TW201910821A - Laminated body and method of manufacturing the same - Google Patents

Laminated body and method of manufacturing the same Download PDF

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Publication number
TW201910821A
TW201910821A TW107109035A TW107109035A TW201910821A TW 201910821 A TW201910821 A TW 201910821A TW 107109035 A TW107109035 A TW 107109035A TW 107109035 A TW107109035 A TW 107109035A TW 201910821 A TW201910821 A TW 201910821A
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film
value
light diffusion
light
diffusion control
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TW107109035A
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Chinese (zh)
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TWI760454B (en
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片桐麦
草間健太郎
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日商琳得科股份有限公司
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B27/00Layered products comprising a layer of synthetic resin
    • B32B27/06Layered products comprising a layer of synthetic resin as the main or only constituent of a layer, which is next to another layer of the same or of a different material
    • B32B27/08Layered products comprising a layer of synthetic resin as the main or only constituent of a layer, which is next to another layer of the same or of a different material of synthetic resin
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/02Diffusing elements; Afocal elements
    • G02B5/0205Diffusing elements; Afocal elements characterised by the diffusing properties
    • G02B5/0236Diffusing elements; Afocal elements characterised by the diffusing properties the diffusion taking place within the volume of the element
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B27/00Layered products comprising a layer of synthetic resin
    • B32B27/36Layered products comprising a layer of synthetic resin comprising polyesters
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B37/00Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding
    • B32B37/12Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding characterised by using adhesives
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B37/00Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding
    • B32B37/14Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding characterised by the properties of the layers
    • B32B37/24Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding characterised by the properties of the layers with at least one layer not being coherent before laminating, e.g. made up from granular material sprinkled onto a substrate
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B7/00Layered products characterised by the relation between layers; Layered products characterised by the relative orientation of features between layers, or by the relative values of a measurable parameter between layers, i.e. products comprising layers having different physical, chemical or physicochemical properties; Layered products characterised by the interconnection of layers
    • B32B7/04Interconnection of layers
    • B32B7/12Interconnection of layers using interposed adhesives or interposed materials with bonding properties
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/02Diffusing elements; Afocal elements
    • G02B5/0268Diffusing elements; Afocal elements characterized by the fabrication or manufacturing method
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B37/00Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding
    • B32B37/14Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding characterised by the properties of the layers
    • B32B37/24Methods or apparatus for laminating, e.g. by curing or by ultrasonic bonding characterised by the properties of the layers with at least one layer not being coherent before laminating, e.g. made up from granular material sprinkled onto a substrate
    • B32B2037/243Coating
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B38/00Ancillary operations in connection with laminating processes
    • B32B2038/0052Other operations not otherwise provided for
    • B32B2038/0076Curing, vulcanising, cross-linking
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B2305/00Condition, form or state of the layers or laminate
    • B32B2305/72Cured, e.g. vulcanised, cross-linked
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B2307/00Properties of the layers or laminate
    • B32B2307/40Properties of the layers or laminate having particular optical properties
    • B32B2307/418Refractive
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B2457/00Electrical equipment
    • B32B2457/20Displays, e.g. liquid crystal displays, plasma displays

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Optical Elements Other Than Lenses (AREA)
  • Laminated Bodies (AREA)
  • Liquid Crystal (AREA)

Abstract

The provided is a laminated body and a method for producing the same having a uniform light diffusing property among the different points in a film. The present invention relates to a laminated body and the like, wherein an over film is laminated on at least one side of a light diffusion control film, and there is an internal region having a plurality of regions having a relatively high refractive index in a region having a relatively low refractive index, when a direction perpendicular to the coating transfer direction of a composition for the light diffusion control film is defined as length direction and a direction traverse to the coating direction is defined as a short direction, and the maximum value of the phase difference Re (nm) measured along the short direction of the over film Is set to Remax and the minimum value is set to Remin, a following relational equation (1) is satisfied. (Remax-Remin)/(Remax+Remin) x 100 < 35 (%) (1).

Description

層合體及層合體之製造方法Laminated body and manufacturing method of laminated body

[0001] 本發明有關層合體及層合體之製造方法。   尤其有關藉由上覆層合薄膜層合由光擴散控制薄膜用組成物所成之塗佈層之狀態下進行光硬化所得之光擴散控制薄膜與上覆層合薄膜之層合體,係光擴散控制薄膜之光擴散特性不管薄膜面內之部位為何而均為均一的層合體、以及有關此等層合體之製造方法。[0001] The present invention relates to a laminate and a method for producing the laminate. In particular, the laminated body of the light-diffusion control film and the overlying laminated film obtained by photo-hardening in a state in which a coating layer made of a composition for a light-diffusion control film is laminated with the overlying laminated film is light diffusion. The light-diffusion characteristics of the control film are uniform laminates regardless of the locations within the surface of the film, and a method for manufacturing such laminates.

[0002] 以往,於例如液晶顯示裝置或投影螢幕等所屬之光學技術領域中,提案使用光擴散控制薄膜。   該光擴散控制薄膜具有如下之光擴散特性者:於特定入射角度範圍(以下有時稱為「光擴散入射角度區域」)時顯示一定之光擴散狀態,於偏離光擴散入射角度區域之入射角度範圍,使入射光直接透過,或顯示與在光擴散入射角度區域之光擴散狀態不同之光擴散狀態。   [0003] 作為此等光擴散控制薄膜,已知有多種態樣,尤其已廣泛使用於薄膜內具有於折射率相對低之區域中林立有折射率相對高的複數柱狀物而成之柱構造的光擴散控制薄膜。   [0004] 又,作為其他類型之光擴散控制薄膜,已廣泛使用具有於薄膜內,於沿薄膜面沿任意一方向相互配置折射率不同之複數板狀區域而成之百葉窗構造之光擴散薄膜。   [0005] 不過,具有此等柱構造或百葉窗構造之光擴散控制薄膜,已知係藉由對於將含有折射率不同之2種以上的聚合性化合物之光擴散控制薄膜用組成物塗佈成膜狀之塗佈層,以特定方法照射活性能量線而獲得。   亦即,藉由對塗佈層照射經控制行進方向之特定活性能量線,邊使塗佈層中之2種以上之聚合性化合物相分離邊硬化,可獲得具有特定內部構造之光擴散控制薄膜。   [0006] 然而,對於塗佈層直接照射特定活性能量線時,見到難以於薄膜膜厚方向全面,亦即直至薄膜上面形成特定之內部構造之問題。   亦即,雖可於薄膜膜厚方向之下方部分形成特定之內部構造,但見到於上方部分會發生未形成內部構造之區域的問題。   因此,揭示有不發生未形成內部構造之區域而用以直至薄膜上面形成特定之內部構造的技術(例如參考專利文獻1)。   [0007] 亦即,專利文獻1中,揭示擴散性根據光之入射角而變化之異向性光學薄膜之製造方法,其特徵係包含下述步驟:於光硬化性之未硬化樹脂組成物層之一面上,接合濁度值為1.0~50.0%之光照射遮罩之光照射遮罩接合步驟,於光照射遮罩接合步驟後,藉由透過光照射遮罩照射光而使未硬化樹脂組成物層硬化而形成異向性擴散層之硬化步驟。   又,亦記載有光照射遮罩之表面粗糙度為0.05~0.50μm,或光照射遮罩之氧透過係數為1.0×10-11 cm3 (STP)cm/(cm2 .s.Pa)以下。   亦即,對於由光擴散控制薄膜用組成物所成之塗佈層,以層合特定上覆層合薄膜之狀態進行光硬化,而抑制發生未形成內部構造之區域。 [先前技術文獻] [專利文獻]   [0008]   [專利文獻1] 日本特開2016-194687號公報(申請專利範圍)[0002] Conventionally, in the field of optical technology, such as a liquid crystal display device or a projection screen, it has been proposed to use a light diffusion control film. The light-diffusion control film has the following light-diffusion characteristics: it shows a certain light-diffusion state in a specific incident angle range (hereinafter sometimes referred to as "light-diffusion incident angle area"), and an incident angle deviating from the light-diffusion incident angle area The range allows the incident light to pass directly, or displays a light diffusion state different from the light diffusion state in the light diffusion incident angle region. [0003] As such light diffusion control films, various aspects are known. In particular, they have been widely used in film structures having a plurality of pillars having relatively high refractive indexes in a region having a relatively low refractive index. Light diffusion control film. [0004] In addition, as other types of light diffusion control films, light diffusing films having a louver structure in which a plurality of plate-shaped regions having different refractive indexes with different refractive indexes are arranged in the film in any direction along the film surface have been widely used. [0005] However, it is known that a light diffusion control film having such a pillar structure or a louver structure is formed by coating a film with a composition for a light diffusion control film containing two or more polymerizable compounds having different refractive indices. The coating layer is obtained by irradiating active energy rays by a specific method. That is, by irradiating the coating layer with a specific active energy ray controlled in the direction of travel, the coating layer is hardened while phase-separating two or more polymerizable compounds to obtain a light diffusion control film having a specific internal structure. . [0006] However, when the coating layer is directly irradiated with a specific active energy ray, it is difficult to see the entire thickness direction of the film, that is, until a specific internal structure is formed on the film. That is, although a specific internal structure can be formed in a portion below the film thickness direction, a problem that an area in which the internal structure is not formed occurs in the upper portion is seen. Therefore, a technique is disclosed in which a specific internal structure is not formed on a thin film without a region where an internal structure is not formed (for example, refer to Patent Document 1). [0007] That is, Patent Document 1 discloses a method for manufacturing an anisotropic optical film whose diffusivity changes according to the incident angle of light, which is characterized by including the following steps: a photocurable uncured resin composition layer On one side, a light irradiation mask joining step for joining a light irradiation mask having a turbidity value of 1.0 to 50.0%, and after the light irradiation mask joining step, the uncured resin is composed by transmitting light through the light irradiation mask. A hardening step in which the material layer is hardened to form an anisotropic diffusion layer. It is also described that the surface roughness of the light irradiation mask is 0.05 to 0.50 μm, or the oxygen transmission coefficient of the light irradiation mask is 1.0 × 10 -11 cm 3 (STP) cm / (cm 2 .s.Pa) or less. . That is, the coating layer formed of the composition for a light diffusion control film is subjected to photohardening in a state where a specific overlying laminated film is laminated, and the occurrence of a region where no internal structure is formed is suppressed. [Prior Art Document] [Patent Document] [0008] [Patent Document 1] Japanese Patent Application Publication No. 2016-194687 (Scope of Patent Application)

[發明欲解決之課題]   [0009] 然而,即使使用專利文獻1中記載之光照射遮罩之情況,亦難以穩定地抑制未形成內部構造之區域發生。   尤其,於有某寬度之1片連續之光擴散控制薄膜中,見到未發生未形成內部構造之區域之部位,亦見到發生之部位。由此,薄膜面內之光擴散特性亦因光之入射部位而變化,而於全體見到光擴散特性變不均一之問題。   [0010] 因此,本發明人等鑑於如以上之情況而積極努力後,發現藉由將沿上覆層合薄膜面內之特定方向測定的相位差之偏差設為特定範圍內之值,即使於未發生未形成內部構造之區域時,或即使發生時,內部構造均可均一形成,因而完成本發明。   亦即,本發明之目的在於提供藉由上覆層合薄膜層合由光擴散控制薄膜用組成物所成之塗佈層之狀態下進行光硬化所得之光擴散控制薄膜與上覆層合薄膜之層合體,係光擴散控制薄膜之光擴散特性不管薄膜面內之部位為何而均為均一的層合體、以及有關此等層合體之製造方法。 [用以解決課題之手段]   [0011] 依據本發明,提供如下之層合體,而可解決上述問題,該層合體之特徵係於源自光擴散控制薄膜用組成物之光擴散控制薄膜之至少一面上層合有上覆層合薄膜之狀態之層合體,且光擴散控制薄膜具有於低折射率區域中具有複數高折射率區域且該高折射率區域沿厚度方向延伸之內部構造,且係層合體之層合面內,將形成光擴散控制薄膜時之移動方向設為長邊方向,將與該長邊方向垂直之方向設為短邊方向,且將沿上覆層合薄膜之短邊方向測定之相位差Re(nm)之最大值設為Remax ,最小值設為Remin 時,滿足下述關係式(1),   (Remax -Remin )/(Remax +Remin )×100<35(%) (1)。   亦即,依據本發明之層合體,由於將沿上覆層合薄膜面內之特定方向測定的相位差Re的偏差設為特定範圍內之值,故藉由對於由光擴散控制薄膜用組成物所成之塗佈層層合上覆層合薄膜之狀態下進行硬化,可獲得由光擴散特性不管薄膜面內之部位為何均為均一的光擴散控制薄膜與上覆層合薄膜之層合體。   [0012] 又,構成本發明之層合體時,上覆層合薄膜之短邊方向之長度較好為100~10000mm之範圍內之值。   藉由如此構成,可獲得短邊方向之長度充分的層合體,進而可獲得短邊方向之長度充分的光擴散控制薄膜。   [0013] 又,構成本發明之層合體時,上覆層合薄膜之相位差Re之中央值較好為1000~3000nm之範圍內之值。   藉由如此構成,可有效地抑制光擴散控制薄膜中發生未形成內部構造之區域。   [0014] 又,構成本發明之層合體時,上覆層合薄膜之膜厚較好為5~5000μm之範圍內之值。   藉由如此構成,可獲得進而安定地滿足關係式(1)之上覆層合薄膜。   [0015] 又,構成本發明之層合體時,作為光擴散控制薄膜之內部構造,較好包含於折射率相對低之區域中,於薄膜膜厚方向林立有折射率相對較高之複數柱狀物而成之柱構造。   藉由如此構成,可獲得具有等向性之光擴散特性之光擴散控制薄膜。   [0016] 又,構成本發明之層合體時,作為光擴散控制薄膜之內部構造,較好包含於沿薄膜面之任意一方向交替配置折射率不同之複數板狀區域而成之百葉窗構造。   藉由如此構成,可獲得具有異向性之光擴散特性之光擴散控制薄膜。   [0017] 又,本發明之另一態樣係一種層合體之製造方法,其特徵係上述之層合體之製造方法,且包含下述步驟(a)~(d),   (a)準備包含高折射率活性能量線硬化成分及低折射率活性能量線硬化成分之光擴散控制薄膜用組成物之步驟,   (b)對步驟薄片膜狀塗佈光擴散控制薄膜用組成物而形成塗佈層之步驟,   (c)對於塗佈層之露出面層合滿足關係式(1)之上覆層合薄膜之步驟,   (d)邊使塗佈層移動,邊透過上覆層合薄膜,對該塗佈層照射活性能量線之步驟。   亦即,依據本發明之層合體之製造方法,係將沿上覆層合薄膜面內之特定方向測定的相位差Re的偏差設為特定範圍內之值。因此藉由對於由光擴散控制薄膜用組成物所成之塗佈層層合上覆層合薄膜之狀態下藉由照射活性能量線而硬化(光硬化)。其結果可獲得由光擴散特性不管薄膜面內之部位為何均為均一的光擴散控制薄膜與上覆層合薄膜之層合體。[Problems to be Solved by the Invention] [0009] However, even in the case of using a light irradiation mask described in Patent Document 1, it is difficult to stably suppress the occurrence of a region where an internal structure is not formed. In particular, in a continuous light-diffusion control film having a certain width, a part where a region where an internal structure is not formed does not occur, and a part where the occurrence occurs are also seen. As a result, the light diffusion characteristics in the film surface also change depending on the incident position of the light, and the problem of uneven light diffusion characteristics is seen in the entirety. [0010] Therefore, the present inventors, after actively working in view of the above, found that by setting the deviation of the phase difference measured in a specific direction in the plane of the overlying laminated film to a value within a specific range, The present invention is completed when no area where no internal structure is formed, or even if it occurs, the internal structure can be uniformly formed. That is, an object of the present invention is to provide a light diffusion control film and an overlying laminated film obtained by light curing in a state in which a coating layer made of a composition for a light diffusion control film is laminated with the overlying laminated film. The laminated body is a light-diffusion control film having uniform light-diffusion characteristics regardless of the location within the surface of the film, and a method for manufacturing such a laminated body. [Means for Solving the Problems] [0011] According to the present invention, the above-mentioned problems can be solved by providing a laminated body characterized by at least a light diffusion control film derived from a composition for a light diffusion control film. A laminated body in a state where an overlying laminated film is laminated on one side, and the light diffusion control film has an internal structure having a plurality of high refractive index regions in a low refractive index region and the high refractive index region extends in a thickness direction, and is a layer In the laminated surface of the composite, the moving direction when forming the light diffusion control film is set to the long side direction, the direction perpendicular to the long side direction is set to the short side direction, and the short side direction of the overlying laminated film is to be set. When the maximum value of the measured phase difference Re (nm) is set to Re max and the minimum value is set to Re min , the following relational expression (1) is satisfied, (Re max -Re min ) / (Re max + Re min ) × 100 <35 (%) (1). That is, according to the laminated body of the present invention, since the deviation of the phase difference Re measured along a specific direction in the surface of the overlying laminated film is set to a value within a specific range, the composition for a film for controlling a film by light diffusion is used. The formed coating layer is hardened in a state where the overlying laminated film is laminated, and a laminated body of the light diffusion control film and the overlying laminated film with uniform light diffusion characteristics regardless of the location within the film surface can be obtained. [0012] In forming the laminate of the present invention, the length in the short-side direction of the overlying laminate film is preferably a value in the range of 100 to 10,000 mm. With such a configuration, a laminate having a sufficient length in the short-side direction can be obtained, and a light diffusion control film having a sufficient length in the short-side direction can be obtained. [0013] In the case where the laminated body of the present invention is configured, the central value of the phase difference Re of the overlying laminated film is preferably a value in the range of 1000 to 3000 nm. With such a configuration, it is possible to effectively suppress occurrence of a region in the light diffusion control film in which an internal structure is not formed. [0014] When forming the laminate of the present invention, the film thickness of the overlying laminated film is preferably a value in a range of 5 to 5000 μm. With such a configuration, the overlying laminated film that satisfies the relationship (1) can be obtained in a stable manner. [0015] In the case where the laminate of the present invention is configured, the internal structure of the light diffusion control film is preferably contained in a region having a relatively low refractive index, and a plurality of columns having a relatively high refractive index are formed in the film thickness direction. Structure made of objects. With this configuration, a light diffusion control film having isotropic light diffusion characteristics can be obtained. [0016] In the case where the laminated body of the present invention is configured, the internal structure of the light diffusion control film preferably includes a shutter structure in which a plurality of plate-shaped regions having different refractive indexes are alternately arranged along any direction of the film surface. With this configuration, a light diffusion control film having anisotropic light diffusion characteristics can be obtained. [0017] Another aspect of the present invention is a method for manufacturing a laminate, which is characterized by the method for manufacturing a laminate described above, and includes the following steps (a) to (d). (B) a step of coating the composition for a light diffusion control film in the form of a thin film to form a coating layer; Step, (c) the step of laminating the exposed surface of the coating layer to satisfy the lamination film on the relational expression (1), (d) moving the coating layer through the overlying lamination film, The step of irradiating the cloth layer with active energy rays. That is, according to the method for manufacturing a laminated body of the present invention, the deviation of the phase difference Re measured along a specific direction in the surface of the overlying laminated film is set to a value within a specific range. Therefore, in a state where the overlying laminated film is laminated on the coating layer formed of the composition for a light diffusion control film, it is hardened (photocured) by irradiating active energy rays. As a result, it is possible to obtain a laminated body of a light diffusion control film and an overlying laminated film that are uniform in terms of light diffusion characteristics regardless of the location within the film surface.

[0019] [第1實施形態]   本發明之第1實施形態係如圖1(a)所示,於源自光擴散控制薄膜用組成物之光擴散控制薄膜10之至少一面上層合上覆層合薄膜4之狀態的層合體100。   而且,係如下特徵之層合體:光擴散控制薄膜10具有於低折射率區域14中具有複數高折射率區域12,且該高折射率區域12於厚度方向延伸之內部構造20,係層合體100之層合面內,於將形成光擴散控制薄膜10時之移動方向設為長邊方向,將與該長邊方向垂直之方向設為短邊方向,且將沿上覆層合薄膜4之短邊方向測定之相位差Re(nm)之最大值設為Remax ,最小值設為Remin 時,滿足下述關係式(1),   (Remax -Remin )/(Remax +Remin )×100<35(%) (1)。   [0020] 亦即,係如下特徵之層合體100:於光擴散控制薄膜10之至少一面上層合上覆層合薄膜4之狀態的層合體100,且光擴散控制薄膜10係由包含高折射率硬化成分(高折射率活性能量線硬化成分)及低折射率硬化成分(低折射率活性能量線硬化成分)之光擴散控制薄膜用組成物的硬化物所構成。   而且,作為硬化物之光擴散控制薄膜內,具有於折射率相對較低之區域14中具備折射率相對較高之複數區域12之內部構造20,且如圖1(b)所示,於將源自光擴散控制薄膜用組成物之塗佈層1光硬化時之該塗佈層1之移動方向MD設為長邊方向LD,將於層合體100之層合面內且與長邊方向LD垂直之方向設為短邊方向SD,且將沿上覆層合薄膜4之短邊方向SD測定之相位差Re(nm)之最大值設為Remax ,最小值設為Remin 時,滿足上述關係式(1)。   以下,參考適當圖式具體說明本發明之第1實施形態。   但,關於光擴散控制薄膜用組成物及其硬化態樣係於第2實施形態中說明。   [0021] 1.上覆層合薄膜   本發明之上覆層合薄膜係如圖1(b)所示,使源自光擴散控制薄膜用組成物之塗佈層1光硬化時之該塗佈層1之移動方向MD設為長邊方向LD,將層合體之層合面內且與長邊方向LD垂直方向設為短邊方向SD,且將沿上覆層合薄膜4之短邊方向SD測定之相位差Re(nm)之最大值設為Remax ,最小值設為Remin 時,滿足下述關係式(1)。   (Remax -Remin )/(Remax +Remin )×100<35(%) (1)   [0022] 其理由為若關係式(1)之左邊表示之相位差Re之偏差值為35%以上之值,則透過上覆層合薄膜光硬化所得之光擴散控制薄膜之內部構造會依薄膜面內之部位過度變化之故。因此難以保持薄膜面內之光擴散特性之均一性之故。   亦即,關係式(1)之左邊表示之相位差Re之偏差值之上限值更好設為30%以下之值,又更好設為25%以下之值,特加設為10%以下之值。   且,關係式(1)之左邊表示之相位差Re之偏差值越小越好,但若為過小的值,則材料選擇幅度過度受限制。   因此,關係式(1)之左邊表示之相位差Re之偏差值之下限值較好為0.1%以上之值,更好為0.5%以上之值,又更好為1%以上之值。   又,算出相位差Re的偏差時,較好沿上覆層合薄膜之短邊方向SD,以等間隔於5~100部位測定相位差Re(關於後述相位差Re之中央值亦相同)。   又,如由圖1(b)所明瞭,上覆層合薄膜之長邊方向LD及短邊方向SD與層合體之長邊方向LD及短邊方向SD一致,亦與構成層合體之光擴散控制薄膜及步驟薄片之長邊方向LD及短邊方向SD一致。   又,相位差Re可藉由薄膜之延伸處理而調整,尤其較好藉由雙軸延伸而調整。   [0023] 此處,針對上覆層合薄膜之相位差Re之偏差與光擴散控制薄膜之光擴散特性之均一性的關係簡單予以說明。   亦即,認為所照射之活性能量線之振動方向與所形成之折射率分佈構造之間有密切關係。且,活性能量線照射於上覆層合薄膜時,根據上覆層合薄膜之相位差,上覆層合薄膜之長邊方向LD與短邊方向SD之振動受到不同影響。因此,推測為產生之分歧使活性能量線之振動方向變化。   其結果,推測上覆層合薄膜下方所形成之光擴散控制薄膜之光擴散特性被上覆層合薄膜之相位差Re大為左右。因此,認為相位差Re於短邊方向SD偏差時,光擴散特性亦對應地偏差。   [0024] 又,上覆層合薄膜之相位差Re的中央值較好為1000~3000nm之範圍內之值。   其理由為若相位差Re之中央值為未達1000nm之值,則由於為相位差Re過度低之薄膜,故有材料選定困難之情況。   另一方面,若相位差Re之中央值為超過3000nm之值,則由於為相位差Re過度高之薄膜,故有材料選定困難之情況。   因此,相位差Re之中央值之下限值更好為1100nm以上之值,又更好為1200nm以上之值。   又,相位差Re之中央值之上限值更好為2800nm以下之值,又更好為2900nm以下之值。   [0025] 又,上覆層合薄膜之活性能量線照射側表面之算術平均粗糙度(Ra)較好為1~200nm之範圍內之值。   若該Ra成為未達1nm之值,則上覆層合薄膜捲出時,會有該薄膜彼此密著,剝離時之振動變大之情況。因此有該振動傳導至活性能量線照射部分,而使光擴散控制薄膜之內部構造形成精度降低之虞。   另一方面,若該Ra成為超過200nm之值,則由於表面形狀過大,故有活性能量線產生擴散而對構造形成造成阻礙之情況之故。   因此,上覆層合薄膜之算術平均粗糙度(Ra)之下限值更好為5nm以上之值,又更好為10nm以上之值。   且,上覆層合薄膜之算術平均粗糙度(Ra)之上限值更好為100nm以下之值,又更好為40nm以下之值,特佳為30nm以下。   又,作為表面粗糙度之一的算術平均粗糙度(Ra)可依據JIS B 0601:2001,以與其吻合之方式測定,亦可依據ANSI B46.1測定。   [0026] 又,上覆層合薄膜之最大隆起(Rp)較好為20~5000nm之範圍內之值。   其理由為該Rp若成為未達20nm之值,則上覆層合薄膜捲出時,有該薄膜彼此密著,剝離時之振動變大之情況。因此,有該振動傳導至活性能量線照射部分,而使光擴散控制薄膜之內部構造形成精度降低之虞。另一方面,若該Rp成為超過5000nm之值,則由於表面形狀過大,故有活性能量線產生擴散而對構造形成造成阻礙之情況之故。   因此,上覆層合薄膜之最大隆起(Rp)之下限值更好為50nm以上之值,又更好為100nm以上之值,特佳為300nm以上。   且,上覆層合薄膜之最大隆起(Rp)之上限值更好為2000nm以下之值,又更好為1000nm以下之值,特佳為600nm以下。   又,作為表面粗糙度之一的最大隆起(Rp)可依據JIS B 0601:2001,以與其吻合之方式測定,亦可依據ANSI B46.1測定。   [0027] 又,上覆層合薄膜之濁度較好成為1~25%之範圍內之值。   其理由為若濁度成為未達1%之值,則上覆層合薄膜捲出時,有該薄膜彼此密著,剝離時之振動變大之情況。因此,有該振動傳導至活性能量線照射部分,而使光擴散控制薄膜之內部構造形成精度降低之虞。   另一方面,若濁度成為超過25%之值,則由於表面形狀過大,故有活性能量線產生擴散而對構造形成造成阻礙之情況之故。   因此,上覆層合薄膜之濁度之下限值更好為3%以上之值,又更好為5%以上之值。   且,上覆層合薄膜之濁度之上限值更好為20%以下之值,又更好為15%以下之值。   [0028] 又,上覆層合薄膜之全光線透過率較好成為70~97%之範圍內之值。   其理由為若該全光線透過率成為未達70%之值,則活性能量線之透過性過於降低,而有難以效率良好地形成光擴散控制薄膜中之特定內部構造之情況。另一方面,若該全光線透過率成為超過97%之值,則有材料選擇幅度過於受到限制之情況。   因此,上覆層合薄膜之全光線透過率之下限值更好為75%以上之值,又更好為80%以上之值。   且,上覆層合薄膜之全光線透過率之上限值更好為95%以下之值,又更好為93%以下之值。   [0029] 又,作為上覆層合薄膜之材料並未特別限制,但舉例為聚對苯二甲酸乙二酯薄膜、三乙醯基纖維素薄膜、環烯烴聚合物薄膜、環狀烯烴薄膜、離子聚合物薄膜、聚乙烯薄膜、聚氯乙烯薄膜、聚偏氯乙烯薄膜、聚乙烯醇薄膜、聚丙烯薄膜、聚酯薄膜、聚碳酸酯薄膜、聚苯乙烯薄膜、聚丙烯腈薄膜、乙烯乙酸乙烯酯共聚物薄膜、乙烯-乙烯醇共聚物薄膜、乙烯-甲基丙烯酸共聚物薄膜、尼龍薄膜、賽璐吩等,可單獨使用該等中之1種,亦可組合2種以上使用。   其理由為若為該等材料,則可更穩定地獲得滿足關係式(1)之上覆層合薄膜之故。   [0030] 又,上覆層合薄膜之短邊方向之長度較好成為100~10000mm之範圍內之值。   其理由為該短邊方向之長度成為未達100mm之值時,構成層合體之光擴散控制薄膜之短邊方向之長度亦成為未達100mm之值,而有使光擴散控制薄膜不滿足實用上要求之尺寸的情況。   另一方面,該短邊方向之長度成為超過10000mm之值時,有難以於寬度方向均一照射活性能線之情況。   因此,上覆層合薄膜之短邊方向之長度之下限值更好為200mm以上之值,又更好為300mm以上之值,特佳為600mm以上之值。   又,上覆層合薄膜之短邊方向之長度之上限值更好為8000mm以下之值,又更好為6000mm以下之值,特佳為3000mm以下之值。   [0031] 又,上覆層合薄膜之膜厚較好成為5~5000μm之範圍內之值。   其理由為該膜厚成為未達5μm之值時,處理變難,上覆層合薄膜貼合時有產生皺摺之情況之故。   另一方面,該膜厚成為超過5000μm之值時,處理變難,上覆層合薄膜搬送時有產生皺摺之情況之故。   因此,上覆層合薄膜之膜厚之下限值更好為10μm以上之值,又更好為30μm以上之值。   又,上覆層合薄膜之膜厚之上限值更好為1000μm以下之值,又更好為400μm以下之值,再更佳為100μm以下之值。   又,上覆層合薄膜之兩面中,與光擴散控制薄膜接觸之側的面亦可塗佈聚矽氧樹脂等之剝離劑而設置剝離層。   [0032] 2.光擴散控制薄膜 (1)光擴散控制薄膜之光擴散的基本原理   最初,作為本發明之光擴散控制薄膜之一例,使用圖2~3針對於薄膜內具有柱構造20a之具有等向性光擴散特性之等向性光擴散控制薄膜10a加以說明。   首先,圖2(a)顯示薄膜內具有柱構造20a之等向性光擴散控制薄膜10a之俯視圖,圖2(b)係顯示沿虛線A-A於垂直方向切斷圖2(a)所示之等向性光擴散控制薄膜10a,自箭頭方向觀看切斷面之情況的等向性光擴散控制薄膜10a之剖面圖。   又,圖3(a)顯示薄膜內具有柱構造20a之等向性光擴散控制薄膜10a之全體圖,圖3(b)係顯示藉由圖3(a)之等向性光擴散控制薄膜10a而擴散之光的擴散程度(擴散光之擴展形狀)。   如該圖2(a)之俯視圖所示,等向性光擴散控制薄膜10a具有由折射率相對較高的柱狀物12a與折射率相對較低之區域14a所成之柱構造20a。   又,如圖2(b)之剖面圖所示,於等向性光擴散控制薄膜10a之內部,具有折射率相對較高的柱狀物12a與折射率相對較低之區域14a,複數之折射率相對較高的柱狀物12a以具有特定間隔之方式以林立狀態配置。   [0033] 藉此推定為如圖3(a)所示,於入射角θ1為光擴散入射角度區域內的入射光藉由等向性光擴散控制薄膜10a而擴散。   亦即推定為如圖2(b)所示,對於等向性光擴散控制薄膜10a之入射光的入射角係自對於柱構造20a之邊界面20a’平行至特定角度範圍內之值,亦即,為光擴散入射角度區域內之值之情況,入射光(52、54)以邊變化方向邊沿膜厚方向通過柱構造20a之折射率相對較高之柱狀物12a之內部,而使出光面側之光的行進方向變得不一樣。   其結果推定為,於入射角為光擴散入射角度區域內之情況,入射光藉由等向性光擴散控制薄膜10a而擴散而成為特定之擴散光(52’、54’)。   另一方面,入射光對於等向性光擴散控制薄膜10a之入射角偏離光擴散入射角度區域之情況時,推定為如圖2(b)所示,入射光56並未藉由等向性光擴散控制薄膜10a而擴散,而是直接通過,成為透過光56’。   [0034] 藉由以上基本原理,具備柱構造20a之等向性光擴散控制薄膜10a例如如圖3(a)所示,可能發揮光之透過與擴散中之入射角依存性。   又,如圖2(b)所示,具備柱構造20a之等向性光擴散控制薄膜10a作為其光擴散特性通常成為具有「等向性」。   此處,本發明中所謂「等向性」意指如圖3(b)所示,入射光藉由薄膜而擴散時,經擴散之出射光於與薄膜平行之面內(有時稱為俯視),該光的擴散程度不因該面內之方向而變化之性質。   更具體而言,如圖3(a)所示,入射光藉由等向性光擴散控制薄膜10a而擴散時,經擴散之出射光之擴散程度於與薄膜平行之面內成為圓狀。   [0035] 又,如圖3(a)所示,等向性光擴散控制薄膜,於入射光之入射角θ1包含於光擴散入射角度區域時,即使其入射角θ1不同之情況,於出光面側亦可大致同樣地進行光擴散。   因此,等向性光擴散控制薄膜可謂具有將光集中於特定部位之聚光作用。   又,柱構造內之柱狀物12a內部之入射光之方向變化,認為除了成為如圖2(b)所示般藉由全反射而方向以直線狀鋸齒狀變化之步進指數型之情況以外,亦有成為方向以曲線狀變化之梯度指數型之情況。   [0036] 又,本發明之光擴散控制薄膜具有之內部構造若為包含高折射率區域與低折射率區域者,則不限定於上述柱構造。   亦即,光擴散控制薄膜之技術領域中,若為可藉由過去以來已知之相分離而形成之內部構造,則於本發明之光擴散控制薄膜中,亦同樣可形成。   例如,如圖4(a)所示,亦可為具有折射率不同之複數板狀區域(12b、14b)沿薄膜面沿任意一方向交互配置而成之百葉窗構造20b。   或者,亦可如圖4(b)所示,係柱狀物沿薄膜膜厚方向於中間點具有彎曲部16之彎曲柱構造20c。   或者,亦可如圖4(c)所示,係於折射率相對較低之區域14d中,折射率相對較高之複數薄片狀物12d沿薄膜面沿任意一方向排列複數行之特定內部構造20d。   或者,亦可如圖4(d)所示,係百葉窗構造20b與柱構造20a組合而成。   亦即,光擴散控制薄膜之技術領域中已知之內部構造之種類持續有多樣,但本發明之光擴散控制薄膜為該等內部構造之任一者均可。   [0037] 且,無論哪種內部構造,光擴散之基本原理均與柱構造20a之情況相同。   但,因各內部構造之形態,擴散光之擴散形狀產生差異。   例如,圖4(a)所示之百葉窗構造20b之情況,異向性光擴散之俯視中產生棒狀擴散光,於圖4(b)所示之彎曲柱構造20c時,於彎曲部之上方等向性光擴散之光的一部分於彎曲部之下方產生進而經等向性光擴散之擴散光。   又,圖4(c)所示之特定內部構造20d時,由於係百葉窗構造20b與柱構造20a之混雜型,故產生俯視下橢圓形狀之擴散光,如圖4(d)所示組合百葉窗構造20b及柱構造20a時,於柱構造20a經光擴散之光的一部分進而於百葉窗構造20b被光擴散,故而產生俯視時子彈狀之擴散光。   [0038] (2)內部構造   本發明之光擴散控制薄膜中之內部構造,若為包含高折射率區域與低折射率區域,而獲得光擴散特性者,則未特別限制,可為柱構造或百葉窗構造等之各種態樣。   以下作為一例,針對柱構造加以說明,但百葉窗構造等之其他內部構造,亦可基於有關柱構造的內容。   [0039] 如圖2(a)~(b)所示,柱構造20a為用以將入射光等向性擴散之內部構造,具體而言,係於折射率相對較低的區域中,林立折射率相對較高的複數柱狀物而成之內部構造。   [0040] (2)-1折射率   柱構造中之折射率相對較低之區域的折射率與折射率相對較高的複數柱狀物之折射率差較好為0.01以上之值。   其理由為若該折射率差成為0.01以上之值,則入射光於柱構造內全反射之角度區域變窄,故有使入射角度依存性過度降低之情況之故。   因此,該折射率差之下限值更好成為0.03以上之值,又更好為0.1以上之值。   又,該折射率差雖較大較好,但基於選定可形成柱構造之材料之觀點,認為0.3左右為上限。   [0041] (2)-2最大徑   又,於如圖2(a)~(b)所示之柱構造20a中,柱狀物之剖面中之最大徑較好成為0.1~15μm之範圍內之值。   其理由為該最大徑若為未達0.1μm之值,則儘管為入射光之入射角度,亦有難以顯示光擴散特性之情況。另一方面,該最大徑若為超過15μm之值,則於柱構造內直進的光增加,有使擴散光之均一性降低之情況之故。   因此,柱構造中,該最大徑之下限值更好為0.5μm以上之值,又更好為1μm以上之值。   且,柱構造中,該最大徑之上限值更好為10μm以下之值,又更好為5μm以下之值。   又,關於柱狀物之剖面形狀,雖未特別限定,但較好為例如圓、橢圓、多邊形、不規則形等。   且,所謂柱狀物之剖面意指藉由與薄膜表面平行之面切斷而得之剖面。   又,柱狀物之最大徑或長度等可藉由光學數位顯微鏡觀察而測定。   又,上述最大徑之數值範圍於柱狀物間之距離亦同樣。   [0042] (2)-3厚度   又,如圖2(b)所示之柱構造20a之厚度(膜厚方向之長度)較好成為10~700μm之範圍內之值。   其理由為該厚度若為未達10μm之值,則於柱構造內會直進之入射光增加,有難以獲得充分光擴散特性之範圍之情況。另一方面,若該厚度成為超過700μm之值,則對於光擴散控制薄膜用組成物照射活性能量線而形成柱構造時,因初期形成之柱構造會使光聚合之進行方向擴散,而有難以形成期望之柱構造之情況之故。   因此,柱構造之厚度下限值更好為30μm以上之值,又更好為50μm以上之值。   且,柱構造之厚度上限值更好為200μm以下之值,又更好為100μm以下之值。   又,所謂「光擴散特性之範圍」意指顯示光擴散特性之入射角的範圍及擴散光之擴大範圍。   [0043] (2)-4傾斜角   又,如圖2(b)所示,柱構造20a中,柱狀物12a等較好對於光擴散控制薄膜之膜厚方向以一定傾斜角度林立。   其理由為藉由使柱狀物之傾斜角為一定,而於柱構造內使入射光更穩定反射,可進一步提高源自柱構造之入射角度依存性之故。   更具體而言,柱構造中,柱狀物對於薄膜面之法線的傾斜角較好成為0~80°之範圍內之值。   其理由為若該傾斜角成為超過80°之值,則有伴隨此活性能量線之入射角度之絕對值亦變大,故空氣與塗佈層之界面中之活性能量線之反射比例會增加,於形成柱構造時,有產生必須照射更高照度之活性能量線之情況之故。   因此,該傾斜角度之上限值更好為60°以下之值,又更好為40°以下之值。   又,傾斜角度意指於對薄膜面垂直,且藉由將1根柱狀物全體沿軸線切斷為二的面而切斷薄膜時之剖面中所測定之對於薄膜表面之法線與柱狀物之最上部所成之角度中較窄側的角度。   [0044] (3)膜厚   又,本發明之光擴散控制薄膜之膜厚較好成為10~700μm之範圍內之值。   其理由為光擴散控制薄膜之膜厚若為未達10μm之值,則於柱構造內直進之入射光增加,有難以顯示特定之光擴散特性之情況。另一方面,若光擴散控制薄膜之膜厚成為超過700μm之值,則對於光擴散控制薄膜用組成物照射活性能量線而形成柱構造時,因初期形成之柱構造會使光聚合之進行方向擴散,而有難以形成期望之柱構造之情況之故。且應用於顯示器等時,有易於顯示圖像產生起皺之情況之故。   因此,光擴散控制薄膜之膜厚下限值更好為30μm以上之值,又更好為50μm以上之值。   且,光擴散控制薄膜之膜厚上限值更好為300μm以下之值,又更好為100μm以下之值。   [0045] (4)特性   又,有關本發明之光擴散控制薄膜之特性,濁度70%以上之入射角度區域之幅度較好處於60°以上之值。   藉由如此限制特定之入射角度區域之幅度,由於可有效率地擷取入射光,並均一擴散,故有提高擴散光之明亮度之情況。   因此,濁度70%以上之入射角度區域之幅度較好設為80°以上之值,更好設為100°以上之值。   [0046] 又,有關本發明之光擴散控制薄膜之特性,於將薄膜表面之法線方向設為0°,自入射角度區域於與該區域偏離之方向照射傾斜60°之入射光時之直進透過光強度P.T之中央值較好設為0.1~99%之範圍內之值。   其理由為若該中央值成為未達0.1%之值,則有作為薄膜全體之透過率惡化之情況。   另一方面,該中央值成為超過99%之值時,有入射角度區域不足之情況。   因此,該中央值之下限更好設為1%以上,又更好為5%以上。   且,該中央值之上限更好設為50%以下,又更好設為15%以下。   又,所謂直進透過光強度係將與入射光相同角度射出之出射光強度除以入射光全體之強度,以百分比表示者。   [0047] 又,有關本發明之光擴散控制薄膜之特性,直進透過光強度P.T之偏差較好設為0.1~3.8%之範圍內之值。   其理由為該偏差若成為未達0.1%之值,則有難以控制之情況。   另一方面,該偏差若設為超過3.8%之值,則有光擴散狀態發生濃淡之情況。   因此該偏差之下限更好設為1%以上,又更好為2%以上。   且,該偏差之上限更好設為3.5%以下,又更好設為2.8%以下。   [0048] 3.步驟薄片   又,如圖1(a)所示,本發明之層合體100亦可於光擴散控制薄膜10之一面,亦即與層合上覆層合薄膜4之側相反側之面上,層合步驟薄片2。   如此,藉由以上覆層合薄膜及步驟薄片挾持光擴散控制薄膜之兩面,而可有效地保護光擴散控制薄膜。   此處,所謂步驟薄片係製造層合體時,供光擴散控制薄膜用組成物塗佈之薄片。   作為該步驟薄片,可使用通常之剝離薄膜,舉例為例如對於聚對苯二甲酸乙二酯、聚對苯二甲酸丁二酯、聚萘二甲酸乙二酯等之聚酯薄膜、或聚丙烯、聚乙烯等之聚烯烴薄膜塗佈聚矽氧樹脂等之剝離劑而設置剝離層者。   又,該步驟薄片之膜厚通常較好設為20~150μm之範圍內之值。   [0049] [第2實施形態]   本發明之實施形態係層合體之製造方法,係第1實施形態之層合體之製造方法,其特徵為包含下述步驟(a)~(d)。   (a)準備包含高折射率活性能量線硬化成分及低折射率活性能量線硬化成分之光擴散控制薄膜用組成物之步驟,   (b)對步驟薄片膜狀塗佈光擴散控制薄膜用組成物而形成塗佈層之步驟,   (c)對於塗佈層之露出面層合滿足關係式(1)之上覆層合薄膜之步驟,   (d)邊使塗佈層移動,邊透過上覆層合薄膜,對該塗佈層照射活性能量線之步驟。   以下,以與第1實施形態不同為中心,參考適當圖式具體說明本發明之第2實施形態。   [0050] 1.步驟(a):準備光擴散控制薄膜用組成物之步驟   步驟(a)係準備特定之光擴散控制薄膜用組成物之步驟。   更具體而言,係混合以下說明之(A)~(B)成分以及依需要之其他成分的步驟。   且,混合時,可於室溫下直接攪拌,但基於提高均一性之觀點,較好於例如40~80℃之加溫條件下攪拌,成為均一混合液。   又,為成為適於塗佈之期望黏度,亦較好進而添加稀釋溶劑。   [0051] (1)(A)成分:高折射率活性能量線硬化成分   本發明之光擴散控制薄膜用組成物之特徵係包含高折射率硬化成分(高折射率活性能量線硬化成分)作為(A)成分。   其理由為藉由包含高折射率活性能量線硬化成分作為(A)成分,而與後述之作為(B)成分之低折射率硬化成分(低折射率活性能量線硬化成分)之間於聚合速度產生特定差,而抑制兩成分彼此均一共聚合,藉此可邊有效率地將(A)成分及(B)成分相分離(phase separation)邊進行硬化之故。   藉此,由於在硬化前之階段儘管為均一組成物,於硬化時亦可形成柱構造或百葉窗構造之特定內部構造,故可對作為所得硬化物之光擴散控制薄膜,賦予可效率良好地使入射光擴散之優異光擴散特性。   [0052] (1)-1折射率   作為(A)成分之高折射率活性能量線硬化成分的折射率較好成為1.5~1.65之範圍內之值。   其理由為若(A)成分之折射率成為未達1.5之值,則與作為(B)成分之低折射率活性能量線硬化成分的折射率差變得過小,而有難以獲得有效光擴散特性之情況之故。另一方面,若(A)成分之折射率成為超過1.65之值,則與(B)成分之折射率差雖變大,但有亦難以形成與(B)成分之外觀上的相溶狀態之情況之故。   因此,(A)成分之折射率之下限值更好成為1.55以上之值,又更好為1.56以上之值。   且,(A)成分之折射率之上限值更好成為1.6以下之值,又更好為1.59以下之值。   又,所謂上述之(A)成分之折射率,意指藉由光照射硬化前之(A)成分之折射率。   又,折射率可依據例如JIS K0062:1992測定。   [0053] (1)-2種類   又,(A)成分種類並未特別限制,但較好為含有複數芳香環之(甲基)丙烯酸酯。   其理由係若為該等化合物,則可更有效率地邊將(A)成分及(B)成分相分離邊進行光硬化,而可獲得更優異之光擴散特性之故。   作為此等化合物,可舉例為例如(甲基)丙烯酸聯苯酯、(甲基)丙烯酸萘酯、(甲基)丙烯酸蒽酯、(甲基)丙烯酸苄基苯酯、(甲基)丙烯酸聯苯氧基烷酯、(甲基)丙烯酸萘氧基烷酯、(甲基)丙烯酸蒽氧基烷酯、(甲基)丙烯酸苄基苯氧基烷酯、(甲基)丙烯酸鄰-苯氧基苄酯、(甲基)丙烯酸間-苯氧基苄酯、(甲基)丙烯酸對-苯氧基苄酯等,或該等之一部分藉由鹵素、烷基、烷氧基、鹵化烷基等取代者等。   又,所謂「(甲基)丙烯酸」意指丙烯酸及甲基丙烯酸兩者。   [0054] 又,作為(A)成分,更好為包含含有聯苯環之化合物,尤其更好為包含以下述通式(1)表示之聯苯化合物。   [0055][0056] (通式(1)中,R1 ~R10 係分別獨立,R1 ~R10 之至少1個為以下述通式(2)表示之取代基,其餘為氫原子、羥基、羧基、烷基、烷氧基、鹵化烷基、羥基烷基、羧基烷基及鹵原子之任一取代基)。   [0057][0058] (通式(2)中,R11 為氫原子或甲基,碳數n為1~4之整數,重複數m為1~10之整數)。   [0059] 其理由推定為藉由包含具有特定構造之聯苯化合物作為(A)成分,可於(A)成分及(B)成分之聚合速度產生特定差,使(A)成分與(B)成分之相溶性降低至特定範圍,而可使兩成分彼此之共聚合性降低之故。   又,提高源自(A)成分之折射率相對高的區域的折射率,可更容易調節將與源自(B)成分之折射率相對低的區域的折射率之差設為特定以上之值。   [0060] 又,作為以通式(1)表示之聯苯化合物之具體例可較好地舉例下述式(3)~(4)表示之化合物。   [0061][0062][0063] (2)(B)成分:低折射率活性能量線硬化成分   本發明之光擴散控制薄膜用組成物之特徵係包含低折射率活性能量線硬化成分作為(B)成分。   其理由為藉由包含低折射率活性能量線硬化成分作為(B)成分,而與上述之作為(A)成分之高折射率活性能量線硬化成分之間於聚合速度產生特定差,而抑制兩成分彼此均一共聚合,藉此可邊有效率地將(A)成分及(B)成分相分離邊進行光硬化之故。   藉此,由於於光硬化前之階段儘管為均一組成物,於光硬化時亦可形成柱構造或百葉窗構造之特定內部構造,故可對作為所得硬化物之光擴散控制薄膜,賦予可效率良好地使入射光擴散之優異光擴散特性。   [0064] (2)-1折射率   作為(B)成分之低折射率活性能量線硬化成分的折射率較好成為1.4~1.5之範圍內之值。   其理由為若(B)成分之折射率成為未達1.4之值,則與(A)成分之折射率差雖變大,但有與(A)成分之相溶性極端惡化,而難以形成特定內部構造之情況之故。另一方面,若(B)成分之折射率成為超過1.5之值,則與(A)成分之折射率差變得過小,而有難以獲得期望光擴散特性之情況之故。   因此,(B)成分之折射率之下限值更好成為1.45以上之值,又更好為1.45以上之值。   且,(B)成分之折射率之上限值更好成為1.49以下之值,又更好為1.48以下之值。   又,所謂上述之(B)成分之折射率,意指藉由光照射硬化前之(B)成分之折射率。而且,折射率如上述可依據例如JIS K0062:1992測定。   [0065] 又,上述之(A)成分的折射率與(B)成分的折射率之差較好設為0.01以上之值。   其理由為該折射率之差若成為未達0.01之值,則入射光於特定內部構造內全反射之角度變窄,故有光擴散特性之範圍變過度狹窄之情況之故。另一方面,該折射率差若成為過度大之值,則(A)成分與(B)成分之相溶性過度惡化,而有難以形成特定之內部構造之情況之故。   因此,(A)成分的折射率與(B)成分的折射率之差的下限值更好設為0.05以上之值,又更好設為0.1以上之值。   且,(A)成分的折射率與(B)成分的折射率之差的上限值更好設為0.5以下之值,又更好設為0.2以下之值。   又,此處所謂(A)成分與(B)成分的折射率意指藉由光照射硬化前之(A)成分與(B)成分之折射率。   [0066] (2)-2種類   又,(B)成分種類並未特別限制,但可舉例為例如胺基甲酸酯(甲基)丙烯酸酯、於側鏈具有(甲基)丙烯醯基之(甲基)丙烯酸系聚合物、含有(甲基)丙烯醯基之聚矽氧樹脂、不飽和聚酯樹脂等,但特佳為胺基甲酸酯(甲基)丙烯酸酯。   其理由係若為胺基甲酸酯(甲基)丙烯酸酯,則可更有效率地邊將(A)成分及(B)成分相分離邊進行光硬化,而可獲得更優異之光擴散特性之故。   又,所謂(甲基)丙烯酸酯意指丙烯酸酯及甲基丙烯酸酯兩者。   [0067] 又,胺基甲酸酯(甲基)丙烯酸酯係由(B1)含有至少2個異氰酸酯基之化合物、(B2)多元醇化合物,較好為二醇化合物,特佳為聚烷二醇、及(B3)(甲基)丙烯酸羥基烷酯所形成。   又,(B)成分為亦包含具有胺基甲酸酯鍵之重複單位的寡聚物者。   其中作為(B1)成分之含有至少2個異氰酸酯基之化合物可舉例為例如2,4-甲苯二異氰酸酯、2,6-甲苯二異氰酸酯、1,3-二甲苯二異氰酸酯、1,4-二甲苯二異氰酸酯、4,4’-二異氰酸亞甲基二苯(MDI)等之芳香族異氰酸酯、六亞甲基二異氰酸酯等之脂肪族聚異氰酸酯、異佛酮二異氰酸酯(IPDI)、氫化二苯基甲烷二異氰酸酯等之脂環式聚異氰酸酯、及該等之縮脲體、異氰脲酸酯體、進而為乙二醇、丙二醇、新戊二醇、三羥甲基丙烷、蓖麻油等之低分子含活性氫之化合物的反應物的加成物(例如二甲苯二異氰酸酯系3官能加成物)等。   [0068] 又,形成胺基甲酸酯(甲基)丙烯酸酯之成分中,作為(B2)成分的聚烷二醇舉例為例如聚乙二醇、聚丙二醇、聚丁二醇、聚己二醇等,其中,特佳為聚丙二醇。   其理由為若為聚丙二醇,則使(B)成分硬化時,可成為該硬化物中之良好軟鏈段,而可有效提高所得光擴散控制薄膜之處理性或安裝性之故。   又,(B)成分之重量平均分子量主要可藉由(B2)成分之重量平均分子量調節。此處,(B2)成分之重量平均分子量通常為2300~19500,較好為4300~14300,特佳為6300~12300。   [0069] 又,形成胺基甲酸酯(甲基)丙烯酸酯之成分中,作為(B3)成分的(甲基)丙烯酸羥基烷酯舉例為例如(甲基)丙烯酸2-羥基乙酯、(甲基)丙烯酸2-羥基丙酯、(甲基)丙烯酸3-羥基丙酯、(甲基)丙烯酸2-羥基丁酯、(甲基)丙烯酸3-羥基丁酯、(甲基)丙烯酸4-羥基丁酯等。   且,基於降低所得胺基甲酸酯(甲基)丙烯酸酯之聚合速度,更有效地形成特定內部構造之觀點,尤其更好為甲基丙烯酸羥基烷酯,又更好為甲基丙烯酸2-羥基乙酯。   [0070] (2)-3摻合量   又,將(A)成分及(B)成分之合計量設為100重量份時,(A)成分與(B)成分之摻合比((A)成分;(B)成分(重量比))較好設為20:80~80:20之範圍內之值。   亦即,將(A)成分及(B)成分之合計量設為100重量份時,(B)成分之摻合比例較好設為20~80質量份之範圍內之值。   其理由係若(B)成分之摻合比例成為未達20重量份之值,則源自(A)成分之折射率相對較高的區域幅度與源自(B)成分之折射率相對較低的區域幅度相比較,過度變大,而有難以獲得良好光擴散特性之情況之故。另一方面,若(B)成分之摻合比例成為超過80重量份之值,則(A)成分相對於(B)成分之存在比例變少,源自(A)成分之折射率相對較高的區域幅度與源自(B)成分之折射率相對較低的區域幅度相比較,過度變小,而有難以獲得良好光擴散特性之情況之故。   因此,將(A)成分及(B)成分之合計量設為100重量份時,(B)成分之摻合比例之下限值更好設為40質量份以上之值,又更好較好設為55質量份以上之值。   且,將(A)成分及(B)成分之合計量設為100重量份時,(B)成分之摻合比例之上限值更好設為70質量份以下之值,又更好較好設為65質量份以下之值。   [0071] (3)(C)成分:光聚合起始劑   又,光擴散控制薄膜用組成物中,較好含有光聚合起始劑作為(C)成分。   其理由為藉由含有光聚合起始劑,對於光擴散控制薄膜用組成物照射活性能量線時,可更有效率地邊將(A)成分及(B)成分相分離邊進行光硬化,而可獲得更優異之光擴散特性之故。   [0072] 此處,作為光聚合起始劑,舉例為苯偶因、苯偶因甲醚、苯偶因乙醚、苯偶因異丙醚、苯偶因正丁醚、苯偶因異丁醚、苯乙酮、二甲胺基苯乙酮、2,2-二甲氧基-2-苯基苯乙酮、2,2-二乙氧基-2-苯基苯乙酮、2-羥基-2-甲基-1-苯基丙烷-1-酮、1-羥基環己基苯基酮、2-甲基-1-[4-(甲硫基)苯基]-2-嗎啉基-丙烷-1-酮、4-(2-羥基乙氧基)苯基-2-(羥基-2-丙基)酮、二苯甲酮、對-苯基二苯甲酮、4,4-二乙胺基二苯甲酮、二氯二苯甲酮、2-甲基蒽醌、2-乙基蒽醌、2-第三丁基蒽醌、2-胺基蒽醌、2-甲基噻噸酮、2-乙基噻噸酮、2-氯噻噸酮、2,4-二甲基噻噸酮、2,4-二乙基噻噸酮、苄基二甲基縮醛、苯乙酮二甲基縮醛、對-二甲胺基苯甲酸酯、寡聚[2-羥基-2-甲基-1-[4-(1-甲基乙烯基)苯基]丙烷]等,可單獨使用該等中之1種,亦可組合2種以上使用。   [0073] 作為(C)成分之光聚合起始劑之摻合量,相對於(A)成分及(B)成分之合計量100質量份,較好設為0.2~20質量份之範圍內之值。   其理由係(C)成分之摻合量若成為未達0.2重量份之值,則缺乏聚合起始點,因此有難以使光擴散控制薄膜用組成物充分硬化之情況之故。另一方面,(C)成分之摻合量若成為超過20重量份之值,則有易產生光擴散控制薄膜之黃變或耐久性降低之情況之故。   因此,(C)成分之摻合量下限值更好設為0.5重量份以上之值,又更好設為1重量份以上之值。   且,(C)成分之摻合量上限值更好設為15重量份以下之值,又更好設為10重量份以下之值。   [0074] (4)其他添加劑   又,在不損及本發明效果之範圍內,亦可適當摻合其他添加劑。   作為其他添加劑舉例為例如抗氧化劑、抗靜電劑、聚合促進劑、聚合抑制劑、紅外線吸收劑、紫外線吸收劑、可塑劑、稀釋溶劑及調平劑等。   又,其他添加劑之含量,一般相對於(A)成分及(B)成分之合計量100重量份,較好設為0.01~5重量份之範圍內之值。   [0075] 且,尤其較好摻合紫外線吸收劑作為其他添加劑。   其理由為藉由摻合紫外線吸收劑,而照射活性能量線時,可於特定範圍內選擇性吸收特定波長之活性能量線之故。   其結果,不會阻礙光擴散控制薄膜用組成物之硬化,而可如例如圖4(b)所示,於所得光擴散控制薄膜之內部形成之特定內部構造產生彎曲部之故。   [0076] 又,紫外線吸收劑較好為自由羥基苯基三嗪系紫外線吸收劑、苯并三唑系紫外線吸收劑、二苯甲酮系紫外線吸收劑及羥基苯甲酸酯系紫外線吸收劑所成之群中選擇之至少一種。   其理由係若為該等紫外線吸收劑,則可於特定內部構造中更明確產生彎曲,故所得光擴散控制薄膜中之光擴散特性之範圍可更有效地擴大之故。   亦即,若為於高壓水銀燈之主波長的365nm之波長於更接近部位具有波峰之該等紫外線吸收劑,則即使為少的摻合量,亦可確認產生彎曲之故。   [0077] 且,光擴散控制薄膜用組成物中之紫外線吸收劑之摻合量,相對於(A)成分及(B)成分之合計量100重量份,較好為未達2重量份之值(但0重量份除外)。   其理由係若紫外線吸收劑之摻合量成為2重量份以上之值,則會阻礙光擴散控制薄膜用組成物之硬化,於薄膜表面產生收縮皺褶,或有無法完全硬化之情況之故。另一方面,若紫外線吸收劑之摻合量過度少,則有對於光擴散控制薄膜之內部所形成之內部構造難以產生充分彎曲之情況之故。   因此,紫外線吸收劑之摻合量下限值,相對於(A)成分及(B)成分之合計量100重量份,更好為0.01重量份以上之值,又更好為0.02重量份以上之值。   又,紫外線吸收劑之摻合量上限值,相對於(A)成分及(B)成分之合計量100重量份,更好為1.5重量份以下之值,又更好為1重量份以下之值。   [0078] 2.步驟(b):塗佈步驟   步驟(b)係如圖5(a)所示,對步驟薄片2膜狀塗佈光擴散控制薄膜用組成物而形成塗佈層1之步驟。   作為該步驟,可如第1實施形態所記載,使用通常之剝離薄膜。   [0079] 又,作為於步驟薄片上塗佈光擴散控制薄膜用組成物之方法,可使用例如棒塗佈法、刮刀塗佈法、輥塗佈法、刮板塗佈法、模嘴塗佈法、凹版塗佈法等。   又,此時之塗佈層厚度較好設為10~700μm之範圍內之值。   [0080] 3.步驟(c):層合步驟   步驟(c)係如圖5(b)所示,對塗佈層1之露出面層合滿足關係式(1)之上覆層合薄膜4之步驟。   亦即,係保有步驟薄片2與上覆層合薄膜4之間隙,以未按壓硬化前之塗佈層1之方式進行層合之步驟。   [0081] 4.步驟(d):活性能量線照射步驟   步驟(d)係如圖5(c)所示,邊使塗佈層1移動,邊透過上覆層合薄膜4,對該塗佈層1照射平行光60的活性能量線,而於薄膜內形成柱構造或百葉窗構造等之特定內部構造,作成光擴散控制薄膜10之步驟。   以下,作為一例,針對形成柱構造之情況加以說明。   [0082] 亦即,如圖5(c)所示,對於步驟薄片2上形成之塗佈層1照射光線之平行度高的平行光60。   此處,所謂平行光,意指光的行進方向於任一方向觀察時均不具有擴展之略平行之光。   更具體而言,例如如圖5(c)所示,可將來自點光源102之照射光70藉由透鏡104而作成平行光60。   [0083] 又,照射光之平行度較好設為10°以下之值。   其理由係藉由將照射光之平行度設為該範圍內之值,可有效率且穩定地形成柱構造之故。   因此,照射光之平行度更好設為5°以下之值,又更好設為2°以下之值。   [0084] 又,作為照射光之照射角,如圖6所示,於將對於塗佈層1的表面之法線的角度設為0°時之照射角θ×通常較好設為-80~80°之範圍內之值。   其理由係若照射角成為-80~80°之範圍外之值,則於塗佈層1表面之反射等的影響變大,有難以充分形成柱構造之情況之故。   又,圖6中之箭頭MD係指塗佈層之移動方向。   [0085] 又,作為活性能量線的照射光較好使用紫外線。   其理由係為電子束之情況,由於聚合速度非常快,因此於聚合過程中(A)成分與(B)成分無法充分相分離,而有難以形成柱構造之情況之故。   另一方面,與可見光相比較時,由於藉由紫外線照射而可硬化之紫外線硬化樹脂或可使用之光聚合起始劑之變化較為豐富,故可增廣(A)成分及(B)成分之選擇幅度。   [0086] 又,作為於使用紫外線作為活性能量線時之照射條件,於塗佈層表面之峰值照度較好設為0.1~10mW/cm2 之範圍內之值。   其理由為該峰值照度若為未達0.1mW/cm2 之值,則有難以明確形成柱構造之情況之故。另一方面,該峰值照度若為超過10mW/cm2 之值,則推定為硬化速度過快,而有難以有效形成柱構造之情況之故。   因此,塗佈層表面之峰值照度之下限值更好設為0.3mW/cm2 以上之值,又更好設為0.5mW/cm2 以上之值。   又,塗佈層表面之峰值照度之上限值更好設為8mW/cm2 以下之值,又更好設為6mW/cm2 以下之值。   [0087] 又,於使用紫外線作為活性能量線時之塗佈層表面之累積光量較好設為5~200mJ/cm2 之範圍內之值。   其理由為該累積光量若為未達5mJ/cm2 之值,則有難以使柱構造自上方向下方充分伸長之情況之故。另一方面,該累積光量若為超過200mJ/cm2 之值,則有所得光擴散控制薄膜產生著色之情況之故。   因此,塗佈層表面之累積光量下限值更好設為7mJ/cm2 以上之值,又更好設為10mJ/cm2 以上之值。   且,塗佈層表面之累積光量上限值更好設為150mJ/cm2 以下之值,又更好設為100mJ/cm2 以下之值。   [0088] 又,基於維持量產性並且穩定地形成柱構造之觀點,照射紫外線作為活性能量線照射時,步驟薄片上形成之塗佈層較好以0.1~10m/分鐘之範圍內之速度移動。   尤其更好以0.2m/分鐘以上之速度移動,且更好以3m/分鐘以下之速度移動。   [0089] 又,本發明中,使光擴散控制薄膜用組成物硬化而成之光擴散控制薄膜內形成之內部構造若為包含高折射率區域及低折射率區域者,則並未限制於上述柱構造。   例如形成如圖4(a)所示之百葉窗構造20b時,只要對於步驟薄片2上形成之塗佈層1,照射於一方向觀看時實質上為平行光且自其他方向觀看時看似非平行之雜亂光的光作為照射光即可。   又,形成如圖4(c)所示之特定內部構造20d時,只要對於步驟薄片2上形成之塗佈層1,照射於一方向觀看時實質上為平行光且自其他方向觀看時並非全部為雜亂光而是經調節至某程度平行度的光即可。 [實施例]   [0090] 以下藉由實施例更詳細說明本發明。但本發明不限定於該等記載。   [0091] [實施例1] 1.上覆層合薄膜之準備   準備厚度38μm、短邊方向(寬度方向)之長度1000mm之雙軸延伸聚對苯二甲酸乙二酯薄膜捲筒(以下有時稱「薄膜A」)作為上覆層合薄膜。   [0092] (1)相位差Re之測定   測定所準備之上覆層合薄膜之相位差Re。   亦即,將所準備之上覆層合薄膜之長邊方向中任意部位作為測定部位予以特定。   其次,於經特定之測定部位中沿短邊方向1000mm,每50mm共20個部位作為測定點,使用王子測量機器(股)製之相位差測定裝置KOBRA-WR,測定相位差Re(nm)。所得結果示於圖7之特性曲線A。   該圖7係以橫軸作為上覆層合薄膜之短邊方向的位置(mm),縱軸作為相位差Re(nm)的短邊方向位置-相位差Re圖表。   且,由所得測定值,算出相位差Re之中央值(nm)及以式(1)表示之偏差((Remax -Remin )/(Remax +Remin )×100)(%)。所得結果示於表1。   [0093] (2)表面粗糙度Rp及Ra   又,測定所準備之上覆層合薄膜之算術平均粗糙度(Ra)及最大隆起(Rp)。   亦即,使用Veeco公司製之表面形狀測定裝置WYKO NT110 (ANSI B46.1規格),測定所準備之上覆層合薄膜之算術平均粗糙度(Ra)(nm),並且測定最大隆起(Rp)(nm)。所得結果示於表1。   [0094] (3)濁度及全光線透過率之測定   又,測定所準備之上覆層合薄膜之濁度。   亦即,使用日本電色工業(股)製之濁度計NDH 5000,測定所準備之上覆層合薄膜之濁度(%)及全光線透過率。所得結果示於表1。   [0095] 2.低折射率活性能量線硬化成分之合成   於容器內對於作為(B2)成分之重量平均分子量9200之聚丙二醇(PPG) 1莫耳,收納作為(B1)成分之異佛酮二異氰酸酯(IPDI) 2莫耳及作為(B3)成分之甲基丙烯酸2-羥基乙酯(HEMA) 2莫耳後,依據常用方法進行反應,獲得作為(B)成分之重量平均分子量9900之聚醚胺基甲酸酯甲基丙烯酸酯。   [0096] 又,聚丙二醇及聚醚胺基甲酸酯甲基丙烯酸酯之重量平均分子量係藉凝膠滲透層析(GPC)按下述條件測定之聚苯乙烯換算值。   .GPC測定裝置:TOSOH(股)製,HLC-8020   .GPC管柱:TOSOH(股)製(以下記載為通過順序)     TSK防護管柱HXL-H     TSK gel GMHXL(×2)     TSK gel G2000HXL   .測定溶劑:四氫呋喃   .測定溫度:40℃   [0097] 3.光擴散控制薄膜用組成物之調製   其次,添加作為(A)成分之上述式(3)表示之分子量268之丙烯酸鄰-苯基苯氧基乙氧基乙酯(新中村化學(股)製,NK ESTER A-LEN-10) 62.5重量份及經合成之作為(B)成分之重量平均分子量9900之聚醚胺基甲酸酯甲基丙烯酸酯37.5重量份、對於(A)成分及(B)成分之合計量=100重量份之作為(C)成分之2-羥基-2-甲基-1-苯基丙烷-1-酮1.25重量份後,於80℃之條件下進行加熱混合,獲得光擴散控制薄膜用組成物。   又,(A)成分及(B)成分之折射率係使用阿貝折射計(ATAGO(股)製,阿貝折射計DR-M2,Na光源,波長589nm),依據JIS K0062測定後,分別為1.58及1.46。   [0098] 4.塗佈步驟   其次,邊將短邊方向長度1000mm之施以剝離處理之作為步驟薄片之透明聚對苯二甲酸乙二酯捲筒拉出邊於其剝離處理面塗佈所得之光擴散控制薄膜用組成物,形成膜厚60μm之塗佈層。   [0099] 5.層合步驟   其次,對於塗佈層之露出面側,藉由輥對輥層合所準備之上覆層合薄膜。   其次,如圖5(c)所示,使用中心光線平行度控制於±3°以內之紫外線點平行光源(JATEC(股)製),將平行度為2°以下之平行光以圖6所示之照射角θx大致成為10°之方式,對塗佈層照射。   此時之峰值照度設為2.00mW/cm2 ,累積光量設為53.13mJ/cm2 ,燈高度設為1480mm,塗佈層之移動速度設為1.0m/分鐘。   又,上述峰值照度及累積光量係將安裝有受光器之UV計(EYE GRAPHIC(股)製,EYE紫外線累積照度計UVPF-A1)設置於塗佈層之位置而測定。   又,光擴散控制薄膜之膜厚係使用定壓厚度測定器(寶製作所(股)製,TECLOCK PG-02J)測定。   [0100] 又,具有所得柱構造之光擴散控制薄膜於與塗佈層移動方向平行且與薄膜面正交之面切斷之剖面相片示於圖8(a)。   又,膜厚方向之柱構造之長度為60μm,其傾斜角為 7°。   且,光擴散控制薄膜之切斷係使用剃刀進行,剖面照片之拍攝係使用keyence製,數位顯微鏡VHX-1000藉由反射觀察而進行。   [0101] 6.評價   (1)變角濁度之測定   測定所得光擴散控制薄膜之變角濁度。   亦即自所得步驟薄片/光擴散控制薄膜/上覆層合薄膜層合體之任意部位,切出沿長邊方向之短條狀試驗片(120mm寬),使用東洋精機製作所(股)製,Haze Gard Plus測定變角濁度(%)。   此時,將積分球開口與光擴散控制薄膜之距離設為62mm,參考光之入射點設為試驗片之光擴散控制薄膜之短邊方向之中心點。   又,如圖9(a)所示,參考光係自試驗片之步驟薄片側入射,且使參考光之入射角度沿光擴散控制薄膜之長邊方向變化進行測定。所得結果示於圖9(b)之特性曲線A。   該圖9(b)係以橫軸作為參考光之入射角度(°),縱軸作為變角濁度(%)之入射角度-變角濁度圖表。又,自圖9(b)算出濁度70%以上之入射角度區域之幅度,並示於表1。   因此,由特性曲線A,可確認光擴散程度隨入射角度而異之性質,亦即入射角度依存性(特性曲線B:實施例2,特性曲線C:比較例1亦同)。   [0102] (2)直進透過光強度P.T之測定   測定所得光擴散控制薄膜之直進透過光強度。   亦即,沿與變角濁度測定所用者同樣之試驗片之短邊方向1000mm,每50mm共20部位作為測定點,使用SUGA試驗機(股)製,變角測色計VC-2,測定直進透過光強度P.T(%)。   此時,如圖10(a)所示,對於試驗片之步驟薄片側,自光擴散控制薄膜之柱狀物傾斜方向相反向傾斜60°之方向入射光而測定。所得結果示於圖10(b)之特性曲線A。   該圖10(b)係橫軸為光擴散控制薄膜之短邊方向的位置(mm),縱軸為直進透過光強度(%)之短邊方向位置-直進透過光強度圖表。   又,由所得測定值,算出直進透過光強度P.T之中央值(%)及以式(1)表示之偏差((P.Tmax -P.Tmin )/(P.Tmax +P.Tmin )×100)(%)。所得結果示於表1。   [0103] [實施例2]   實施例2中,除了作為上覆層合薄膜係使用具有表1所示之相位差Re及表面粗糙度之厚度38μm、短邊方向之長度1000mm之雙軸延伸聚對苯二甲酸乙二酯捲筒(以下有時稱為薄膜B)以外,與實施例1同樣製造層合體並評價。   所得結果分別示於表1、圖8(b)、圖9(b)之特性曲線B及圖10(b)之特性曲線B。   [0104] [比較例1]   比較例1中,除了作為上覆層合薄膜係使用具有表1所示之相位差Re及表面粗糙度之厚度75mm、短邊方向之長度1000mm之雙軸延伸聚對苯二甲酸乙二酯捲筒(以下有時稱為「薄膜C」)以外,與實施例1同樣製造層合體並評價。   所得結果分別示於表1、圖8(b)、圖9(b)之特性曲線C及圖10(b)之特性曲線C。   [0105][產業上之可利用性]   [0106] 如以上所詳述,依據本發明,藉由將上覆層合薄膜面內之沿特定方向測定之相位差的偏差設為特定範圍內之值,即使於未發生未形成內部構造區域之情況,或發生之情況,均可均一形成內部構造。   其結果,可獲得光擴散特性不管薄膜面內部位為何均為均一的光擴散控制薄膜。   因此,藉由本發明所得之光擴散控制薄膜期待可顯著有助於液晶顯示裝置或投影螢幕等之高品質化。[First Embodiment] As shown in FIG. 1 (a), a first embodiment of the present invention is such that a cover layer is laminated on at least one side of a light diffusion control film 10 derived from a composition for a light diffusion control film. The laminated body 100 in the state of the laminated film 4. Further, the light diffusion control film 10 has an internal structure 20 having a plurality of high-refractive-index regions 12 in the low-refractive-index region 14 and the high-refractive-index region 12 extending in the thickness direction, and is a laminate 100 In the lamination plane, the moving direction when the light diffusion control film 10 is formed is set to the long side direction, the direction perpendicular to the long side direction is set to the short side direction, and the length along the short side of the overlying laminated film 4 is set. When the maximum value of the phase difference Re (nm) measured in the lateral direction is set to Re max and the minimum value is set to Re min , the following relational expression (1) is satisfied, (Re max -Re min ) / (Re max + Re min ) × 100 <35 (%) (1). [0020] That is, the laminated body 100 has the following characteristics: the laminated body 100 in a state where the laminated film 4 is laminated on at least one side of the light diffusion control film 10, and the light diffusion control film 10 includes a high refractive index The hardened component (high refractive index active energy ray hardened component) and the low refractive index hardened component (low refractive index active energy ray hardened component) are composed of a cured product of a composition for a light diffusion control film. Further, the light diffusion control film as a hardened material has an internal structure 20 including a plurality of regions 12 having a relatively high refractive index in a region 14 having a relatively low refractive index, and as shown in FIG. 1 (b), The direction of movement MD of the coating layer 1 derived from the coating layer 1 of the composition for a light diffusion control film during light curing is set to the longitudinal direction LD, and it will be in the lamination plane of the laminate 100 and in the longitudinal direction LD. The vertical direction is set to the short-side direction SD, and the maximum value of the phase difference Re (nm) measured along the short-side direction SD of the overlying laminated film 4 is set to Re max and the minimum value is set to Re min , which satisfies the above. Relationship (1). Hereinafter, a first embodiment of the present invention will be specifically described with reference to appropriate drawings. However, the composition for a light diffusion control film and its hardened state will be described in the second embodiment. [0021] 1. Overlay Laminated Film The overlaminated film of the present invention is shown in FIG. 1 (b), which is applied when the coating layer 1 derived from the composition for a light diffusion control film is light cured. The moving direction MD of layer 1 is set to the long-side direction LD, the direction of lamination within the laminate plane and perpendicular to the long-side direction LD is set to the short-side direction SD, and the short-side direction SD of the overlying laminated film 4 is set When the maximum value of the measured phase difference Re (nm) is set to Re max and the minimum value is set to Re min , the following relational expression (1) is satisfied. (Re max -Re min ) / (Re max + Re min ) × 100 <35 (%) (1) The reason is that if the deviation value of the phase difference Re shown on the left side of the relationship (1) is 35% The above values cause the internal structure of the light diffusion control film obtained by photocuring through the overlying laminated film to be excessively changed depending on the location within the film surface. Therefore, it is difficult to maintain the uniformity of the light diffusion characteristics in the film plane. That is, the upper limit value of the deviation value of the phase difference Re shown on the left side of the relational expression (1) is more preferably set to a value of 30% or less, more preferably set to a value of 25% or less, and more specifically set to 10% or less. Value. In addition, the smaller the deviation value of the phase difference Re shown on the left side of the relational expression (1), the better, but if it is too small, the material selection range is excessively limited. Therefore, the lower limit of the deviation value of the phase difference Re shown on the left side of the relational expression (1) is preferably a value of 0.1% or more, more preferably a value of 0.5% or more, and still more preferably a value of 1% or more. When calculating the deviation of the retardation Re, it is preferable to measure the retardation Re at equally spaced positions from 5 to 100 along the short-side direction SD of the overlying laminated film (the same applies to the central value of the retardation Re described later). In addition, as is clear from FIG. 1 (b), the long-side direction LD and short-side direction SD of the overlying laminated film are consistent with the long-side direction LD and short-side direction SD of the laminate, and also the light diffusion constituting the laminate. The long-side direction LD and the short-side direction SD of the control film and the step sheet are the same. The phase difference Re can be adjusted by stretching the film, and is particularly preferably adjusted by biaxial stretching. [0023] Here, the relationship between the deviation of the phase difference Re of the overlying laminated film and the uniformity of the light diffusion characteristics of the light diffusion control film will be briefly described. That is, it is considered that there is a close relationship between the vibration direction of the irradiated active energy rays and the refractive index distribution structure formed. In addition, when the active energy ray is irradiated to the overlying laminated film, the vibration in the long-side direction LD and the short-side direction SD of the overlying laminated film is affected differently according to the phase difference of the overlying laminated film. Therefore, it is presumed that the divergence caused changes the vibration direction of the active energy ray. As a result, it is presumed that the light diffusion characteristics of the light diffusion control film formed under the overlying laminated film is approximately controlled by the phase difference Re of the overlying laminated film. Therefore, it is considered that when the phase difference Re deviates from the short-side direction SD, the light diffusion characteristics also deviate correspondingly. [0024] The median value of the phase difference Re of the overlying laminated film is preferably a value in the range of 1000 to 3000 nm. The reason is that if the median value of the retardation Re is less than 1000 nm, the material may be difficult to select because it is a thin film with an excessively low retardation Re. On the other hand, if the central value of the phase difference Re exceeds 3,000 nm, it may be difficult to select a material because it is a thin film with an excessively high phase difference Re. Therefore, the lower limit of the median value of the phase difference Re is more preferably a value of 1100 nm or more, and more preferably a value of 1200 nm or more. The upper limit of the median value of the phase difference Re is more preferably a value of 2800 nm or less, and even more preferably a value of 2900 nm or less. [0025] The arithmetic mean roughness (Ra) of the surface of the active energy ray-irradiated side of the overlying laminated film is preferably a value in a range of 1 to 200 nm. If the Ra value is less than 1 nm, when the overlying laminate film is rolled out, the films may adhere to each other, and vibration during peeling may increase. Therefore, the vibration may be transmitted to the active energy ray irradiated portion, and the formation accuracy of the internal structure of the light diffusion control film may be reduced. On the other hand, if this Ra has a value exceeding 200 nm, the surface shape is too large, and therefore the active energy rays may be diffused to prevent the formation of the structure. Therefore, the lower limit of the arithmetic average roughness (Ra) of the overlying laminated film is more preferably a value of 5 nm or more, and more preferably a value of 10 nm or more. In addition, the upper limit of the arithmetic mean roughness (Ra) of the overlying laminated film is preferably a value of 100 nm or less, more preferably a value of 40 nm or less, and particularly preferably 30 nm or less. The arithmetic mean roughness (Ra), which is one of the surface roughnesses, can be measured in accordance with JIS B 0601: 2001, or can be measured in accordance with ANSI B46.1. [0026] The maximum ridge (Rp) of the overlying laminated film is preferably a value in a range of 20 to 5000 nm. The reason is that if the Rp value is less than 20 nm, when the overlying laminate film is rolled out, the films may adhere to each other and vibrations during peeling may increase. Therefore, the vibration may be transmitted to the active energy ray irradiated portion, and the internal structure formation accuracy of the light diffusion control film may be reduced. On the other hand, if the Rp exceeds a value of more than 5000 nm, the surface shape is too large, which may cause diffusion of the active energy rays and hinder the formation of the structure. Therefore, the lower limit of the maximum ridge (Rp) of the overlying laminated film is more preferably a value of 50 nm or more, more preferably a value of 100 nm or more, and particularly preferably 300 nm or more. In addition, the upper limit of the maximum ridge (Rp) of the overlying laminated film is preferably a value of 2000 nm or less, more preferably a value of 1000 nm or less, and particularly preferably 600 nm or less. The maximum ridge (Rp), which is one of the surface roughness, can be measured in accordance with JIS B 0601: 2001, or it can be measured according to ANSI B46.1. [0027] The turbidity of the overlying laminated film is preferably a value in a range of 1 to 25%. The reason is that if the turbidity is less than 1%, when the overlying laminated film is rolled out, the films may adhere to each other and the vibration during peeling may increase. Therefore, the vibration may be transmitted to the active energy ray irradiated portion, and the internal structure formation accuracy of the light diffusion control film may be reduced. On the other hand, if the turbidity exceeds a value of 25%, the surface shape is too large, which may cause diffusion of the active energy rays and hinder the formation of the structure. Therefore, the lower limit of the turbidity of the overlying laminated film is more preferably a value of 3% or more, and more preferably a value of 5% or more. The upper limit of the turbidity of the overlying laminated film is more preferably a value of 20% or less, and even more preferably a value of 15% or less. [0028] The total light transmittance of the overlying laminated film is preferably a value in a range of 70 to 97%. The reason is that if the total light transmittance is less than 70%, the transmittance of the active energy ray is too low, and it may be difficult to efficiently form a specific internal structure in the light diffusion control film. On the other hand, if the total light transmittance exceeds a value of 97%, the material selection range may be too limited. Therefore, the lower limit of the total light transmittance of the overlying laminated film is more preferably a value of 75% or more, and more preferably a value of 80% or more. In addition, the upper limit of the total light transmittance of the overlying laminated film is more preferably a value of 95% or less, and even more preferably a value of 93% or less. [0029] In addition, the material used as the overlying laminated film is not particularly limited, but examples include polyethylene terephthalate film, triethyl cellulose film, cyclic olefin polymer film, cyclic olefin film, Ionic polymer film, polyethylene film, polyvinyl chloride film, polyvinylidene chloride film, polyvinyl alcohol film, polypropylene film, polyester film, polycarbonate film, polystyrene film, polyacrylonitrile film, ethylene acetic acid The vinyl ester copolymer film, ethylene-vinyl alcohol copolymer film, ethylene-methacrylic acid copolymer film, nylon film, and cellophane can be used alone or in combination of two or more. The reason is that if these materials are used, a laminated film satisfying the relational expression (1) can be obtained more stably. [0030] The length in the short-side direction of the overlying laminated film is preferably a value in a range of 100 to 10,000 mm. The reason is that when the length in the short-side direction is less than 100 mm, the length in the short-side direction of the light diffusion control film constituting the laminate also becomes less than 100 mm, and the light-diffusion control film does not satisfy the practical requirements. Case of required size. On the other hand, when the length in the short side direction exceeds a value of 10,000 mm, it may be difficult to uniformly irradiate the active energy rays in the width direction. Therefore, the lower limit of the length in the short-side direction of the overlying laminated film is more preferably a value of 200 mm or more, more preferably a value of 300 mm or more, and particularly preferably a value of 600 mm or more. In addition, the upper limit value of the length in the short-side direction of the overlying laminated film is more preferably a value of 8000 mm or less, still more preferably a value of 6000 mm or less, and particularly preferably a value of 3000 mm or less. [0031] The film thickness of the overlying laminated film is preferably a value in a range of 5 to 5000 μm. The reason is that when the film thickness is less than 5 μm, handling becomes difficult, and wrinkles may occur when the overlaminate film is bonded. On the other hand, when the film thickness exceeds a value of 5000 μm, handling becomes difficult, and wrinkles may occur when the overlaminate film is transferred. Therefore, the lower limit of the film thickness of the overlying laminated film is more preferably a value of 10 μm or more, and more preferably a value of 30 μm or more. The upper limit of the film thickness of the overlying laminated film is more preferably a value of 1000 μm or less, still more preferably a value of 400 μm or less, and even more preferably a value of 100 μm or less. In addition, on both surfaces of the overlying laminate film, a surface on the side in contact with the light diffusion control film may be coated with a release agent such as silicone resin to provide a release layer. [0032] 2. Light diffusion control film (1) Basic principle of light diffusion of light diffusion control film Initially, as an example of the light diffusion control film of the present invention, the use of FIGS. The isotropic light diffusion control film 10a having isotropic light diffusion characteristics will be described. First, FIG. 2 (a) shows a top view of an isotropic light diffusion control film 10a having a pillar structure 20a in the film, and FIG. 2 (b) shows a vertical cut along the dotted line AA and the like shown in FIG. 2 (a) A cross-sectional view of the isotropic light diffusion control film 10a when the cut surface is viewed from the direction of the arrow. Fig. 3 (a) shows an overall view of an isotropic light diffusion control film 10a having a pillar structure 20a in the film, and Fig. 3 (b) shows an isotropic light diffusion control film 10a shown in Fig. 3 (a). The degree of diffusion of the diffused light (the expanded shape of the diffused light). As shown in the top view of FIG. 2 (a), the isotropic light diffusion control film 10a has a pillar structure 20a formed of a pillar 12a having a relatively high refractive index and a region 14a having a relatively low refractive index. As shown in the cross-sectional view of FIG. 2 (b), inside the isotropic light diffusion control film 10a, there are pillars 12a having a relatively high refractive index and regions 14a having a relatively low refractive index. The relatively high rate of the pillars 12a are arranged in a standing state so as to have a certain interval. [0033] It is thus estimated that as shown in FIG. 3 (a), the incident light in the region where the incident angle θ1 is a light diffusion incident angle is diffused by the isotropic light diffusion control film 10a. That is, as shown in FIG. 2 (b), the incident angle of the incident light to the isotropic light diffusion control film 10a is a value parallel to a specific angle range from the boundary surface 20a 'of the pillar structure 20a, that is, Is the value in the area of the incident angle of light diffusion. The incident light (52, 54) passes through the inside of the pillar 12a with a relatively high refractive index in the pillar structure 20a along the film thickness direction while changing the direction, so that the light exit side The direction of light travel is different. As a result, it is estimated that when the incident angle is within the light diffusion incident angle region, the incident light is diffused by the isotropic light diffusion control film 10a to become specific diffused light (52 ', 54'). On the other hand, when the incident angle of the incident light to the isotropic light diffusion control film 10a deviates from the light diffusion incident angle region, it is estimated as shown in FIG. 2 (b), and the incident light 56 does not pass through the isotropic light. The diffusion control film 10a diffuses and passes directly, and becomes transmitted light 56 '. [0034] Based on the above basic principle, the isotropic light diffusion control film 10a having the pillar structure 20a, for example, as shown in FIG. 3 (a), may exhibit the dependence of the incident angle on the transmission and diffusion of light. Moreover, as shown in FIG. 2 (b), the isotropic light diffusion control film 10a provided with the pillar structure 20a generally has "isotropic property" as its light diffusion characteristic. Herein, the "isotropic" in the present invention means that as shown in FIG. 3 (b), when incident light is diffused through a thin film, the diffused outgoing light is in a plane parallel to the thin film (sometimes referred to as a top view) ), A property that the degree of diffusion of the light does not change due to the direction in the plane. More specifically, as shown in FIG. 3 (a), when the incident light is diffused by the isotropic light diffusion control film 10a, the diffusion degree of the emitted light becomes circular in a plane parallel to the film. [0035] In addition, as shown in FIG. 3 (a), when the incident light angle θ1 of the isotropic light diffusion control film is included in the light diffusion incident angle region, even if the incident angle θ1 is different, it is on the light exit surface. The side can also perform light diffusion in substantially the same manner. Therefore, an isotropic light-diffusion control film can be said to have a light-concentrating effect of concentrating light on a specific portion. In addition, it is considered that the direction of incident light inside the columnar object 12a in the column structure is changed to a step-exponential type in which the direction changes in a linear zigzag manner by total reflection as shown in FIG. 2 (b). There are also cases where the gradient index type changes in a curve shape. [0036] The internal structure of the light diffusion control film of the present invention is not limited to the above-mentioned pillar structure as long as the internal structure includes a high refractive index region and a low refractive index region. That is, in the technical field of the light diffusion control film, if it has an internal structure that can be formed by phase separation known in the past, it can also be formed in the light diffusion control film of the present invention. For example, as shown in FIG. 4 (a), the shutter structure 20b may be a louver structure 20b having a plurality of plate-like regions (12b, 14b) having different refractive indices alternately arranged along the film surface in any one direction. Alternatively, as shown in FIG. 4 (b), the columnar object may have a curved column structure 20c having a curved portion 16 at an intermediate point in the film thickness direction. Alternatively, as shown in FIG. 4 (c), in a region 14d having a relatively low refractive index, a plurality of thin sheet objects 12d having a relatively high refractive index are arranged along a film surface in a plurality of rows in a specific internal structure. 20d. Alternatively, as shown in FIG. 4 (d), the blind structure 20b and the pillar structure 20a may be combined. That is, the types of internal structures known in the technical field of light diffusion control films continue to be diverse, but the light diffusion control film of the present invention may be any of these internal structures. [0037] Moreover, the basic principle of light diffusion is the same as in the case of the pillar structure 20a, regardless of the internal structure. However, due to the shape of each internal structure, the shape of the diffused light is different. For example, in the case of the louver structure 20b shown in FIG. 4 (a), a rod-shaped diffused light is generated in a plan view of the anisotropic light diffusion, and when the curved column structure 20c shown in FIG. 4 (b) is above the curved portion Part of the light diffused by the isotropic light is generated below the bent portion, and the diffused light is diffused by the isotropic light. In addition, when the specific internal structure 20d shown in FIG. 4 (c) is a hybrid type of the blind structure 20b and the column structure 20a, diffused light with an oval shape in a plan view is generated, as shown in FIG. 4 (d). In the case of 20b and the pillar structure 20a, a part of the light diffused by the pillar structure 20a is further diffused by the light in the louver structure 20b, so that bullet-like diffused light is generated when viewed from above. [0038] (2) Internal structure The internal structure in the light diffusion control film of the present invention is not particularly limited as long as it includes a high refractive index region and a low refractive index region to obtain light diffusion characteristics, and may be a pillar structure or Various aspects of shutter structure. The pillar structure is described below as an example, but other internal structures such as the shutter structure may also be based on the contents of the pillar structure. [0039] As shown in FIGS. 2 (a) to 2 (b), the pillar structure 20a is an internal structure for isotropically diffusing incident light. Specifically, the pillar structure 20a is located in a relatively low refractive index area, and has a large amount of refraction. An internal structure with a relatively high rate of multiple pillars. [0040] (2) The refractive index difference between the relatively low refractive index region in the refractive index column structure and the relatively high refractive index of the plurality of pillars is preferably a value of 0.01 or more. The reason is that if the refractive index difference becomes a value of 0.01 or more, the angular region of total reflection of incident light in the column structure becomes narrow, so that the incident angle dependency may be excessively reduced. Therefore, the lower limit of the refractive index difference is more preferably a value of 0.03 or more, and more preferably a value of 0.1 or more. In addition, although this difference in refractive index is large and good, from the viewpoint of selecting a material that can form a pillar structure, about 0.3 is considered to be the upper limit. [0041] (2) -2 Maximum diameter. In the pillar structure 20a shown in FIGS. 2 (a) to (b), the maximum diameter in the cross section of the pillar is preferably within a range of 0.1 to 15 μm. value. The reason is that if the maximum diameter is less than 0.1 μm, it may be difficult to display the light diffusion characteristics in spite of the incident angle of incident light. On the other hand, if the maximum diameter exceeds a value of 15 μm, the amount of light traveling straight in the column structure may increase, which may reduce the uniformity of the diffused light. Therefore, in the column structure, the lower limit of the maximum diameter is more preferably a value of 0.5 μm or more, and more preferably a value of 1 μm or more. In the column structure, the upper limit of the maximum diameter is more preferably a value of 10 μm or less, and even more preferably a value of 5 μm or less. The cross-sectional shape of the pillar is not particularly limited, but is preferably, for example, a circle, an ellipse, a polygon, or an irregular shape. The cross-section of the pillar means a cross-section obtained by cutting a plane parallel to the film surface. The maximum diameter, length, and the like of the pillars can be measured by observation with an optical digital microscope. The same applies to the distance between the pillars in the numerical range of the maximum diameter. (2) -3 Thickness The thickness (length in the film thickness direction) of the pillar structure 20a shown in FIG. 2 (b) is preferably a value in the range of 10 to 700 μm. The reason is that if the thickness is less than 10 μm, incident light that goes straight in the column structure increases, and it may be difficult to obtain a range of sufficient light diffusion characteristics. On the other hand, if the thickness is more than 700 μm, when the composition for a light diffusion control film is irradiated with active energy rays to form a pillar structure, the pillar structure formed initially may diffuse the direction of photopolymerization, making it difficult to diffuse. The reason for the formation of the desired pillar structure. Therefore, the lower limit of the thickness of the pillar structure is more preferably a value of 30 μm or more, and more preferably a value of 50 μm or more. The upper limit of the thickness of the pillar structure is more preferably a value of 200 μm or less, and even more preferably a value of 100 μm or less. The "range of light diffusion characteristics" means the range of the incident angle showing the light diffusion characteristics and the expanded range of the diffused light. (2) -4 Inclination angle As shown in FIG. 2 (b), in the pillar structure 20a, the pillars 12a and the like preferably stand at a certain inclined angle with respect to the film thickness direction of the light diffusion control film. The reason is that by making the inclination angle of the pillars constant and reflecting the incident light more stably within the pillar structure, the dependency of the incident angle from the pillar structure can be further improved. More specifically, in the column structure, the inclination angle of the column with respect to the normal of the film surface is preferably a value in a range of 0 to 80 °. The reason is that if the inclination angle exceeds 80 °, the absolute value of the incident angle accompanying this active energy ray will also increase, so the reflection ratio of the active energy ray at the interface between the air and the coating layer will increase. When forming a pillar structure, there may be a case where an active energy ray having a higher illuminance must be irradiated. Therefore, the upper limit of the inclination angle is more preferably a value of 60 ° or less, and even more preferably a value of 40 ° or less. In addition, the inclination angle means the normal to the film surface and the columnar shape measured in the cross section when the film is cut by cutting the entire column into two surfaces along the axis perpendicular to the film surface. The angle of the narrower side of the angle formed by the uppermost part of the object. (3) Film thickness The film thickness of the light diffusion control thin film of the present invention is preferably a value in a range of 10 to 700 μm. The reason is that if the film thickness of the light diffusion control film is less than 10 μm, incident light that goes straight in the column structure may increase, and it may be difficult to display specific light diffusion characteristics. On the other hand, if the film thickness of the light diffusion control film exceeds 700 μm, when the composition for a light diffusion control film is irradiated with active energy rays to form a column structure, the initially formed column structure will cause the direction of photopolymerization to proceed. Diffusion, and it may be difficult to form a desired pillar structure. In addition, when applied to a display or the like, wrinkles may be easily generated in the displayed image. Therefore, the lower limit of the film thickness of the light diffusion control film is more preferably a value of 30 μm or more, and more preferably a value of 50 μm or more. The upper limit of the thickness of the light diffusion control film is more preferably a value of 300 μm or less, and even more preferably a value of 100 μm or less. (4) Characteristics Further, regarding the characteristics of the light diffusion control film of the present invention, it is preferable that the amplitude of the incident angle region with a turbidity of 70% or more is at a value of 60 ° or more. By limiting the amplitude of a specific incident angle region in this way, since the incident light can be efficiently captured and uniformly diffused, the brightness of the diffused light may be increased. Therefore, the width of the incident angle region with a turbidity of 70% or more is preferably set to a value of 80 ° or more, and more preferably set to a value of 100 ° or more. [0046] In addition, regarding the characteristics of the light diffusion control film of the present invention, the normal direction of the film surface is set to 0 °, and the incident light from a region of incidence angle is incident in a direction deviating from the region, when the incident light is inclined at 60 °, The central value of the transmitted light intensity PT is preferably set to a value in the range of 0.1 to 99%. The reason is that if the median value is less than 0.1%, the transmittance of the entire film may deteriorate. On the other hand, when the median value exceeds 99%, the incident angle region may be insufficient. Therefore, the lower limit of the median value is more preferably set to 1% or more, and more preferably 5% or more. The upper limit of the median value is more preferably 50% or less, and even more preferably 15% or less. In addition, the so-called straight-through transmitted light intensity is the percentage of the intensity of the outgoing light emitted from the same angle as the incident light divided by the intensity of the entire incident light. [0047] Regarding the characteristics of the light-diffusion control film of the present invention, the deviation of the linearly transmitted light intensity PT is preferably set to a value in the range of 0.1 to 3.8%. The reason is that if the deviation is less than 0.1%, it may be difficult to control. On the other hand, when the deviation is set to a value exceeding 3.8%, the light diffusion state may be darkened. Therefore, the lower limit of the deviation is more preferably 1% or more, and more preferably 2% or more. The upper limit of the deviation is more preferably 3.5% or less, and even more preferably 2.8% or less. [0048] 3. Step sheet As shown in FIG. 1 (a), the laminated body 100 of the present invention may also be on one side of the light diffusion control film 10, that is, the side opposite to the side on which the laminated film 4 is laminated On the surface, the step sheet 2 is laminated. In this way, by covering the two sides of the light diffusion control film with the above laminated film and the step sheet, the light diffusion control film can be effectively protected. Here, the so-called step sheet is a sheet to which a composition for a light diffusion control film is applied when a laminate is produced. As the sheet in this step, a common release film can be used, and examples thereof include polyester films such as polyethylene terephthalate, polybutylene terephthalate, polyethylene naphthalate, and the like. Polyolefin films such as polyethylene and polyethylene are coated with a release agent such as silicone resin to provide a release layer. The film thickness of the sheet in this step is usually preferably a value in the range of 20 to 150 μm. [Second Embodiment] A method for producing a laminated body according to an embodiment of the present invention is a method for producing a laminated body according to the first embodiment, which is characterized by including the following steps (a) to (d). (a) a step of preparing a composition for a light diffusion control film containing a high refractive index active energy ray hardening component and a low refractive index active energy ray hardening component; (b) coating the composition for a light diffusion control film in a thin film step; And the step of forming the coating layer, (c) the step of laminating the exposed surface of the coating layer to satisfy the relational expression (1) to cover the laminated film, (d) while moving the coating layer, passing through the upper coating layer The step of closing the thin film and irradiating the coating layer with active energy rays. Hereinafter, the second embodiment of the present invention will be specifically described with reference to appropriate drawings, focusing on differences from the first embodiment. [0050] 1. Step (a): Step of preparing a composition for a light diffusion control film Step (a) is a step of preparing a specific composition for a light diffusion control film. More specifically, it is a step of mixing the components (A) to (B) described below and other components as necessary. In addition, it is possible to directly stir at room temperature during mixing, but from the viewpoint of improving uniformity, it is preferable to stir under a heating condition of, for example, 40 to 80 ° C. to obtain a homogeneous mixed solution. Further, in order to obtain a desired viscosity suitable for coating, it is also preferable to further add a diluent solvent. (1) (A) component: high refractive index active energy ray hardening component A feature of the composition for a light diffusion control film of the present invention includes a high refractive index hardening component (high refractive index active energy ray hardening component) as ( A) ingredients. The reason is that by including a high refractive index active energy ray hardening component as the component (A), and the low refractive index hardening component (low refractive index active energy ray hardening component) described later as the component (B), the polymerization rate is between A specific difference is generated, and the two components are prevented from being uniformly copolymerized with each other, whereby the component (A) and the component (B) can be hardened while being phase-separated. Thereby, although it is a uniform composition at the stage before hardening, it is possible to form a specific internal structure of a column structure or a shutter structure during hardening, so that the light diffusion control film as the obtained hardened material can be efficiently used. Excellent light diffusion characteristics for incident light diffusion. (1) The refractive index of the high refractive index active energy ray-hardened component having a refractive index of (A) -1 is preferably a value in a range of 1.5 to 1.65. The reason is that if the refractive index of the component (A) is less than 1.5, the refractive index difference with the low-refractive-index active energy ray-hardened component as the component (B) becomes too small, making it difficult to obtain effective light diffusion characteristics. The reason. On the other hand, if the refractive index of the component (A) exceeds 1.65, the refractive index difference between the component (B) and the component (B) becomes large, but it is also difficult to form an appearance compatible with the component (B). The reason. Therefore, the lower limit of the refractive index of the (A) component is more preferably a value of 1.55 or more, and more preferably a value of 1.56 or more. The upper limit of the refractive index of the (A) component is more preferably a value of 1.6 or less, and even more preferably a value of 1.59 or less. The refractive index of the component (A) means the refractive index of the component (A) before curing by light irradiation. The refractive index can be measured in accordance with JIS K0062: 1992, for example. [0053] (1) -2 Kinds of (A) component types are not particularly limited, but (meth) acrylic acid esters containing plural aromatic rings are preferred. The reason is that if these compounds are used, it is possible to perform light hardening while phase-separating the component (A) and the component (B) more efficiently, and to obtain more excellent light diffusion characteristics. Examples of these compounds include, for example, biphenyl (meth) acrylate, naphthyl (meth) acrylate, anthracene (meth) acrylate, benzylphenyl (meth) acrylate, and biphenyl (meth) acrylate Phenoxyalkyl ester, naphthyloxyalkyl (meth) acrylate, anthryloxyalkyl (meth) acrylate, benzylphenoxyalkyl (meth) acrylate, o-phenoxy (meth) acrylate Benzyl ester, m-phenoxy benzyl (meth) acrylate, p-phenoxy benzyl (meth) acrylate, etc., or a part of these by halogen, alkyl, alkoxy, halogenated alkyl And so on. The "(meth) acrylic acid" means both acrylic acid and methacrylic acid. [0054] As the component (A), a compound containing a biphenyl ring is more preferable, and a biphenyl compound represented by the following general formula (1) is more preferable. [0055] (In the general formula (1), R 1 to R 10 are each independently, at least one of R 1 to R 10 is a substituent represented by the following general formula (2), and the rest are a hydrogen atom, a hydroxyl group, and a carboxyl group. , Alkyl, alkoxy, halogenated alkyl, hydroxyalkyl, carboxyalkyl, and any of the halogen atom substituents). [0057] (In the general formula (2), R 11 is a hydrogen atom or a methyl group, the carbon number n is an integer of 1 to 4, and the repeating number m is an integer of 1 to 10). [0059] The reason is presumed that by including a biphenyl compound having a specific structure as the (A) component, a specific difference may occur in the polymerization speed of the (A) component and the (B) component, and the (A) component and the (B) The compatibility of the components is reduced to a specific range, and the copolymerizability of the two components can be reduced. In addition, by increasing the refractive index of a region having a relatively high refractive index derived from the component (A), it is easier to adjust the difference from the refractive index of a region having a relatively low refractive index originating from the (B) component to a value greater than a specific value. . [0060] As specific examples of the biphenyl compound represented by the general formula (1), compounds represented by the following formulae (3) to (4) can be preferably exemplified. [0061] [0062] (2) Component (B): Low-refractive index active energy ray hardening component The composition for a light diffusion control film of the present invention includes a low-refractive index active energy ray hardening component as the (B) component. The reason is that by including a low refractive index active energy ray hardening component as the (B) component and a specific difference in polymerization rate between the high refractive index active energy ray hardening component and the high refractive index active energy ray hardening component described above as the (A) component, the two are suppressed Since the components are uniformly copolymerized with each other, the components (A) and (B) can be effectively light-cured while being phase-separated. Thereby, although it is a uniform composition at the stage before light hardening, a specific internal structure of a column structure or a shutter structure can also be formed during light hardening, so that the light diffusion control film as the obtained hardened material can be given a good efficiency. Excellent light diffusion characteristics to diffuse incident light. (2) The refractive index of the low-refractive-index active energy ray-hardened component whose refractive index is (B) component is preferably a value in the range of 1.4 to 1.5. The reason is that if the refractive index of the component (B) is less than 1.4, the refractive index difference between the component (A) and the component (A) becomes large, but the compatibility with the component (A) is extremely deteriorated, making it difficult to form a specific internal structure. The reason for the construction. On the other hand, if the refractive index of the component (B) exceeds 1.5, the difference in refractive index between the component (A) and the component (A) becomes too small, and it may be difficult to obtain desired light diffusion characteristics. Therefore, the lower limit of the refractive index of the component (B) is more preferably a value of 1.45 or more, and more preferably a value of 1.45 or more. The upper limit of the refractive index of the (B) component is more preferably a value of 1.49 or less, and even more preferably a value of 1.48 or less. The refractive index of the component (B) means the refractive index of the component (B) before curing by light irradiation. The refractive index can be measured in accordance with JIS K0062: 1992 as described above. [0065] The difference between the refractive index of the component (A) and the refractive index of the component (B) is preferably set to a value of 0.01 or more. The reason is that if the difference in refractive index is less than 0.01, the angle of total reflection of incident light in a specific internal structure becomes narrow, so that the range of light diffusion characteristics may become excessively narrow. On the other hand, if this refractive index difference becomes an excessively large value, the compatibility between the (A) component and the (B) component is excessively deteriorated, and it may be difficult to form a specific internal structure. Therefore, the lower limit value of the difference between the refractive index of the (A) component and the refractive index of the (B) component is more preferably a value of 0.05 or more, and more preferably a value of 0.1 or more. The upper limit of the difference between the refractive index of the (A) component and the refractive index of the (B) component is more preferably a value of 0.5 or less, and even more preferably a value of 0.2 or less. In addition, the refractive index of (A) component and (B) component here means the refractive index of (A) component and (B) component before hardening by light irradiation. (2) The type of (2) -2 and the type of (B) component are not particularly limited, but examples thereof include a urethane (meth) acrylate and a group having a (meth) acrylfluorenyl group in a side chain. A (meth) acrylic polymer, a (meth) acrylfluorene-containing silicone resin, an unsaturated polyester resin, and the like are particularly preferably a urethane (meth) acrylate. The reason is that if it is a urethane (meth) acrylate, the component (A) and component (B) can be more effectively light-cured while being phase-separated, and more excellent light diffusion characteristics can be obtained. The reason. The (meth) acrylate means both acrylate and methacrylate. [0067] The urethane (meth) acrylate is (B1) a compound containing at least two isocyanate groups, (B2) a polyol compound, preferably a diol compound, and particularly preferably a polyalkylene diene. Alcohol and (B3) hydroxyalkyl (meth) acrylate. In addition, the component (B) is an oligomer that also includes a repeating unit having a urethane bond. The compound containing at least two isocyanate groups as the component (B1) may be exemplified by 2,4-toluene diisocyanate, 2,6-toluene diisocyanate, 1,3-xylene diisocyanate, and 1,4-xylene. Diisocyanates, aromatic isocyanates such as 4,4'-diisocyanuric acid methylene diphenyl (MDI), aliphatic polyisocyanates such as hexamethylene diisocyanate, isophorone diisocyanate (IPDI), hydrogenated diisocyanates Alicyclic polyisocyanates such as phenylmethane diisocyanate, etc., and these ureton bodies, isocyanurate bodies, and further ethylene glycol, propylene glycol, neopentyl glycol, trimethylolpropane, castor oil, etc. Adducts of reactants of low molecular weight active hydrogen-containing compounds (for example, xylene diisocyanate trifunctional adducts) and the like. [0068] Among the components that form the urethane (meth) acrylate, the polyalkylene glycol as the (B2) component is exemplified by polyethylene glycol, polypropylene glycol, polybutylene glycol, and polyhexamethylene glycol. Alcohols and the like are particularly preferably polypropylene glycol. The reason is that if it is polypropylene glycol, when the component (B) is cured, it can be a good soft segment in the cured product, and the rationality or mountability of the obtained light diffusion control film can be effectively improved. The weight average molecular weight of the component (B) can be adjusted mainly by the weight average molecular weight of the component (B2). Here, the weight average molecular weight of the component (B2) is usually 2300 to 19500, preferably 4300 to 14300, and particularly preferably 6300 to 12300. [0069] Among the components that form the urethane (meth) acrylate, the hydroxyalkyl (meth) acrylate as the (B3) component is exemplified by 2-hydroxyethyl (meth) acrylate, ( 2-hydroxypropyl (meth) acrylate, 3-hydroxypropyl (meth) acrylate, 2-hydroxybutyl (meth) acrylate, 3-hydroxybutyl (meth) acrylate, 4- (meth) acrylate 4- Hydroxybutyl esters, etc. In addition, based on the viewpoint that the polymerization rate of the urethane (meth) acrylate obtained is lowered and a specific internal structure is formed more effectively, hydroxyalkyl methacrylate is particularly preferable, and 2-methyl methacrylate is more preferable. Hydroxyethyl ester. (2) -3 blending amount When the total amount of (A) component and (B) component is 100 parts by weight, the blending ratio of (A) component and (B) component ((A) (Component; (B) component (weight ratio)) is preferably set to a value within a range of 20:80 to 80:20. That is, when the total amount of the (A) component and the (B) component is 100 parts by weight, the blending ratio of the (B) component is preferably a value within a range of 20 to 80 parts by mass. The reason is that if the blending ratio of the (B) component is less than 20 parts by weight, the width of the region where the refractive index derived from the (A) component is relatively high and the refractive index derived from the (B) component is relatively low. In comparison, the region width is excessively large, and it may be difficult to obtain good light diffusion characteristics. On the other hand, if the blending ratio of the (B) component exceeds 80 parts by weight, the proportion of the (A) component relative to the (B) component will decrease, and the refractive index derived from the (A) component will be relatively high. Compared with the region width where the refractive index derived from the component (B) is relatively low, the range width of Zn is excessively small, and it may be difficult to obtain good light diffusion characteristics. Therefore, when the total amount of the (A) component and the (B) component is set to 100 parts by weight, the lower limit value of the blending ratio of the (B) component is more preferably set to a value of 40 parts by mass or more, and more preferably. The value is 55 mass parts or more. When the total amount of the (A) component and the (B) component is 100 parts by weight, the upper limit value of the blending ratio of the (B) component is more preferably set to a value of 70 parts by mass or less, and more preferably The value is set to 65 parts by mass or less. (3) Component (C): Photopolymerization initiator. In the composition for a light diffusion control film, a photopolymerization initiator is preferably contained as the component (C). The reason is that by containing a photopolymerization initiator, when the composition for a light diffusion control film is irradiated with an active energy ray, the component (A) and the component (B) can be more effectively photocured while being phase separated, and This is because more excellent light diffusion characteristics can be obtained. [0072] Here, examples of the photopolymerization initiator include benzoin, benzoin methyl ether, benzoin ethyl ether, benzoin isopropyl ether, benzoin n-butyl ether, and benzoin isobutyl ether. , Acetophenone, dimethylaminoacetophenone, 2,2-dimethoxy-2-phenylacetophenone, 2,2-diethoxy-2-phenylacetophenone, 2-hydroxy 2-methyl-1-phenylpropane-1-one, 1-hydroxycyclohexylphenyl ketone, 2-methyl-1- [4- (methylthio) phenyl] -2-morpholinyl- Propane-1-one, 4- (2-hydroxyethoxy) phenyl-2- (hydroxy-2-propyl) one, benzophenone, p-phenylbenzophenone, 4,4-dione Ethylaminobenzophenone, dichlorobenzophenone, 2-methylanthraquinone, 2-ethylanthraquinone, 2-tert-butylanthraquinone, 2-aminoanthraquinone, 2-methylthiazine Tonketone, 2-ethylthioxanthone, 2-chlorothioxanthone, 2,4-dimethylthioxanthone, 2,4-diethylthioxanthone, benzyldimethylacetal, phenethyl Ketodimethylacetal, p-dimethylaminobenzoate, oligo [2-hydroxy-2-methyl-1- [4- (1-methylvinyl) phenyl] propane], etc., One of these may be used alone, or two or more of them may be used in combination. [0073] The blending amount of the photopolymerization initiator as the component (C) is preferably within a range of 0.2 to 20 parts by mass relative to 100 parts by mass of the total amount of the components (A) and (B). value. The reason is that if the blending amount of the component (C) is less than 0.2 parts by weight, the polymerization initiation point is lacking, and therefore it may be difficult to sufficiently harden the composition for a light diffusion control film. On the other hand, if the blending amount of the component (C) is more than 20 parts by weight, yellowing of the light diffusion control film or reduction in durability may occur. Therefore, the lower limit of the blending amount of the component (C) is more preferably a value of 0.5 parts by weight or more, and even more preferably a value of 1 part by weight or more. In addition, the upper limit of the blending amount of the component (C) is more preferably a value of 15 parts by weight or less, and even more preferably a value of 10 parts by weight or less. [0074] (4) Other additives As long as the effect of the present invention is not impaired, other additives may be appropriately blended. Examples of the other additives include antioxidants, antistatic agents, polymerization accelerators, polymerization inhibitors, infrared absorbers, ultraviolet absorbers, plasticizers, diluents, and leveling agents. The content of other additives is generally set to a value in the range of 0.01 to 5 parts by weight based on 100 parts by weight of the total amount of the components (A) and (B). [0075] Furthermore, it is particularly preferable to incorporate an ultraviolet absorber as another additive. The reason is that when an active energy ray is irradiated by mixing an ultraviolet absorber, the active energy ray of a specific wavelength can be selectively absorbed within a specific range. As a result, the hardening of the composition for a light diffusion control film is not inhibited, but a specific internal structure formed inside the obtained light diffusion control film may have a bent portion as shown in FIG. 4 (b), for example. [0076] The ultraviolet absorber is preferably a free hydroxyphenyltriazine-based ultraviolet absorber, a benzotriazole-based ultraviolet absorber, a benzophenone-based ultraviolet absorber, and a hydroxybenzoate-based ultraviolet absorber. At least one selected from the group. The reason is that if these ultraviolet absorbers are used, bending can be more clearly generated in a specific internal structure, so that the range of light diffusion characteristics in the obtained light diffusion control film can be more effectively expanded. That is, if the ultraviolet absorber having a peak at a wavelength closer to the wavelength of 365 nm of the main wavelength of the high-pressure mercury lamp is used, it can be confirmed that the bending occurs even with a small blending amount. [0077] The blending amount of the ultraviolet absorber in the composition for a light diffusion control film is preferably less than 2 parts by weight based on 100 parts by weight of the total amount of the components (A) and (B). (Except 0 parts by weight). The reason is that if the blending amount of the ultraviolet absorber is 2 parts by weight or more, the curing of the composition for a light diffusion control film may be hindered, shrinkage wrinkles may be generated on the film surface, or the film may not be completely cured. On the other hand, when the blending amount of the ultraviolet absorber is excessively small, it may be difficult to sufficiently bend the internal structure formed inside the light diffusion control film. Therefore, the lower limit of the blending amount of the ultraviolet absorber is more preferably 0.01 part by weight or more and 0.02 part by weight or more relative to 100 parts by weight of the total amount of the component (A) and the component (B). value. The upper limit of the amount of the ultraviolet absorber is more preferably 1.5 parts by weight or less and still more preferably 1 part by weight or less based on 100 parts by weight of the total amount of the (A) component and the (B) component. value. [0078] 2. Step (b): As shown in FIG. 5 (a), the coating step (b) is a step of coating the composition for a light diffusion control film on the step sheet 2 with a film to form a coating layer 1. . As this step, a general release film can be used as described in the first embodiment. [0079] As a method for applying the composition for a light diffusion control film to the step sheet, for example, a bar coating method, a doctor blade coating method, a roll coating method, a blade coating method, and a die coating method can be used. Method, gravure coating method, and the like. The thickness of the coating layer at this time is preferably set to a value in the range of 10 to 700 μm. [0080] 3. Step (c): The laminating step, step (c), as shown in FIG. 5 (b), laminates the exposed surface of the coating layer 1 with a laminated film 4 satisfying the relationship (1). The steps. That is, it is a step of laminating in a manner that the gap between the step sheet 2 and the overlying laminated film 4 is maintained without pressing the coating layer 1 before curing. [0081] Step (d): The step (d) of the active energy ray irradiation step is shown in FIG. 5 (c). While moving the coating layer 1, the coating layer 1 is transmitted through the overlying laminated film 4, and the coating is applied. The layer 1 is irradiated with the active energy rays of the parallel light 60 to form a specific internal structure such as a column structure or a shutter structure in the film, thereby forming a light diffusion control film 10. Hereinafter, a case where a pillar structure is formed will be described as an example. [0082] That is, as shown in FIG. 5 (c), the coating layer 1 formed on the step sheet 2 is irradiated with parallel light 60 having high parallelism of light rays. Here, the term “parallel light” means a light that is slightly parallel and does not expand when viewed in any direction. More specifically, for example, as shown in FIG. 5 (c), the irradiation light 70 from the point light source 102 can be made into parallel light 60 by the lens 104. [0083] The parallelism of the irradiation light is preferably set to a value of 10 ° or less. The reason is that by setting the parallelism of the irradiation light to a value within this range, a pillar structure can be formed efficiently and stably. Therefore, the parallelism of the irradiated light is more preferably set to a value of 5 ° or less, and further preferably set to a value of 2 ° or less. [0084] As the irradiation angle of the irradiation light, as shown in FIG. 6, the irradiation angle θ when the angle of the normal to the surface of the coating layer 1 is 0 ° is usually preferably -80 to Values in the range of 80 °. The reason is that if the irradiation angle is outside the range of -80 to 80 °, the influence of reflection and the like on the surface of the coating layer 1 becomes large, and it may be difficult to sufficiently form a pillar structure. The arrow MD in FIG. 6 indicates the moving direction of the coating layer. [0085] As the irradiation light of the active energy ray, ultraviolet rays are preferably used. The reason for this is the case of an electron beam. Since the polymerization rate is very fast, the components (A) and (B) cannot be sufficiently separated from each other during polymerization, and it may be difficult to form a column structure. On the other hand, when compared with visible light, the UV-curable resin that can be hardened by UV irradiation or the photopolymerization initiator that can be used are more abundant, so the components of (A) and (B) can be broadened. Select the amplitude. [0086] Further, as to the irradiation conditions of ultraviolet rays as the active energy ray, the peak illuminance of the surface coating layer is preferably set to 0.1 ~ 10mW / 2 value within the range of the cm. The reason is that if the peak illuminance is less than 0.1 mW / cm 2 , it may be difficult to clearly form a pillar structure. On the other hand, if the peak illuminance is a value exceeding 10 mW / cm 2 , it is presumed that the curing rate is too fast, and it may be difficult to effectively form a column structure. Therefore, the lower limit of the peak illuminance on the surface of the coating layer is more preferably set to a value of 0.3 mW / cm 2 or more, and more preferably to a value of 0.5 mW / cm 2 or more. The upper limit of the peak illuminance on the surface of the coating layer is more preferably a value of 8 mW / cm 2 or less, and even more preferably a value of 6 mW / cm 2 or less. [0087] In addition, when the ultraviolet ray is used as the active energy ray, the accumulated light amount on the surface of the coating layer is preferably set to a value in a range of 5 to 200 mJ / cm 2 . The reason is that if the accumulated light amount is less than 5 mJ / cm 2 , it may be difficult to sufficiently extend the column structure from above to below. On the other hand, if the cumulative light amount exceeds a value of 200 mJ / cm 2 , the obtained light diffusion control film may be colored. Thus, the surface of the integrated light quantity of the coating layer to better limit 7mJ / cm & lt value of 2 or more, and better to 10mJ / 2 values of more cm. In addition, the upper limit value of the accumulated light amount on the surface of the coating layer is more preferably a value of 150 mJ / cm 2 or less, and even more preferably a value of 100 mJ / cm 2 or less. [0088] From the viewpoint of maintaining mass productivity and stably forming a column structure, it is preferable that the coating layer formed on the step sheet is moved at a speed in the range of 0.1 to 10 m / min when irradiating ultraviolet rays as active energy rays. . It is particularly preferable to move at a speed of 0.2 m / min or more, and more preferably to move at a speed of 3 m / min or less. [0089] In the present invention, the internal structure formed in the light diffusion control film formed by curing the composition for light diffusion control film is not limited to the above if it includes a high refractive index region and a low refractive index region. Column construction. For example, when the louver structure 20b shown in FIG. 4 (a) is formed, as long as the coating layer 1 formed on the step sheet 2 is irradiated in one direction, it is substantially parallel light when viewed, and it looks non-parallel when viewed in other directions. The light of the stray light may be used as the irradiation light. In addition, when forming the specific internal structure 20d shown in FIG. 4 (c), as long as the coating layer 1 formed on the step sheet 2 is irradiated in one direction, it is substantially parallel light when viewed, and not all when viewed from other directions. The light may be a messy light but may be adjusted to a certain degree of parallelism. [Examples] [0090] Hereinafter, the present invention will be described in more detail through examples. However, the present invention is not limited to these descriptions. [Example 1] 1. Preparation of Overlay Laminated Film A biaxially-stretched polyethylene terephthalate film roll having a thickness of 38 μm and a short side direction (width direction) of 1000 mm was prepared (sometimes below) (Referred to as "film A") as the overlying laminated film. [0092] (1) Measurement of Phase Difference Re The phase difference Re of the overlying laminated film prepared was measured. That is, an arbitrary part in the longitudinal direction of the prepared over-clad film is specified as a measurement part. Next, among the specific measurement locations, 1000 locations along the short side direction and 20 locations per 50 mm were used as measurement points, and a phase difference Re (nm) was measured using a phase difference measuring device KOBRA-WR made by Oji Measurement Co., Ltd. The results obtained are shown in the characteristic curve A in FIG. 7. This FIG. 7 is a short-side position-phase difference Re graph using the horizontal axis as the position (mm) in the short-side direction of the overlying laminated film, and the vertical axis as the phase difference Re (nm). Then, from the obtained measured values, the median value (nm) of the phase difference Re and the deviation ((Re max -Re min ) / (Re max + Re min ) × 100) (%) expressed by the formula (1) were calculated. The results obtained are shown in Table 1. [0093] (2) Surface Roughness Rp and Ra The arithmetic average roughness (Ra) and the maximum ridge (Rp) of the prepared overlying laminated film were measured. That is, using the surface shape measuring device WYKO NT110 (ANSI B46.1 standard) manufactured by Veeco, the arithmetic average roughness (Ra) (nm) of the prepared overlying film was measured, and the maximum bulge (Rp) was measured. (nm). The results obtained are shown in Table 1. (3) Measurement of turbidity and total light transmittance The turbidity of the prepared overlying laminated film was measured. That is, the turbidity (%) and total light transmittance of the prepared overlying laminated film were measured using a turbidimeter NDH 5000 manufactured by Nippon Denshoku Industries Co., Ltd. The results obtained are shown in Table 1. [0095] 2. Synthesis of low-refractive-index active energy ray hardening component In a container, 1 mol of polypropylene glycol (PPG) having a weight average molecular weight of 9200 as (B2) component is stored as isophorone di (B1) component. After 2 mols of isocyanate (IPDI) and 2 hydroxyethyl methacrylate (HEMA) as (B3) components, the reaction was carried out according to a common method to obtain a polyether having a weight average molecular weight of 9900 as a component (B). Urethane methacrylate. [0096] The weight average molecular weight of polypropylene glycol and polyether urethane methacrylate is a polystyrene conversion value measured by gel permeation chromatography (GPC) under the following conditions. . GPC measuring device: TOSOH (stock) system, HLC-8020. GPC column: made of TOSOH (share) (Through description below) TSK protective column HXL-H TSK gel GMHXL (× 2) TSK gel G2000HXL. Determination solvent: tetrahydrofuran. Measurement temperature: 40 ° C 3. Preparation of the composition for a light diffusion control film Next, o-phenylphenoxyethoxyethyl acrylate having a molecular weight of 268 represented by the above formula (3) was added as the component (A) Ester (62.5 parts by weight, manufactured by Shin Nakamura Chemical Co., Ltd., NK ESTER A-LEN-10) and 37.5 parts by weight of a polyether urethane methacrylate having a weight average molecular weight of 9,900 as a component (B) after synthesis For the total amount of (A) component and (B) component = 100 parts by weight of 1.25 parts by weight of 2-hydroxy-2-methyl-1-phenylpropane-1-one as component (C), then at 80 The mixture was heated and mixed under the condition of ℃ to obtain a composition for a light diffusion control film. The refractive indices of the components (A) and (B) are measured using an Abbe refractometer (manufactured by ATAGO Co., Ltd., Ab-Refractometer DR-M2, Na light source, and wavelength 589 nm). 1.58 and 1.46. [0098] 4. The coating step is followed by applying a peeling treatment to the transparent polyethylene terephthalate roll with a length of 1000 mm in the short-side direction as a step sheet, and applying the coating on the peeling treatment surface. The composition for a light diffusion control film forms a coating layer with a thickness of 60 μm. [0099] 5. Laminating Step Next, the exposed surface side of the coating layer is laminated with a prepared film by roll-to-roll lamination. Next, as shown in FIG. 5 (c), an ultraviolet point parallel light source (manufactured by JATEC) is used to control the parallelism of the central rays within ± 3 °, and the parallel light with a parallelism of 2 ° or less is shown in FIG. 6 The coating layer is irradiated so that the irradiation angle θx becomes approximately 10 °. The peak illuminance at this time was set to 2.00 mW / cm 2 , the cumulative light amount was set to 53.13 mJ / cm 2 , the lamp height was set to 1480 mm, and the moving speed of the coating layer was set to 1.0 m / min. In addition, the above-mentioned peak illuminance and cumulative light amount were measured by installing a UV meter (EYE GRAPHIC (Eye) Co., Ltd., EYE ultraviolet cumulative illuminance meter UVPF-A1)) provided with a photoreceptor at the position of the coating layer. The film thickness of the light diffusion control film was measured using a constant-pressure thickness measuring device (TECLOCK PG-02J, manufactured by Takara Seisakusho Co., Ltd.). [0100] A cross-sectional photograph of the light diffusion control film having the obtained pillar structure cut along a plane parallel to the moving direction of the coating layer and orthogonal to the film plane is shown in FIG. 8 (a). The length of the pillar structure in the film thickness direction was 60 μm, and the inclination angle thereof was 7 °. The cutting of the light diffusion control film was performed using a razor, and the photographing of the cross-section photograph was performed using a keyence product. The digital microscope VHX-1000 was performed by reflection observation. [0101] 6. Evaluation (1) Measurement of angle-varying turbidity The angle-varying turbidity of the obtained light diffusion control film was measured. That is, a short strip-shaped test piece (120 mm wide) in the long side direction was cut out from any part of the obtained sheet / light diffusion control film / overlay laminated film laminate, and used by Toyo Seiki Seisakusho Co., Ltd., Haze Gard Plus measures the angular turbidity (%). At this time, the distance between the opening of the integrating sphere and the light diffusion control film was set to 62 mm, and the incident point of the reference light was set to the center point in the short side direction of the light diffusion control film of the test piece. In addition, as shown in FIG. 9 (a), the reference light is incident from the sheet side of the test piece, and the incident angle of the reference light is changed along the longitudinal direction of the light diffusion control film and measured. The obtained results are shown in the characteristic curve A in Fig. 9 (b). FIG. 9 (b) is an incident angle-variable angle turbidity chart with the horizontal axis as the incident angle (°) of the reference light and the vertical axis as the variable angle turbidity (%). The width of the incident angle region with a turbidity of 70% or more was calculated from FIG. 9 (b) and shown in Table 1. Therefore, from the characteristic curve A, it is possible to confirm the property that the degree of light diffusion varies with the incident angle, that is, the incident angle dependency (characteristic curve B: Example 2, characteristic curve C: Same as Comparative Example 1). [0102] (2) Measurement of Straight Forward Transmission Light Intensity PT The direct transmission light intensity of the obtained light diffusion control film was measured. That is, the measurement point is 1000 mm along the short side of the same test piece as that used for the variable angle turbidity measurement, and a total of 20 locations are used as measurement points per 50 mm. The measurement is performed using a variable angle colorimeter VC-2 manufactured by SUGA testing machine (strand). Straight forward transmitted light intensity PT (%). At this time, as shown in FIG. 10 (a), for the step sheet side of the test piece, light was incident from the pillar oblique direction of the light diffusion control film in a direction inclined at an angle of 60 ° and measured. The obtained results are shown in the characteristic curve A in Fig. 10 (b). FIG. 10 (b) is a position (mm) in the short-side direction of the light diffusion control film on the horizontal axis, and a position in the short-side direction of the straight-through transmission light intensity (%)-a straight-through transmission light intensity chart. From the obtained measured values, the median value (%) of the linear transmitted light intensity PT and the deviation ((PT max -PT min ) / (PT max + PT min ) × 100) (%) expressed by the formula (1) were calculated. . The results obtained are shown in Table 1. [Example 2] In Example 2, a biaxially stretched polymer having a thickness of 38 μm having a phase difference Re and a surface roughness shown in Table 1 and a length of 1,000 mm in the short side direction was used as the overlying laminated film in addition to the overlying laminated film. Except for a terephthalate roll (hereinafter, sometimes referred to as a film B), a laminate was produced and evaluated in the same manner as in Example 1. The obtained results are shown in Table 1, the characteristic curve B of FIG. 8 (b), FIG. 9 (b), and the characteristic curve B of FIG. 10 (b). [Comparative Example 1] In Comparative Example 1, a biaxially stretched polymer having a thickness of 75 mm having a phase difference Re and a surface roughness shown in Table 1 and a length of 1,000 mm in the short-side direction was used as the overlying laminated film. Except for a terephthalate roll (hereinafter sometimes referred to as "film C"), a laminate was produced and evaluated in the same manner as in Example 1. The obtained results are shown in Table 1, the characteristic curve C of FIG. 8 (b), FIG. 9 (b), and the characteristic curve C of FIG. 10 (b). [0105] [Industrial Applicability] As described in detail above, according to the present invention, by setting the deviation of the phase difference measured in a specific direction in the surface of the overlying laminated film to a value within a specific range, In the case where no internal structure region is not formed, or in the case where it occurs, the internal structure can be uniformly formed. As a result, a light diffusion control film having uniform light diffusion characteristics regardless of the internal position of the film surface can be obtained. Therefore, the light diffusion control film obtained by the present invention is expected to contribute significantly to the improvement of the quality of a liquid crystal display device, a projection screen, and the like.

[0107][0107]

1‧‧‧塗佈層1‧‧‧ coated layer

2‧‧‧步驟薄片2‧‧‧ step flakes

10‧‧‧光擴散控制薄膜10‧‧‧light diffusion control film

10a‧‧‧等向性光擴散控制薄膜10a‧‧‧Isotropic light diffusion control film

10b~10d‧‧‧光擴散控制薄膜10b ~ 10d‧‧‧‧Light diffusion control film

12、12b~12d‧‧‧折射率相對較高的區域(包含折射率相對較高的板狀區域)12, 12b ~ 12d‧‧‧‧ area with relatively high refractive index (including plate-shaped area with relatively high refractive index)

12a‧‧‧折射率相對較高的柱狀物12a‧‧‧ relatively high refractive index pillars

14、14a~14d‧‧‧折射率相對較低的區域(包含折射率相對較低的板狀區域)14, 14a to 14d ‧‧‧ areas with relatively low refractive index (including plate-shaped areas with relatively low refractive index)

16‧‧‧彎曲部16‧‧‧ Bend

20‧‧‧內部構造20‧‧‧ Internal structure

20a’‧‧‧邊界面20a’‧‧‧ boundary surface

20a‧‧‧柱構造20a‧‧‧column structure

20b‧‧‧百葉窗構造20b‧‧‧ Blind structure

20c‧‧‧彎曲柱構造20c‧‧‧curved column structure

20d‧‧‧特定內部構造20d‧‧‧Specific internal structure

52、54‧‧‧入射光52, 54‧‧‧ incident light

52’、54’‧‧‧特定擴散光52 ’, 54’ ‧‧‧ specific diffused light

56‧‧‧入射光56‧‧‧ incident light

56’‧‧‧透過光56’‧‧‧ through light

60‧‧‧平行光60‧‧‧ Parallel Light

70‧‧‧來自點光源之放射光70‧‧‧ radiated light from a point light source

100‧‧‧層合體100‧‧‧ laminated

102‧‧‧點光源102‧‧‧point light source

104‧‧‧透鏡104‧‧‧Lens

[0018]   圖1(a)~(b)係供於用以說明本發明之層合體概略的圖。   圖2(a)~(b)係供於用以說明於薄膜內具有柱構造之光擴散控制薄膜之概略的圖。   圖3(a)~(b)係供於用以說明於薄膜內具有柱構造之光擴散控制薄膜中入射角度依存性及等向性光擴散的圖。   圖4(a)~(d)係供於用以說明本發明之光擴散控制薄膜中之內部構造態樣的圖。   圖5(a)~(c)係供於用以說明本發明之層合體之製造方法的圖。   圖6係供於用以說明活性能量線之照射角的圖。   圖7係供於用以顯示實施例1及比較例1中之上覆層合薄膜之寬度方向之位置與相位差Re之關係的圖。   圖8(a)~(c)係供於用以顯示實施例1~2及比較例1中之光擴散控制薄膜之剖面照片的圖。   圖9(a)~(b)係供於用以顯示實施例1~2及比較例1中之參考光對於光擴散控制薄膜之入射角度與變角濁度之關係的圖。   圖10(a)~(b)係供於用以顯示實施例1~2及比較例1中之光擴散控制薄膜之短邊方向的位置與直進透過光強度P.T之關係的圖。[0018] FIG. 1 (a) to (b) are diagrams for explaining the outline of the laminated body of the present invention. FIGS. 2 (a) to 2 (b) are diagrams for explaining the outline of a light diffusion control film having a pillar structure in the film. FIGS. 3 (a) to 3 (b) are diagrams for explaining the dependency of the incident angle and the isotropic light diffusion in a light diffusion control film having a pillar structure in the film. FIGS. 4 (a) to 4 (d) are diagrams for explaining the state of the internal structure in the light diffusion control film of the present invention. (5) FIGS. 5 (a) to (c) are diagrams for explaining a method for producing a laminated body of the present invention. FIG. 6 is a diagram for explaining an irradiation angle of an active energy ray. FIG. 7 is a diagram for showing the relationship between the position in the width direction of the overlying laminated film and the retardation Re in Example 1 and Comparative Example 1. 8 (a) to 8 (c) are views for showing photographs of cross sections of the light diffusion control films in Examples 1 to 2 and Comparative Example 1. FIGS. 9 (a) to (b) are diagrams for showing the relationship between the incident angle of the reference light to the light diffusion control film and the variable-angle turbidity in Examples 1 to 2 and Comparative Example 1. (FIGS. 10 (a) to (b) are diagrams for showing the relationship between the position in the short-side direction of the light diffusion control films in Examples 1 to 2 and Comparative Example 1 and the intensity of P.T.

Claims (7)

一種層合體,其係於源自光擴散控制薄膜用組成物之光擴散控制薄膜之至少一面上層合有上覆層合薄膜之狀態之層合體,   其特徵為前述光擴散控制薄膜具有於低折射率區域中具有複數高折射率區域且該高折射率區域沿厚度方向延伸之內部構造,且   前述層合體之層合面內,將形成前述光擴散控制薄膜時之移動方向設為長邊方向,將與該長邊方向垂直之方向設為短邊方向,且   將沿前述上覆層合薄膜之短邊方向測定之相位差Re(nm)之最大值設為Remax ,最小值設為Remin 時,滿足下述關係式(1),   (Remax -Remin )/(Remax +Remin )×100<35(%) (1)。A laminated body is a laminated body in a state where an overlying laminated film is laminated on at least one side of a light diffusion controlling film derived from a composition for a light diffusion controlling film, characterized in that the light diffusion controlling film has a low refractive index. The high-refractive-index region has an internal structure having a plurality of high-refractive-index regions and the high-refractive-index region extends in the thickness direction, and the moving direction when the light diffusion control film is formed in the lamination plane of the laminate is set to the long side direction. A direction perpendicular to the long side direction is set to a short side direction, and a maximum value of the phase difference Re (nm) measured along the short side direction of the above-mentioned laminated film is set to Re max and the minimum value is set to Re min In this case, the following relational expression (1) is satisfied, and (Re max −Re min ) / (Re max + Re min ) × 100 <35 (%) (1). 如請求項1之層合體,其中前述上覆層合薄膜之前述短邊方向之長度為100~10000mm之範圍內之值。For example, the laminated body of claim 1, wherein the length in the short-side direction of the overlying laminated film is a value in a range of 100 to 10,000 mm. 如請求項1或2之層合體,其中前述上覆層合薄膜之相位差Re之中央值為1000~3000nm之範圍內之值。For example, the laminated body of claim 1 or 2, wherein the central value of the phase difference Re of the above-mentioned laminated film is a value in the range of 1000 to 3000 nm. 如請求項1或2之層合體,其中前述上覆層合薄膜之膜厚為5~5000μm之範圍內之值。For example, the layered product of claim 1 or 2, wherein the film thickness of the aforementioned overlying laminated film is a value in a range of 5 to 5000 μm. 如請求項1或2之層合體,其中作為前述光擴散控制薄膜之內部構造,包含於折射率相對低之區域中,於薄膜膜厚方向林立有折射率相對較高之複數柱狀物而成之柱構造。For example, the laminated body of claim 1 or 2, wherein the internal structure of the aforementioned light diffusion control film is included in a region with a relatively low refractive index, and a plurality of pillars having a relatively high refractive index are lined in the film thickness direction. Pillar structure. 如請求項1或2之層合體,其中作為前述光擴散控制薄膜之內部構造,包含於沿薄膜面之任意一方向交替配置折射率不同之複數板狀區域而成之百葉窗構造。For example, the laminated body of claim 1 or 2, wherein the internal structure of the light diffusion control film includes a louver structure formed by alternately arranging a plurality of plate-shaped regions having different refractive indexes along any direction of the film surface. 一種層合體之製造方法,其特徵係如請求項1~6中任一項之層合體之製造方法,且包含下述步驟(a)~(d),   (a)準備包含高折射率活性能量線硬化成分及低折射率活性能量線硬化成分之光擴散控制薄膜用組成物之步驟,   (b)對步驟薄片膜狀塗佈前述光擴散控制薄膜用組成物而形成塗佈層之步驟,   (c)對於前述塗佈層之露出面層合滿足前述關係式(1)之上覆層合薄膜之步驟,   (d)邊使前述塗佈層移動,邊透過前述上覆層合薄膜,對該塗佈層照射活性能量線之步驟。A method for manufacturing a laminate, which is characterized in that it is the method for manufacturing a laminate according to any one of claims 1 to 6, and includes the following steps (a) to (d), (a) preparing to include active energy of high refractive index The step of forming a composition for a light-diffusion control film of a linear hardening component and a low-refractive index active energy ray-hardening component, (b) a step of forming a coating layer by applying the aforementioned composition for a light-diffusion control film in a thin film form, ( c) For the step of laminating the exposed surface of the coating layer that satisfies the above-mentioned relational formula (1), a step of laminating the laminated film, (d) while moving the coating layer, passing through the upper laminating film, The step of irradiating the coating layer with active energy rays.
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KR20190013437A (en) 2019-02-11
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KR102473934B1 (en) 2022-12-06
CN109307895B (en) 2022-03-25

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