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TW201042294A - Process for producing light-diffusing element, light-diffusing element, and processes for producing polarizing plate with light-diffusing element and liquid-crystal display device - Google Patents

Process for producing light-diffusing element, light-diffusing element, and processes for producing polarizing plate with light-diffusing element and liquid-crystal display device Download PDF

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Publication number
TW201042294A
TW201042294A TW099108037A TW99108037A TW201042294A TW 201042294 A TW201042294 A TW 201042294A TW 099108037 A TW099108037 A TW 099108037A TW 99108037 A TW99108037 A TW 99108037A TW 201042294 A TW201042294 A TW 201042294A
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Taiwan
Prior art keywords
light diffusing
light
fine particles
diffusing element
resin component
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TW099108037A
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Chinese (zh)
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TWI461745B (en
Inventor
Takehito Fuchida
Hiroyuki Takemoto
Shunsuke Shutou
Minoru Miyatake
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Nitto Denko Corp
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/02Diffusing elements; Afocal elements
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B29WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
    • B29DPRODUCING PARTICULAR ARTICLES FROM PLASTICS OR FROM SUBSTANCES IN A PLASTIC STATE
    • B29D11/00Producing optical elements, e.g. lenses or prisms
    • B29D11/00663Production of light guides
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B29WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
    • B29DPRODUCING PARTICULAR ARTICLES FROM PLASTICS OR FROM SUBSTANCES IN A PLASTIC STATE
    • B29D11/00Producing optical elements, e.g. lenses or prisms
    • B29D11/0074Production of other optical elements not provided for in B29D11/00009- B29D11/0073
    • B29D11/00798Producing diffusers
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/30Polarising elements
    • 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

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

Abstract

A process for producing a light-diffusing element is provided by which a light-diffusing element having a high haze and high diffusing properties and reduced in backward scattering can be produced at low cost with high productivity. The process for producing a light-diffusing element comprises a step in which a matrix-forming material comprising a resin-ingredient precursor and an ultrafine-particle ingredient is brought into contact with fine light-diffusing particles, a step in which at least some of the precursor is infiltrated into an inner part of the fine light-diffusing particles, and a step in which the precursor that has infiltrated into the inner part of the fine light-diffusing particles and the precursor that has not infiltrated into the fine light-diffusing particles are simultaneously polymerized to form a matrix comprising the resin ingredient and the ultrafine-particle ingredient and simultaneously form a concentration gradation region in the vicinity of the inner side of the surface of the fine light-diffusing particles.

Description

201042294 六、發明說明: 【發明所屬之技術領域】 本發明係關於一種光擴散元件之製造方法、光擴散元 件、以及附光擴散元件之偏光板及液晶顯示裝置之製造方 法。 【先前技術】 Ο ❹ 光擴散元件正被廣泛用於照明燈罩、背投電視之榮幕、 面發光裝置(例如液晶顯示裝置)等。近年來,光擴散元件 在提高液晶顯示裝置等之顯示品質、改善視角特性等方面 之利用正在推進。作為光擴散元件’已提出有使微粒分散 於樹脂片材等基質中而成者等(例如參照專利文獻丨)。於此 種光擴散元件中,所入射之光之大部分係向前方(出射面 側)散射,而有一部分則向後方(入射面側)散射。微粒與基 質之折射率差越大則擴散性(例如霧度值)越大,但另一^ 面,若折射率差較大則背向散射會增大。若背向散射較 大,則於將光擴散元件用於液晶顯示裝置之情形時,當外 部光入射至液晶顯示裝置時畫面會變得發白,因此難:顯 示具有對比度之影像或圖像。 · 作為解決上述問題之方法’基於抑制微粒與基質之界面 上之反射的構想’已提出有使核與殼之折射率不同之核殼 微粒e-sheH partiele)、或折射率自微粒之中心部 側^變化之所謂G削(gradientindex,梯度指數)微粒等 之梯又折射率微粒分散於樹脂中之方法(例如參照專利文 獻2 4),、、、而’此等微粒與普通微粒相比,製造製程較為 147072.doc 201042294 複雜,因此生產率不充分而不具有實用性。 先前技術文獻 專利文獻 專利文獻1:日本專利第3071538號 專利文獻2:曰本專利特開平6_347617號公報 專利文獻3 :日本專利特開2003_262710號公報 專利文獻4 :曰本專利特開2〇〇2 212245號公報 【發明内容】 發明所欲解決之問題 本發明係為解決上述先前之課題開發而成者,其目的在 於提供一種可低成本且高生產率地製造霧度值較高,具有 較強之擴散性’且抑制背向散射之光擴散元件的光擴散元 件之製造方法。 解決間題之技術手段 本發明之光擴散元件之製造方法包括如下步驟:使包含 樹脂成分之前驅物及超微粒成分之基質形成材料與光擴散 性微粒相接觸;使該前驅物之至少一部分滲透至該光擴散 性微粒之内部;以及使已滲透至該光擴散性微粒之内部之 前驅物及未滲透至該光擴散性微粒之前驅物同時發生聚合 而形成包含樹脂成分及超微粒成分之基質,並同時於該光 擴散性微粒之表面附近内部形成濃度調變區域。 於較佳實施形態中’上述製造方法係於上述滲透步驟 中’使上述前驅物自上述光擴散性微粒之表面滲透至該光 擴散性微粒之平均粒徑之1 0°/〇以上95%以下之範圍為止。 147072.doc 201042294 於較佳實施形態中,上述製造方法係使上述樹脂成分之 前驅物與該光擴散性微粒接觸較上述光擴散性 微粒之粒徑 實質上達到最大為止之時間更長之時間。 於較佳實施形態中’上述樹脂成分為電離放射線硬化型 樹月曰’上述製造方法係藉由照射電離放射、線而使該樹脂成 分之前驅物發生聚合。 根據本發明之另-態樣,提供_種光擴散元件。該光擴 散元件係藉由上述之方法而獲得,包括包含樹脂成分及超 微粒成分之基質、以及分散於該基質中之光擴散性微粒, 且於該光擴散性微粒之表面附近内部具有該樹脂成分經滲 透而形成之濃度調變區域。 根據本發明之進而另一態樣,提供一種附光擴散元件之 偏光板之製造方法。該方法中使用上述光擴散元件之製造 方法。 根據本發明之進而另一態樣,提供一種液晶顯示裝置之 製造方法。該方法中使用上述光擴散元件之製造方法。 發明之效果 根據本發明,於藉由組合使用特定之基質樹脂成分(實 貝上為其别驅物)與特定之光擴散性微粒而製造光擴散元 件時,可使基質樹脂成分之前驅物滲透至光擴散性微粒内 部。可藉由使該基質樹脂成分之前驅物發生聚合而形成基 質’並同時於該光擴散性微粒之表面附近内部形成濃度調 變區域(即’可一次性地(one batch)形成基質與濃度調變區 域)。如此’根據本發明,無需為形成濃度調變區域而進 147072.doc 201042294 行特殊之處理或操作’因此可低成本且高生產率地製造光 擴政元件巾且’藉由本發明之製造方法所獲得之光擴散 兀件於光擴散性微粒之表面附近内部形成有濃度調變區 域’因此可於光擴散性元件與基質之界面附近使折射率階 段性地或實質上連續性地變化。因此,可良好地控制基質 與光擴散性微粒之界面之反射’從而可抑制背向散射。此 外,根據本發明,藉由使用具有特定之折射率及對於樹脂 成分有特定相溶性之超微粒成分,可容易地調整基質之折 射率。特別是根據本發明,藉由使樹脂成分滲透至光擴散 性微粒内部而可提高基質中之超微粒成分之濃度,因此可 容易地擴大基質與光擴散性微粒之折射率差。其結果為, 藉由本發明之製造方法所獲得之Μ散元件之霧度值較 尚,具有較強之擴散性,且抑制了背向散射。 【實施方式】 以下’ -面參照圖式,—面就本發明之較佳實施形態加 以說明,⑮本發明並不限定於此等具體實施形態。 Α·光擴散元件之製造方法 本發明之光擴散元件之製造方法包括如下㈣:使包含 樹脂成分之前驅物及超微粒成分之基質形成材料與光擴散 性微粒相接觸(設為步驟Α);使該前驅物之至少一部分滲 透至該光擴散性微粒之内部(設為步驟以及㈣前驅 物發生聚合而形成包含樹脂成分及超微粒成分之基質,並 同時於該光擴散性微粒之表面附近内部形成濃度調變區域 (設為步驟C)。 147072.doc 201042294[Technical Field] The present invention relates to a method of manufacturing a light diffusing element, a light diffusing element, and a polarizing plate with a light diffusing element and a method of manufacturing the liquid crystal display device. [Prior Art] Ο ❹ Light diffusing elements are widely used in lighting shades, rear projection televisions, surface light-emitting devices (such as liquid crystal display devices), and the like. In recent years, the use of light diffusing elements for improving the display quality of liquid crystal display devices and the like, and improving viewing angle characteristics are progressing. As the light-diffusing element, it has been proposed to disperse fine particles in a matrix such as a resin sheet (for example, see Patent Document). In such a light diffusing element, most of the incident light is scattered toward the front (the exit surface side), and a part of the light is scattered toward the rear (incidence surface side). The larger the refractive index difference between the fine particles and the matrix, the larger the diffusibility (for example, the haze value), but the other side, if the refractive index difference is large, the backscattering increases. If the backscattering is large, when the light diffusing element is used in a liquid crystal display device, the screen becomes white when external light is incident on the liquid crystal display device, so that it is difficult to display an image or an image having contrast. · As a method to solve the above problem, 'the concept of suppressing the reflection at the interface between the particle and the substrate' has been proposed to have a core-shell particle e-sheH partiele having a different refractive index between the core and the shell, or a refractive index from the center of the particle. A method in which a gradient-indexed particle such as a gradient index particle is dispersed in a resin (for example, see Patent Document 24), and "the particles are compared with ordinary particles. The manufacturing process is more complicated than 147072.doc 201042294, so the productivity is not sufficient and not practical. CITATION LIST Patent Literature Patent Literature 1: Japanese Patent No. 3071538 Patent Document 2: Japanese Patent Laid-Open Publication No. Hei No. Hei. No. Hei. No. Hei. No. Hei. No. Hei. SUMMARY OF THE INVENTION PROBLEMS TO BE SOLVED BY THE INVENTION The present invention has been made in order to solve the above-mentioned problems, and an object thereof is to provide a high haze value which is low in cost and high in productivity, and has a strong A method of manufacturing a light diffusing element that diffuses and suppresses backscattering light diffusing elements. Means for Solving the Problem The method for producing a light diffusing element of the present invention comprises the steps of: contacting a matrix forming material comprising a resin component precursor and an ultrafine particle component with light diffusing fine particles; and infiltrating at least a portion of the precursor Up to the inside of the light diffusing fine particles; and simultaneously polymerizing the precursors that have penetrated into the light diffusing fine particles and the precursors before they penetrate into the light diffusing fine particles to form a matrix containing the resin component and the ultrafine particle component At the same time, a concentration modulation region is formed inside the vicinity of the surface of the light diffusing fine particles. In a preferred embodiment, the method of the present invention is characterized in that the precursor is infiltrated from the surface of the light diffusing fine particles to 10%/〇 or more and 95% or less of the average particle diameter of the light diffusing fine particles. The scope is up to now. In a preferred embodiment, the manufacturing method is such that the precursor of the resin component is in contact with the light diffusing fine particles for a longer period of time than when the particle diameter of the light diffusing fine particles is substantially maximized. In the preferred embodiment, the resin component is an ionizing radiation-curable tree. The above-described manufacturing method is to polymerize the resin component by irradiating ionizing radiation or a wire. According to another aspect of the invention, a light diffusing element is provided. The light diffusing element is obtained by the above method, and includes a substrate containing a resin component and an ultrafine particle component, and light diffusing fine particles dispersed in the matrix, and having the resin in the vicinity of the surface of the light diffusing fine particle. A concentration-modulating region formed by penetration of a component. According to still another aspect of the present invention, a method of manufacturing a polarizing plate with a light diffusing element is provided. In the method, a method of manufacturing the above light diffusing element is used. According to still another aspect of the present invention, a method of manufacturing a liquid crystal display device is provided. In the method, a method of manufacturing the above light diffusing element is used. Advantageous Effects of Invention According to the present invention, when a light diffusing element is produced by using a specific matrix resin component (on its shell) and a specific light diffusing fine particle in combination, the matrix resin component precursor can be infiltrated. To the inside of the light diffusing particles. The matrix can be formed by polymerizing the precursor of the matrix resin component and simultaneously forming a concentration-modulating region in the vicinity of the surface of the light-diffusing microparticle (ie, 'the matrix can be formed in one batch” Variable area). Thus, according to the present invention, it is not necessary to perform special processing or operation for forming a concentration-modulating region. Therefore, it is possible to manufacture a light-expanding elemental towel at low cost and high productivity and 'obtained by the manufacturing method of the present invention. The light diffusing element is formed with a concentration modulation region in the vicinity of the surface of the light diffusing fine particles. Therefore, the refractive index can be changed stepwise or substantially continuously in the vicinity of the interface between the light diffusing element and the substrate. Therefore, the reflection of the interface between the substrate and the light diffusing fine particles can be well controlled so that backscattering can be suppressed. Further, according to the present invention, the refractive index of the substrate can be easily adjusted by using an ultrafine particle component having a specific refractive index and a specific compatibility with respect to the resin component. In particular, according to the present invention, since the concentration of the ultrafine particle component in the matrix can be increased by infiltrating the resin component into the inside of the light diffusing fine particles, the refractive index difference between the matrix and the light diffusing fine particles can be easily increased. As a result, the haze element obtained by the production method of the present invention has a relatively high haze value, has strong diffusibility, and suppresses backscattering. [Embodiment] Hereinafter, the preferred embodiments of the present invention will be described with reference to the drawings, and the present invention is not limited to the specific embodiments.制造·Light diffusing element manufacturing method The method for producing a light diffusing element according to the present invention includes the following (4): contacting a matrix forming material containing a resin component precursor and an ultrafine particle component with light diffusing fine particles (step Α); At least a part of the precursor is allowed to permeate into the inside of the light diffusing fine particles (the step and (4) the precursor is polymerized to form a matrix containing the resin component and the ultrafine particle component, and simultaneously in the vicinity of the surface of the light diffusing fine particle A concentration modulation region is formed (set to step C). 147072.doc 201042294

Α-1·步驟A 於步驟A巾,具代表性的是製備塗敷液,該塗敷液係使 包含樹脂成分之前驅物及超微粒成分之基質形成材料與光 擴散性微粒溶解或分散於揮發性溶劑中而成之溶液。具代 表性的是,該塗敷液係將超微粒成分及光擴散性微粒分散 於前驅物及揮發性溶劑中而成之分散體。作為使超微粒成 分及光擴散性微粒分散之方法,可採用任意適當之方法 (例如超聲波處理)。於該塗敷液中,光擴散性微粒與樹脂 成分之前驅物接觸。 A-1-1.樹脂成分 上述樹脂成分只要能良好地形成上述濃度調變區域便 可包含任意適當之材料。樹脂成分之折射率宜滿足下述式 (1)之關係: 〇< I Πρ-ΠΑ | · · . (1 )。 式(1)中’ ηΑ表示基質之樹脂成分之折射率,〜表示光擴 ❹ 散性微粒之折射率。I ηΡ-ηΑ I宜為〇.〇1〜〇」〇,更佳為 〇_〇1〜0.06,特佳為0.02〜〇.06。若丨ηρ·ηΑ丨未達〇 〇1,則 存在不形成上述濃度調變區域之情形。若丨ηΡ-ηΑ丨超過 〇·1〇 ’則有背向散射增大之虞。 樹脂成分宜包含與光擴散性微粒為同系之化合物。更佳 為’樹脂成分包含與光擴散性微粒為同系之化合物中相溶 性較高之化合物。藉此’樹脂成分因係與光擴散性微粒同 系之材料’故而其前驅物(單體)可滲透至光擴散性微粒内 部。該前驅物(單體)藉由後述之聚合步驟而發生聚合之結 147072.doc 201042294 果為, …可利用樹脂成分於光擴散性 好地形占、、曲+_Α-1·Step A In the step A, a coating liquid is prepared, which is obtained by dissolving or dispersing a matrix-forming material and a light-diffusing fine particle containing a resin component precursor and an ultrafine particle component. A solution made from a volatile solvent. Typically, the coating liquid is a dispersion in which an ultrafine particle component and light diffusing fine particles are dispersed in a precursor and a volatile solvent. As a method of dispersing the ultrafine particle component and the light diffusing fine particles, any appropriate method (e.g., ultrasonic treatment) can be employed. In the coating liquid, the light diffusing fine particles are in contact with the resin component precursor. A-1-1. Resin component The above-mentioned resin component may contain any appropriate material as long as the concentration-modulating region can be favorably formed. The refractive index of the resin component preferably satisfies the relationship of the following formula (1): 〇 < I Πρ-ΠΑ | · · (1). In the formula (1), 'ηΑ represents the refractive index of the resin component of the matrix, and ~ represents the refractive index of the optically dilated particles. I ηΡ-ηΑ I should be 〇.〇1~〇"〇, more preferably 〇_〇1~0.06, especially preferably 0.02~〇.06. If 丨ηρ·ηΑ丨 does not reach 〇 〇1, there is a case where the above-described concentration modulation region is not formed. If 丨ηΡ-ηΑ丨 exceeds 〇·1〇 ', there is an increase in backscattering. The resin component preferably contains a compound which is homologous to the light diffusing fine particles. More preferably, the resin component contains a compound having high compatibility with a compound of the same type as the light diffusing fine particles. Thereby, the resin component is a material which is the same as the light diffusing fine particles, and the precursor (monomer) can penetrate into the inside of the light diffusing fine particles. The precursor (monomer) is polymerized by a polymerization step described later. 147072.doc 201042294 As a result, ... the resin component can be utilized for light diffusibility, and the topography is __

微粒之表面附近内部良 本說明書中所謂「同 頃似’所謂「不同系」 上述樹脂成分宜包含有機化合物,更佳為包含電離放射 線硬化型樹脂。電離放射線硬化型樹脂之塗膜硬度優異。 作為電離放射線,可列舉例如紫外線、可見光、紅外線、 電子束。以紫外線為宜,因此樹脂成分特佳為包含紫外線 硬化型樹脂。作為紫外線硬化型樹脂,可列舉例如丙烯酸 s曰樹月曰(環氧丙烯酸酯、聚酯丙烯酸酯、丙稀酸丙烯酯、 趟丙稀酸酯)等自由基聚合型單體或者低聚物等。構成丙 稀®31酿樹脂之單體成分(前驅物)之分子量宜為200〜700。 作為構成丙烯酸酯樹脂之單體成分(前驅物)之具體例,可 列舉季戊四醇三丙稀酸醋(PETA(pentaerythritol triacrylate): 分子量為298)、新戊二醇二丙烯酸酯(NPGDA(neopentyl glycol diacrylate):分子量為212)、二季戊四醇六丙烯酸 醋(DPHA(dipentaerythritol hexaacrylate):分子量為 632)、 147072.doc 201042294 二季戊四醇五丙稀酸醋(DPPA(dipentaerythritol pentaacrylate): 分子量為578)、三羥曱基丙烷三丙烯酸酯 (TMPTA(trimethylolpropane triacrylate):分子量為 296)。 此種單體成分(前驅物)具有適於滲透至光擴散性微粒之交 聯結構(三維網狀結構)之分子量及立體結構,故而較佳。 亦可根據需要添加起始劑。作為起始劑,可列舉例如 UV(ultravi〇let,紫外線)自由基產生劑(汽巴精化(CibaIn the present invention, the resin component preferably contains an organic compound, and more preferably contains an ionizing radiation curable resin. The coating film of the ionizing radiation curable resin is excellent in hardness. Examples of the ionizing radiation include ultraviolet rays, visible light, infrared rays, and electron beams. Ultraviolet rays are preferred, and therefore, the resin component is particularly preferably an ultraviolet curable resin. Examples of the ultraviolet curable resin include radical polymerizable monomers or oligomers such as acrylonitrile sulphate (epoxy acrylate, polyester acrylate, propylene acrylate, isopropyl acrylate). . The monomer component (precursor) constituting the propylene resin 31 resin preferably has a molecular weight of 200 to 700. Specific examples of the monomer component (precursor) constituting the acrylate resin include pentaerythritol triacrylate (PETA (pentaerythritol triacrylate): molecular weight: 298) and neopentyl glycol diacrylate (NPGDA (neopentyl glycol diacrylate). ): molecular weight: 212), dipentaerythritol hexaacrylate (molecular weight: 632), 147072.doc 201042294 dipentaerythritol pentaacrylate (molecular weight: 578), trioxindole Methyl propane triacrylate (TMPTA (trimethylolpropane triacrylate): molecular weight 296). Such a monomer component (precursor) is preferred because it has a molecular weight and a three-dimensional structure suitable for infiltration into a crosslinked structure (three-dimensional network structure) of light diffusing fine particles. An initiator can also be added as needed. As the initiator, for example, UV (ultravi〇let, ultraviolet) radical generator (Ciba essence (Ciba) can be cited.

Specialty Chemicals)公司製造之 Irgacure 907、Irgacure 127、Irgacure 192等)、過氧化苯曱醯。上述樹脂成分除包 含上述電離放射線硬化型樹脂以外,亦可包含其他樹脂成 分。其他樹脂成分可為電離放射線硬化型樹脂,亦可為熱 固性樹脂,亦可為熱塑性樹脂。作為其他樹脂成分之代表 例,可列舉脂肪族系(例如聚烯烴)樹脂、胺酯系樹脂。於 使用其他樹脂成分之情形時,對其種類或調配量進行調 整,以使得良好地形成上述濃度調變區域,且折射率滿足 上述式(1)之關係。 上述樹脂成分之折射率宜為1.40〜1.6〇。 相對於所形成之基質100重量份,上述塗敷液中之上述 樹脂成分之調配量宜為20重量份〜80重量份,更佳為45重 量份〜65重量份。 Α-1-2.超微粒成分 上述超微粒成分中,具代表性的是可作為調整基質折射 率之成分而發揮作用。藉由使用超微粒成分,可容易地調 整基質之折射率,從而可擴大光擴散性微粒與基質之折射 147072.doc 201042294 率差。特別是根據本發明,藉由樹脂成分渗透至光擴散性 微粒内部,可提高基質中之超微粒成分之濃度,因二容 易地擴大基質與光擴散性微粒之折射率差。其結果為,= 獲得雖為薄膜卻具有高霧度值(強擴散性)之光擴散:件可 超微粒成分之折射率nB宜滿足下述式(2): 〇< I nP-nA | < | nP-nB | · · ·⑺。 式(2)中’以及〜為如上所述。丨np_nB丨宜為〇 1〇〜丨5〇, 更佳為0.20〜0.80。若丨np_nB丨未達〇 1〇,則多數情形 度為90%以下,其結果為,存在當裝入至液晶顯示裝置時 無法充分擴散來自光源之光而使得視角變窄之虞。若丨 nP-nB |超過1.50,則存在背向散射增大之虞。 超微粒成分宜包含與上述樹脂成分及光擴散性微粒為不 同系之化合物,更佳為包含無機化合物。作為較佳之無機 化合物,可列舉例如金屬氧化物、金屬氟化物。作為金屬 氧化物之具體例,可列舉氧化鍅(zirc〇nia)(折射率: 2.19)、氧化銘(折射率:丨56〜2 62)、氧化鈦(折射率: 2.49〜2.74)、氧化矽(折射率:125〜146)。作為金屬氟化 物之具體例,可列舉氟化鎂(折射率:丨.37)、氟化鈣(折射 率:1.40〜1.43)。此等金屬氧化物及金屬氟化物對光之吸 收較少,並且具有在電離放射線硬化型樹脂或熱塑性樹脂 等有機化合物中難以體現之折射率,因此可擴大光擴散性 微粒與基質之折射率差。而且,此等金屬氧化物及金屬氟 化物因與樹脂成分之分散性適當’故而可於光擴散性微粒 與基質之界面附近(光擴散性微粒之周邊部)形成其他濃度 147072.doc 10 201042294 調變區域—將此種其他濃度調變區域亦形成於光擴散微粒 之外。p,糟此與僅在光擴散性微粒内部形成濃度調變區域 之情形時相比,可進一步抑制背向散射。無機化合物特佳 &氧化錯。其原因在於,由於與光擴散性微粒之折射率差 肖大’且與樹脂成分之分散性適當,因而可良好地形成具 有所期望之特性(或結構)之其他濃度調變區域。再者,於 本發明中,只要於光擴散性微粒之表面附近内部形成濃度 〇 調變區域即可,亦可不形成上述其他濃度調變區域。X 上述超微粒成分之折射率宜為14〇以下或16〇以上更 ::為㈣以下紅70〜2.8〇,肖佳為i 4〇以下或2 〇〇〜2 8〇。 右折射率超過1.40或未達uo,則有可能導致光擴散性微 粒與基質之折射率差不充分,當將所獲得之光擴散元件用 於準直背光前面擴散系統之液晶顯示裝置中時,無法充分 擴政來自準直背光之光而導致視角變窄。 上述超微粒成分亦可藉由多孔質化而降低折射率。 〇 上述超微粒成分之平均粒徑宜為1 nm〜1〇〇 nm,更佳為 10nm〜8〇nm,進而更佳為2〇nm〜7〇nm。如此,藉由使用 小於光之波長之平均粒徑的超微粒成分’可獲得於超微粒 成分與樹脂成分之間不產生幾何光學反射、折射、散射而 光學上均勻之基質。其結果為,可獲得光學上均勻之光擴 散元件。 ' 上述超微粒成分宜為與上述樹脂成分之分散性良好。於 本說明書中,所謂「分散性良好」,係指塗佈將上述樹脂 成分、超微粒成分、(根據需要而少量之uv起始劑)及揮發 147072.doc -11 - 201042294 並將溶劑加以乾燥去除 溶劑進行混合所得之塗敷液, 得之塗膜為透明。 上述超微粒成分宜已進行表面 改質。Specialty Chemicals) Irgacure 907, Irgacure 127, Irgacure 192, etc., benzoquinone peroxide. The resin component may contain other resin components in addition to the ionizing radiation curable resin. The other resin component may be an ionizing radiation curable resin, a thermosetting resin, or a thermoplastic resin. Representative examples of other resin components include aliphatic (e.g., polyolefin) resins and amine ester resins. In the case of using other resin components, the kind or the amount of blending is adjusted so that the above-mentioned concentration modulation region is favorably formed, and the refractive index satisfies the relationship of the above formula (1). The refractive index of the above resin component is preferably from 1.40 to 1.6 Å. The compounding amount of the above resin component in the coating liquid is preferably from 20 parts by weight to 80 parts by weight, more preferably from 45 parts by weight to 65 parts by weight, based on 100 parts by weight of the substrate to be formed. Α-1-2. Ultrafine particle component The above ultrafine particle component is typically used as a component for adjusting the refractive index of the matrix. By using the ultrafine particle component, the refractive index of the matrix can be easily adjusted, thereby expanding the refractive index of the light diffusing fine particles and the matrix. In particular, according to the present invention, the penetration of the resin component into the inside of the light diffusing fine particles increases the concentration of the ultrafine particle component in the matrix, and the refractive index difference between the matrix and the light diffusing fine particles is easily expanded. As a result, = light diffusion having a high haze value (strong diffusibility) is obtained as a film: the refractive index nB of the ultrafine particle component should satisfy the following formula (2): 〇 < I nP-nA | < | nP-nB | · · · (7). In the formula (2), 'and' are as described above.丨np_nB should be 〇 1〇~丨5〇, more preferably 0.20~0.80. If 丨np_nB丨 is less than 〇1, most cases are 90% or less. As a result, there is a possibility that the light source from the light source cannot be sufficiently diffused when it is loaded into the liquid crystal display device, so that the viewing angle is narrowed. If 丨nP-nB| exceeds 1.50, there is a tendency for backscattering to increase. The ultrafine particle component preferably contains a compound different from the above resin component and light diffusing fine particles, and more preferably contains an inorganic compound. Preferred examples of the inorganic compound include metal oxides and metal fluorides. Specific examples of the metal oxide include zirconia (refractive index: 2.19), oxidation (refractive index: 丨56 to 2 62), titanium oxide (refractive index: 2.49 to 2.74), and cerium oxide. (refractive index: 125~146). Specific examples of the metal fluoride include magnesium fluoride (refractive index: 丨.37) and calcium fluoride (refractive index: 1.40 to 1.43). These metal oxides and metal fluorides have less absorption of light, and have a refractive index which is difficult to be expressed in an organic compound such as an ionizing radiation-curable resin or a thermoplastic resin, thereby expanding the refractive index difference between the light-diffusing particles and the matrix. . Further, since these metal oxides and metal fluorides have appropriate dispersibility with the resin component, other concentrations can be formed in the vicinity of the interface between the light diffusing fine particles and the substrate (the peripheral portion of the light diffusing fine particles). 147072.doc 10 201042294 Variable region - This other concentration-modulating region is also formed outside of the light-diffusing particles. In the case of p, the backscattering can be further suppressed as compared with the case where the concentration modulation region is formed only inside the light diffusing fine particles. Inorganic compounds are particularly good & oxidation. This is because the difference in refractive index from the light diffusing fine particles is large, and the dispersibility with the resin component is appropriate, so that other concentration-modulating regions having desired characteristics (or structures) can be favorably formed. Further, in the present invention, the concentration 〇 modulation region may be formed inside the vicinity of the surface of the light diffusing fine particles, and the other concentration modulation regions may not be formed. X The refractive index of the above ultrafine particle component is preferably 14 〇 or less or 16 〇 or more :: for (four) the following red 70 to 2.8 〇, Xiao Jia is i 4 〇 or 2 〇〇 〜 2 8 〇. When the right refractive index exceeds 1.40 or does not reach uo, the refractive index difference between the light diffusing fine particles and the substrate may be insufficient, and when the obtained light diffusing element is used in a liquid crystal display device for collimating the backlight front diffusion system, The inability to fully expand the light from collimating the backlight causes the viewing angle to narrow. The ultrafine particle component may also have a reduced refractive index by being made porous. The average particle diameter of the above ultrafine particle component is preferably from 1 nm to 1 Å, more preferably from 10 nm to 8 Å, and still more preferably from 2 Å to 7 〇 nm. Thus, by using an ultrafine particle component 'having an average particle diameter smaller than the wavelength of light, a matrix which is optically uniform without causing geometric optical reflection, refraction, and scattering between the ultrafine particle component and the resin component can be obtained. As a result, an optically uniform optical diffusing element can be obtained. The above ultrafine particle component preferably has good dispersibility with the above resin component. In the present specification, the term "good dispersibility" means applying the resin component, the ultrafine particle component, (a small amount of a uv initiator as needed), and volatilizing 147072.doc -11 - 201042294 and drying the solvent. The coating liquid obtained by mixing the solvent was removed, and the coating film was made transparent. The above ultrafine particle component should preferably be surface modified.

之具體例,可列舉矽烷系偶合劑、鈦 鈦酸酯系偶合劑等偶合 劑、脂肪酸系界面活性劑等界面活性劑。冑由使用此種表 面改質劑,可提高樹脂成分與超微粒成分之潤濕性,使樹 脂成分與超微粒成分之界面穩定化,使超微粒成分良好地 分散於樹脂成分中,且良好地形成上述其他濃度調變區 域。 相對於所形成之基質100重量份,上述塗敷液中之超微 粒成分之調配量宜為1〇重量份〜70重量份,更佳為35重量 份〜55重量份。 A·1·3.光擴散性微粒 上述光擴散性微粒只要能良好地形成上述濃度調變區 域’便可包含任意適當之材料。上述光擴散性微粒之折射 率宜滿足上述式(1)之關係。如上所述,光擴散性微粒宜包 含與上述基質之樹脂成分為同系之化合物。例如’於構成 基質之樹脂成分之電離放射線硬化型樹脂為丙烯酸酯系樹 脂之情形時,光擴散性微粒亦以包含丙烯酸酯系樹脂為 147072.doc •12· 201042294 宜。更具體而言,於構成基質之樹脂成分之丙烯酸酯系樹 脂之單體成分為例如上述之PETA、NPGDA、DPHA、 DPPA及/或ΤΜΡΤΑ之情形時,構成光擴散性微粒之丙烯酸 醋系樹脂宜為聚甲基丙烯酸甲酯(PMMA,polymethyl methacrylate)、聚丙烯酸甲酯(PMA,p〇lymethyl acrylate) Ο ❹ 及此等之共聚物與此等之交聯物。作為與PMMA及PMA之 共聚合成分,可列舉聚胺醋、聚苯乙烯(PSt,p〇lystyrene)、 二聚氰胺樹脂。光擴散性微粒特佳為包含PMMA。其原因 在於,與基質之樹脂成分之折射率或熱力學特性之關係適 田此外,光擴散性微粒宜具有交聯結構(三維網狀結 構)。具有父聯結構之光擴散性微粒可膨潤。因此,此種 光擴散性微粒與緻密或實心之無機粒子不同,可使具有適 當相溶性之樹脂成分之前驅物良好地滲透至其内部。光擴 散性微粒之交聯密度宜為小(稀疏)至可獲得所期望之滲透 i巳圍(下述)之程度。例如,塗佈上述塗敷液時之光擴散性 微粒相對於樹脂成分前驅物(亦可包含溶劑)之膨潤度宜為 顧〜義。於此’所謂「膨潤度」,係指膨潤狀態之粒 子之平均粒徑相對於膨潤前之粒子之平均粒徑的比率。 上述光擴散性微粒之平均粒徑宜為i _〜5㈣,更佳為 〜〜4·— ’進而更佳為2〇叫〜3〇_,特佳為21 μηι〜2.4 μιη。光擴散性微粒 ^ ώ Τ〈十均粒徑宜為光擴散元件之 厚度之1/2以下(例如,1/2〜1/2 口 件)八要係相對於光擴散元 真:八 之比率之平均粒徑,便可於光擴散元件 度方向上排列複數個光擴散性微粒,因此可於入射光 147072.doc 201042294 使該光多重擴散,其結果為可獲 透過光擴散元件之期間 得充分之光擴散性。 光擴散性微粒之重量平均粒徑分布之 丁阳左且為1 〇 μπ^以下,更佳為〇.5㈣以下。若混合存在多個粒徑小 量平均粒徑之光擴散性微粒,則存在擴散性過於增大而無 法良好地抑制背向散射之情形。若混合存在多個”大: 重量平均粒徑之光擴散性微粒,則存在無法於光擴散元件 之厚度方向上排列複數個光擴散性微粒而無法獲得多重擴 政之情形,其結果為存在光擴散性變得不充分之情形。、 作為上述光擴散性微粒之形狀,可根據目的採用任意適 當之形狀。作為具體例,可列舉圓球狀、鱗片狀、板狀^ 橢圓球狀、不定形。於多數情形時,可使用圓球狀微粒作 為上述光擴散性微粒。 上述光擴散性微粒之折射率宜為〖.儿〜丨7〇,更佳為 1 ·40〜1 ·60 〇 相對於所形成之基質1 〇〇重量份,上述塗敷液中之光擴 散性微粒之調配量宜為10重量份〜100重量份,更佳為15重 量份〜40重量份。藉由包含例如此種調配量之具有上述較 佳範圍之平均粒徑的光擴散性微粒,可獲得具有非常優異 之光擴散性之光擴散元件。 Α_1-4.塗敷液之整體構成 作為上述揮發性溶劑,只要可使上述各成分溶解或均勻 分散’便可採用任意適當之溶劑。作為揮發性溶劑之具體 例’可列舉乙酸乙酯、乙酸丁酯、乙酸異丙酯' 2- 丁酮(甲 147072.doc -14- 201042294 基乙基酮)、曱基異丁基酮、環戍_、甲笨、異丙醇、正 丁醇、環戊烷、水。 上述塗敷液可根據目的’進而含有任意適當之添加劑。 例如於使用上述超微粒成分之情形時,為使超微粒成分良 好地分散’可適當地使用分散劑。作為添加劑之其他具體 例,可列舉抗老化劑、改質劑、界面活性劑、防變色劑、 紫外線吸收劑、均化劑、消泡劑。 述塗敷液之固體成分濃度可進行調 ΟSpecific examples thereof include a coupling agent such as a decane coupling agent or a titanium titanate coupling agent, and a surfactant such as a fatty acid surfactant.使用 By using such a surface modifier, the wettability of the resin component and the ultrafine particle component can be improved, the interface between the resin component and the ultrafine particle component can be stabilized, and the ultrafine particle component can be well dispersed in the resin component, and is good. The above other concentration modulation regions are formed. The amount of the ultrafine particle component in the coating liquid is preferably from 1 part by weight to 70 parts by weight, more preferably from 35 parts by weight to 55 parts by weight, based on 100 parts by weight of the substrate to be formed. A·1·3. Light-diffusing fine particles The light-diffusing fine particles may contain any suitable material as long as the concentration-modulating region can be formed satisfactorily. The refractive index of the above light diffusing fine particles preferably satisfies the relationship of the above formula (1). As described above, the light diffusing fine particles preferably contain a compound which is homologous to the resin component of the above matrix. For example, when the ionizing radiation-curable resin constituting the resin component of the matrix is an acrylate-based resin, the light-diffusing fine particles are preferably 147072.doc •12·201042294. More specifically, when the monomer component of the acrylate resin constituting the resin component of the matrix is, for example, the above-mentioned PETA, NPGDA, DPHA, DPPA, and/or hydrazine, the acrylic vinegar resin constituting the light diffusing fine particles should preferably be It is a polymethyl methacrylate (PMMA), a polymethyl methacrylate (PMA), and a copolymer of these and the like. Examples of the copolymerization component with PMMA and PMA include polyamine vinegar, polystyrene (PSt, p〇lystyrene), and melamine resin. The light diffusing fine particles are particularly preferably composed of PMMA. The reason for this is that the relationship between the refractive index or the thermodynamic property of the resin component of the matrix is appropriate. Further, the light diffusing fine particles preferably have a crosslinked structure (three-dimensional network structure). Light diffusing particles having a parent structure can be swollen. Therefore, such light-diffusing fine particles are different from dense or solid inorganic particles, and the resin component having the appropriate compatibility can be well penetrated into the interior thereof. The crosslink density of the light-diffusing particles is preferably small (sparse) to the extent that the desired penetration (described below) can be obtained. For example, the degree of swelling of the light diffusing fine particles in the coating liquid with respect to the resin component precursor (which may also include a solvent) is preferably determined. The term "swelling degree" as used herein refers to the ratio of the average particle diameter of the particles in the swollen state to the average particle diameter of the particles before swelling. The average particle diameter of the light-diffusing fine particles is preferably i _ 5 5 (four), more preferably 〜 4 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 Light-diffusing particles ^ ώ Τ <The average particle size should be less than 1/2 of the thickness of the light-diffusing element (for example, 1/2 to 1/2 mouthpieces). The average particle diameter allows a plurality of light diffusing fine particles to be aligned in the direction of the light diffusing element, so that the light can be multi-diffused at the incident light 147072.doc 201042294, and as a result, the period during which the light diffusing element can be transmitted is sufficient. Light diffusivity. The weight average particle size distribution of the light diffusing fine particles is preferably 1 〇 μπ^ or less, more preferably 〇5 (4) or less. When a plurality of light-diffusing fine particles having a small particle diameter and a small average particle diameter are mixed, the diffusibility is excessively increased, and the backscattering cannot be satisfactorily suppressed. When a plurality of "light-diffusion particles having a large average particle diameter are mixed, there are cases where a plurality of light-diffusing fine particles cannot be arranged in the thickness direction of the light-diffusing element, and multiple expansions cannot be obtained. As a result, there is light diffusion. The shape of the light diffusing fine particles may be any suitable shape depending on the purpose. Specific examples thereof include a spherical shape, a scaly shape, a plate shape, an elliptical shape, and an amorphous shape. In many cases, spherical spherical particles may be used as the light diffusing fine particles. The refractive index of the light diffusing fine particles is preferably 〖. 〜 丨 7 〇, more preferably 1 · 40 〜 1 · 60 〇 relative to The amount of the light diffusing fine particles in the coating liquid is preferably from 10 parts by weight to 100 parts by weight, more preferably from 15 parts by weight to 40 parts by weight, based on the weight of the substrate. The light diffusing fine particles having an average particle diameter of the above preferred range can obtain a light diffusing element having excellent light diffusibility. Α_1-4. The overall composition of the coating liquid is used as the above volatile solvent. Any suitable solvent can be used as long as the above components can be dissolved or uniformly dispersed. Specific examples of the volatile solvent include ethyl acetate, butyl acetate, and isopropyl acetate '2-butanone (A 147072). .doc -14- 201042294 base ethyl ketone), mercaptoisobutyl ketone, cyclopentanyl, acetophenone, isopropanol, n-butanol, cyclopentane, water. The above coating liquid can be further contained according to the purpose For example, in the case of using the above ultrafine particle component, a dispersing agent can be suitably used in order to disperse the ultrafine particle component well. Examples of other specific examples of the additive include an anti-aging agent, a modifier, and an interface. Active agent, anti-tarnishing agent, ultraviolet absorber, leveling agent, antifoaming agent. The solid content concentration of the coating liquid can be adjusted.

。/〇〜70重量%左右為宜。只要為如此之固體成分濃度便可 獲得具有容易塗敷之黏度之塗敷液。 Α-2.步驟Β 作為於步驟Β中使上述前驅物之至少一部分滲透至上述 光擴散性微粒之内部之方法,具代表性的可列舉將上述塗 敷液靜置之方法。樹脂成分與光擴散性微粒宜包含同系之 材料,更佳為包含相溶性高之材料,因此藉由將塗敷液靜 置即使不進行特殊之處理或操作,樹脂成分之前驅物 (单旬亦會渗透至光擴散性微粒之㈣。即,藉由使樹脂 =之前驅物與光擴散性微粒接觸特定時間,樹脂成分之 叫驅物會滲透至光擴散性微粒之内部。靜置時間宜為較光 擴散性微粒之粒經實質上遠到畏…:’宜為較先 貝質上達到最大為止之時間更長之時 :广所謂「光擴散性微粒之粒徑實質上達到最大為 、去φ、隹止係心直至光擴散性微粒膨潤至最大限度而無 稱作最大膨潤時間間(以下,亦 藉由使樹脂成分之前驅物與光擴散 147072.doc 15 201042294 性微粒經過較最大膨潤時間更長之時間接觸,樹骑成分前 驅物對光擴散性微粒之滲透會達到飽和狀態,而無法更進 一步進入至光擴散性微粒内部之交聯結構。其結果為,藉 由下述聚合步驟]良好且穩定地於光擴散性:教:表: 附近内部形成濃度調變區域。最大膨潤時間可根據樹脂成 分與光擴散性微粒之相溶性而發生變化。因此,靜置時間 可根據樹脂成分及光擴散性微粒之構成材料而變化。例 如,靜置時間宜為1小時〜48小時,更佳為2小時〜4〇小時, 進而更佳為3小時〜3 5小時,特佳為4小時〜3 〇小時。若靜置 %間未達1小時,則存在前驅物未充分地滲透至光擴散性 微粒内部之情形,其結果為,存在不會良好地形成濃度調 變區域之情形。若靜置時間超過48小時,則有可能因光擴 散性微粒間之物理性相互作用,而導致光擴散性微粒凝 I 塗敷液之黏度升南’塗敷性變得不充分。靜置可於室 皿下進行’亦可於根據目的或使用材料所設定之特定溫度 條件下進行。 於步驟B中,上述前驅物只要自上述光擴散性微粒之表 面參透至該光擴散性微粒之一部分即可,例如宜滲透至上 述光擴散性微粒之平均粒徑之10%〜95%之範圍為止。於滲 透範圍未達1 〇%之情形時,存在不會良好地形成濃度調變 區域而無法充分降低背向散射之情形。即使滲透範圍超過 95% ’亦與滲透範圍較小之情形時同樣,存在不會良好地 形成濃度調變區域而無法充分降低背向散射之情形。滲透 範圍可藉由調整樹脂成分及光擴散性微粒之材料、光擴散 147072.doc -16- 201042294 性微粒之交聯密度、靜置時間、靜置溫度等而加以控制。 於本發明中,重要的是控制上述前驅物向光擴散性微粒 之滲透。例如,如圖3所示,於製備上述塗敷液後隨即將 該塗敷液塗佈於基材上而形成光擴散元件之情形時,擴散 半值角會根據乾燥溫度而大幅變化。另一方面,於將上述 塗敷液靜置例如24小時後塗佈於基材上而形成光擴散元件 之情形時,擴散半值角會不受乾燥溫度之影響而大致固 〇 定。可認為其原因在於,藉由靜置,前'驅物會向光擴散性 微粒滲透至飽和狀態為止,因此濃度調變區域之形成不受 乾燥溫度之影響。因此,如上所述,靜置時間宜為較最大 膨潤時間更長之時間。藉由如此設定靜置時間,可獲得不 受乾燥時間之影響而大致固定且良好之擴散半值角,因此 可無偏差地穩定地製造擴散性高之光擴散元件。此外,例 如可藉由6(TC之低溫乾燥進行製造,因此自安全性或成本 方面而言亦較佳。另一方面,只要可根據前驅物及光擴散 〇 性微粒之種類決定直至滲透達到飽和狀態為止之時間,即 使縮短靜置時間,亦可藉由適當地選擇乾燥溫度,而無偏 差地穩定地製造擴散性高之光擴散元件。例如,即使於製 備上述塗敷液後隨即將該塗敷液塗佈於基材上而形成光擴 散元件之情形時,亦可藉由將乾燥溫度設定為1〇〇七,使 月,j驅物參透至光擴散性微粒内部而形成濃度調變區域,從 而無偏差地穩定製造擴散性高之光擴散元件。 A-3·步驟c 具代表性的是,於步驟C(使前驅物發生聚合之步驟)之 147072.doc -17- 201042294 前,將上述塗敷液塗佈於基材。作為基材,只要可獲得本 發明之效果’便可採用任意適當之膜。作為具體例,可列 舉三乙醯纖維素(TAC,triacetyl celiui〇se)膜、聚對苯二甲 酸乙二醇酯(PET,polyethylene terephthalate)膜、聚丙烯 (PP,polypropylene)膜、尼龍膜、丙烯酸膜、内酯改質丙 烯酸膜等。上述基材亦可根據需要而進行易接著處理等夺 面改質,且亦可包含潤滑劑、抗靜電劑、紫外線吸收劑^ 添加劑。該基材於下述附光擴散元件之偏光板中,存在可 作為保護層而發揮作用之情形。 作為向基材塗佈上述塗敷液之塗佈方法,可採用使用有 任意適當之塗佈機之方法。作為塗佈機之具體例,可列舉 棒式塗佈機、反向塗佈機、吻合式塗佈機、凹板塗佈機、 模塗機、刮刀式塗佈機。 其次,使上述前驅物發生聚合。聚合方法可根據樹脂成 分(因而其前驅物)之種類而採用任意適當之方法。例如, 於樹脂成分為電離放射線硬化型樹脂之情形時,藉由照射 電離放射線而使前驅物發生聚合。於使用紫外線作為電離 放射線之情形時’其累計光量宜為200 mJ〜400 mJ。電離 放射線相對於光擴散性微粒之穿透率宜為70%以上,更佳 為80%以上。又,例如於樹脂成分為熱固型樹脂之情形 時’藉由加熱而使前驅物發生聚合。加熱溫度及加熱時間 可根據樹脂成分之種類而適當地設定。聚合宜藉由照射電 離放射線而進行。只要係電離放射線照射,便可於良好地 保持折射率分布結構(濃度調變區域)之狀態下使塗膜硬 147072.doc -18- 201042294 化’因此可製作擴散特性良好之光擴散元件。藉由使前驅 物發生聚合’而形成基質,並同時於光擴散性微粒之表面 附近内部形成》辰度調變區域。更詳細而言,濃度調變區域 係藉由已滲透至光擴散性微粒之内部之前驅物進行聚合而 形成;基質係藉由未滲透至光擴散性微粒之前驅物進行聚 合而形成。即,根據本實施形態之製造方法,藉由使已滲 透至光擴散性微粒内部之前驅物及未滲透至光擴散性微粒. / 〇 ~ 70% by weight or so is appropriate. As long as such a solid component concentration is obtained, a coating liquid having an easily applied viscosity can be obtained. Α-2. Step Β As a method of allowing at least a part of the precursor to permeate into the inside of the light diffusing fine particles in the step, a method of allowing the coating liquid to stand is exemplified. The resin component and the light diffusing fine particles preferably contain the same material, and more preferably contain a material having high compatibility. Therefore, the resin component is preliminarily discharged by leaving the coating liquid without special treatment or operation. It will penetrate into the light diffusing particles (4). That is, by bringing the resin = precursor to the light diffusing particles for a specific time, the resin component will penetrate into the light diffusing particles. The standing time should be The particles of the light diffusing particles are substantially far from the fear...: 'It should be longer when the first shellfish is maximized: the so-called "the size of the light diffusing particles is substantially the largest, go φ, stop the core until the light diffusing particles swell to the maximum without being called the maximum swelling time (hereinafter, also by making the resin component precursor and light diffusion 147072.doc 15 201042294 When it is contacted for a longer period of time, the penetration of the light-diffusing particles by the tree-ride component precursor will reach a saturated state, and it will not be able to further enter the cross-linked structure inside the light-diffusing particles. In order to achieve good and stable light diffusibility by the following polymerization step: a concentration modulation region is formed in the vicinity of the polymerization step. The maximum swelling time may vary depending on the compatibility of the resin component and the light diffusing fine particles. The standing time may vary depending on the constituent materials of the resin component and the light diffusing fine particles. For example, the standing time is preferably from 1 hour to 48 hours, more preferably from 2 hours to 4 hours, and still more preferably from 3 hours to 3 hours. 5 hours, particularly preferably 4 hours to 3 hours. If the amount of standing is less than 1 hour, there is a case where the precursor does not sufficiently penetrate into the inside of the light diffusing fine particles, and as a result, the formation does not form well. In the case of a concentration-modulated region, if the standing time exceeds 48 hours, there may be a physical interaction between the light-diffusing particles, and the viscosity of the light-diffusing microparticles can be increased. Insufficient. The standing can be carried out under the chamber. It can also be carried out under the specific temperature conditions set according to the purpose or the material used. In the step B, the precursor is only from the surface of the light diffusing particles. It is sufficient to penetrate into one part of the light diffusing fine particles, for example, preferably to the range of 10% to 95% of the average particle diameter of the light diffusing fine particles. When the penetration range is less than 1%, there is no possibility. The concentration modulation region is formed well and the backscattering cannot be sufficiently reduced. Even if the penetration range exceeds 95% ', as in the case where the penetration range is small, the concentration modulation region is not formed well and the back cannot be sufficiently lowered. In the case of scatter, the penetration range can be controlled by adjusting the resin composition and the material of the light diffusing fine particles, the crosslinking density of the light diffusion, the standing time, the standing temperature, and the like. In the present invention, it is important to control the penetration of the precursor into the light diffusing fine particles. For example, as shown in FIG. 3, after the preparation of the coating liquid, the coating liquid is applied to the substrate to form light diffusion. In the case of components, the diffuse half-value angle varies greatly depending on the drying temperature. On the other hand, when the coating liquid is allowed to stand for 24 hours and then applied to a substrate to form a light diffusing element, the diffusion half angle is substantially fixed without being affected by the drying temperature. The reason for this is considered to be that the precursor is driven to the state in which the light-diffusing particles penetrate to the saturated state by standing, so that the formation of the concentration-modulating region is not affected by the drying temperature. Therefore, as described above, the rest time should be longer than the maximum swelling time. By setting the standing time in this manner, it is possible to obtain a substantially fixed and good diffusion half-value angle without being affected by the drying time, and therefore it is possible to stably manufacture a light diffusing element having high diffusibility without any deviation. Further, for example, it can be produced by low temperature drying of 6 (TC), and therefore it is preferable in terms of safety or cost. On the other hand, it can be determined according to the type of precursor and light-diffusing smear particles until the penetration reaches saturation. In the time until the state, even if the standing time is shortened, the light diffusing element having high diffusibility can be stably produced without any deviation by appropriately selecting the drying temperature. For example, even after the preparation of the above coating liquid, the coating liquid is applied. When the light diffusing element is formed on the substrate, the drying temperature can be set to 1〇〇7, so that the Moon and the J are penetrated into the light diffusing fine particles to form a concentration modulation region. The light diffusing element having high diffusibility is stably produced without deviation. A-3·Step c Typically, the above coating liquid is applied before step 147 (the step of polymerizing the precursor) 147072.doc -17- 201042294 It can be applied to a substrate. Any suitable film can be used as the substrate as long as the effect of the present invention can be obtained. Specific examples thereof include triacetyl cellulose (TAC, triacetyl celiui). Se) film, polyethylene terephthalate (PET) film, polypropylene (PP) film, nylon film, acrylic film, lactone modified acrylic film, etc. If necessary, it is easy to carry out the treatment, such as surface modification, and may also include a lubricant, an antistatic agent, and an ultraviolet absorber. The substrate may be used as a protective layer in the polarizing plate with the light diffusing element described below. In the case of applying the coating liquid to the substrate, any suitable coating machine can be used. Specific examples of the coating machine include a bar coater and a counter. To the coater, the coater, the gravure coater, the die coater, and the knife coater. Next, the precursor is polymerized. The polymerization method can be based on the type of the resin component (and thus its precursor). In any case, when the resin component is an ionizing radiation-curable resin, the precursor is polymerized by irradiation with ionizing radiation. Ultraviolet rays are used as ionizing radiation. In the case of the line, the cumulative light amount is preferably 200 mJ to 400 mJ. The penetration rate of the ionizing radiation with respect to the light diffusing fine particles is preferably 70% or more, more preferably 80% or more. Further, for example, the resin component is thermosetting. In the case of a resin, the precursor is polymerized by heating. The heating temperature and the heating time can be appropriately set depending on the type of the resin component. The polymerization is preferably carried out by irradiating the ionizing radiation. When the refractive index distribution structure (concentration modulation region) is well maintained, the coating film is hardened 147072.doc -18- 201042294. Therefore, a light diffusion element having good diffusion characteristics can be produced. By polymerizing the precursor The matrix is formed, and at the same time, a "Zhangdu modulation region" is formed inside the surface of the light diffusing fine particles. More specifically, the concentration modulation region is formed by polymerization of a precursor which has penetrated into the light diffusing fine particles; the matrix is formed by polymerization without being infiltrated into the light diffusing fine particles. That is, according to the production method of the present embodiment, the precursor which has penetrated into the inside of the light diffusing fine particles and which does not penetrate into the light diffusing fine particles

之前驅物同時發生聚合,可於光擴散性微粒之表面附近内 部形成濃度調變區域,並同時形成基質。於一實施形態 中,可進而於光擴散性微粒與基質之界面附近(光擴散性 微粒之周邊部)形成有其他濃度調變區域。其他濃度調變 區域主要係因樹脂成分、超微粒成分及光擴散性微粒之相 溶性而形成。 本發明之光擴散元件之製造方法除包含上述步驟A〜步驟 C以外,當然亦可於任意適當之時間點包含任意適當之步 驟、處理及/或操作。如此之步驟等之種類及進行如此之 步驟等之時間點可根據目的而適當地設定。例如,本發明 之光擴散7G件之製造方法可根據需要而進*包含將塗佈於 基材上之塗敷液加以乾焊 ,^ ^ ^ ^ 、 ▲ 屎之步驟。如Λ之乾燥例如可於聚 ”驟之則進行,亦可於聚合步驟之後進行。 作敷液之乾燥方法’可採用任意適當之方法。 作為具體例,可列|白缺、 …'乾燥、加熱乾燥 '減壓乾焊。 加熱乾燥為宜。加埶溫斧主 。 ’、 …伽·度為例如60 (:〜1 50。(:,加埶日本R卷 例如30秒〜5分鐘。 …、夺間為 147072.doc -19· 201042294 以上述方式於基材上形成光擴散元件。所獲得之光擴散 凡件可自基材剝離而用作單一構件,亦可用作附基材之光 擴散70件,亦可自基材轉印於偏光板等而用作複合構件 (例如附光擴散元件之偏光板),亦可連同基材一起貼附於 偏光板等而用作複合構件(例如附光擴散元件之偏光板)。 於連同基材一起貼附於偏光板等而用作複合構件(例如附 光擴散几件之偏光板)之情形時,該基材可作為偏光板之 保護層而發揮作用。 Β.光擴散元件 本發明之光擴散元件可藉由上述A-1項〜Α_3項所記載之 方法而獲得。本發明之光擴散元件含有包含樹脂成分及超 微粒成分之基質、以及分散於該基質中之光擴散性微粒。 本發明之光擴散元件係藉由基質與光擴散性微粒之折射率 差而體現光擴散功能。圖丨係用以說明藉由本發明之較佳 實施形態之製造方法而獲得之光擴散元件中的基質之樹脂 成分及光擴散性微粒之分散狀態的模式圖。本發明之光擴 散元件100包括含有樹脂成分U及超微粒成分12之基質 10、以及分散於基質1〇中之光擴散性微粒2〇。基質之樹脂 成分及光擴散性微粒之折射率宜滿足下述式(丨): 〇&lt; | nP-nA | · . · (1)。 上述超微粒成分之折射率滿足下述式(2): 〇&lt; | np-nA | &lt; | nP-nB | · · . (2)。 使用具有上述式(1)之關係之基質之樹脂成分及光擴散性 微粒、以及使用具有上述式(2)之關係之超微粒成分,藉 147072.doc •20· 201042294 此可獲得既維持著較高之霧度又抑制背向散射之光擴散元 件。 本發明之光擴散元件中,於光擴散性微粒20之表面附近 内部形成有濃度調變區域30。如上述A-1項〜A-3項中所說 明般,濃度調變區域30係藉由樹脂成分11之前驅物(單體) 滲透至光擴散性微粒20内部後發生聚合而形成。於一實施 形態中’於濃度調變區域30内,樹脂成分11之重量濃度實 0 質上為固定。於另一實施形態中,於濃度調變區域3〇内, 樹脂成分11之重量濃度係隨著自光擴散性微粒2〇之表面遠 離(即’隨著朝向光擴散性微粒20之中心)而降低。濃度調 變區域30宜形成於光擴散性微粒2〇之内部,只要如此便可 發揮其效果。例如,濃度調變區域形成於自光擴散性微粒 20之表面至該光擴散性微粒之平均粒徑之丨〇%〜95%之範 圍。濃度調變區域30之厚度(自光擴散性微粒表面至濃度 調變區域最内部為止之距離)既可為固定,亦可根據光擴 Q 散性微粒表面之位置而不同。濃度調變區域30之厚度宜為 100 nm〜4 μπι,更佳為1〇〇 nm〜2 μιη。樹脂成分滲透而 形成濃度調變區域30’藉此可獲得以下效果:(〗)可於光擴 散微粒與基質之界面附近,使折射率階段性地或實質上連 續性地變化(參照圖2(a))。另一方面,於先前之光擴散元 件中’則未形成此種濃度調變區域,微粒與基質之界面明 顯,因此折射率係自微粒之折射率間斷地變化至基質之折 射率(參照圖2(b))。如圖2(a)所示,形成濃度調變區域3〇而 使付於基質1 〇與光擴散性微粒2 〇之界面附近折射率階段性 147072.doc -21- 201042294 地或實質上連續性地變化’藉此即使擴大基㈣與光擴散 性元件20之折射率差,亦可抑制基質與光擴散性微粒之界 面之反射’從而可抑制背向散射。另-方面,&gt; 圖2⑻所 不,根據先前之光擴散元件,當欲藉由擴大折射率差而賦 予較強之擴散性(齡g Φ ώ + 月又r I钗阿之霧度值)時,無法消除界面上之折 射率之差距。其結果為,因界面反射所致之背向散射變 大:⑺於主要因超微粒成分而形成其他濃度調變區域之情 形日寸’可促進其形成;(3)藉由樹脂成分⑴參透至光擴散性 微粒20内部’而與未渗透之情料相比,基質1G巾之樹脂 成刀11之/辰度降低。其結果為,超微粒成分ι2之折射率對 基質整體之折射率之幫助變大,因此於超微粒成分之折射 率較大之情形時,基質整體之折射率增大(反之,於超微 粒成分之折射率較小之情形時,基質整體之折射率變 小),基質與光擴散性微粒之折射率差進一步增大。因 此,與樹脂成分未滲透之情形時相比,可實現更高之擴散 性(霧度值)。 如上述A-1項〜A_3項中所說明般’上述濃度調變區域係 可藉由適當地選擇基質之樹脂成分及光擴散性微粒之構成 材料、以及化學及熱力學特性而形成。例如,由同系材料 中相溶性較高之材料一族構成樹脂成分及光擴散性微粒, 藉此可良好地形成濃度調變區域。濃度調變區域之厚度及 濃度梯度可藉由調整基質之樹脂成分及光擴散性微粒之化 學及熱力學特性而加以控制。 根據上述樹脂成分及上述光擴散性微粒之種類而適當地 147072.doc -22- 201042294 選擇上述超微粒成分’藉此可於基質10與光擴散性微粒2〇 之界面附近(光擴散性微粒之周邊部)進而形成其他濃度調 變區域(未圖示)。例如,由同系之材料(例如有機化合物一 族)構成樹脂成分及光擴散性微粒’且由與樹脂成分及光 擴散性微粒為不同系之材料(例如無機化合物)構成超微粒 成分’藉此可良好地形成其他濃度調變區域。更詳細而 言,關於上述樹脂成分,與局部性地於光擴散性微粒之附 〇 近與超微粒成分均勻溶解或者分散之狀態相比,僅由樹脂 成分包圍光擴散性微粒,會使整個系之能量穩定。其結果 為,樹脂成分之重量濃度於最接近光擴散性微粒之區域 中,高於基質整體中之樹脂成分之平均重量濃度,且隨著 自光擴散性微粒遠離而降低。因此,可形成其他濃度調變 區域。 於上述其他濃度調變區域中,隨著自光擴散性微粒20遠 離,樹脂成分11之重量濃度降低,且超微粒成分之重量濃 〇 度變高。換言之,於其他濃度調變區域内之最接近光擴散 性微粒20之區域中,超微粒成分係以相對較低之濃度分 散,且超微粒成分之濃度隨著自光擴散性微粒20遠離而增 大=如,於其他濃度調變區域中之最接近光擴散性微粒 20之區域中,樹脂成分之重量濃度高於基質整體中之樹脂 成分之平均重量濃度,且超微粒成分之重量濃度低於基質 f體中之超微粒成分之平均重量濃度。另_方面,於其他 /辰度調變區域中之自光擴散性微粒算起最遠區域中,樹 月曰成刀之重量濃度等於或有時低於基質整體中之樹脂成分 147072.doc -23- 201042294 之平均重量濃度’超微粒成分之重量濃度等於或有時高於 基質整體中之超微粒成分之平均重量濃度。藉由將如此之 其他濃度調變區域亦形成於光擴散微粒之外部,可增大上 述折射率呈階段性地或實f上連續性地變化之區域(即, 可自光擴散性微粒内側之濃度調變區域至光擴散性微粒外 側之其他濃度調變區域為止,使折射率階段性地或實質上 連續性地變化)。其結果為,與僅在光擴散性微粒内部形 成濃度調變區域之情形時相比,可進—步抑制背向散射。 此外,於其他濃度調變區域之外側,折射率與光擴散性微 粒20之折射率相差較大之超微粒成分的重量濃度相對地變 尚,因此可擴大基質1〇與光擴散性微粒2〇之折射率差。其 結果為,即使為薄膜,亦可實現較高之霧度(較強之擴散 性)。如此之特徵特別適用於如準直背光前面擴散系統中 所使用之光擴散元件般要求較強之擴散性(霧度為9〇%以 上)之用途。 上述其他濃度調變區域之厚度(自光擴散性微粒表面至 其他濃度調變區域末端為止之距離)既可為固定(即,其他 濃度調變區域亦可於光擴散性微粒之周圍呈同心球狀擴 展)’亦可根據光擴散性微粒表面之位置而使厚度不同(例 如亦可成為如糖果之外部輪廓形狀其他濃度調變區域 之厚度宜根據光擴散性微粒表面之位置而不同。只要為此 種構成’便可於基質10與光擴散性微粒20之界面附近使折 射率連續性地變化。只要以充分之厚度形成其他濃度調變 區域’便可於光擴散性微粒之周邊部使折射率更平滑地連 147072.doc -24· 201042294 續性地變化,從而可非常有效地抑制背向散射。另一方 面,若厚度過大,則存在其他濃度調變區域甚至佔用本來 光擴散性微粒應存在之區域,而無法獲得充分之光擴散性 (例如霧度值)的情形。因此’其他濃度調變區域之厚度宜 為H&gt;nm〜5〇〇nm,更佳為2〇nm〜4〇〇nm,進而更佳為3〇 ⑽〜300 nm。又,其他濃度調變區域之厚度相對於光擴散 性微粒之平均粒徑宜為i G%〜5G% ’更佳為·〜桃。 Ο 上述光擴散元件之霧度越高越好,具體而言,宜為 9〇〜99%,更佳為92〜99%,進而更佳為心㈣,特佳為 97〜99%。藉由霧度為9〇%以上,可較佳地用作準直背光前 面擴散系統之前面光擴散元件。再者,所謂準直背光前面 擴散系統’係指於液晶顯示裝置中使用準直背光光(向固 定方向聚光且亮度半值寬較窄之背光光),且於上側偏光 板之視認側設有前面光擴散元件之系統。The precursor is simultaneously polymerized, and a concentration-modulating region is formed inside the surface of the light-diffusing fine particles, and a matrix is simultaneously formed. In one embodiment, another concentration modulation region may be formed in the vicinity of the interface between the light diffusing fine particles and the substrate (the peripheral portion of the light diffusing fine particles). The other concentration-modulating regions are mainly formed by the compatibility of the resin component, the ultrafine particle component, and the light diffusing fine particles. The method for producing the light diffusing element of the present invention may of course include any suitable steps, processes and/or operations at any suitable point in time, in addition to the above steps A to C. The types of such steps and the like, and the timing at which such steps are performed, etc., can be appropriately set depending on the purpose. For example, the method for producing a light-diffusing 7G member of the present invention may include, as needed, a step of dry-welding a coating liquid applied to a substrate, ^ ^ ^ ^, ▲ 屎. For example, the drying of the crucible can be carried out, for example, in the case of polymerization, or after the polymerization step. The drying method of the coating liquid can be carried out by any appropriate method. As a specific example, it can be listed as white, ... Heating and drying 'decompression dry welding. Heating and drying is appropriate. Add 埶 warm axe main. ', ... gamma degrees for example 60 (: ~ 1 50. (:, crowned Japanese R roll for example 30 seconds ~ 5 minutes. ... 147072.doc -19· 201042294 The light diffusing element is formed on the substrate in the above manner. The obtained light diffusing member can be peeled off from the substrate and used as a single member, and can also be used as a substrate-attached light. 70 pieces may be used as a composite member (for example, a polarizing plate with a light diffusing element) by transferring a substrate to a polarizing plate or the like, or may be attached to a polarizing plate or the like together with a substrate to be used as a composite member (for example, a polarizing plate with a light diffusing element). When used as a composite member (for example, a polarizing plate with a light diffusing member) together with a substrate and attached to a polarizing plate, the substrate can be used as a protective layer of a polarizing plate. And play a role. Β. Light diffusing element The light diffusion of the present invention The material can be obtained by the method described in the above items A-1 to Α3. The light diffusing element of the present invention contains a matrix containing a resin component and an ultrafine particle component, and light diffusing fine particles dispersed in the matrix. The light diffusing element exhibits a light diffusing function by a difference in refractive index between the substrate and the light diffusing fine particles. The figure is used to explain the matrix in the light diffusing element obtained by the manufacturing method of the preferred embodiment of the present invention. A schematic diagram of a state in which the resin component and the light diffusing fine particles are dispersed. The light diffusing element 100 of the present invention includes a matrix 10 containing a resin component U and an ultrafine particle component 12, and light diffusing fine particles 2〇 dispersed in the matrix 1〇. The refractive index of the resin component and the light diffusing fine particles of the matrix preferably satisfy the following formula (丨): 〇 &lt; | nP-nA | · (1) The refractive index of the above ultrafine particle component satisfies the following formula (2) 〇 lt | | 树脂 树脂 树脂 树脂 树脂 树脂 树脂Ultrafine particle composition Borrowing 147072.doc • 20· 201042294 It is possible to obtain a light diffusing element which maintains a high haze and suppresses backscattering. In the light diffusing element of the present invention, a concentration is formed inside the surface of the light diffusing fine particle 20 The modulation region 30. As described in the above items A-1 to A-3, the concentration modulation region 30 is polymerized by the resin component 11 precursor (monomer) permeating into the interior of the light diffusing fine particles 20 In one embodiment, the weight concentration of the resin component 11 is fixed in the concentration-modulating region 30. In another embodiment, in the concentration-modulating region 3, the resin component 11 is The weight concentration decreases as it goes away from the surface of the light diffusing fine particles 2 (i.e., 'as it goes toward the center of the light diffusing fine particles 20). The concentration modulation region 30 is preferably formed inside the light diffusing fine particles 2, and as such, the effect can be exerted. For example, the concentration modulation region is formed in a range from 丨〇% to 95% of the average particle diameter of the light diffusing fine particles 20 to the light diffusing fine particles. The thickness of the concentration-modulating region 30 (the distance from the surface of the light-diffusing particle to the innermost portion of the concentration-modulating region) may be fixed or different depending on the position of the surface of the diffusing particle. The thickness of the concentration modulation region 30 is preferably 100 nm to 4 μm, more preferably 1 nm to 2 μm. The resin component is infiltrated to form the concentration-modulating region 30', whereby the following effects can be obtained: ()) the refractive index can be changed stepwise or substantially continuously in the vicinity of the interface between the light-diffusing particles and the substrate (refer to FIG. 2 (refer to FIG. 2 a)). On the other hand, in the prior light diffusing element, the concentration modulation region is not formed, and the interface between the particles and the substrate is obvious, so the refractive index changes intermittently from the refractive index of the particles to the refractive index of the matrix (refer to FIG. 2). (b)). As shown in Fig. 2(a), the concentration modulation region 3〇 is formed so as to be near the interface between the substrate 1 〇 and the light diffusing fine particles 2 折射率 refractive index phase 147072.doc -21 - 201042294 or substantially continuous The ground change "by this, even if the refractive index difference between the base (4) and the light diffusing element 20 is increased, the reflection at the interface between the substrate and the light diffusing fine particles can be suppressed, and backscattering can be suppressed. On the other hand, Fig. 2 (8) does not, according to the previous light diffusing element, when it is intended to impart a strong diffusibility by expanding the refractive index difference (age g Φ ώ + month and r I 钗 haze value) When it is impossible to eliminate the difference in refractive index on the interface. As a result, the backscattering due to interface reflection becomes large: (7) the formation of other concentration-modulating regions mainly due to the ultrafine particle component can promote the formation thereof; (3) the resin component (1) is penetrated to The inside of the light diffusing fine particles 20 is lower than that of the non-infiltrated material, and the resin 1 of the base 1G towel is reduced. As a result, the refractive index of the ultrafine particle component ι2 contributes to the refractive index of the entire matrix. Therefore, when the refractive index of the ultrafine particle component is large, the refractive index of the entire matrix increases (instead, in the ultrafine particle component). When the refractive index is small, the refractive index of the entire matrix becomes small, and the difference in refractive index between the matrix and the light diffusing fine particles is further increased. Therefore, higher diffusibility (haze value) can be achieved as compared with the case where the resin component is not permeable. As described in the above items A-1 to A_3, the concentration modulation region can be formed by appropriately selecting a constituent material of the resin component and the light diffusing fine particles of the matrix, and chemical and thermodynamic properties. For example, a resin component and light diffusing fine particles are composed of a material having a high compatibility in a homologous material, whereby a concentration-modulated region can be favorably formed. The thickness and concentration gradient of the concentration modulation region can be controlled by adjusting the chemical composition and thermodynamic properties of the resin component of the matrix and the light diffusing particles. According to the type of the resin component and the light diffusing fine particles described above, 147072.doc -22- 201042294 is appropriately selected to be in the vicinity of the interface between the substrate 10 and the light diffusing fine particles 2 (light diffusing fine particles) The peripheral portion further forms another concentration modulation region (not shown). For example, a resin component and a light-diffusing fine particle ' are composed of a material of the same type (for example, an organic compound), and a fine particle component is formed of a material (for example, an inorganic compound) different from the resin component and the light diffusing fine particle. The ground forms other concentration modulation regions. More specifically, the resin component is partially surrounded by the light diffusing fine particles, and the light diffusing fine particles are uniformly dissolved or dispersed in the vicinity of the light diffusing fine particles. The energy is stable. As a result, the weight concentration of the resin component is higher in the region closest to the light diffusing fine particles than the average weight concentration of the resin component in the entire matrix, and decreases as the light diffusing fine particles are separated. Therefore, other concentration modulation regions can be formed. In the other concentration-modulating region described above, as the light-diffusing fine particles 20 are distant from each other, the weight concentration of the resin component 11 is lowered, and the weight concentration of the ultrafine particle component is increased. In other words, in the region closest to the light diffusing fine particles 20 in the other concentration modulation region, the ultrafine particle component is dispersed at a relatively low concentration, and the concentration of the ultrafine particle component increases as it is distant from the light diffusing fine particle 20. Large = For example, in the region of the other concentration-modulating region closest to the light diffusing fine particles 20, the weight concentration of the resin component is higher than the average weight concentration of the resin component in the entire matrix, and the weight concentration of the ultrafine particle component is lower than The average weight concentration of the ultrafine particle components in the matrix f body. On the other hand, in the farthest region from the light diffusing particles in the other/length modulation region, the weight concentration of the tree is equal to or sometimes lower than the resin composition in the matrix as a whole 147072.doc - 23-201042294 Average Weight Concentration 'The weight concentration of the ultrafine particle component is equal to or sometimes higher than the average weight concentration of the ultrafine particle component in the bulk of the matrix. By forming such other concentration-modulating regions also outside the light-diffusing particles, it is possible to increase the region in which the refractive index changes continuously in a stepwise or real-f (ie, from the inside of the light-diffusing particles) The concentration modulation region is changed to the other concentration modulation region outside the light diffusing fine particles, and the refractive index is changed stepwise or substantially continuously). As a result, the backscattering can be further suppressed as compared with the case where the concentration modulation region is formed only inside the light diffusing fine particles. Further, on the outer side of the other concentration modulation region, the weight concentration of the ultrafine particle component having a large difference in refractive index from the refractive index of the light diffusing fine particle 20 is relatively large, so that the matrix 1〇 and the light diffusing fine particle 2〇 can be enlarged. The difference in refractive index. As a result, even if it is a film, a high haze (strong diffusibility) can be achieved. Such a feature is particularly suitable for use in applications such as a light diffusing element used in a collimated backlight front diffusing system which requires a relatively high diffusibility (haze of 9 % or more). The thickness of the other concentration modulation region (the distance from the surface of the light diffusing particle to the end of the other concentration modulation region) may be fixed (that is, other concentration modulation regions may also be concentric around the light diffusing particles). The shape may be different depending on the position of the surface of the light diffusing fine particles (for example, the thickness of the outer contour such as the outer contour of the candy may be different depending on the position of the surface of the light diffusing fine particle. In such a configuration, the refractive index can be continuously changed in the vicinity of the interface between the substrate 10 and the light-diffusing fine particles 20. As long as the other concentration-modulated regions are formed in a sufficient thickness, the refractive index can be refracted in the peripheral portion of the light-diffusing particles. The rate is more smoothly connected with 147072.doc -24· 201042294, which can change the backscattering very effectively. On the other hand, if the thickness is too large, there are other concentration-modulating regions and even occupying the light diffusing particles. The area where it exists, and sufficient light diffusivity (such as haze value) cannot be obtained. Therefore, the thickness of other concentration-modulated areas It is H>nm~5〇〇nm, more preferably 2〇nm~4〇〇nm, and even more preferably 3〇(10)~300 nm. Moreover, the thickness of other concentration modulation regions is relative to the average of light diffusing particles. The particle size is preferably i G%~5G% 'better than · peach. Ο The higher the haze of the above light diffusing element, the better, specifically, 9 〇 to 99%, more preferably 92 to 99%. Further better for the heart (four), particularly preferably 97 to 99%. With a haze of 9% or more, it can be preferably used as a front light diffusing element in front of the collimated backlight front diffusing system. Further, the so-called collimated backlight The front diffusion system refers to a system in which a collimated backlight (a backlight that is concentrated in a fixed direction and has a narrow half-value width) is used in a liquid crystal display device, and a front light diffusing element is provided on the viewing side of the upper polarizing plate. .

上述光擴散元件之擴散特性若以光擴散半值角表示, 宜為10。~150。(單側5。〜75。),更佳為1〇。〜1〇〇。(單 5°〜50°),進而更佳為3〇。〜8〇。(單側15。〜4〇〇)。 則 側 上述光擴散元件之職可根據目的或所期望之擴散特性 而適當地設定。具體而言,上述光擴散元件之厚度宜為4 μηι〜50 μηι,更佳為4 μιη〜20 μηι。根據本發明,儘管為如 此般非常薄之厚度’亦可獲得具有如上所述般非常高之霧 度之光擴散元件。 上述光擴散元件適合用於液晶顯示裝置之視認侧構件、 液晶顯示裝置之背光用構件、照明器具(例如有機 147072.doc -25· 201042294 EL(electroluminescence,電致發光)、led⑴咖 _出叩 發光二極體))用擴散構件,尤其適合用作準直背光 前面擴散系統之前面擴散元件。上述光擴散元件既可單獨 作為膜狀或板狀構件提供,亦可貼附於任意適當之基材或 偏光板而作為複合構件提供。又,亦可於光擴散元件上積 層抗反射層。 C.附光擴散元件之偏光板 C-1.附光擴散元件之偏光板之整體構成 本發明之附光擴散元件之偏光板之製造方法係使用上述 A-1項〜A-3項中所記載之本發明之光擴散元件之製造方法 而進行。藉由本發明之製造方法而獲得之附光擴散元件之 偏光板,具代表性的是配置於液晶顯示裝置之視認側。圖 4係本發明之較佳實施形態之附光擴散元件之偏光板的概 略剖面圖。該附光擴散元件之偏光板2〇〇包括光擴散元件 100以及偏光元件110。光擴散元件1〇〇係上述A1項〜A_3項 及B項中所記載之本發明之光擴散元件。光擴散元件1〇〇係 以於附光擴散元件之偏光板配置於液晶顯示裝置之視認側 之情形時成為最靠視認側之方式進行配置。於一實施形態 中,於光擴散元件100之視認側配置有低反射層或抗反射 處理層(antireflection處理層)(未圖示)。於圖示例中,附光 擴散元件之偏光板200係於偏光元件之兩側包括保護層12〇 及130。光擴散元件、偏光元件及保護層係經由任意適當 之接著劑層或黏著劑層而貼附。保護層12〇及130中之至少 一者亦可根據目的、偏光板之構成及液晶顯示裝置之構成 147072.doc •26- 201042294 而省略。例如,於形成光擴散元件時所使用之基材可作為 保護層而發揮作用之情形時,可省略保護層12〇。本發明 之附光擴散元件之偏光板尤其可適合用作採用有準直背光 前面擴散系統之液晶顯示裝置中之視認側偏光板。 C - 2.偏光元件 作為上述偏光元件110,可根據目的而採用任意適當之The diffusion characteristics of the light diffusing element are preferably 10 as indicated by a half value angle of light diffusion. ~150. (single side 5. ~ 75.), more preferably 1 〇. ~1〇〇. (single 5°~50°), and more preferably 3〇. ~8〇. (single side 15. ~ 4 〇〇). Then, the position of the light diffusing element described above can be appropriately set depending on the purpose or the desired diffusion characteristics. Specifically, the thickness of the light diffusing element is preferably 4 μηη to 50 μηι, more preferably 4 μηη to 20 μηι. According to the present invention, a light diffusing member having a very high haze as described above can be obtained although it is a very thin thickness as described above. The light diffusing element is suitably used for a viewing side member of a liquid crystal display device, a backlight member for a liquid crystal display device, and a lighting fixture (for example, organic 147072.doc -25·201042294 EL(electroluminescence), led(1) coffee_outlight emission Diode)) is a diffusion member that is particularly suitable for use as a front diffusing element in front of a collimated backlight front diffusing system. The light diffusing element may be provided as a film or a plate member alone, or may be attached to any appropriate substrate or polarizing plate as a composite member. Further, an antireflection layer may be laminated on the light diffusing element. C. Polarizing plate with light diffusing element C-1. Whole polarizing plate with light diffusing element The manufacturing method of the polarizing plate with light diffusing element of the present invention is the use of the above items A-1 to A-3. The method for producing a light diffusing element of the present invention is described. The polarizing plate with a light diffusing element obtained by the manufacturing method of the present invention is typically disposed on the viewing side of the liquid crystal display device. Fig. 4 is a schematic cross-sectional view showing a polarizing plate of a light diffusing element according to a preferred embodiment of the present invention. The polarizing plate 2 of the light diffusing element includes a light diffusing element 100 and a polarizing element 110. The light diffusing element 1 is the light diffusing element of the present invention described in the above items A1 to A_3 and B. The light diffusing element 1 is disposed so as to be the most visible side when the polarizing plate attached to the light diffusing element is disposed on the viewing side of the liquid crystal display device. In one embodiment, a low reflection layer or an antireflection treatment layer (antireflection treatment layer) (not shown) is disposed on the viewing side of the light diffusing element 100. In the illustrated example, the polarizing plate 200 with the light diffusing element is provided on both sides of the polarizing element including the protective layers 12 and 130. The light diffusing element, the polarizing element and the protective layer are attached via any suitable adhesive layer or adhesive layer. At least one of the protective layers 12A and 130 may be omitted depending on the purpose, the constitution of the polarizing plate, and the composition of the liquid crystal display device 147072.doc • 26- 201042294. For example, when the substrate used for forming the light diffusing element can function as a protective layer, the protective layer 12A can be omitted. The polarizing plate with light diffusing element of the present invention is particularly suitable for use as a viewing side polarizing plate in a liquid crystal display device using a collimated backlight front diffusing system. C - 2. Polarizing element As the above-mentioned polarizing element 110, any appropriate one may be adopted depending on the purpose.

偏光元件。例如可列舉〔使碘或二色性染料等二色性物質 吸附於聚乙烯醇系膜、部分縮甲醛化聚乙烯醇系膜、乙 烯-乙酸乙烯酉旨共聚物系、部分皂化膜等親水性冑分子膜並 加以單軸延伸而成者;%乙稀醇之脫水處理物或聚氣乙婦 之脫鹽酸處理物等多烯系配向膜等。此等之中,使硤等二 色性物質吸㈣聚乙婦醇系膜並加以單軸延伸而成之偏光 件之偏光二色比較高’故而尤佳。對於此等偏光元件之 厚度並無特別限定,通常為1〜80 μηι左右。 使碘吸附於聚乙烯醇系膜並加以單軸延伸而成之偏光元 牛例如可藉由將聚乙婦醇膜浸潰於破之水溶液中進行染 色二延伸至原長之3〜7倍來製作。亦可根據需要而包含 =或硫酸鋅、氯化辞等,亦可浸潰於埃化卸等之水溶液 :二卜,亦可根據需要而於染色之前將聚乙稀醇系膜浸 潰於水中進行水洗。 藉由對聚乙烯酵系膜進行 # Μ ^ ^ 尺洗不僅可清洗掉聚乙烯醇 糸膜表面之污垢或抗結 膨润而防止染色不均等具有因使聚乙賴膜 進行染色之後進行二:=效果。延伸可於卿 邊染色一邊延伸,又,亦可於 147072.doc •27- 201042294 延伸之後隨即利用碘進行染色。亦可於硼酸或碘化鉀等之 水溶液中或水浴中進行延伸。 C-3 ·保護層 上述保護層〗20及130係由可用作偏光板之保護層之任意 適田之膜所形成。作為成為該膜之主成分之材料的具體 例’可列舉三乙醯纖維素(TAC)等纖維素系樹脂;或聚酯 系聚乙烯醇系、聚碳酸酯系、聚醯胺系、聚醯亞胺系、 聚系m聚苯乙烯系、聚耗烯系、聚稀煙 系、(甲基)丙烯酸系、乙酸酯系等之透明樹脂等。又,亦 可列舉(甲基)丙稀酸系、氨醋系、(甲基)丙烯酸氨醋系、 %氧系、矽氧系等之熱固型樹脂或紫外線硬化型樹脂等。 除此以外,亦可列舉例如矽氧烷系聚合物等玻璃質系聚合 物又’亦可使用日本專利特開2001-343529號公報 (WO01/37007)中所記載之聚合物膜。作為該膜之材料,可 使用例如含有侧鏈上具有經取代或未經取代之醯亞胺基之 熱塑性樹脂、以及側鏈上具有經取代或未經取代之苯基與 腈基之熱塑性樹脂之樹脂組合物,例如,可列舉含有包含 異丁稀與N-甲基順丁烯二酿亞胺之交替共聚物、以及丙烯 腈-苯乙烯共聚物之樹脂組合物。該聚合物膜可為例如上 述樹脂組合物之擠壓成形物。 上述保護層(内側保護層)130宜於光學上具有各向同性 性質。具體而言,内側保護層之厚度方向之相位差 Rth(550)宜為-20 nm〜+20 nm,更佳為 _1〇 nm〜+1〇 nm,特 佳為-6nm〜+6nm,最佳為·3ηιη〜+3ηηι。内側保護層之面 147072.doc • 28 - 201042294 内相位差Re(550)宜為〇 nm以上10 nm以下,更佳為0 nm以 上6 nm以下,特佳為〇 nm以上3 nm以下。關於可形成如此 之光學上具有各向同性性質之保護層的膜的具體情況,記 載於日本專利特開2008-180961號公報中,該記載作為參 考而引用於本說明書中。 D.液晶顯示裝置 本發明之液晶顯示裝置之製造方法,係使用上述Α_ι項 〜A·3項中所記載之本發明之光擴散元件之製造方法而進 Ό y 行。圖5係藉由本發明之較佳實施形態之製造方法而獲得 之液晶顯示裝置之概略剖面圖。液晶顯示裝置5〇〇包括: 液晶胞5 10 ;配置於液晶胞兩側之偏光板520及530 ;設置 於偏光板530外側之背光單元540 ;以及設置於偏光板520 外側(視認側)之光擴散元件1 〇〇。可根據目的,將任意適當 之光學補償板(相位差板)配置於液晶胞51 〇與偏光板520及/ 或530之間。液晶胞510包括一對基板(具代表性的是玻璃 Q 基板)511及512、以及配置於基板511與512之間的包含作 為顯不媒體之液晶之液晶層5 13。 光擴散元件100係上述A-1項〜A-3項及B項中所記載之本 發明之光擴散元件。或者,亦可配置上述C項中所記載之 本發明之附光擴散元件之偏光板,來代替光擴散元件1〇〇 及視認側偏光板520。光擴散元件係使透過液晶胞之光(具 代表性的是如下所述之準直光)穿透及擴散。 上述为光早元540係朝向液晶胞510射出準直光之平行光 光源裝置。背光單元可具有能射出準直光之任意適當之構 147072.doc -29· 201042294 成。例如,背光單元包括光源、以及對自光源射出之光進 行準直處理之聚光元件(均未圖示)。於該情形時,作為聚 光元件’可採用能對自光源射出之光進行準直處理之任意 適田之聚光元件。於光源本身可射出準直光之情形時,可 省略聚光元件。作為背光單元(平行光光源裝置)之具體構 成,可列舉例如以下所述者:(1)將於扁豆狀透鏡 (Lenticular· Lens)或炮彈型透鏡之平坦面側之除透鏡焦點 乂外之。卩分设有遮光層或反射層之聚光元件配置於光源 (例如冷陰極螢光燈)之液晶胞側的構成(例如日本專利特開 2008-2620 12號公報);包括側光型lED光源、其導光 板 '以及於導光板側形成有凸面且配置於該導光板之液晶 胞側之變角稜鏡的構成(於本構成中,可根據需要進而使 用各向異性擴散元件;例如,曰本專利第3442247號);(3) 將光吸收性樹脂與透明性樹脂交替地形成為條紋狀之遮光 層配置於背光源與背光源側偏光板之間的構成(例如,日 本專利特開2007-279424號公報);(4)使用炮彈型LED作為 光源之構成(例如,曰本專利特開平6_13〇255號公報);(5) 使用有菲涅耳透鏡及根據需要而使用之擴散板的構成(例 如,曰本專利特開平1-126627號公報卜記載有此等之詳細 構成之上述公報係作為參考而引用於本說明書中。 液晶層513宜包含黑色顯示時為垂直配向之液晶分子。 作為具有此種液晶層之液晶胞之驅動模式,可列舉例如 MVA(MulU-domain Vertical Alignment,多域垂直配向)模 式、PVA(圖案 VA(Pattern Vertical Alignment,圖案垂直配 147072.doc -30- 201042294 向))模式、TN(扭轉向列(Twisted Nematic))模式、ECB(電 控雙折射(Electrically Controlled Birefringence))模式、 OCB(Optically Compensated Bend 5 光學補償彎曲)(彎曲向 列(bend nematic))模式。 實施例 以下’藉由實施例而具體說明本發明,但本發明並不限 定於此等實施例。實施例中之評價方法為如下所述。又, 只要未特別註明,則實施例中之「份」及「%」為重量基 °隼。 (1) 光擴散元件之厚度 利用微计測式厚度計(三豐(Mitutoyo)公司製造)測定基 材與光擴散元件之合計厚度,並自該合計厚度減去基材之 厚度而計算出光擴散元件之厚度。 (2) 濃度調變區域之有無 對實施例及比較例中所獲得之光擴散元件與基材之積層 〇 體,一面使用液體氮進行冷卻,一面利用切片機切片成 0.1 μηι之厚度’而設為測定樣品。使用穿透式電子顯微鏡 (TEM,transmission electr〇n micr〇sc〇pe),觀察該測定樣 品之光擴散兀件部分之微粒之狀態。將於微粒内部可確認 出由前驅物滲透所引起之對比度之情形設為「有濃度調= 區域」,並將於微粒内部無法確認出對比度而為均勻色之 情形設為「無濃度調變區域」。 (3) 霧度 依照JIS 713 6中所規定之古、土 叮观疋之方法,使用霧度計(村上色彩科 147072.doc 31 201042294 學研究所公司製造,商品名「HN_150」)測定霧度。 (4) 光擴散半值角 自光擴散元件之正面照射雷射光,並利用側角光度計 (goniophotometer)每隔1°地測定所擴散之光之相對於擴散 角度之擴散亮度,如圖6所示,於擴散之兩側測定除雷射 之直進穿透光以外之光自擴散亮度最大值變為一半亮度之 擴散角度,將加上該兩側之角度而得者(圖6之角度a +角 度A')作為光擴散半值角。 (5) 背向散射率 將實施例及比較例中所獲得之光擴散元件與基材之積層 體經由透明黏著劑貼合於黑色丙烯酸板(住友化學公司製 造,商品名「SUMIPEX」(註冊商標),厚度為2 mm)上, 而设為測定樣品。利用分光光度計(日立計測器公司製 造,商品名「U4100」)測定該測定樣品之積分反射率。另 一方面,使用自上述光擴散元件用塗敷液去除微粒而成之 塗敷液’製作基材與透明塗敷層之積層體,而設為對照樣 品,並利用與上述相同之方式測定積分反射率(即表面反 射率)自上述測&amp;樣品之積分反射率減去上料照樣品 之積分反射率(表面反射率),藉此計算出光擴散元件之背 向散射率。 (6)前驅物之滲透範圍 自以上述(2)中杯 職光擴散性微粒Λ 序拍攝之雇照片隨機選奉 測定光擔;y對所選擇之光擴散性微粒之各個, 定先擴散性微粒之粒徑及光擴㈣《之未«有㈣ 147072.doc -32- 201042294 物之部分(非滲透部分)之粒徑,並根據下述式計算出滲透 範圍。將ίο個光擴散性微粒之平均值設為滲透範圍。 (滲透範圍)={1-(非滲透部分之粒徑/光擴散性微粒之粒 徑)}X100(%) &lt;實施例1 :光擴散元件之製作&gt; 於含有62%之作為超微粒成分之氧化錯奈米粒子(平均粒 徑為60 nm,折射率為2.19)之硬塗用樹脂(JSR公司製造, 商品名「Opstar KZ6661」(包含 MEK(methyl ethyl ketone ’ 曱基乙基酮)/MIBK(methyl isobutyl ketone,曱基 異丁基綱))18.2份中’添加作為樹脂成分之前驅物之季戊 四酵三丙烯酸酯(大阪有機化學工業公司製造,商品名 「Viscoat#300」,折射率為1.52)之50% ΜΕΚ溶液6.8份、光 t合起始劑(汽巴精化公司製造,商品名「Irgaeure9〇7」)〇.〇68 份、調平劑(DIC公司製造,商品名「GRANDIC PC 4100」)0.625份、及作為光擴散性微粒之聚曱基丙烯酸曱 醋(PMMA)微粒(根上工業公司製造,商品名r artpearl J4P」,平均粒徑為2·1 μπι,折射率為1.49)2.5份。對該混 合物進行5分鐘超聲波處理’製備均勻分散有上述各成分 之塗敷液。使用棒式塗佈機將該塗敷液塗敷於TAC膜(富士 膠片公司製造,商品名「Fujitac」)上,並以l〇〇°C乾燥1 分鐘後’照射累計光量為300 mJ之紫外線,而獲得厚度為 15 μπι之光擴散元件。將所獲得之光擴散元件用於上述 (1)〜(6)之評價。將結果與下述實施例2~4之結果一併示於 表1中。此外’將光擴散元件剖面之ΤΕΜ照片示於圖7中。 147072.doc •33- 201042294 根據該TEM照片,確認出於光擴散性微粒之内部形成有濃 度調變區域。 &lt;實施例2 :光擴散元件之製作&gt; 以與實施例1相同之方式製備塗敷液。將該塗敷液靜置4 小時後’以與實施例1相同之方式進行塗敷。將塗敷後之 乾燥溫度設為60°C,以及將厚度設為1 〇 μΓη,除此以外, 以與實施例1相同之方式獲得光擴散元件。將所獲得之光 擴散元件用於上述(1)〜(6)之評價。將結果示於表1。 &lt;實施例3 :光擴散元件之製作&gt; 將塗敷塗敷液後之乾餘溫度設為6 〇 ,除此以外,以與 實此例1相同之方式獲得光擴散元件。將所獲得之光擴散 7G件用於上述(1)〜(6)之評價。將結果示於表1。此外,將 光擴散元件刮面之TEM照片示於圖7中。根據該tem照 片,確認出於光擴散性微粒之内部形成有濃度調變區域。 &lt;貫施例4 :光擴散元件之製作&gt; 使用PMMA微粒(總研化學公司製造,Μχι8〇ΤΑ)作為光 擴散性微粒,以及將厚度設為2〇 μιη,除此以外,以與實 施例1相同之方式獲得光擴散元件。將所獲得之光擴散元 件用於上述(1)〜(6)之評價。將結果示於表丨中。此外,將 光擴散兀件剖面之ΤΕΜ照片示於圖7中。根據該ΤΕΜ照 片,確認出於光擴散性微粒之内部形成有濃度調變區域。 &lt;實施例5 :光擴散元件之製作&gt; 以與實施例1相同之方式製備塗敷液。將該塗敷液靜置2 小時之後,以與實施例2相同之方式獲得光擴散元件。將 147072.doc 201042294 所獲知之光擴散兀件用於上述⑴〜⑹之評價。將結果示於 表1中。 &lt;實施例6 :光擴散元件之製作&gt; 以與實施例1相同之方式製備塗敷液。將該塗敷液靜置7 小時之後,以與實施例2相同之方式獲得光擴散元件。將 所獲侍之光擴散70件用於上述之評價。將結果示於 表1中。 &lt;實施例7 ··光擴散元件之製作&gt; 以與貫施例1相同之方式製備塗敷液。將該塗敷液靜置 24小時之後,以與實施例2相同之方式獲得光擴散元件。 將所獲得之光擴散元件用於上述(1)〜(6)之評價。將結果示 於表1中。 [表1] 靜置時間 (h) 乾燥溫度 CC) 滲透範圍 (%) 厚度 (μιη) 霧度 (%) 光擴散 半值角 (。) 背向 散射率 (0/Λ 施例1 0 100 76.3 15 98.4 62 〇 39 — 實施例2 4 60 79.5 10 98.5 63 ~〇 4? 貪施例3 0 60 27.7 15 95.4 32 0 19 實施例4 0 100 25.8 20 98.3 60 0.50~ 實施例5 2 60 54.9 10 97.7 45 0.31 實施例6 7 60 81.3 10 98.5 63 0.43 \trnm 24 60 81.5 10 98.5 63 0.45 &lt;實施例8 :液晶顯示裝置之製作&gt; 自包括多域型VA模式之液晶胞的市售之液晶電視(s〇NY 公司製造,BRAVIA20型,商品名「KDL20J3000」)取出 液晶胞。於該液晶胞之兩側,以使各自之偏光元件之吸收 軸正交之方式貼合市售之偏光板(日東電工公司製造,商 147072.doc •35- 201042294 品名「NPF-SEG1423DU」)。更具體而言,以背光側偏光 板之偏光元件之吸收軸方向成為垂直方向(相對於液晶面 板之長邊方向為90°),且視認側偏光板之偏光元件之吸收 軸方向成為水平方向(相對於液晶面板之長邊方向為〇。)之 方式進行貼合。進而,將實施例i之光擴散元件自基材轉 印並貼合於視認側偏光板之外側,而製作液晶面板。 另一方面,於PMMA片材之單面,使用轉印輥熔融熱轉 印扁豆狀透鏡之圖案。於與形成有透鏡圖案之面相反之側 的面(平滑面)上,以使光僅穿透透鏡焦點之方式蒸鍍鋁之 圖案,形成開口部之面積比率為7%(反射部之面積比率為 93%)之反射層。以如此方式製作聚光元件。❹冷陰極營 光燈⑽NY公司製造,BRAVIA2〇J之CCFL(c〇id⑽邊 F1U〇reSCeiU LamP,冷陰極勞光燈))作為背光之光源,於該 光源上安裝聚光元件,而製作射出準直光之平行光光源裝 置(背光單元)。 义於上述液晶面板中裝入上述背光單元,而製作準直背光 刖面擴散系統之液晶顯示裝置。 A a ^冑所㈣之液晶顯示裝置 暗處進订白色顯示及黑色顯示,並目測觀察其顯示狀 態。其結果為’顯示出自斜方向觀古:一 示較黑且於暗處之白色顯示之二之黑色顯 性。 儿度較咼之良好的顯示特 &lt;評價&gt; 由實施例之依序記載及表丨可知, 元件之製造方法,纟需進行 根據本發明之光擴散 之處理或操作(實質上, 147072.doc -36 - f 201042294 僅藉由在混合光擴散性微粒與基質樹脂成分之前驅物之後 使該前驅物發生聚合)’便可製造具有濃度調變區域之光 擴散元件。藉由將此種光擴散元件用於準直背光前面擴散 系統之液晶顯示裝置,可獲得具有於亮處之黑色顯示較黑 且於暗處之白色顯示之亮度較高之良好的顯示特性之液晶 顯示裝置。又,對實施例1〜3及5〜7進行比較可知,只要係 前驅物向光擴散性微粒内之滲透達到飽和狀態為止,則靜 ❹ 置時間越長,將獲得具有越高之擴散性的光擴散元件,若 已達到飽和狀態,則即使靜置時間變長,所獲得之光擴散 元件之擴散性亦為大致固定。此外可知,藉由確保特定之 靜置時間而形成濃度調變區域,即使以低溫進行乾燥,亦 可獲彳于具有較咼之霧度值之光擴散元件(低溫乾燥於製造 時之成本及安全性方面優異,故而較佳)。 產業上之可利用性 藉由本發明之製造方法而獲得之光擴散元件及附光擴散 〇 兀件之偏光板,適合用於液晶顯示裝置之視認侧構件、液 晶顯示裝置之背光用構件、照明器具(例如有機EL、LED) 用擴散構件,尤其適合用作準直背光前面擴散系統之前面 擴散元件。 【圖式簡單說明】 圖1係用以說明藉由本發明之較佳實施形態之製造方法 而獲得的光擴散元件中之基質之樹脂成分及光擴散性微粒 之分散狀態之模式圖; 圖2(a)係用以說明本發明之光擴散元件中之自光擴散性 147072.doc -37- 201042294 微粒中心部至基質為止之折射率變化之概念圖,圖2(b)係 用以說明先前之光擴散元件中之自微粒中心部至基質為止 之折射率變化之概念圖; 圖3係表示關於靜置時間不同之塗敷液,乾燥溫度與所 獲得之擴散半值角之關係之圖表; 圖4係藉由本發明之較佳實施形態之製造方法而獲得之 附光擴散元件之偏光板的概略剖面圖; 圖5係藉由本發明之較佳實施形態之製造方法而獲得之 液晶顯示裝置的概略剖面圖; 圖6係用以說明計算光擴散半值角之方法的模式圖;及 圖7係表示關於實施例1、3及4之光擴散元件之濃度調變 區域的穿透式顯微鏡照片。 【主要元件符號說明】 10 基質 11 樹脂成分 20 光擴散性微粒 30 濃度調變區域 100 光擴散元件 110 偏光元件 120 保護層 130 保護層 200 附光擴散元件之偏光板 500 液晶顯示裝置 147072.doc -38-Polarized component. For example, hydrophilicity such as adsorption of a dichroic substance such as iodine or a dichroic dye to a polyvinyl alcohol-based film, a partially formalized polyvinyl alcohol-based film, an ethylene-vinyl acetate-based copolymer system, or a partially saponified film The molecular film is uniaxially stretched; a polyether-based alignment film such as a dehydrated material of ethylene glycol or a dehydrochloric acid-treated product of a gas-gathered woman. Among these, it is preferable to use a dichroic substance such as ruthenium to absorb (4) a polyhedral alcohol-based film and to uniaxially extend the polarizing element. The thickness of these polarizing elements is not particularly limited, but is usually about 1 to 80 μηι. A polarizing element obtained by adsorbing iodine on a polyvinyl alcohol-based film and uniaxially stretching can be carried out, for example, by dipping the polyethyl ethoxylate film into a broken aqueous solution to carry out dyeing and stretching to 3 to 7 times of the original length. Production. If necessary, it may contain = or zinc sulphate, chlorinated, etc., or may be immersed in an aqueous solution such as Aihua, etc., or may be immersed in water before dyeing as needed. Washed with water. By performing the # Μ ^ ^ rule washing on the polyethylene fermentation membrane, not only the dirt or anti-swelling of the surface of the polyvinyl alcohol film can be washed away, but the dyeing unevenness is prevented from being caused by the dyeing of the polyethylene film. = effect. The extension can be extended on the side of the dyeing side, or it can be dyed with iodine after the extension of 147072.doc •27- 201042294. It may also be extended in an aqueous solution of boric acid or potassium iodide or in a water bath. C-3 · Protective layer The above protective layers 20 and 130 are formed of any suitable film which can be used as a protective layer of a polarizing plate. Specific examples of the material which is a main component of the film include cellulose-based resins such as triethyl cellulose (TAC); polyester-based polyvinyl alcohol-based, polycarbonate-based, polyamid-based, and polyfluorene-based polymers. A transparent resin such as an imide-based, poly-m-polystyrene-based, polyene-based, poly-smoke-based, (meth)acrylic, or acetate-based resin. Further, examples thereof include thermosetting resins such as (meth)acrylic acid, ammonia vinegar, (meth)acrylic acid vinegar, % oxygen, and xenon, and ultraviolet curable resins. In addition, a polymer film such as a siloxane polymer or a polymer film described in JP-A-2001-343529 (WO01/37007) can also be used. As the material of the film, for example, a thermoplastic resin having a substituted or unsubstituted quinone imide group in a side chain, and a thermoplastic resin having a substituted or unsubstituted phenyl group and a nitrile group in a side chain can be used. The resin composition may, for example, be a resin composition containing an alternating copolymer of isobutylene and N-methylbutylenimine and an acrylonitrile-styrene copolymer. The polymer film may be, for example, an extruded product of the above resin composition. The protective layer (inner protective layer) 130 is preferably optically isotropic. Specifically, the phase difference Rth (550) in the thickness direction of the inner protective layer is preferably -20 nm to +20 nm, more preferably _1 〇 nm to +1 〇 nm, and particularly preferably -6 nm to +6 nm, most Jia is · 3ηιη~+3ηηι. The inner protective layer 147072.doc • 28 - 201042294 The internal phase difference Re(550) should be below 10 nm below 〇 nm, more preferably below 6 nm above 0 nm, and especially below 3 nm above 3 nm. A specific example of a film which can form such a protective layer having an optically isotropic property is described in Japanese Laid-Open Patent Publication No. 2008-180961, the disclosure of which is incorporated herein by reference. D. Liquid crystal display device The method for producing a liquid crystal display device of the present invention is carried out by using the method for producing a light diffusing element of the present invention described in the above paragraphs 1-3 to A. Fig. 5 is a schematic cross-sectional view showing a liquid crystal display device obtained by a manufacturing method of a preferred embodiment of the present invention. The liquid crystal display device 5 includes: a liquid crystal cell 5 10; polarizing plates 520 and 530 disposed on both sides of the liquid crystal cell; a backlight unit 540 disposed outside the polarizing plate 530; and light disposed outside the polarizing plate 520 (viewing side) Diffusion element 1 〇〇. Any appropriate optical compensation plate (phase difference plate) may be disposed between the liquid crystal cells 51 and the polarizing plates 520 and/or 530, depending on the purpose. The liquid crystal cell 510 includes a pair of substrates (typically glass Q substrates) 511 and 512, and a liquid crystal layer 513 disposed between the substrates 511 and 512 and containing liquid crystal as a display medium. The light diffusing element 100 is the light diffusing element of the present invention described in the above items A-1 to A-3 and B. Alternatively, instead of the light diffusing element 1A and the viewing side polarizing plate 520, the polarizing plate with the light diffusing element of the present invention described in the above item C may be disposed. The light diffusing element penetrates and diffuses light transmitted through the liquid crystal cell (typically collimated light as described below). The above is a parallel light source device in which the light early element 540 emits collimated light toward the liquid crystal cell 510. The backlight unit can have any suitable configuration capable of emitting collimated light 147072.doc -29· 201042294. For example, the backlight unit includes a light source and a concentrating element (none of which is shown) for collimating the light emitted from the light source. In this case, as the concentrating element ‘, any concentrating element capable of collimating the light emitted from the light source can be used. When the light source itself can emit collimated light, the concentrating element can be omitted. The specific configuration of the backlight unit (parallel light source device) may be, for example, the following: (1) The lens focus on the flat side of the Lenticular Lens or the cannonball lens. A concentrating element provided with a light shielding layer or a reflective layer is disposed on a liquid crystal cell side of a light source (for example, a cold cathode fluorescent lamp) (for example, Japanese Patent Laid-Open Publication No. 2008-2620 12); The light guide plate ′ and the light guide plate side are formed with a convex surface and disposed at a liquid crystal cell side of the light guide plate. In the present configuration, an anisotropic diffusion element can be used as needed; for example, transcript Patent No. 3442247) (3) A configuration in which a light-absorbing resin and a transparent resin are alternately formed in a stripe-like light shielding layer between a backlight and a backlight-side polarizing plate (for example, Japanese Patent Laid-Open No. 2007-279424) (4) The use of a bullet-type LED as a light source (for example, Japanese Patent Laid-Open Publication No. Hei 6-13-255); (5) A configuration using a Fresnel lens and a diffusion plate used as needed ( For example, the above-mentioned publications having the detailed configurations described above are incorporated herein by reference. The liquid crystal layer 513 preferably includes a vertical display in black display. Liquid crystal molecules. Examples of the driving mode of the liquid crystal cell having such a liquid crystal layer include MVA (MulU-domain Vertical Alignment) mode and PVA (Pattern Alignment VA (Pattern Vertical Alignment). Doc -30- 201042294 to)) mode, TN (Twisted Nematic) mode, ECB (Electrically Controlled Birefringence) mode, OCB (Optically Compensated Bend 5 optically compensated bending) (bending nematic) (Bend nematic) mode. EXAMPLES Hereinafter, the present invention will be specifically described by way of examples, but the present invention is not limited to the examples. The evaluation methods in the examples are as follows. The "parts" and "%" in the examples are weight basis. (1) Thickness of light diffusing element The substrate and the light diffusing element are measured by a micrometer thickness gauge (manufactured by Mitutoyo Co., Ltd.). The total thickness is calculated, and the thickness of the light diffusing element is calculated by subtracting the thickness of the substrate from the total thickness. (2) The presence or absence of the concentration modulation region for the examples and comparison The laminated body of the light-diffusing element and the substrate obtained by the method is cooled by liquid nitrogen, and sliced to a thickness of 0.1 μm by a microtome to prepare a measurement sample. Using a transmission electron microscope (TEM) 〇n micr〇sc〇pe), the state of the particles of the light-diffusing component of the measurement sample was observed. The case where the contrast caused by the penetration of the precursor is confirmed in the inside of the particle is "the concentration adjustment = region", and the case where the contrast cannot be confirmed inside the particle and the uniform color is set to "no concentration modulation region" "." (3) Haze The haze is measured by a haze meter (Murako Color Department 147072.doc 31 201042294, Institute of Research, Ltd., trade name "HN_150") according to the method of the ancient and the earthworms specified in JIS 713. . (4) Light diffusion half-value angle The laser beam is irradiated from the front side of the light-diffusing element, and the diffusion brightness of the diffused light with respect to the diffusion angle is measured every 1° by a goniophotometer, as shown in Fig. 6. It is shown that the diffusion angle of the light from the diffused brightness maximum value to the half brightness of the light other than the direct penetration light of the laser is measured on both sides of the diffusion, and the angles of the two sides are added (the angle of the figure a + Angle A') acts as a light diffusion half value angle. (5) Backscattering ratio The laminate of the light-diffusing element and the substrate obtained in the examples and the comparative examples was bonded to a black acrylic plate (manufactured by Sumitomo Chemical Co., Ltd. under the trade name "SUMIPEX" (registered trademark). ), the thickness is 2 mm), and it is set as the measurement sample. The integral reflectance of the measurement sample was measured by a spectrophotometer (manufactured by Hitachi Instruments Co., Ltd., trade name "U4100"). On the other hand, a laminate obtained by removing fine particles from the coating liquid for a light-diffusing element is used to form a laminate of a substrate and a transparent coating layer, and is used as a control sample, and the integral is measured in the same manner as described above. The reflectance (i.e., surface reflectance) is calculated from the integrated reflectance of the sample & sample minus the integrated reflectance (surface reflectance) of the sample, thereby calculating the backscattering ratio of the light diffusing element. (6) The penetration range of the precursor is randomly selected from the photographs taken by the light diffusing particle sequence of the above-mentioned (2), and the diffusedness is selected for each of the selected light diffusing particles. Particle size and light expansion (4) "There is no" (4) 147072.doc -32- 201042294 The particle size of the part (non-permeable part), and the penetration range is calculated according to the following formula. The average value of the light diffusing particles is set as the penetration range. (Permeation range) = {1 - (particle diameter of non-permeable portion / particle diameter of light diffusing fine particles)} X100 (%) &lt;Example 1: Preparation of light diffusing element&gt; A hard coating resin (manufactured by JSR Corporation, trade name "Opstar KZ6661" (containing MEK (methyl ethyl ketone ' mercapto ethyl ketone), a component of oxidized tymallose particles (average particle diameter: 60 nm, refractive index: 2.19) /MIBK (methyl isobutyl ketone, fluorenyl isobutyl ketone)) 18.2 parts of the pentylene tetraacetate which is added as a resin component precursor (manufactured by Osaka Organic Chemical Industry Co., Ltd., trade name "Viscoat #300", refractive index 1.52) 50% ΜΕΚ solution 6.8 parts, light t-starting agent (manufactured by Ciba Specialty Chemicals Co., Ltd., trade name "Irgaeure9〇7") 〇. 68 parts, leveling agent (manufactured by DIC Corporation, trade name " GRANDIC PC 4100") 0.625 parts and polyacrylic acid ruthenium vinegar (PMMA) fine particles (manufactured by Kasei Kogyo Co., Ltd., trade name r artpearl J4P) as light diffusing fine particles, the average particle diameter is 2·1 μπι, and the refractive index is 1.49) 2.5 parts. The mixture was subjected to ultrasound for 5 minutes. The preparation was carried out to prepare a coating liquid in which the above components were uniformly dispersed. The coating liquid was applied onto a TAC film (manufactured by Fujifilm Co., Ltd., trade name "Fujitac") using a bar coater, and l〇〇° After drying for 1 minute, C was irradiated with ultraviolet light having an integrated light amount of 300 mJ to obtain a light diffusing element having a thickness of 15 μm. The obtained light diffusing element was used for the evaluation of the above (1) to (6). The results of Examples 2 to 4 are shown together in Table 1. Further, 'Photograph of the cross section of the light diffusing element is shown in Fig. 7. 147072.doc • 33- 201042294 According to the TEM photograph, it is confirmed that the light diffusibility is obtained. A concentration-modulating region was formed inside the fine particles. <Example 2: Preparation of Light-Diffusing Element> A coating liquid was prepared in the same manner as in Example 1. After the coating liquid was allowed to stand for 4 hours, The coating was carried out in the same manner as in Example 1. A light diffusing element was obtained in the same manner as in Example 1 except that the drying temperature after the coating was changed to 60 ° C and the thickness was set to 1 μμηη. The obtained light diffusing element is used for the evaluation of (1) to (6) above. The results are shown in Table 1. <Example 3: Preparation of light diffusing element> The same manner as in Example 1 except that the dry temperature after applying the coating liquid was 6 Torr. The light diffusing element was obtained, and the obtained light-diffusing 7G piece was used for the evaluation of the above (1) to (6). The results are shown in Table 1. Further, the TEM photograph of the light-diffusing element scraping surface is shown in Fig. 7. According to this tem photograph, it was confirmed that a concentration modulation region was formed inside the light diffusing fine particles. &lt;Example 4: Production of Light-Diffusing Element&gt; Using PMMA fine particles (manufactured by Konica Chemical Co., Ltd., Μχι8〇ΤΑ) as light-diffusing fine particles, and having a thickness of 2 μm, The light diffusing element was obtained in the same manner as in Example 1. The obtained light diffusing element was used for the evaluation of the above (1) to (6). The results are shown in the table. Further, a photograph of the cross section of the light diffusing element is shown in Fig. 7. According to the photographic film, it was confirmed that a concentration modulation region was formed inside the light diffusing fine particles. &lt;Example 5: Production of Light-Diffusing Element&gt; A coating liquid was prepared in the same manner as in Example 1. After the coating liquid was allowed to stand for 2 hours, a light diffusing element was obtained in the same manner as in Example 2. The light diffusing element known from 147072.doc 201042294 is used for the evaluation of the above (1) to (6). The results are shown in Table 1. &lt;Example 6: Production of light diffusing element&gt; A coating liquid was prepared in the same manner as in Example 1. After the coating liquid was allowed to stand for 7 hours, a light diffusing element was obtained in the same manner as in Example 2. The obtained light was diffused by 70 pieces for the above evaluation. The results are shown in Table 1. &lt;Example 7··Preparation of light diffusing element&gt; A coating liquid was prepared in the same manner as in Example 1. After the coating liquid was allowed to stand for 24 hours, a light diffusing element was obtained in the same manner as in Example 2. The obtained light diffusing element was used for the evaluation of the above (1) to (6). The results are shown in Table 1. [Table 1] Settling time (h) Drying temperature CC) Permeation range (%) Thickness (μιη) Haze (%) Light diffusion half value angle (.) Backscattering rate (0/Λ Example 1 0 100 76.3 15 98.4 62 〇39 - Example 2 4 60 79.5 10 98.5 63 ~〇4? Greedy Example 3 0 60 27.7 15 95.4 32 0 19 Example 4 0 100 25.8 20 98.3 60 0.50~ Example 5 2 60 54.9 10 97.7 45 0.31 Example 6 7 60 81.3 10 98.5 63 0.43 \trnm 24 60 81.5 10 98.5 63 0.45 &lt;Example 8: Production of liquid crystal display device&gt; Commercially available liquid crystal television from liquid crystal cell including multi-domain type VA mode (Manufactured by s〇NY, BRAVIA20, trade name "KDL20J3000"), the liquid crystal cells are taken out. On both sides of the liquid crystal cell, a commercially available polarizing plate is attached to each other so that the absorption axes of the respective polarizing elements are orthogonal. Manufactured by the Electrician Co., Ltd., 147072.doc • 35- 201042294, the product name "NPF-SEG1423DU". More specifically, the absorption axis direction of the polarizing element of the backlight-side polarizing plate is perpendicular (relative to the longitudinal direction of the liquid crystal panel) 90°), and the absorption axis of the polarizing element of the polarizing plate In the horizontal direction (the direction in which the longitudinal direction of the liquid crystal panel is 〇.), the light diffusing element of Example i is transferred from the substrate and bonded to the outside of the viewing side polarizing plate. On the other hand, on one side of the PMMA sheet, the pattern of the lentil lens is melt-transferred using a transfer roller, on the surface (smooth surface) opposite to the surface on which the lens pattern is formed, so that The pattern of aluminum was vapor-deposited only by penetrating the focus of the lens, and a reflective layer having an area ratio of the opening portion of 7% (the area ratio of the reflecting portion was 93%) was formed. The concentrating element was fabricated in this manner. Lamp (10) manufactured by NY Company, BRAVIA2〇J CCFL (c〇id(10) side F1U〇reSCeiU LamP, cold cathode discharge lamp)) as a light source of backlight, a concentrating element is mounted on the light source, and parallel light that emits collimated light is produced. Light source device (backlight unit). A liquid crystal display device in which the above-described backlight unit is incorporated in the above liquid crystal panel to produce a collimated backlight diffusion system. A a ^ 胄 (4) liquid crystal display device In the dark place the white display and black display, and visually observe its display status. The result is 'displayed from the oblique direction of the ancient: a black display that is darker and white in the dark. The display is excellent in terms of goodness. <Evaluation> From the sequential description and the description of the examples, it is known that the method of manufacturing the element does not require the treatment or operation of light diffusion according to the present invention (essentially, 147072. Doc-36-f 201042294 A light diffusing element having a concentration-modulating region can be produced only by polymerizing the precursor after mixing the light-diffusing particles with the matrix resin component. By using such a light diffusing element for a liquid crystal display device for collimating a backlight front diffusing system, it is possible to obtain a liquid crystal having a good display characteristic in which a black display in a bright portion is black and a white display in a dark portion has a high luminance. Display device. Further, comparing Examples 1 to 3 and 5 to 7, it is understood that as long as the penetration of the precursor into the light diffusing fine particles is saturated, the longer the static standing time, the higher the diffusibility is obtained. When the light diffusing element has reached a saturated state, the diffusibility of the obtained light diffusing element is substantially constant even if the standing time becomes long. In addition, it can be seen that by ensuring a specific resting time to form a concentration-modulating region, even if drying at a low temperature, it is possible to obtain a light diffusing element having a haze value (the cost and safety of low-temperature drying in manufacturing) Excellent in terms of sex, so it is better). Industrial Applicability The light diffusing element and the light-diffusing element-attached polarizing plate obtained by the manufacturing method of the present invention are suitable for use as a viewing side member of a liquid crystal display device, a backlight member for a liquid crystal display device, and a lighting fixture. (For example, organic EL, LED) With a diffusion member, it is particularly suitable for use as a front diffusing element in front of a collimated backlight front diffusion system. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic view for explaining a dispersion state of a resin component and a light diffusing fine particle of a matrix in a light diffusing element obtained by a manufacturing method of a preferred embodiment of the present invention; a) is used to illustrate the conceptual diagram of the refractive index change from the center of the particle to the substrate in the light diffusing element of the present invention, and FIG. 2(b) is used to illustrate the previous A conceptual diagram of the change in refractive index from the center of the particle to the substrate in the light diffusing element; FIG. 3 is a graph showing the relationship between the drying temperature and the obtained diffusion half-value angle for the coating liquid having different standing times; 4 is a schematic cross-sectional view of a polarizing plate with a light diffusing element obtained by the manufacturing method of the preferred embodiment of the present invention; and FIG. 5 is a schematic view of a liquid crystal display device obtained by the manufacturing method of the preferred embodiment of the present invention. FIG. 6 is a schematic view for explaining a method of calculating a half-value angle of light diffusion; and FIG. 7 is a view showing a transmissive display of a concentration modulation region of the light diffusing elements of Embodiments 1, 3, and 4. Micrograph. [Description of main components] 10 Substrate 11 Resin component 20 Light diffusing fine particles 30 Density modulation region 100 Light diffusing element 110 Polarizing element 120 Protective layer 130 Protective layer 200 Polarizing plate with light diffusing element 500 Liquid crystal display device 147072.doc - 38-

Claims (1)

201042294 七、申請專利範圍: 1· 一種光擴散元件之製造方法,其包括如下步驟: 使包含樹脂成分之前驅物及超微粒成分之基質形成材 料與光擴散性微粒相接觸; 使該前驅物之至少一部分滲透至該光擴散性微粒之内 部;以及 使已滲透至§亥光擴散性微粒之内部之前驅物及未滲透 至該光擴散性微粒之前驅物同時發生聚合而形成包含樹 〇 知成分及超微粒成分之基質,並同時於該光擴散性微粒 之表面附近内部形成濃度調變區域。 2. 如凊求項1之光擴散元件之製造方法,其中於上述滲透 步驟中,使上述前驅物自上述光擴散性微粒之表面滲透 至该光擴散性微粒之平均粒徑之1 〇 %以上9 5 %以下之範 圍為止。 3. 如請求項1或2之光擴散元件之製造方法,其中使上述樹 0 脂成分之前驅物與該光擴散性微粒接觸較上述光擴散性 微粒之粒徑實質上達到最大為止之時間更長之時間。 4. 如請求項1之光擴散元件之製造方法,其中上述樹脂成 分為電離放射線硬化型樹脂’藉由照射電離放射線而使 該樹脂成分之前驅物發生聚合。 5. 一種光擴散元件,其係藉由如請求項1至4中任一項之方 法而獲得者; 包括包含樹脂成分及超微粒成分之基質、以及分散於 該基質中之光擴散性微粒;且 147072.doc 201042294 於該光擴散性微粒之表面附近内部具有該樹脂成分經 滲透而形成之濃度調變區域。 6. 7. -種附光擴散元件之偏光板之製造方法,其係使用如請 求項1至4中任-項之光擴散元件之製造方法。 一種液晶顯示裝置之製造 咬乃沄再係使用如請求項〗5 4 中任—項之光擴散元件之製造方法。201042294 VII. Patent application scope: 1. A method for manufacturing a light diffusing element, comprising the steps of: contacting a matrix forming material comprising a resin component precursor and an ultrafine particle component with light diffusing particles; At least a portion of the material diffuses into the interior of the light diffusing fine particles; and simultaneously forms a precursor containing the tree before it penetrates into the internal precursor of the light diffusing fine particles and does not penetrate the light diffusing fine particles And a matrix of the ultrafine particle component, and at the same time, a concentration modulation region is formed inside the surface of the light diffusing fine particle. 2. The method of producing a light diffusing element according to claim 1, wherein in the permeating step, the precursor is allowed to permeate from the surface of the light diffusing fine particles to 1% or more of an average particle diameter of the light diffusing fine particles. 9 5 % or less. 3. The method of producing a light diffusing element according to claim 1 or 2, wherein a time period in which the precursor of the resin component and the light diffusing fine particle are substantially larger than a particle diameter of the light diffusing fine particle is substantially greater Long time. 4. The method of producing a light-diffusing element according to claim 1, wherein the resin component is ionized radiation-curable resin, and the resin component precursor is polymerized by irradiation of ionizing radiation. A light diffusing element obtained by the method of any one of claims 1 to 4, comprising a matrix comprising a resin component and an ultrafine particle component, and light diffusing particles dispersed in the matrix; Further, 147072.doc 201042294 has a concentration modulation region formed by permeation of the resin component in the vicinity of the surface of the light diffusing fine particles. 6. A method of producing a polarizing plate with a light diffusing element, which is a method of manufacturing a light diffusing element according to any one of claims 1 to 4. Manufacture of a liquid crystal display device The method of manufacturing a light diffusing element according to any one of the claims is provided. 147072.doc -2-147072.doc -2-
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