TW201137409A - Antiglare film and antiglare polarizing sheet - Google Patents

Antiglare film and antiglare polarizing sheet Download PDF

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Publication number
TW201137409A
TW201137409A TW100107512A TW100107512A TW201137409A TW 201137409 A TW201137409 A TW 201137409A TW 100107512 A TW100107512 A TW 100107512A TW 100107512 A TW100107512 A TW 100107512A TW 201137409 A TW201137409 A TW 201137409A
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Taiwan
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film
glare
energy spectrum
mold
spatial frequency
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TW100107512A
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Chinese (zh)
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TWI498603B (en
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Tsutomu Furuya
Takashi Fujii
Sho Kanzaki
Toru Jinno
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Sumitomo Chemical Co
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/30Polarising elements
    • G02B5/3025Polarisers, i.e. arrangements capable of producing a definite output polarisation state from an unpolarised input state
    • G02B5/3033Polarisers, i.e. arrangements capable of producing a definite output polarisation state from an unpolarised input state in the form of a thin sheet or foil, e.g. Polaroid
    • G02B5/3041Polarisers, i.e. arrangements capable of producing a definite output polarisation state from an unpolarised input state in the form of a thin sheet or foil, e.g. Polaroid comprising multiple thin layers, e.g. multilayer stacks
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/0001Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings specially adapted for lighting devices or systems
    • G02B6/0011Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings specially adapted for lighting devices or systems the light guides being planar or of plate-like form
    • G02B6/0065Manufacturing aspects; Material aspects
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1335Structural association of cells with optical devices, e.g. polarisers or reflectors
    • G02F1/133502Antiglare, refractive index matching layers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/30Accessories, mechanical or electrical features
    • G01N2223/345Accessories, mechanical or electrical features mathematical transformations on beams or signals, e.g. Fourier
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B2006/12035Materials
    • G02B2006/12069Organic material
    • G02B2006/12071PMMA

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  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • General Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Mathematical Physics (AREA)
  • Engineering & Computer Science (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Manufacturing & Machinery (AREA)
  • Optical Elements Other Than Lenses (AREA)
  • Laminated Bodies (AREA)
  • Polarising Elements (AREA)
  • Liquid Crystal (AREA)

Abstract

The present invention provides an antiglare film and an antiglare polarizing sheet using the same, the antiglare film having a base film and an antiglare layer laminated on the base film and having a concave-convex surface, the base film containing an acrylic resin, the ratio H12/H22 of the energy spectrum H12 of altitude of the concave-convex surface at the space frequency of 0.01 μ m<SP>-1</SP> to the energy spectrum H22 at the space frequency of 0.04 μ m<SP>-1</SP> being within the range of 3 to 20, the ratio H32/H22 of the energy spectrum H32 at the space frequency of 0.1 μ m<SP>-1</SP> to the energy spectrum H22 being 0.1 or less, and the concave-convex surface containing 95% or more of planes having a tilting angle equal to or lower than 5 DEG.

Description

201137409 六、發明說明: 【發明所屬之技術領域】 本發明係關於防眩(防眩光;antiglare)膜及使用該防 眩膜之防眩性偏光板。 【先前技術】BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an anti-glare (antiglare) film and an anti-glare polarizing plate using the anti-glare film. [Prior Art]

液晶顯示器、電漿顯示面板、映像管(陰極射線管:CRT (Cathode Ray Tube))顯示器、有機電致發光(EL: Electroluminescence)顯示器等圖像顯示裝置,當外光映 射至該顯示面時’會顯著地損及觀看性。為了防止此般外 光的映射’在重視畫質之電視和個人電腦、於外光較強的 室外所用之攝影機及數位照相機、以及利用反射光來進行 顯示之行動電話等中’以往即已在圖像顯示裝置的表面設 置有用以防止外光的映射之防眩膜。 例如’在日本特開2006-053371號公報中,係記載有 對於經研磨的模具基材施以喷砂加工後,施以無電解鍍 鎳,藉此製造出表面具有細微凹凸之模具,然後一邊將形 成於二乙S义纖維素(Tac : Triacetyl Cellulose)上之光硬 化性樹脂層按壓於該模具的凹凸面一邊進行硬化,藉此得 到於光硬化性樹脂層的表面轉印有該模具的凹凸面之防眩 膜。 【發明内容】 對於防眩膜’除了要求防眩性外,亦期望當配置在圖 像顯不裝置的表面時可顯現高對比,當配置在圖像顯示裝 置的表面時’可抑制因散射光使顯示面全體變白而產生顯 4 322870 201137409 示濁化之所謂「泛白」的產生,以及當配置在圖像顯示裝 置的表面時,可抑制因圖像顯示裝置的像素與防眩膜的表 面凹凸形狀產生干涉導致亮度分布的產生而難以觀看之所 謂「閃斑」的產生。然而,上述日本特開2006-053371號 公報所記載之防眩膜,由於使用以喷砂加工來形成凹凸形 狀之模具來進行製作者,故形成於防眩膜之凹凸形狀的精 度不足,尤其可能會製作出具有50//m以上的周期之相對 較大的凹凸形狀,故存在有容易產生「閃斑」的問題。 此外,同一文獻所記載之防眩膜,容易產生損傷,就 機械強度之觀點來看並不必然充分。再者,同一文獻所記 載之防眩膜,耐濕性不足,當將該防眩膜貼合於偏光膜來 使用時,可能使該偏光膜因吸濕而劣化。 因此,本發明之目的係以提供一種防眩膜,能夠顯示 較佳的防眩性並顯現良好的對比,並且可防止因「泛白」 及「閃斑」的產生所導致之觀看性的降低,並且機械強度 及耐濕性佳,以及一種防眩性偏光板,其為由該防眩膜與 偏光膜之積層體所構成之防眩性偏光板,可有效地抑制該 偏光膜的劣化之。 本發明係提供一種防眩膜,具備:基材膜、以及積層 於該基材膜上並具有凹凸表面之防眩層,其中,該基材膜 係含有丙烯酸系樹脂;空間頻率0.01# πΓ1中之該凹凸表面 之標高的能譜Hi2與空間頻率0.04# πΓ1中之該凹凸表面之 標高的能譜Η22之比Η!2/^2,係位於3至20的範圍内;空 間頻率0. 1从πΓ1中之該凹凸表面之標高的能譜Η32與空間頻 5 322870 201137409 率2 〇.04/zm中之該凹凸表面之標高的能譜Η,之比η&quot; 仏2 ’為o.i以下;並且該凹凸表面含有95%以上之傾斜角 度為5°以下的面。基材膜的厚度較佳為2〇ym以上l〇〇&quot;m 以下。 此外,本發明係提供一種防眩性偏光板,係具備有: 上述防眩膜、以及積層於基材膜之與防眩層為相反側的面 之偏光膜。 本發明之防眩膜,能夠顯示較佳的防眩性並顯現良好 的對比,可有效地防止因「泛白」及「閃斑」的產生所導 致之觀看性的降低。此外,本發明之防眩膜,該機械強度 及耐濕性佳。使用該防眩膜之本發明之防眩性偏光板中, 可有效地抑制因吸濕所導致之偏光膜的劣化。 【實施方式】 &lt;防眩膜&gt; 第1圖係示意性顯示本發明之防眩膜的一例之剖面 圖。本發明之防眩膜,如第丨圖所示之例子,係具備:含 有丙烯酸系樹脂之基材膜1〇1、以及積層於基材膜1〇1上 之防眩層102。防眩層1〇2之與基材膜1〇1為相反側的表 面,係由細微的凹凸表面(細微凹凸表面1〇3)所構成。以 下更詳細的說明本發明之防眩膜。 (防眩層) 本發明之防眩膜所具備的防眩層102中,空間頻率 0. 01 1中之細微凹凸表面1〇3之標高的能譜Ηι2與空間頻 率〇. (Μβπτ1中之細微凹凸表面1〇3之標高的能譜出2之比 322870 6 201137409An image display device such as a liquid crystal display, a plasma display panel, a cathode ray tube (CRT (Cathode Ray Tube)) display, or an organic electroluminescence (EL) display, when external light is mapped to the display surface Will significantly damage the viewing. In order to prevent such mapping of external light, in the case of TVs and personal computers that emphasize image quality, cameras and digital cameras that are used outdoors, and mobile phones that use reflected light for display, The surface of the image display device is provided with an anti-glare film for preventing the mapping of external light. For example, JP-A-2006-053371 discloses that a mold for a polished mold base is subjected to sandblasting, and then electroless nickel plating is applied to produce a mold having fine irregularities on the surface, and then a side is produced. The photocurable resin layer formed on the polyethylene terephthalate (Tac : Triacetyl Cellulose) is pressed against the uneven surface of the mold to be cured, whereby the mold is transferred onto the surface of the photocurable resin layer. Anti-glare film for uneven surface. SUMMARY OF THE INVENTION In addition to anti-glare properties, it is desirable for the anti-glare film to exhibit high contrast when disposed on the surface of the image display device, and to suppress scattered light when disposed on the surface of the image display device. Whitening the entire display surface to produce the so-called "whitening" of the liquid crystal display, and when it is disposed on the surface of the image display device, the pixel and the anti-glare film of the image display device can be suppressed. The surface uneven shape produces a so-called "flash spot" which interferes with the generation of a luminance distribution and is difficult to see. However, the anti-glare film described in the above-mentioned Japanese Patent Publication No. 2006-053371 is produced by using a mold which is formed into a concave-convex shape by sandblasting, so that the accuracy of the uneven shape formed on the anti-glare film is insufficient, and it is particularly possible. Since a relatively large uneven shape having a period of 50/m or more is produced, there is a problem that "flash spots" are likely to occur. Further, the antiglare film described in the same document is liable to cause damage, and is not necessarily sufficient from the viewpoint of mechanical strength. Further, the antiglare film described in the same document has insufficient moisture resistance, and when the antiglare film is bonded to a polarizing film, the polarizing film may be deteriorated by moisture absorption. Accordingly, it is an object of the present invention to provide an anti-glare film which can exhibit better anti-glare properties and exhibit good contrast, and can prevent deterioration of visibility due to "whitening" and "flash spots". And an anti-glare polarizing plate which is an anti-glare polarizing plate which is composed of a laminate of the anti-glare film and the polarizing film, and can effectively suppress deterioration of the polarizing film. . The present invention provides an anti-glare film comprising: a base film; and an anti-glare layer laminated on the base film and having an uneven surface, wherein the base film contains an acrylic resin; and the spatial frequency is 0.01# πΓ1 The ratio of the energy spectrum Hi2 of the elevation of the concave-convex surface to the energy spectrum Η22 of the elevation of the concave-convex surface in the spatial frequency 0.04# πΓ1 is in the range of 3 to 20; the spatial frequency is 0.1. From the energy spectrum Η32 of the elevation of the concave-convex surface in πΓ1 and the energy spectrum 标 of the elevation of the concave-convex surface in the spatial frequency 5 322870 201137409 rate 2 〇.04/zm, the ratio η&quot; 仏2 ' is oi or less; The uneven surface contains 95% or more of a surface having an inclination angle of 5 or less. The thickness of the base film is preferably 2 〇 ym or more and 1 〇〇 or less. Furthermore, the present invention provides an anti-glare polarizing plate comprising: the anti-glare film; and a polarizing film laminated on a surface of the base film opposite to the anti-glare layer. The anti-glare film of the present invention can exhibit better anti-glare properties and exhibit good contrast, and can effectively prevent deterioration of visibility due to the occurrence of "whitening" and "flash spots". Further, the antiglare film of the present invention is excellent in mechanical strength and moisture resistance. In the anti-glare polarizing plate of the present invention using the anti-glare film, deterioration of the polarizing film due to moisture absorption can be effectively suppressed. [Embodiment] &lt;Anti-glare film&gt; Fig. 1 is a cross-sectional view schematically showing an example of an anti-glare film of the present invention. The antiglare film of the present invention has a base film 1〇1 containing an acrylic resin and an antiglare layer 102 laminated on the base film 1〇1 as shown in the figure. The surface of the antiglare layer 1 to 2 opposite to the base film 1〇1 is composed of a fine uneven surface (fine uneven surface 1〇3). The antiglare film of the present invention will be described in more detail below. (Anti-glare layer) In the anti-glare layer 102 of the anti-glare film of the present invention, the energy spectrum Ηι2 and the spatial frequency of the elevation of the fine concave-convex surface 1〇3 in the spatial frequency of 0.011 are small (the fineness in Μβπτ1) The energy of the elevation of the bump surface 1〇3 is 2 ratio 322870 6 201137409

Hi2/H22 ’係位於3至20的範圍内,空間頻率〇. 1从m_1中之 細微凹凸表面103之標高的能譜Ha2與空間頻率0.04//^ 中之細微凹凸表面103之標高的能譜HJ之比H32/H22,為0. 1 以下。 以往’對於防眩膜之細微凹凸表面的週期,係以jISB 0601所§己載之粗糖度曲線要素的平均長度RSm、剖面曲線 要素的平均長度PSm、以及彎曲曲線要素的平均長度wSm 等來進行評估。然而,在此般以往的評估方法中,無法正 確地評估細微凹凸表面中所含之複數個週期。因此,對於 閃斑與細微凹凸表面之相關性以及防眩性與細微凹凸表面 之相關性’亦無法正確地評估,就以RSm、pSm、WSm等之 值的控制下,係難以製作出可兼具閃斑的抑制與充分的防 眩性能之防眩膜。 本發明者們係發現到,在將具有細微凹凸表面之防眩 ,積層於含有丙烯酸系樹脂之基材膜上之防眩膜中,該細 微I凸表面顯示出使用「細微凹凸表面之標高的能譜」所 規疋之特㈣空間頻率分布,亦即標高的能譜比仏2/仏2位 於3至20的範圍内’且&quot;愚2為〇1以下之防眩膜,可顯 現出較佳的防眩性能並防止因泛㈣產生所造成之觀看性 的降低’即使當運时高精細賴像顯示裝置時,亦不會 產生閃斑而能夠顯現高對比。 日 域。:t說明防眩膜所具有之細微凹凸表面之標高的能 圓曰二2圖係示意性顯示本發明之防眩膜的表面之透視 第2圖所示,本發明之防_丨係具備具有由細微 322870 7 201137409 凹凸2所構成之細微凹凸表面的防眩層。在此,本發明中 所明細微凹凸表面的標高」,係意味著在防眩膜1表面的 任意點Ρ中之細微凹凸表面的最低點的高度中,從具有該 高度之虛擬平面(標高係 以0//Π1為基準)之防眩膜的主法 線方向5(上述虛擬平面之法線方向)之直線距離。如第2 圖所不’當以(x,y)來表示防眩膜面内的正交座標時,細微 凹凸表面的標高可由座標(X,y)的二維函數h(x,y)來表 不。第2圖中’係以投影面3來表示防眩膜全體的面。 細微凹凸表面的標高,可從藉由共焦顯微鏡、干涉顯 微鏡原子力顯微鏡(AFM : Atomic Force Microscope)等 裝置所測定之表面形狀的三維資訊中求取。測定機所要求 的水平分解能’至少為5以111以下,較佳為2//m以下,此 外’垂直分解能至少為〇. lym以下,較佳為0. 01/zm以下。 適合於此測定之非接觸式三維表面形狀·粗糙度測定機, 可列舉出 New View 5000 系列(Zygo Corporation 公司製、 在日本可從Zygo有限公司來取得)、三維顯微鏡PL# 2300 (Sensofar公司製)等。關於測定面積,由於標高之能譜的 分解能必須為0. Ol/ζπΓ1以下,所以較佳至少為20〇emx200 // m以上,尤佳為500/z mx500 // m以上。 接著說明從二維函數h(x,y)來求取標高的能譜之方 法。首先,係從二維函數h(x,y)中,藉由下列式(1)所定 義之二維傅利葉轉換來求取二維函數H(fx,fy)。 Λ) ^ J fKx,y)^p[- +fyy)]^fy 式⑴ 8 322870 201137409 :此’匕及fy分別為x方向及y方向的空間頻係 之倒數的維度。此外,式⑴中的率 f虛數早位。藉由將所得之二維函數H(fx,fy)進行平方運 舁,可求取f票高的能譜竹fx,fy)。此能譜H2(fx,w係表示 防眩膜之細微凹凸表面的空間頻率分布。 以下更具體地說明求取防眩膜所具有之細微凹凸表面 之標高的能譜之方法。藉由上述共焦顯微鏡、干涉顯微鏡、 原子力顯微鏡等所實際敎之表面形狀的三維資訊,一般 可作為離散值、亦即對應於多數個測定點之標高而獲得。 第3圖係顯示離散地獲得表示標高之函數h 模式圖:如第3圖㈣,㈣(x,y)表示賊_内的:交 座標,並以虛線來表示防眩膜的投影面3上之χ軸方向上 以每Δχ所分割的線以及y軸方向上以每Ay所分割的線 時’在實際的測定中,細微凹凸表面的標高,可作為防眩 膜的杈衫面3上之各虛線的每個交又點之離散的標高值而 獲得。 所得之標高值的數目,是由測定範圍與所決 定,如第3圖所示,當以x軸方向的測定範圍為χ=ΜΔχ, 以y軸方向的測定範圍為Y=NAy時,所得之標高值的數目 為(Μ+1)χ(Ν+1)個。 如第3圖所示,當將防眩膜的投影面3上之著眼點A 的座4示没為(j^X,k^y)(在此,j為〇以上μ以下,k為〇 以上N以下)時,對應於著眼點A之防眩膜表面上之點p的 標高可表示為h(j Ax, kAy)。 9 322870 201137409 在此,測定間隔Δχ及Ay係與測定機器的水平分解能 相依,為了精度佳地評估細微凹凸表面,如上述般,Δχ 及Δγ較佳均為5/zm以下,尤佳均為2em以下。此外, 測疋範圍X及γ如上述般,較佳均為以上,尤佳均 為500 # m以上。 如此,在實際的測定中,表示細微凹凸表面的標高之 函數,可作為具有(M+l)x(N+l)個值之離散函數h(x,y)而 獲得。因此,係藉由以測定所獲得之離散函數h(x,y)與下 列式(2)所定義之離散傅利葉轉換,來求取離散函數 H(fx, fy),並藉由將離散函數fj(fx,fy)進行平方運算,可求 取能譜的離散函數H2(fx,fy^式(2)中的}為—⑶+丨)“以 上(MH)/2以下之整數’m為_(n+i)/2以上(許1)/2以下之 整數。此外,△乜及^匕分別為χ方向及y方向的空間頻 率間隔,並由式(3)及式(4)所分別定義。相當 於標高之能譜的水平分解能。 &quot;(Ky )s + 】)(#+】)石 |^(/Δχ,Μ;/)βχρ[- 2m\jUsxisfx +km6ybfy\ 式(2)The Hi2/H22 ' is located in the range of 3 to 20, and the spatial frequency 〇. 1 is the energy spectrum of the energy spectrum Ha2 of the level of the fine uneven surface 103 in m_1 and the level of the fine uneven surface 103 of the spatial frequency of 0.04//^. The ratio of HJ is H32/H22, which is 0.1 or less. In the past, the period of the fine uneven surface of the anti-glare film is based on the average length RSm of the coarse sugar curve elements contained in jISB 0601, the average length PSm of the profile curve elements, and the average length wSm of the curved curve elements. Evaluation. However, in such conventional evaluation methods, it is not possible to correctly evaluate the plurality of periods included in the surface of the fine uneven surface. Therefore, the correlation between the speckle and the fine uneven surface and the correlation between the anti-glare property and the fine uneven surface cannot be correctly evaluated. Under the control of the values of RSm, pSm, WSm, etc., it is difficult to produce An anti-glare film with suppression of flash spots and sufficient anti-glare properties. The present inventors have found that in an anti-glare film having an anti-glare layer having a fine uneven surface and laminated on a base film containing an acrylic resin, the fine I convex surface exhibits the use of "the level of the fine uneven surface. The special (4) spatial frequency distribution of the energy spectrum, that is, the energy spectrum of the elevation is in the range of 3 to 20 in the range of 至2/仏2, and the anti-glare film of "2" is less than 1 and can be revealed. It has better anti-glare properties and prevents a decrease in visibility due to the generation of ubi-(4). Even when the high-definition image display device is in operation, no speckle is generated and high contrast can be exhibited. Day domain. :t illustrates the energy level of the fine uneven surface of the anti-glare film. The schematic diagram shows the surface of the anti-glare film of the present invention. FIG. 2 is a perspective view of the anti-glare system of the present invention. The anti-glare layer of the fine uneven surface composed of the fine 322870 7 201137409 unevenness 2. Here, the elevation of the surface of the fine uneven surface in the present invention means a virtual plane having the height at the lowest point of the fine uneven surface in any point on the surface of the anti-glare film 1 (the elevation plane) The linear distance of the main normal direction 5 (the normal direction of the imaginary plane) of the anti-glare film based on 0//Π1. As shown in Fig. 2, when the orthogonal coordinates in the plane of the anti-glare film are expressed by (x, y), the elevation of the fine concave-convex surface can be represented by the two-dimensional function h(x, y) of the coordinates (X, y). No. In Fig. 2, the surface of the entire anti-glare film is indicated by the projection surface 3. The elevation of the fine uneven surface can be obtained from three-dimensional information of the surface shape measured by a device such as a confocal microscope or an AFM (Atomic Force Microscope). The lower resolution energy required for the measuring machine is at least 5 to be 111 or less, preferably 2/m or less, and the other 'vertical decomposition energy is at least 〇. lym or less, preferably 0. 01/zm or less. A non-contact three-dimensional surface shape and roughness measuring machine suitable for the measurement is a New View 5000 series (manufactured by Zygo Corporation, available from Zygo Co., Ltd. in Japan), and a three-dimensional microscope PL# 2300 (manufactured by Sensofar Co., Ltd.) )Wait. Regarding the measurement area, since the decomposition energy of the energy spectrum of the elevation must be 0. Ol/ζπΓ1 or less, it is preferably at least 20 〇emx200 // m or more, and more preferably 500/z mx500 // m or more. Next, a method of obtaining the energy spectrum of the elevation from the two-dimensional function h(x, y) will be described. First, the two-dimensional function H(fx, fy) is obtained from the two-dimensional function h(x, y) by the two-dimensional Fourier transform defined by the following equation (1). Λ) ^ J fKx, y)^p[- +fyy)]^fy Equation (1) 8 322870 201137409: This '匕 and fy are the dimensions of the reciprocal of the spatial frequency system in the x direction and the y direction, respectively. Further, the rate f imaginary in the equation (1) is early. By squaring the obtained two-dimensional function H(fx, fy), the energy spectrum bamboo fx, fy) of the f-score can be obtained. This energy spectrum H2 (fx, w represents the spatial frequency distribution of the fine uneven surface of the anti-glare film. Hereinafter, a method for obtaining the energy spectrum of the level of the fine uneven surface of the anti-glare film will be more specifically described. The three-dimensional information of the actual surface shape of a focal microscope, an interference microscope, an atomic force microscope, etc. can generally be obtained as a discrete value, that is, an elevation corresponding to a plurality of measurement points. Fig. 3 shows a function of discretely obtaining an elevation value. h mode diagram: as shown in Fig. 3 (4), (4) (x, y) represents the thief_inside: the intersection mark, and the dotted line indicates the line divided by Δχ in the direction of the yaw axis on the projection surface 3 of the anti-glare film. And the line divided by Ay in the y-axis direction. 'In the actual measurement, the elevation of the fine uneven surface can be used as the discrete elevation of each intersection of each dotted line on the shirt face 3 of the anti-glare film. The value of the obtained elevation value is determined by the measurement range and as shown in Fig. 3, when the measurement range in the x-axis direction is χ = Μ Δ χ, and the measurement range in the y-axis direction is Y = NAy When the number of elevation values obtained is Μ+1)χ(Ν+1). As shown in Fig. 3, when the projection 4 of the projection point 3 on the projection surface 3 of the anti-glare film is shown as (j^X, k^y) (in Therefore, when j is 〇 or more and μ or less, and k is 〇 or more and N or less, the elevation of the point p on the surface of the anti-glare film corresponding to the point of view A can be expressed as h(j Ax, kAy). 9 322870 201137409 The measurement interval Δχ and the Ay system are dependent on the horizontal decomposition energy of the measuring device, and the fine uneven surface is evaluated for accuracy. As described above, Δχ and Δγ are preferably 5/zm or less, and more preferably 2em or less. The 疋 range X and γ are preferably all of the above, and more preferably 500 # m or more. Thus, in actual measurement, a function indicating the elevation of the fine uneven surface can be obtained as (M+l)x. Obtained by a discrete function h(x, y) of (N + 1) values. Therefore, by the discrete function h(x, y) obtained by the measurement and the discrete Fourier transform defined by the following formula (2), To obtain the discrete function H(fx, fy), and by squaring the discrete function fj(fx,fy), we can obtain the discrete function H2 of the energy spectrum (fx, fy^ in the formula (2) is —(3)+丨) The integer 'm of the above (MH)/2 or less is an integer of _(n+i)/2 or more (1)/2 or less. Further, Δ乜 and 匕 are the spatial frequency intervals in the χ direction and the y direction, respectively. It is defined by equations (3) and (4) respectively. It is equivalent to the horizontal decomposition energy of the energy spectrum of the elevation. &quot;(Ky )s + 】)(#+))石|^(/Δχ,Μ;/) Χρ[- 2m\jUsxisfx +km6ybfy\ (2)

(Λ^ + 1)Δχ 式(3) ¥y = (N+l)Ay 式U) 第4圖係以二維離散函數h(x,y)來表示本發明之防眩 膜所具備之防眩層的細微凹凸表面的標高之圖的一例。第 4圖中,標高係以白與黑的階度來表示。第4圖所示之離 322870 10 201137409 散函數h(x, y)係具有512x512個值,水平分解能Δχ及Ay . 為 1. 66 y m。 % 此外,第5圖係以白與黑的階度來表示將第4圖所示 之二維函數h(x,y)進行離散傅利葉轉換所得之標高的能譜 H2(fx,fy)之圖。第5圖所示之標高的能譜H2(fx,fy)亦為具 有512x512個值之離散函數,標高之能譜的水平分解能△ 及△。為 0.0012VHT1。 如第4圖所示之例子般,由於本發明之防眩膜所具備 之防眩層的細微凹凸表面係由隨機地形成之凹凸所構成, 所以標南的能譜H2係如第5圖所示,以原點為中心呈對 稱。因此,可從通過屬於二維函數之能譜H2(fx,fy)的原點 之剖面,來求取空間頻率0.01 ynf1中之標高的能譜Η!2、 空間頻率0. 04μ m_1中之標高的能譜⑴2及空間頻率〇. 1 enf1 中之標高的能譜Η/。第6圖係顯示第5圖所示之能譜 H ( f X, f y )中的f χ= 〇時之剖面的圖。從第6圖中可得知,空 間頻率0.01/zm-1中之標高的能譜⑴2為4. 4,空間頻率〇 〇4 以πΓ1中之標高的能譜仏2為0.35,空間頻率〇. 1 enf1中之 標高的能譜H32為〇· 00076,比Η,2/%2為14,比H32/H22為 0.0022。 如上述般,本發明之防眩膜中,空間頻率O.Wyf 中之細微凹凸表面的標高的能譜Hl2與空間頻率0.04^^ 中之標向的能譜HJ之比Hi2/H22被設定在3至20的範圍内。 標高的能譜之比Hl2/H22低於3者,係顯示防眩層的細微凹 凸表面中所含之1〇〇/zm以上的長週期之凹凸形狀較少,未 322870 11 201137409 達25_的短週期之凹凸形狀較多者。 止外光的映射,而無法獲得充分的防眩性能Γ此夕 相對 於此,標高的能譜之比h,VH22高於20者,係顯示細微凹凸 表面中所3之1叫'以上的長週期之凹凸形狀較多,未達 25 = m的短週期之凹凸形狀較少者。此時,當將防眩膜配 置在南精細的圖像顯示裝置時,有產生閃斑之傾向。為了 顯不出2更,的防眩性能並更有效地抑制閃斑’標高的能譜 /H2 #乂佳為5至18的範圍内,更佳為8至15的範 圍内。 此外,本發明之防眩膜中,空間頻率G. 1^中之細 微凹凸表面的標高的能譜H32與空間頻率L,中之標 同的月匕4 '之比H32/H22被設定在〇. i以下,較佳設為〇 〇1 以下:比H3/H22為〇」以下者,係顯示可充分地降低細微 凹凸表面中所含之未達10_的短週期成分,藉此可有效 地抑制泛白的產生。細微凹凸表面中所含之未達的 3週期成分1僅未有效地賦作雜,更會使入射於細 从凹凸表面之光散射而成為泛白之原因。 上述日本特開2_-053371號公報等所記載之以往所 知的防眩膜中’由於該空間頻率〇 〇1_ ^之細微凹凸表 面的標南的能譜Hl2與空間頻率0.04^令之標高的能古並 Γ之比Ηΐ7ίί22較本_請案更大,所以有容易產賴斑之問 十因此,為了將比Η冰設定在3至2〇的範圍内,必須 降低辦令之細微凹凸表面的標高的能譜 仏。如此,具有使空間頻率〇鳥〇之細微凹凸表面的 322870 12 201137409 標高的能譜Η’被降低之細微凹凸表面之防眩膜,如後述 般,可藉由使用顯示出在空間頻率大於且為〇._ m以下的⑱H内不具有極大值之能譜的圖案,而理想地製 作出。在此,所謂「圖案」,典型上係意味著絲形成防眩 膜的細微凹凸表面所用之藉由計算機所製作之由2階調 (例如、”呈一值化為白與黑之圖像資料)或3階調以上的階度 所構成之圖像資料,但亦可含有可單—意義地轉換為該圖 像資料之資料(行列#料等)。可單一意義地轉換為圖像資 料之資料,例如有各像素的座標以及僅保存階調之資料等。 如此,藉由使用顯示出在空間頻率大於〇以^且為 〇·〇4从m以下的範圍内不具有極大值之能譜的圖案來形成 防眩膜的細微凹凸表面,可有效地降低空間頻率〇· 中之細微凹凸表面的標高的能譜Hi、而將比HiVH22設定在 3至20的範圍内。 再者,為了獲得具有空間頻率〇. 中之細微凹凸 表面的標高的能譜⑴2與空間頻率0.04/ζπΓ1中之標高的能 譜仏2之比札2/!^為〇. 1以下之細微凹凸表面之防眩膜,前 述圖案的能譜,較佳係在空間頻率較γ大且未達 〇. 1//ΠΓ1之範圍内具有極大值。藉由使用具有此般能譜之圖 案來形成防眩膜的細微凹凸表面,可有效地增大空間頻率 〇. 04 μ nf1中之細微凹凸表面的標高的能譜m2,而將比 Η32/Η22設定在〇. 1以下。 使用此般圖案來形成防眩膜的細微凹凸表面之方法, 較佳為使用該圖案來製作具有凹凸面之模具,並將該模具 322870 13 201137409 的凹凸面轉印至基材膜上所形成之樹脂層的表面之方法 (壓花法)。 本發明者們更發現到,防眩層的細微凹凸表面顯示出 特疋的傾斜角度分布者,可顯示較佳的防眩性能’且更能 夠有效地防止泛白。亦即,本發明之防眩膜中,防眩層的 細微凹凸表面係含有95%以上之傾斜角度為5。以下的面。 當細微凹凸表面的傾斜角度為5。以下之面的比例低於9⑽ 時,凹凸表面的傾斜角度變陡,會將來自周圍的光予以聚 光’而容易產生顯示面全體變白之泛白現象。為了抑制此 聚光效果以防止泛白,細微凹凸表面的傾斜角度為以下 之面的比例愈高者愈佳,較佳為97%以上,尤佳為99%以上。 在此,本發明中所謂「細微凹凸表面的傾斜角度」,是 指參照第2圖,在防眩膜i表面的任意點p中,相對於防 眩膜的主法線方向5’在將該處之凹凸進行加權後之局部 的法線6所成之角度(表面傾斜角度)0。關於細微凹凸表 面的傾斜角度’與標高相同,可從藉由共焦顯微鏡、干涉 顯微鏡、原子力顯微鏡⑽)等裝置所測定之表面形狀的三 維資訊中求取。 第7圖係用以說明細微凹凸表面之傾斜角度的測定方 法之模式圖。說明具體的傾斜角度決定方法時,如第7圖 所不’首先決定出以虛線所示之虛擬平面FG{n上的著眼點 A ’在通過該處之X軸上的著眼點A附近,取相對於點a幾 乎呈對稱之點M D,且在通聰ky紅㈣眼點A 附近’取相對於_點A幾乎呈對稱之點c及E,決 322870 14 201137409 於此等點B、C、D、E之防眩膜面上的點Q、R、S、T。第7 圖中,以(x,y)表示防眩膜面内的正交座標,以z來表示防 眩膜厚度方向的座標。平面FGHI,為分別由通過y軸上的 點C之平行於X轴的直線、以及同樣通過y轴上的點E之 平行於X轴的直線、通過X軸上的點B之平行於y軸的直 線、以及同樣通過X軸上的點D之平行於y軸的直線與各 交叉點F、G、Η、I所形成之面。此外,第7圖中,係以實 際之防眩膜面的位置相對於平面FGHI往上方之方式來描 繪,但當然可因著眼點A的取點位置之不同,使實際之防 眩膜面的位置往平面FGHI的上方或下方。 關於傾斜角度,可藉由從所測得之表面形狀的三維資 訊中,求取將對應於著眼點A之實際防眩膜面上的點p、 與對應於在著眼點A附近所取點之4點B、C、D、E之實際 防眩膜面上的點Q、R、S、τ的合計5點所構成之多邊形的 4個平面、亦即四個三角形?卯、?防、15釘、151^的各法線 向量6a、6b、6c、6d進行平均所得之平均法線向量(平均 法線向量係與第2 ®卿之將凹凸進行加權後之局部的法 線6同義)之相對於防眩膜的主法線方向之極角而獲得。對 各測定點求取傾斜角度後,計算出直方圖。 第8圖係顯示防眩膜所具備之防眩層的細微凹凸表面 之傾斜角度分布的直方圖的_例之圖表。帛8圖所示之圖 表中’橫軸為傾斜角度,且以〇. 為刻度來分割。例如最 左=的直柱,係表示傾斜角度位於〇至〇.^的範圍之集合 的刀布,之後隨著往右方移動,角度每次增加〇. 5。。第8 322870 15 201137409 圖中,係表示出橫轴的每2個刻度之值的下限值,例如, 橫轴2 1_1的部分’表示傾斜角度位於1至I5。的範圍 之集σ的力布。此外,縱軸表示傾斜角度的分布,是合計 為1(100%)之值。此例中,傾斜角度為5。以下之面的比例 大致為100%。 為了製作出防眩層的細微凹凸表面含有95%以上之傾 斜角度為5°以下的面之防_ ’較佳仍是採取使用圖案來 製作具有凹凸面之模具’並將該模具的凹凸面轉印至基材 膜上所形成之樹脂層的表面之方法(壓花法)。此般壓花法 中’防眩層的細微凹凸表面之傾斜角度,是由具有凹凸面 之模具的製造條件來決定。具體而言,可藉由改變後述模 具的製造方法中之㈣卫序的㈣量來進行控制。亦即, 藉由減少第1㈣:L序之㈣量’可減少所形成之第i表 面凹凸形狀的高低差,而增加傾斜角度為5。以下的面之比 率。為了製得具備含有95%以上之傾斜角度為5。以下的面 之細微凹凸表_防眩膜,帛丨㈣卫序之#刻量較佳為 2至8以111。當蝕刻量未達2#m時,金屬表面幾乎無法形成 凹凸形狀而成為幾乎平坦之模具,使用此模具所製作之防 眩膜,無法顯示出充分的防眩性。此外,當蝕刻量超過8 時,形成於金屬表面之凹凸形狀的高低差増大,可能 使傾斜角度為5。以下的面未達95%β使用此模具所製作2 防眩膜’會有產生泛白之疑慮。 此外’亦可藉由第2蝕刻工序之蝕刻量,來控制防眩 層的細微凹凸表面之傾斜角度。藉由增加第2蝕刻工序之 322870 16 201137409 侧量’可有效地將第1表面凹凸形狀之表面傾斜較陡的 部分予以鈍化,而增加傾斜角度為5。以 了製得具備含有95%以上之傾斜角度為5。以下的面之細微 凹凸表面的防眩膜’第2_卫序之餘刻量較佳設為4至 2〇_之範圍内。當_量較小時,將藉由第^刻工序 所得之凹凸的表面雜h鈍化之效料足,轉印該凹凸 形狀所製得之㈣膜的光學特性並㈣。另—方面,者钱 刻量太大時,凹凸形狀幾乎消失而成為幾乎平坦之模:, 所以無法顯示出防眩性。 本發明中,防眩層可由光硬化型樹脂等之硬化型樹脂 的硬化物或熱可塑性樹脂等所構成,當中較佳是由光硬化 型樹脂的硬化物所構成π㈣巾,亦可分散有與硬化型 樹脂的硬化物或熱可龍樹脂具有㈣折射率之微粒。夢 由使微粒分散,更可有效地抑制閃斑。 9 當使上述微粒分散於_層時,微粒的平均粒徑 為5 // m以上,女,伯兔r ,, m ,、,, 可設為ln以為Win μ上。此外,微粒的平均粒獲 欠為,以下“ ’較佳為以下。當平均粒徑低 、㈣時’微粒所造叙廣肖侧的㈣光 用在圖像顯示裳置時,有使對比降低之傾向。田運 塑性:=二折射率〜與硬化型樹脂的硬化物或熱可 ’、3、斤射率ηι_之折射率比w⑴,較佳為以上 以下:下或h 〇1以上h 〇4以下’尤佳為〇· 97以上0.98 或言1 ί·01以上⑽以下。當折射率比Wnr低於0.93 s门;.G4 a夺,硬化型樹脂的硬化物或熱可塑性樹脂與微 322870 17 201137409 粒之界面的反射率增大’結果使後方散射上升,而有總透 光率降低之傾向。總透光率的降低會使防眩膜的霧度增 大’運用在®像顯4置時會產生對比的降低。此外,當 折射率比nb/nr超過〇. 98且未達丨.〇1時,由於微粒所形成 之内部散射效果較小’為了將預定的散射特性賦予至防眩 層以獲付由微粒所致之閃斑抑制效果時,可能必須增加微 粒的添加量。 微粒的含里’相對於硬化型樹脂或熱可塑性樹脂刚 重量份而言’通常為50重量份以下,較佳為40重量份以 下。此外,微粒的含量’較佳為10重量份以上,尤佳為 15重量份以上。當微粒的含量未達1()重量份時微粒所 形成之閃斑抑制效果可能會不足。 構成微粒之材料’較佳為滿足上述較佳折射率比者。 如後述般’本發日种,防眩層的形成較佳係使用ϋν壓花 法’ UV壓花法中’較佳為使用紫外線硬化型樹脂。此時, 由於紫外線硬化型樹脂的硬化物較多係顯示出150左右 的折射率,所以可配合防眩膜的設計,從折射率為i•仙至 1· 60左右者中適田地選擇作為微粒^微粒較佳係使用樹脂 珠粒且為幾乎呈球狀者。該較佳的樹脂珠粒之例,有下列 所揭示者。 二1氣胺珠粒(折射率1 57)、 聚甲基丙婦酸甲酉旨珠粒(折射率1.49)、 曱基丙烯酸甲s旨/苯乙稀共聚物樹脂珠粒(折射率i 5〇. 322870 201137409 聚碳酸酯珠粒(折射率1.55)、 聚乙烯珠粒(折射率1. 53)、 聚苯乙烯珠粒(折射率1. 6)、 聚氯乙烯珠粒(折射率1.46)、 聚矽氧烷樹脂珠粒(折射率1.46)等。 (基材膜) 本發明之防眩膜中所使用之基材膜,是以透明性、耐 濕性、耐候性佳,且機械強度亦佳之丙烯酸系樹脂為主成 分,或是由丙烯酸系樹脂所構成。在此,本發明中所謂丙 烯酸系樹脂,係意味著將曱基丙烯酸樹脂及因應必要所添 加之添加劑等予以混合,並進行溶融摻混而得之材料。 所謂上述曱基丙烯酸樹脂,為以曱基丙烯酸酯為主體 之聚合物。甲基丙烯酸樹脂可為1種甲基丙烯酸酯的單聚 物,或是曱基丙烯酸酯與其他曱基丙烯酸酯或丙烯酸酯等 之共聚物。曱基丙烯酸酯可列舉出曱基丙烯酸曱酯、曱基 丙烯酸乙酯、曱基丙烯酸丁酯等之曱基丙烯酸烷酯,該烷 基的碳數通常約為1至4左右。此外,可與曱基丙烯酸酯 共聚合之丙烯酸酯,較佳為丙烯酸烷酯,例如可列舉出丙 烯酸曱酯、丙烯酸乙酯、丙烯酸丁酯、丙烯酸2-乙基己酯 等,該烷基的碳數通常約為1至8左右。此等之外,亦可 於共聚物中,含有在分子内具有至少1個聚合性碳-碳雙鍵 之化合物之如苯乙烯的芳香族乙烯化合物、或是如丙烯腈 之乙烯氰化合物等。 就基材膜的耐衝擊性和製膜性之觀點來看,丙烯酸樹 19 322870 201137409 脂較佳為含有丙烯酸橡膠粒子。可含有於丙烯酸樹脂之丙 烯酸橡膠粒子的量,較佳為5重量%以上,尤佳為10重量% 以上。丙烯酸橡膠粒子量的上限並無臨限,但當丙烯酸橡 膠粒子量過多時,基材膜的表面硬度會降低,此外,對基 材膜施以表面處理時,會使相對於表面處理劑中的有機溶 劑之财溶劑性降低。因此,可含有於丙稀酸樹脂之丙稀酸 橡膠粒子的量,較佳為80重量%以下,尤佳為60重量%以 下。 上述丙烯酸橡膠粒子,為將以丙烯酸酯為主體之彈性 聚合體用作為必要成分之粒子,可為實質上僅由該彈性聚 合體所構成之單層構造,或是將該彈性聚合體構成為1層 之多層構造。具體而言,該彈性聚合體較佳為使用藉由下 列單體組成物的聚合所得之交聯彈性共聚物,該單體組成 物是由:丙烯酸烧醋50至99.99重量%、至少1種之可與 該丙烯酸烷酯共聚合之其他乙烯系單體0至49. 9重量%、 以及共聚合性的交聯性單體0. 1至10重量%所構成。 形成彈性聚合體之上述丙烯酸烷酯,例如可列舉出丙 烯酸甲酯、丙烯酸乙酯、丙烯酸丁酯、丙烯酸2-乙基己酯 等,該烷基的碳數通常約為1至8左右。此外,可與上述 丙烯酸烷酯共聚合之其他乙烯系單體,可列舉出在分子内 具有1個聚合性碳-碳雙鍵之化合物,更具體而言,可列舉 出如甲基丙烯酸曱酯的曱基丙烯酸酯、如苯乙烯的芳香族 乙烯化合物、如丙烯腈之乙烯氰化合物等。此外,上述共 聚合性的交聯性單體,可列舉出在分子内具有至少2個聚 20 322870 201137409 合性碳-碳雙鍵之交聯性的化合物,具體而言,可列舉出如 二(甲基)丙烯酸乙二醇酯和二(甲基)丙烯酸丁二醇酯之多 元醇的(甲基)丙稀酸酯、如(曱基)丙烯酸埽丙酯和(甲基) 丙稀酸甲基烯丙醋之基)丙烯酸的烯酯、二乙稀苯等。 本就明書令,所謂(甲基)丙烯酸酯,是指甲基丙烯酸酯或 丙烯酸酯,所謂(甲基)丙烯酸,是指甲基丙烯酸或丙烯酸。 丙烯酸系樹脂中,除了上述丙烯酸橡膠粒子外,亦可 含有通常的添加劑,例如有紫外線吸收劑、有機系染料、 顏料、無機系色素、抗氧化劑、防帶電劑、界面活性劑等。 當中就提高耐候性來看,可較佳地使用紫外線吸收劑。紫 外線吸收劑的例子,可列舉出如2,2,_亞甲基雙[4_〇, ^ 3,3-四曱基丁基)-6一(211_苯并三唑_2_基)酚]、2_(5_甲基 -2-羥笨基)-2H-苯并三唑、2—[2-羥基-3, 5-雙(α,α 一二曱 基苯曱基)苯基-2Η-笨并兰唾、2_(3,5一二_三級丁基_2_經 苯基)-2Η-苯并三唾、2-(3-三級丁基_5_甲基_2_經苯基) -5-氣普苯并三唾、2_(3,5_二_三級丁基_2_經苯基)_5_ 氯普苯并三唾、2'(3,5_二-三級戊基-2-經苯基)-2H-苯 并三嗤、2-(2’-經基十―三級辛基苯基)_2H_苯并三嗤之笨 并三°坐系紫外線吸收劑;如2-減-4-曱氧二苯基嗣、2_ 經基-4-辛氧二笨基酮、2,4_二經基二苯基酮、2_經基+ 甲氧-4二-氯二苯基,、2,2,-二經基―&quot;氧二苯基鋼、 , 丰工土 ’4 一甲氧二苯基酮之2-經基二苯基酮系 紫外線吸收劑;如柳酸對三級丁基苯S旨、柳酸對辛基苯醋 之柳酸笨酯系紫外線圾收兔,&amp; ^ 收Μ 4,可因應必要使用此等的2 322870 21 201137409 種以上。當丙烯酸系樹脂中含有紫外線吸收劑時,該量通 常為0. 1重量%以上,較佳為0. 3重量%以上,此外,較佳 為2重量%以下。 基材膜的厚度,就機械強度及處理性之觀點,並且就 防眩層形成時防止膜片的捲曲之觀點來看,較佳為 以上,此外,就圖像顯示裝置的薄型化及成本等觀點來看, 較佳為100_以下。基材膜的厚度,尤佳為4心 80 a m以下。 本發明之防眩膜中所使用之基材膜的製造方法,例如 可使用熔融擠壓成形等一般所知的種種方法。當中,就了 製得表面性狀良好的膜片之觀點來看,較佳為從了模^進 行熔融擠壓成形,並將所得之熔融狀膜片的至少單面接觸 於親表面或皮帶表面來製膜之方法。尤其就提升基材膜的 表面平滑性及表面光澤性之觀點來看,較佳為使上述溶融 擠壓成形所得之熔融狀膜片的雙面接觸铃輥表面或皮^表 面來製膜之方法。此時所使用之輥或皮帶十,與丙烯$樹 月曰的熔融狀膜片接觸之輥表面或皮帶表面, 表面賦予平滑性,較佳為鏡面。 ’ 土材膜 基材膜可由多層構造所構成,此般多層構造可列舉出 含有丙烯酸橡膠粒子之層與不含有丙稀酸橡膠粒子之屛之 積層構造。具有多層構造之基材膜,例如可藉由採用有八 流器(feed block)或多歧管鑄模等之多層熔融擠壓成形1 適當地製作出。藉由將基材膜構成為多層構造,可將^反 的特性賦予至基材膜。例如,於中間層具備含有丙稀 322870 22 201137409 膠粒子之層,且於表層的最表面具備不含有丙稀酸橡膠粒 •子之層之多層構造的基材膜,可藉由含有丙婦酸橡膠粒子 •之中間層而具有高耐衝擊性,並且藉由不含有丙烯酸橡朦 粒子之表層而具有高表面硬度。 此外’本發明之防眩膜中所使用之基材膜,亦可為對 ^上迷所得的丙烯酸系樹脂所構成之膜片施以拉伸處理後 者。藉由拉伸處理,可賦予更強的耐衝擊性。拉伸方法可 為任意方法,並無特別限定,可列舉出在玻璃轉移溫度从 上的溫度,以拉幅機進行橫向拉伸後施以熱固定處理之方 法,或是在玻璃轉移溫度以上的溫度,以拉幅機進行縱向 =伸後施以熱固定處理,然後再進行横向拉伸後施以熱固 疋處理之方法。 &lt;防眩膜的製造方法&gt; 上述本發明之防眩膜,較佳係藉由含有下列工序(A) 及工序(B)之方法來製造出。 (A) 根據顯示出在空間頻率大於0“^且為0.04“^! 以下的fe圍内不具有極大值之能譜的圖案,來製作出具有 凹凸面之模具之工序;以及 (B) 將模具的凹凸面,轉印至形成於基材膜上並含有光 硬化性樹脂等硬化性樹脂或熱可塑性樹脂等之樹脂層的表 面之工序。 ^藉由使用在空間頻率大於ΟΜΠΓ1且為0.04/ζπΓ1以下的 範圍内不具有極大值之能譜的圖案,能夠精度佳地形成具 有上述特定的空_率分布之細微凹凸表面。此外,藉由 322870 23 201137409 根據該圖案製作出具有凹凸面之模具,並將該模具的凹凸 面轉印至形成於基材膜上之樹脂層的表面之方法(壓花 法),能夠精度佳且重現性良好地製得具有細微凹凸表面之 防眩層。在此,所謂「圖案」,典型上係意味著用來形成防 眩膜的細微凹凸表面所用之藉由計算機所製作之由2階調 (例如經二值化為白與黑之圖像資料)或3階調以上的階度 所構成之圖像資料,但亦可含有可單一意義地轉換為該= 像資料之資料(行列資料等)。可單—意義地轉換為圖像資 料之資料’例如有各料的絲以及鶴雜敵資料等。 上述序(A)所用之圖案的能譜,例如若為圖像資料 時’可藉由在將圖像資料轉換為2階調的(Λ^ + 1) Δχ (3) ¥y = (N+l)Ay Formula U) Figure 4 shows the anti-glare film of the present invention with a two-dimensional discrete function h(x, y) An example of a map of the elevation of the fine uneven surface of the glare layer. In Fig. 4, the elevation is expressed in terms of white and black gradations. Figure 4 shows the scatter function h(x, y) with 512x512 values, horizontal decomposition energy Δχ and Ay . 1.66 y m. % Fig. 5 is a diagram showing the energy spectrum H2(fx, fy) of the elevation obtained by discrete Fourier transform of the two-dimensional function h(x, y) shown in Fig. 4 in white and black gradation. . The energy spectrum H2(fx,fy) of the elevation shown in Fig. 5 is also a discrete function with 512x512 values, and the horizontal decomposition energy Δ and Δ of the energy spectrum of the elevation. It is 0.0012VHT1. As shown in Fig. 4, since the fine uneven surface of the antiglare layer provided in the antiglare film of the present invention is composed of randomly formed irregularities, the energy spectrum H2 of the standard south is as shown in Fig. 5. It is symmetrical with the origin as the center. Therefore, the energy spectrum of the elevation in the spatial frequency of 0.01 ynf1 can be obtained from the profile of the origin of the energy spectrum H2 (fx, fy) belonging to the two-dimensional function 2、! 2, the elevation of the spatial frequency of 0. 04 μ m_1 Energy spectrum (1) 2 and spatial frequency 〇. 1 The energy spectrum of the elevation in enf1 Η /. Fig. 6 is a view showing a cross section of f χ = 〇 in the energy spectrum H ( f X, f y ) shown in Fig. 5. It can be seen from Fig. 6 that the energy spectrum (1) 2 of the elevation in the spatial frequency of 0.01/zm-1 is 4.4, and the spatial frequency 〇〇4 has an energy spectrum 仏2 of the elevation of πΓ1 of 0.35, and the spatial frequency 〇. 1 The energy spectrum H32 of the elevation in enf1 is 〇· 00076, which is 14 for 2/%2 and 0.0022 for H32/H22. As described above, in the anti-glare film of the present invention, the ratio Hi2/H22 of the energy spectrum Hl2 of the level of the fine uneven surface in the spatial frequency O.Wyf and the energy spectrum HJ of the spatial frequency of 0.04^^ is set at 3 to 20 range. The ratio of the energy spectrum of the elevation is lower than that of the Hl2/H22, which indicates that the long-period irregular shape of 1 〇〇/zm or more contained in the fine uneven surface of the anti-glare layer is small, and 322870 11 201137409 is 25_ There are many irregular shapes in short cycles. The external light is not mapped, and sufficient anti-glare performance cannot be obtained. On the other hand, the ratio of the energy spectrum of the elevation h, VH22 is higher than 20, and it is shown that 3 of the fine uneven surface is longer than ' There are many irregularities in the period, and the uneven shape of the short period of 25 = m is less. At this time, when the anti-glare film is disposed in the south-fine image display device, there is a tendency to generate a flare. In order to show the anti-glare property of 2, the energy spectrum of the speckle level is more effectively suppressed, and the H2 #乂 is preferably in the range of 5 to 18, more preferably in the range of 8 to 15. Further, in the anti-glare film of the present invention, the ratio H32/H22 of the energy spectrum H32 of the level of the fine uneven surface in the spatial frequency G. 1^ and the space frequency L, which is the same as the same, is set at 〇 i or less, preferably 〇〇1 or less: less than H3/H22 ,", it is shown that the short period component of less than 10 _ contained in the surface of the fine uneven surface can be sufficiently reduced, thereby effectively Inhibit the generation of whitening. The three-cycle component 1 which is not contained in the fine uneven surface is not effectively miscible, and the light incident on the fine uneven surface is scattered to cause whitening. In the conventional anti-glare film described in the above-mentioned Japanese Patent Publication No. 2-053371, the energy spectrum Hl2 of the southmost surface of the fine uneven surface of the spatial frequency 〇〇1_^ and the spatial frequency of 0.04^ are used. The ratio of the ancient Γ Ηΐ ί 7 ί Ηΐ ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί ί The energy spectrum of the elevation is 仏. In this way, the anti-glare film having the fine embossed surface of the 322870 12 201137409 elevation of the surface of the ostrich 空间 空间 , 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被 被18._m below 18H does not have a pattern of maximum energy spectrum, and is ideally produced. Here, the "pattern" generally means that the silk is formed into a fine concavo-convex surface of the anti-glare film by a computer-made image data of a second-order tone (for example, "valued to white and black". ) or image data composed of gradations above the 3rd order, but may also contain data that can be converted into the image data in a single meaning - (in the order ##, etc.). It can be converted into image data in a single meaning. The data includes, for example, the coordinates of each pixel and the data of only the tone, etc. Thus, by using the spectrum which shows that the spatial frequency is larger than 〇 and that 〇·〇4 has a maximum value from m or less The pattern is formed to form a fine uneven surface of the anti-glare film, and the energy spectrum Hi of the elevation of the fine uneven surface in the spatial frequency 有效· can be effectively reduced, and the HiVH22 is set in the range of 3 to 20. Further, in order to obtain The ratio of the energy spectrum (1)2 of the elevation of the surface of the fine uneven surface in the spatial frequency 〇. to the energy spectrum 仏2 of the elevation in the spatial frequency of 0.04/ζπΓ1 is 2/!^ is 防. 1 below the anti-glare film of the fine uneven surface The energy spectrum of the aforementioned pattern is preferably The frequency is larger than γ and does not reach 〇. The maximum value is in the range of 1//ΠΓ 1. By using the pattern with such energy spectrum to form the fine concave and convex surface of the anti-glare film, the spatial frequency can be effectively increased. The energy spectrum m2 of the level of the fine uneven surface in 04 μ nf1 is set to be less than or equal to 1 Η 32/Η22. The method of forming the fine uneven surface of the anti-glare film using such a pattern is preferably used. A method of producing a mold having a concave-convex surface and transferring the uneven surface of the mold 322870 13 201137409 to the surface of the resin layer formed on the base film (embossing method). The inventors have found that anti-glare The fine uneven surface of the layer exhibits a characteristic oblique angle distribution, which can exhibit better anti-glare performance' and is more effective in preventing whitening. That is, in the anti-glare film of the present invention, the fine unevenness of the anti-glare layer The surface system contains 95% or more of the inclined angle of 5. The following surface. When the inclination angle of the fine uneven surface is 5. When the ratio of the surface below is less than 9 (10), the inclination angle of the uneven surface becomes steep, and the light from the surroundings is obtained. Collecting light' It is easy to cause a whitening phenomenon in which the entire display surface is whitened. In order to suppress the condensing effect to prevent whitening, the inclination of the surface of the fine uneven surface is preferably as high as possible, preferably 97% or more. Here, the "inclination angle of the fine uneven surface" in the present invention means the main normal direction with respect to the anti-glare film at any point p on the surface of the anti-glare film i with reference to Fig. 2 5' The angle (surface tilt angle) of the local normal 6 which is weighted by the unevenness at this point is 0. The inclination angle ' of the fine uneven surface is the same as the elevation, and can be obtained from three-dimensional information of the surface shape measured by a device such as a confocal microscope, an interference microscope, or an atomic force microscope (10). Fig. 7 is a schematic view for explaining a method of measuring the inclination angle of the fine uneven surface. When the specific tilt angle determining method is described, as shown in FIG. 7, it is first determined that the eye point A' on the virtual plane FG{n indicated by the broken line is near the eye point A on the X-axis passing through the point. The point MD is almost symmetric with respect to point a, and is near the point A of the Tongchong ky red (four) eye point 'points c and E which are almost symmetrical with respect to _ point A, 322870 14 201137409 at these points B, C, Points Q, R, S, and T on the anti-glare film surface of D and E. In Fig. 7, (x, y) denotes an orthogonal coordinate in the plane of the anti-glare film, and z denotes a coordinate in the thickness direction of the anti-glare film. The plane FGHI is a line parallel to the X-axis passing through the point C on the y-axis, and a line parallel to the X-axis passing through the point E on the y-axis, respectively, passing through the point B on the X-axis parallel to the y-axis. The straight line and the line formed by the straight line parallel to the y-axis of the point D on the X-axis and the intersections F, G, Η, and I. In addition, in Fig. 7, the position of the actual anti-glare film surface is drawn upward with respect to the plane FGHI, but of course, the actual anti-glare film surface can be made different depending on the position of the eye point A. Position above or below the plane FGHI. Regarding the tilt angle, the point p corresponding to the actual anti-glare film surface corresponding to the eye point A and the point corresponding to the point near the eye point A can be obtained from the three-dimensional information of the measured surface shape. Four points B, C, D, and E The four planes of the polygon formed by the total of five points Q, R, S, and τ on the anti-glare film surface, that is, four triangles? Hey,? The average normal vector obtained by averaging the normal vectors 6a, 6b, 6c, and 6d of the anti-fence, 15 nails, and 151^ (the average normal vector system and the local normal 6 of the 2nd s Synonymous) is obtained with respect to the polar angle of the main normal direction of the anti-glare film. After obtaining the tilt angle for each measurement point, the histogram is calculated. Fig. 8 is a graph showing a histogram of a histogram of the inclination angle distribution of the fine uneven surface of the antiglare layer provided in the antiglare film. In the graph shown in Fig. 8, the horizontal axis is the oblique angle and is divided by 〇. For example, the straight column of the leftmost = is a knife cloth whose inclination angle is located in the range of 〇 to 〇.^, and then the angle increases by 〇. 5 each time as it moves to the right. . No. 8 322870 15 201137409 In the figure, the lower limit value of the value of every two scales of the horizontal axis is shown. For example, the portion ' of the horizontal axis 2 1_1 indicates that the inclination angle is from 1 to I5. The scope of the set of σ force cloth. Further, the vertical axis indicates the distribution of the inclination angles and is a value of 1 (100%) in total. In this case, the tilt angle is 5. The ratio of the following is approximately 100%. In order to produce a surface of a fine uneven surface of the anti-glare layer, which has a surface having an inclination angle of 5° or less of 5° or less, it is preferable to use a pattern to form a mold having a concave-convex surface and to rotate the uneven surface of the mold. A method of printing onto the surface of a resin layer formed on a substrate film (embossing method). In the embossing method, the inclination angle of the fine uneven surface of the antiglare layer is determined by the manufacturing conditions of the mold having the uneven surface. Specifically, it is possible to control by changing the (four) amount of the (four) guard sequence in the manufacturing method of the mold described later. That is, by reducing the (fourth)th of the first (fourth):th order, the height difference of the uneven shape of the i-th surface formed can be reduced, and the inclination angle is increased by five. The ratio of the following faces. In order to obtain an angle of inclination of 5 with 95% or more. The following surface fine embossing table _ anti-glare film, 帛丨 (4) 卫序# is preferably 2 to 8 to 111. When the etching amount is less than 2 #m, the metal surface is hardly formed into a concave-convex shape and becomes a nearly flat mold, and the anti-glare film produced by using the mold cannot exhibit sufficient anti-glare property. Further, when the etching amount exceeds 8, the height difference of the uneven shape formed on the metal surface is large, and the inclination angle may be 5. The following surface is less than 95% β. The anti-glare film produced by using this mold has the suspicion of whitening. Further, the inclination angle of the fine uneven surface of the antiglare layer can be controlled by the etching amount of the second etching step. By increasing the side amount 322870 16 201137409 of the second etching step, the portion of the surface of the first surface uneven shape which is steeply inclined can be effectively passivated, and the inclination angle is increased to 5. In order to obtain an angle of inclination of 5 or more. The amount of the second anti-glare film of the fine uneven surface of the following surface is preferably set to be in the range of 4 to 2 Å. When the amount of _ is small, the optical characteristics of the film obtained by transferring the uneven shape by the surface of the uneven surface obtained by the second etching step are transferred (4). On the other hand, when the amount of money is too large, the uneven shape almost disappears and becomes an almost flat mold: therefore, the anti-glare property cannot be exhibited. In the present invention, the antiglare layer may be composed of a cured product of a curable resin such as a photocurable resin or a thermoplastic resin, and among them, a π (four) towel composed of a cured product of a photocurable resin is preferably used, and may be dispersed. The hardened resin or the heat-resistant resin has (four) refractive index particles. Dream By dispersing the particles, it is more effective in suppressing the flare. 9 When the above particles are dispersed in the layer, the average particle size of the particles is 5 // m or more, and the female, rabbit, r, m, and , can be set to ln to be Win μ. In addition, the average particle yield of the microparticles is less than, the following "' is preferably the following. When the average particle diameter is low, (4)" when the microparticles are used to make the (4) light on the side of the image, the contrast is lowered when the image is displayed. Tendency of the field: plasticity of the field: = the ratio of the refractive index of the second refractive index to the cured product of the hardened resin or the heat, '3, and the ratio of the refractive index ηι_, w(1), preferably the above or lower: lower or h 〇 1 or more h 〇4 or less 'Easy is 〇·97 or more 0.98 or 言1 ί·01 or more (10) or less. When the refractive index ratio Wnr is lower than 0.93 s; G4 a, hardened resin or thermoplastic resin and micro 322870 17 201137409 Increased reflectivity at the interface of the grain 'The result is that the backscattering increases, and the total light transmittance decreases. The decrease in total light transmittance increases the haze of the anti-glare film. When the refractive index ratio nb/nr exceeds 〇. 98 and does not reach 丨.〇1, the internal scattering effect due to the microparticles is small' in order to impart predetermined scattering characteristics to When the anti-glare layer is subjected to the effect of suppressing the speckle caused by the particles, it may be necessary to increase the micro The amount of the fine particles is usually 50 parts by weight or less, preferably 40 parts by weight or less, relative to the hardening type of the resin or the thermoplastic resin. Further, the content of the fine particles is preferably 10 parts by weight. More preferably, it is 15 parts by weight or more. When the content of the fine particles is less than 1 part by weight, the effect of suppressing the speckle formed by the fine particles may be insufficient. The material constituting the fine particles preferably satisfies the above preferred refractive index ratio. As described later, it is preferable to use the ϋν embossing method in the UV embossing method. It is preferable to use an ultraviolet curing resin. In this case, the curing of the ultraviolet curing resin is used. Since a large amount of material exhibits a refractive index of about 150, it can be combined with the design of an anti-glare film, and it is preferable to use a resin bead as a fine particle from a refractive index of i•xian to about 1.60. It is almost spherical. Examples of the preferred resin beads are as follows. 1-2 Amine beads (refractive index 1 57), polymethyl propyl acetoacetate beads (refractive index) 1.49), mercapto acrylate styrene / styrene Polymer resin beads (refractive index i 5〇. 322870 201137409 polycarbonate beads (refractive index 1.55), polyethylene beads (refractive index 1.53), polystyrene beads (refractive index 1. 6), Polyvinyl chloride beads (refractive index 1.46), polyoxyalkylene resin beads (refractive index 1.46), etc. (Substrate film) The substrate film used in the antiglare film of the present invention is transparent and resistant. An acrylic resin which is excellent in wetness and weather resistance and which is excellent in mechanical strength is mainly composed of an acrylic resin. Here, the acrylic resin in the present invention means a thiol based acrylic resin and a necessary The added additives and the like are mixed and melt-blended and obtained. The above-mentioned mercaptoacrylic resin is a polymer mainly composed of mercaptoacrylate. The methacrylic resin may be a monomeric methacrylate or a copolymer of mercapto acrylate with other mercapto acrylate or acrylate. The mercapto acrylate may, for example, be an alkyl acrylate such as decyl acrylate, decyl acrylate or butyl methacrylate, and the alkyl group usually has a carbon number of about 1 to 4. Further, an acrylate copolymerizable with a mercapto acrylate, preferably an alkyl acrylate, may, for example, be decyl acrylate, ethyl acrylate, butyl acrylate, 2-ethylhexyl acrylate or the like, the alkyl group The carbon number is usually about 1 to 8. Further, in the copolymer, an aromatic vinyl compound such as styrene having a compound having at least one polymerizable carbon-carbon double bond in the molecule or an ethylene cyanide compound such as acrylonitrile may be used. The acrylic tree 19 322870 201137409 preferably contains acrylic rubber particles from the viewpoint of impact resistance and film forming properties of the base film. The amount of the acrylic rubber particles which may be contained in the acrylic resin is preferably 5% by weight or more, and particularly preferably 10% by weight or more. The upper limit of the amount of the acrylic rubber particles is not limited, but when the amount of the acrylic rubber particles is too large, the surface hardness of the base film is lowered, and when the surface treatment is applied to the base film, it is relative to the surface treatment agent. The solvent solubility of organic solvents is reduced. Therefore, the amount of the acrylic rubber particles which may be contained in the acrylic resin is preferably 80% by weight or less, and particularly preferably 60% by weight or less. The acrylic rubber particles are particles in which an elastic polymer mainly composed of acrylate is used as an essential component, and may be a single layer structure consisting essentially of only the elastic polymer, or the elastic polymer may be composed of 1 Multilayer construction of layers. Specifically, the elastic polymer is preferably a crosslinked elastic copolymer obtained by polymerization of the following monomer composition, which is composed of: acrylic vinegar 50 to 99.99% by weight, at least one type 1至十重量百分比的。 The other vinyl monomer copolymerized with the alkyl acrylate is 0 to 49.9% by weight, and the copolymerizable crosslinkable monomer 0.1 to 10% by weight. The alkyl acrylate which forms the elastic polymer may, for example, be methyl acrylate, ethyl acrylate, butyl acrylate or 2-ethylhexyl acrylate. The alkyl group usually has a carbon number of about 1 to 8. Further, examples of the other vinyl monomer copolymerizable with the above alkyl acrylate include a compound having one polymerizable carbon-carbon double bond in the molecule, and more specifically, decyl methacrylate. A mercapto acrylate, an aromatic vinyl compound such as styrene, an ethylene cyanide compound such as acrylonitrile, or the like. Further, the above-mentioned copolymerizable crosslinkable monomer may, for example, be a compound having at least two crosslinks of poly 20 322870 201137409 conjugated carbon-carbon double bond in the molecule, and specifically, for example, (Meth) acrylates of polyols of (meth)acrylic acid glycol and butylene glycol di(meth)acrylate, such as (mercapto) propyl acrylate and (meth) acrylic acid An allyl ester of methacrylic acid acrylate, diethyl benzene, and the like. In the present specification, the term "(meth)acrylate" means methacrylate or acrylate, and the term "(meth)acrylic acid" means methacrylic acid or acrylic acid. The acrylic resin may contain a usual additive in addition to the above acrylic rubber particles, and examples thereof include an ultraviolet absorber, an organic dye, a pigment, an inorganic dye, an antioxidant, an antistatic agent, and a surfactant. In view of improving weather resistance, an ultraviolet absorber can be preferably used. Examples of the ultraviolet absorber include, for example, 2,2,-methylenebis[4_fluorene, ^3,3-tetradecylbutyl)-6-(211-benzotriazole-2-yl). Phenol], 2_(5-methyl-2-hydroxyphenyl)-2H-benzotriazole, 2-[2-hydroxy-3,5-bis(α,α-dimercaptophenyl)phenyl -2Η-stupid and salivary, 2_(3,5-di-tertiary butyl-2-phenyl)-2-indole-benzotrisole, 2-(3-tri-butyl-5-methyl- 2_Phenyl) -5-gas benzotrisole, 2_(3,5-di-tertiary butyl-2-yl-phenyl)_5_ chloroprobenzo-salt, 2' (3,5_ Di-tertiary pentyl-2-phenyl)-2H-benzotrimethylene, 2-(2'-transyl-10-thanooctylphenyl)_2H_benzotrimide UV absorber; such as 2- minus 4-oxime diphenyl hydrazine, 2_ thio-4-octyloxy dipyridyl ketone, 2,4-di-diphenyl ketone, 2 _ base + methoxy -4 di-chlorodiphenyl, 2,2,-di-based-&quot;oxydiphenyl steel, , Fenggong soil '4-methoxydiphenyl ketone 2-based diphenyl ketone Ultraviolet absorber; such as salicylic acid for tertiary butylbenzene, salicylic acid, octyl benzene vinegar, stearic acid, ultraviolet light, rabbit, &amp; ^ receiving 4, can be necessary The use of such above 232287021 201137409 kinds. When the amount of the ultraviolet ray absorbing agent is, the amount is usually 0.1% by weight or more, preferably 0.3% by weight or more, and more preferably 2% by weight or less. The thickness of the base film is preferably from the viewpoint of preventing the film from being curled when the antiglare layer is formed, from the viewpoint of the mechanical strength and the handleability, and the thickness and cost of the image display device. From the viewpoint, it is preferably 100_ or less. The thickness of the base film is preferably 4 or less and 80 a m or less. In the method for producing the base film used in the antiglare film of the present invention, for example, various methods generally known, such as melt extrusion molding, can be used. Among them, from the viewpoint of producing a film having a good surface property, it is preferred to carry out melt extrusion molding from the mold, and to contact at least one side of the obtained molten film sheet to the surface of the surface or the belt surface. The method of film making. In particular, from the viewpoint of improving the surface smoothness and surface gloss of the base film, it is preferred to form a film by double-sided contact with the surface of the ring roll or the surface of the molten film obtained by the melt extrusion molding. . The roll or belt 10 used at this time has a smooth surface, preferably a mirror surface, on the surface of the roll or the surface of the belt which is in contact with the molten film of propylene. The earth material film base film may be composed of a multilayer structure, and the multilayer structure may be a laminated structure including a layer containing acrylic rubber particles and a crucible containing no acrylic rubber particles. The substrate film having a multilayer structure can be suitably produced, for example, by multilayer melt extrusion molding 1 using a feed block or a multi-manifold mold. By forming the base film into a multilayer structure, the properties of the substrate can be imparted to the substrate film. For example, a substrate film having a layer containing propylene 322870 22 201137409 gel particles in the intermediate layer and having a multilayer structure not containing a layer of acrylic rubber particles on the outermost surface of the surface layer may be provided with a propylene glycol acid layer The intermediate layer of the rubber particles has high impact resistance and has high surface hardness by not containing the surface layer of the acrylic rubber particles. Further, the substrate film used in the antiglare film of the present invention may be subjected to a stretching treatment on a film formed of the acrylic resin obtained above. By the stretching treatment, stronger impact resistance can be imparted. The stretching method may be any method, and is not particularly limited, and examples thereof include a method in which the glass transition temperature is higher than the temperature, a transverse stretching by a tenter, and a heat setting treatment, or a glass transition temperature or higher. The temperature is longitudinally set by a tenter = heat-fixed after stretching, and then subjected to transverse solid stretching and then subjected to a heat-solid treatment. &lt;Method for Producing Antiglare Film&gt; The antiglare film of the present invention is preferably produced by a method comprising the following steps (A) and (B). (A) a process of producing a mold having a concave-convex surface according to a pattern showing an energy spectrum having a maximum value in a space having a spatial frequency greater than 0"^ and 0.04"^! or less; and (B) The uneven surface of the mold is transferred to a surface of the resin layer formed of a curable resin such as a photocurable resin or a thermoplastic resin, which is formed on the base film. By using a pattern having an energy spectrum having a maximum value in a range where the spatial frequency is larger than ΟΜΠΓ1 and 0.04/ζπΓ1 or less, the fine uneven surface having the above-described specific space-rate distribution can be formed with high precision. Further, by the method of producing a mold having a concave-convex surface from the pattern by 322870 23 201137409, and transferring the uneven surface of the mold to the surface of the resin layer formed on the base film (embossing method), the precision can be improved. An anti-glare layer having a fine uneven surface is produced with good reproducibility. Here, the "pattern" generally means a second-order tone (for example, binarized image data of white and black) which is used by a computer for forming a fine uneven surface of an anti-glare film. Or image data consisting of gradation above the 3rd order, but may also contain information (array, etc.) that can be converted into the image data in a single sense. It can be converted into information of image data in a single sense. For example, there are silks of various materials and information on cranes and other enemies. The energy spectrum of the pattern used in the above sequence (A), for example, if it is image data, can be converted into a 2nd order by image data.

後’以二維函…來表示圖綱的階調,=: 之-維函數g(X,y)進行離散傅利葉轉換而計算出二維 咖,w ’然後將所得之二維函數G(fx,f〇進行平方運算而 求取。在此,X及y係表示圖像資料面内的正交座桿,£ 及fy分別表示X方向的空間頻率及y方向的空間頻率「。X 與求取細微凹凸表面的標高之能譜相同’關於求取圖 案的能譜時,階調的二維函數g(x,y),一般是作為離散函 數而獲得。此時,與求取細微凹凸表面的標高之能譜 可藉由離散傅利葉轉換來計算出能譜。具體而 式⑸所定義之離散傅利葉轉換來計算出‘ 咖,,然後將所得之離散函數邮,fy)進 数 求取能峰,fy)。在此,式⑸中的V為圓周率,= 數早位。此外,Μ為X方向的像素數,方向的像素數, 322870 24 201137409 1為-M/2以上M/2以下之整數,m為_^/2以上N/2以下之 整數。再者’ 分別為χ方向及y方向的空間頻 率間隔,並分別由式(6)及式(7)所定義。式(6)及式(7)中 之Δχ及Ay分別為X軸方向及y軸方向的水平分解能。當 圖案為圖像資料時分別與!個像素轴方: 的長度及y軸方向的長度相等。亦即,當將圖案製作為 6棚dpi的圖像資料時,化…㈣,當將圖案製作為 12800dpi的圖像資料時, 也 Λ)=敎叙㈣ exp[-2 如 式(5)After the 'two-dimensional letter... to represent the tone of the figure, =: the -dimensional function g (X, y) performs discrete Fourier transform to calculate the two-dimensional coffee, w 'and then the resulting two-dimensional function G (fx , f 〇 is calculated by squaring. Here, X and y represent the orthogonal seatpost in the image data plane, and £ and fy respectively represent the spatial frequency in the X direction and the spatial frequency in the y direction. The energy spectrum of the elevation of the surface of the fine concave and convex surface is the same. 'When the energy spectrum of the pattern is obtained, the two-dimensional function g(x, y) of the tone is generally obtained as a discrete function. At this time, the surface of the fine concave surface is obtained. The energy spectrum of the elevation can be calculated by the discrete Fourier transform to calculate the energy spectrum. Specifically, the discrete Fourier transform defined by equation (5) is used to calculate the 'caffe, and then the obtained discrete function is sent, fy) to obtain the energy peak. Fy) Here, V in the formula (5) is a pi, and a number is early. Further, Μ is the number of pixels in the X direction, and the number of pixels in the direction, 322870 24 201137409 1 is an integer of -M/2 or more and M/2 or less. , m is an integer of _^/2 or more and N/2 or less. Further, 'the space between the χ direction and the y direction is respectively And are defined by equations (6) and (7), respectively. Δχ and Ay in equations (6) and (7) are horizontal decomposition energies in the X-axis direction and the y-axis direction, respectively. When the pattern is image data It is equal to the length of the pixel axis: and the length of the y-axis direction. That is, when the pattern is made into 6 shed dpi image data, (4), when the pattern is made into 12800 dpi image data , also Λ) = 敎 ( (4) exp[-2 as in (5)

Afy^¥^ 式⑺ 第9圖係顯示可用以製作本發明之防眩膜所使用之圖 案的圖像資料的-部分之圖,為以階調的二維離散函數 g(x’y)來表不者。第9圖所示之圖案的圖像資料為2_2咖 的大小,且以12800dpi來製作。 第10圖係以白與黑的階度來表示將第9圖所示之階調 1 一維函數g(x,y)進行離散傅利葉轉換所得之能譜 G (fx, fy)之圖。由於第9圖所示之圖案係隨機地配置點者, 因此,該能譜G2(fx,fy)如第1〇圖所示,係以原點為中心呈 對稱。因此,可從通過能譜的原點之剖面,來求取圖案之 顯不能譜G(fx,fy)的極大值的空間頻率。第n圖係顯示第 322870 25 201137409 10圖所示之能譜G2(fx,fy)中的fx=〇時之刮面的圖。從該圖 中可得知,第9圖所示之圖案在空間頻率〇· 〇45#mH中具 有極大值,但在較O/im 1還大且為〇 Q4wra-i以下時不具有 極大值。 當用以製作防眩膜之圖案的能譜G2(fx,fy),在較〇 //πΓ1還大且為〇.〇4vnT1以下的空間頻率範圍内具有極大 值時,所得之防眩膜的細微凹凸表面並未顯示出上述特定 的空間頻率分布,所以無法同時達成閃斑的消除以及充分 的防眩性。 能譜G2(fx,fy)在較〇 # γ還大且為〇. 〇4 # γ,以下的空 間頻率範圍内不具有極大值之圖案,例如第9圖所示之圖 案舨,可藉由隨機且均一地配置多數個點而製作出。隨機 地配置之點徑可為1種或複數種。此外,隨機地配置多數 個點所製作之圖案中,能譜係在屬於點間的平均距離的倒 數之空間頻率上顯示出第一極大值(空間頻率較0“^還 大之最小的空間頻率中的極大值^因此,為了製作出能譜 在較W還大且為0.04/zm-i以下的空間頻率範圍内不: 有極大值之圖案,只需以使點間的平均距離未達25am之 方式製作圖案即可。此外’為了將防眩膜之空間頻率〇1 中之細微凹凸表面的標高的能譜⑴2與空間頻率〇 〇4 中之標高的能譜仏2之比設為〇.丄以下,圖案的 能譜較佳係在空間頻率大於〇. 〇4 μ γ且未達〇· i #心的範 圍内具有極大值。此般圖案,可藉由以使點_平均距^ 位於較1〇以m還大且未達“^^之範圍内之方式製得。 322870 26 201137409 =外’亦可使用從隨機地配置此般多數個點所製作之 、玄&lt; Γ v ^吏其通過用以去除特定空間頻率以下的低空間頻 之高通紐⑼得之圖案H亦可使用從隨機 2配置此般多數個點所製作之,使其通過用以去除 特疋空間頻率以下的低空間頻率成分與特定空間頻率以上 的南空間頻率成分之帶通遽波器而得之圖案。 如第11圖所示’隨機地配置多數個點所製作之圖案的 能譜’係表示出與所配置之點的陳與點間的平均距離相 册之,大i冑由使此般圖案通過前述高通紐器或前述 皮器,可去除不必要的成分。如此通過高通滤波器 或帶通濾'波器之圖案的能譜,由於藉由錢器來去除成 分,所以在空間頻率大於“心且為0场^以下的範圍 内不具有極大值。此外,能夠更有效率地製作出在空間頻 率大於G.OWnfi絲達(UW的範_具有極大值之圖 案。在此,當使用前述高通攄波器時,為了去除空間頻率 大於0/znf1且為G.G4/ZIU.1以下的範圍内之極大值,所去除 之低空間頻率成分的上限空間頻率,較佳為以 下。此外,當使用前述帶通據波器時,為了去除空間頻率 大於0/ζπΓ1且為請“1以下的範_之極大值,且在空 間頻率大於0·0—丨且未達u⑽-丨的範圍内具有極= 值’所去除之低空間頻率成分的上限”頻率,較佳為〇肩 //in以下,所去除之高空_率成分的下限空間頻率 佳為0. 08 a nf1以上。 當採用通過高通滤波器或帶通濾、波器等之手法來製作 322870 27 201137409 圖案時’通過濾波器前的圖案,可使用藉由以亂數或計算 機所生成之虛擬亂數來決定濃淡而具有隨機的明亮度分布 之圖案。 關於根據上述方式所得之圖案來製作出模具之方法的 詳細内容,將於之後詳述。 上述工序(B) ’為藉由壓花法,將具有細微凹凸表面之 防眩層形成於基材膜上之工序。壓花法可例示出使用光硬 化性樹脂之UV壓花法、以及使用熱可塑性樹脂之熱 法’當中就生產性之觀點來看,較佳為UV壓花法。ϋν壓 花法中,是將光硬化性樹脂層形成於基材膜的表面,並一 邊將該光硬化性樹脂層按壓於模具的凹凸面一邊進行硬 化’藉此將模具的凹凸面轉印至光硬化性樹脂層之方法。 更具體而言,將含有光硬化型樹脂之塗佈液塗佈於基材骐 上,在將塗佈後的光硬化型樹脂密著於模具的凹凸面之狀 態下,從基材膜側照射紫外線等的光使光硬化型樹脂硬 化,然後從該模具中,將形成有硬化後的光硬化型樹脂層 之基材膜剝離,藉此可製得將模具的凹凸形狀轉印至硬化 後的光硬化型樹脂層(防眩層)之防眩膜。 使用UV壓花法時之光硬化性樹脂,較佳為使用藉由紫 外線進行硬彳bn線硬化型麟,亦可將適當選擇的光 起始劑組合於紫外線硬化型樹脂,而㈣使用可藉由波 ,線還長之可見光進行硬化之樹脂。紫外線二樹 並無特別限定,可使用市售的適當品。紫外線硬 ί脂的較佳例子,為含有三丙烯酸三經曱基丙院酉旨、 322870 28 201137409 四丙烯酸季戊四醇酯等之多官能丙烯酸酯的i種或2種以 上’以及 Irgacure 907(Chiba Specialty Chemicals 公司 製)、Irgacure 184(Chiba Specialty Chemicals 公司製)、Afy^¥^ Formula (7) Fig. 9 is a view showing a portion of an image data which can be used to produce a pattern used for the antiglare film of the present invention, which is a two-dimensional discrete function g(x'y) of a tone. The table is not. The image data of the pattern shown in Fig. 9 is 2_2 coffee, and is made at 12800 dpi. Fig. 10 is a diagram showing the energy spectrum G (fx, fy) obtained by performing discrete Fourier transform on the one-dimensional function g(x, y) of the tone 1 shown in Fig. 9 in white and black gradations. Since the pattern shown in Fig. 9 is randomly arranged, the energy spectrum G2(fx, fy) is symmetrical about the origin as shown in Fig. 1 . Therefore, the spatial frequency of the maximum value of the apparent spectrum G(fx, fy) of the pattern can be obtained from the profile passing through the origin of the energy spectrum. The nth figure shows the shaving surface of fx=〇 in the energy spectrum G2(fx, fy) shown in Fig. 322870 25 201137409. As can be seen from the figure, the pattern shown in Fig. 9 has a maximum value in the spatial frequency 〇·〇45#mH, but does not have a maximum value when it is larger than O/im 1 and is less than 〇Q4wra-i. . When the energy spectrum G2(fx, fy) of the pattern for forming the anti-glare film has a maximum value in a spatial frequency range larger than 〇//πΓ1 and less than 〇.〇4vnT1, the obtained anti-glare film The fine uneven surface does not exhibit the above-described specific spatial frequency distribution, so that the elimination of the flare and the sufficient anti-glare property cannot be achieved at the same time. The energy spectrum G2(fx,fy) is larger than 〇# γ and is 〇. 〇4 # γ, and the following spatial frequency range does not have a pattern of maximum values, such as the pattern shown in Fig. 9, by A plurality of points are randomly and uniformly arranged to be produced. The spot diameters to be randomly arranged may be one or plural. Further, in a pattern in which a plurality of points are randomly arranged, the spectrum is displayed in a spatial frequency at a reciprocal of the average distance between the points, and the first maximum value is displayed (the spatial frequency is smaller than the minimum spatial frequency of 0" The maximum value ^ Therefore, in order to produce a spectrum whose energy spectrum is larger than W and is less than 0.04/zm-i, there is no: a pattern with a maximum value, so that the average distance between the points is less than 25am. It is sufficient to make a pattern. In addition, the ratio of the energy spectrum (1)2 of the elevation of the fine concave-convex surface in the spatial frequency 〇1 of the anti-glare film to the energy spectrum 仏2 of the elevation in the spatial frequency 〇〇4 is set to 〇.丄Hereinafter, the energy spectrum of the pattern is preferably such that the spatial frequency is greater than 〇. 〇4 μ γ and does not reach 〇· i #心 has a maximum value. Such a pattern can be obtained by making the point _ average distance ^ 1〇 is made in a way that m is still large and does not reach the range of “^^. 322870 26 201137409 = outside' can also be used from a random configuration of such a majority of points, Xuan &lt; Γ v ^吏Through the high-pass (9) to remove the low spatial frequency below the specific spatial frequency The pattern H can also be formed by using a plurality of points from the random 2 arrangement to pass the band-pass chopper for removing the low spatial frequency components below the special spatial frequency and the south spatial frequency components above the specific spatial frequency. And the pattern obtained. As shown in Fig. 11, the 'energy spectrum of the pattern created by randomly arranging a plurality of points' indicates the average distance between the points and the points of the arranged points, and the larger the album. Such a pattern can remove unnecessary components through the aforementioned high-passor or the aforementioned leather device. Thus, the energy spectrum of the pattern of the high-pass filter or the band pass filter is removed in the space by the money device, so in the space The frequency is greater than "heart and does not have a maximum value in the range of 0 field ^ or less. In addition, it is possible to more efficiently produce a pattern having a spatial frequency greater than G.OWnfi (UW's _maximum value. Here, When the aforementioned high-pass chopper is used, in order to remove the maximum value in the range of the spatial frequency greater than 0/znf1 and below G.G4/ZIU.1, the upper limit spatial frequency of the removed low spatial frequency component is preferably the following In addition, When the aforementioned bandpass damper is used, in order to remove the spatial frequency greater than 0/ζπΓ1 and the maximum value of the range of 1 or less, and the spatial frequency is greater than 0·0-丨 and not within the range of u(10)-丨The upper limit of the frequency of the low-frequency component removed by the pole value is preferably 〇 shoulder//in, and the lower-order spatial frequency of the removed high-altitude-rate component is preferably 0.08 a nf1 or more. High-pass filter or bandpass filter, waver, etc. to make 322870 27 201137409 pattern 'passing the pattern before the filter, you can use the random number generated by random numbers or computer to determine the shade and have random Pattern of Brightness Distribution The details of the method of producing a mold according to the pattern obtained as described above will be described in detail later. The above step (B)' is a step of forming an antiglare layer having a fine uneven surface on the base film by an embossing method. The embossing method is exemplified by a UV embossing method using a photo-curable resin and a thermal method using a thermoplastic resin. From the viewpoint of productivity, a UV embossing method is preferred. In the ϋν embossing method, a photocurable resin layer is formed on the surface of the base film, and the photocurable resin layer is pressed while being pressed against the uneven surface of the mold, thereby transferring the uneven surface of the mold to A method of photocurable resin layer. More specifically, the coating liquid containing the photocurable resin is applied onto the substrate crucible, and the coated photocurable resin is adhered to the uneven surface of the mold, and is irradiated from the substrate film side. The light-curable resin is cured by light such as ultraviolet rays, and then the base film on which the cured photo-curable resin layer is formed is peeled off from the mold, whereby the uneven shape of the mold can be obtained and transferred to the cured state. An anti-glare film of a photo-curable resin layer (anti-glare layer). It is preferable to use a photocurable resin in the case of using the UV embossing method, and it is preferable to use a hard 彳b line hardening type lining by ultraviolet rays, or to combine an appropriately selected photoinitiator into an ultraviolet curable resin, and (4) A resin that is hardened by visible light of a wave or a line. The ultraviolet ray tree is not particularly limited, and a commercially available suitable product can be used. A preferred example of the ultraviolet ray grease is i or more than one or more of the polyfunctional acrylates including tris-acrylic acid triacetate, 322870 28 201137409 pentaerythritol tetraacrylate, and Irgacure 907 (Chiba Specialty Chemicals) Company), Irgacure 184 (manufactured by Chiba Specialty Chemicals),

Lucirin TP0(BASF公司製)等之光聚合起始劑之樹脂組成 物。可因應必要將微粒和溶劑等添加於此等紫外線硬化型 樹脂中,來調製出上述塗佈液。 &lt;防眩膜製造用之模具的製造方法&gt; 以下係說明本發明之防眩膜的製造中所用之模具的製 造方法。關於本發明之防眩膜的製造中所用之模具的製造 方法’只要是可獲得依據上述圖案所得之特定的表面形狀 之方法,則無特別限制,但為了精度佳且重現性佳地製造 出細微凹凸表面’較佳係基本上含有[1]第j鍍覆工序、[2] 研磨工序、[3]感光性樹脂膜形成工序、曝光工序、 顯影工序、[6]第1蝕刻工序、[7]感光性樹脂膜剝離工序、 以及[8]第2鐘覆卫序。第12圖係示意性顯示模具的製造 方法之前半部分的較佳-例之圖。第13圖係示意性顯示模 具的製造方法之後半部分的較佳一例之圖。第12圖及第 13圖中,係示意性顯不各工序中之模具的剖面。以下參照 第12圖及第13圖,詳細地說明上述各工序。 [1]第1鍍覆工序 本工序中,係對模具中所用之基材的表面施以鍵銅或 鍍鎳。如此,藉由對模具用基材的表面施以鍍銅或鍍鎳, 可提升之後的第2鍍覆工序中之鍍鉻的密著性與光澤性。 此係由於鍍銅或鍍鎳的被覆性高且平滑化作用強,可埋填 322870 29 201137409 模具用基材的微小凹凸或坑洞(Cavity)等而能夠形成平坦 且具光澤的表面之故。藉由此㈣銅或錢錄的特性,即使 在後述的第2鍵覆工序中施以鍍鉻,亦可消除被視為起因 ;基材上所存在的微小凹凸或坑洞(㈤⑼之鍍鉻表面的 =化’且由於_或麟的被覆性高,而能夠減少細微龜 裂的產生。 第1錢覆工序中所用之鋼或錄,除了分別為純金屬之 亦可為以鋼為主體之合金或以錄為主體之合金因此, ^說明書中所謂「銅」,係含有鋼及銅合金之涵義,此外, 鎳」係含有鎳及鎳合金之涵義。鍍銅及鍍鎳可分別藉由 解鍍覆來進行或是無電解鍍覆來進行,—般係採 锻覆。 # 施以链銅或鍵錄時,當鍍層太薄時,無法完全排除底 曰表面的影響,所以該厚度較佳為5G//m以上。鑛層厚产 ^限並無臨限性,以成本等來看,-般較宜為5叫^ 右。 構成模具用基㈣形成之金屬材料,就成本的觀點來 可列舉出鋁、鐵等。此外,就處理便利性來看,尤佳 ’:輕量的!s。在此所謂的銘或鐵,除了分別為純金屬之外, 亦了刀別為以銘或鐵為主體之合金。 此外’模具用基材的形狀,只要是該領域中以往所採 用:適备的形狀者即可,除了平板狀之外,可為圓柱狀或 圓筒狀的輥。若使用輥狀的基材來製作模具,則具有能夠 以連續的輥狀來製造防眩膜之優點。 322870 30 201137409 [2]研磨工序 在接續的研磨工序中,係將已在上述第1鍍覆工序中 施以鍍銅或鍍鎳之基材表面進行研磨。較佳係經由此工序 將基材表面研磨至接近鏡面之狀態。此係由於成為基材之 金屬板或金屬輥’為了達到期望精度,較多情況係施以切 割或研磨等機械加工,因而在基材表面殘留加工痕跡,即 使在施以鍍銅或鍍鎳之狀態下,亦可能殘留此等加工痕 跡,或是在經鍍覆之狀態下,表面不見得會完全地平滑之 故。亦即’即使將後述工序施於此般殘留有較深的加工痕 跡之表面’加工痕跡等的凹凸亦可能較施以各工序後所形 成之凹凸還深,有殘留加工痕跡的影響之可能性,當使用 此般模具來製造防眩膜時,可能對光學特性產生無法預期 之影響。第12 ® (a)巾’係示意性顯示平板狀的模具用基 材7,在第1鍍覆工序中其表面被施以鍍銅或鍍鎳(該工序 中所形狀賴或㈣㈣縣_),紐_研磨工序 而具有經鏡面研磨之表面8的狀態。 關於將施以鍍鋼或鍍鎳之基材表面進行研磨之方法並 無特別限定,可使用機械研磨法、電解研磨法、化學研磨 法的任-種。機械研磨法可例示出超加工法、研光法 (lapping)、流體研磨法、拋光研磨(buffing)法等。此外, 可藉由使用切削X具進行鏡面切削,將模具用基材表面設 為鏡面。此時所使用之切削卫具的材質或形狀等並益特別 限制’可使用超硬刀、CBN W、陶竞刀、鑽石刀等,從加 工精度之觀點而言較宜使用鑽石刀。 322870 31 201137409 研磨後的表面粗糙度’依據JIS B 0601的規定之中心 線平均粗糙度Ra,較佳為〇. lym以下,尤佳為〇 〇5#m 以下。當研磨後的中心線平均粗糙度Ra大於〇, Jem時, 可月t在最終形成之模具表面的凹凸形狀上殘留研磨後之表 面粗糙度的影響。此外,中心線平均粗糙度Ra的下限並無 特別限制,可考慮加工時間及加工成本等適當決定。 [3]感光性樹脂膜形成工序 在接續的感光性樹脂膜形成工序中,係將在溶劑中溶 解有感光性樹脂之溶液,塗佈於藉由上述研磨工序施以鏡 面研磨之模具用基材7之經研磨的表面8,並進行加熱、 乾燥而形成感光性樹脂膜。第12圖⑻t,係示意性顯示 在模具用基材7之經研磨的表面8形成有感光性樹脂膜9 之狀態。 、 感光性樹脂可使用以往所知的感光㈣脂。㈣ 為具有感光部分可硬化之性質的負型感光性樹脂, 於分子中具有丙烯酸基或甲基丙烯酸 或預聚物、雙疊氮化物與二稀橡膠之混合物;= 竣酉旨系化合物等。此外,作為具有藉 歸肉桂 =僅:留未感光部分之性質的正型感光:樹;旨,= :樹脂线祕樹此外,於感光 ^ 要而調配增感劑、顯影促進劑、密 T因應义 質劑等各種添加劑。 劑、塗佈性改 -、用基材7之經研磨的 ^佳係稀釋於適當的溶 當將此等感光性樹脂塗佈於才莫 表面8時’為了形成良好的塗膜, 322870 32 201137409 劑來塗佈。可使用溶纖劑系溶劑、丙二醇系溶劑、酯系溶 劑、醇系溶劑、酮系溶劑、高極性溶劑等做為溶劑。 塗佈感光性樹脂溶液之方法,可使用凹凸塗佈、喷流 塗佈、浸泡塗佈、旋轉塗佈、輥塗佈、線棒塗佈、空氣刀 塗佈、刮刀塗佈、淋幕塗佈等之一般所知的方法。塗佈膜 的厚度,較佳係設為乾燥後1至6#m之範圍。 [4]曝光工序 在接續的曝光工序中,係將上述能譜在大於Oynf1且 為0· 04# nf1以下空間頻率範圍内不具有極大值之圖案,曝 光於上述感光性樹脂膜形成工序令所形成之感光性樹脂膜 9上。曝光工序中所用之光源,可配合感光性樹脂的感光 強度及/或感度等來適當地選擇’例如可使用高壓水銀燈 的g射線(波長·· 436nm)、高壓水銀燈的h射線(波長: 405nm)、高壓水銀燈的i射線(波長:365nm)、半導體雷射 (波長:830nm、532 nm、488 nm、405 nm 等)、YAG 雷射(波 長:1064nm)、KrF準分子雷射(波長:248nm)、ArF準分子 雷射(波長:193nm)、F2準分子雷射(波長:15711111)等。 為了精度佳地形成模具的表面凹凸形狀以及防眩層的 表面凹凸形狀,在曝光工序中,較佳係在精密地控制之狀 態下將上述圖案曝光於感光性樹脂膜上,具體而言,係在 電腦中製作圖案作為圖像資料,並依據該圖像資料,藉由 從經電腦控制的雷射頭所發出之雷射光,將圖案描緣於感 光性樹脂膜上。進行雷射描繪時’可使用印刷版製作用的 雷射描繪裝置。此般雷射描繪裝置’可列舉出Laser St ream 322870 33 201137409 FX(Think Laboratory 製)等。 第12圖(c)中,係示意性顯示圖案被曝光於感光性樹 月曰膜9之狀態。當以負型感光性樹脂來形成感光性樹脂膜 ,曝光的區域1 〇係藉由曝光使樹脂的交聯反應進行, 使相對於後述顯影液之溶解性降低。因此,顯影工序中未 场gg、區域1 1藉由顯影液所溶解,僅有經曝光的區域1 〇 性榭2材表面上而成為遮罩。另一方面,當以正型感光 」印來形成感光性樹脂膜時,經曝光的區域1〇,係藉由 ^光使樹脂的鍵結被切斷,使相對於後述顯影液之溶解性 ^加從因此,顯影工序中經曝光的區域1()藉由顯影液所溶 ’有未曝朗區域丨丨殘留於基材表面上 [5]顯影工序 在接續的顯影工序中,當使用負型感光性樹脂作為感 '生樹脂膜9時’未曝光的區域11藉由顯影液所溶解,僅 曝光的區域10殘存於模具用基材上’並在接續的第i 腊;SI::為遮單。另一方面’當使用正型感光性樹 液所==1旨膜9時’僅有經曝㈣區域lQ藉由顯影 ^解,未曝先的區域u殘存於模具用基材上 -的第1蝕刻工序中作用為遮罩。 在接 〜工序巾所用之顯景彡液,可使用以往所知 納列舉m鈉、氫氧化鉀、碳酸鈉、矽酸鈉、讀 己扩機鹼類;乙胺、正丙胺等之第-胺類;二 第三胺類正:::之第-胺類;三乙胺、甲基二乙胺等之 ―甲基乙醇胺、三乙醇胺等之醇胺類;氫氧化 322870 34 201137409 四甲基錄、氫氧化四乙其、&amp; 四級銨鹽丨吡咯、哌 畑氧氧化二甲基羥乙基銨等之 甲苯、甲笨等之有機緣劑$環狀胺等的驗性水溶液;及二 顯影工序中的顯影方 影、喷霧顯影、磁刷“、、特別限制,可使用浸潰_ 第12圖⑷中,係音波顯影等之方法。 為感光性樹脂膜g來進行*’’、員不使用負型感光性樹脂作 未曝光的區域11 錢理之狀態。第12圖(c)令, 10殘留於基材表面^ ·成^所溶解’僅有經曝光的區織 意性顯示使用正型感:性成:=。第。圖⑷t,係示 顯影處理之狀態。第12 f日為感光性樹脂膜9來進行 影液所溶解,财未❹/中,經曝光的區域10藉由顯 為遮罩12。未爆先的區域11殘留於基材表面上而成 [6 ]第1韻刻工序 在接續的第1蝕灸丨τ严&amp; 殘存於模具用基材表面之咸心於^述顯影工序後,係將 對無遮罩之處的模具用=膜用作為遮罩,主要 覆面上形成凹凸。第^圖(二在經研磨後之鑛 一主要對無遮罩:二:具 之狀態。料12下部的模 、基材7進雜刻 表面被蝕刻,伸隨著# 土 ,雖未從模具用基材 行侧。因此:= 的進行,亦從無遮⑽ 遮罩12下部的^^:與無遮罩之處心交界附近, 遮罩12與無遮罩之^ 下,係將在此般 处13的父界附近’遮罩12下部的模具 322870 35 201137409 用基材7亦被蝕刻之情形,稱為側蝕β 第1蝕刻工序之蝕刻處理,一般係使用氣化鐵(FeCl3) 液、氣化銅(CuCl2)液、鹼蝕刻液(Cu⑽ACL)等,藉由使 金屬表面進行腐蝕來進行’但亦可使用鹽酸或硫酸等之強 酸’或是藉由施加與電解鍍覆時為相反的電位來進行之反 電解姓刻。施以蝕刻處理時之形成於模具用基材之凹形 狀’係因底層金屬的種類、感光性樹脂膜的種類及蝕刻手 法等有所不同,無法一概而論’但當蝕刻量為10/zm以下 時,可從接觸於蝕刻液之金屬表面,大致等向地進行蝕刻。 在此所謂敍刻量’是指藉由蝕刻所去除之基材的厚度。 第1餘刻工序之钕刻量’較佳為1至# m,尤佳為2 至l〇em。當蝕刻量未達i 時,金屬表面幾乎無法形成 凹凸形狀而成為幾乎平坦之模具,所以無法顯示出 防眩 性。此外,當蝕刻量超過5〇以m時,形成於金屬表面之凹 凸形狀的高低差增大,使用所得之模具所製作之防眩膜的 圖像顯示裝置中’會有產生泛自之疑慮。為了製得具備含 有95%以上之傾斜角度為5。以下的面之細微凹凸表面的防 眩膜,第1蝕刻工序之蝕刻量尤佳為2至8#m。第i蝕刻 工序之蝕刻處理,可藉由1次的蝕刻處理來進行,或是將 触刻處理分為2次以上來進行。當將蝕刻處理分為2次以 上來進行時,2次以上之蝕刻處理的蝕刻量合計,較佳係 設為上述範圍内。 [7]感光性樹脂膜剝離工序 在接續的感光性樹脂膜剝離工序中,係將第1蝕刻工 36 322870 201137409 序中用作為遮罩所殘存之感光性樹脂膜完全地 除。感光性樹脂膜剝離工序中,係使用剝離液來溶 性樹脂膜。剝離液可使用與上述顯影液為: 變PH、溫度、濃度及浸潰時間等,#使用 ^ 時’可將曝光部的感光性樹脂膜完全地溶解, 感光性樹脂時,可將非曝光部的感光性樹脂臈完全地溶解 而去除。關於感光性樹脂_離工序中之 並 顯影等之方法。㈣顯影、磁刷顯影、超音波 工库第^圖⑹中’係示意性顯示藉由感光性樹脂膜剝離 入^將第1㈣工序中用作為遮罩U之感光性樹脂膜完 去除之狀態。藉由使用有由感光性樹脂膜所形 侧,可將第1表面凹凸形狀15形成於模 [8]第2鍍覆工序 藉由對所形成之凹凸面(第1表面凹凸形狀 中,俜/ 將表面的凹凸形狀予以鈍化。第13圖㈦ 理所鉻層16形成於藉由第1㈣轉_刻處 Ζ形成之第1表面凹凸形狀15,以形成有使凹凸較第! 凹凸形狀15更為鈍化之表面(鍍鉻表面17)之狀態。 高、tit係採用在平板或輕等的表面上具光澤、硬度 鉻並無^ +、且可賦予良好的脫模性之祕。此般鍵 鉻等:可/制’但較佳為使用所謂光澤鍍鉻或裝飾用鍍 w舰出良好的光澤之鍍鉻。—般是藉由電解 322870 37 201137409 來進行,其鍍覆浴可使用含有無水鉻酸(CrOO與少量硫酸 之水溶液。藉由調節電流密度與電解時間,可控制鍍鉻的 厚度。 第2鍍覆工序中,施以鍍鉻以外的鍍覆者並不佳。此 係由於在鍍鉻以外的鍍覆中,由於硬度或耐磨耗性低,使 模具之耐久性降低,可能在使用中使凹凸磨損或損傷模 具。藉由此般模具所製得之防眩膜中,很可能難以獲得充 分的防眩功能,此外,防眩膜上產生缺陷的可能性亦高。 此外,鍍覆後的表面研磨亦不佳。亦即,較佳係在第 2鍍覆工序後不設置將表面進行研磨之工序,並將施以鍍 鉻後的凹凸面直接用作為轉印至基材膜上的樹脂層的表面 之模具的凹凸面。此係由於進行研磨會在最表面產生平坦 部分,而有導致光學特性惡化之可能性,此外,會導致形 狀的控制因素增加,而難以進行重現性佳之形狀控制等理 由。 如此,藉由對形成有細微表面凹凸形狀之表面施以鍵 鉻,可將凹凸形狀予以鈍化,並獲得其表面硬度被提高之 模具。此時之凹凸的鈍化程度,因底層金屬的種類、藉由 第1蝕刻工序所得之凹凸的尺寸及深度、以及鍍覆的種類 及厚度等而不同,無法一概而論,但控制鈍化程度之最大 因素仍是鍍覆厚度。當鍍鉻厚度較薄時,將鍍鉻加工前所 得之凹凸的表面形狀予以鈍化之效果不足,轉印該凹凸形 狀所製得之防眩膜的光學特性並不佳。另一方面,當鍍鉻 厚度太厚時,除了生產性惡化外,更會產生稱為突粒之突 38 322870 201137409 1狀:圍覆:陷’故不佳。因此,厚度較佳為1至10 /zm之fe圍内,尤佳為3至6//m之範圍内。 堆氏工序中所形成之鍍鉻層,較佳係形成為 維氏硬度成為_以上,尤佳形成為咖以上。并 當鍍鉻層的維氏硬度未達_時,除了模具使用時的= 性降低之外,祕層的硬度降低 梦薄 成'電解條件等產生異常之可能性高,==組 況產生較不佳的影響之可能性提高之故。、狀 此外’用以製作本發明的防眩膜之模具的製 覆述m感光性樹脂膜_卫序與⑻第2鍍 之凹3有藉由餘刻處理將由第1钱刻工序所形成 二純化之第2餘刻工序12餘刻工序中,係 藉由㈣處理’將由使用感光性樹脂膜作為遮罩 絲 2刻=形成之第1表面凹凸形狀15予以鈍化。藉由此第 2姓刻處理,可消除由第i餘刻工序所形成之第】表面凹 ^形狀15之表面傾斜較陡的部分’使採用所得之模具所製 造出=防眩膜的鮮特性往較佳的方向變化。帛14圖中, 係7^思性顯示藉由第2触刻處理將模具用基材7的第1表 面凹凸形狀15予以鈍化,使表面傾斜較陡的部分被鈍化, 而形成有具有和緩的表面傾斜之第2表面凹凸形狀18之狀 態。 第2蝕刻工序之蝕刻處理,與第1蝕刻工序相同,一 般係使用氣化鐵(FeCh)液、氯化銅(CuCl2)液、鹼蝕刻液 (Xu(NU3)4C12)等,藉由將金屬表面進行腐姓來進行,但亦 39 322870 201137409 可使用鹽酸或硫酸等之強酸,或是藉由施加與電解鍍覆時 為相反的電位來進行之反電解蝕刻。施以蝕刻處理後之凹 凸的鈍化程度,因底層金屬的種類、蝕刻手法、以及藉由 第1蝕刻工序所得之凹凸的尺寸及深度等而不同,無法一 概而論,但控制鈍化程度之最大因素為蝕刻量。在此所謂 蝕刻量,與第1蝕刻工序相同,是指藉由蝕刻所去除之基 材的厚度。當蝕刻量較小時,將藉由第1蝕刻工序所得之 凹凸的表面形狀予以鈍化之效果不足,轉印該凹凸形狀所 製得之防眩膜的光學特性並不佳。另一方面,當蝕刻量太 大時,凹凸形狀幾乎消失而成為幾乎平坦之模具,所以無 法顯示出防眩性。因此,触刻量較佳為1至5 0 // m之範圍 内,此外,為了製得具備含有95%以上之傾斜角度為5°以 下的面之細微凹凸表面的防眩膜,尤佳為4至20/zm之範 圍内。關於第2蝕刻工序之蝕刻處理,與第1蝕刻工序相 同,可藉由1次的蝕刻處理來進行,或是將蝕刻處理分為 2次以上來進行。在此,當將蝕刻處理分為2次以上來進 行時,2次以上之蝕刻處理的蝕刻量合計,較佳係設為上 述範圍内。 &lt;防眩性偏光板&gt; 本發明之防眩膜,由於能夠顯示較佳的防眩性並顯現 良好的對比,並有效地防止因「泛白」及「閃斑」的產生 所導致之觀看性的降低,所以在裝著於圖像顯示裝置時, 觀看性佳。當圖像顯示裝置為液晶顯示器時,可將此防眩 膜運用在偏光板。亦即,偏光板一般較多是在由吸附配向 40 322870 201137409 之聚乙烯醇系樹脂所構成之偏光膜的至 〆早面上貼合有保護膜之形態,但可 來構成該-方的保護膜。 偏 ==防眩膜,可構成防眩 a他光1之/為未積層之㈣,或是積層有保護膜或 先予膜之狀態’或是積層有用以貼合於液曰單元之黏 此外’於偏光膜的至少單面上 先板的該保護膜上’可在其基材膜侧貼合本發明之防眩膜 而構成防眩性偏光板。再者,偏光臈的至少單面上貼合有 保護膜之偏光板中,亦可將上述基材膜作為該顯膜二人 於偏光膜後,將防眩層形成於此基材膜上而藉此構成防: 性偏光板。 例 以下係列舉出實施例來更詳細地說明本發明,伸本發 明並不限定於此等實施例。下列例子之防眩膜及防眩祺 造用圖案之評估方法,係如以下所述。 、 [1]防眩膜之表面形狀的測定 使用二維顯微鏡PL// 2300(Sensofar公司製)來、、 防眩膜的表面形狀。為了防止樣本的麵曲,係使用光j疋 透明之黏著劑,以使凹凸面成為表面之方式貼合於予呈 板後,再用於測定。測定時,將物鏡的倍率設為1()俾基 =則定。水平分解能Λχ及= 850 ^rax850 ^m ° 買马 (標高的能譜之比Hi2/H22與H32/H22) 201137409 從以上所測得之資料中,求取防 ΛΑ J.® -S' 、之細微凹凸表面 作為二維函數h(x,y),將所得之二維函數 進仃離散傅利葉轉換而求得二維 , ^ f( X,W進行平方運算以計算出能譜的二維函數H2 (X,W ’並從fx=0的剖面曲線之h2(〇 率0.0W中的能譜η,與空間頻率&quot;二間頻 H&quot;並计算出能譜之HlVH22。此外’求取空間頻率〇1 中的能譜m2,並計算出能譜之比h32/H22。 (細微凹凸表面的傾斜角度) •根據以上所測得H並根據前述演算法進行計算, 製作出凹凸面的傾斜角度之直方®,從該时求取每個傾 斜角度之分布,並計算出傾斜角度為5。以下之面的比例。 [2 ]防眩膜之光學特性的測定 (霧度) 防眩膜的霧度係藉由JISK 7136所規定之方法來進行測 定。具體而言,係使用依據此規格之霧度計HM_15〇型(村 上色彩技術研究所製)來測定霧度。為了防止防眩膜的翹 曲’係使用光學呈透明之黏著劑,以使凹凸面成為表面之 方式貼合於玻璃基板後,再供於測定。一般而言,當霧度 增大時,運用在圖像顯示裝置時之圖像會變暗,結果容易 使正面對比降低。因此,霧度較低者為佳。 [3]防眩膜的機械強度(鉛筆硬度)及透濕度的測定 (鉛筆硬度) 防眩膜的鉛筆硬度係藉由JIS K 5600-5-4所規定之方 42 322870 201137409 法來進行測定。具體而言,係使用依據此規格之電動鉛筆 刮搔硬度試驗機(安田精機製作所公司製)並以荷重500g 進行測定。 (透濕度) 防眩膜的透濕度係藉由JIS Z0208所規定之方法,在 溫度40°C、相對濕度90%的條件下進行測定。 [4]防眩膜之防眩性能的評估 (映射、泛白的目視評估) 為了防止來自防眩膜内面之反射,係以使凹凸面成為 表面之方式將防眩膜貼合於黑色丙烯酸樹脂板,在打開螢 光燈之明亮室内,從凹凸面側以目視來觀察,並以目視來 評估榮光燈之映射的有無、泛白的程度。映射、泛白及質 感,係分別以1至3的3階段,藉由下列基準來評估。 映射1 :未觀察到映射。 2:觀察到些許映射。 3:明顯地觀察到映射。 泛白1 :未觀察到泛白。 2:觀察到些許泛白。 3:明顯地觀察到泛白。 (閃斑的評估) 閃斑係以下列方法來評估。亦即,從市售的液晶電視 (LC-32GH3(Sharp公司製))中將表裏兩面的偏光板剝離。 然後將偏光板「Sumikalan SRDB31E」(住友化學公司製), 以各自的吸收軸與原先偏光板的吸收軸一致之方式,中介 43 322870 201137409 黏著劑貼合於背面側與顯示面側以取代原先的偏光板,然 後將下列各例所示之防眩膜,以使凹凸面成為表面之方 式,中介黏著劑進一步貼合於顯示面側偏光板上。在此狀 態下,從距離樣本約30cm之位置以目視進行觀察,藉此, 以7階段將閃斑進行官能性評估。等級1為完全未觀察到 閃斑之狀態,等級7相當於觀察到極嚴重的閃斑之狀態, 等級3為觀察到些許閃斑之狀態。 [4]防眩膜製造用圖案的評估 以二維的離散函數g(x,y)來表示所製作之圖案資料的 階調。離散函數g(x,y)的水平分解能Δχ及Δγ均為2#πι。 將所得之二維函數g(x,y)進行離散傅利葉轉換而求得二維 函數G(fx, fy)。將二維函數G(fx,fy)進行平方運算以計算出 能譜的二維函數G2(fx,fy),並從fx = 0的剖面曲線之G2(0, fy) 中,評估在大於0/ζπΓ1且為0.04//πΓ1以下的空間頻率範圍 内是否具有極大值。 &lt;實施例1&gt; (防眩膜製造用之模具的製作) 首先製備在直徑200mm的銘親(依據JIS之Α5056)的 表面施以銅巴拉德鍍覆者。銅巴拉德鍍覆是由鍍銅層/薄鍍 銀層/表面鍍銅層所形成者,鍍層全體的厚度係設定為大約 200 # m。將該鍍銅表面進行鏡面研磨,將感光性樹月旨塗佈 於經研磨的鍍銅表面,並進行乾燥而形成感光性樹脂膜。 接著將連續地重複排列有複數個由第15圖所示之圖像資 料所構成之圖案的圖案,於感光性樹脂膜上藉由雷射光進 44 322870 201137409 行曝光與顯影。依據雷射光所進行之曝光鱼 ,、.峨%,係侫mA resin composition of a photopolymerization initiator such as Lucirin TP0 (manufactured by BASF Corporation). The coating liquid can be prepared by adding fine particles, a solvent, or the like to the ultraviolet curable resin as necessary. &lt;Manufacturing method of mold for producing anti-glare film&gt; Hereinafter, a method for producing a mold used in the production of the anti-glare film of the present invention will be described. The method for producing a mold used in the production of the anti-glare film of the present invention is not particularly limited as long as it can obtain a specific surface shape obtained according to the above-described pattern, but is manufactured with high precision and reproducibility. The fine uneven surface 'preferably basically contains [1] the jth plating step, the [2] polishing step, the [3] photosensitive resin film forming step, the exposure step, the developing step, and [6] the first etching step, [ 7] The photosensitive resin film peeling process, and [8] the second clock cover order. Fig. 12 is a view schematically showing a preferred example of the first half of the manufacturing method of the mold. Fig. 13 is a view schematically showing a preferred example of the latter half of the method of manufacturing the mold. In Figs. 12 and 13, the cross section of the mold in each step is schematically shown. Hereinafter, each of the above steps will be described in detail with reference to Figs. 12 and 13. [1] First plating step In this step, the surface of the substrate used in the mold is subjected to key copper or nickel plating. As described above, by applying copper plating or nickel plating to the surface of the substrate for a mold, the adhesion and gloss of chrome plating in the subsequent second plating step can be improved. This is because copper plating or nickel plating has high coating properties and high smoothing effect, and it is possible to form a flat and shiny surface by embedding 323870 29 201137409 fine irregularities or voids of the substrate for a mold. By the characteristics of (4) copper or money recording, even if chrome plating is applied in the second bonding step described later, the cause of the rust plating or the pits ((5) (9) of the chrome-plated surface can be eliminated. ==' and because of the high coverage of _ or lin, it can reduce the occurrence of fine cracks. The steel or record used in the first money-receiving process, in addition to pure metal, may be steel-based alloy or Therefore, the term "copper" in the specification refers to the meaning of steel and copper alloy. In addition, nickel" contains the meaning of nickel and nickel alloy. Copper plating and nickel plating can be respectively performed by deplating. For the purpose of carrying out or electroless plating, it is generally forged. # When applying copper or key recording, when the plating is too thin, the influence of the surface of the bottom is not completely eliminated, so the thickness is preferably 5G//. More than m. The thickness of the ore layer is not limited. In terms of cost, etc., it is generally preferred to be 5: ^. The metal material formed by the base (4) of the mold is used to list aluminum from the viewpoint of cost. , iron, etc. In addition, in terms of handling convenience, especially good ': lightweight! s. In this case, the so-called Ming or iron, in addition to pure metal, also the alloy is the alloy with Ming or iron as the main body. In addition, the shape of the substrate for the mold is as long as used in the field: A suitable shape may be a cylindrical or cylindrical roll in addition to a flat plate shape. When a roll-shaped base material is used to form a mold, the anti-glare film can be produced in a continuous roll shape. Advantages: 322870 30 201137409 [2] Polishing step In the subsequent polishing step, the surface of the substrate which has been subjected to copper plating or nickel plating in the first plating step is polished. The surface of the material is ground to a state close to the mirror surface. This is because the metal plate or the metal roll that serves as the base material is often subjected to machining such as cutting or grinding in order to achieve the desired precision, so that processing marks remain on the surface of the substrate, even if In the case where copper plating or nickel plating is applied, such processing marks may remain, or in the plated state, the surface may not be completely smoothed. That is, even if the process described later is applied thereto Residual The surface of the deep processing mark may be deeper than the unevenness formed by the process, and may have the influence of residual processing marks. When using such a mold to manufacture an anti-glare film, it may be The optical properties are unpredictable. The 12th (a) towel is a schematic display of a flat substrate 7 for a mold, and the surface is subjected to copper plating or nickel plating in the first plating process (this process) The shape of the medium is in the form of (4) (four) prefecture _), and the surface of the substrate 8 having the mirror-polished surface is not particularly limited. The method of polishing the surface of the substrate to which the plated steel or the nickel is applied is not particularly limited. Any of the polishing method, the electrolytic polishing method, and the chemical polishing method. The mechanical polishing method may, for example, be a super processing method, a lapping method, a fluid polishing method, a buffing method, or the like. The X-cutting tool is mirror-cut, and the surface of the substrate for the mold is mirror-finished. The material or shape of the cutting aid used at this time is particularly limited. 'Superhard knives, CBN W, Tao Jing knives, diamond knives, etc. can be used, and diamond knives are preferred from the viewpoint of processing accuracy. 322870 31 201137409 Surface roughness after grinding' The center line average roughness Ra according to JIS B 0601 is preferably 〇. lym or less, and particularly preferably 〇 〇5#m or less. When the average center roughness Ra of the center line after grinding is larger than 〇, Jem, the influence of the surface roughness after polishing may remain on the uneven shape of the surface of the finally formed mold. Further, the lower limit of the center line average roughness Ra is not particularly limited, and may be appropriately determined in consideration of processing time and processing cost. [3] Photosensitive resin film forming step In the subsequent photosensitive resin film forming step, a solution in which a photosensitive resin is dissolved in a solvent is applied to a substrate for a mold which is mirror-polished by the polishing step. The polished surface 8 of 7 is heated and dried to form a photosensitive resin film. Fig. 12 (8) t is a view schematically showing a state in which the photosensitive resin film 9 is formed on the polished surface 8 of the substrate 7 for a mold. As the photosensitive resin, a conventionally known photosensitive (tetra) grease can be used. (4) A negative photosensitive resin having a photohardenable property of a photosensitive portion, which has an acrylic group or a methacrylic acid or a prepolymer, a mixture of a double azide and a dilute rubber in the molecule; In addition, as a positive type photosensitive having the property of borrowing cinnamon = only: leaving the photosensitive portion: tree; purpose, =: resin line secret tree, in addition, sensitizing agent, development accelerator, dense T in response to photosensitive Various additives such as a clarifying agent. The coating agent is modified, and the ground material of the substrate 7 is diluted in a suitable solution. When the photosensitive resin is applied to the surface 8, the film is formed 322870 32 201137409 The agent is applied. A cellosolve solvent, a propylene glycol solvent, an ester solvent, an alcohol solvent, a ketone solvent, a highly polar solvent or the like can be used as the solvent. The method of applying the photosensitive resin solution may be a bump coating, a jet coating, a dip coating, a spin coating, a roll coating, a wire bar coating, an air knife coating, a knife coating, or a curtain coating. A method generally known. The thickness of the coating film is preferably in the range of 1 to 6 #m after drying. [4] Exposure step In the subsequent exposure step, the above-described spectrum of the photosensitive resin film formation process is exposed to a pattern having a maximum value in the spatial frequency range of more than Oynf1 and less than 0·04#nf1. The photosensitive resin film 9 is formed. The light source used in the exposure step can be appropriately selected in accordance with the photosensitivity and/or sensitivity of the photosensitive resin. For example, g-rays (wavelength··436 nm) of a high-pressure mercury lamp and h-rays of a high-pressure mercury lamp (wavelength: 405 nm) can be appropriately selected. , i-ray (wavelength: 365nm) of high-pressure mercury lamp, semiconductor laser (wavelength: 830nm, 532 nm, 488 nm, 405 nm, etc.), YAG laser (wavelength: 1064 nm), KrF excimer laser (wavelength: 248 nm) , ArF excimer laser (wavelength: 193 nm), F2 excimer laser (wavelength: 15711111) and the like. In order to accurately form the surface uneven shape of the mold and the surface uneven shape of the antiglare layer, it is preferable to expose the pattern to the photosensitive resin film in a state of being precisely controlled in the exposure step, specifically, A pattern is created in the computer as image data, and based on the image data, the pattern is drawn onto the photosensitive resin film by laser light emitted from a computer-controlled laser head. When performing laser drawing, a laser drawing device for printing plate production can be used. Such a laser drawing device is exemplified by Laser St ream 322870 33 201137409 FX (manufactured by Think Laboratory). In Fig. 12(c), the state in which the pattern is exposed to the photosensitive dendrite film 9 is schematically shown. When the photosensitive resin film is formed of a negative photosensitive resin, the exposed region 1 is subjected to a crosslinking reaction of the resin by exposure, so that the solubility with respect to the developer described later is lowered. Therefore, in the developing process, the field gg and the region 1 1 are dissolved by the developer, and only the exposed region 1 is formed on the surface of the material to form a mask. On the other hand, when the photosensitive resin film is formed by positive photosensitive printing, the exposed region is cut by the light, and the solubility of the developer is described later. Therefore, the exposed region 1 () is exposed by the developer in the developing process, and the unexposed region remains on the surface of the substrate. [5] The development process is performed in the subsequent development process, when the negative type is used. When the photosensitive resin is used as the raw resin film 9, the unexposed region 11 is dissolved by the developer, and only the exposed region 10 remains on the substrate for the mold' and is in the succeeding i-th wax; SI:: single. On the other hand, 'When positive-type photosensitive sap is used = 1 to film 9', only the exposed (four) region lQ is developed, and the unexposed region u remains on the substrate for the mold - the first It acts as a mask in the etching process. In the case of the sputum sputum used in the process towel, it is possible to use the conventionally known m sodium, potassium hydroxide, sodium carbonate, sodium citrate, and sodium hexamine; the amines such as ethylamine and n-propylamine. Class II; second amines:::--amines; triethylamine, methyldiethylamine, etc. - methylethanolamine, triethanolamine and other alcohol amines; oxidant 322870 34 201137409 tetramethyl record An aqueous solution of tetramethylammonium hydroxide, &amp; quaternary ammonium salt pyrrole, piperazine oxyoxylated dimethyl hydroxyethyl ammonium, toluene, methyl ester, etc. In the development process, the development method, the spray development, and the magnetic brush are particularly limited, and a method such as sound wave development in the immersion _ 12 (4) can be used. The photosensitive resin film g is subjected to *'', The member does not use the negative photosensitive resin as the unexposed area. In the 12th figure (c), 10 remains on the surface of the substrate. ^·Dissolved in the 'only exposed area'. The positive feeling is used: sex: =. Fig. 4 (t) t shows the state of the development treatment. On the 12th fth day, the photosensitive resin film 9 is used for the liquid solution. Dissolved, in the future, the exposed area 10 is marked by the mask 12. The unexploded area 11 remains on the surface of the substrate [6] The first rhyme process is followed by the first moxibustion丨τ strict &amp; After the development of the surface of the substrate for the mold, the mold is used as a mask for the mold without the mask, and the main surface is formed with irregularities. Second, after the grinding, the main one is unmasked: two: the state of the material. The lower part of the material 12, the substrate 7 into the surface of the engraved surface is etched, extending along with #土, although not from the mold substrate line Side: Therefore: the progress of = is also from the unobstructed (10) mask 12 in the lower part of the ^^: near the border with the unshielded heart, the mask 12 and the unshielded ^, will be in this place 13 Near the parent boundary, the mold 322870 35 201137409 in the lower part of the mask 12 is also etched by the substrate 7. This is called the side etching. The etching process of the first etching process generally uses gasified iron (FeCl3) liquid and vaporized copper. (CuCl2) liquid, alkali etching solution (Cu(10) ACL), etc., by performing corrosion on the metal surface, 'but a strong acid such as hydrochloric acid or sulfuric acid may be used' or The reverse electrolysis is performed by applying a potential opposite to that at the time of electrolytic plating. The concave shape formed on the substrate for a mold during the etching treatment is based on the type of the underlying metal, the type of the photosensitive resin film, and etching. The technique is different, and it cannot be generalized. However, when the etching amount is 10/zm or less, the etching can be performed substantially in the same direction from the metal surface contacting the etching liquid. The so-called "sampling amount" means by etching. The thickness of the substrate to be removed. The engraving amount 'in the first remaining step' is preferably from 1 to #m, particularly preferably from 2 to 10 μm. When the etching amount is less than i, the metal surface is hardly formed into a concave-convex shape. It becomes an almost flat mold, so it cannot show anti-glare properties. Further, when the etching amount exceeds 5 Torr, the height difference of the concave-convex shape formed on the metal surface is increased, and there is a fear that the image display apparatus using the anti-glare film produced by the obtained mold has a ubiquity. In order to obtain an angle of inclination of 5 with more than 95%. The anti-glare film on the surface of the fine uneven surface of the following surface is preferably 2 to 8 #m in the etching amount in the first etching step. The etching treatment in the i-th etching step can be performed by one etching process or by dividing the etching process into two or more times. When the etching treatment is carried out in two or more steps, the total etching amount of the etching treatment of two or more times is preferably within the above range. [7] Photosensitive resin film peeling step In the subsequent photosensitive resin film peeling step, the photosensitive resin film remaining as a mask in the first etching work 36 322870 201137409 is completely removed. In the photosensitive resin film peeling step, a peeling liquid is used to dissolve the resin film. The peeling liquid can be used in the above-mentioned developing solution: changing pH, temperature, concentration, and immersion time, etc., when the film is used, the photosensitive resin film in the exposed portion can be completely dissolved, and in the case of the photosensitive resin, the non-exposed portion can be used. The photosensitive resin 臈 is completely dissolved and removed. The method of developing the photosensitive resin _ away from the process, etc. (4) Development, magnetic brush development, and ultrasonication. In the figure (6), the photosensitive resin film is peeled off by the photosensitive resin film, and the photosensitive resin film used as the mask U in the first step (4) is removed. By using the side formed by the photosensitive resin film, the first surface uneven shape 15 can be formed in the mold [8]. The second plating step is formed by the uneven surface formed (the first surface uneven shape, 俜/ The uneven shape of the surface is passivated. Fig. 13 (7) The chrome layer 16 is formed on the first surface uneven shape 15 formed by the first (fourth) turn, so that the unevenness is formed more than the first! The state of the passivated surface (chrome-plated surface 17). The high-tit is made of a glossy surface on a flat plate or a light surface, and the hardness of the chromium is not + +, and can give a good release property. : can be / made 'but preferably using so-called glossy chrome or decorative chrome plating with good gloss. It is usually carried out by electrolysis 322870 37 201137409, the plating bath can be used with anhydrous chromic acid (CrOO With a small amount of aqueous solution of sulfuric acid, the thickness of chrome plating can be controlled by adjusting the current density and the electrolysis time. In the second plating step, plating other than chrome plating is not preferable. This is due to plating in chrome plating. Due to the low hardness or wear resistance, the mold is made The durability is lowered, and the unevenness may be worn or damaged during use. In the anti-glare film produced by the mold, it is likely that it is difficult to obtain sufficient anti-glare function, and in addition, the possibility of defects on the anti-glare film is generated. Further, the surface polishing after plating is also poor. That is, it is preferable that the surface is not polished after the second plating step, and the uneven surface after the chrome plating is directly used as the transfer. The uneven surface of the mold printed on the surface of the resin layer on the substrate film. This causes a flat portion to be formed on the outermost surface due to polishing, which may cause deterioration of optical characteristics, and may cause an increase in shape control factors. Therefore, it is difficult to perform shape control such as reproducibility. Thus, by applying a key chrome to the surface on which the fine surface unevenness is formed, the uneven shape can be passivated, and a mold whose surface hardness is improved can be obtained. The degree of passivation differs depending on the type of the underlying metal, the size and depth of the unevenness obtained by the first etching step, and the type and thickness of the plating. However, the biggest factor in controlling the degree of passivation is still the plating thickness. When the chrome plating thickness is thin, the effect of passivating the surface shape of the unevenness obtained before chrome plating is insufficient, and the anti-glare obtained by transferring the concave-convex shape is obtained. On the other hand, when the thickness of the chrome plating is too thick, in addition to the deterioration of productivity, a protrusion called a bulge is produced. 38 322870 201137409 1 shape: Surrounding: It is not good. The thickness is preferably in the range of 1 to 10 /zm, particularly preferably in the range of 3 to 6 / / m. The chrome plating layer formed in the stacking process is preferably formed to have a Vickers hardness of _ or more. In addition, when the Vickers hardness of the chrome plating layer is less than _, the hardness of the secret layer is lowered, and the hardness of the secret layer is lowered, and the possibility of abnormality such as electrolysis conditions is high. == The possibility that the group situation has a less favorable impact is increased. In addition, in the case of the mold for producing the anti-glare film of the present invention, the m-thickness resin film _Wei order and (8) the second plated recess 3 are formed by the first etching process by the residual processing. In the second remaining step of the second step of the purification step, the first surface uneven shape 15 formed by using the photosensitive resin film as the masking wire 2 is passivated by the (four) process. By the second surname processing, it is possible to eliminate the portion of the surface of the first surface concave shape 15 formed by the i-th remaining process, which is steeply inclined, so that the obtained mold can be used to produce the fresh characteristic of the anti-glare film. Change in the preferred direction. In the drawing of Fig. 14, it is shown that the first surface uneven shape 15 of the substrate 7 for a mold is passivated by the second etch processing, and the portion having a steep surface is passivated, and is formed to be gentle. The state of the second surface uneven shape 18 in which the surface is inclined. The etching process in the second etching step is generally the same as in the first etching step, in which a metal oxide iron (FeCh) solution, a copper chloride (CuCl 2 ) solution, an alkali etching solution (Xu (NU 3 ) 4 C 12 ), or the like is used. The surface is subjected to a rot, but it is also possible to use a strong acid such as hydrochloric acid or sulfuric acid, or a reverse electrolytic etching by applying a potential opposite to that at the time of electrolytic plating, in 39 322870 201137409. The degree of passivation of the unevenness after the etching treatment differs depending on the type of the underlying metal, the etching method, and the size and depth of the unevenness obtained by the first etching step, and cannot be generalized, but the maximum factor for controlling the degree of passivation is etching. the amount. Here, the etching amount is the same as the first etching step, and refers to the thickness of the substrate removed by etching. When the etching amount is small, the effect of passivating the surface shape of the unevenness obtained by the first etching step is insufficient, and the optical characteristics of the anti-glare film obtained by transferring the uneven shape are not good. On the other hand, when the etching amount is too large, the uneven shape almost disappears and becomes a nearly flat mold, so that the anti-glare property cannot be exhibited. Therefore, the amount of the etch is preferably in the range of 1 to 50 // m, and further, in order to obtain an anti-glare film having a fine uneven surface containing 95% or more of the surface having an inclination angle of 5 or less, it is particularly preferable. Within the range of 4 to 20/zm. The etching treatment in the second etching step can be performed by one etching treatment or the etching treatment can be divided into two or more steps as in the first etching step. Here, when the etching treatment is carried out in two or more steps, the total etching amount of the etching treatment of two or more times is preferably within the above range. &lt;Anti-glare polarizing plate&gt; The anti-glare film of the present invention can exhibit good anti-glare properties and exhibit good contrast, and is effectively prevented from being caused by "whitening" and "flash spots". Since the visibility is lowered, the viewing property is good when it is mounted on the image display device. When the image display device is a liquid crystal display, the anti-glare film can be applied to the polarizing plate. In other words, the polarizing plate is generally in the form of a protective film bonded to the early surface of the polarizing film composed of the polyvinyl alcohol-based resin of 40 322870 201137409, but it can constitute the protection of the square. membrane. Partial == anti-glare film, can constitute anti-glare a light 1 / is un-layered (four), or a layer of protective film or pre-film state 'or laminated to be useful for bonding to the liquid helium unit The anti-glare film of the present invention can be bonded to the base film side of the polarizing film on the protective film of at least one of the first sheets to constitute an anti-glare polarizing plate. Further, in the polarizing plate in which the protective film is bonded to at least one surface of the polarizing film, the base film may be formed as a polarizing film on the substrate, and the anti-glare layer may be formed on the substrate film. Thereby, it constitutes an anti-polarity plate. EXAMPLES The following examples are given to illustrate the invention in more detail, and the invention is not limited to the examples. The evaluation methods of the anti-glare film and the anti-glare pattern for the following examples are as follows. [1] Measurement of the surface shape of the anti-glare film The surface shape of the anti-glare film was measured using a two-dimensional microscope PL// 2300 (manufactured by Sensofar Co., Ltd.). In order to prevent the surface curvature of the sample, a transparent adhesive is used, and the surface of the concave-convex surface is attached to the pre-formed sheet, and then used for measurement. In the measurement, the magnification of the objective lens is set to 1 () 俾 base = then. Horizontal decomposition energy = 850 ^rax850 ^m ° Buy horses (the ratio of the energy spectrum of the elevations Hi2/H22 and H32/H22) 201137409 From the above measured data, find the defensive J.® -S', The fine concave and convex surface is used as a two-dimensional function h(x, y), and the obtained two-dimensional function is transformed into a discrete Fourier transform to obtain two-dimensional, ^ f (X, W is squared to calculate the two-dimensional function H2 of the energy spectrum) (X, W 'and h2 from the profile curve of fx = 0 (the energy spectrum η in the 0.0W rate, and the spatial frequency &quot; two-frequency H&quot; and calculate the energy spectrum of HlVH22. In addition, 'seeking spatial frequency The energy spectrum m2 in 〇1, and calculate the energy spectrum ratio h32/H22. (The inclination angle of the fine concave and convex surface) • According to the above measured H and calculated according to the above algorithm, the inclination angle of the concave and convex surface is made. Rectangular®, from which the distribution of each inclination angle is obtained, and the ratio of the inclination angle to 5. The ratio of the following surface is calculated. [2] Measurement of optical characteristics of anti-glare film (haze) Anti-glare film haze The measurement is carried out by the method specified in JIS K 7136. Specifically, a haze meter HM_15 according to this specification is used. (The Murakami Color Technology Research Institute) measures the haze. In order to prevent the warpage of the anti-glare film, an optically transparent adhesive is used, and the surface of the uneven surface is bonded to the glass substrate, and then applied to the measurement. In general, when the haze is increased, the image used in the image display device is darkened, and as a result, the front contrast is easily lowered. Therefore, the haze is lower. [3] Anti-glare film Measurement of mechanical strength (pencil hardness) and moisture permeability (pencil hardness) The pencil hardness of the anti-glare film is measured by the method of 42 322870 201137409 specified in JIS K 5600-5-4. Specifically, the basis for use is determined. The electric pencil scraping hardness tester (manufactured by Yasuda Seiki Co., Ltd.) of this specification was measured at a load of 500 g. (Hypothelium) The moisture permeability of the anti-glare film was measured at a temperature of 40 ° C by the method specified in JIS Z0208. The measurement was carried out under the condition of a relative humidity of 90%. [4] Evaluation of the anti-glare property of the anti-glare film (mapping, visual evaluation of whitening) In order to prevent reflection from the inner surface of the anti-glare film, the surface of the uneven surface is made to be a surface will The glare film was attached to a black acrylic plate, and it was visually observed from the side of the uneven surface in a bright room in which the fluorescent lamp was turned on, and the degree of whitening of the map of the glory lamp was visually evaluated. Mapping, whitening, and The texture was evaluated by the following criteria in 3 stages of 1 to 3. Mapping 1: No mapping was observed 2: Some mappings were observed 3: Mappings were clearly observed. Whitening 1: No pans were observed White. 2: A little whitening was observed. 3: Whitening was clearly observed. (Evaluation of the freckle) The freckle was evaluated by the following method. In other words, the polarizing plate on both sides of the front and back sides was peeled off from a commercially available liquid crystal television (LC-32GH3 (manufactured by Sharp Corporation)). Then, the polarizing plate "Sumikalan SRDB31E" (manufactured by Sumitomo Chemical Co., Ltd.) was placed in the same manner as the absorption axis of the original polarizing plate, and the adhesive was bonded to the back side and the display side to replace the original one. In the polarizing plate, the antiglare film shown in the following examples was applied so that the uneven surface became a surface, and the intermediate adhesive was further bonded to the display surface side polarizing plate. In this state, observation was visually observed from a position of about 30 cm from the sample, whereby the speckle was evaluated for functionality in 7 stages. Level 1 is the state in which no flash spots are observed at all, level 7 is equivalent to the state in which very severe flash spots are observed, and level 3 is the state in which some flash spots are observed. [4] Evaluation of pattern for manufacturing an anti-glare film The two-dimensional discrete function g(x, y) is used to express the tone of the created pattern data. The horizontal decomposition energies Δχ and Δγ of the discrete function g(x, y) are both 2#πι. The obtained two-dimensional function g(x, y) is subjected to discrete Fourier transform to obtain a two-dimensional function G(fx, fy). The two-dimensional function G(fx,fy) is squared to calculate the two-dimensional function G2(fx,fy) of the energy spectrum, and is evaluated from G2(0, fy) of the profile curve of fx=0. /ζπΓ1 and whether it has a maximum value in the spatial frequency range of 0.04//πΓ1 or less. &lt;Example 1&gt; (Production of mold for producing an anti-glare film) First, a copper ball-plated plate was applied to the surface of a crystal of 200 mm in diameter (according to JIS 5056). The copper ballard plating is formed by a copper plating layer/thin silver plating layer/surface copper plating layer, and the thickness of the entire plating layer is set to be about 200 #m. The copper-plated surface was mirror-polished, and a photosensitive resin was applied to the polished copper-plated surface and dried to form a photosensitive resin film. Then, a pattern in which a plurality of patterns composed of the image data shown in Fig. 15 are successively repeated is repeatedly exposed and developed on the photosensitive resin film by laser light into 44 322870 201137409. Exposure fish based on laser light, .峨%, system 侫m

Laser Stream FX(Think Laboratory 製)來埃^ ^ 樹脂膜係使用正型感光性樹脂。第15圖所示&gt; :感*光性 &lt;圖案,為料 於隨機地配置多數個點徑12# m的點之圖案, τ 運用用以+ β ffl'1 以 除空間頻率0· 04/ζπΓ1以下的低空間頻率成分與〇 j 戈 上的高空間頻率成分之帶通濾波器而製作出。 然後以氯化銅液進行第1餘刻處理(钱刻量.3 第1蝕刻處理後,從輥中去除感光性樹脂膜, ° 銅液進行第2蝕刻處理(蝕刻量:10 ym)。銬接,、,=氣化 、、叹u使鍍鉻原 度成為4# m之方式進行鍍鉻加工而製作出模具A。 (基材膜的製作) 將使30重量份的丙婦酸橡膠粒子含有於甲&amp; 曱酯/丙烯酸甲酯=96/4(重量比)的共聚物(折射率j 49)= 重董份之丙稀酸糸樹脂組成物’於第1擠壓機(螺产句 65mm、單軸、附有通氣孔(東芝機械公司製))進行炼融^ 混’並供給至分流器(feed block)。此外,將使3〇重量严 的丙烯酸橡膠粒子含有於甲基丙烯酸曱酯/丙烯酸甲醋= 96/4(重量比)的共聚物(折射率1.49)70重量份之丙烯酸 系樹脂組成物,於第2擠壓機(螺桿徑45mm、單轴、附有 通氣孔(日立造船公司製))進行熔融摻混,並供給至分流 器。以使從第1擠壓機供給至分流器之樹脂成為中間層, 從第2擠壓機供給至分流器之樹脂成為表層(雙面)之方 式’在265°C下進行共擠壓成形,並經由被設定在85°C之 親早元’製作出厚度為80/zm(中間層50&quot;m、表層15y mx 45 322870 201137409 2)之3層構造的基材膜A。 (防眩層的形成) 將光硬化性樹脂組成物「GRANDIC 806T」(大日本油墨 化學工業公司製)溶解於乙酸乙酯,形成50重量%濃度的溶 液,然後將屬於光聚合起始劑的Lucirin TP0(BASF公司 製、化學名稱:2, 4, 6-三甲基苯甲醯二笨基膦氧化物),以 硬化性樹脂成分每1〇〇重量份添加5重量份之方式調製出 塗佈液。在基材膜A上,以使乾燥後的塗佈厚度成為6/zm 之方式塗佈此塗佈液,在設定為6(TC之乾燥機中進行3分 鐘的乾燥。將乾燥後的基材膜A,以使光硬化性樹脂組成 物層成為模具側之方式,藉由橡膠輥按壓於先前所得之模 具A的凹凸面並使密著。在此狀態下,從基材膜A側,以 經h射線換昇的光量成為200mJ/cm2之方式,將來自強度 20mW/cm2之高壓水銀燈的光予以照射,使光硬化性樹脂組 成物層硬化。然後係每個硬化樹脂將基材膜A從模具中剝 離,而製作出由表面具有凹凸之硬化樹脂(防眩層)與基材 膜A之積層體所構成的透明防眩膜a。 &lt;實施例2&gt; 2模具製作的曝光工序中,將連續地重複排列有複數 個由第 16 f51 βρί* — 斤不之圖像-貝料所構成之圖案的圖案,於感光 =膜上藉由雷射光進行曝光,以使第1蝕刻處理的蝕 、為5以m之方式來設定,且使第2触刻處理的姓刻量 _ ,以m之方式來設定,除此之外,其他與實施例1相 同而製作出模具B。除了使用所得之模具B之外,其他與 322870 46 201137409 實施例1相同而製作出防眩膜B。第16 對於隨機地配置多數舰徑12心的點之圖案’為 去除空間财〇.〇35_、下的低空間頻率成;^用用以 W以上的高空間頻率成分之帶通濾波 ^、0.135 &lt;比較例1&gt; 教1下出。 基材膜A之外,其他與實施例代 〈比較例2&gt; 珥丨万眩膜0 首先將直徑__的料(依據JIS之A5Q56)的裊面 進行鏡面研磨,並使用喷砂裝置(不二製作所公司製),以 ,,壓力旦0· lMPa(計示壓)、珠粒用量(輕表面積每 cm之用1),將二氧化錯珠粒Tz_sx_17(T〇s〇h公司製, 平均粒徑.20/zm)噴砂至經研磨的銘面,於表面形成凹 凸。對所得之附有凹凸的鋁輥進行無電解鍍鎳加工,而製 作出模具〇此時,無電解鍍鎳厚度係設定為15#m。除了 使用所知之模具C之外,其他與實施例1相同而製作出防 眩膜D。 關於所得之防眩膜A至D的上述[1 ]至[4 ]的測定、評 估結果,係匯總如第1表所示。此外,第17圖係顯示出從 實施例1的模具A及實施例2的模具B的製作中所使用之 圖案所得之能譜G2(fx,fy)中的fx=〇時之剖面。從第17圖 中,可得知實施例1的模具A及實施例2的模具b的製作 中所使用之圖案的能譜,在大於ΟμπΓ1且為〇. 〇4/ζπΓΐ以下 的空間頻率範圍内不具有極大值。 47 322870 201137409 第1表 1 —-一 實施例1 實施例2 比較例1 比較例2 防眩膜 ____ A B C D 基材膜 __—' A (丙烯酸系 樹脂) A (丙缔酸系 樹脂) TAC膜 A (丙烯酸系 榭脂) 棋具 A B A C 表面形狀 能譜之比 H.VH^ 19 4 19 41 — ^ HaVH^ 0. 002 0. 001 0. 002 0. 003 傾斜角度 面的tt 5 ·以下之 ,例(¾) 100 100 100 100 光學特性 霧度(¾) 0.4 0. 6 0. 4 0. 4 防眩性能 映射 1 1 1 1 泛白 1 1 1 1 閃斑 1 1 1 6 鉛筆硬度 4H 4H 3H 4H 透濕度(g/m2 . 24hr) 52 48 287 50 從第1表所示的結果中,可得知滿足本發明的所有要 件之防眩膜A及防眩膜B,完全未產生閃斑,顯示出充分 的防眩性’且亦未產生泛白。此外,由於霧度亦低,即使 配置在圖像顯示裝置時,亦不會引起對比的降低。再者, 鉛筆硬度高而具有強機械強度,且透濕性低而具有高耐濕 性。 另一方面’未使用由丙烯酸系樹脂所構成之基材膜之 防眩膜C,雖顯示出較佳的防眩性能,但錯筆硬度及耐濕 卜生幸乂防眩膜A及_膜B更低。此外,未根據預定圖案所 I作之防眩膜D’由於該能譜比HiVH22未滿足本發明的要 48 322870 201137409 件’所以產生閃斑。 【圖式簡單說明】 第1圖係示思性顯示本發明之防眩膜的一例之剖面 圖。 第2圖係不意性顯示本發明之防眩膜的表面之立體 圖。 第3圖係顯示離散地獲彳!表示標高之函數h(x,y)之狀 悲的模式圖。 第4圖係以二維離散函數h(x,y)來表示本發明的防眩 膜所具備之防眩層的細微凹凸表面的標高之圖的一例。 第5圖係以白與黑的階度來表示將第4圖所示之二維 函數h(x,y)進行離散傅利葉轉換所得之標高的能譜 H2(fx,fy)之圖。 第6圖係顯示第5圖所示之能譜H2(fx,fy)中的fx=〇時 之剖面的圖。 第7圖係用以說明細微凹凸表面之傾斜角度的測定方 法之模式圖。 第8圖係顯示防眩膜所具備之防眩層的細微凹凸表面 之傾斜角度分布的直方圖的一例之圖表。 第9圖係顯示可用以製作本發明之防眩膜所使用之圖 案的圖像資料的一部分之圖。 第10圖係以白與黑的階度來表示將第9圖所示之階調 的二維函數g(X, y)進行離散傅利葉轉換所得之能譜 G2(fx,fy)之圖。 49 322870 201137409 第11圖係顯示第10圖所示之能譜G2(fx,fy)中的h=〇 時之剖面的圖。 “第12圖(3)至(6)係示意性顯示模具的製造方法之前 半部分的較佳一例之圖。 第13圖(a)至(c)係示意性顯示模具的製造方法之後 半部分的較佳一例之圖。 第14圖(a)至(b)係示意性顯示在第丨蝕刻工序中所形 成之凹凸面,藉由第2蝕刻工序予以鈍化之狀態的圖。 第15圖係顯示實施例丨之模具製作時所使用的圖案之 圖。 第16圖係顯示實施例2之模具製作時所使用的圖案之 圖。 第17圖係表示第15圖及第16圖所示之圖案之能譜 G (fx, fy)令的fx = 〇時之剖面的圖。 【主要元件符號說明】 1 防眩膜 2 細微凹凸 3 防眩膜投影面 6a、 6b、6c、6d法線向量 7 模具用基材 8 經研磨的表面 9 感光性樹脂膜 10 經曝光的區域 11 未曝光的區域 12 遮罩 13 無遮罩之處 15 第1表面凹凸形狀 16 鍍鉻層 17 鑛絡表面 18 第2表面凹凸形狀 101 基材膜 102 防眩層 103 細微凹凸表面 322870 50Laser Stream FX (manufactured by Think Laboratory) uses a positive photosensitive resin for the resin film. Fig. 15 shows a pattern of dots that are randomly arranged with a plurality of dot diameters 12#m, and τ is used to divide +β ffl'1 to remove the spatial frequency of 0·04. It is produced by a band-pass filter with a low spatial frequency component below ζπΓ1 and a high spatial frequency component on 〇j 戈. Then, the first residual treatment was carried out with a copper chloride solution (the amount of money was measured. 3. After the first etching treatment, the photosensitive resin film was removed from the roll, and the copper solution was subjected to a second etching treatment (etching amount: 10 μm). The mold A is produced by chrome-plating the chrome-plating degree to 4#m. (Production of the base film) 30 parts by weight of the propylene oxide rubber particles are contained in the sinter A & oxime ester / methyl acrylate = 96 / 4 (by weight) copolymer (refractive index j 49) = heavy Dong 丙 丙 糸 resin composition 'in the first extruder (screw sentence 65mm A single shaft and a vent hole (manufactured by Toshiba Machine Co., Ltd.) are supplied and fused and supplied to a feed block. In addition, 3 Å of acryl rubber particles are contained in methacrylate. /Acrylic acid methyl vinegar = 96/4 (by weight) copolymer (refractive index 1.49) 70 parts by weight of acrylic resin composition, in the second extruder (screw diameter 45 mm, uniaxial, with vent holes (Hitachi Produced by the shipbuilding company)) melt blended and supplied to the splitter to supply the tree from the first extruder to the splitter In the intermediate layer, the resin supplied from the second extruder to the flow divider is formed into a surface layer (double-sided), which is co-extruded at 265 ° C, and is produced by a premature element set at 85 ° C. A base film A having a three-layer structure having a thickness of 80/zm (intermediate layer 50 &quot; m, surface layer 15y mx 45 322870 201137409 2). (Formation of an anti-glare layer) The photocurable resin composition "GRANDIC 806T" ( Dissolved in ethyl acetate to form a 50% by weight solution, and then Lucirin TP0 (manufactured by BASF Corporation, chemical name: 2, 4, 6-trimethyl), which is a photopolymerization initiator The benzamidine diphenylphosphon oxide is prepared by adding 5 parts by weight per 1 part by weight of the curable resin component. The base film A is coated to have a coating thickness after drying. This coating liquid was applied in a 6/zm method, and dried in a dryer set to 6 (TC) for 3 minutes. The base film A after drying was used to make the photocurable resin composition layer a mold side. In this manner, the rubber sheet is pressed against the uneven surface of the previously obtained mold A and adhered. In this state, light from a high-pressure mercury lamp having a strength of 20 mW/cm 2 was irradiated from the side of the base film A so that the amount of light that was changed by h-rays was 200 mJ/cm 2 , and the photocurable resin composition layer was cured. Then, the base film A is peeled off from the mold by each of the hardening resins, and a transparent anti-glare film a composed of a laminate of a cured resin (anti-glare layer) having irregularities on the surface and the base film A is produced. [Example 2] 2 In the exposure process of the mold making process, a pattern in which a plurality of patterns of the image of the 16th f51 βρί* is not continuously arranged is repeatedly repeated, and the light is applied to the photosensitive film. Exposure to light is performed so that the etch of the first etching process is set to 5 m, and the surrogate amount of the second etch process is set to m, and other implementations are performed. In the same manner as in Example 1, the mold B was produced. An anti-glare film B was produced in the same manner as in Example 1 of 322870 46 201137409 except that the obtained mold B was used. The 16th pattern for the point where the majority of the ship's 12-heart point is randomly arranged is 'to remove the space. 〇35_, the lower spatial frequency is formed; ^Use the band-pass filter for the high spatial frequency component above W^, 0.135 &lt;Comparative Example 1&gt; In addition to the base film A, other examples and comparative examples <Comparative Example 2> 珥丨 眩 眩 0 0 First, the surface of the material of diameter __ (according to A5Q56 of JIS) was mirror-polished, and a sand blasting device was used (not (Second production company), to, pressure denier 0 · lMPa (measured pressure), the amount of beads (light surface area per cm used 1), the second oxidation of the beads Tz_sx_17 (T〇s〇h company, average The particle size of .20/zm) is blasted to the polished inscription surface to form irregularities on the surface. The obtained aluminum roll with irregularities was subjected to electroless nickel plating to prepare a mold. At this time, the thickness of the electroless nickel plating was set to 15 #m. An anti-glare film D was produced in the same manner as in Example 1 except that the known mold C was used. The measurement and evaluation results of the above [1] to [4] of the obtained antiglare films A to D are summarized in Table 1. Further, Fig. 17 is a cross-sectional view showing fx = 中 in the energy spectrum G2 (fx, fy) obtained from the pattern used in the production of the mold A of the first embodiment and the mold B of the second embodiment. From Fig. 17, it can be seen that the energy spectrum of the pattern used in the production of the mold A of the first embodiment and the mold b of the second embodiment is in a spatial frequency range larger than ΟμπΓ1 and less than 〇. 〇4/ζπΓΐ. Does not have a maximum value. 47 322870 201137409 1st Table 1 - 1st Example 1 Example 2 Comparative Example 1 Comparative Example 2 Anti-glare film ____ ABCD base film __-' A (acrylic resin) A (propionic acid resin) TAC Film A (acrylic resin) chessboard ABAC surface shape energy spectrum ratio H.VH^ 19 4 19 41 — ^ HaVH^ 0. 002 0. 001 0. 002 0. 003 Tilt angle surface tt 5 · below, Example (3⁄4) 100 100 100 100 Optical characteristic haze (3⁄4) 0.4 0. 6 0. 4 0. 4 Anti-glare performance map 1 1 1 1 Whitening 1 1 1 1 Flash spot 1 1 1 6 Pencil hardness 4H 4H 3H 4H moisture permeability (g/m2. 24hr) 52 48 287 50 From the results shown in Table 1, it can be seen that the anti-glare film A and the anti-glare film B satisfying all the requirements of the present invention have no flare at all. It shows sufficient anti-glare properties and does not produce whitening. In addition, since the haze is also low, even when it is disposed in the image display device, the contrast is not lowered. Further, the pencil has high hardness and strong mechanical strength, and has low moisture permeability and high moisture resistance. On the other hand, the anti-glare film C which does not use the base film composed of the acrylic resin exhibits excellent anti-glare properties, but the erroneous pen hardness and the wet-resistant anti-glare film A and _ film B are more low. Further, the anti-glare film D' which is not made according to the predetermined pattern I produces a flare spot because the energy spectrum ratio HiVH22 does not satisfy the requirement of the present invention 48 322870 201137409 pieces. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a cross-sectional view showing an example of an anti-glare film of the present invention. Fig. 2 is a perspective view showing the surface of the antiglare film of the present invention. Figure 3 shows a pattern of the sorrows of the function h(x, y) representing the elevation. Fig. 4 is a view showing an example of the elevation of the fine uneven surface of the antiglare layer of the antiglare film of the present invention by a two-dimensional discrete function h(x, y). Fig. 5 is a diagram showing the energy spectrum H2(fx, fy) of the elevation obtained by performing the discrete Fourier transform of the two-dimensional function h(x, y) shown in Fig. 4 in white and black gradations. Fig. 6 is a view showing a cross section of fx = 中 in the energy spectrum H2 (fx, fy) shown in Fig. 5. Fig. 7 is a schematic view for explaining a method of measuring the inclination angle of the fine uneven surface. Fig. 8 is a graph showing an example of a histogram of the oblique angle distribution of the fine uneven surface of the antiglare layer provided in the antiglare film. Fig. 9 is a view showing a part of image data which can be used to fabricate the pattern used for the antiglare film of the present invention. Fig. 10 is a diagram showing the energy spectrum G2(fx, fy) obtained by performing discrete Fourier transform on the two-dimensional function g(X, y) of the gradation shown in Fig. 9 in white and black gradations. 49 322870 201137409 Figure 11 is a diagram showing the profile of h = 中 in the energy spectrum G2 (fx, fy) shown in Fig. 10. "Twelfth, (3) to (6) are diagrams schematically showing a preferred example of the first half of the manufacturing method of the mold. Fig. 13 (a) to (c) are schematic diagrams showing the latter half of the manufacturing method of the mold. Fig. 14 (a) to (b) are diagrams schematically showing a state in which the uneven surface formed in the second etching step is passivated by the second etching step. Fig. 16 is a view showing a pattern used in the production of the mold of the embodiment. Fig. 17 is a view showing a pattern used in the production of the mold of the second embodiment. Fig. 17 is a view showing the patterns shown in Figs. 15 and 16. The spectrum of the energy spectrum G (fx, fy) fx = 〇. [Main component symbol description] 1 Anti-glare film 2 Fine bumps 3 Anti-glare film projection surfaces 6a, 6b, 6c, 6d Normal vector 7 Substrate for mold 8 Polished surface 9 Photosensitive resin film 10 Expoched area 11 Unexposed area 12 Mask 13 No mask 15 First surface uneven shape 16 Chrome plating layer 17 Mineral surface 18 Second surface Concavo-convex shape 101 Substrate film 102 Anti-glare layer 103 Fine uneven surface 322870 50

Claims (1)

201137409 * 七、申請專利範圍: 1. 一種防眩膜,具備:基材膜、以及積層於前述基材膜上 並具有凹凸表面之防眩層,該防眩膜之特徵為: &quot; 前述基材膜係含有丙烯酸系樹脂; 空間頻率0.01 ynf1中之前述凹凸表面之標高的能 譜12與空間頻率0.04# nf1中之前述凹凸表面之標高的 能譜Η22之比Ηι2/Η22,係位於3至20的範圍内; 空間頻率0.1 gnf1中之前述凹凸表面之標高的能 譜H32與空間頻率0. 04# πΓ1中之前述凹凸表面之標高的 能譜Η22之比Η32/Η22,為0. 1以下;並且 前述凹凸表面含有95%以上之傾斜角度為5°以下 的面。 2. 如申請專利範圍第1項所述之防眩膜,其中,前述基材 膜的厚度為20以上100// m以下。 3. 如申請專利範圍第1項所述之防眩膜,其中,前述基材 膜係含有丙烯酸橡膠粒子。 4. 一種防眩性偏光板,具備有:如申請專利範圍第1項所 述之防眩膜、以及積層於前述基材膜之與前述防眩層為 相反側的面之偏光膜。 1 322870201137409 * VII. Patent application scope: 1. An anti-glare film comprising: a base film, and an anti-glare layer laminated on the base film and having a concave-convex surface, the anti-glare film is characterized by: The material film contains an acrylic resin; the ratio of the energy spectrum 12 of the elevation of the aforementioned concave-convex surface in the spatial frequency 0.01 ynf1 to the energy spectrum Η22 of the elevation of the aforementioned concave-convex surface in the spatial frequency 0.04# nf1 is located at 3 to The ratio of the energy spectrum H32 of the elevation of the aforementioned concave-convex surface in the spatial frequency of 0.1 gnf1 to the spatial frequency of 0. 04# πΓ1 is the ratio of the energy spectrum Η22 of the elevation of the surface of the concave-convex surface Η32/Η22, which is 0.1 or less. And the uneven surface contains 95% or more of a surface having an inclination angle of 5 or less. 2. The antiglare film according to claim 1, wherein the base film has a thickness of 20 or more and 100//m or less. 3. The anti-glare film according to claim 1, wherein the substrate film contains acrylic rubber particles. An anti-glare polarizing plate comprising: an anti-glare film according to claim 1; and a polarizing film laminated on a surface of the base film opposite to the anti-glare layer. 1 322870
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CN102193113B (en) 2014-09-03
TWI498603B (en) 2015-09-01

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