manufacturing original disk for optical disks, and method of manufacturing optical disk - Google Patents

Method of manufacturing original disk for optical disks, and method of manufacturing optical disk Download PDF

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TW200414183A
TW200414183A TW92127431A TW92127431A TW200414183A TW 200414183 A TW200414183 A TW 200414183A TW 92127431 A TW92127431 A TW 92127431A TW 92127431 A TW92127431 A TW 92127431A TW 200414183 A TW200414183 A TW 200414183A
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manufacturing
disc
photoresist
exposure
photoresist layer
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TW92127431A
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Chinese (zh)
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TWI243372B (en
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Akira Kouchiyama
Katsuhisa Aratani
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Sony Corp
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Abstract

The present invention provides a method of producing an optical disk-use original and a method of producing an optical disk, capable of realizing the higher storage capacity of an optical disk by using an existing exposure system. The present invention is characterized in using an original formed with a specified uneven pattern that is formed by forming on a substrate a resist layer consisting of a resist material containing the imperfect oxide of a transition metal such as W and Mo, the imperfect oxide having an oxygen content smaller than that of a stoichiometric composition according to a valency capable of being possessed by the transition metal, and then by selectively exposing and developing the resist layer by a laser beam in conformity with a recording signal pattern, the uneven pattern then being transferred onto the optical disk.

Description

183 玫、發明說明: 【發明所屬之技術領域】 及使用 本發明有關於高精度之光碟用原盤之製造方法 5亥原盤之光碟之製造方法。 【先技術】 先引。己錄保存各種貢訊之記錄媒體之開發非常顯著, 特別是關於小型之記錄媒體,在記錄方式由磁記錄媒體朝 一彔媒體移轉之同時,s己錄容量之增大則由MB(Mega 恥化:兆位元)級朝GB(GigaByte :千兆位元)級進展。 近年,光記錄媒體中,由小型碟片(CD)(登錄商標)朝光 ,之移轉亦進展,出現直徑12cm之唯讀光碟之 單面具有4.7GB容量者。藉此,可進行彩色標準方式(ntsc) 之2小時之影像記錄。 然而,伴隨近年之資訊通信及圖像處理技術之急速發 展,達成將記錄容量提升至現在之數倍亦於上述之光碟中 成為課題。例如:位於數位式影音光碟之延長線上之次世 代光碟係破要求使直徑12 cm之光碟之單面具有25 gb之資 訊容量。此為可記錄2小時程度之數位高晝質方式之影像的 位準。 上述光碟係具有於聚碳酸酯等光學上透明之基板之一主 面上,形成表示資訊信號之凹坑(Pit)或溝槽(Gr〇〇ve)等微細 之凹凸圖案,於其上形成鋁等金屬薄膜所組成之反射膜, 並進一步於該反射膜上形成保護膜之構造。 於此種構造之記錄媒體,可藉由使上述凹凸圖案更微細183. Description of the invention: [Technical field to which the invention belongs] and uses The present invention relates to a method for manufacturing a high-precision optical disc original disc. [Prior technology] First cited. The development of recorded media for all kinds of tribute is very significant, especially for small-sized recording media, while the recording method is being transferred from magnetic recording media to a mass of media, the increase in the recording capacity of s is recorded by MB (Mega shame (Megabit) level towards GB (GigaByte: Gigabit) level. In recent years, in the optical recording medium, the migration from compact discs (registered trademarks) toward light has also progressed, and 12-cm diameter read-only discs have a capacity of 4.7 GB on one side. This allows 2 hours of image recording in color standard mode (ntsc). However, with the rapid development of information communication and image processing technology in recent years, achieving several times the current recording capacity has become a problem in the above-mentioned optical discs. For example, the next generation of optical discs located on the extension line of digital video discs requires a single disc with a diameter of 12 cm to have a data capacity of 25 gb. This is the level at which digital high-day quality images can be recorded for about 2 hours. The above-mentioned optical disc has a fine uneven pattern such as a pit (Pit) or a groove (Groove) representing an information signal on one main surface of an optically transparent substrate such as polycarbonate, and aluminum is formed thereon. And a reflective film composed of a metal thin film, and further forming a protective film structure on the reflective film. In such a recording medium, the above-mentioned uneven pattern can be made finer.

O:\87\87377.DOC -6- 200414183 化,以增加記錄密度,進而達成記錄容量之增大。在此, 以下苓考圖10,說明有關此光碟之凹凸圖案之微細化之光 碟之製程。 、’先於基板90上,均一地形成光阻層91 (圖1 〇(a))。 其次,於光阻層91施加對應信號圖案之選擇性曝光,使 其感光(圖10(b)),藉由顯影光阻層91,獲得形成特定之凹 凸圖案之原盤92(圖l〇(c))。關於此原盤之製作,以下係表 示先前以來所進行之方法之一例。 使用表面充分平滑之玻璃基板作為基板,將該基板載置 於旋轉基台,使玻璃基板在以特定之旋轉數旋轉之狀態 下,供給感光性之光阻(有機光阻)至玻璃基板上而塗佈。其 次,使玻璃基板旋轉而延伸光阻,全面旋轉塗佈而形成光 阻層。其次,藉由記錄用雷射光,曝光光阻為特定之圖案, 形成對應貧訊信號之潛像。其次,以顯影液將此顯影,除 去曝光部或未曝光部。藉此,於玻璃基板上獲得光阻形成 特定之凹凸圖案所構成之光阻原盤。 其次,藉由電鑄法,使光阻原盤92之凹凸圖案面上析出 金屬鎳膜(圖10(d)),使此由光阻原盤92剝離後,施加特定 之加工,獲得光阻原盤92之凹凸圖案所轉印之成型用沖壓 模 93(圖 10(e))。 使用該成型用沖壓模93,藉由射出成型法成型熱塑性樹 脂之聚碳酸酯所組成之樹脂製碟片基板94(圖10(f))。其 次,剝離沖壓模(圖10(g》,藉由於該樹脂製碟片基板料之 凹凸面成膜A1合金之反射膜95(圖10(h))及保護膜%而獲得O: \ 87 \ 87377.DOC -6- 200414183 to increase the recording density and thus increase the recording capacity. Here, FIG. 10 will be described below to explain the manufacturing process of the optical disc with the miniaturization of the concave-convex pattern of the optical disc. First, a photoresist layer 91 is uniformly formed on the substrate 90 (FIG. 10 (a)). Next, a selective exposure corresponding to the signal pattern is applied to the photoresist layer 91 to make it photosensitive (FIG. 10 (b)). By developing the photoresist layer 91, an original disc 92 (FIG. 10 (c )). Regarding the production of this master disk, the following is an example of the method performed previously. A glass substrate with a sufficiently smooth surface is used as a substrate, and the substrate is placed on a rotating base, so that the glass substrate is rotated at a specific rotation number, and a photosensitive photoresist (organic photoresist) is supplied onto the glass substrate. Coated. Next, the glass substrate is rotated to extend the photoresist, and the entire surface is spin-coated to form a photoresist layer. Secondly, by using the laser light for recording, the exposure photoresist has a specific pattern to form a latent image corresponding to the lean signal. Next, this is developed with a developing solution to remove the exposed or unexposed portions. Thereby, a photoresist master made of a specific uneven pattern formed by photoresist is obtained on a glass substrate. Next, a metal nickel film is deposited on the concave-convex pattern surface of the photoresist master disk 92 by the electroforming method (FIG. 10 (d)), and after the photoresist master disk 92 is peeled off, a specific process is applied to obtain the photoresist master disk 92. The stamping die 93 for molding to which the uneven pattern is transferred (FIG. 10 (e)). Using this molding die 93, a resin-made disc substrate 94 made of polycarbonate made of thermoplastic resin is molded by injection molding (Fig. 10 (f)). Next, the stamping die (Fig. 10 (g)) was obtained by forming a reflective film 95 (Fig. 10 (h)) and a protective film% of the A1 alloy film formed on the uneven surface of the resin-made disc substrate material.

O:\87\87377.DOC 200414183 光碟(圖10(i))。 如此,光碟之微細凹凸圖案係藉由經過使用高精度形' 微細凹凸圖案之沖壓模’於基板上忠實且即刻複製:圖1 之製程而製作者,進一步追溯的話,其係按照藉由雷射= 於光阻層進行曝光而形成潛像,亦即藉由切割如何形成^ 細之凹凸圖案而決定。 例如:於先前所述之資訊容量4 7GB之唯讀 (DVD-ROM),於沖壓模上使最短凹坑長〇4 μηι、執道間隔 0.74 μπι之凹坑行成為螺旋狀而施加切割。該切割中係使= 波長413 mn之雷射,數值孔徑!^為〇9〇前後(例如: 之物鏡。 而,若將光源之波長設為;I (μιη),物鏡之數值孔徑設為 να,則被曝光之最短凹坑長Ρ(μιη)係以下式(丨)表示。再者: Κ為比例常數。 ρ= Κ · λ /ΝΑ …(1) 在此,光源之波長λ、物鏡之數值孔徑ΝΑ係按照成為光 原之雷射裝置之樣式而決定之項目,比例常數尺係以雷射裝 置及光阻原盤之組合所決定之項目。 於製作前述資訊容量4.7GB之光碟之情況,由於波長為 〇·413μπι、數值孔徑ΝΑ為0.90、最短凹坑長為〇4〇pm,故 根據上述式(1),比例常數Κ = 〇. 8 7。 相對於此’為了回應上述25 GB之光碟之要求,必須將最 短凹坑長微細化至0·17 μπι,執道間隔微細化至〇·32 程 度0O: \ 87 \ 87377.DOC 200414183 disc (Figure 10 (i)). In this way, the micro-embossed pattern of the optical disc is faithfully and instantly copied on the substrate by using a high-precision 'micro-embossed pattern stamping die': the process of Figure 1 was produced by the producer, and if traced further, it is based on the use of laser = Latent image is formed by exposure to the photoresist layer, that is, determined by cutting how to form a ^ fine uneven pattern. For example, in the previously described DVD-ROM with an information capacity of 4 7GB, the shortest pits with a length of 0.4 μηι and a track interval of 0.74 μπm are formed in a spiral shape on the stamping die to apply cutting. In this cutting, a laser with a wavelength of 413 mn is used, and the numerical aperture! ^ Is around 0.90 (for example, an objective lens. If the wavelength of the light source is set to; I (μιη), the numerical aperture of the objective lens is set to να , The shortest pit length P (μιη) that is exposed is represented by the following formula (丨). Furthermore: κ is a proportionality constant. Ρ = κ · λ / NA… (1) Here, the wavelength λ of the light source, and the length of the objective lens The numerical aperture NA is an item determined according to the style of the laser device that becomes the light source, and the proportionality constant rule is an item determined by the combination of the laser device and the photoresist master disk. In the case of making the aforementioned 4.7GB optical disc, Since the wavelength is 0.413 μm, the numerical aperture NA is 0.90, and the shortest pit length is 0.40 pm, according to the above formula (1), the proportionality constant K = 0.8 8. In contrast, in order to respond to the above 25 GB For the requirements of optical discs, the shortest pit length must be miniaturized to 0 · 17 μπι, and the interval between tracks must be miniaturized to a degree of 0.32.

O:\87\87377.DOC 200414183 一般而言,先前所述之凹凸圖案之微細化(極微細凹坑之 形成)藉由雷射波長之短波長化達成係被視為有效。亦即' 為了獲得單面25 GB之高密度光碟所要求之最短凹坑長 〇·17 μηι程度,於比例常數κ=〇·87、數值孔徑1^八=〇95之 情況’必須有雷射波長λ = 〇 ·丨8 μιη之光源。 在此所必要之波長〇 · 1 8 μηι比作為次世代半導體微影用 光源而開發之波長193nmiArF雷射之波長短。實現此種短 波長之曝光裝置不僅是成為光源之雷射,連透鏡等光學零 件亦需要特殊者,價格非常高昂。亦即’ #由曝光波長又 之短波長化及物鏡之數值孔徑NA之大口徑化,提升光學解 像度以對應極微細加工之手法係隨著微細化之進展,無法 使用既存之曝光裝置,反而不得不導入昂貴的曝光裝置, 故極不適於達成廉價提供㈣之目的。故,藉由曝光裝置 中之雷射裝置之高機能化’以增大光碟之記憶容量係存在 極限。 〜卞/久八7TG r且寻3 機光阻、及作為曝光源之紫外線之曝光方法一般廣受# ^。有機先阻具有泛用性,於微影之領域廣受使用,然而 由^子量高而造成曝光部與未曝光部之 明瞭,對應25GB位準之高 丨間案耳 面的問題。 里先碟之镟細加工係具有精茂 相對於此,無機光阻 小構造單位為原子位準 部之境界部明瞭的圖案 ,特別是非晶矽無機光阻係由於最 之大小,故可獲得曝光部與未曝光 ’相較於有機光阻,可進行高精度O: \ 87 \ 87377.DOC 200414183 In general, the miniaturization of the uneven pattern (formation of extremely fine pits) described earlier is achieved by shortening the wavelength of the laser wavelength. That is, 'in order to obtain the shortest pit length of 1.7 μm required for a single-sided 25 GB high-density optical disc, a laser must be used in the case of a proportionality constant κ = 0.87 and a numerical aperture of 1 ^ 8 = 0095'. Light source with a wavelength of λ = 〇 · 丨 8 μιη. The wavelength required here is 0.18 μm, which is shorter than the wavelength of 193 nmiArF laser developed as a light source for next-generation semiconductor lithography. Realizing such a short-wavelength exposure device is not only a laser for a light source, but also optical components such as lenses require special ones, which are very expensive. In other words, the number of exposure wavelengths and short wavelengths and the numerical aperture NA of the objective lens have been increased to increase the optical resolution to correspond to the ultra-fine processing. With the progress of miniaturization, it is not possible to use the existing exposure device. Since an expensive exposure device is not introduced, it is extremely unsuitable to achieve the purpose of providing a low cost. Therefore, there is a limit to increase the memory capacity of the optical disc by increasing the function of the laser device in the exposure device. ~ 卞 / 久 八 7TG r and 3 camera photoresistance, and the exposure method of ultraviolet light as an exposure source is generally widely accepted. Organic pre-resistance is universal, and is widely used in the field of lithography. However, the exposed part and the unexposed part are clear due to the high volume, which corresponds to the earphone problem at the high level of 25GB. In contrast, the fine processing system of the Lixian disc has a fine pattern. In contrast, the small structure of the inorganic photoresist has a clear pattern at the boundary portion of the atomic level. In particular, the inorganic photoresist of the amorphous silicon can obtain exposure because of its largest size. And unexposed 'compared with organic photoresist, it can achieve high precision

O:\87\87377.DOC 200414183 之微細加工,被認為有希望適用於高容量光碟。此係有使 用Mo〇3或W〇3等作為光阻材料,使用離子束作為曝光源之 禮支、細力口 工合J (參考合1J 士口 : Nobuyoshi Koshida, KazuyoshiO: \ 87 \ 87377.DOC 200414183 is considered to be suitable for high-capacity optical discs. This system is provided with MoO3 or W03 as photoresist materials, and ion beams as exposure sources. Gonghe J (Reference 1J Shikou: Nobuyoshi Koshida, Kazuyoshi

Yoshida, Shinichi Watanuki, Masanori Komuro and Nobufumi Atoda ' ff50-nm Metal Line Fabrication by Focused Ion Beam and Oxide Resists(以聚焦式離子束及氧化光阻製 作 50-nm 金屬導線)’·,Jpn· J· Appl. Phys. Vol· 30 (1991)Yoshida, Shinichi Watanuki, Masanori Komuro and Nobufumi Atoda 'ff50-nm Metal Line Fabrication by Focused Ion Beam and Oxide Resists' ·, Jpn · J · Appl. Phys. Vol. 30 (1991)

ρρ3 246。)。又,有使用Si02作為光阻材料,使用電子束作 為曝光源之加工例(參考例如·· Sucheta M· Gorwadkar,ρρ3 246. ). In addition, there is a processing example using SiO 2 as a photoresist material and using an electron beam as an exposure source (refer to, for example, Sucheta M Gorwadkar,

Toshimi Wada? Satoshi Hiraichi, Hiroshi Hiroshima, Kenichi Ishii and Masanori Komuro · f,Si02/c-Si BilayerToshimi Wada? Satoshi Hiraichi, Hiroshi Hiroshima, Kenichi Ishii and Masanori Komuro · f, Si02 / c-Si Bilayer

Electron-Beam Resist Process for Nano-Fabrication(奈米製 作之Si〇2/c-Si雙層電子束光阻製程),Jpn. J· Appl· Phys· Vol. 35 (1996) pp6673)。甚而,亦檢討使用硫硒碲玻璃作為光阻 材料,使用波長476 nm及波長532 nm之雷射及來自水銀氙 燈之紫外光作為曝光源之方法(參考例如·· S· A· Kostyukevych : "Investigations and modelling of physical processes in inorganic resists for the use in UV and laser lithography(用 於uv及雷射微影之無機光阻之物理過程之調查及模型r, SPIE Vol. 3424 (1998) pp20。)。 然而,使用離子束或電子束作為曝光源之情況,可組合 如上述之多種類之無機光阻材料,藉由細窄會眾電子束或 離子束,亦可將凹凸圖案微細化,然而,搭載電子束及離 子束照射源之裝置之構造複雜,並且極為昂貴,故不適於 O:\87\87377 DOC -10- 廉價光碟之供給。 關於該點,,、,, 可利用搭载於既存之暖 一 寻之先,亦即紫外線或可 田耵衣置 中旎以紫外線或 …機先阻材科 右炉成泣 先刀。彳之材料有限,至今之報主中僅 爪碲材料。此乃因為紫外線 。 以外之無機光阻材料丄 策次了視先透過硫碼碲材料 所致。 ’先能量之吸收明顯少,不具實用性 既存之曝光裝置與硫硒蹄 之袓人呷诃抖之組合在經濟面上為實用 ,硫场蹄材料具有Electron-Beam Resist Process for Nano-Fabrication (Si〇2 / c-Si double-layer electron beam photoresistance process), Jpn. J. Appl. Phys. Vol. 35 (1996) pp6673). Furthermore, the method of using selenium-selenium-tellurium glass as a photoresist material, using lasers with a wavelength of 476 nm and a wavelength of 532 nm, and ultraviolet light from a mercury-xenon lamp as an exposure source is also reviewed (refer to, for example, ······ Kostyukevych: " Investigations and modelling of physical processes in inorganic resists for the use in UV and laser lithography (SPIE Vol. 3424 (1998) pp20.). However, in the case of using an ion beam or an electron beam as an exposure source, various types of inorganic photoresist materials can be combined, and the concavo-convex pattern can be miniaturized by narrowing congregation electron beams or ion beams. Beam and ion beam irradiation source devices have complicated structures and are extremely expensive, so they are not suitable for the supply of O: \ 87 \ 87377 DOC -10- cheap discs. Regarding this point, you can use the existing heaters. The first to find, that is, the ultraviolet or keratin clothes are placed in the center. The ultraviolet or the machine first resists the material into the right furnace to become the first knife. The material of 彳 is limited. Materials. This is because of ultraviolet rays. Inorganic photoresist materials other than inorganic light-resistance materials are considered to pass through sulfur-coded tellurium materials. 'The absorption of energy is significantly less, and the existing exposure device and sulfur-selenium hoof are not practical. The combination of trembling is practical in economic terms. The sulfur field hoof material has

Ag2Se-GeSe 等對 gAs2S3、 . 哥耵人“害之材料之問題點,由工 硯點考量係難以使用。 ” 、 釺ΓΓ上所述,至今尚未實現藉由既存之曝光裝置之高記 錄谷3:之光碟之製造。 本’:明係為了解決此種先前之問題點而提案者,其目的 者提^不使用電子束或離子束等昂貴之照射裝置,而使 用實現高精度之微細加工之安全 <文王爻九阻材料,利用既存之 曝光裝置,可實現弁;隹 ^ _ 貝現九碟之進一步之高記憶容量化之光碟用 原盤之製造方法及光碟之製造方法。 、 【發明内容】 如上所述,先前以來係使用厘0〇3或评〇3等過渡金屬之完 全匕减物作為電子束或離子束用之光阻材料,&等之對於 紫外線或可視光為透明,吸收明顯很小,故難以進行以紫 外線或可視光作為曝光源之微細加工。 相對於此,本發明者等檢討之結果發現,只要氧含有量Ag2Se-GeSe, etc. on gAs2S3,. "The problem of harmful materials is difficult to use from the point of view of work." As mentioned above, 所述 ΓΓ has not yet achieved the high record valley 3 with the existing exposure device. : Manufacture of optical discs. Ben ': The author proposed to solve this kind of previous problems, and its purpose was to propose the safety of micromachining with high precision without using expensive irradiation equipment such as electron beam or ion beam. Resist material, using the existing exposure device, can realize 弁; 隹 _ _ _ _ _ _ _ _ _ _ _ _ _ is now a nine-disc further high memory capacity of the original disc manufacturing method and optical disc manufacturing method. [Summary of the Invention] As mentioned above, previously, a complete reduction of a transition metal such as 0.30 or 0.33 has been used as a photoresist material for electron beam or ion beam, and for UV or visible light, etc. Because it is transparent and its absorption is obviously small, it is difficult to perform microfabrication using ultraviolet or visible light as an exposure source. In contrast, as a result of a review by the inventors, it was found that as long as the oxygen content

O:\87\87377.DOC -11 - 200414183 從過渡金屬氧化物之化學計量組成稍微偏離,此氧化物對 於紫外線或可視光之吸收會突然變大,同時藉由吸收紫外 線或可視光,其化學性f變化,可應用於光阻材料及光 用原盤之製造方法。亦’藉此,上述式⑴之比例常數κ 改善’可達成減低最短凹坑長ρ。 本發明之光碟用原盤..之製造方法係根據上述酌見而設計 者,其特徵在於:於基板上成膜含有過渡金屬之不完:氧 化物,且該不完全氧化物之氧之含有量比按照前述過渡金 屬之可抓j貝數之化學計量組成之氧含有量小之光阻材料所 組成之光阻層後’使該光阻層對應記錄用信號圖案選擇性 曝光、顯影而形成特定之凹凸圖案。 又,本發明之光碟之製造方法^其特徵在於:於基板上 成膜含有過渡金屬之不6入备 离之不兀全虱化物,且該不完全氧化物之 氧之含有量比按照前述過渡金屬之價數之化學計量組成之 氧含有量小之光阻材料所組成之光阻層後,使用使該光阻 層對應§己錄用信號圖案選擇性曝光、顯影而形成特定之凹 凸圖案之原盤,製作該凹凸圖案所轉印之碟片。 在此所謂過渡金屬之不完全氧化物係定義為:朝氧含有 =比=過渡金屬之可採價數之化學計量組成少之方向偏 離之化合物,亦即過渡金屬之不完全氧化物之氧之含有量 比按照上述過渡金屬 之化合物。 、數之化于f且成之氧含有物少 再者’含有複數種類之過渡金屬之情況,有結晶構造U 種過渡金屬原子之—部分可能被其他過渡金屬原子置換,O: \ 87 \ 87377.DOC -11-200414183 Slightly deviates from the stoichiometric composition of the transition metal oxide. This oxide's absorption of ultraviolet or visible light will suddenly increase. At the same time, by absorbing ultraviolet or visible light, its chemical The change in property f can be applied to the manufacturing methods of photoresist materials and optical masters. Also 'by this, the improvement of the proportional constant κ of the above formula (i)' can reduce the shortest pit length ρ. The manufacturing method of the original disc for optical discs of the present invention is designed based on the above considerations, and is characterized in that a film containing transition metal incomplete: oxide is formed on the substrate, and the oxygen content of the incomplete oxide is contained A photoresist layer composed of a photoresist material having a smaller oxygen content than the stoichiometric composition of the transition metal according to the aforementioned transition metal can be used to selectively expose and develop the photoresist layer corresponding to the signal pattern for recording to form a specific photoresist layer. Bump pattern. In addition, the manufacturing method of the optical disc according to the present invention is characterized in that a non-single lice compound containing a transition metal is formed on a substrate, and the oxygen content ratio of the incomplete oxide is in accordance with the transition described above. After the photoresist layer composed of a photoresist material with a small stoichiometric composition of metal and oxygen content is used, the photoresist layer is used to selectively expose and develop the signal pattern corresponding to the recorded signal pattern in § to form the original disc with a specific uneven pattern. , Making a disc transferred with the uneven pattern. The so-called incomplete oxide of a transition metal is defined herein as a compound that deviates in a direction that contains less oxygen than the stoichiometric composition of the recoverable valence of the transition metal, that is, the oxygen of the incomplete oxide of the transition metal. The content ratio is based on the compound of the transition metal described above. The number is reduced to f and the oxygen content is small. Furthermore, when there are multiple types of transition metals, there are crystal transition structures of U transition metal atoms—part of them may be replaced by other transition metal atoms.

O:\87\87377.DOC -12- 200414183 …、而,以氧含有量對於此等複數種類之過渡 ^ 學言十晉相士 θ 又金屬之可採化 、、且成疋否足夠,來判斷是否為不完全氧化物 , 對材料所使用之過渡金屬之不完全氧化物係 ,外線或可視光顯示出吸收’故不使用電子束或離子 束寻特殊曝光源而可進行曝光。又,過渡 =低分子,故相較於高分子所組成之有機光= 可:::二:之境界明瞭,故藉由使用此作為光阻材料, 了 3又侍回精度之光阻圖案。 【實施方式】 χ下參考圖式詳細說明本發明《光碟之製造一 實施型態。 以下’根據圖1說明關於適用本發明之光碟之製造方 製程之概要。 首先,於基板100上,藉由賤射法均一成臈特定之益機率 先阻材料所組成之光阻層1G2(光阻層形成卫序、圖 適用於光阻層1G2之材料之心待後述。又,為了改盖光阻 之曝光感度,亦可於基板1〇〇與光阻層1〇2之間形成特 疋之中間層101。圖1(a)係表示其狀態。再者,光阻層1〇2 之膜厚可任意設定’然而’在1〇〜8〇胆之範圍内為佳。 其次,利用具備既存之雷射裝置之曝光裝置,於光阻声 1〇2施加制信號圖案之選擇性曝光,使其感光(光阻層: 光工序圖1(b))。甚而,藉由顯影光阻層1〇2,獲得形成特 疋之凹凸圖案之原盤103(光阻層顯影工序、圖⑽)。 其次,藉由電鑄法,於原盤1〇3之凹凸圖案面上析出金屬O: \ 87 \ 87377.DOC -12- 200414183…, and the transition of these plural types with oxygen content ^ Doctrine 10 Jin Xiangshi θ and the metal can be mined, and is it enough? Judge whether it is an incomplete oxide. For the incomplete oxide system of the transition metal used in the material, external lines or visible light show absorption. Therefore, exposure can be performed without using an electron beam or ion beam to find a special exposure source. In addition, the transition = low-molecule, so compared to the organic light composed of high-molecular = can be ::: 2 :: The realm is clear, so by using this as a photoresist material, the photoresist pattern with 3 accuracy is returned. [Embodiment] The following describes in detail the "manufacturing of an optical disc according to the present invention" with reference to the drawings. Hereinafter, the outline of the manufacturing process of the optical disc to which the present invention is applied will be described with reference to FIG. First of all, on the substrate 100, a photoresist layer 1G2 composed of a first resistive material is uniformly formed by a low-intensity shot method. (The photoresist layer forms a guard order, and the figure shows the material suitable for the photoresist layer 1G2. In addition, in order to change the exposure sensitivity of the photoresist, a special intermediate layer 101 may be formed between the substrate 100 and the photoresist layer 102. Fig. 1 (a) shows the state. Furthermore, light The film thickness of the resist layer 10 can be arbitrarily set. However, it is better to be within the range of 10 to 80 g. Second, using an exposure device with an existing laser device, a signal is applied to the photoresistor 102. Selective exposure of the pattern to make it photosensitive (photoresist layer: photo process diagram 1 (b)). Furthermore, by developing the photoresist layer 102, a master 103 (photoresist layer development) forming a special uneven pattern is obtained. Process, figure ⑽) Next, metal is deposited on the uneven pattern surface of the original plate 103 by the electroforming method.

O:\87\87377.DOC -13- 200414183 鎳膜(圖1(d)),將此由原盤103剝離後,施加特定之加工, 獲得原盤103之凹凸圖案所轉印之成型用沖壓模1〇4(圖 1(e))。 使用該成型用沖壓模丨〇 4,藉由射出成型法成型熱塑性樹 脂之聚碳酸酯所組成之樹脂製碟片基板1〇5(圖1(f))。其 -人,剝離沖壓模(圖1 (g》,藉由於該樹脂製碟片基板之凹凸 面成膜A1合金等之反射膜ι〇6(圖1(h))及膜厚〇1 mm程度之 保護膜107而獲得光碟(圖1(1))。再者,以上由光阻原盤獲 得光碟為止之工序以先前習知之技術製造即可。 光阻材料 適用於上述光阻層1〇2之光阻材料為過渡金屬之不完全 虱化物。在此,過渡金屬之不完全氧化物係定義為:氧含 有量朝比按照過渡金屬之可採價數之化學計量組成少之方 向偏離之化合物,亦即過渡金屬之不完全氧化物之氧之含 有里比按照上述過渡金屬之價數之可採化學計量組成之氧 含有物少之化合物。 例如·舉例化學式M〇〇3作為過渡金屬之氧化物而進行說 明。若將化學式MQ〇3之氧化狀態換算為組成比例MQix〇x, 相對於X — 0.75之情況為完全氧化物,以〇<χ<〇·75表示之 I*月况可況為氧含有量比化學計量組成不足之不完全氧化 物。 又,過渡金屬中,亦有丨個元素可形成價數相異之氧化物 者,然而,於此種情況,本發明之範圍内係指實際之氧含 有里比按照過渡金屬之可採價數之化學計量組成不足之情O: \ 87 \ 87377.DOC -13- 200414183 Nickel film (Figure 1 (d)). After peeling this from the original plate 103, a specific process is applied to obtain the stamping die for molding 1 transferred from the uneven pattern of the original plate 103 〇4 (Figure 1 (e)). Using this stamping die for molding, a resin-made disc substrate 105 made of polycarbonate made of a thermoplastic resin by injection molding was molded (Fig. 1 (f)). It is a person, peeling the stamping die (Fig. 1 (g), and forming a reflective film such as A1 alloy, etc. (Fig. 1 (h)) and a film thickness of about 0.1 mm due to the uneven surface of the resin-made disc substrate. The protective film 107 is used to obtain an optical disc (Fig. 1 (1)). In addition, the above steps until the optical disc is obtained from a photoresist original disc can be manufactured by a conventional technique. The photoresist material is suitable for the above photoresist layer 10.2. Photoresistive materials are incomplete liceates of transition metals. Here, incomplete oxides of transition metals are defined as compounds whose oxygen content deviates in a direction that is less than the stoichiometric composition of the transition metal based on its recoverable valence, That is, compounds containing oxygen in the incomplete oxides of transition metals that contain less oxygen than the oxygen content of the recoverable stoichiometric composition according to the valence of the transition metals described above. For example: Example: Chemical formula M03 as a transition metal oxide For explanation, if the oxidation state of the chemical formula MQ〇3 is converted to the composition ratio MQix〇x, it is a complete oxide with respect to the case of X-0.75, and the I * monthly condition expressed by 〇 < χ < 〇.75 is available. The oxygen content ratio is not the stoichiometric composition Incomplete oxides. In transition metals, there are 丨 elements that can form oxides with different valences. However, in this case, the scope of the present invention means that the actual oxygen contains the liberty in accordance with the transition. Insufficient stoichiometric composition of metal's recoverable value

O:\87\87377 DOC -14- 200414183 〉兄。/列士口 · Λ/f _ • 10細以先前所述之3價之氧化物(Mo〇3)為最安 八他亦存在1價之氧化物(Mo0)。於此種情況若 換t為組成比例Μ0ΐ χ0χ,則〇<χ<〇 ·5之範圍内時,可說為 氧3有里比化學計量組成不足之不完全氧化物。再者,過 度金屬虱化物之價數可以市售之分析裝置分析。 、,此種過渡金屬之不完全氧化物顯示出對於紫外線或可視 光之吸收,因被紫外線或可視光照射,其化學性質變化。 孑細有待後述,然而其結果,雖為無機光阻,但顯影工序 中,曝光部與未曝光部之蝕刻速度產生差異,獲得所謂選 擇^。又,過渡金屬之不完全氧化物所組成之光阻材料由 於膜材料之較小的微粒子大4、,故未曝光部與曝光部之境 界部之圖案明瞭,可提高解析度。 兄 然而,過渡金屬之不完全氧化物因氧化之程度,其作為 光阻材料之特性亦變化,故應適當選擇最適之氧化程度: 例如··氧含有量大幅比過渡金屬之完全氧化物之化學^量 組成少之不完全氧化物,其係伴隨於曝光工序需要大的: 射功率,或者顯影處理需要長時間等不便。因&,以氧: 有量稍微比過渡金屬之完全氧化物之化學計量組成少= 完全氧化物為佳。 構成光阻材料之具體之過渡金屬可舉O: \ 87 \ 87377 DOC -14- 200414183〉 Brother. / 列 士 口 · Λ / f _ • 10 is based on the trivalent oxide (Mo〇3) described previously as the most stable. He also exists monovalent oxide (Mo0). In this case, if t is replaced by the composition ratio M0ΐχ0χ, then within the range of 0 < x < 0.5, it can be said that the oxygen 3 has an incomplete oxide having a lower stoichiometric composition. Furthermore, the value of excessive metal lice can be analyzed by a commercially available analysis device. The incomplete oxide of this transition metal shows absorption of ultraviolet or visible light, and its chemical properties change due to being irradiated by ultraviolet or visible light. The details will be described later. However, as a result, although the photoresist is an inorganic photoresist, in the developing process, the etching speed of the exposed portion and the unexposed portion differs, and a so-called selection ^ is obtained. In addition, since the photoresist material composed of incomplete oxide of transition metal is smaller than the fine particles of the film material, the pattern of the boundary portion between the unexposed portion and the exposed portion is clear, and the resolution can be improved. However, due to the degree of oxidation of incomplete oxides of transition metals, their characteristics as photoresist materials also change. Therefore, the most appropriate degree of oxidation should be appropriately selected: For example, the chemical content of oxygen content is significantly higher than that of complete oxides of transition metals. Incomplete oxides with a small amount of composition are those that require a large amount with the exposure process: the injecting power, or the development process requires a long time and other inconveniences. Because of & oxygen: the amount is slightly less than the stoichiometric composition of the complete oxide of the transition metal = complete oxide is preferred. Specific transition metals constituting the photoresist material can be exemplified.

-、Fe、Nb、CU、Ni、C0、M0、Ta、W、ZrTiR LG 乙r、ru、a等 其中又以使用Mo、W、Cr、Fe、Nb為佳,由 丨土 田刊用紫外線- 可視光可獲得大幅之化學變化之觀點 、、:-, Fe, Nb, CU, Ni, C0, M0, Ta, W, ZrTiR, LG, r, ru, a, etc. Among them, it is better to use Mo, W, Cr, Fe, Nb. Visible light can obtain the viewpoint of large chemical changes ,:

Mo、W為佳。 特別以使〗Mo and W are preferred. Specially

O:\87\87377.DOC -15- 200414183 再者,作為過渡金屬之不完全氧化物,除了丨種過渡金屬 之不完全氧化物以外,添加第二過渡金屬者,甚至添加複 數種類之過渡金屬者,添加過渡金屬以外之其他金屬者等 均包含於本發明之範圍内,特別以含有複數種金屬元素者 為佳。 、 再者,除了 1種過渡金屬之不完全氧化物以外,添加第二 過渡金屬者,甚至添加3種以上之過渡金屬者之情況,有結 晶構造之1種過渡金屬原子之一部分可能被其他過渡金屬ϋ 原子置換,然而,以氧含有量相對於此等複數種類之過渡 金屬之可採化學計量組成是否足夠,來判斷是否為不完全 氧化物。 又,過渡金屬以外之其他元素可使用A1、c、Β、Si、Ge 等中之至少1種。藉由組合2種以上之過渡金屬使用,或者 添加過渡金屬以外之其他元素,由於過渡金屬之不完全氧 化物之結晶粒變小,故曝光部與非曝光部之境界部更佳明 瞭,達成大幅提升解析度之目的,又可改善曝光感度。 再者,上述光阻材料藉由於使用含有特定之過渡金屬之 靶材之Ar +〇2氣氛中之濺射法製作即可。例如:相對於導 入於反應室内之氣體之全流量’ 〇2為5〜2()%,氣體壓為通 常之濺射法之氣體壓(1〜l〇Pa)。 光碟用原盤之製造方法 其次,說明構成上述光碟之製造方法之根本之光碟用原 盤之製造方法之詳細。 作為本發明之光碟用原盤之製造方法之一實施型態,其 O:\87\87377.DOC -16- 係由例如:如上述之 此 ;基板上成膜過渡金屬之不完全41 物所組成之光阻材料 丨…化O: \ 87 \ 87377.DOC -15- 200414183 In addition, as an incomplete oxide of a transition metal, in addition to an incomplete oxide of a transition metal, a second transition metal is added, or even a plurality of types of transition metals are added. Those metals other than transition metals are included in the scope of the present invention, and those containing a plurality of metal elements are particularly preferred. In addition, in addition to the incomplete oxide of one transition metal, in the case of adding a second transition metal, or even adding three or more transition metals, a part of one transition metal atom with a crystalline structure may be transitioned by other The metal rhenium is replaced by an atom. However, whether the oxygen content is sufficient relative to the recoverable stoichiometric composition of these plural kinds of transition metals is sufficient to judge whether it is an incomplete oxide. For other elements other than the transition metal, at least one of A1, c, B, Si, and Ge can be used. By combining two or more kinds of transition metals or adding other elements than the transition metals, the crystal grains of the incomplete oxides of the transition metals become smaller, so the boundary between the exposed and non-exposed parts is better and clearer, achieving a large The purpose of improving the resolution can also improve the exposure sensitivity. In addition, the above-mentioned photoresist material can be produced by a sputtering method in an Ar + 02 atmosphere using a target material containing a specific transition metal. For example: Relative to the total flow of gas introduced into the reaction chamber '〇2 is 5 ~ 2 ()%, and the gas pressure is the gas pressure (1 ~ 10Pa) of the usual sputtering method. Manufacturing method of optical disc master Next, a detailed description will be given of a manufacturing method of the optical disc master which constitutes the fundamental method of manufacturing the optical disc. As one embodiment of the manufacturing method of the original disc for optical discs of the present invention, its O: \ 87 \ 87377.DOC -16- is composed of, for example, as described above; an incomplete 41 of the transition metal formed on the substrate Photoresist material 丨 ...

取尤阻層之工序;於光阻M 性曝光而感光之工序丄 尤I且層遥擇 之凹&圖^ “ _光阻層’製造形成特定 細。"’、皿之工序所構成者。以下說明各工序之詳 光阻層形成工序 百先於表面充分平滑之基板上,成膜過渡金屬之不完 全乳化物所組成之光阻層。具體之成膜方法可舉例··使用 錢金屬之單體社成之,於氬或氧氣氛中藉由 錢射法而進行成膜之方法。 々 ^ 此禋憬況中,藉由改變真空氣 氛中之氧氣體濃度,可控制過渡金屬之不完全氧化物之氧 化程度。藉由賤射法成膜含有2種類以上之過渡金屬之過渡 金屬之不完全氧化物之情況,藉由於相異種類之濺射靶J 上使基板經常旋轉,而使複數種類之過渡金屬混合。混合 比例係藉由改變分別之濺射投入功率而控制。 口 、又,,了先前所述之使用金屬乾材之氧氣氛中之機射法 二外,藉由使用預先含有期望量之氧之過渡金屬之不完全 氧化物所組成之乾材’於通常之氬氣氛中進行賤射法,亦 可同樣成膜過渡金屬之不完全氧化物所組成之光阻層。 甚而,濺射法以外,藉由蒸鍍法亦可容易成膜過渡金屬 之不完全氧化物所組成之光阻層。 基板可使用玻璃、聚碳酸酯等塑膠、矽、氧化鋁碳化鈦、 鎳等。 光阻層之膜厚可任意設定,例如:可設定在10〜8〇11111之 O:\87\87377.DOC -17- 200414183 範圍内。 光阻層曝光工序 其次,將光阻層之成膜結束之基板(以下稱為光阻基板1) 以光阻成膜面配置於上側而安裝於圖2所示之曝光裝置之 旋轉台11。 此曝光裝置係設置曝光光阻層之例如:發生雷射光之光 束發生源12,並具有藉此產生之雷射光通過準直透鏡π、 光束分波器14、及物鏡15而聚焦於光阻基板1之光阻層並照 射之構成。又,此曝光裝置具有將來自光阻基板1之反射 光’經由光束分波器14及聚光物鏡16,連結至分割光感測 為17上之構成。分割光感測器17檢出來自光阻基板1之反射 光’形成由此檢出結果所獲得之聚焦誤差信號丨8,並傳送 主聚焦致動器19。聚焦致動器19係進行物鏡15之高度方向 之位置控制者。於旋轉台Η設置移送機構(省略圖式),能以 良好精度改變光阻基板1之曝光位置。又,於此曝光裝置, 雷射驅動電路23係根據資料信號20、反射光量信號21、及 循執誤差信號22,一面控制光束發生源12,一面進行曝光 或聚焦。甚而,於旋轉台丨丨之中心軸設置主軸馬達控制系 、’’充24,根據光學系統之半徑位置及期望之線速度,設定最 適之主軸旋轉數,進行主軸馬達之控制。 先岫之對於有機光阻所組成之光阻層之曝光工序中,並 未於曝光之光源本身,&光阻層進行聚焦。此乃由於 有機光阻之曝光對於化學性f之變化為連續性,故即使為 水焦所必要程度之微弱&,因該光之照射,於有機材料所The process of taking the special resist layer; the process of exposing and photosensitizing the photoresist, especially the concave of the layer I & Figure ^ "_Photoresist layer 'is made into a specific thin." The following explains the detailed process of forming the photoresist layer in each step. A photoresist layer composed of an incomplete emulsion of a transition metal is formed on a substrate with a sufficiently smooth surface. The specific film formation method can be exemplified by using money. The single metal is formed by the method of film formation in the argon or oxygen atmosphere by coinjection method. 々 ^ In this situation, the transition metal can be controlled by changing the oxygen gas concentration in the vacuum atmosphere. Degree of oxidation of incomplete oxides. In the case of forming incomplete oxides of transition metals containing two or more types of transition metals by the low-level shot method, the substrate is often rotated on the sputtering target J of a different type, and A plurality of kinds of transition metals are mixed. The mixing ratio is controlled by changing the power of each sputtering input. In addition, the mechanical injection method in an oxygen atmosphere using a dry metal material as described above is used. Use pre-containment period A dry material composed of an incomplete oxide of a transition metal in an amount of oxygen is subjected to a low-temperature shot method in a general argon atmosphere, and a photoresist layer composed of an incomplete oxide of a transition metal can also be formed into a film. In addition to the radiation method, a photoresist layer composed of incomplete oxides of transition metals can also be easily formed by evaporation. The substrate can be made of plastic such as glass, polycarbonate, silicon, alumina titanium carbide, nickel, etc. The film thickness of the resist layer can be arbitrarily set, for example, it can be set within the range of O: \ 87 \ 87377.DOC -17- 200414183 of 10 ~ 8011111. The photoresist layer exposure process is followed by the film formation of the photoresist layer. The substrate (hereinafter referred to as the photoresist substrate 1) is arranged on the upper side with a photoresist film-forming surface and is mounted on the rotating table 11 of the exposure device shown in Fig. 2. This exposure device is provided with an exposure photoresist layer, for example: laser light is generated The light beam generating source 12 has a structure in which the laser light generated thereby is focused and irradiated on the photoresist layer of the photoresist substrate 1 through the collimator lens π, the beam splitter 14, and the objective lens 15. Also, this exposure device With reflected light from the photoresist substrate 1 ' The beam splitter 14 and the condenser objective lens 16 are connected to the divided light sensor 17. The divided light sensor 17 detects the reflected light from the photoresist substrate 1 and forms the light obtained from the detection result. The focus error signal is transmitted to the main focus actuator 19. The focus actuator 19 is a position controller for the height direction of the objective lens 15. A transfer mechanism (omitted diagram) is provided on the rotary table, which can be changed with good accuracy. The exposure position of the photoresist substrate 1. In this exposure device, the laser driving circuit 23 is based on the data signal 20, the reflected light amount signal 21, and the compliance error signal 22, while controlling the light beam generating source 12, and performing exposure or focusing. In addition, a spindle motor control system and a 24 are set on the center axis of the rotary table, and the optimal spindle rotation number is set according to the radial position of the optical system and the desired linear speed to control the spindle motor. First, in the exposure process of a photoresist layer composed of an organic photoresist, the light source itself, which is not exposed, & the photoresist layer is focused. This is because the exposure of the organic photoresist is continuous to the change in the chemical f, so even if the necessary degree of water coke is weak &

O:\87\87377.DOC -18- 200414183O: \ 87 \ 87377.DOC -18- 200414183

組成之光阻層將進轩π、,恶> a T 丁不必要之曝光。因此,另外準備有機 光阻不具有感度之波 一 長之光源,例如·波長633 nm之紅色 光源’以該光進行平隹 丄、, 士 τ來焦。如此,先則之有機光阻用之曝光 裝置使用2個不同波長之氺、、原 一 我之光,原因此不付不設置可分離波長 之光學系統,故具有光學系統變成非常複雜,或者其成本 曰力等缺’』4而,先前之有機光阻用之曝光裝置中,由 於用於物鏡之高度位置控制之聚焦誤差信號之解析度係盘 用於檢出之光源(例如:波長633 nm)之波長成比例,故無法 獲得以用於曝光之光源所獲得之解析度,具有無法進行高 精度且安定之聚焦的問題。 相對於此,無機材料之本發明之光阻材料係如圖3之用於 曝光之光源之照射功率,及曝光部與未曝光部之姓刻速度 之差(對比)之關係所示,曝光對於化學性質之變化極為陡 肖亦即,對於未滿曝光開始之照射臨限值功率P0之照射 功率’即使對於重複之照射亦不進行不必要之曝光,故藉 由未滿p〇之照射功率,能以曝光光源本身進行聚焦。因此: 本發明之光碟用原盤之製造方法不需要進行波長分離之光 學系統’從而達成曝光裝置之低成本化,同時實現相當於 曝光波長之高精度之聚焦,可達成正確之微細加工。又, 以未滿照射臨限值功率P0之微弱光,無機光阻之本發明之 1阻材料不致被曝光,故亦不需要使用通常之有機光阻之 製程中所必要之遮斷室内照明之紫外光。 如上述,使用未滿照射臨限值功率P0之光進行聚焦後, 使旋轉台丨丨移動至期望之半徑位置。在此,固定2鏡15等The composition of the photoresist layer will cause unnecessary exposure. Therefore, prepare an organic photoresist that has no sensitivity. A long light source, such as a red light source with a wavelength of 633 nm, is used to focus the light. In this way, the first exposure device for organic photoresist uses two different wavelengths of chirp and original light. Because of this, there is no need to set up an optical system with separable wavelengths, so the optical system becomes very complicated, or its The cost and power are lacking. ”4 In the previous exposure devices for organic photoresistors, the resolution of the focus error signal used for the height and position control of the objective lens was determined by the light source used for detection (for example, a wavelength of 633 nm). ) Is proportional to the wavelength, so the resolution obtained with a light source for exposure cannot be obtained, and there is a problem that high-precision and stable focusing cannot be performed. In contrast, the photoresist material of the present invention of inorganic materials is shown in the relationship between the irradiation power of the light source for exposure and the difference (contrast) between the engraved speed of the exposed and unexposed parts. The change in chemical properties is extremely steep, that is, the irradiation power of the irradiation threshold power P0 for the incomplete exposure start is not performed even for repeated irradiation. Therefore, with the irradiation power of less than p0, Focusing can be performed with the exposure light source itself. Therefore: The manufacturing method of the original disc for optical discs of the present invention does not require a wavelength-separated optical system 'so as to reduce the cost of the exposure device, and at the same time achieve high-precision focusing equivalent to the exposure wavelength, and achieve accurate micro-processing. In addition, the weak light of the threshold power P0 is not fully irradiated, and the 1-resistance material of the present invention of the inorganic photoresist will not be exposed. Therefore, it is not necessary to use the ordinary organic photoresist to block indoor lighting. UV light. As described above, after focusing with light under the irradiation threshold power P0, the rotary stage 丨 丨 is moved to a desired radial position. Here, fixed 2 mirrors, 15 etc.

O:\87\87377 DOC -19- 200414183 之光學系統之面方向之位置,藉由使旋轉⑼移動而改變 光阻基板1之曝光位置’然而,無需贅述,亦可固定載置光 阻基板1之旋轉台11,改變光學系統之位置。 且’由光束發生源12照射雷射光,同時使旋轉旋轉, 對於光阻層進行曝光。此曝光係藉由_面使旋轉台㈣ 轉,-面使旋轉台11朝光阻基板i之半徑方向連續移動些微 距離,以形成微細凹凸之潛像,,亦即記錄用碟片之情況係 形成螺旋狀之導引溝。x,光碟之情況係形成資訊資料用 凹凸凹坑及導引溝之蛇行以作為微細凹凸之潛像。又,製 作磁硬碟等採用同心圓狀之執道之碟片之際,可藉由不是 連縯性,而是逐步移送旋轉台丨i或光學系統而對應。 藉由上述没定,按照資訊資料,將對應於凹坑或導引溝 之照射臨限值功率P0以上之期望之功率之照射脈衝或連續 光,由光阻基板1之期望位置依序照射於光阻層,進行曝 光。照射脈衝之例係表示於圖4A及圖4B,連續光之例係表 示於圖4C。 ' 本發明之過渡金屬之不完全氧化物所組成之光阻材料藉 由照射臨限值功率?〇以上之紫外線或可視光之照射,其化 子丨生貝麦化,對於鹼或酸之蝕刻速度於曝光部及未曝光呷 係相異,亦即可獲得選擇比。 σ 此蚪,使照射功率越低,越可形成短且窄之凹坑,然而, 方使照射功率極端低,由於接近照射臨限值功率,故難以 形成安定之圖案。因此,必須適當設定最適之照射功率而 曝光。O: \ 87 \ 87377 DOC -19- 200414183 The position of the optical system in the face direction changes the exposure position of the photoresistive substrate 1 by moving the rotation ⑼. However, without further description, the photoresistive substrate 1 can be fixedly mounted The rotating table 11 changes the position of the optical system. Further, 'the laser light is irradiated from the light beam generating source 12 while rotating, and the photoresist layer is exposed. This exposure is based on the rotation of the rotary table by the _ side, and the rotary table 11 is continuously moved a little distance toward the radial direction of the photoresist substrate i by the _ side to form a latent image with fine unevenness, that is, the case of a recording disc A spiral guide groove is formed. x, In the case of optical discs, the concave and convex pits and guide grooves for information and data are formed as latent images of fine unevenness. In addition, when manufacturing concentric circular disks such as magnetic hard disks, it is possible to respond to the rotation stage or optical system step by step instead of successively. Based on the above, according to the information, the irradiation pulse or continuous light corresponding to the desired power of the irradiation threshold power P0 of the pit or the guide groove is sequentially irradiated from the desired position of the photoresist substrate 1 to Photoresist layer for exposure. Examples of the irradiation pulse are shown in Figs. 4A and 4B, and examples of the continuous light are shown in Fig. 4C. '' The photoresist material composed of the incomplete oxide of the transition metal of the present invention, by irradiating the threshold power? 〇 Irradiation of ultraviolet rays or visible light above, the chemical conversion of raw beaker and wheat, the etching rate for alkali or acid is different in the exposed part and the unexposed part, and the selection ratio can also be obtained. σ This means that the lower the irradiation power, the shorter and narrower pits can be formed. However, the irradiation power is extremely low, and it is difficult to form a stable pattern because it is close to the irradiation threshold power. Therefore, it is necessary to appropriately set the optimum irradiation power for exposure.

O:\87\87377.DOC -20- 200414183 再者’本發明者等實際確認,藉由組合本發明之光阻材料、 波長660 nm之紅色半導體雷射、及來自在波長185nm、254 iim、 及405 nm程度具有峰值之水銀燈之曝光,可獲得選擇比, 形成微細之凹坑圖案。 光阻層顯影工序 其次’藉由將如此圖案曝光之光阻基板1顯影,可獲得光 碟用之光阻原盤,其係形成按照特定之曝光圖案之凹坑或 導引溝之微細凹凸所構成者。 頌衫處理可藉由酸或驗等液體之濕式製程而獲得選擇 比,可依照使用目的、用途、裝置設備等而適當區分使用。 用於乾式製程之鹼顯影液可使用氫氧化四甲基銨溶液、 KOH、NaOH、NaWO3等無機鹼水溶液,酸顯影液可使用鹽 酸、硝酸、硫酸、磷酸等。又,本發明者等確認,除了濕 式製程以外,即使藉由稱為電漿或反應性離子蝕刻 (Reactlve Ion Etchlng: RIE)之乾式製程,亦可利用調整氣 體種類及複數氣體之混合比而進行顯影。 在此,說明關於曝光感度之調整方法。例如:將以化學 式w〇3表示之過渡金屬之氧化物換算為組成比例 時,在議0」大 '未滿0.75之範_,可獲得良好之曝光X感 度。此時,mg發生曝光工序需要大的照射功率,或 者顯影處理需要長時間等不便之臨界值…_〇4〜0.7 程度’可獲得最高之曝光感度。 又,將以化學式M〇〇3表示之過渡金屬之氧化物換算為组 成比例Μ〇1·Λ時,在x比0·1大、未滿0.75之範圍内,可獲O: \ 87 \ 87377.DOC -20- 200414183 Furthermore, the present inventors have actually confirmed that by combining the photoresist material of the present invention, a red semiconductor laser with a wavelength of 660 nm, And exposure of a mercury lamp with a peak of about 405 nm, a selection ratio can be obtained to form a fine pit pattern. Photoresist layer development process is followed by 'developing the photoresist substrate 1 exposed in such a pattern to obtain a photoresist master for optical discs, which is formed by forming fine depressions or depressions according to a specific exposure pattern . Song shirt treatment can be obtained through the wet process of acid or test liquid, and the selection ratio can be appropriately used according to the purpose, application, equipment and so on. For the alkaline developer used in the dry process, an inorganic alkali aqueous solution such as a tetramethylammonium hydroxide solution, KOH, NaOH, and NaWO3 can be used, and as the acid developer, hydrochloric acid, nitric acid, sulfuric acid, and phosphoric acid can be used. In addition, the inventors have confirmed that, in addition to the wet process, even by a dry process called plasma or reactive ion etching (Reactlve Ion Etchlng: RIE), the type of gas and the mixing ratio of plural gases can be adjusted by Develop. Here, a method for adjusting the exposure sensitivity will be described. For example, when the oxide of a transition metal represented by the chemical formula w03 is converted into a composition ratio, a good exposure X sensitivity can be obtained in the range of "0" and "less than 0.75". At this time, a critical value of inconvenience such as a large irradiation power required for the mg exposure step, or a long time required for the development process, etc. _04 ~ 0.7 degree 'can obtain the highest exposure sensitivity. In addition, when the oxide of the transition metal represented by the chemical formula M03 is converted to the composition ratio M1 · Λ, it can be obtained in a range where x is larger than 0 · 1 and less than 0.75.

O:\87\87377 DOC -21 - 200414183 侍良好之曝光感度。此時,㈣“系發生曝光工序需要大 的知、射功率’或者顯影處理需要長時間等不便之臨界值: 又’ X為G.4〜G.7程度,可獲得最高之曝光感度。 、又’將以化學式MoQ表示之過渡金屬之氧化物換算為組 成比例Μ〇1-χ〇χ時,在X比0·1大、未滿0.5之範圍内,可獲得 好之曝光感度。此時,χ=〇1係發生曝光工序需要大的 知、射功率’或者顯影處理需要長時間等不便之臨界值。 光阻材料之曝域度越高,除了可減低曝光時之照射功 率以外’還具有可縮短對應脈衝寬或線速度之曝光時間等 k 2然而反之,右感度過高’產生聚焦設定時發生不必 要之曝光’或者由於製程室照明環境而受到不良影響等不 便,故按照用途適當選擇最適之曝光感度。本發明之光阻 材料之曝光感度之調整,除了增減氧含有量以外,於過渡 金屬之不完全氧化物添加第二過渡金屬亦有效。例如:藉 由於WhOx添加Mo,可改善曝光感度約3〇%程度。 又,曝光感度之調整除了使光阻材料之組成變化以外, 逛可藉由選擇基板材料,或者於基板施加曝光前處理而進 仃。實際上,使用石英、矽、玻璃、及塑膠(聚碳酸酯)作為 基板之情況,調查因基板種類之不同所造成之曝光感度的 έ異’確認由於基板種類不@ ’曝光感度亦不同,具體而 言,感度由高至低的順序為石夕、石英、玻璃、塑膠。此順 序與熱傳導率之順序對應,結果熱傳導率越小的基板,曝 光感度越良好。此乃由於熱傳導率越小的基板,曝光時之 溫度上升越明顯,故伴隨溫度上升,光阻材料之化學性質O: \ 87 \ 87377 DOC -21-200414183 Good exposure sensitivity. At this time, the threshold value of the inconvenience such as the large exposure and radiation power required for the exposure process or the long time required for the development process: and X is about G.4 to G.7, which can obtain the highest exposure sensitivity. Also, when the oxide of the transition metal represented by the chemical formula MoQ is converted into a composition ratio MO1-χ〇χ, a good exposure sensitivity can be obtained in a range where X is larger than 0.1 and less than 0.5. At this time , Χ = 〇1 is the critical value of inconvenience such as the large exposure and radiation power required for the exposure process to occur or the development process requires a long time. The higher the exposure range of the photoresist material, the more it can reduce the exposure power during exposure. It can shorten the exposure time corresponding to the pulse width or line speed, etc. k 2 However, on the other hand, the right sensitivity is too high, 'unnecessary exposure occurred during focus setting', or the inconvenience caused by the lighting environment of the process room is inconvenient, so it is appropriate according to the application. Select the optimal exposure sensitivity. In addition to increasing or decreasing the oxygen content, the adjustment of the exposure sensitivity of the photoresist material of the present invention is also effective by adding a second transition metal to an incomplete oxide of the transition metal. : By adding Mo to WhOx, the exposure sensitivity can be improved by about 30%. In addition to adjusting the sensitivity of the exposure, in addition to changing the composition of the photoresist material, the substrate can be selected by selecting a substrate material or applying a pre-exposure treatment to the substrate.实际上. In fact, when using quartz, silicon, glass, and plastic (polycarbonate) as the substrate, investigate the difference in exposure sensitivity due to the type of substrate. 'Confirm that the sensitivity of the substrate is not the same as the exposure sensitivity.' Specifically, the order of sensitivity is Shi Xi, Quartz, Glass, and Plastic. This order corresponds to the order of thermal conductivity. As a result, the smaller the thermal conductivity, the better the exposure sensitivity. This is because the more the thermal conductivity The smaller the substrate, the more obvious the temperature rise during exposure, so as the temperature rises, the chemical properties of the photoresist material

O:\87\87377.DOC -22- 200414183 大幅變化所致。 *光前處理有於基板與光阻材料間形成中間層之處理' 熱處理、紫外線照射處理等。 特別是使用如單晶矽所組成 成之矽日日®寺之熱傳導率大的 基板吋,藉由於基板上形成執傳 力乂…得v羊較低之層作為中間 g,可適當改善曝光感度,因為藉 句稭田干間層,曝光時之埶 朝光阻材料之蓄積被改善。再者W二氧切(si〇i 乳化罐N)、氧化铭(Al2〇3)等係適於作為構成該中間層之 熱傳導率低之材料。又,該中 Τ间層右稭由濺射法或其他蒸 鍍法而形成亦可。 又,於石英基板上旋轉塗佈5 μηι之紫外線硬化樹脂後, 措由照射紫外線使液狀樹脂硬化之基板,確認其曝光感度 相較於未處理之石英基板改善。此亦可由紫外線硬化樹脂 之熱傳導率為塑膠程度之低而說明。 又,藉由熱處理、紫外線照射等之曝光前處理,亦可改 善曝光感度。因為藉由施加此等曝光前處理,雖不完全, 但本發明之光阻材料之化學性質已某種程度改變。 如上述,藉由材料組成、顯影條件、基板之選擇等,可 使具有各種特性之過渡金屬之不完全氧化物所組成之光阻 ,生機能,進一步由擴大光阻材料之應用範圍之觀點考 里,2層光阻法係極為有效。以下,參考圖5α至圖說明2 層光阻法之概要。 f先,使本發明之過渡金屬之不完全氧化物所組成之第 一光阻層30堆積前,如圖5A所示,於基板”上構成此第一O: \ 87 \ 87377.DOC -22- 200414183 due to significant changes. * Photopre-treatment includes a process of forming an intermediate layer between the substrate and the photoresist material, such as heat treatment, ultraviolet irradiation treatment, and the like. In particular, a substrate with a large thermal conductivity, such as single crystal silicon, is used. By forming the substrate on the substrate, the lower layer of v is used as the middle g, which can appropriately improve the exposure sensitivity. Because of the dry layer of the straw field, the accumulation of the photoresist material during the exposure is improved. Furthermore, W dioxin (SiOi emulsification tank N), oxidized aluminum (Al203), etc. are suitable as materials having low thermal conductivity for forming the intermediate layer. The middle layer of the T layer may be formed by a sputtering method or another evaporation method. In addition, after spin-coating a 5 μm UV-curable resin on a quartz substrate, the substrate was cured by irradiating ultraviolet rays to the liquid resin, and it was confirmed that the exposure sensitivity was improved compared to the untreated quartz substrate. This can also be explained by the low thermal conductivity of the UV-curable resin. In addition, the exposure sensitivity can be improved by pre-exposure treatment such as heat treatment and ultraviolet irradiation. Because by applying such pre-exposure treatments, although not completely, the chemical properties of the photoresist material of the present invention have changed to some extent. As mentioned above, the photoresist composed of incomplete oxides of transition metals with various characteristics can be made functional by the choice of material composition, development conditions, and substrates. From the viewpoint of expanding the application range of photoresist materials, Here, the 2-layer photoresist method is extremely effective. Hereinafter, the outline of the two-layer photoresist method will be described with reference to FIGS. 5α to 5. f First, before the first photoresist layer 30 composed of the incomplete oxide of the transition metal of the present invention is stacked, as shown in FIG. 5A, the first photoresist layer 30 is formed on the substrate.

O:\87\87377.DOC -23- 414183 j阻層30之過渡金屬之不完全氧化物之間,使可獲得非常 南之選擇比之材料堆積,作為第二光阻層32。 - 其—欠、’’如圖5B所示,對於第一光阻層30施加曝光及顯影 处理,並圖案第一光阻層3〇。 “其次,將第一光阻層30所組成之圖案作為掩膜,於第二 =層32’以高選擇比之_條件進行㈣。藉此,'㈣ 所不’轉印第-光阻層30之圖案於第二光阻層32。 二% 二 使用 使用 最後,藉由除去第一光阻層3〇,結束如圖⑺所示 光阻層32之圖案。 二者’於2層光阻法適用本發明之情況,藉由例如 Γ英作為基板’使用㈣過渡金屬作為第二光阻層,使用 i孔糸之氣體進行RIE、電漿㈣等,可於構成第 之過渡金屬之不完全氧化物盥 以層 無限大之選擇比。 ”第一先阻層之間’獲得大致 如以上說明,本發明之光碟用原盤之製造方法中 Γ先前所述之過渡金屬之不完全氧化物所組成之光阻材 料、,故具有可使用無機光阻,„可組合紫外線或可視2 而進行曝光之優點。此先 視光在光4m 不间於由於對於紫外線或可 == 無法使用此等作為曝光源,電子 束或離子束等昂責之曝光 之無機光阻。 六足先別 又,可使用描晝速度快之紫外線或可 用電子束之先前之使用盔機 / 相較於採 、 史…、祙先阻之光碟用原盤之製f 法,可大幅縮短曝光所需要的時間。 k方O: \ 87 \ 87377.DOC -23- 414183 j Between the incomplete oxides of the transition metals of the barrier layer 30, a material with a very low selection ratio can be stacked as the second photoresist layer 32. -Its-under, '' As shown in FIG. 5B, exposure and development processes are applied to the first photoresist layer 30, and the first photoresist layer 30 is patterned. "Second, the pattern formed by the first photoresist layer 30 is used as a mask, and the second photoresist layer is subjected to a high selection ratio of _ conditions at the second layer 32 '. Thus, the first photoresist layer is transferred by' ㈣ 所 不 ' The pattern of 30 is on the second photoresist layer 32. At the end of the second use, the pattern of the photoresist layer 32 is ended by removing the first photoresist layer 30, as shown in FIG. In the case where the method is applicable to the present invention, for example, by using Γying as a substrate 'using a rhenium transition metal as the second photoresist layer, and performing RIE, plasma rheology, etc. using i-hole rhenium gas, the transition metal constituting the first transition metal can be incomplete The oxide layer has an infinitely large selection ratio. "Between the first resistive layers" is obtained as described above. In the method for manufacturing an original disc for an optical disc of the present invention, it is composed of incomplete oxides of transition metals previously described. It is a photoresist material, so it has the advantage of using inorganic photoresist, „can be combined with UV or visible 2 for exposure. This first look at the light at 4m is not inconsistent because for UV or may == can not use these as exposure Source, electron beam or ion beam, etc. Hexapods can be used separately, you can use the ultraviolet light with fast daylight speed or the previous helmet machine that can use the electron beam. Compared with the mining, history, etc., the optical disc can be made using the original f method. Significantly reduce the time required for exposure.

O:\87\87377 DOC -24- 200414183 又’使用過渡金屬之不完全氧化物所組成之無機光阻材 料,^曝光部與未曝光部之境界部之圖案明瞭,實現高精 度之U細加工。又,曝光時能以曝光源本身進行聚焦, 可獲得向解析度。 制如此、’於形成微細之圖案之際,本發明之光碟用原盤之 製造方法係以Ρ=κ· λ/ΝΑ所表示之關係中,使比例常數κ 下降之手法’ $同於使曝光波長又短波長化,將物鏡之數 值孔徑ΝΑ大口徑化而實現微細加工之先前之手法,可利用 既存之曝光裝置進展更進一步之微細化。具體而言,根據 本么明,可使比例常數κ未滿〇8,被加工物之最小微細加 工週期f小至以下所示。 f< 0.8 λ /ΝΑ 根據本發明,藉由原樣利用既存之曝光裝置,可供 給實現廉價且更甚於以往之微細加工之光碟用原盤。〃 實施例 以下,根據實驗結果說明有關適用本發明之具體實施例。 實施例1 實2例1使用W(鎢)之3價之不完全氧化物作為光阻材 料’實際製作光碟用光阻原盤。 首先,於充分平滑化之玻璃基板上,藉由濺射法均一成 膜W之不完全氧化物所組成之光阻層。此時,使用w之單體 所組成之賤射乾材,於氬及氧之混合氣氛中進㈣射,改 變氧氣體濃度以控制不完全氧化物之氧化程度。 以能量分散型X光譜儀(Energy Dispersive χO: \ 87 \ 87377 DOC -24- 200414183 It also uses an inorganic photoresist material composed of an incomplete oxide of a transition metal. The pattern of the boundary between the exposed and unexposed parts is clear, and high precision U fine processing is realized. . In addition, during exposure, focusing can be performed with the exposure source itself, and the resolution can be obtained. In this way, 'when forming a fine pattern, the manufacturing method of the original disc for optical discs of the present invention is a method of reducing the proportionality constant κ in the relationship represented by P = κ · λ / ΝΑ' $ Same as the exposure wavelength With the short wavelength, the previous method of increasing the numerical aperture NA of the objective lens to achieve microfabrication can be further refined by using the existing exposure device. Specifically, according to the present invention, the proportionality constant κ can be less than 0.8, and the minimum fine processing cycle f of the workpiece can be made as shown below. f < 0.8 λ / NA According to the present invention, by using the existing exposure device as it is, it is possible to provide an original disc for an optical disc which is cheaper and more finely processed than before. 〃 Examples The following describes specific examples to which the present invention is applicable based on experimental results. Example 1 Example 2 Example 1 uses a trivalent incomplete oxide of W (tungsten) as a photoresist material 'to actually make a photoresist master for optical discs. First, on a sufficiently smooth glass substrate, a photoresist layer composed of incomplete oxide of W was uniformly formed by a sputtering method. At this time, a dry base material composed of w monomer is used to shoot in a mixed atmosphere of argon and oxygen to change the oxygen gas concentration to control the degree of oxidation of incomplete oxides. 2. Energy Dispersive X-ray spectrometer

O:\87\87377 DOC -25- 200414183O: \ 87 \ 87377 DOC -25- 200414183

SpeCtr〇metei·: EDX)解析堆積之光阻層,以組成比例u 表不時,X=〇.63。又’光阻層之膜厚為4〇證。又,折射 率之波長依存性係藉由分光橢圓儀法而測定。 載置結束光阻層之成膜之光阻基板於圖2所示之曝光褒 置之旋轉台上。且,一 使疑轉口以期望之旋轉數旋轉, 一面照射未滿照射臨 一 卩很刀半之雷射,以致動器設定物鏡 之高度方向之位置,以便對焦於光阻層。 其次’在固定光學系# & 士如 干糸、、先之狀恶下,猎由設置於旋轉台之 移送機構,使旋轉台移動 秒助主期望之+徑位置,按照資訊資 料’於光阻層照射對廣、凹仿 士 μ 几之’、、、射脈衝,曝光光阻層。此 …在使旋轉台旋轉之狀態下,一面使旋轉台朝光阻基板 之半控方向連續移動些微距離,一面進行曝光。再者,曝 光波長為4〇5 nm,曝光光學系統之數值孔徑ΝΑ為〇.95。又, 曝光時之線速度為2.5 m/s,照射功率為6 〇讀。 "其次,ϋ由利用驗顯影液之濕式製程,顯影曝光結束之 先阻基板。此顯影工序係在光阻基板浸泡於顯影液之狀態 下,為了使姓刻之均-性提升,於施加超音波之狀態下進 行顯影,顯影結束後,#由純水及異丙醇充分洗淨,並以 :風㈧ΓΒ1—等使其乾燥’結束製程。驗顯影液使用四甲 基鉍氫虱化水溶液,顯影時間為3〇分。 圖6係表示以掃描型電子顯微鏡(Scaring Electr〇n Μ咖scope ·· SEM)觀察顯影後之光阻圖案。圖6中,凹坑部 分對應於曝光部’未曝光部之光阻層成為凹部。如此,W 之不完全氧化物所組成之光阻材料成為所謂正型之光阻。SpeCtrometei :: EDX) Analyze the stacked photoresist layer, and express from time to time with the composition ratio u, X = 0.63. The thickness of the photoresist layer is 40%. The wavelength dependence of the refractive index was measured by a spectroscopic ellipsometry method. The photoresist substrate on which the film formation of the photoresist layer is finished is placed on a rotating stage in the exposure setup shown in FIG. 2. In addition, once the suspicious port is rotated by a desired number of rotations, the laser beam is irradiated on the side of the laser beam, and the actuator is used to set the position of the objective lens in the height direction so as to focus on the photoresist layer. Secondly, in the case of fixed optics #, such as the dry and the first, the hunting mechanism is set on the rotating table to move the rotating table to help + the desired position of the master in accordance with the information. The photoresist layer is exposed by irradiating the photoresist layer with pulses on the photoresist layer. This… In the state of rotating the rotary table, while the rotary table is continuously moved a little distance toward the half-control direction of the photoresist substrate, exposure is performed. The exposure wavelength was 4.05 nm, and the numerical aperture NA of the exposure optical system was 0.95. The linear velocity during exposure was 2.5 m / s, and the irradiation power was 60 reads. " Second, a wet process using a developer is used to block the substrate before the exposure of the developer is completed. This development process is to immerse the photoresist substrate in a developing solution. In order to improve the uniformity of the last name, development is performed in the state of applying ultrasonic waves. After the development is completed, #wash thoroughly with pure water and isopropyl alcohol. Clean, and end with: wind ㈧ΓΒ1-wait for it to dry. A tetramethylbismuth hydrogenated aqueous solution was used as the developing solution, and the developing time was 30 minutes. FIG. 6 shows a photoresist pattern after development was observed with a scanning electron microscope (Scaring Electron scope · SEM). In Fig. 6, the photoresist layer corresponding to the exposed portion 'and the unexposed portion of the pit portion becomes a concave portion. In this way, a photoresist material composed of an incomplete oxide of W becomes a so-called positive photoresist.

O:\87\87377.DOC -26- 414183 4、卩於w之不完全氧化物所組成之光阻層,未曝光部之 虫刻速度較曝光部之㈣速度慢,故未曝光部之光阻層於 顯影後亦大致維持成膜後之膜厚。相對於此,曝光部;光 阻層係藉由餘刻被除去’玻璃基板之表面露出於曝光部。 再者,圖6所示之4個凹坑中,最小的凹坑為寬〇15叫, 長度0.16障。如此,可知藉由使用本發明之光阻材料之光 碟用原盤之製造方法’相較於先前之有機光阻所期待之凹 ^寬〇.39 μΐΏ,可明顯提升解像度。又’由圖6亦可知,凹 坑之邊緣非常明瞭。 又,可知顯影後之凹坑之寬及長度係藉由曝光光源之照 射功率及脈衝寬而變動。 比較例1 比較例1使用W之完全氧化物W〇3作為光阻 作光碟用絲原盤。 1 首先,藉由濺射法,於玻璃基板上堆積w之完全氧化物 所組成之光阻層。以EDX分析堆積之光阻層,以組成比例 WkOx表示時,x= 0.75。再者,由利用透過型電子束顯微 鏡之電子束繞射之解析結果,確認w〇不完全氧化物之曝光 前之結晶狀態為非晶矽。 以與實施例1同等或充分強度之照射功率曝光此光阻 層,無法獲得比1大之選擇比,不能形成期望之凹坑圖案。 總言之,W之完全氧化物對於曝光源在光學上為透明,故 吸收小,不至於使光阻材料產生化學變化。 實施例2 O:\87\87377.DOC -27- 200414183 一於實施例2’使料之3價及—之3價之不完全氧化物作為 f阻材料,按照® 1所*之製程實際製作光碟用光阻原盤' 最終亚製作光碟。以下,參考圖1說明實施内容。 首先,以石夕晶圓作為基板100,於該基板上,ϋ由濺射法 均一成膜膜厚80 nm之非晶矽所組成之中間層1〇1。其次\ 错由錢射法’於其上均—成膜慨⑽之不完全氧化物所組 成之光阻層102(圖i(a))。此時,使用w&M〇之不完全氧化 物所組成之濺射靶材,於氬氣氛中進行濺射。此時,以 解析堆積之光阻層,成膜之觀心之不完全氧化物之界與O: \ 87 \ 87377.DOC -26- 414183 4. In the photoresist layer composed of incomplete oxides that are exposed to w, the insect engraving speed of the unexposed part is slower than that of the exposed part, so the light of the unexposed part is light. The film thickness of the resist layer after development is also maintained substantially after development. On the other hand, the exposed portion and the photoresist layer are exposed to the exposed portion by removing the surface of the glass substrate. Furthermore, among the four pits shown in FIG. 6, the smallest pit is 0.15 in width and 0.16 in length. In this way, it can be seen that by using the manufacturing method of the original disc for optical discs using the photoresist material of the present invention, compared with the concave width expected by the previous organic photoresist, the width is 0.39 μΐΏ, which can significantly improve the resolution. It can also be seen from Fig. 6 that the edges of the pits are very clear. It is also known that the width and length of the pits after development are changed by the irradiation power and pulse width of the exposure light source. Comparative Example 1 Comparative Example 1 uses W complete oxide W03 as a photoresist as a silk master for optical discs. 1 First, a photoresist layer composed of a complete oxide of w is deposited on a glass substrate by a sputtering method. When the stacked photoresist layer is analyzed by EDX and expressed in composition ratio WkOx, x = 0.75. Furthermore, from the analysis results of electron beam diffraction using a transmission electron beam microscope, it was confirmed that the crystal state before the exposure of the incomplete oxide was amorphous silicon. Exposing this photoresist layer with an irradiation power equal to or sufficient intensity as in Example 1 could not achieve a selectivity greater than 1, and a desired pit pattern could not be formed. In summary, the complete oxide of W is optically transparent to the exposure source, so it has a small absorption and does not cause chemical changes in the photoresist material. Example 2 O: \ 87 \ 87377.DOC -27- 200414183 As in Example 2 ', the trivalent and -trivalent incomplete oxides are used as f-resistance materials, and are actually produced according to the manufacturing process of ® 1 Discs with photoresist masters' Final sub-production discs. Hereinafter, implementation contents will be described with reference to FIG. 1. First, a Shixi wafer is used as the substrate 100. On the substrate, an intermediate layer 101 composed of amorphous silicon with a uniform film thickness of 80 nm is sputtered. Secondly, the photoresist layer 102 composed of the incomplete oxide that is formed on top of the film-forming method is wrong (Fig. I (a)). At this time, a sputtering target composed of an incomplete oxide of w & M0 was used, and sputtering was performed in an argon atmosphere. At this time, in order to analyze the stacked photoresist layer

Mo之比率為80 : 2〇,氧之含有率為6〇此%。又,光阻層之 膜厚為55 nm。再者,由利用透過型電子束顯微鏡之電子束 繞射之解析結果,確認WM〇〇不完全氧化物之曝光前之結 晶狀態為非晶碎。 光阻層之曝光卫序以後,除了曝光條件,其餘均以與實 施例1相同之條件進行處理,製作光碟用光阻原盤1〇3(圖 1(b)、(c))。實施例2之曝光條件如以下所示。 •曝光波長:405 nm •曝光光學系統之數值孔徑N A : 0.9 5The ratio of Mo is 80:20, and the oxygen content is 60%. The thickness of the photoresist layer was 55 nm. Furthermore, from the analysis results of electron beam diffraction using a transmission electron beam microscope, it was confirmed that the crystalline state before the exposure of the WMOO incomplete oxide was amorphous. After the exposure of the photoresist layer, except for the exposure conditions, the rest were processed under the same conditions as in Example 1 to produce a photoresist master 103 for optical discs (Fig. 1 (b), (c)). The exposure conditions of Example 2 are shown below. • Exposure wavelength: 405 nm • Numerical aperture of exposure optical system N A: 0.9 5

•調變:17PP •凹坑長:112 nm •軌道間隔:320 nm • 曝光時之線速度:4.92 m/s• Modulation: 17PP • Pit length: 112 nm • Track interval: 320 nm • Linear speed during exposure: 4.92 m / s

• 曝光照射功率:6.0 mW •寫入方式:與相變化碟片相同之簡易寫入方弋 O:\87\87377.DOC •28- :係表示以㈣觀察顯影後之光碟用光阻原盤之光阻 =案之-例。W及M。之不完全氧化物所組成之光阻材料成 為正型之弁阳,+ 、 圖中,凹坑部對應曝光部,未曝光部之光 阻層成為凹部。又,形成之凹坑長(徑)㈣〜,確認達成 早面25 GB之高密度光碟所要求之最短凹坑長 以I甚而,觀察到光阻圖案以凹坑行方向300 nm間隔、 執運^向320 nm間隔之一定之間隔而形成同一形狀之凹坑 之狀態,確認可安定形成凹坑。 其次,藉由電鑄法,使光阻原盤之凹凸圖案面上析出金 屬鎳膜(圖1(d)),使此由光阻原盤剝離後,施加特定之加 工,獲得光阻原盤之凹凸圖案所轉印之成型用沖壓模 1〇4(圖 1(e))。 ' 使用該成型用沖壓模,藉由射出成型法形成熱塑性樹脂 之聚碳酸酯所組成之樹脂製碟片基板1〇5(圖1(f))。其次, 剝離沖壓模(圖1(g)),藉由於該樹脂製碟片基板之凹凸面成 膜A1合金之反射膜1〇6(圖1(h))及膜厚^ mm之保護膜1〇7 而獲得直徑12 cm之光碟(圖1(i))。再者,以上由光阻原盤獲 得光碟為止之工序係以先前習知之技術所製造。 圖8係表示以SEM觀察上述光碟表面之凹坑圖案之一 例。在此,長150 nm之凹坑、寬130 nm之線狀凹坑等係在 與實際之信號圖案對應之狀態下形成凹坑,確認成為記錄 容量25 GB之光碟。 其次,以下述條件讀取上述光碟,其RIMt號作為眼圖而 獲得,並進行#號汗估。其結果表示於圖9 A至圖9 C。 O:\87\87377.DOC -29- 200414183 •循執伺服:推拉計算定位法 •調變:17PP 一 • 凹坑長·· 1 12 nm •執道間隔·· 320 nm • 讀取線速度·· 4.92 m/s• Exposure irradiation power: 6.0 mW • Writing method: The same simple writing method as phase change discs: O: \ 87 \ 87377.DOC Photoresistance = case-example. W and M. The photoresist material composed of incomplete oxide becomes positive type. In the figure, the pits correspond to the exposed parts, and the photoresist layer in the unexposed part becomes the concave part. In addition, the formed pit length (diameter) ㈣ ~ was confirmed to be the shortest pit length required to achieve a high-density disc of 25 GB on the early side, and even the photoresist pattern was observed at 300 nm intervals in the direction of the pit row. ^ The state where pits of the same shape are formed toward a certain interval of 320 nm, and it is confirmed that the pits can be formed stably. Secondly, a metal nickel film is deposited on the concave-convex pattern surface of the photoresist master by electroforming (Fig. 1 (d)). After peeling from the photoresist master, a specific process is applied to obtain a concave-convex pattern on the photoresist master The transferred stamping die 104 (Fig. 1 (e)). '' Using this stamping die for molding, a resin-made disc substrate 105 made of polycarbonate made of a thermoplastic resin by injection molding is formed (Fig. 1 (f)). Next, the stamping die (Fig. 1 (g)) is peeled off, and a reflective film 106 (Fig. 1 (h)) of A1 alloy and a protective film 1 having a thickness of ^ mm are formed by forming the A1 alloy reflective film due to the uneven surface of the resin-made disc substrate. 〇7 to obtain a disc with a diameter of 12 cm (Figure 1 (i)). In addition, the above steps until the optical disc is obtained from the photoresist master are manufactured by a conventionally known technique. Fig. 8 shows an example of the pit pattern on the surface of the optical disc observed by SEM. Here, pits having a length of 150 nm, linear pits having a width of 130 nm, and the like are formed in a state corresponding to the actual signal pattern, and are confirmed to be a disc with a recording capacity of 25 GB. Next, the above-mentioned optical disc was read under the following conditions, the RIMt number thereof was obtained as an eye diagram, and a ## sweat estimate was performed. The results are shown in Figs. 9A to 9C. O: \ 87 \ 87377.DOC -29- 200414183 • Obedient servo: Push-pull calculation positioning method • Modulation: 17PP 1 • Pit length · 1 12 nm • Road interval · 320 nm • Reading line speed · 4.92 m / s

• 讀取照射功率·· 0.4 mW 關於讀取之眼圖(圖9A),進行過基本等化處理之眼圖(圖 9B)之抖動值為8.0%,進行過限制等化處理之眼圖(圖9c)之 抖動值為極低值之4.6%,作為記錄容量25 GB2R〇M碟片, 獲得無實用上問題之良好結果。 再者,本發明所進行之光阻層形成至顯影為止之微影技 術亦可應用於 DRAM(Dynamic Rand〇m Access Mem〇ry :動 態隨機存取記憶體)' 快閃記憶體、⑽❿加㈤ρΓ〇__• Reading irradiation power ... 0.4 mW For the eye diagram (Figure 9A), the eye diagram (Figure 9B) that has undergone the basic equalization process has a jitter value of 8.0% and the eye diagram that has undergone the limiting equalization process ( The jitter value of Fig. 9c) is 4.6%, which is an extremely low value. As a disc with a recording capacity of 25 GB2 ROM, a good result without practical problems is obtained. Furthermore, the photolithography technology from the formation of the photoresist layer to the development of the present invention can also be applied to DRAM (Dynamic Random Access Memory): flash memory, ⑽❿ ㈤ρΓ 〇__

Unit 中央處理單元)、ASIC(Applicati〇n Specific IC :特殊 應用積體電路)等半導體元件;磁頭等磁元件;液晶、 EL(EleCtro Luminescence :電致發光)、漬⑺—叩⑽Unit Central Processing Unit), ASIC (Application Specific IC) and other semiconductor components; magnetic components such as magnetic heads; liquid crystal, EL (EleCtro Luminescence: electroluminescence),

Panel ·電漿顯不面板)等顯示元件;光記錄媒體、光調變元 件等光元件等各種元件之製作。 士 X上所述,本發明之光碟用原盤之製造方法中,由於 ^且層係由對於紫外線或可視光顯示吸收之過渡金屬之不 π王氧化物所組成’故可於既存之以紫外線或可視光為曝 光源之曝光裝置進杆^ +光。又’根據本發明,使用分子大 小較小之過渡金屬之不6入 +凡王虱化物作為光阻材料,故於光 阻層之顯影階段獲得良 I好之邊緣圖案,可達成高精度之圖Panel (plasma display panel) and other display elements; optical recording media, light modulation elements and other optical elements and other components. According to the above-mentioned X, in the manufacturing method of the original disc for optical discs of the present invention, since the layer is composed of non-π oxide of a transition metal that absorbs ultraviolet or visible light, it can be used in the existing ultraviolet or The visible light is the light of the exposure device of the exposure source. According to the present invention, a transition metal with a smaller molecular size is used as a photoresist material, so a good edge pattern can be obtained in the development stage of the photoresist layer, and a high-precision map can be achieved.

O:\87\87377 DOC -30- 200414183 案。 故,使用此種光碟甩原盤之光碟、生 夕一 衣方法,里_ γ糸可 由使用既存之曝光裝置之製法, ’、、曰 容量光碟。 衣心己憶容量25GB級之高 【圖式簡單說明】 圖1(a)至圖l(i)係表示適用本 碟之製程圖。 u之先碟之製造方法之光 圖2係表示用於適用本發 , 之先碟用原盤之製造方法之 曝光裝置之模式圖。 辰&万法之 圖3係表示曝光本發明之古 月之先阻材㈣組 況之用於曝光之光源之昭射 '、、、射功率及曝光部與未曝光部之蝕 刻速度之差之關係之特性圖。 圖表示曝光工序之照射圖案之例之特性 圖。圖4Α及圖仙係表示照射脈衝之例,圖鄉表示連續光 之例。 ㈣至圖灣表示2層光阻之重要部分概略剖面圖。圖 5Α為弟-光阻層及第二光阻層成膜工序,圖5β為第一光阻 層圖案工序’圖%為第二光阻層姓刻工序,圖π為第一光 阻層除去工序。 圖6為以SEM觀察顯影後之w(鎢)之不完全氧化物所組成 之光阻層之照片。 圖7為以SEM觀察顯影後之%與]^〇之不完全氧化物所組 成之光阻層之照片。 圖8為以SEM觀察於實施例2所製造之記錄容量25 gb之O: \ 87 \ 87377 DOC -30- 200414183. Therefore, by using such a disc to shake the original disc and the method of producing clothes, the _ γ 糸 can be made by using the existing exposure device manufacturing method, and the capacity disc. Yixin has a memory capacity as high as 25GB. [Schematic description] Figures 1 (a) to 1 (i) show the process diagrams applicable to this disc. Light of the manufacturing method of the pre-disc of u Figure 2 is a schematic diagram showing an exposure device used in the manufacturing method of the original disc for the pre-disc to which the present invention is applied. Chen & Wanfa's Figure 3 shows the exposure of the light source used for exposure, the exposure power, and the difference in etching speed between the exposed and unexposed parts of the light source used for exposure. The relationship between the characteristic map. The figure shows a characteristic diagram of an example of an irradiation pattern in an exposure process. Fig. 4A and Fig. 1 show examples of irradiation pulses, and Fig. 4 shows examples of continuous light. ㈣ to Tuwan are schematic cross-sectional views of the important part of the 2-layer photoresist. FIG. 5A is a step of forming a photoresist layer and a second photoresist layer, and FIG. 5β is a first photoresist layer pattern step. FIG.% Is a second photoresist layer engraving step, and FIG. Π is a first photoresist layer removal. Procedure. Fig. 6 is a photograph of a photoresist layer composed of incomplete oxides of w (tungsten) after development, observed by SEM. Fig. 7 is a SEM observation of a photoresist layer composed of% incomplete oxide and ^^ after development. 8 is a SEM observation of a recording capacity of 25 gb manufactured in Example 2.

O:\87\87377 DOC -31 - 200414183 光碟表面之凹坑圖案之照片。 圖9A至圖9C係表示於實施例2所製造之記錄容量25 之光碟之信號評估結果圖。 圖10(a)至圖10(i)係表示先前之光碟之製程圖。 【圖式代表符號說明】 1 光阻基板 11 旋轉台 12 光束發生源 13 準直透鏡 14 光束分波器 15 物鏡 16 聚光物鏡 17 分割光感測器 18 聚焦誤差信號 19 聚焦致動器 20 資料信號 21 反射光量信號 22 循執誤差信號 23 雷射驅動電路 24 主軸馬達控制系統 30 第一光阻層 31 、 90 、 100 基板 32 第二光阻層 91 、 102 光阻層 O:\87\87377.DOC -32- 200414183 92 、 103 原盤 93 、 104 成型用沖壓模 94 、 105 樹脂製碟片基板 95 、 106 反射膜 96 、 107 保護膜 101 中間層 f 最小微細加工週期 K 比例常數 ΝΑ 數值孔徑 Ρ 最短凹坑長 Ρ0 照射臨限值功率 λ (光源之)波長、曝光波長 O:\87\87377.DOC - 33 -O: \ 87 \ 87377 DOC -31-200414183 Photo of the pit pattern on the surface of the disc. 9A to 9C are diagrams showing signal evaluation results of an optical disc with a recording capacity of 25 manufactured in Example 2. FIG. FIG. 10 (a) to FIG. 10 (i) are process diagrams showing a conventional optical disc. [Illustration of representative symbols of the drawings] 1 Photoresistive substrate 11 Rotary table 12 Beam generation source 13 Collimator lens 14 Beam splitter 15 Objective lens 16 Condensing objective lens 17 Split light sensor 18 Focus error signal 19 Focus actuator 20 Information Signal 21 Reflected light signal 22 Compliance error signal 23 Laser drive circuit 24 Spindle motor control system 30 First photoresist layer 31, 90, 100 Substrate 32 Second photoresist layer 91, 102 Photoresist layer O: \ 87 \ 87377 .DOC -32- 200414183 92, 103 Original discs 93, 104 Stamping dies 94, 105 Resin-made disc substrates 95, 106 Reflective films 96, 107 Protective films 101 Intermediate layer f Minimum fine processing cycle K Proportional constant NA NA Numerical aperture P Shortest pit length P0 Radiation threshold power λ (of the light source) Wavelength, exposure wavelength O: \ 87 \ 87377.DOC-33-

Claims (1)

拾、申請專利範圍: :種光碟用原盤之製造方法,其特徵在於:於基板上將 含金屬之不完全氧化物,且該不完全氧化物之; 之3有置比因應前述過渡金屬之可採價數之化學計量,且 成之乳含有量小之綠材料所構叙光阻層成膜後,使 遠先阻層對應記錄㈣號圖案選擇㈣光、 特定之凹凸圖案。 A 2. 3. 4. 5. 如申請專利範圍第i項之光碟用原盤之製造方法,其中前 述光阻材料為合有氧化物之非晶性無機材料。 如申請專利範圍第丄項之光碟用原盤之製造方法,豆中上 述過渡金屬為 Tl、v、Cr、Mn、Fe、Nb、Cu、Ni、c〇、 Mo、Ta、W、Zr、Ru、Ag 中之至w 種。 如申請專利範圍第i項之光碟用原盤之製造方法,其中上 述過渡金屬為Mo、W之任一者或兩者。 如申w專利範圍第1項之光碟用原盤之製造方法,其中於 上述過渡金屬之不完全氧化物進一步添加過渡金屬以外 之其他元素。 6·如申請專利範圍第5項之光碟用原盤之製造方法,其中上 述過渡金屬以外之其他元素為A卜c、B、Si、Ge中之至 少1種。 7·如申請專利範圍第1項之光碟用原盤之製造方法,其中係 藉由紫外線或可視光曝光。 8·如申請專利範圍第1項之光碟用原盤之製造方法,其中上 述I、外線或可視光為波長15 〇 nm〜410 nm。 O:\87\87377.DOC 200414183 9. 10. 11. 12. 13. 之製造方法,其中於 鎳中之至少1種所組 如申請專利範圍第!項之光碟用原盤 由玻璃、塑膠、矽、氧化紹碳化鈦、 成之基板上形成上述光阻層。 ;:申請專㈣㈣9項之光碟用《之製造方法,里中於 别述基板及前述光阻層之間,形成熱傳導率比基板小之 中間層。 如申請專利範圍第10項之光碟用原盤之製造方法,其令 上述中間層係由非晶梦、二氧化石夕、氮化石夕、氧化銘中 之至少1種所組成之薄膜。 t申請專利範圍第i項之光碟用原盤之製造方法,其中係 藉由濺射法或蒸鍍法形成上述光阻層。 ” 一種光碟之製造方法,其特徵在於:於基板上將含有過 渡金屬之不完全氧化物,且該不完全氧化物之氧之含有 量比因應前述過渡金屬之可採價數之化學計量組成之氧 含有量小之光阻材料所組成之光阻層成膜後,使該光随 層對應記錄用信號圖案選擇性曝光、顯影而形成特定之 凹凸圖案之原盤,使用該原盤製作經轉印凹凸圖案之碟 片。 ^ O:\87\87377.DOCScope of patent application: A method for manufacturing a master disc for optical discs, which is characterized in that: a metal-containing incomplete oxide is contained on the substrate, and the incomplete oxide is included; The stoichiometry of the valence number and the formation of the photoresist layer made of a green material with a small milk content, after forming the photoresist layer, the far-resistance layer should be selected to have a satin pattern and a specific concave-convex pattern corresponding to the recording pattern. A 2. 3. 4. 5. For the manufacturing method of the original disc for optical discs in the scope of patent application item i, wherein the aforementioned photoresist material is an amorphous inorganic material with an oxide. For example, the manufacturing method of the original disc for optical discs in the scope of the patent application, the transition metals in beans are Tl, v, Cr, Mn, Fe, Nb, Cu, Ni, co, Mo, Ta, W, Zr, Ru, From w to Ag. For example, in the method for manufacturing an original disc for an optical disc in the scope of application for patent i, the transition metal is either one or both of Mo and W. For example, the manufacturing method of the original disc for optical discs according to item 1 of the patent application, wherein an element other than a transition metal is further added to the incomplete oxide of the transition metal. 6. The manufacturing method of the original disc for optical discs according to item 5 of the scope of patent application, wherein the elements other than the transition metal are at least one of A, B, Si, and Ge. 7. The manufacturing method of the original disc for the optical disc as described in item 1 of the patent application scope, wherein the exposure is performed by ultraviolet or visible light. 8. The manufacturing method of the original disc for the optical disc as described in the item 1 of the scope of patent application, wherein the above-mentioned I, external line or visible light has a wavelength of 150 nm to 410 nm. O: \ 87 \ 87377.DOC 200414183 9. 10. 11. 12. 13. Manufacturing method, in which at least one kind of nickel is grouped as in the scope of patent application! The original disc for optical discs is made of glass, plastic, silicon The titanium oxide is used to form the photoresist layer on the substrate. ;: The manufacturing method for the application of 9 items of the optical disc is described below. Between the substrate and the aforementioned photoresist layer, an intermediate layer having a lower thermal conductivity than the substrate is formed. For example, in the method for manufacturing a master disc for an optical disc in the tenth aspect of the patent application, the above intermediate layer is a thin film composed of at least one of amorphous dream, stone dioxide, nitride stone, and oxide inscription. The method for manufacturing an original disc for an optical disc in the item i of the patent application, wherein the above-mentioned photoresist layer is formed by a sputtering method or an evaporation method. A method for manufacturing an optical disc, characterized in that an incomplete oxide of a transition metal is contained on a substrate, and an oxygen content ratio of the incomplete oxide is based on a stoichiometric composition of the foregoing valence of the transition metal. After forming a photoresist layer composed of a photoresist material having a small oxygen content, the light is selectively exposed and developed with the signal pattern corresponding to the recording layer to develop a master with a specific uneven pattern. The master is used to make a transferred bump Graphic disc. ^ O: \ 87 \ 87377.DOC
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