TW200928521A - Phase difference film and elliptical polarizing plate using the same - Google Patents

Phase difference film and elliptical polarizing plate using the same Download PDF

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Publication number
TW200928521A
TW200928521A TW97141327A TW97141327A TW200928521A TW 200928521 A TW200928521 A TW 200928521A TW 97141327 A TW97141327 A TW 97141327A TW 97141327 A TW97141327 A TW 97141327A TW 200928521 A TW200928521 A TW 200928521A
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Taiwan
Prior art keywords
film
polarizing plate
phase difference
wavelength plate
plate
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TW97141327A
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Chinese (zh)
Inventor
Yuuhei Inokuchi
Hideo Kuroiwa
li-yang Ju
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Sumitomo Chemical Co
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Publication of TW200928521A publication Critical patent/TW200928521A/en

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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B29WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
    • B29CSHAPING OR JOINING OF PLASTICS; SHAPING OF MATERIAL IN A PLASTIC STATE, NOT OTHERWISE PROVIDED FOR; AFTER-TREATMENT OF THE SHAPED PRODUCTS, e.g. REPAIRING
    • B29C55/00Shaping by stretching, e.g. drawing through a die; Apparatus therefor
    • B29C55/02Shaping by stretching, e.g. drawing through a die; Apparatus therefor of plates or sheets
    • B29C55/04Shaping by stretching, e.g. drawing through a die; Apparatus therefor of plates or sheets uniaxial, e.g. oblique
    • B29C55/08Shaping by stretching, e.g. drawing through a die; Apparatus therefor of plates or sheets uniaxial, e.g. oblique transverse to the direction of feed
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/30Polarising elements
    • G02B5/3083Birefringent or phase retarding elements
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B29WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
    • B29KINDEXING SCHEME ASSOCIATED WITH SUBCLASSES B29B, B29C OR B29D, RELATING TO MOULDING MATERIALS OR TO MATERIALS FOR MOULDS, REINFORCEMENTS, FILLERS OR PREFORMED PARTS, e.g. INSERTS
    • B29K2023/00Use of polyalkenes or derivatives thereof as moulding material
    • B29K2023/10Polymers of propylene
    • B29K2023/12PP, i.e. polypropylene
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B29WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
    • B29KINDEXING SCHEME ASSOCIATED WITH SUBCLASSES B29B, B29C OR B29D, RELATING TO MOULDING MATERIALS OR TO MATERIALS FOR MOULDS, REINFORCEMENTS, FILLERS OR PREFORMED PARTS, e.g. INSERTS
    • B29K2995/00Properties of moulding materials, reinforcements, fillers, preformed parts or moulds
    • B29K2995/0018Properties of moulding materials, reinforcements, fillers, preformed parts or moulds having particular optical properties, e.g. fluorescent or phosphorescent
    • B29K2995/0034Polarising

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Polarising Elements (AREA)
  • Liquid Crystal (AREA)

Abstract

Provided is a phase difference film formed of a laterally extended film of polypropylene resin, wherein the thickness is 25μ m or less, an in-plan phase difference value (R0) is within a range of 70 to 400nm, and an Nz coefficient which is defined by a general formula: Nz=(nx-nz)/(nx-ny) when nx is the refractive index in the direction of in-plan phase retardation axis of the film, ny is the refractive index in the direction of in-plan phase advancing axis of the film, and nz is the refractive index in the thickness direction is within a range of 0. 9 to 1. 1. The phase difference value is adjusted so that the phase difference film is functioned as a 1/4 wavelength plate 10. By laminating the phase difference film onto a linear polarizing plate 20, an elliptical polarizing plate 30 is obtained.

Description

200928521 六、發明說明: 【發明所屬之技術領域】 本發明係關於一種由聚丙烯樹脂所構成之相位差膜及 使用該相位差膜之橢圓偏光板。更詳而言之’係關於一種 可使膜厚極薄之相位差膜’及使用該膜之膜厚極薄的橢圓 偏光板者。本發明係又關於一種使用該橢圓偏光板之液晶 顯示裝置。 【先前技術】 Ο ❹ 近年,消耗電力低、以低電壓動作、輕量且薄型之液 晶顯示器,係急速普及作為行動電話、行動資訊終端、電 腦用監視器、電視等資訊用顯示裝置。伴隨液晶技術之發 展,已提出各種模式之液晶顯示器或光學構件,而改良應 答速度、對比度、視角、廣帶域性。 _ 以行動電話等為代表之反射型或半穿透反射型液晶顯 不器中’係使用一種橢圓偏光板,其係使作為1/4波長板 發揮功能之相位差膜、或使1/4波長板與1/2波長板組合 ;廣帶域作為1/4波長板發揮功能之相位差膜,以預定 低古^二合於直線偏光板者。如此之橢圓偏光板、尤其圓 =:=:止功能’在各用途中,對於人類眼晴 射,而期盼得到…的全部入射光可充分抑制其内部反 件至j良好的遮光性能。 相位差膜、之波長中作為1/4波長板發揮功能之 差膜予以組^,、二^中作為1/2波長板發揮功能之相位 '對於廣波長區域之入射光作為1/4 320734 4 200928521 ^波長板發揮功能之所謂廣帶域1/4波長板者係自以往即已 ^實施,例如,在日本特開平5—100114號公報(專利文獻υ 中係已揭示組合由聚碳酸酯膜所構成之1/4波長板與1/2 波長板之例。但使用聚碳酸酯之廣帶域1/4波長板中,要 *在全部的波長中作為完全的174波長板發揮功能乃很難, •又,很難充分地控制内部反射,無法得到良好的遮光性能。 再者’聚碳酸酯膜之光彈性係數高達約27xl(T13cm2/dyne, ❾故會有貼合於直線偏光板時產生貼合不均、或因使用時之 /里度變化而在黑顯示中部分地產生背光之光脫漏的白斑現 象等問題。 因此’在曰本特開平)^49015號公報中(專利文獻 2)中’已揭示:使在波長4〇〇nm中之面内的最大折射率與 最小折射率的差(雙折射)Δη400、與在波長500nm中之面 内的最大折射率與最小折射率的差(雙折射)Δη500之比 (△η4〇〇/Αη50〇)未達1. 05之1/2波長板與1/4波長板組 ©合’其具體例(實施例〉中,係組合分別由環狀聚烯烴樹脂 膜所構成之1/4波長板與1/2波長板。環狀聚烯烴樹脂膜 光彈後係數小至約4xl0_13cm2/dyne,故於貼合不均或白 斑之抑制亦有效。 但’使聚碳酸酯膜或環狀聚烯烴樹脂膜延伸時,若使 延伸倍率太大,會因為其膜厚變薄而使面内相位差值變 j因此,為顯現所希望的相位差值,锌一種膜均必須某 種程度地確保其膜厚,而無法因應依照市場尋求之膜薄的 要求。 320734 5 200928521 又,聚碳酸酯或環狀聚烯烴樹脂中係很難藉橫延伸而 製作完全單軸性之相位差膜,而不得不依賴縱延伸。一般 於縱延伸中,寬方向係成為自由端,於延伸膜產生縮進 (neck-in),故很難製作膜薄的相位差膜。 . 再者,在最近,就薄膜化之一方法而言,已研究藉液 '晶性化合物之塗佈顯現相位差。但,形成如此之塗佈型的 相位差膜時,液晶性化合物一般而言係含有具芳香環之液 晶原(Mesogen),故有波長分散成為正分散,或使液晶性化 合物之配向適於相位差膜之單軸配向性的單域(m 〇 η 〇 domain)乃很難之問題。再者,在其製造時之乾燥步驟易產 生膜厚不均,亦有面内之相位差报難控制之問題。 因此,本發明之課題係在於提供一種相位差膜,其厚 度極薄,同時相位差之波長分散為平坦,當組合1/4波長 板與1/2波長板而形成廣帶域1/4波長板時顯現良好的遮 光性能,且可解決貼合時之貼合不均或白班且包含單軸性 Q 的1/4波長板或1/2波長板。 又,本發明之再另一課題在於提供一種相位差膜,其 延料製作大致完全的單祕膜,_達成薄膜化 與見廣化’利用效率優異。 【發明内容】 亦即 ㈣靜^ ,可提供—_位差膜,再你由 伸膜所構成,且厚度為25㈣以下,面 S i: 權,範圍,而且,當使膜之 内遲相軸方向的折射率為ηχ、面内進相財向之折射率 320734 6 200928521 ny、厚度方向之折射率為ηζ時, 以式:Nz=(nx-nz)/(nx-ny) 所定義之Nz係數在0. 9至1. 1的範圍。 構成此相位差膜之聚丙烯樹脂係宜由含有1〇 窃 下之乙稀基單元的丙稀與乙烯的共聚物所構成。又ϊο以 者為該聚丙烯樹脂係實質上由丙烯單獨聚合物所構’、較佳 聚丙烯掛脂係宜含有造核劑。 成。該 ❹ Ο 上述相位差膜可調整其面内相位差值,以發揮 長板之功能。又,亦可調整其面内相位差值,以 波 波長板之功能。 1/2 若依本發明,可提供一種橢圓偏光板,其係將上、 相位差膜層合於直線偏光板上而構成。具體而言,例=之 ^述發揮1/4波長板功能的相位差膜層合於直線偏光將 可形成橢®偏光板。又,將上述之發揮1/4波長 膜、與上述之發揮1/2波長板之功能的相位差: 玲。,並進一步於其1/2波長板側層合直線偏光 形成橢圓偏光板。 j、可 再者’若依本發明,亦可提供一種液晶顯示I 係將上述任一去 、置,其 側而成怯者之橢圓偏光板被層合於液晶單元之至少一 【實施方式】 「以下,詳細說明本發明之實施形態。 L相位差膜] 在本發明中係以聚丙烯樹脂之橫延伸膜構成相位差 320734 7 200928521 膜。由於聚丙烯樹脂膜具有結晶性,故相位差值的顯現率 .極高,藉延伸而可簡單地得到大的相位差值。因此,可以 薄的膜厚得到具有所希望的相位差值之相位差膜。 又,由於聚丙稀樹脂之在波長4〇〇nm中之面内的最大 折射率與最小折射率的差(雙折射)△“〇〇、與在波長5〇〇nm '中之面内的最大折射率與最小折射率的差(雙折射)ΔΜΟΟ 之比(Δι^ΟΟ/Δη500)未達1· 〇5,故將分別以聚丙烯樹脂 所構成之1/2波長板、與1/4波長板予以組合而形成廣帶 域的1/4波長板時,可得到優異的遮光性能。在本說明書 中係以上述之Δη400/Δη500之值而定義為相位差的波長 分散。亦僅稱之為「波長分散」。 再者’聚丙烯樹脂之光彈性係數約小至2U0—W/ dyne ’故貼合1/2波長板與1/4波長板時,或貼合於直線 偏光板時,可抑制貼合不均或白斑。尚且發現,由於聚丙 稀樹脂能以咼倍率延伸’故能以橫延伸製作完全單軸性的 〇 薄膜。藉此’可同時連成薄膜化與寬廣化,利用效率優異。 使從如此之聚丙烯樹脂所製膜的素材膜進行橫延伸, 而使其顯現相位差。此時,可使相位差膜的膜厚為25#m 以下。其膜厚更宜為20/zm以下。若膜厚超過25#m,薄 膜化之優點很難有效地發揮。又’若其膜厚太小,於薄膜 ,易產生皺折等,有捲取或貼合時之操作性惡化之傾向。因 此’其膜厚宜為以上’更宜為以上。 當薄膜之面内遲相轴方向的折射率為ηχ、面内進相轴 方向(與遲相轴於面内正交之方向)之折射率為ny、厚度方 320734 8 200928521 向之折射率為nz、且使厚度為d時,面内之相位差值(Ro)、 厚度方向之相位差值(Rth)、及Nz係數係分別以下式(I)、 (II)及(III)定義。 Ro=(nx-ny)xd (I) Rth=[(nx+ny)/2-nz]xd (II) Nz=(nx-nz)/(nx-ny) (III) 又,從此等之式(I)、(II)及(III),Nz係數與面内之 相位差值(Ro)及厚度方向之相位差值(Rth)之關係係可以 ®下述之式(IV)表示。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a retardation film composed of a polypropylene resin and an elliptically polarizing plate using the retardation film. More specifically, it relates to a retardation film which can make a film thickness extremely thin, and an elliptical polarizer which is extremely thin in film thickness using the film. The present invention is also directed to a liquid crystal display device using the elliptically polarizing plate. [Prior Art] Ο ❹ In recent years, liquid crystal displays that consume low power, operate at low voltage, and are lightweight and thin have been rapidly popularized as information display devices such as mobile phones, mobile information terminals, computer monitors, and televisions. Along with the development of liquid crystal technology, liquid crystal displays or optical components of various modes have been proposed, and the response speed, contrast, viewing angle, and wide-band domain have been improved. _ In a reflective or transflective liquid crystal display represented by a mobile phone, etc., an elliptically polarizing plate is used, which is a retardation film that functions as a quarter-wave plate, or 1/4 The wavelength plate is combined with the 1⁄2 wavelength plate; the wide band is used as a retardation film that functions as a 1⁄4 wavelength plate, and is intended to be a low-profile optical polarizer. Such an elliptically polarizing plate, in particular, a circle =:=: a stop function 'in all applications, for the human eye to be clear, and all of the incident light expected to obtain ... can sufficiently suppress the good light-shielding performance of the internal counter-piece to j. In the retardation film, the difference between the wavelengths and the wavelength of the 1/4 wavelength plate is set, and the phase that functions as the 1/2 wavelength plate is used as the 1/4 320734 for the incident light in the wide wavelength region. 200928521 ^The so-called wide-band domain 1/4 wavelength plate function of the wavelength plate has been implemented since the past. For example, in Japanese Patent Laid-Open No. Hei 5-100114 (Patent Document υ, it has been disclosed that the combination is made of a polycarbonate film. An example of a 1⁄4 wavelength plate and a 1⁄2 wavelength plate. However, in a wide-band domain 1⁄4 wavelength plate using polycarbonate, it is necessary to function as a complete 174-wavelength plate at all wavelengths. Difficult, • Again, it is difficult to adequately control the internal reflection, and good shading performance is not obtained. Furthermore, the photoelastic coefficient of the polycarbonate film is as high as about 27xl (T13cm2/dyne, so it will be attached to the linear polarizer) There is a problem of unevenness of the bonding, or a white spot phenomenon in which the light of the backlight is partially leaked in the black display due to the change in the degree of use/inversion. Therefore, in the publication of "Kemoto Tekai Kai", No. 4,490,15 (Patent Document) 2) Medium 'disclosed: making the in-plane in the wavelength 4〇〇nm The difference between the maximum refractive index and the minimum refractive index (birefringence) Δη400, and the difference between the maximum refractive index and the minimum refractive index (birefringence) Δη500 in the plane at a wavelength of 500 nm (Δη4〇〇/Αη50〇) The 1/2 wavelength plate and the 1⁄4 wavelength plate group are not combined with each other. In the specific example (in the embodiment), the quarter-wave plate and the ring-shaped polyolefin resin film are respectively combined. /2-wavelength plate. The coefficient of photoelasticity of the cyclic polyolefin resin film is as small as about 4x10_13cm2/dyne, so it is effective in suppressing unevenness or white spot. But 'extend the polycarbonate film or the cyclic polyolefin resin film When the stretching ratio is too large, the in-plane retardation value becomes j because the film thickness is thinned. Therefore, in order to develop a desired phase difference value, a film of zinc must have a certain thickness to ensure its film thickness. However, it is not possible to respond to the requirements of thin film sought by the market. 320734 5 200928521 In addition, in polycarbonate or cyclic polyolefin resin, it is difficult to make a completely uniaxial retardation film by lateral stretching, and it has to rely on longitudinal stretching. Generally, in the longitudinal extension, the wide direction becomes the free end, and is extended. The film is produced by a neck-in, so that it is difficult to produce a film having a thin retardation film. Further, in recent years, in one of the methods of thin film formation, the coating appearance of a liquid crystal compound has been studied. However, when such a coating type retardation film is formed, the liquid crystal compound generally contains a liquid crystal precursor having an aromatic ring, so that the wavelength dispersion is positively dispersed or the alignment of the liquid crystal compound is caused. A single domain (m 〇η 〇 domain) suitable for the uniaxial alignment of the retardation film is difficult. Further, the drying step at the time of manufacture tends to cause uneven film thickness, and also has an in-plane phase difference. Reporting problems that are difficult to control. Therefore, the subject of the present invention is to provide a retardation film which is extremely thin and has a wavelength dispersion of a phase difference which is flat. When a quarter-wavelength plate and a 1/2 wavelength plate are combined to form a wide-band domain 1/4 wavelength The plate exhibits good light-shielding properties, and can solve the unevenness of the bonding or the 1/4 wavelength plate or the 1/2 wavelength plate including the uniaxial Q. Further, another object of the present invention is to provide a retardation film which is formed into a substantially complete mono-secret film, which is excellent in utilization efficiency. [Summary of the Invention] That is, (4) static ^, can provide - _ dislocation film, and then you are composed of a stretch film, and the thickness is 25 (four) or less, the surface S i: weight, range, and, when the film is within the retardation axis direction When the refractive index is ηχ, the refractive index of the in-plane phase-in-phase is 320734 6 200928521 ny, and the refractive index in the thickness direction is ηζ, the Nz coefficient defined by the formula: Nz=(nx-nz)/(nx-ny)范围范围内。 The range of 0.9 to 1.1. The polypropylene resin constituting the retardation film is preferably composed of a copolymer of propylene and ethylene containing 1 Å of the stolen ethylene unit. Further, it is preferable that the polypropylene resin is substantially composed of a propylene single polymer, and it is preferable that the polypropylene hang-hanging agent contains a nucleating agent. to make. The 相位 Ο The retardation film can adjust the in-plane retardation value to function as a long board. In addition, it is also possible to adjust the in-plane phase difference value to function as a wave wavelength plate. 1/2 According to the present invention, an elliptically polarizing plate which is formed by laminating an upper and a retardation film on a linear polarizing plate can be provided. Specifically, the retardation film which functions as a quarter-wave plate function in the example = laminated to linearly polarized light can form an ellips® polarizing plate. Further, the above-described 1/4 wavelength film is used to exhibit a phase difference from the above-described function of the 1/2 wavelength plate: Ling. And further linearly polarizing the 1/2 wavelength plate side to form an elliptically polarizing plate. j. Further, according to the present invention, it is also possible to provide a liquid crystal display, in which at least one of the above-mentioned elliptically polarizing plates is laminated and laminated to a liquid crystal cell. "The embodiment of the present invention will be described in detail below. L retardation film] In the present invention, a phase difference of 320734 7 200928521 is formed by a transversely stretched film of a polypropylene resin. Since the polypropylene resin film has crystallinity, the retardation value The rate of development is extremely high, and a large phase difference can be easily obtained by extension. Therefore, a phase difference film having a desired phase difference can be obtained with a thin film thickness. Also, since the polypropylene resin is at a wavelength of 4 The difference between the maximum refractive index and the minimum refractive index in the plane of 〇〇nm (birefringence) Δ“〇〇, the difference between the maximum refractive index and the minimum refractive index in the plane at the wavelength 5〇〇nm′ (double The ratio of refracting ΔΜΟΟ (Δι^ΟΟ/Δη500) is less than 1·〇5, so a 1⁄2 wavelength plate made of a polypropylene resin and a 1⁄4 wavelength plate are combined to form a wide band 1 When the /4 wavelength plate is used, excellent light shielding performance can be obtained. In the present specification, the wavelength dispersion of the phase difference is defined by the value of Δη400/Δη500 described above. It is also called "wavelength dispersion". Furthermore, the photoelastic coefficient of the polypropylene resin is as small as 2U0-W/dyne', so that when the 1/2 wavelength plate and the 1/4 wavelength plate are attached, or when laminated to a linear polarizing plate, uneven bonding can be suppressed. Or white spots. It has also been found that since the polypropylene resin can be stretched at a 咼 magnification, it is possible to produce a completely uniaxial ruthenium film by lateral stretching. Thereby, it can be simultaneously thinned and broadened, and the utilization efficiency is excellent. The material film formed from the film made of such a polypropylene resin was laterally stretched to exhibit a phase difference. At this time, the film thickness of the retardation film can be made 25 μm or less. The film thickness is preferably 20/zm or less. If the film thickness exceeds 25 #m, the advantage of thin film formation is difficult to effectively exert. Further, if the film thickness is too small, wrinkles are likely to occur in the film, and the handling property at the time of winding or bonding tends to deteriorate. Therefore, it is preferable that the film thickness is preferably "above". When the refractive index of the in-plane axis of the film is ηχ, the in-plane phase axis direction (the direction orthogonal to the retardation axis in the plane) is ny, and the thickness is 320734 8 200928521. When nz and the thickness d, the in-plane phase difference (Ro), the thickness direction phase difference (Rth), and the Nz coefficient are defined by the following formulas (I), (II), and (III), respectively. Ro=(nx-ny)xd (I) Rth=[(nx+ny)/2-nz]xd (II) Nz=(nx-nz)/(nx-ny) (III) Again, from this (I), (II), and (III), the relationship between the Nz coefficient and the phase difference (Ro) in the plane and the phase difference (Rth) in the thickness direction can be expressed by the following formula (IV).

Nz=Rth/Ro+0. 5 (IV) 在本發明之相位差膜中,面内之相位差值(Ro)為70至 400nm的範圍,尤其更宜在80至330nm的範圍。厚度方向 之相位差值(Rth)宜在28至240nm的範圍。又,Nz係數為 0. 9至1. 1的範圍,尤宜在0. 95至1. 05的範圍。只要從 此等的範圍,配合所適用之液晶顯示裝置要求之特性,而 φ 適當選擇即可。此處,若Nz係數約為1,在上述式(III) 中表示ny與nz約相等之意味,此種相位差膜係成為大鼓 完全的單軸性者。 [聚丙烯樹月旨] 構成本發明之相位差膜的聚丙烯樹脂係丙烯之單獨聚 合物或丙烯與其他共聚合性共單體的共聚物。丙烯之單獨 聚合物相較於丙烯與其他共聚合性共單體的共聚物,結晶 化度較高,故可更提昇薄膜剛性與降伏強度。因此,藉由 從丙烯之單獨聚合物構成相位差膜,俾可更提昇相位差膜 9 320734 200928521 製作步驟、偏光板化步驟及與τν之貼合步驟的處理性。 構成本發明之相位差膜的聚丙烯樹脂可使用公知之聚 合用觸媒’而單獨聚合丙烯之方法、或將丙烯與其他之共 1合性共單體進行共聚合之方法來製造。公知之聚合用觸 媒係可舉例如以下者。 (1) 由以鎂、鈦、及齒素作為必須成分之固體觸媒成分 所構成的Ti-Mg系觸媒; (2) 於以鎂、鈦及i素作為必須成分之固體觸媒成分 中’組合有機紹化合物、與依需要之電子供與性化合物等 之第三成分的觸媒系; (3) 單點聚合觸媒(Metan〇cene)系觸媒等。 ❹ 在此等觸媒系之中,於本發明之相位差膜所使用之聚 丙烯樹脂的製造中’最為—般者可使用於以鎮、鈦及齒素 作為必須成分之固體觸媒成分中,組合有機鋁化合物與電 子供與|±化合物者。更具體地,有機紹化合物較佳係可 例如三乙某叙、—田 4 齡物、四丁基銘、三乙基銘與氣化二乙基&之 土一鋁氧烷(alumoxane)等,就電子供與性化 ;兵=較佳?可舉例如環己基乙基二甲氧基石夕烷、、第三 環^Α 氧基錢、第三丁基乙基二甲氧基魏、二 裱戍基一甲氧基發燒等。 成分二:::曰、鈦及函素作為必須成分之固體觸媒 61-2_4t^本特開昭㈣細6號公報、日本特開昭 日本㈣平7-2_7號公«記狀 早點聚合觸媒系觸媒係可舉例如曰本特許第 320734 10 200928521 2587251號公報、日本特許第2627669號公報、日本特許 ' 第2668732號公報等記載之觸媒系。 聚丙烯樹脂係可依如下方法來製造:使用以己烧、庚 烷、辛烷、癸烷、環己烷、曱基環己烷、苯、曱苯、二曱 苯之烴化合物為代表之隋性溶劑的溶液聚合法;使用液狀 • 的單體作為溶劑之塊狀聚合法;使氣體之單體直接聚合的 氣相聚合法等。以此等之方法進行聚合係亦可以批式進 行,亦可以連續式進行。 ® 聚丙烯樹脂之立體規則性亦可為同排(isotactic)、對 排(syndiotactic)、亂排(atactic)之任一者。在本發明 中,從对熱性之點,宜使用對排或同排之聚丙烯樹脂。 在本發明所使用之聚丙烯樹脂係可以丙烯的單獨聚合 物構成外,亦可為以丙烯作為主體並使其與可與其共聚合 之共單體以少量(例如20重量%以下,宜10重量%以下)之 比率共聚合者。進行共聚合時,共單體之量宜為1重量% ❹ 以上。 被共聚合於丙烯之共單體例如可為乙烯、或碳原子數 4至20之α-烯烴。此時之α-烯烴具體而言可舉例如以下 者。 1-丁烯、2-甲基-1-丙烯(以上C4); 1-戊烯、2-曱基-1-丁烯、3-曱基-1-丁烯(以上C5); 1~己稀、2_乙基-1_丁婦、2,3_二曱基_1_丁稀、2 -曱 基-1-戍烯、3-曱基-1-戊烯、4_甲基-1-戊烯、3, 3-二曱基 _1-丁婦(以上C6); 11 320734 200928521 1 -庚稀、2~甲基+己烯、2,3_m—戍烯、2_乙 基-1-戊烯、2-甲基—3__乙基丁烯(以上C7),· 1_辛稀、5~甲基+庚烯、2-乙基-1-己烯、3,3_二甲 基1己烯2甲基、3_乙基_卜戊烯、2 3 4一三甲基-卜戊 烯、2-丙基-1-戊埽、23_二乙基_卜丁稀(以上⑻;Nz = Rth / Ro + 0.5 (IV) In the retardation film of the present invention, the in-plane phase difference (Ro) is in the range of 70 to 400 nm, particularly preferably in the range of 80 to 330 nm. The phase difference (Rth) in the thickness direction is preferably in the range of 28 to 240 nm.范围范围内。 The range of 0. 9 to 1. 05, especially in the range of 0.95 to 1. 05. As long as the range is within the range, the characteristics required for the liquid crystal display device to be applied can be matched, and φ can be appropriately selected. Here, if the Nz coefficient is about 1, it means that ny and nz are approximately equal in the above formula (III), and such a retardation film is a uniaxial property in which the drum is completely uniaxial. [Polypropylene tree] The polypropylene resin constituting the retardation film of the present invention is a single polymer of propylene or a copolymer of propylene and another copolymerizable comonomer. The propylene alone polymer has a higher degree of crystallization than the copolymer of propylene and other copolymerized comonomers, so that the film rigidity and the lodging strength can be further improved. Therefore, by forming a retardation film from a single polymer of propylene, the retardation film can be further improved. The process of the production step, the polarizing plate forming step, and the bonding step with τν can be further improved. The polypropylene resin constituting the retardation film of the present invention can be produced by a method of separately polymerizing propylene using a known polymerization catalyst, or a method of copolymerizing propylene with another co-combination comonomer. The known catalyst for polymerization can be exemplified by the following. (1) Ti-Mg-based catalyst composed of a solid catalyst component containing magnesium, titanium, and dentate as essential components; (2) in a solid catalyst component containing magnesium, titanium, and i as essential components 'A catalyst system that combines an organic compound and a third component such as an electron-donating compound as needed; (3) A single-site polymerization catalyst (Metan〇cene) is a catalyst. Among these catalyst systems, in the manufacture of the polypropylene resin used in the retardation film of the present invention, the most common ones can be used in solid catalyst components containing iron, titanium and dentate as essential components. , combined with organoaluminum compounds and electrons supplied with |± compounds. More specifically, the organic compound is preferably, for example, a triethyl sulfonate, a 4-year-old, a tetrabutylamine, a triethylamine, and a vaporized diethyl &alumoxane; Electronic supply and sex; soldiers = better? For example, cyclohexylethyldimethoxy-xanthene, a third ring-oxycarbonyl group, a tert-butylethyldimethoxy-wei, a decyl-monomethoxy group or the like can be mentioned. Ingredient 2:::Antimony, titanium and a solid element as a necessary component of the solid catalyst 61-2_4t^ This special open (4) fine 6th bulletin, Japan's special open Japan (4) flat 7-2_7 public « note early aggregation touch The catalyst system described in, for example, Japanese Patent No. 320734 10 200928521 2587251, Japanese Patent No. 2627669, and Japanese Patent No. 2668732. The polypropylene resin can be produced by using a hydrocarbon compound such as hexane, heptane, octane, decane, cyclohexane, nonylcyclohexane, benzene, toluene or diphenyl. A solution polymerization method using a solvent; a bulk polymerization method using a liquid monomer as a solvent; a gas phase polymerization method in which a monomer of a gas is directly polymerized. The polymerization system can be carried out in batches or in a continuous manner. ® The stereoregularity of polypropylene resin can also be any of isotactic, syndiotactic, and atactic. In the present invention, it is preferred to use a polypropylene resin in a row or in the same row from the point of heat resistance. The polypropylene resin used in the present invention may be composed of a single polymer of propylene, or may be propylene as a main component and a small amount (for example, 20% by weight or less, preferably 10% by weight) of the comonomer copolymerizable therewith. % below) the ratio of the co-aggregators. When the copolymerization is carried out, the amount of the comonomer is preferably 1% by weight or more. The co-monomer copolymerized with propylene may be, for example, ethylene or an α-olefin having 4 to 20 carbon atoms. Specifically, the α-olefin at this time may, for example, be the following. 1-butene, 2-methyl-1-propene (above C4); 1-pentene, 2-mercapto-1-butene, 3-mercapto-1-butene (above C5); Dilute, 2_ethyl-1_丁妇, 2,3_dimercapto-1_butylene, 2-mercapto-1-decene, 3-mercapto-1-pentene, 4-methyl- 1-pentene, 3, 3-dimercapto-1-dean (above C6); 11 320734 200928521 1 - heptano, 2~methyl + hexene, 2,3_m-nonene, 2_ethyl- 1-pentene, 2-methyl-3__ethylbutene (above C7), · 1_octane, 5~methyl + heptene, 2-ethyl-1-hexene, 3,3_2 Methyl 1 hexene 2 methyl, 3-ethyl-p-pentene, 2 3 4-trimethyl-p-pentene, 2-propyl-1-pentanyl, 23-diethyl-butadiene Above (8);

1-壬烯(C9);卜癸烯(cl〇);卜十一碳烯(cii);卜十 二礙烯(C12) ; 1-十三碳稀(C13);卜十四碳稀(c⑷:卜 十五碳烯(C15) ’卜十六碳稀(G16);卜十七碳埽(c⑺; 1-十八碳烯(C18) ; 1 —十九碳烯^“)等。 α烯烃之中較佳者係碳數4至12的江—烯烴,具體而 言係可舉例如1-丁缔、2_f基_卜丙烯;卜戊稀、2—甲基 -1-丁婦、3-甲基+丁缔;卜己埽、2_乙基+丁缔、2,3_ 二甲基一卜丁烯、2~甲基+戊烯、3-甲基+戊烯、4—甲基 -1-戊稀、3, 3-二甲基一卜丁烯;i一庚烯,2_甲基+己烯、 2,3 一曱基1戊烯、2_乙基_卜戊烯、2_甲基—3—乙基—卜 丁婦,1辛婦、卜甲基―卜庚烯、2-乙基-1-己婦、3 3_: 甲基-卜己烯、2—甲基+乙基+戊稀、23,4_三甲^一卜 戊烯:2-丙基-1—戊埽、2,3_二乙基+丁烯;卜壬婦.;卜 癸烯’ l-十-碳烯;p十二碳料^從共聚合性之觀點, 更且為1 丁烯、卜戊烯、卜己烯及卜辛烯,尤宜為卜丁 稀及1 -己稀·。 共聚物係可為隨機共聚物,亦可為嵌段共聚物。 較佳之共聚物係可舉例如丙稀/乙烯共聚物或丙稀/卜 丁婦共聚物。在丙烯/乙烯共聚物或丙烯/1-丁婦共聚物 320734 12 200928521 w 中例如藉由r高分子分析手冊」(1995年、紀伊國屋書 七、第616頁記載的方法進行紅外線(Ir)光譜測 了求知乙稀單元的含量或1_ 丁烯單元的含量。 • 、、Λ提歼作為相位差膜之透明度或加工性之觀點,係宜 =豆烯作為主體而形成與任意之不飽和烴的隨機共聚 、且為與乙烯之共聚物。形成共聚物時,丙烯以外 =飽和煙類係以使其共聚合比率成為】至重量%左右 © 二夕χ^更铨之共聚合比率為3至7重量%。藉由使丙烯以 七 和烴類的單元為1重量%以上’有出現提昇加工性 或^明性之效果的傾向。另外,若其比率超過1〇重量%, 樹脂之融點降低’有耐熱性變差之傾向,故不佳。又,設 成2種類以上之共單體與聚丙烯之共聚物時,源自於其共 聚物所含有之全部共單體的單元之合計量宜為前述範圍。 本發明之相位差膜所使用的聚丙烯樹脂係依據JIS K7210 ’以溫度23(rc、荷重21. 18N所測定之熔融流動率 ❹(MFR)為〇. 1至200g/l〇分鐘,尤其,宜在〇 5至5〇g/1〇 分鐘的範圍。藉由使用MFR在於此範圍之聚丙烯樹脂,可 在不對押出機施加大的負荷之狀態下,得到均一的膜狀物。 係衫阻礙本發明之效果的範圍、,亦可 收劑、抗靜電劑、滑劑、造核劑、=:化劑、㈣線吸 抗氧化劑中可舉例如酚系抗氧化劑、:系結塊劑等: 抗氧化劑、阻胺系光安定劑等 糸氧化劑、硫系 一併具有例如•、機構與 320734 13 200928521 紫外線吸收劑可舉例如2-經基二苯 並三,'之紫外線㈣劑、苯甲酸酷 靜電劑亦可為聚合物型、募聚物 之高級脂肪酸醯胺、如硬脂酸之高級脂肪酸及== 結塊劑係球狀或相球狀之形狀的微粒子, 機均可使用。此等之添加物亦可併用複數種:,、 有 Ο1-decene (C9); decimene (cl〇); b-undecene (cii); 卜12 olefin (C12); 1-trifluorocarbon (C13); c(4): b-pentadecene (C15) 'b-hexadecene (G16); b-seven-carbon ruthenium (c(7); 1-octadecene (C18); 1-19-nonene) "", etc. Preferred among the olefins are the hydrocarbon-olefins having a carbon number of 4 to 12, and specific examples thereof include 1-butane, 2-f-based propylene, pentylene, 2-methyl-1-butene, and 3 -Methyl+Butane; Buhexium, 2_Ethyl+Butane, 2,3-Dimethyl-P-butene, 2-Methyl+Pentene, 3-Methyl+Pentene, 4-Methyl -1-pentene, 3,3-dimethyl-butene; i-heptene, 2-methyl+hexene, 2,3-mercapto-1 pentene, 2-ethyl-p-pentene, 2_Methyl-3-ethyl-Bu Ding, 1 Xin, Bu-M-Heptene, 2-Ethyl-1-hexyl, 3 3_: Methyl-Bhexene, 2-Methyl+B Base + pentacene, 23,4_trimethyl-p-pentene: 2-propyl-1 -pentanyl, 2,3-diethyl+butene; 壬 壬.; 癸 ' ' l- 十 - Carbene; p-dodecene material ^ from the viewpoint of copolymerization, more is 1 butene, pentene, hexene and The alkene is particularly preferably dibutyl and 1-hexacene. The copolymer may be a random copolymer or a block copolymer. Preferred copolymers are, for example, propylene/ethylene copolymer or propylene/卜丁妇 copolymer. In the propylene/ethylene copolymer or propylene/1-butan copolymer 320734 12 200928521 w, for example, by the method described in the r Polymer Analysis Manual (1995, Kiyokiya VII, p. 616) The infrared (Ir) spectrum is used to determine the content of the ethylene unit or the content of the 1-butene unit. • The viewpoint of transparency and workability of the retardation film is determined by the choice of peasene as the main body. Random copolymerization of unsaturated hydrocarbons and copolymerization with ethylene. When forming a copolymer, propylene is not saturated with saturated copolymers so that the copolymerization ratio is about 5% by weight. The ratio is from 3 to 7% by weight, and the propylene has a tendency to improve workability or clarity by using seven or more hydrocarbon units. In addition, if the ratio exceeds 1% by weight, Resin melting point reduces 'heat resistance In the case where a copolymer of two or more kinds of comonomers and polypropylene is used, the total amount of units derived from all the comonomers contained in the copolymer is preferably in the above range. The polypropylene resin used in the retardation film of the present invention is based on JIS K7210', and has a melt flow rate ❹ (MFR) measured at a temperature of 23 (rc, load 21.18 N) of from 1 to 200 g/l , minute, in particular, It is preferably in the range of 5 to 5 〇g / 1 〇 minutes. By using a polypropylene resin having an MFR in this range, a uniform film can be obtained without applying a large load to the extruder. The range of the effect of the present invention, the absorbing agent, the antistatic agent, the slip agent, the nucleating agent, the chemical agent, and the (4) wire absorbing antioxidant may, for example, be a phenolic antioxidant or an agglomerate. Agents and the like: antioxidants, amine-blocking stabilizers, and the like, and sulphur-based oxidants, for example, and mechanisms 320730 13 200928521 ultraviolet absorbers such as 2-perylene dibenzotriene, 'ultraviolet (four) agents, The benzoic acid static electrostatic agent may also be a polymer type, a polymer of a higher fatty acid guanamine, a higher fatty acid such as stearic acid, and a == agglomerating agent in the form of spherical or spheroidal particles, which can be used. . These additives may also be used in combination with multiple types:

G 本發明所使用之造核劑可為無機造核劑、有機造核劑 之任一者。無機造核劑可舉例如滑石、黏土俨 = 又,有機造核劑可舉例如芳香族敌酸之金屬鹽二二; 填酸之金屬鹽類等金屬鹽類、高密度聚乙烯、聚令甲基丁 稀-卜聚環朗、聚乙烯基環己科。此等之中,亦二 有機造核劑’更宜為前述之金屬鹽類及高密度聚乙稀。又, 造核劑對聚丙烯樹脂之添加量宜為0 01至3重量Ρ 為0.05至1.5(wt%)。以上之添加物亦可併甩複數種。且 [聚丙烯樹脂之原材膜] 聚丙烯樹脂係可以任意的方法進行製膜而形成原材 膜。此原材膜係透明實質上無面内相位差者。例如,藉由: 來自溶融獅之押出成形法;使轉於有機溶劑之樹曰脂垂 流於平板上’並除去溶劑而進行製膜之溶雜鑄法等,而 可得到實質上無面内相位差之聚丙烯樹脂的原材膜。 做為製造原材膜之方法的例子者,係詳細說明有關以 押出成型之製膜法。聚丙烯樹脂係在押出機中藉螺桿之旋 轉而熔融混練,從T模頭押出成片狀。所押出之熔二狀= 320734 14 200928521 片的溫度為180至300〇C左右。若此時之熔融狀薄片的溫 度降低於18(Tc,延展性不充分,所得到之薄膜的厚度變 成不均’有可能成為具有相位差不均之薄膜。. 又’若其溫度超過3〇(TC,易引起樹脂之劣化或分解, * 於薄片中產生氣泡,或含有碳化物。 押出機係可為單軸押出機,亦可為雙軸押出機 。例如,G The nucleating agent used in the present invention may be any of an inorganic nucleating agent and an organic nucleating agent. Examples of the inorganic nucleating agent include talc and clay 俨. Further, the organic nucleating agent may, for example, be a metal salt of an aromatic acid or a dicarboxylic acid; a metal salt such as a metal salt filled with an acid, a high-density polyethylene, or a poly-cable Keding thin - Bu Polycyclic, polyvinylcyclohexyl. Among these, the organic nucleating agent' is more preferably the aforementioned metal salt and high-density polyethylene. Further, the nucleating agent is preferably added to the polypropylene resin in an amount of from 0 to 3 parts by weight, preferably from 0.05 to 1.5 (% by weight). The above additives may also be plural. [Original material film of polypropylene resin] The polypropylene resin can be formed into a film by any method. The raw material film is transparent and substantially free of in-plane retardation. For example, it is possible to obtain a substantially no-in-plane method by a method of extruding a molten lion; a method of forming a film by transferring a resin rot on an organic solvent to a flat plate and removing the solvent to form a film; Raw material film of polypropylene resin with phase difference. As an example of a method for producing a raw material film, a film forming method for extrusion molding is described in detail. The polypropylene resin was melted and kneaded by a screw in an extruder, and extruded from a T die into a sheet shape. The melted flakes = 320734 14 200928521 The temperature of the flakes is about 180 to 300 〇C. If the temperature of the molten flakes at this time is lowered to 18 (Tc, the ductility is insufficient, and the thickness of the obtained film becomes uneven), it may become a film having a phase difference unevenness. Further, if the temperature exceeds 3 〇 (TC, easily causes deterioration or decomposition of the resin, * generates bubbles in the sheet, or contains carbides. The extruder can be a single-axis extruder or a two-axis extruder. For example,

單軸押出機之情形中,螺桿之長度L與直徑d之比、即l/D Ο 為24至36左右,屬於在樹脂供給部之螺紋溝的空間容積、 - . 與樹脂計量部中之螺紋溝的空間容積的比(前者/後者)之 壓縮比為1.5至4左右,可使用全螺紋型(fuii fight type)、阻障型(barrier type)、或進一步具有 Maddock 型 之混練部分之型式等的螺桿。從抑制聚丙烯樹脂之劣化或 分解、均一地熔融混練之觀點’宜使用L/D為28至36, 壓縮比為2. 5至3. 5之阻障型螺桿。又,為了可有效地抑 制聚丙烯樹脂之劣化或分解,押出機内宜形成氮環境或真 ❹二再者,為了除去因I丙稀樹脂劣化或分解所產生.的揮 發氣體,較宜於押出機之前端設有lmm0以上5mm0以下之 微孔,並提高押出機前端部分的樹脂壓力。所謂將微孔之 押出機前端部分的樹脂壓力予以提高係意指使前端之背壓 提高,藉此可提高押出之安定性9所使用之微孔的直秤 宜為2mm0以上以下。 二文 於押出所使用之T模頭係宜於樹脂之流路表面 段差或刮傷者,又其唇部分較宜以與熔融之聚丙:微 之間的摩擦係數小之材料來鍍覆或塗覆,進一步〜2樹 32〇734 15 200928521 =丨砧成〇.3咖0以下之尖銳的邊緣形狀者。摩擦係 去用、如;斗可舉例如碳化鵡系或氟系的特殊鍍覆等。藉由 如八槿^ τ_ ’可抑制眼排出物的產生,同時並可抑 制刀模線’故可得到外觀均-性優之樹脂膜。此τ模頭之 分歧管較宜為為衣架形狀,且滿足以τ之條件⑴或⑵, 更宜滿足條件(3)或(4)。 度 >180mm ...(1) T模頭的唇寬為1500fflm以上時;T 度 >220mm 時;T模頭的高度方向 Ο τ模頭的唇寬為未達15〇〇mm時;Τ模頭的厚度方向長 度 >180mm ...(1) 模頭的厚度方向長 T模頭的唇寬為未達1500mm 度 >250mm ...(3) T模頭的唇寬為15〇〇匪以上時;τ模頭的高度方向長 度 >280mm ...(4) 藉由使用滿足如此之條件的T模頦,可對T模頭内部 ❹之溶融狀聚丙烯樹脂的流動進行整流,且,即使在唇部部 刀亦可邊抑制厚度不均一邊進行押出’故可得到厚度精 度優異且相位差更均一的原材膜。 從抑制聚丙烯樹脂之押出變動的觀點’宜於押出機與 T模頭之間介由接頭而安裝齒輪泵。又,為了除去位於聚 丙烯樹脂中之異物,宜安裝葉片式過瀘器(leaf disk filter)。 從T模頭所押出之熔融狀薄片係被挾押於金屬製冷却 輥(亦稱冷却輥(chi 11 roller)或澆鑄輥(casting 320734 16 200928521 .r°ller))、與接於該金·冷她之周方向進行旋轉並含 .有彈性體的接觸輥之間,而進行冷却固化,以得到所^ 的膜。此時,接觸輥可為將橡膠等之彈性體直接 面者,亦可將彈性體輥之表面以金屬套筒所構成之外= 被覆者。使用將彈性_之表面以金屬套筒所構成之: 同予以被覆的接觸輥時,一般係於金屬製冷却輕與接觸輕 之間,直接挾住聚丙稀樹脂之溶融狀薄片進行冷却。另一 ❹ 方面,使用表面為彈性體之接觸輥時,亦可於聚__旨 之熔融狀薄片與接觸輥之間介置熱塑性樹脂的雙轴延伸膜 而予以挾壓。 、 ❹ 使聚丙烯樹脂之熔靴薄片以如上述之冷城與接觸 輥挾住而使其冷却固化時,冷却輥與接觸輥任-者均須預 先降低其表面溫度’以急速冷却熔融狀薄片。例如,兩輥 之表面溫度宜調整至以上30。〇以下之範圍。若此等之 表面溫度超過3(rc,溶融狀薄片之冷却固化花時間,故聚 丙稀樹月曰中之結晶成分會成長,所得到之薄膜係有時透明 性f。輥之表面溫度較佳係未達3(TC,更佳係未達25。〇。 Ϊ合,若輕之表面溫度低於〇°C,金屬製冷却輥的表 曰而有水滴附著’而有使薄膜之外觀惡化之傾向。In the case of a uniaxial extruder, the ratio of the length L of the screw to the diameter d, that is, l/D Ο is about 24 to 36, which is the space volume of the thread groove in the resin supply portion, - and the thread in the resin metering portion. The ratio of the space volume of the groove (the former/the latter) is about 1.5 to 4, and a fuii fight type, a barrier type, or a mixed type of the Maddock type may be used. Screw. The barrier-type screw having a compression ratio of 2.5 to 3.5, and a compression ratio of 2.5 to 3.5, is preferably used. Further, in order to effectively suppress the deterioration or decomposition of the polypropylene resin, it is preferable to form a nitrogen atmosphere or a true enthalpy in the extruder, and to remove the volatile gas generated by the deterioration or decomposition of the I propylene resin, it is preferable to use the extruder. The front end is provided with micropores of lmm0 or more and 5 mm or less, and the resin pressure of the front end portion of the extruder is increased. Increasing the resin pressure at the tip end portion of the microporous extruder means that the back pressure of the tip end is increased, whereby the straight scale of the micropores used for improving the stability of the extrusion 9 is preferably 2 mm0 or less. The T-die used in the extrusion is suitable for the surface of the resin with poor surface or scratches, and the lip portion is preferably plated or coated with a material having a small coefficient of friction with the molten polypropylene: , further ~ 2 trees 32 〇 734 15 200928521 = 丨 anvil into a 〇. 3 coffee 0 below the sharp edge shape. The friction system may be used, for example, a special type of carbonization or fluorine-based plating. By, for example, 槿^ τ_ ' can suppress the generation of ocular effluent, and at the same time, the stencil line can be suppressed, so that a resin film having an excellent uniform appearance can be obtained. The branch pipe of the τ die is preferably in the shape of a hanger, and satisfies the condition (1) or (2) of τ, and more preferably satisfies the condition (3) or (4). Degree >180mm ...(1) When the lip width of the T die is 1500fflm or more; T degree >220mm; the height direction of the T die Ο τ The lip width of the die is less than 15〇〇mm; The thickness direction of the die is 180 mm (1) The thickness of the die is long. The lip width of the die is less than 1500 mm. 250 mm (3) The lip width of the T die is 15 When the 〇〇匪 is above; the height of the τ die is 280 mm (4) By using a T die that satisfies such conditions, the flow of the molten polypropylene resin inside the T die can be performed. By rectifying, even if the lip blade is used, it is possible to suppress the thickness unevenness and perform the extrusion. Thus, a raw material film having excellent thickness precision and uniform phase difference can be obtained. From the viewpoint of suppressing the change in the extrusion of the polypropylene resin, it is preferable to mount a gear pump between the extruder and the T die via a joint. Further, in order to remove foreign matter located in the polypropylene resin, a leaf disk filter is preferably installed. The molten sheet extruded from the T die is held by a metal cooling roll (also known as a chill roll (chi 11 roller) or a casting roll (casting 320734 16 200928521 .r°ller)), and is connected to the gold The film is rotated in the circumferential direction of the cold and contains the elastic contact roller, and is cooled and solidified to obtain the film. In this case, the contact roller may be formed by directly coating an elastic body such as rubber, or the surface of the elastomer roller may be made of a metal sleeve. The surface of the elastic _ is made of a metal sleeve: When the contact roller is coated, it is generally cooled between the metal cooling light and the contact light, and directly smashes the molten sheet of the polypropylene resin to be cooled. On the other hand, when a contact roll having an elastic surface is used, a biaxially stretched film of a thermoplastic resin may be interposed between the molten sheet and the contact roll. ❹ When the polypropylene resin sheet is cooled and solidified by the cold water and the contact roller as described above, both the cooling roll and the contact roll must be previously lowered in surface temperature to rapidly cool the molten sheet. . For example, the surface temperature of the two rolls should be adjusted to above 30. 〇 The following range. If the surface temperature exceeds 3 (rc, the cooling and solidification time of the molten sheet is delayed, the crystal component in the polypropylene sap will grow, and the obtained film may have transparency f. The surface temperature of the roll is preferably The system is less than 3 (TC, more preferably less than 25. Ϊ. If the surface temperature is lower than 〇 ° C, the surface of the metal chill roll is attached with water droplets, and the appearance of the film is deteriorated. tendency.

,膣ϋί用之金屬製冷却輥之表面狀態會轉印至聚丙烯樹 面,故其表面有凹凸時,有可能降低所得到之聚 膜的厚度精度。因此,金屬製冷卻輥之表面宜儘 二ΐ士:鏡面狀態。具體而言,金屬製冷卻輥之表面粗度 网度的標準數列表示,宜為G. 3S以下,更宜為〇. 1S 320734 17 200928521 ^ 至 0.2S。 • 關於形成與金屬製冷卻輥之央持(nip)部分之接觸 親,其彈性體中之表面硬度’就於JIS K6301所規定之彈 箸式硬度試驗(A形)所測定的值而言,宜為65至80,更宜 為70至80 °藉由使用如此之表面硬度的橡膠輥,可容易 地均一地維持施加於熔融狀薄片之鍊壓,且,於金屬製冷 部輥與接觸輕之間不會產生熔融狀薄片的滯料堤(bank;樹 ❹脂滯留),而容易地形成膜。 挾壓熔融狀薄片時之壓力(線壓)係係將接觸輥押抵於 金屬製冷部輥之壓力來決定。線壓係宜為50N/cm以上 3〇〇N/cm以下者’更宜為lOON/cm以上250N/Cm以下者。 藉由使線壓為前述範圍,不形成滞料堤,而容易地一邊雄 持一定的線壓一邊製造聚丙烯樹脂膜。 於金屬製冷卻輥與接觸輥之間,挾壓聚丙烯樹脂之熔 融狀薄片以及熱塑性樹脂的雙軸延伸膜時,構成此雙軸延 ❹伸膜之熱塑性樹脂係只要為不與聚丙烯樹脂牢固地熱熔接 之樹脂即可’具體上,可舉例如聚酯、聚醯胺、聚氣化乙 烯、聚乙烯醇、乙烯-乙烯醇共聚物、聚丙烯腈等。此等之 中,最宜為以溫度或熱等所致之尺寸變化少的聚酯。此時 之雙軸延伸膜之厚度一般為5至50#m左右,宜為1〇至 30 /z m ° 在此方法中,宜使從T模頭的唇部到被金屬製冷卻輥 與接觸輥挾壓之距離(空氣間隙)為2〇〇腿以下,更宜予以 設為160mm以下。從τ模頭所押出之熔融狀薄片係從唇部 320734 18 200928521 至輥之間被拉伸,而易產生配向。#由如 =,可得到配向更小之薄膜。空氣間隙之下限^ 使用之金>1製冷卻輥的徑與接_之徑 的前端形狀來決定,-般為5_以上。斤使用之唇部 以此方法製造聚丙烯樹脂膜時之加工速度係由用以广 却固化熔融狀薄片所需的時間來決定。 7The surface state of the metal chill roll used for 膣ϋί is transferred to the polypropylene tree surface, so that when the surface has irregularities, the thickness accuracy of the obtained film may be lowered. Therefore, the surface of the metal chill roll should be as good as two gentlemen: mirror state. Specifically, the standard number of surface roughness of the metal cooling roll is expressed by a standard number of lines, preferably G. 3S or less, more preferably 〇. 1S 320734 17 200928521 ^ to 0.2S. • For the contact with the nip portion of the metal chill roll, the surface hardness in the elastomer is the value measured by the elastic hardness test (A shape) specified in JIS K6301. It is preferably 65 to 80, more preferably 70 to 80 °. By using such a rubber roller having a surface hardness, the chain pressure applied to the molten sheet can be easily and uniformly maintained, and the roll and the contact in the metal refrigerating portion are light. A stagnation bank (bank; tree stagnation) which does not produce a molten sheet is formed, and a film is easily formed. The pressure (linear pressure) at the time of rolling the molten sheet is determined by pressing the contact roller against the pressure of the metal refrigerating section roll. The line pressure system is preferably 50 N/cm or more and 3 〇〇 N/cm or less. More preferably, it is 1OO/cm or more and 250 N/cm or less. By setting the linear pressure to the above range, a polypropylene resin film can be easily produced while maintaining a constant line pressure without forming a stagnant bank. When the molten sheet of the polypropylene resin and the biaxially stretched film of the thermoplastic resin are pressed between the metal cooling roll and the contact roll, the thermoplastic resin constituting the biaxially stretched stretched film is not strong with the polypropylene resin. The resin to be geothermally welded can be specifically mentioned, for example, polyester, polyamine, polyglycolized ethylene, polyvinyl alcohol, ethylene-vinyl alcohol copolymer, polyacrylonitrile or the like. Among these, it is most preferable that the polyester has a small dimensional change due to temperature or heat. The thickness of the biaxially stretched film at this time is generally about 5 to 50 #m, preferably about 1 to 30 /zm °. In this method, it is preferable to make the lip from the T die to the metal cooling roller and the contact roller. The distance of the rolling (air gap) is 2 〇〇 or less, and it is more preferably set to 160 mm or less. The molten flakes extruded from the τ die are stretched from the lips 320734 18 200928521 to the rolls, and are easily aligned. #由如, can get a smaller film. The lower limit of the air gap is determined by the shape of the front end of the diameter of the cooling roller used in the gold >1, and is generally 5 or more. The lip used in the production of the polypropylene resin film in this way is determined by the time required to broadly cure the molten sheet. 7

❹ m徑變大’由於熔融狀薄片與該冷却輥接 變長,故可以更高的速度來製造n, 的金屬製冷卻輥時,加玉速度最大為5至2Gm/分鐘左:。 =金屬製冷卻輥與接觸輥之間所抉壓线融狀薄片係 藉由純之接觸進行冷㈣化。而且,依需要於端部形成 m俘:r機捲取而成為膜。此時,至使用膜為止 之間’為㈣其表面,亦可以在於其單面或雙面貼合 一熱塑性樹脂所構成的表面保護膜之狀態下予以捲取 將聚丙烯樹脂之㈣㈣片料熱難樹脂所構成之雙= 延伸膜一起於金屬製冷卻輥與接觸輥之間予以挾壓之情形 中,亦可使該雙軸延伸膜成為一方之表面保護薄祺。月 [相位差膜之製造方法]. 、 本發明之相位差膜係可藉由使如前述之由聚丙婦樹脂 所構成的原材膜進行橫延伸而製造。此處,所謂横延伸係 使從輕所捲出之長型膜朝寬方向(橫方向)延伸之情形。' 橫延伸一般係具有以下之步驟。 (A)將原材膜以聚丙烯樹脂之融點附近的預熱溫产予 以預熱之預熱步驟; 320734 19 200928521 * (Β)對被預熱後之膜以低於前述預熱溫度的延伸溫度 朝橫方向進行延伸之延伸步驟;及 ^ (C)使已朝橫方向延伸之膜熱固定的熱固定步騍。 Ο 代表性橫延伸的方法可舉例如拉張器法。拉張器法/ 為將已藉由夾頭(chuck)固定膜寬方向的兩端之原材祺係 烘箱中以加寬夾頭間隔之方式進行延伸之方法。使用於$ 張器法之延伸機(拉張器延伸機)一般係具備在進行預熱= 驟之區域、進行延伸步驟之區域、及進行熱固定步驟^區 域中,可獨立地調節各別的溫度之機構。藉由使用如此二 拉張器延伸機而進行橫延伸,可得到軸精度優異,且具 均一的相位差之相位差膜。' 橫延伸之預熱步驟係設置於使臈朝橫方向延伸之步驟 之前的步驟,係為將膜加熱至為了延伸臈之充分溫度的步 驟。預熱步驟之預熱温度係意指進行烘箱的預熱步驟之區 域的環境溫度,係採用所延伸之聚丙烯樹脂膜的融點附近 ❹之溫度。所延伸之膜的預熱步驟中之滯留時間宜為3〇至 120秒。此預熱步驟中之滯留時間不足30秒時,於延伸歩 驟中膜被延伸時會有應力分散,而對作為相位差膜之轴精 度或相位差均一性造成不利的影響的可能性,又,其滞留 時間超過120秒時’係受熱至必要以上,而有膜會部分地 融解,而垂下(下垂)之可能性。預熱步驟中之滯留時間更 宜為30至60秒。 橫延伸之延伸步驟係使膜朝寬方向延伸之步驟。在此 延伸步驟之延伸溫度一般為低於預熱溫度之溫度。延伸步 20 320734 200928521 驟之延伸溫㈣意餘制线行延伸㈣㈣域中之環 境溫度。藉由使被韻過謂錢於職步狀溫度進行 延伸’可均—地延伸膜,結果,可得到光軸及相位差的均 -性優異之相位差膜。延伸溫度宜較賴步驟中之預熱溫 度低5至m:,更宜為低7至15t。此時之延伸倍率係於 顯現先軸之方向(成為遲相_方向)配合必須之相位差值 從3至10倍左右的範圍適當選擇即可,較佳係3至6倍的 耗圍。藉由使此時之延伸倍率為3倍以上,可使前述之Nz 係數為u至ι·丨之範m面,若延伸倍率太大, 有可能損及相位差值之均—性,故宜止於ig倍左右。 橫延伸之熱固定步驟係以維持延伸步驟終了時之膜寬 的狀態’為使該膜通過烘箱内之預定溫度的區域之步驟。 為了有效地提昇膜之相位差或光軸等光學特性的安定性, 熱固定溫度宜為從較延伸步驟之延伸溫度低代之溫度至 較延伸溫度高3〇°C之温度的範圍内。 ☆橫延伸之步驟亦可進一步具有熱緩和步驟。關於此熱 緩和步驟’在&張器法中_般係在延伸步驟與熱固定步驟 之間進行,一般係設定成,熱緩和的區域可與其他之區域 獨立地設定溫度。具體而言,熱緩和步驟係在延伸步驟中 使膜延伸至預定的寬之後,為除去無用的應力,使夾頭的 間隔變窄達數%,一般係較延伸終止時之間隔變窄〇 5至 7%左右。 [使用來作為波長板時之光學特性] 使用本發明之相位差膜作為1/4波長板時,其面内相 320734 21 200928521 位差值(Ro)宜在70至160nm的範圍,更宜為8〇至15〇nm . 的範圍。1/4波長板係具有分別使以直線偏光進行入射之 光變換成以圓偏光為首之橢圓偏光,或者使以圓偏光為首 之橢圓偏光進行入射之光變換成直線偏光而射出之功能。 •另一方面,使用本發明之相位差膜作為1/2波長板時,其 • 面内相位差值(Ro)宜在240至400nm的範圍,更宜為26〇 至330nm的範圍。1/2波長板係具有使直線偏光之方向旋 轉之功能。 ❹[翻偏光板] 藉由將1/4波長板以預定之軸角度與直線偏光板層 合,或與1/2波長板同時地以預定之軸角度與直線偏光板 層合,從而可形成橢圓偏光板。第1圖係用以對本發明之 橢圓偏光板的一形態,說明表示層構成的截面示意圖及軸 角度之關係的圖’第2圖係用以對本發明之橢圓偏光板的 另一形態,說明表示層構成的截面示意圖及軸角度之關係 ❹ 的圖。 參照第1圖之(A),於本發明之一形態中,係將由前述 之聚丙烯樹脂膜所構成的1/4波長板1〇層合於直線偏光板 20,而可形成橢圓偏光板30。此時係參照第1圖之(B), 以直線偏光板20之吸收軸22為基準’以逆時針方向為正, 使到達1/4波長板10之面内遲相軸12的角度0成為4〇至 5〇度(較佳係約成為45度)之方式進行配置,藉此具有大 致為圓偏光板之功能。或者,以直線偏光板2〇之吸收轴 22為基準,以逆時針方向為正,使到達1/4波長板^之 320734 22 200928521 面内遲相軸12的角度θ成為i3〇至14〇度(較佳係約成為 • 135度)之方式進行配置,藉此具有大致為圓偏光板功能。 以下,表示角度時,係與此處說明同樣,相對於基準軸而 使逆時針為正。 又,參照第2圖之(Α) ’於本發明之另一形態中,係分 .別將由前述之聚丙烯樹脂膜所構成的1/4波長板1()與1/2 波長板15層合,並進一步於該1/2波長板15側層合直線 偏光板20,而可形成橢圓偏光板35。此時係參照第2圖之 ® (Β) ’以直線偏光板20之吸收軸22為基準,使到達1/2波 長板15之面内遲相軸π的角度$成為1〇至2〇度(較佳係 約成為15度)’使從1 /2波長板15之面内遲相軸17至1 /4 波長板10之面内遲相軸12的角度ψ成為55至65度(較佳 係約成為60度)之方式進行配置,而使其具有大致為圓偏 光板之功能。或者,以直線偏光板2〇之吸收軸22為基準, 使達至1/2波長板15之面内遲相軸π的角度0成為1〇〇 ❹至110度(較佳係約成為1〇5度),使從丨/2波長板15之面 内遲相軸17至1/4波長板1〇之面内遲相軸12的角度诅成 為55至65度(較佳係約成為60度)之方式進行配置,則仍 然使其具有大约為圓偏光板之功能。後者之關係(從直線偏 光板之吸收轴至1/2波長板之面内遲相軸的角度為1〇〇至 110度)’係相當於在第2圖(Β)中使符號22改讀為「直線 偏光板之穿透軸」的狀態。在直線偏光板中,吸收軸與透 過軸係於面内呈正交之關係。 如第2圖所示般,使1/4波長板10與1/2波長板15 320734 23 200928521 層合者係在可見光區域的廣波長範 • 1/4波長板發揮功能,於其1/2波長’、廣帶域)作為 板20之橢圓偏光板35係於廣帶 :=:線偏光 光,或使圓偏光變換成直線偏光。再者直換成圓偏 •亦可降低反射防止效果之角度依存性。曰此地構成, • 直線偏光板20係為被賦與有:吸收且有羊 面的直線偏充,並使具有與其正交 ^ 向之振動 ❹ :光穿透的功能之光學元件’而可為域線 板。藉由使雙色性色素吸附配向於聚乙;線偏光 述,可賦與:吸收具有某方向的振動面之直“光,如上 具有與其正交之方向的振'動面之直線=先’並使 色性色素係可使用蛾或雙色性有機染料。藉=力能。雙 色後之餐處理,可得到:偏色^素所進行之染色、及染 :::2。之透明保護層係例如能藉 以往 =1件的保護層之三乙醯基纖維素(二 ===之乙醯基,_膜構成t _' b a 冰片烯樹脂為代表之環狀聚烯烴樹脂 、、、聚丙烯樹脂之臈、聚艨、 聚(甲^丙稀酸曱酯之膜等所構成。乙一酉曰樹如 當製作橢圓偏光板時,於波長板 合、戒 波長板間α/4波長板與1/2波長板)之=使用例如 24 320734 200928521 感麗接著劑(黏著劑)。感壓接著劑係尤宜使用以透明性及 • 耐久性優異之丙烯酸聚合物為主體者。感壓接著劑層之厚 度係一般為5至50/zm之範圍。 如以上所構成之橢圓偏光板30, 35係可於其1/4波長 • 板10之面側配置感壓接著劑(黏著劑)’而使其可貼合於液 • 晶單元(cell)。使此橢圓偏光板層合於液晶單元的至少一 者之側,構成液晶顯示裝置。可於液晶單元之雙面配置此 橢圓偏光板,亦可於液晶單元之單面配置此橢圓偏光板, ❹ 於另一面配置另一偏光板。當貼合於液晶單元時,以1/4 波長板10侧面向液晶早元之方式配置。 [液晶顯示裝置] 第3圖及第4圖中分別以模式性截面圖表示於液晶單 元的雙面配置本發明之橢圓偏光板的液晶顯示裝置之例。 第3圖係表示將屬於第1圖(A)所示之1/4波長板10與直 線偏光板20的層合物之橢圓偏光板30配置於液晶單元50 ^ 的兩侧之例。亦即,在此例中,於液晶單元50之下侧介由 感壓接著劑層40,而使由1/4波長板10/直線偏光板20所 構成的橢圓偏光板30以令其1/4波長板10侧面向液晶單 元50之方式予以層合,亦於液晶單元60之上側,介由感 壓接著劑層40,使由1/4波長板10/直線偏光板20所構成 的橢圓偏光板30以令其1/4波長板1〇側面向液晶單元50 之方式予以層合。各別之橢圓偏光板30係以令其直線偏光 板20之吸收軸正交之方式配置。將此液晶顯示裝置作為穿 透塑或半穿透反射型予以使用時,係於一方之橢圓偏光板 25 320734 200928521 的外側(在圖中係下側)配置背光60。 ' 第4圖係表示將屬於第2圖(A)所示之174波長板10、 1/2波長板15與直線偏光板20的層合物之橢圓偏光板35 配置在液晶單元50的兩側之例。亦即,在此例中,於液晶 * 單元50之下侧介由感壓接著劑層40,使由1/4波長板 • 10/1/2波長板15/直線偏光板20所構成的橢圓偏光板35, 以令其1/4波長板10側面向液晶單元50之方式予以層 合,亦於液晶單元50之上側,介由感壓接著劑層40,使 ® 由1/4波長板10/1/2波長板15/直線偏光板20所構成的 橢圓偏光板35,以令其1/4波長板10側面向液晶單元50 之方式予以層合。各別之橢圓偏光板35係以令其直線偏光 板20之吸收軸正交之方式配置。將此液晶顯示裝置作為穿 透型或半穿透反射型予以使用時,亦於一方之橢圓偏光板 的外侧(在圖中係下側)配置背光60。 以下將顯示實施例而更具體地說明本發明,但本發明 ❹ 係不受此等之例限定。例中,表示含量之%只要無特別記載 均為重量基準。 [實施例1] (a)l/4波長板之製作 對含有乙烯單元約5%之丙烯/乙烯隨機共聚物[由住友 化學(股)販售之“住友NoblenW151” ]進行製膜,得到厚 40/zm之原材膜。將此原材膜以拉張器橫延伸機朝橫單軸 進行延伸。延伸係以線速度1〇m/分鐘、首先通過溫度被調 節至131°C之預熱區域、繼而於溫度被調節至i21°C之延伸 26 320734 200928521 區域使最終的延伸倍率 測機器(股)製之相位差,、、' °之方式來進行。以王子計 差測疋裝置“K0BRA-21ADH”測定所 2差值Rth N r目位差膜)的面内相位差值1^。、厚度方向相 ,之數位測微計“MH、15m,,測以度,其結果表示絲= 中。此相位差膜之面肉士 / μ 内相位差值R〇為14〇nm,為作為1/4 波長板發揮功能者。❹ m diameter becomes large. Since the molten flakes are connected to the chill roll, it is possible to produce a metal chill roll at a higher speed, and the jade speed is at most 5 to 2 Gm/min left:. = The rolled line of the rolled wire between the metal cooling roll and the contact roll is cooled (four) by pure contact. Further, as needed, a m-capture:r machine is wound up at the end to form a film. In this case, the surface of the film is "four", and the surface of the (4) (four) sheet of the polypropylene resin may be taken up in a state in which the surface protective film composed of a thermoplastic resin is bonded to one side or both sides. In the case where the stretched film is pressed together between the metal cooling roll and the contact roll, the biaxially stretched film may be formed into one surface protection thinner. [Manufacturing method of retardation film] The retardation film of the present invention can be produced by laterally stretching a raw material film composed of the above-mentioned polypropylene-based resin. Here, the lateral extension is a case where the long film rolled out from the light is extended in the width direction (lateral direction). 'Horizontal extension generally has the following steps. (A) a preheating step of preheating the raw material film with a preheating temperature near the melting point of the polypropylene resin; 320734 19 200928521 * (Β) for the preheated film at a temperature lower than the aforementioned preheating temperature An extension step of extending the temperature in the lateral direction; and (C) a heat-fixing step of thermally fixing the film extending in the lateral direction.代表性 Representative method of lateral stretching may be, for example, a stretcher method. The tensioner method is a method of extending the gap between the ends of the raw material in the width direction of the film by a chuck to widen the gap between the chucks. The extension machine (stretcher extension machine) used in the tensor method generally has an area in which the preheating step is performed, an area where the stretching step is performed, and a step of performing the heat fixing step, and the individual can be independently adjusted. The mechanism of temperature. By performing the lateral stretching using the two-stretcher stretching machine, a retardation film having excellent axial precision and a uniform phase difference can be obtained. The step of preheating the lateral extension is a step before the step of extending the crucible in the lateral direction, which is a step of heating the membrane to a sufficient temperature for extending the crucible. The preheating temperature of the preheating step means the ambient temperature in the region where the preheating step of the oven is carried out, and the temperature of the crucible near the melting point of the stretched polypropylene resin film is used. The residence time in the preheating step of the stretched film is preferably from 3 Torr to 120 seconds. When the residence time in the preheating step is less than 30 seconds, stress is dispersed when the film is extended in the stretching step, and the possibility of adversely affecting the axial precision or phase difference uniformity of the retardation film is When the residence time exceeds 120 seconds, it is heated to more than necessary, and there is a possibility that the film will partially melt and hang down (sagging). The residence time in the preheating step is preferably from 30 to 60 seconds. The step of extending the lateral extension is a step of extending the film in the width direction. The extension temperature in this extension step is generally a temperature lower than the preheating temperature. Extension step 20 320734 200928521 The extension temperature of the step (4) The residual line is extended (4) (4) The ambient temperature in the domain. By extending the film to the temperature of the step-like temperature, the film can be uniformly stretched, and as a result, a phase difference film excellent in uniformity of the optical axis and the phase difference can be obtained. The extension temperature should be 5 to m lower than the preheating temperature in the step, and more preferably 7 to 15 t lower. In this case, the stretching ratio is appropriately selected from the range of about 3 to 10 times in the direction in which the direction of the preceding axis (the direction of the late phase _ direction) is matched, and preferably 3 to 6 times. By making the stretching ratio at this time 3 times or more, the aforementioned Nz coefficient can be a range of u to ι·丨, and if the stretching ratio is too large, the uniformity of the phase difference may be impaired. Stop at around ig. The laterally extending heat-fixing step is a step of maintaining the film width at the end of the stretching step as a step of passing the film through a predetermined temperature in the oven. In order to effectively improve the phase difference of the film or the stability of the optical characteristics such as the optical axis, the heat setting temperature is preferably in a range from a temperature lower than the extension temperature of the stretching step to a temperature higher than the stretching temperature by 3 °C. ☆ The step of lateral extension may further have a heat relaxation step. The heat relaxation step ‘ is generally performed between the stretching step and the heat fixing step in the & tensor method, and is generally set such that the heat-relaxed region can be independently set with other regions. Specifically, the heat relaxation step is such that after the film is extended to a predetermined width in the stretching step, the interval of the chuck is narrowed by several % in order to remove unnecessary stress, and the interval is generally narrower than when the stretching is terminated. To about 7%. [Optical characteristics when used as a wavelength plate] When the retardation film of the present invention is used as a quarter-wave plate, the in-plane phase 320734 21 200928521 difference (Ro) is preferably in the range of 70 to 160 nm, more preferably The range of 8〇 to 15〇nm. The quarter-wavelength plate system has a function of converting light incident by linearly polarized light into elliptically polarized light including circularly polarized light, or converting light incident by elliptically polarized light including circularly polarized light into linearly polarized light and emitting the light. On the other hand, when the retardation film of the present invention is used as the 1/2 wavelength plate, the in-plane retardation value (Ro) is preferably in the range of 240 to 400 nm, more preferably in the range of 26 Å to 330 nm. The 1/2 wavelength plate has a function of rotating the direction of linear polarization. ❹[Flip polarizer] can be formed by laminating a quarter-wavelength plate with a linear polarizing plate at a predetermined axial angle, or laminating with a linear polarizing plate at a predetermined axial angle simultaneously with a 1⁄2 wavelength plate. Elliptical polarizer. 1 is a view showing a relationship between a cross-sectional view showing a layer structure and a shaft angle in an embodiment of an elliptically polarizing plate of the present invention. FIG. 2 is a view showing another embodiment of the elliptically polarizing plate of the present invention. A schematic diagram of the cross-sectional view of the layer structure and the relationship between the axial angles ❹. Referring to Fig. 1 (A), in one aspect of the present invention, a quarter-wavelength plate 1 made of the above-mentioned polypropylene resin film is laminated on the linear polarizing plate 20 to form an elliptically polarizing plate 30. . In this case, referring to Fig. 1(B), the counterclockwise direction is positive with respect to the absorption axis 22 of the linearly polarizing plate 20, and the angle 0 of the in-plane slow axis 12 reaching the quarter-wavelength plate 10 becomes The configuration is performed in a manner of 4 to 5 degrees (preferably about 45 degrees), thereby having a function of a substantially circular polarizing plate. Alternatively, based on the absorption axis 22 of the linear polarizing plate 2, the counterclockwise direction is positive, so that the angle θ of the in-plane slow axis 12 reaching the quarter wave plate 320734 22 200928521 becomes i3 〇 to 14 〇. It is preferably arranged in such a manner as to be approximately 135 degrees, thereby having a substantially circular polarizing plate function. Hereinafter, when the angle is expressed, the counterclockwise direction is positive with respect to the reference axis as described herein. Further, referring to Fig. 2 (Α), in another aspect of the present invention, the 1/4 wavelength plate 1 () and the 1/2 wavelength plate 15 layers composed of the above-mentioned polypropylene resin film are separated. Further, the linear polarizing plate 20 is further laminated on the side of the 1⁄2 wavelength plate 15 to form the elliptically polarizing plate 35. In this case, referring to FIG. 2 (Β) ' with the absorption axis 22 of the linear polarizing plate 20 as a reference, the angle $ of the in-plane slow axis π reaching the half-wavelength plate 15 is 1 〇 to 2 〇. (preferably, about 15 degrees) 'The angle ψ of the in-plane slow axis 12 from the in-plane phase axis 17 of the 1 / 2 wavelength plate 15 to the 1/4 wavelength plate 10 is 55 to 65 degrees (preferably It is configured in such a manner as to be approximately 60 degrees), so that it has a function of a substantially circular polarizing plate. Alternatively, the angle 0 of the in-plane retardation axis π of the half-wavelength plate 15 is set to 1 〇〇❹ to 110 degrees with respect to the absorption axis 22 of the linear polarizing plate 2 ( (preferably about 1 〇) 5 degrees), the angle 诅 of the in-plane slow axis 12 from the in-plane slow phase axis 17 to the quarter-wavelength plate 1 of the 丨/2-wavelength plate 15 is 55 to 65 degrees (preferably about 60 degrees) The way it is configured, it still has the function of being a circular polarizer. The relationship of the latter (from the absorption axis of the linear polarizing plate to the angle of the slow phase axis in the plane of the 1/2 wavelength plate is 1 〇〇 to 110 degrees) is equivalent to the rewriting of the symbol 22 in Fig. 2 (Β) It is the state of the "transparent axis of the linear polarizer". In the linear polarizing plate, the absorption axis and the transmission axis are orthogonal to each other in the plane. As shown in Fig. 2, the 1⁄4 wavelength plate 10 and the 1⁄2 wavelength plate 15 320734 23 200928521 are laminated to the wide-wavelength 1/4 wavelength plate in the visible light region, and 1/2 of them are used. The wavelength Å, the wide band, and the elliptically polarizing plate 35 as the plate 20 are connected to a wide band: =: linearly polarized light, or converted into circularly polarized light. In addition, it can be changed into a circular deviation. • The angle dependence of the reflection prevention effect can also be reduced.直线 地 • • • • • • • • • • • • 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线 直线Domain line board. By displacing the dichroic dye to the polyethylene, the linear polarization can be applied to: absorb the straight line of the vibration surface having a certain direction, and the straight line of the vibration surface having the direction orthogonal thereto = first For the coloring pigment system, a moth or a dichroic organic dye can be used. By the method of the two-color post-treatment, it is possible to obtain the dyeing of the color-developing pigment and the dyeing::: 2. The transparent protective layer is, for example. A cyclic polyolefin resin represented by the conventional protective layer of tridecyl cellulose (two === 醯 ,, _膜 constitutes t _' ba borneol resin, and polypropylene resin It is composed of a film of polyfluorene, poly(methyl acrylate), etc. When an ellipsoid is produced, the eucalyptus is at the wavelength plate, and the α/4 wavelength plate between the wavelength plates is 1/ 2 wave plate) = For example, use 24 320734 200928521 sensible adhesive (adhesive). Pressure-sensitive adhesives are preferably made of acrylic polymer with excellent transparency and durability. Pressure-sensitive adhesive layer The thickness system is generally in the range of 5 to 50/zm. As described above, the elliptically polarizing plate 30, 35 series can be 1/4 wavelength • A pressure-sensitive adhesive (adhesive) is disposed on the surface side of the board 10 so that it can be attached to a liquid crystal cell. The elliptical polarizer is laminated on at least one of the liquid crystal cells. On the side, the liquid crystal display device is configured. The elliptically polarizing plate can be disposed on both sides of the liquid crystal cell, and the elliptically polarizing plate can be disposed on one side of the liquid crystal cell, and the other polarizing plate can be disposed on the other side. In the case of the 1/4 wavelength plate 10, the liquid crystal display device is arranged on the side of the liquid crystal cell. [Liquid crystal display device] The ellipses of the present invention are arranged on both sides of the liquid crystal cell in a schematic cross-sectional view in FIGS. 3 and 4, respectively. Example of the liquid crystal display device of the panel. Fig. 3 is a view showing that the elliptically polarizing plate 30 which is a laminate of the quarter-wavelength plate 10 and the linear polarizing plate 20 shown in Fig. 1(A) is disposed in the liquid crystal cell 50 ^ For example, in this example, an elliptically polarizing plate composed of a quarter-wavelength plate 10/linear polarizing plate 20 is provided on the lower side of the liquid crystal cell 50 via the pressure-sensitive adhesive layer 40. 30 is laminated such that the side surface of the 1⁄4 wavelength plate 10 is directed to the liquid crystal cell 50, On the upper side of the liquid crystal cell 60, the elliptically polarizing plate 30 composed of the 1⁄4 wavelength plate 10 / the linear polarizing plate 20 is placed on the liquid crystal cell 50 by the side surface of the 1⁄4 wavelength plate 1 through the pressure sensitive adhesive layer 40. The elliptically polarizing plates 30 are arranged such that the absorption axes of the linear polarizing plates 20 are orthogonal to each other. When the liquid crystal display device is used as a penetrating plastic or semi-transparent reflection type, The backlight 60 is disposed on the outer side (the lower side in the figure) of one of the elliptically polarizing plates 25 320734 200928521. ' Fig. 4 shows a 174-wavelength plate 10 and a 1/2 wavelength plate which will be shown in Fig. 2(A) An example in which the elliptically polarizing plate 35 of the laminate with the linear polarizing plate 20 is disposed on both sides of the liquid crystal cell 50. That is, in this example, an ellipse composed of a quarter-wavelength plate • 10/1/2 wavelength plate 15/linear polarizing plate 20 is provided on the lower side of the liquid crystal* unit 50 via the pressure-sensitive adhesive layer 40. The polarizing plate 35 is laminated such that the side surface of the 1/4 wavelength plate 10 faces the liquid crystal cell 50, and also on the upper side of the liquid crystal cell 50, via the pressure sensitive adhesive layer 40, so that the 1/4 wavelength plate 10 is used. The elliptically polarizing plate 35 composed of the /1/2 wavelength plate 15/linear polarizing plate 20 is laminated such that the side surface of the quarter-wavelength plate 10 faces the liquid crystal cell 50. Each of the elliptically polarizing plates 35 is disposed such that the absorption axes of the linear polarizing plates 20 are orthogonal to each other. When the liquid crystal display device is used as a transmissive type or a transflective type, the backlight 60 is disposed on the outer side (the lower side in the figure) of one of the elliptically polarizing plates. The invention will be more specifically described below by showing examples, but the invention is not limited by the examples. In the examples, the % content is based on weight unless otherwise specified. [Example 1] (a) Preparation of a 1/4 wavelength plate A film of a propylene/ethylene random copolymer containing about 5% of an ethylene unit [Sumitomo Noblen W151" sold by Sumitomo Chemical Co., Ltd. was formed to obtain a thick film. 40/zm raw film. The raw material film is stretched toward the horizontal uniaxial axis by a stretcher transverse stretcher. The extension is at a line speed of 1 〇 m / min, first through the temperature is adjusted to 131 ° C in the preheating zone, and then the temperature is adjusted to i21 ° C extension 26 320734 200928521 area to make the final extension ratio measuring machine (share) The phase difference of the system is made, and the method of '° is used. The in-plane phase difference value 1^ of the difference Rth N r target film was measured by the odometer differential measuring device "K0BRA-21ADH". , the thickness direction phase, the digital micrometer "MH, 15m,, measured degrees, the result shows the wire = medium. The phase difference film of the phase difference film / μ internal phase difference R 〇 is 14 〇 nm, as The 1/4 wavelength plate functions as a function.

(b) 橢圓偏光板之製作 準備下述之直線偏光板[由住友化學(股)販售之“SR-W062” ]:具有藉由2片的三乙醯基纖維素膜挾住於聚乙烯 醇吸附配向有碘之偏光件膜之構造,並於其單面設有丙烯 酸系感壓接著劑層。另一方面,將上述(a)所製作之1/4波 長板朝離遲相軸45。的方向予以裁切,對其單面以累積照 射量1680J的條件實施電暈放電處理,於此電暈放電處理 後30秒以内使其電暈放電處理面貼合於上述直線偏光板 * * 的丙烯酸系感壓接著劑層側。此時,以令直線偏光板之吸 收轴與1/4波長板之遲相軸以45度的角度交叉之方式進行 配置。如此一來,得到於直線偏光板層合有由丙烯樹脂所 構成之1/4波長板的橢圓偏光板。 (c) 橢圓偏光板之橢圓率測定. 使用王子計測機器(股)製之相位差測定裝置“K0BRA-21ADH”測定於上述(b)所製作之橢圓偏光板的橢圓率。此 處,所謂橢圓率係指,從橢圓偏光板的直線偏光板侧入射 光時,從1/4波長板側射出之擴圓偏光之短轴的長度對長 27 320734 200928521 軸之長度的比。此例所得到之橢圓偏光板的橢圓率係 ’ 〇. 925。此係與使用後述之比較例1所示的降冰片埽樹脂所 構成之1/4波長板的橢圓偏光板之橢圓率925為同等之 值。 [實施例2] (另一 1/4波長板的製作) 對與實施例1所使用者相同之丙烯/乙烯隨機共聚物 [“住友Noblen W151” ]進行製膜而得到厚4〇Am之原材 〇 膜,並將此原材膜與實施例1之(a)同樣地以拉張器橫延伸 機朝橫單轴進行延伸。但線速度係變更成5m/分鐘,預熱 溫度係變更成136t:,延伸溫度係變更成126t:,最終的延 伸倍率係變更成4倍。所得到之延伸膜(相位差膜)的面内 相位差值Ro、厚度方向相位差值、Nz係數、相位差的 波長分散及厚度,係以與實施例丨之(&)同樣之方法進行測 定,其結果表示於表1中。此相位差膜之面内相位差值肋 ❹ 為90nm,為作為1/4波長板發揮功能者。 [實施例3] (1/2波長板的製作) 對與實施例1所使用者相同之丙烯/乙烯隨機共聚物 [“住友Noblen Ψ151” ]進行製膜,而得到厚6〇#ω之原 材膜2使此原材膜以拉張器橫延伸機朝橫單軸進行延伸 延伸係以線速度20m/分鐘、首先通過溫度被調節至126艺 之預熱區域、繼而於溫度被調節至116。〇之延伸區域以最 、’s的延伸倍率成為5倍之方式來進行。所得到之延伸膜(相 320734 28 200928521 、位差膜)的面内相位差值R〇、厚度方向相位差值Rth、Nz 係數及厚度,係以與實施例1之㈤同樣之方法進行測定, 其結果表示於表1中。此相位差膜係面内相位差值R〇為 28Onm ’為作為1/2波長板發揮功能者。 * [實施例4] '(a)l/4波長板的製作 對在熔融流動率8gdO分鐘且具有同排的立體規則性 之丙稀單獨聚合物中添加有京葉聚乙稀股份公司製高密度 聚乙烯G1900 1重量%之聚丙烯樹脂膜進行製膜,得到厚 40ym之原材膜。將此原材膜以拉張器橫延伸機朝橫單轴 進行延伸。延伸係以線速度5m/分鐘、首先通過溫度被調 谛至140C之預熱區域、繼而於溫度被調節至16〇。匸之延伸 區域、其後於被調節至12〇°c之熱固定區域以最終的延伸 倍率成為4倍之方式來進行。所得到之延伸膜(相位差膜) 的面内相位差值R〇、厚度方向相位差值Rth、心係數及相 ❹位差的波長分散’係以與實施例1之(a)同樣之方法進行測 定’其結果表示於表1中。此相位差膜係面内相位差值R〇 為150nm,為作為1/4波長板發揮功能者。 (b)橢圓偏光板之製作 準備下述之直線偏光板[由住友化學(股)販售之“ SR_ W062 ]:具有使於聚乙烯醇吸附配向有破之偏光件薄膜藉 由2片的三乙醯基纖維素薄膜挾住之構造,並於其單面設 有丙烯酸系感壓接著劑層。另一方面,將上述(a)所製作之 1 /4波長板朝離遲相轴45。的方向予以裁切’對其單面以累 29 320734 200928521 積照射量1680J的條件實施電暈放電處理,於此電暈放電 處理後30秒以内使其電暈放電處理面貼合於前述直線偏 光板的丙烯酸系感壓接著劑層侧。此時,以令直線偏光板 .之吸收軸與1/4波長板之遲相軸以45度的角度交叉之方式 進行配置。如此一來’得到於直線偏光板層合有由丙烯樹 脂所構成之1/4波長板的橢圓偏光板。 (c)橢圓偏光板之橢圓率測定 ❹使用王子計測機器(股;)製之相位差測定裝置“k〇bra_ 21ADH”測定於上述(〇所製作之橢圓偏光板的橢圓率。此 例所得到之橢圓偏光板的橢圓率係〇. 925。 [實施例5] 對與實施例4所使用者相同之聚丙烯樹脂膜進行製膜 而得到之厚40# m之原材膜,係與實施例4之(a)同樣地以 =張器橫延伸機朝橫單軸進行延伸。但線速度係變更成5 ^ / 。刀鐘,預熱溫度係變更成170¾,延伸溫度係變更成15〇 泛°C,熱固定溫度變更成12〇。(:,最終的延伸倍率係變更成3 '所得到之延伸膜(相位差膜)的面内相位差值、厚度 方向相位差值Rth、Nz係數、及厚度,係以與實施例1之 (a)同樣之方法進行測定,其結果表示於表i中。此相位差 面内相位差值R〇為97nm,為作為1/4波長板發揮功 [實施例6] 對與實施例4所使用者相同之聚丙烯樹脂膜進行製 、,而得到厚40/zm之原材膜。將此原材膜以拉張器橫延 320734 30 200928521 、伸機朝橫單轴進行延伸。其時之線速度係5m/分鐘,預熱 ,度係n〇°c,延伸溫度係160。〇,熱固定溫度係12(rc, 最終的延伸倍率係4倍。所得到之延伸膜(相位差膜)的面 •内相位差值R〇、厚度方向相位差值Rth、Nz係數、及厚度, 係以與實施例1之⑷同樣之方法進行測定,其結果表示於 表1中。此相位差膜之面内相位差值R〇為273nm,為作為 1/2波長板發揮功能者。 [實施例7] 〇 對在熔融流動率為8g/10分鐘且具有同排的立體規則 性之丙烯單絲合物進行製膜’而得到厚卿m之原材 ,’將此膜與實施例4之⑷同樣地以拉張器橫延伸機朝橫 單軸進行延伸。但線速度係變更成5m/分鐘,預熱溫度係 變更成⑽。c,延伸溫度係變更成14〇t,熱固定溫度係變 更成120。(: ’最終的延伸倍率係變更成4倍。所得到之延 伸膜(相位差膜)的面_位差值Rq、厚度方向相位差值 ❹Rth Nz係數、相位差的波長分散及厚度,係以與實施例1 之⑷同樣之綠進行測定’其結果表示於表丨巾。此相位 面内相位錄R。為U7nm,為作為1/4波長板發揮 功月&者。 [實施例8] π對與實施例7所使用者相同之聚丙騎脂膜進行製膜 厚40,之原材膜,係與實施例4之⑷同樣地以 ^讀延㈣錢單軸騎延伸。但料㈣變更成W 刀鐘,預熱溫度係變更成17〇〇c,延伸溫度係變更 320734 31 200928521 C,熱固疋溫度變更成120 C,最終的延伸倍率係變更成3 倍。所得到之延伸膜(相位差膜)的面内相位差值R〇、厚度 方向相位差值Rth、Nz係數及厚度,係以與實施例1之(日) .同樣之方法進行測定,其結果表示於表丨中。此相位差膜 之面内相位差值Ro為91nm ’為作為1/4波長板發揮功能 — 者。 [實施例9] 對與貫施例7所使用者相同之聚丙烯樹脂膜進行製膜 而得到之厚40//m之原材膜,係與實施例4之化)同樣地以 拉張器橫延伸機朝橫單軸進行延伸。但線速度係變更成5 m / 分鐘’預熱溫度係變更成17〇。(:,延伸溫度係變更成ι6〇 C,熱固定溫度變更成12(TC,最終的延伸倍率係變更成4 倍。所得到之延伸膜(相位差膜)的面内相位差值此、厚度 方向相位差值Rth、Nz係數、及厚度,係以與實施例i之 (a)同樣之方法進行測定,其結果表示於表i中。此相位差 ❹膜之面内相位差值Ro為277nm,為作為1/2波長板發揮功 能者。 [比較例1] 針對屬於降冰片烯樹脂膜被縱單軸延伸而成之1/4波 長板的相位差膜[由住友化學(股)販售之 “SES440140Z” ],以與實施例丨之(幻同樣之方法測定面 内相位差值Ro、厚度方向相位差值Rth、Nz係數、相位差 的波長分散及厚度,其結果表示於表丨中。除使用此相位 差膜以外,另外以與'實施例1之(b)同樣的方法製作橢圓偏 320734 32 200928521 ,並針玄對該橢圓偏光板以與實施例1之(Ο同樣的方法 谢疋槽圓率。橢圓偏光板之楕圓率為〇 925。 [比較例2 ] • 針對屬於降冰片婦樹脂膜被橫單轴延伸而成之^波 長板的相位差膜[由住友化學(股)販售之 ' “SES360140Y” ],以盥眚谕仓丨1 ° 以與實施例1之(a)同樣之方法測定面 内相位差值Ro、厚度方向相位差值咖、Μ係數及厚度, 其結果表不於表1中。 ❹[比較例3] 針對屬於降W _樹脂膜被縱單軸延伸而成之 1/2波 長板的相位差膜[(股)〇ptes販售之“ ZM_3〇〇,,卜以與實 %例1之(a)同樣之方法敎面内相位差值R。、厚度方向 相位差值Rth、Nz缝及厚度,其結絲示於表1中。 [比較例4 ] 對與實施例1所使用者相同之丙稀/乙稀隨機共聚物 〇 [“住友Noblen Wl51” ]進行製膜,而得到厚5〇歸之原 材膜使此原材膜朝縱單軸進行延伸。延伸係以線速度 分鐘、首先通過溫度被調節至n5〇c之預熱區域、繼雨於 Μ度被調Bp至118°C之延伸區域以最終的延伸倍率成為 1.37倍之方式來進行。所得到之延伸膜(相位差膜)的面内 相位差值Ro、厚度方向相位差值Rth、Nz係數、相位差的 波長分散及厚度’係以與實施例1之(a)同樣之方法進行測 疋’其結果表示於表1中。此相位差膜係面内相位差值Ro 為275nm,為作為1/2波長板發揮功能者。 33 320734 200928521 _ [表 1] 相位差膜之 材質* 延伸 形態 相位差膜之物性 ~~~ ^ Ro (nm) Rth (nm) Nz 波長分散 厚ί'' (nm) 實施例1 PP 橫 140 77 1.0 1.00 8.0 實施例2 PP 橫 90 46 1.0 1.00 9.0 實施例3 PP 橫 280 153 1. 0 — 12.7 實施例4 PP+造核劑 橫 150 J 79 1.0 1.00 --- 9.7 實施例5 PP+造核劑 橫 97 49 1.0 — 8.0 實施例6 PP+造核劑 橫 273 140 1.0 - 8.5 實施例7 PP 橫 147 75 1.0 1.00 9.3 實施例8 PP 橫 91 46 1.0 — 1 ---- 8.1 實施例9 PP 橫 277 145 1.0 一 8.2~~~ 比較例1 NOR 縱 140 67 1.0 1.01 45.5 比較例2 NOR 橫 139 149 1.6 一 62.0 比較例3 NOR 縱 298 150 1.0 — 116 比較例4 PP 縱 275 138 1.0 1.00 44. 〇 木相位差膜之材質 PP : 聚丙烯系 pp+造核劑:聚丙稀系+造核劑 N0R : 降冰片烯系 〇 在降冰片稀樹脂之情形’如比較例1及3所示般,藉 縱單軸延伸而使Nz係數約成為1之1 /4波長板及1 /2波長 板已被提供至市場上。但,關於其厚度,於1/4波長板(比 較例1)為45. 5/z m,於1/2波長板(比較例3)為116//m。 另一方面,如比較例所示2,關於降冰片烯樹脂之橫單軸 延伸品’亦有1/4波長板被提供於市場上,但其&係數為 1. 6 ’顯示雙軸性’厚度亦成為62#m。 320734 34 200928521 然而’如實施例1至9所示般,藉由使聚内婦樹月旨膜 以高倍率橫單軸延伸,可製造心係數約成為i之ι/4波長 板或1/2波長板,其厚度亦為25//m以下,可形成極薄。 另一方面,如比較例4所示,使聚丙烯樹脂膜進行縱單軸 延伸時,雖可得到1/2波長板,但因縮進而使厚度不會變 小,而很難實現本發明規定之25ym以下所謂極薄型者。 若參照第2圖而以先前所說明之軸角度層合實施例j 之(a)或實施例4之(a)所製作之1/4波長板、與實施例、 或實施例6所製作之1/2波長板,則可得到廣帶域之1/4 波長板。再者,於其丨/2波長板側,使實施例1之(b)或實 施例4之(a)所示之直線偏光板,參照第2圖而以先前所說 明之軸角度進行層合,則可得到廣帶域之橢圓偏光板(圓偏 (產業上之利用可能性) 本發明係使聚丙烯樹脂之延伸膜適用於相位差膜者, ❿籍此,可得到以厚25_以下之極薄之膜顯現所希望的相 位差值之效果。又,藉由採用聚丙烯樹脂膜,即使進行橫 延伸’ ^能以高倍率延伸,藉此,具有可製作大致完 輪性之賴之優點。再者,本發明之相位差職可藉橫延 伸製造,故亦具有在膜厚變薄之同時可加寬有效寬之優點。 〜本發明亦有助於層合有該相位差膜之液晶顯示裝置(b) Preparation of ellipsoidal polarizer The following linear polarizing plate [SR-W062" sold by Sumitomo Chemical Co., Ltd.] has two sheets of triethyl fluorene-based cellulose film stuck to polyethylene. The alcohol adsorbs a structure of a polarizing film having an iodine, and an acrylic pressure-sensitive adhesive layer is provided on one surface thereof. On the other hand, the quarter-wavelength plate produced in the above (a) is directed away from the retardation axis 45. The direction is cut, and a corona discharge treatment is performed on a single surface under the condition of a cumulative irradiation amount of 1680 J, and the corona discharge treatment surface is attached to the linear polarizing plate* within 30 seconds after the corona discharge treatment. The acrylic pressure sensitive adhesive layer side. At this time, the absorption axis of the linear polarizing plate and the slow axis of the quarter-wavelength plate are arranged at an angle of 45 degrees. In this manner, an elliptically polarizing plate in which a quarter-wave plate made of an acrylic resin was laminated on a linear polarizing plate was obtained. (c) Ellipticity measurement of the elliptically polarizing plate. The ellipticity of the elliptically polarizing plate produced in the above (b) was measured using the phase difference measuring device "K0BRA-21ADH" manufactured by Oji Scientific Instruments Co., Ltd. Here, the ellipticity refers to the ratio of the length of the short axis of the circularly polarized light emitted from the side of the 1/4 wavelength plate to the length of the axis of the length of 27 320734 200928521 when light is incident from the side of the linear polarizing plate of the elliptically polarizing plate. The ellipticity of the elliptically polarizing plate obtained in this example is '〇. 925. This is equivalent to the ellipticity 925 of the elliptically polarizing plate of the quarter-wave plate formed of the norbornene resin shown in Comparative Example 1 to be described later. [Example 2] (Production of another 1/4 wavelength plate) The propylene/ethylene random copolymer ["Sumitomo Noblen W151"] which was the same as the user of Example 1 was formed into a film to obtain a thick 4 〇Am original. The raw material film was stretched toward the horizontal uniaxial axis by a stretcher transverse stretching machine in the same manner as in the first embodiment (a). However, the linear velocity was changed to 5 m/min, the preheating temperature was changed to 136 t:, the elongation temperature was changed to 126 t:, and the final elongation ratio was changed to 4 times. The in-plane retardation value Ro, the thickness direction retardation value, the Nz coefficient, the wavelength dispersion of the phase difference, and the thickness of the obtained stretched film (retardation film) were carried out in the same manner as in the example (&). The results are shown in Table 1. The in-plane retardation rib ❹ of the retardation film is 90 nm, and functions as a quarter-wavelength plate. [Example 3] (Production of 1/2 wavelength plate) The propylene/ethylene random copolymer ["Sumitomo Noblen Ψ 151"] which was the same as the user of Example 1 was formed into a film to obtain a thick 6 〇 #ω The material film 2 extends the original film to the horizontal uniaxial axis by a stretcher transverse stretching machine at a linear velocity of 20 m/min, firstly adjusted to a preheating zone of 126 by the temperature, and then adjusted to a temperature of 116. . The extension area of the crucible is carried out in such a manner that the extension ratio of the maximum and the 's is five times. The in-plane retardation value R〇, the thickness direction retardation value Rth, the Nz coefficient, and the thickness of the obtained stretched film (phase 320734 28 200928521, the retardation film) were measured in the same manner as in the first embodiment (5). The results are shown in Table 1. This retardation film has an in-plane retardation value R 〇 of 28 Onm ′ which functions as a 1/2 wavelength plate. * [Example 4] '(a) Preparation of a 1/4 wavelength plate. High density made of Jingye Polyethylene Co., Ltd. was added to a propylene monomer having a melt flow rate of 8 gdO min and having stereoregularity in the same row. Polypropylene G1900 1% by weight of a polypropylene resin film was formed into a film to obtain a raw material film having a thickness of 40 μm. The raw material film is stretched toward the horizontal uniaxial axis by a stretcher transverse stretcher. The extension was adjusted to a preheating zone of 140 C at a line speed of 5 m/min, first by temperature, and then the temperature was adjusted to 16 Torr. The extended region of the crucible is thereafter carried out in such a manner that the heat-fixing region adjusted to 12 ° C is four times the final stretching ratio. The in-plane retardation value R〇, the thickness direction retardation value Rth, the core coefficient, and the wavelength dispersion of the phase difference of the obtained stretched film (retardation film) are the same as in the method of (a) of the first embodiment. The measurement was carried out. The results are shown in Table 1. This retardation film has an in-plane retardation value R 〇 of 150 nm and functions as a quarter-wavelength plate. (b) Preparation of elliptically polarizing plate The following linear polarizing plate [SR_W062] sold by Sumitomo Chemical Co., Ltd.: has a polarizing film made of polyvinyl alcohol adsorbed and detached by two sheets of three The acetaminocellulose film has a structure in which it is sandwiched, and an acrylic pressure-sensitive adhesive layer is provided on one surface thereof. On the other hand, the 1/4 wavelength plate produced in the above (a) is moved away from the retardation axis 45. The direction is cut. The corona discharge treatment is performed on the condition that the single side is accumulating 29 320734 200928521 and the irradiation amount is 1680 J. The corona discharge treatment surface is attached to the linear polarized light within 30 seconds after the corona discharge treatment. The acrylic pressure-sensitive adhesive layer side of the plate is placed such that the absorption axis of the linear polarizing plate and the slow axis of the quarter-wave plate intersect at an angle of 45 degrees. An elliptically polarizing plate in which a quarter-wave plate made of acrylic resin is laminated on a linear polarizing plate. (c) Ellipticity measurement of an elliptically polarizing plate, and a phase difference measuring device "k〇" manufactured by Oji Scientific Instruments Co., Ltd. Bra_ 21ADH" was measured in the above-mentioned ellipse Ellipticity of the light plate. The ellipticity of the elliptically polarizing plate obtained in this example is 925 925. [Example 5] The same polypropylene film as the user of Example 4 was formed to have a thickness of 40# m. The raw material film was stretched toward the horizontal uniaxial axis in the same manner as in the case of (a) of Example 4, but the linear velocity was changed to 5 ^ / . The knives and the preheating temperature were changed to 1702⁄4. The elongation temperature is changed to 15 °C and the heat setting temperature is changed to 12 〇. (: The final stretching ratio is changed to 3'. The in-plane phase difference and thickness of the stretched film (retardation film) obtained are changed. The directional phase difference values Rth, Nz coefficients, and thicknesses were measured in the same manner as in the first embodiment (a), and the results are shown in Table i. The phase difference in-plane phase difference R 〇 was 97 nm. Working as a quarter-wave plate [Example 6] A polypropylene resin film similar to that of the user of Example 4 was produced to obtain a raw material film having a thickness of 40/zm. The raw material film was stretched. Extender 320734 30 200928521, the extension machine extends to the horizontal single axis. The line speed is 5m/min, preheating, degree N〇°c, extension temperature system 160. 〇, heat-fixing temperature system 12 (rc, final stretching ratio is 4 times. Surface/internal phase difference R〇, thickness direction of the obtained stretched film (retardation film) The phase difference values Rth, Nz coefficients, and thicknesses were measured in the same manner as in (4) of the first embodiment, and the results are shown in Table 1. The in-plane retardation value R 此 of the retardation film was 273 nm. The 1/2 wavelength plate functions as a function. [Example 7] 〇 A film of a propylene monofilament having a melt flow rate of 8 g/10 min and having stereoregularity in the same row was obtained, and the original was obtained. In the same manner as (4) of the fourth embodiment, the film was stretched toward the horizontal uniaxial axis by a stretcher transverse stretcher. However, the line speed was changed to 5 m/min, and the preheating temperature was changed to (10). c, the extension temperature is changed to 14 〇t, and the heat setting temperature is changed to 120. (: 'The final stretching ratio is changed to 4 times. The surface-difference value Rq of the obtained stretched film (retardation film), the thickness direction phase difference ❹Rth Nz coefficient, the wavelength dispersion of the phase difference, and the thickness are The measurement was carried out in the same manner as in the green of the first embodiment (4). The result is shown in the table towel. The phase in-phase phase R is U7 nm, and it is used as a quarter-wave plate to perform the power month & [Embodiment 8] π The film thickness of the film of the polypropylene film which is the same as that of the user of Example 7 was 40, and the film of the original material was stretched by a single axis in the same manner as (4) of Example 4, but the material (4) was changed. In the W-knife clock, the preheating temperature is changed to 17〇〇c, the extension temperature is changed to 320734 31 200928521 C, the thermosetting temperature is changed to 120 C, and the final stretching ratio is changed to 3 times. The obtained stretching film ( The in-plane retardation value R〇, the thickness direction retardation value Rth, the Nz coefficient, and the thickness of the retardation film were measured in the same manner as in the first example (day), and the results are shown in the table. The in-plane phase difference Ro of the retardation film is 91 nm' to function as a quarter-wave plate [Example 9] A raw material film having a thickness of 40/m which was obtained by forming a film of the same polypropylene resin as that of the user of Example 7 was used in the same manner as in Example 4). The tensioner transverse stretcher extends toward the horizontal single axis. However, the line speed was changed to 5 m / min. The preheating temperature was changed to 17 〇. (: The elongation temperature is changed to ι6 〇 C, and the heat setting temperature is changed to 12 (TC, and the final stretching ratio is changed to 4 times. The in-plane phase difference value of the obtained stretched film (retardation film) is this. The directional phase difference values Rth, Nz coefficients, and thicknesses were measured in the same manner as in the example i (a), and the results are shown in Table i. The in-plane phase difference Ro of the phase difference ❹ film was 277 nm. [Comparative Example 1] A retardation film for a quarter-wave plate in which a norbornene resin film is longitudinally uniaxially stretched [sold by Sumitomo Chemical Co., Ltd.) "SES440140Z"], the wavelength dispersion and thickness of the in-plane phase difference Ro, the thickness direction phase difference Rth, the Nz coefficient, and the phase difference are measured in the same manner as in the embodiment, and the results are shown in the table. In addition to the use of the retardation film, an ellipse bias 320734 32 200928521 was produced in the same manner as in the first embodiment (b), and the elliptically polarizing plate was applied to the elliptically polarizing plate in the same manner as in the first embodiment. The rounding rate of the groove. The rounding ratio of the elliptically polarizing plate is 〇925. Example 2] • A retardation film [SES360140Y] sold by Sumitomo Chemical Co., Ltd. The in-plane phase difference value Ro, the thickness direction phase difference value, the Μ coefficient, and the thickness were measured in the same manner as in the first embodiment (a), and the results are shown in Table 1. ❹ [Comparative Example 3] The retardation film of the 1/2 wavelength plate in which the W _ resin film is vertically uniaxially stretched [ZM_3〇〇 sold by 〇pts, and is the same as the method of (a) of the example 1) The in-plane phase difference R, the thickness direction phase difference Rth, the Nz slit, and the thickness are shown in Table 1. [Comparative Example 4] The same propylene/eththene as the user of Example 1. The random copolymer 〇 ["Sumitomo Noblen Wl51"] was formed into a film, and a raw film of 5 〇 〇 owed was obtained to extend the raw material film toward the longitudinal uniaxial axis. The extension was adjusted to the linear velocity minute, first by the temperature to The preheating zone of n5〇c, the extension zone where the rain is adjusted to Bp to 118 °C, the final extension ratio is 1.37 times. The in-plane phase difference value Ro of the obtained stretched film (retardation film), the thickness direction retardation value Rth, the Nz coefficient, the wavelength dispersion of the phase difference, and the thickness ' are the same as those of the first embodiment (a) The results are shown in Table 1. The retardation film in-plane phase difference Ro is 275 nm, and functions as a 1/2 wavelength plate. 33 320734 200928521 _ [Table 1] Material of retardation film * Physical properties of extended phase retardation film ~~~ ^ Ro (nm) Rth (nm) Nz Wavelength dispersion thick ί'' (nm) Example 1 PP Cross 140 77 1.0 1.00 8.0 Example 2 PP 90 90 1.0 1.00 9.0 Example 3 PP Transverse 280 153 1. 0 - 12.7 Example 4 PP+ nucleating agent Transverse 150 J 79 1.0 1.00 --- 9.7 Example 5 PP+ nucleating agent Transverse 97 49 1.0 — 8.0 Example 6 PP+ nucleating agent 273 140 1.0 - 8.5 Example 7 PP Transverse 147 75 1.0 1.00 9.3 Example 8 PP Transverse 91 46 1.0 — 1 ---- 8.1 Example 9 PP Transverse 277 145 1.0 8.2~~~ Comparative Example 1 NOR Vertical 140 67 1.0 1.01 45.5 Comparative Example 2 NOR Cross 139 149 1.6 A 62.0 Comparative Example 3 NOR Longitudinal 298 150 1.0 — 116 Comparative Example 4 PP Vertical 275 138 1.0 1.00 44. Material of eucalyptus retardation film PP: Polypropylene pp+ nucleating agent: polypropylene + nucleating agent N0R : norbornene 〇 in the case of norbornene thin resin' as in Comparative Example 1 and As shown in Fig. 3, a 1/4 wavelength plate and a 1/2 wavelength plate having an Nz coefficient of about 1 by a longitudinal uniaxial extension have been provided on the market. However, the thickness thereof was 45. 5 / z m in the 1/4 wavelength plate (Comparative Example 1) and 116 / / m in the 1/2 wavelength plate (Comparative Example 3). On the other hand, as shown in the comparative example 2, the transverse uniaxial extension of the norbornene resin is also provided in the market, but its & coefficient is 1.6. 'The thickness also becomes 62#m. 320734 34 200928521 However, as shown in Examples 1 to 9, by making the poly-mother tree moon film stretch uniaxially at a high magnification, it is possible to manufacture a y/4 wavelength plate having a core coefficient of about i or 1/2. The wavelength plate has a thickness of 25/m or less and can be formed extremely thin. On the other hand, as shown in Comparative Example 4, when the polypropylene resin film was longitudinally uniaxially stretched, a 1/2 wavelength plate was obtained, but the thickness was not reduced by shrinkage, and it was difficult to achieve the present invention. The so-called extremely thin type below 25ym. The 1/4 wavelength plate fabricated in (a) of Example j or (a) of Example 4, and the Example or Example 6 are laminated at the axial angle described above with reference to FIG. On the 1/2 wavelength plate, a 1/4 wavelength plate in the wide band is available. Further, on the 丨/2 wavelength plate side, the linear polarizing plate shown in (b) of Example 1 or (a) of Example 4 is laminated at the axial angle previously described with reference to Fig. 2 In the present invention, the stretched film of the polypropylene resin is applied to the retardation film, and the thickness of the ellipsoidal film is 25 Å or less. The extremely thin film exhibits the effect of the desired retardation value. Further, by using the polypropylene resin film, even if the lateral extension ' ^ can be extended at a high magnification, it is possible to make a substantially complete round. Advantages. Furthermore, the phase difference of the present invention can be manufactured by lateral extension, so that it has the advantage of widening the effective width while thinning the film thickness. The present invention also contributes to laminating the retardation film. Liquid crystal display device

通荆/k。 J ,% ♦ KV , W”丨傅战之相位差膜具: 的臈庳,同時並可顯覌充分的相位差特性。因此, 320734 35 200928521 差膜係可用來作為丨/4波長板或1/2波長板,而使該1/4 波長板層合於直線偏光板之橢圓偏光板、或組合1/4波長 板與1/2波長板而使其層合於直線偏光板之橢圓偏光板係 顯不良好的反射防止特性,同時並有助於液晶顯示裝置之 更薄型化。 【圖式簡單說明】 第1圖係有關本發-明之橢圓偏光板的一形態,為顯示 〇層構成之截面示意圖(A)及用以說明軸角度的關係之圖 (B) 〇 _第2圖係有關本發明之橢圓偏光板的另一形態,為顯 不層構成之截面示意圖(A)及用以說明轴角度的關係之圖 (B) 〇 第3圖係表示將本發明之橢圓偏光板適用於液晶顯元 袭置之例的截面示意圖。 、 【主要元件符號說明 第4圖係表示將本發明之橢圓偏光板適用於液晶顯开 裝置之另一例的截面示意圖。 ^ 】 10 15 20 30 50 Θ 1/4波長板 1 / 2波長板 直線偏光板 35橢圓偏光板 液晶單元 12 17 22 40 60 1/4波長板之遲相軸 1/2波長板之遲相輪 直線偏光板之吸故輕 感壓接著劑層 背光 從直線偏光板之吸收轴至1/4波長板之遲相轴 角度 320734 36 200928521 Φ 從直線偏光板之吸收軸至1/2波長板之遲相軸的 角度 Ψ 從直線偏光板之吸收軸至1/4波長板之遲相軸的 角度 ❹ 37 320734Tong Jing / k. J,% ♦ KV, W” 丨 战 之 之 相位 : : : : : : : : : 臈庳 臈庳 臈庳 臈庳 臈庳 臈庳 臈庳 臈庳 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 320 a wavy plate in which a 1/4 wavelength plate is laminated to a linear polarizing plate, or an elliptically polarizing plate in which a 1/4 wavelength plate and a 1/2 wavelength plate are combined to be laminated on a linear polarizing plate It does not have good reflection prevention characteristics, and contributes to thinner thickness of the liquid crystal display device. [Simple description of the drawing] Fig. 1 is a cross-sectional view showing the structure of the enamel layer according to the present invention. (A) and a diagram for explaining the relationship of the shaft angle (B) 〇 _ 2 is another embodiment of the elliptically polarizing plate of the present invention, which is a schematic cross-sectional view (A) of the display layer and a shaft for explaining the axis Fig. 3 is a cross-sectional view showing an example in which the elliptically polarizing plate of the present invention is applied to a liquid crystal display. Fig. 4 is a diagram showing the ellipse of the present invention. The polarizing plate is suitable for the interception of another example of the liquid crystal display device Fig. ^ 】 10 15 20 30 50 1/4 1⁄4 wavelength plate 1 / 2 wave plate linear polarizer 35 ellipsoidal liquid crystal cell 12 17 22 40 60 1⁄4 wavelength plate slow phase axis 1/2 wavelength plate The retardation of the linear polarizer of the retardation wheel is light-sensitive. The back layer of the backlight is from the absorption axis of the linear polarizer to the retardation angle of the quarter-wave plate. 320734 36 200928521 Φ From the absorption axis of the linear polarizer to the 1/2 wavelength plate Angle of the slow phase axis Ψ Angle from the absorption axis of the linear polarizer to the slow axis of the 1/4 wavelength plate ❹ 37 320734

Claims (1)

200928521 七、申請專利範圍: 1. 一種相位差膜,其係由聚丙婦樹脂之橫延伸膜所構成, 且厚度為25#m以下,面内之相位差值(Ro)在70至 400nm的範圍,而且,當使膜之面内遲相軸方向的折射 率為nx、面内進相軸方向之折射率為ny、厚度方向之 折射率為nz時,以式:Nz=(nx-nz)/(nx-ny)所定義之 Nz係數在0. 9至1. 1的範圍。 2. 如申請專利範第1項之相位差膜,其中,聚丙烯樹脂係 由含有10重量%以下之乙烯基單元的丙烯與乙烯的共 聚物所構成。 3. 如申請專利範第1項之相位差膜,其中,前述聚丙烯樹 脂係實質上由丙烯單獨聚合物所構成。 4. 如申請專利範第1至3項中任一項之相位差膜,其中, 前述聚丙烯樹脂係含有造核劑。 5. 如申請專利範第1或2項之相位差膜,其係發揮1/4 波長板之功能。 6. 如申請專利範第1或2項之相位差膜,其係發揮1/2 波長板之功能。 7. —種橢圓偏光板,係將申請專利範第1或2項之相位差 膜層合於直線偏光板上而構成者。 8. —種橢圓偏光板,係將申請專利範第3項之發揮1/4 波長板之功能的相位差膜層合於直線偏光板而構成者。 9. 一種橢圓偏光板,係使申請專利範第5項之發揮1/4 波長板之功能的相位差膜、與申請專利範第6項之發揮 38 320734 200928521 ' 1/2波長板之功能的相位差膜層合,並於其1/2波長板 ’ 側層合直線偏光板而構成者。 10. —種液晶顯示裝置,其特徵在於··將申請專利範第7 項之橢圓偏光板層合於液晶單元之至少一側而成。 ' 11. 一種液晶顯示裝置,其特徵在於:將申請專利範第8 — 或9項之橢圓偏光板層合於液晶單元之至少一侧而成。 ❹ ❹ 39 320734200928521 VII. Patent application scope: 1. A retardation film consisting of a transversely stretched film of polypropylene resin with a thickness of 25#m or less and a phase difference (Ro) in the range of 70 to 400 nm. Further, when the refractive index in the retardation axis direction of the film is nx, the refractive index in the in-plane axis direction is ny, and the refractive index in the thickness direction is nz, the formula: Nz = (nx - nz) The range of the range of 0.9 to 1.1 is defined by the value of the Nz coefficient defined by /(nx-ny). 2. The retardation film of claim 1, wherein the polypropylene resin is composed of a copolymer of propylene and ethylene containing 10% by weight or less of a vinyl unit. 3. The retardation film of claim 1, wherein the polypropylene resin is substantially composed of a propylene individual polymer. 4. The retardation film according to any one of claims 1 to 3, wherein the polypropylene resin contains a nucleating agent. 5. For the phase difference film of Patent No. 1 or 2, it functions as a quarter-wave plate. 6. For the phase difference film of Patent No. 1 or 2, it functions as a 1/2 wavelength plate. 7. An elliptically polarizing plate comprising a phase difference film of claim 1 or 2 laminated on a linear polarizing plate. 8. An elliptically polarizing plate which is formed by laminating a retardation film which functions as a 1/4 wavelength plate of the third aspect of the patent application to a linear polarizing plate. 9. An elliptically polarizing plate which is a retardation film which functions as a 1/4 wavelength plate in the fifth application of the patent application, and a function of 38 320734 200928521 '1/2 wavelength plate of the patent application model 6 The retardation film is laminated, and a linear polarizing plate is laminated on the side of the 1/2 wavelength plate. A liquid crystal display device characterized in that the elliptically polarizing plate of claim 7 is laminated on at least one side of the liquid crystal cell. 11. A liquid crystal display device characterized in that an elliptical polarizing plate of claim 8 or 9 is laminated on at least one side of a liquid crystal cell. ❹ ❹ 39 320734
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