JP2014002186A - Method of manufacturing light diffusion film - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a method of efficiently manufacturing a longitudinally extending light diffusion film having an effectively increased incident light diffusion area.SOLUTION: A method of manufacturing a longitudinally extending light diffusion film 20 having prescribed louver structures includes steps (a) to (e) as follows: (a) a step for preparing a light diffusion film composition, (b) a step for forming a first coating layer, (c) a step for irradiating the first coating layer with a first active energy ray using a linear light source to form a first louver structure 13a, (d) a step for forming a laminate comprising the first coating layer and a second coating layer, (e) a step for irradiating the second coating layer with a second active energy ray using the linear light source to form a second louver structure 13b such that, looking from the top, an acute angle between a longitudinal direction of the linear light source during the first active energy ray irradiation and a longitudinal direction of the linear light source during the second active energy ray irradiation is within a range of 10 to 90 degrees.

Description

The present invention relates to a method for producing a light diffusion film.
In particular, long light that effectively spreads the diffusion area of incident light by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction perpendicular to the longitudinal direction. The present invention relates to a method for producing a light diffusion film capable of efficiently producing a diffusion film.

  2. Description of the Related Art Conventionally, for example, in the optical technical field to which a liquid crystal display device or the like belongs, light that can be diffused in a specific direction for incident light from a specific direction and transmitted straight as it is for incident light from other directions. The use of diffusion films has been proposed.

  Various forms are known as such a light diffusion film, and in particular, a louver formed by alternately arranging a plurality of plate-like regions having different refractive indexes along any one direction along the film surface. A light diffusion film having a structure is widely used (for example, Patent Documents 1 and 2).

That is, Patent Document 1 discloses a light control plate (light diffusion film) that is a plastic sheet and selectively scatters incident light in two or more angular ranges with respect to the sheet. ing.
In Patent Document 1, a resin composition composed of a plurality of compounds having one or more polymerizable carbon-carbon double bonds in a molecule having a difference in refractive index is maintained in a film shape and specified. A first step of curing the composition by irradiating ultraviolet rays from the direction of the step, and irradiating ultraviolet rays from a direction different from the first step while maintaining the resin composition on the obtained cured product as a film. The manufacturing method of the light control board (light diffusion film) characterized by consisting of the 2nd process hardened in this and repeating a 2nd process as needed is disclosed.

  Further, in Patent Document 2, the haze value has an angle dependency, and when light is incident on the surface at an angle of 0 to 180 °, a light scattering angle region (a haze value of 60% or more) A projection screen comprising a plurality of light control films (light diffusion films) having a light diffusion incident angle region) of 30 ° or more, which are shown in FIGS. As described above, two of the plurality of light control films (light diffusion films) are laminated so that the directions of the light scattering angle region (light diffusion incident angle region) are substantially orthogonal to each other. A screen is disclosed.

JP 63-309902 A (Claims) Japanese Patent Laying-Open No. 2005-316354 (Claims)

However, in Patent Document 1, when mass-producing a light diffusion film continuously, a linear light source is applied to the application layer while moving the application layer made of the composition for light diffusion film on a conveyor or the like. By irradiating with active energy rays, a light diffusion film having a predetermined louver structure is produced.
Therefore, in the case of Patent Document 1, although it is possible to obtain a light diffusion film that diffuses incident light in the moving direction of the coating layer, that is, in the direction along the longitudinal direction of the film, There was a problem that it was not possible to obtain a light diffusion film that diffused light in a direction perpendicular to the direction.

More specifically, in order to obtain a light diffusion film that diffuses incident light in a direction perpendicular to the longitudinal direction of the film, a louver structure consisting of a plate-like region extending in the longitudinal direction of the film is formed. There is a need to.
For this reason, when it is going to form such a louver structure in patent document 1, a linear light source will be arrange | positioned so that the long-axis direction of a linear light source may become the direction along the moving direction of a coating layer.
However, even if the linear light source is arranged in such a manner, when viewed from the cross section in the moving direction of the coating layer, the active energy rays from the linear light source are irradiated at different angles depending on the position in the width direction on the surface of the coating layer. Therefore, the light diffusion characteristics of the obtained light diffusion film become non-uniform.
Therefore, in the cited document 1, when trying to obtain a long light diffusion film that diffuses incident light in a direction orthogonal to the long direction, first, the width direction when the film is viewed from the top surface. It is necessary to obtain a light diffusing film having a louver structure in which plate-like regions are arranged along. Next, it is necessary to cut them and change the 90 ° direction to connect the plurality of light diffusion films. For this reason, the problem that the light diffusibility became non-uniform | heterogenous in the joint part, or the intensity | strength of a film fell easily was seen.
In Cited Document 1, the extending direction of the plate-like region in the louver structure obtained in the first step is basically parallel to the extending direction of the plate-like region in the louver structure obtained in the second step. .
For this reason, there has been a problem that it is fundamentally impossible to diffuse the incident light in the direction perpendicular to the longitudinal direction.

On the other hand, in Patent Document 2, as shown in FIGS. 23A to 23B, two of the plurality of light diffusion films are laminated so that the directions of the light diffusion incident angle regions are substantially orthogonal to each other. Therefore, it seems that incident light can be diffused not only in the direction along the longitudinal direction but also in the direction orthogonal to the longitudinal direction.
However, even in the case of Patent Document 2, when mass-producing a light diffusion film continuously, a linear light source is used while moving a coating layer made of the composition for light diffusion film on a conveyor or the like. Active energy rays will be irradiated.
Therefore, it is difficult to obtain a light diffusion film 221 that diffuses incident light in a direction orthogonal to the longitudinal direction of the film as shown in FIG. It becomes.
Therefore, after all, even the light diffusion film disclosed in Patent Document 2 has a long shape that diffuses incident light as shown in FIG. 23 (a) in a direction orthogonal to the long direction. In order to obtain the light diffusion film 221, it is necessary to connect a plurality of light diffusion films. Therefore, as in the case of Patent Document 1, the light diffusibility becomes uneven at the joint portion, and the strength of the film is reduced. It becomes easy to do.
For this reason, there is a problem that the diffusion area of incident light cannot be effectively expanded by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction perpendicular to the longitudinal direction. It was.
Under such circumstances, there has been a demand for a long light diffusion film that can be easily applied to a large screen or the like and does not cause problems such as joints.
That is, a long light diffusion film that effectively expands the diffusion area of incident light by diffusing incident light not only in the direction along the long direction but also in the direction perpendicular to the long direction. There was a need for a production method.

Therefore, the inventors of the present invention made extensive efforts in view of the above circumstances, and in a predetermined manufacturing method including two active energy ray irradiation steps using a linear light source, the two active activities are performed. It was found that by defining the relationship between the arrangement angles of the respective linear light sources in the energy ray irradiation process within a predetermined range, it is possible to obtain a long light diffusion film that solves the above-mentioned problems, and the present invention is completed. It has been made.
That is, the object of the present invention is to effectively spread the diffusion area of incident light by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction orthogonal to the longitudinal direction. It is providing the manufacturing method of the light-diffusion film which can manufacture the elongate light-diffusion film efficiently.

According to the present invention, the first louver structure and the second louver structure in which a plurality of plate-like regions having different refractive indexes are alternately arranged in parallel in one arbitrary direction along the film surface are provided in the film thickness direction. A method for producing a light diffusion film having a long shape sequentially from below along the line, comprising the following steps (a) to (e), is provided: The problem can be solved.
(A) The process of preparing the composition for light diffusion films containing two polymeric compounds from which refractive index differs (b) The composition for light diffusion films is apply | coated with respect to a process sheet | seat, and a 1st application layer is formed. Step (c) A step of forming a first louver structure by performing first active energy ray irradiation using a linear light source while moving the first coating layer with respect to the first coating layer (d) (E) Applying the composition for light diffusion film to the first coating layer on which the first louver structure is formed, to form a laminate comprising the first coating layer and the second coating layer (e) A second active energy ray is irradiated using a linear light source while moving the laminate composed of the first coating layer and the second coating layer with respect to the second coating layer, and the second louver structure is formed. The first step when the film is viewed from above. Step of the long axis direction of the linear light source in sexual energy ray irradiation, a value within the range of the acute angle .theta.1 10 to 90 ° to the long axis direction of the linear light source in the second active energy ray irradiation, is made

That is, if it is the manufacturing method of the light-diffusion film of this invention, the relationship of the arrangement | positioning angle of each linear light source is prescribed | regulated to the predetermined | prescribed range in two active energy ray irradiation processes using a linear light source. Therefore, the long light diffusion film formed by intersecting the extending direction of the plate-like region in the first louver structure and the extending direction of the plate-like region in the second louver structure at a predetermined angle is efficiently used. Can be manufactured well.
Therefore, long light that effectively spreads the diffusion area of incident light by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction orthogonal to the longitudinal direction. A diffusion film can be manufactured efficiently.
More specifically, incident light can be diffused in a direction along the longitudinal direction and in a direction orthogonal to the longitudinal direction without connecting a plurality of light diffusion films as in the prior art. A long light diffusion film can be obtained.

Further, in carrying out the method for producing a light diffusion film of the present invention, in the step (c), when viewed from above the film, the long axis direction of the linear light source in the first active energy ray irradiation, The acute angle θ2 formed by the virtual line along the moving direction of the coating layer is set to a value within the range of 10 to 80 °, and the second active energy ray when viewed from above the film in the step (e). A value within a range of 10 to 80 degrees of an acute angle θ3 formed by the major axis direction of the linear light source in irradiation and the imaginary line along the moving direction of the laminate composed of the first coating layer and the second coating layer. It is preferable that
By carrying out in this way, not only the direction along the longitudinal direction of the incident light but also light diffusion in the direction orthogonal to the longitudinal direction can effectively expand the diffusion area of the incident light. The long light diffusion film can be manufactured more efficiently.

Further, in carrying out the method for producing a light diffusion film of the present invention, in the step (e), when viewed from above the film, the long axis direction of the linear light source in the first active energy ray irradiation, the second The long axis direction of the linear light source in active energy ray irradiation is symmetrical with respect to a virtual line perpendicular to the moving direction of the laminate composed of the first coating layer and the second coating layer. Is preferred.
By carrying out like this, incident light can be diffused more uniformly in the obtained light diffusion film.

In carrying out the method for producing a light diffusing film of the present invention, in the step (c) and the step (e), the first active energy ray irradiation and the second active energy ray irradiation are performed as long groove-like active energy rays. While performing through the light-shielding plate which has a permeation | transmission part, it is preferable that the longitudinal direction of an active energy ray permeation | transmission part is a direction parallel to the major axis direction of a linear light source.
By carrying out in this way, not only the direction along the longitudinal direction of the incident light but also light diffusion in the direction orthogonal to the longitudinal direction can effectively expand the diffusion area of the incident light. The long light diffusion film can be produced more efficiently.

Moreover, when implementing the manufacturing method of the light-diffusion film of this invention, the peak illumination intensity in the surface of the 1st coating layer in 1st active energy ray irradiation is 0.1-50 mW / cm < ² > in a process (c). It is preferable to set the value within the range and set the integrated light amount on the surface of the first coating layer to a value within the range of 5 to 300 mJ / cm ² .
By carrying out in this way, the first louver structure can be formed more efficiently.
The peak illuminance here means a measured value at a portion where the active energy ray irradiated on the surface of the first coating layer shows the maximum value.

In carrying out the method for producing a light diffusion film of the present invention, in the step (e), the peak illuminance on the surface of the second coating layer in the second active energy ray irradiation is 0.1 to 50 mW / cm ² . It is preferable to set the value within the range and set the integrated light quantity on the surface of the second coating layer to a value within the range of 5 to 300 mJ / cm ² .
By carrying out in this way, the second louver structure can be formed more efficiently.
Here, the peak illuminance means a measured value at a portion where the active energy ray irradiated on the surface of the second coating layer shows the maximum value.

In carrying out the method for producing a light diffusion film of the present invention, in step (b), the thickness of the first coating layer is set to a value in the range of 80 to 700 μm, and in step (d) The thickness of the coating layer 2 is preferably set to a value in the range of 80 to 700 μm.
By carrying out in this way, the first and second louver structures can be formed more efficiently.

In carrying out the method for producing a light diffusing film of the present invention, a laminate comprising the moving speed of the first coating layer in the step (c) and the first coating layer and the second coating layer in the step (e). It is preferable that the moving speed of each be a value within the range of 0.1 to 10 m / min.
This is because the first louver structure and the second louver structure can be formed more efficiently by carrying out in this way.

Fig.1 (a)-(b) is a figure provided in order to demonstrate the outline of the louver structure in a light-diffusion film. FIGS. 2A to 2B are diagrams for explaining incident angle dependency, anisotropy, and an opening angle in a light diffusion film. 3 (a) to 3 (c) are diagrams for explaining the basic configuration of the light diffusion film obtained by the production method of the present invention. 4 (a) to 4 (d) are diagrams provided for explaining each step in the production method of the present invention. FIGS. 5A to 5B are diagrams provided for explaining active energy ray irradiation using a linear light source. FIGS. 6A to 6B are diagrams provided to explain the arrangement angle of the linear light source. FIG. 7 is another diagram provided for explaining active energy ray irradiation using a linear light source. FIGS. 8A to 8E are diagrams provided for explaining the relationship between the arrangement angle of the linear light source and the diffusion area of incident light. FIGS. 9A to 9E are photographs provided for explaining the relationship between the arrangement angle of the linear light source and the diffusion area of incident light. FIGS. 10A and 10B are views for explaining the louver structure. Fig.11 (a)-(b) is a figure provided in order to demonstrate the shape of a elongate light-diffusion film. FIG. 12 is a diagram provided for explaining the configuration of the long light diffusion film of Example 1. FIG. FIGS. 13A to 13B are photographs provided to explain the state of the cross section of the long light diffusion film of Example 1. FIG. 14 (a) to 14 (b) are diagrams provided for explaining the light diffusion characteristics of the long light diffusion film of Example 1. FIG. FIG. 15 is a diagram for explaining the configuration of the long light diffusion film of Comparative Example 1. FIG. FIGS. 16A to 16B are photographs provided to explain the state of the cross section of the long light diffusion film of Comparative Example 1. FIG. FIGS. 17A to 17B are a spectrum diagram and a photograph provided for explaining the light diffusion characteristics of the long light diffusion film of Comparative Example 1. FIG. FIGS. 18A to 18C are diagrams provided to explain the configuration of the first coating layer on which the first louver structure in Comparative Example 2 is formed. FIG. 19 is a diagram for explaining the configuration of the long light diffusion film of Comparative Example 2. FIGS. 20A to 20B are photographs provided to explain the state of the cross section of the long light diffusion film of Comparative Example 2. FIG. FIGS. 21A to 21B are a spectrum diagram and a photograph provided for explaining the light diffusion characteristics in the non-seam portion of the long light diffusion film of Comparative Example 2. FIG. 22A to 22B are a spectrum diagram and a photograph provided to explain the light diffusion characteristics at the joint portion of the long light diffusion film of Comparative Example 2. FIG. FIGS. 23A to 23B are diagrams provided for explaining a conventional light diffusion film.

In an embodiment of the present invention, a first louver structure and a second louver structure, in which a plurality of plate-like regions having different refractive indexes are alternately arranged in parallel in any one direction along the film surface, It is a manufacturing method of the elongate light-diffusion film which has sequentially from the bottom along a direction, Comprising: The manufacturing method of the light-diffusion film characterized by including the following process (a)-(e).
(A) The process of preparing the composition for light diffusion films containing two polymeric compounds from which refractive index differs (b) The composition for light diffusion films is apply | coated with respect to a process sheet | seat, and a 1st application layer is formed. Step (c) A step of forming a first louver structure by performing first active energy ray irradiation using a linear light source while moving the first coating layer with respect to the first coating layer (d) (E) Applying the composition for light diffusion film to the first coating layer on which the first louver structure is formed, to form a laminate comprising the first coating layer and the second coating layer (e) A second active energy ray is irradiated using a linear light source while moving the laminate composed of the first coating layer and the second coating layer with respect to the second coating layer, and the second louver structure is formed. The first step when the film is viewed from above. The step of setting the acute angle θ1 formed by the long axis direction of the linear light source in the irradiation of sexual energy rays and the long axis direction of the linear light source in the second active energy ray irradiation to a value within the range of 10 to 90 °. Embodiments of the present invention will be specifically described with reference to the drawings as appropriate. In order to facilitate understanding of the description, first, the basic principle of light diffusion in a light diffusion film and the light diffusion film of the present invention will be described. A basic configuration of a predetermined light diffusion film obtained by the manufacturing method will be described.

1. Basic Principle of Light Diffusion in Light Diffusion Film First, the basic principle of light diffusion in the light diffusion film will be described with reference to FIGS.
First, FIG. 1A shows a top view (plan view) of the light diffusion film 10, and FIG. 1B shows the light diffusion film 10 shown in FIG. A cross-sectional view of the light diffusion film 10 when cut in the vertical direction along A and viewing the cut surface from the arrow direction is shown.
2A shows an overall view of the light diffusion film 10, and FIG. 2B shows a cross-sectional view when the light diffusion film 10 of FIG. 2A is viewed from the X direction. .
As shown in the plan view of FIG. 1A, the light diffusion film 10 has a plate-like region 12 having a relatively high refractive index and a relatively refractive index in any one direction along the film surface. A low plate-like region 14 and a louver structure 13 arranged alternately in parallel are provided.
In other words, when the film is placed on a horizontal plane, it has a louver structure consisting of a plate-like region extending horizontally in the film.
In addition, as shown in the cross-sectional view of FIG. 1B, the relatively high refractive index plate-like region 12 and the relatively low refractive index plate-like region 14 each have a predetermined thickness. Also in the normal direction (film thickness direction) of the light diffusion film 10, the state of being alternately arranged in parallel is maintained.

Thereby, as shown to Fig.2 (a), when an incident angle is in a light diffusion incident angle area | region, it is estimated that incident light is diffused by the light-diffusion film 10. FIG.
That is, as shown in FIG. 1B, the incident angle of the incident light with respect to the light diffusion film 10 is a value within a predetermined angle range from parallel to the boundary surface 13 ′ of the louver structure 13, that is, the light diffusion incident angle. When the value is within the region, incident light (52, 54) passes through the relatively high refractive index plate-like region 12 in the louver structure along the film thickness direction while changing the direction. Thus, it is estimated that the traveling direction of light on the light exit surface side is not uniform.
As a result, when the incident angle is within the light diffusion incident angle region, it is estimated that the incident light is diffused by the light diffusion film 10 (52 ′, 54 ′).
On the other hand, when the incident angle of the incident light with respect to the light diffusion film 10 deviates from the light diffusion incident angle region, the incident light 56 is not diffused by the light diffusion film as shown in FIG. It is estimated that the light diffusing film 10 is transmitted as it is (56 ').
In the present invention, the “light diffusion incident angle region” refers to the angle of incident light corresponding to emitting diffused light when the angle of incident light from a point light source is changed with respect to the light diffusing film. Means range.
Further, as shown in FIG. 2A, the “light diffusion incident angle region” is an angle region determined for each light diffusion film depending on a refractive index difference or an inclination angle of the louver structure in the light diffusion film. is there.

Based on the above basic principle, the light diffusing film 10 provided with the louver structure 13 can exhibit incident angle dependency in light transmission and diffusion, for example, as shown in FIG.
Moreover, as shown in FIGS. 1-2, the light-diffusion film which has the single louver structure 13 will have "anisotropy" normally.
Here, in the present invention, “anisotropy” means, as shown in FIG. 2 (a), when incident light is diffused by the film, in the plane parallel to the film in the diffused emitted light, It means that the diffusion state of the light (the shape of the spread of the diffused light) has different properties depending on the direction in the same plane.
More specifically, as shown in FIG. 2 (a), the component perpendicular to the direction of the louver structure extending along one arbitrary direction along the film surface is selected from the components included in the incident light. On the other hand, light diffusion occurs on the other hand, among the components included in the incident light, light diffusion is difficult to occur for components parallel to the direction of the louver structure extending along any one direction along the film surface, Anisotropic light diffusion is realized.
Therefore, the shape of the spread of the diffused light in the light diffusion film having anisotropy is substantially elliptical as shown in FIG.

Further, as described above, the incident light component contributing to the light diffusion is a component perpendicular to the direction of the louver structure mainly extending along any one direction along the film surface. In the present invention, the “incident angle θ4” of incident light means an incident angle of a component perpendicular to the direction of the louver structure extending along any one direction along the film surface. Shall. At this time, the incident angle θ4 means an angle (°) when the angle with respect to the normal to the incident side surface of the light diffusion film is 0 °.
In the present invention, the “light diffusion angle region” means an angle range of diffused light obtained by fixing a point light source at an angle at which incident light is most diffused with respect to the light diffusion film. Shall.
Furthermore, in the present invention, the “diffuse light opening angle” is the width of the “light diffusion angle region” described above, and, as shown in FIG. 2B, along any one direction along the film surface. The opening angle θ5 of the diffused light when the section of the film is viewed from the direction X parallel to the direction of the extending louver structure.

In addition, as shown in FIG. 2 (a), the light diffusing film has an incident angle of incident light included in the light diffusing incident angle region. Almost the same light diffusion can be achieved.
Therefore, it can be said that the obtained light-diffusion film has the condensing effect | action which concentrates light on a predetermined location.
In addition, the direction change of the incident light inside the high refractive index region 12 in the louver structure is a step index type in which the direction changes linearly and zigzag by total reflection as shown in FIG. A gradient index type in which the direction changes in a curved shape is also conceivable.
1A and 1B, the interface between the plate-like region 12 having a relatively high refractive index and the plate-like region 14 having a relatively low refractive index is represented by a straight line for the sake of simplicity. In practice, however, the interface is slightly meandering, and each plate-like region forms a complex refractive index distribution structure with branching and extinction.
As a result, it is estimated that these have a complex effect on the light diffusion characteristics.

2. Basic Configuration Next, the basic configuration of the light diffusion film obtained by the manufacturing method of the present invention will be described with reference to FIG.
That is, as shown in FIG. 3 (c), the light diffusion film 20 obtained by the manufacturing method of the present invention includes the first louver structure 13a shown in FIG. 3 (a) and the second louver shown in FIG. 3 (b). The structure 13b is sequentially provided from below along the film thickness direction.
Furthermore, the extending direction of the plate-like region in the first louver structure 13a shown in FIG. 3A is different from the extending direction of the plate-like region in the second louver structure 13b shown in FIG. When viewed from above the film, they intersect.
Therefore, in the case of the light diffusion film 20 obtained by the manufacturing method of the present invention, for example, the light incident on the film is first diffused anisotropically by the second louver structure 13b as shown in FIG. I will let you.
Next, the anisotropic light diffused by the second louver structure 13b is further diffused by the first louver structure 13a in a direction different from that of the second louver structure 13b as shown in FIG. 3B. Will diffuse.
As a result, as shown in FIG. 3C, the light incident on the light diffusion film 20 of the present invention is diffused into a square shape, and the diffusion area of incident light can be effectively expanded. .
In addition, the "downward" mentioned above means the side close | similar to the process sheet | seat in the film thickness direction of a coating layer, when a coating layer is provided on the process sheet | seat. Therefore, it is a convenient term for describing the present invention, and does not restrict the vertical direction of the light diffusion film itself.
In addition, as shown in FIG. 3C, the “diffused area of incident light” means a plane parallel to the film at a predetermined distance from the film in the diffused emitted light when the incident light is diffused by the film. It means the area where diffused light is distributed.
Hereinafter, the manufacturing method of the light-diffusion film which concerns on this embodiment is explained in full detail.

3. Step (a): Preparation Step for Composition for Light Diffusion Film Step (a) is a step for preparing a predetermined composition for light diffusion film.
More specifically, it is preferably a step of mixing at least two polymerizable compounds having different refractive indexes, a photopolymerization initiator, and other additives as required.
In mixing, the mixture may be stirred as it is at room temperature. However, from the viewpoint of improving uniformity, for example, stirring is performed under a heating condition of 40 to 80 ° C. to obtain a uniform mixed solution. Is preferred.
Moreover, it is also preferable to add a dilution solvent so that it may become the desired viscosity suitable for coating.
Hereinafter, the step (a) will be described more specifically.

(1) High Refractive Index Polymerizable Compound (1) -1 Type Among two polymerizable compounds having different refractive indices, a polymerizable compound having a relatively high refractive index (hereinafter sometimes referred to as component (A)). Type) is not particularly limited, but the main component is preferably a (meth) acrylic acid ester containing a plurality of aromatic rings.
The reason for this is that by including a specific (meth) acrylic acid ester as the component (A), the polymerization rate of the component (A) is changed to a polymerizable compound having a relatively low refractive index (hereinafter referred to as (B). It is presumed that the polymerization rate between these components can be effectively reduced by making the polymerization rate faster than the polymerization rate of the component)) It is to be done.
As a result, when photocured, a so-called louver structure in which the plate-like regions derived from the component (A) and the plate-like regions derived from the component (B) extend alternately can be formed efficiently. .
In addition, by including a specific (meth) acrylic acid ester as the component (A), the monomer stage has sufficient compatibility with the component (B), but a plurality of stages in the polymerization process. Then, it is presumed that the louver structure can be formed more efficiently by reducing the compatibility with the component (B) to a predetermined range.
Furthermore, by including a specific (meth) acrylic acid ester as the component (A), the refractive index of the plate-like region derived from the component (A) in the louver structure is increased, and the plate derived from the component (B) The difference from the refractive index of the region can be adjusted to a value greater than or equal to a predetermined value.
Therefore, by including a specific (meth) acrylic acid ester as the component (A), combined with the characteristics of the component (B) described later, the louver structure in which plate-like regions having different refractive indexes are alternately extended can be efficiently used. Can get to.
In addition, "(meth) acrylic acid ester containing a plurality of aromatic rings" means a compound having a plurality of aromatic rings in the ester residue portion of (meth) acrylic acid ester.
“(Meth) acrylic acid” means both acrylic acid and methacrylic acid.

  Examples of the (meth) acrylic acid ester containing a plurality of aromatic rings as the component (A) include, for example, biphenyl (meth) acrylate, naphthyl (meth) acrylate, anthracyl (meth) acrylate, Benzylphenyl (meth) acrylate, biphenyloxyalkyl (meth) acrylate, naphthyloxyalkyl (meth) acrylate, anthracyloxyalkyl (meth) acrylate, benzylphenyloxyalkyl (meth) acrylate, or aromatic Examples thereof include those in which a part of hydrogen atoms on the ring are substituted by halogen, alkyl, alkoxy, halogenated alkyl or the like.

  Moreover, it is preferable that the (meth) acrylic acid ester containing a plurality of aromatic rings as the component (A) includes a compound containing a biphenyl ring, and particularly includes a biphenyl compound represented by the following general formula (1). It is preferable.

(In General Formula (1), R ^{1 to} R ¹⁰ are each independent, and at least one of R ^{1 to} R ¹⁰ is a substituent represented by the following General Formula (2), and the rest is hydrogen. It is a substituent of any one of an atom, a hydroxyl group, a carboxyl group, an alkyl group, an alkoxy group, a halogenated alkyl group, a hydroxyalkyl group, a carboxyalkyl group and a halogen atom.)

(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.)

The reason for this is that by including a biphenyl compound having a specific structure as the component (A), a predetermined difference is caused in the polymerization rate of the component (A) and the component (B), and the component (A) and the component (B) This is because it is estimated that the compatibility between the two components can be reduced by reducing the compatibility with the component to a predetermined range.
In addition, the refractive index of the plate-like region derived from the component (A) in the louver structure is increased, and the difference from the refractive index of the plate-like region derived from the component (B) can be more easily set to a predetermined value or more. Can be adjusted.

Moreover, when R < ¹ > -R < ¹⁰ > in General formula (1) contains either an alkyl group, an alkoxy group, a halogenated alkyl group, a hydroxyalkyl group, and a carboxyalkyl group, carbon number of the alkyl part is set. A value in the range of 1 to 4 is preferable.
The reason for this is that when the number of carbon atoms exceeds 4, the polymerization rate of the component (A) decreases, or the refractive index of the plate-like region derived from the component (A) becomes too low. This is because it may be difficult to efficiently form the structure.
Therefore, when R ^{1 to} R ¹⁰ in the general formula (1) include any of an alkyl group, an alkoxy group, a halogenated alkyl group, a hydroxyalkyl group, and a carboxyalkyl group, the number of carbon atoms in the alkyl portion is determined. A value in the range of 1 to 3 is more preferable, and a value in the range of 1 to 2 is more preferable.

Moreover, it is preferable that R < ¹ > -R < ¹⁰ > in General formula (1) is a substituent other than a halogenated alkyl group or a halogen atom, ie, a halogen-free substituent.
This is because dioxins are prevented from being generated when the light diffusing film is incinerated, and is preferable from the viewpoint of environmental protection.
Incidentally, in a light diffusion film having a conventional louver structure, in order to obtain a predetermined louver structure, it is general that halogen substitution is performed on the monomer component for the purpose of increasing the refractive index of the monomer component.
In this regard, the biphenyl compound represented by the general formula (1) can have a high refractive index even when halogen substitution is not performed.
Therefore, if it is a light-diffusion film formed by photocuring the composition for light-diffusion films in this invention, even if it does not contain a halogen, favorable incident angle dependence can be exhibited.
“Good incident angle dependency” means that the distinction between the light diffusion incident angle region and the non-diffuse incident angle region where the incident light is transmitted without being diffused is clearly controlled. .

Moreover, it is preferable that any one of R < ² > -R < ⁹ > in General formula (1) is a substituent represented by General formula (2).
This is because, by setting the position of the substituent represented by the general formula (2) to a position other than R ¹ and R ¹⁰ , the components (A) are oriented and crystallized in the stage before photocuring. This is because it can be effectively prevented.
Furthermore, it is liquid at the monomer stage before photocuring, and apparently can be uniformly mixed with the component (B) without using a diluting solvent or the like.
Thereby, in the stage of photocuring, the aggregation and phase separation of the component (A) and the component (B) can be performed at a fine level, and a light diffusion film having a louver structure can be obtained more efficiently. Because.
Further, from the same viewpoint, it is particularly preferable that any one of R ³ , R ⁵ , R ⁶ and R ^{8 in} the general formula (1) is a substituent represented by the general formula (2).

Moreover, it is preferable to make the repeating number m in the substituent represented by General formula (2) into the integer of 1-10 normally.
The reason for this is that when the number of repetitions m exceeds 10, the oxyalkylene chain connecting the polymerization site and the biphenyl ring becomes too long, which may inhibit the polymerization of the components (A) at the polymerization site. Because.
Therefore, the repeating number m in the substituent represented by the general formula (2) is more preferably an integer of 1 to 4, and particularly preferably an integer of 1 to 2.
From the same viewpoint, it is preferable that the carbon number n in the substituent represented by the general formula (2) is usually an integer of 1 to 4.
In addition, considering the position of the polymerizable carbon-carbon double bond that is the polymerization site is too close to the biphenyl ring, the biphenyl ring becomes sterically hindered, and the polymerization rate of the component (A) decreases, The carbon number n in the substituent represented by the general formula (2) is more preferably an integer of 2 to 4, and particularly preferably an integer of 2 to 3.

  In addition, specific examples of the biphenyl compound represented by the general formula (1) include compounds represented by the following formulas (3) to (4).

(1) -2 Molecular weight Moreover, it is preferable to make the molecular weight of (A) component into the value within the range of 200-2,500.
The reason for this is that by setting the molecular weight of component (A) within a predetermined range, the polymerization rate of component (A) can be further increased, and the copolymerizability of component (A) and component (B) can be made more effective. This is because it is estimated that it can be lowered.
As a result, it is possible to more efficiently form a louver structure in which plate-like regions derived from the component (A) and plate-like regions derived from the component (B) extend alternately when photocured. .
That is, when the molecular weight of the component (A) is less than 200, the polymerization rate decreases due to steric hindrance, becomes close to the polymerization rate of the component (B), and copolymerization with the component (B) is likely to occur. Because there is. On the other hand, when the molecular weight of the component (A) exceeds 2,500, the polymerization rate of the component (A) decreases as the difference in molecular weight with the component (B) decreases. This is because the polymerization rate of the component is close and it is estimated that copolymerization with the component (B) is likely to occur, and as a result, it may be difficult to efficiently form the louver structure.
Therefore, the molecular weight of the component (A) is more preferably set to a value within the range of 240 to 1,500, and further preferably set to a value within the range of 260 to 1,000.
The molecular weight of component (A) can be determined from the calculated value obtained from the molecular composition and the atomic weight of the constituent atoms, and can also be measured as a weight average molecular weight using gel permeation chromatography (GPC). .

(1) -3 Single use Moreover, the composition for light-diffusion films in this invention is characterized by including (A) component as a monomer component which forms the plate-shaped area | region where the refractive index in a louver structure is relatively high, However, the component (A) is preferably contained as one component.
This is because the louver structure is effectively suppressed by suppressing the variation in the refractive index in the plate-like region derived from the component (A), that is, the plate-like region having a relatively high refractive index. This is because the provided light diffusing film can be obtained more efficiently.
That is, when the compatibility with the component (B) in the component (A) is low, for example, when the component (A) is a halogen compound, the third component for compatibilizing the component (A) with the component (B) In other cases, other components (A) (for example, non-halogen compounds) are used in combination.
However, in this case, due to the influence of the third component, the refractive index in the plate-like region having a relatively high refractive index derived from the component (A) may be varied or easily lowered.
As a result, the refractive index difference from the plate-like region having a relatively low refractive index derived from the component (B) may become non-uniform or may be excessively lowered.
Therefore, it is preferable to select a monomer component having a high refractive index that is compatible with the component (B) and use it as the sole component (A).
For example, since the biphenyl compound represented by the formula (3) as the component (A) has a low viscosity, it has compatibility with the component (B), so it is used as a single component (A). can do.

(1) -4 Refractive index Moreover, it is preferable to make the refractive index of (A) component into the value within the range of 1.5-1.65.
This is because the refractive index of the plate-like region derived from the component (A) and the refractive index of the plate-like region derived from the component (B) are set by setting the refractive index of the component (A) within the range. This is because the light diffusing film having the louver structure can be more efficiently obtained by adjusting the difference from the above.
That is, when the refractive index of the component (A) is less than 1.5, the difference from the refractive index of the component (B) becomes too small, and it may be difficult to obtain an effective light diffusion angle region. Because there is. On the other hand, when the refractive index of the component (A) exceeds 1.65, the difference with the refractive index of the component (B) increases, but even an apparent compatibility state with the component (B) is formed. This is because it may be difficult.
Therefore, the refractive index of the component (A) is more preferably set to a value within the range of 1.52 to 1.65, and further preferably set to a value within the range of 1.56 to 1.6.
In addition, the refractive index of (A) component mentioned above means the refractive index of (A) component before hardening by light irradiation.
The refractive index can be measured according to, for example, JIS K0062.

(1) -5 Content Further, the content of the component (A) in the composition for light diffusion film is 100 parts by weight of the component (B) which is a polymerizable compound having a relatively low refractive index, which will be described later. A value within the range of 25 to 400 parts by weight is preferred.
The reason for this is that when the content of the component (A) is less than 25 parts by weight, the ratio of the component (A) to the component (B) decreases, and the width of the plate-like region derived from the component (A) However, this is because the width of the plate-like region derived from the component (B) is excessively small, and it may be difficult to obtain a louver structure having good incident angle dependency. Moreover, it is because the length of the louver in the thickness direction of the light diffusing film becomes insufficient, and the light diffusing property may not be exhibited. On the other hand, when the content of the component (A) exceeds 400 parts by weight, the ratio of the component (A) to the component (B) increases, and the width of the plate-like region derived from the component (A) increases. This is because the width of the plate-like region derived from the component (B) becomes excessively large, and on the contrary, it may be difficult to obtain a louver structure having good incident angle dependency. Moreover, it is because the length of the louver in the thickness direction of the light diffusing film becomes insufficient, and the light diffusing property may not be exhibited.
Therefore, the content of the component (A) is more preferably set to a value in the range of 40 to 300 parts by weight with respect to 100 parts by weight of the component (B), and a value in the range of 50 to 200 parts by weight. More preferably.

(2) Low Refractive Index Polymerizable Compound (2) -1 Type Among the two polymerizable compounds having different refractive indexes, the type of the polymerizable compound having the relatively low refractive index (component (B)) is particularly The main component is not limited, and examples thereof include urethane (meth) acrylate, (meth) acrylic polymer having (meth) acryloyl group in the side chain, (meth) acryloyl group-containing silicone resin, unsaturated polyester resin, and the like. In particular, urethane (meth) acrylate is preferable.
The reason for this is that if urethane (meth) acrylate is used, the difference between the refractive index of the plate-like region derived from the component (A) and the refractive index of the plate-like region derived from the component (B) can be adjusted more easily. This is because the light diffusion film having a louver structure can be obtained more efficiently by effectively suppressing the variation in the refractive index of the plate-like region derived from the component (B).
Therefore, in the following, urethane (meth) acrylate as the component (B) will be mainly described.
In addition, (meth) acrylate means both acrylate and methacrylate.

First, urethane (meth) acrylate is (B1) a compound containing at least two isocyanate groups, (B2) a polyol compound, preferably a diol compound, particularly preferably a polyalkylene glycol, and (B3) a hydroxyalkyl (meth). Formed from acrylate.
The component (B) includes an oligomer having a urethane bond repeating unit.
Among these, as the compound containing at least two isocyanate groups as the component (B1), for example, 2,4-tolylene diisocyanate, 2,6-tolylene diisocyanate, 1,3-xylylene diisocyanate Arocyclic polyisocyanates such as aromatic polyisocyanates such as 1,4-xylylene diisocyanate, aliphatic polyisocyanates such as hexamethylene diisocyanate, isophorone diisocyanate (IPDI), hydrogenated diphenylmethane diisocyanate, etc. Isocyanates and their biurets, isocyanurates, and adducts that are a reaction with low molecular weight active hydrogen-containing compounds such as ethylene glycol, propylene glycol, neopentyl glycol, trimethylolpropane, castor oil (for example, Xylylene diisocyanate Inert based trifunctional adduct), and the like.

Moreover, among the above-mentioned, it is especially preferable that it is an alicyclic polyisocyanate.
This is because, in the case of alicyclic polyisocyanates, compared to aliphatic polyisocyanates, it is easy to provide a difference in the reaction rate of each isocyanate group due to the conformation and the like.
This suppresses that the (B1) component reacts only with the (B2) component, or the (B1) component reacts only with the (B3) component, and the (B1) component is converted into the (B2) component and (B3) It can react reliably with a component and generation | occurrence | production of an extra by-product can be prevented.
As a result, variation in the refractive index of the plate-like region derived from the component (B) in the louver structure, that is, the low-refractive index plate-like region can be effectively suppressed.

Moreover, if it is an alicyclic polyisocyanate, compared with an aromatic polyisocyanate, the compatibility with the obtained (B) component and (A) component is reduced to a predetermined range, and a louver structure is obtained. It can be formed more efficiently.
Furthermore, if it is an alicyclic polyisocyanate, compared with an aromatic polyisocyanate, the refractive index of the (B) component obtained can be made small, Therefore The difference with the refractive index of (A) component is shown. The louver structure can be formed more efficiently, and the light diffusibility can be expressed more reliably, and the louver structure with high uniformity of diffused light within the light diffusion angle region can be formed more efficiently.
Of these alicyclic polyisocyanates, alicyclic diisocyanates containing only two isocyanate groups are preferred.
This is because if it is an alicyclic diisocyanate, it can react quantitatively with the component (B2) and the component (B3) to obtain a single component (B).
As such an alicyclic diisocyanate, isophorone diisocyanate (IPDI) can be particularly preferably mentioned.
This is because an effective difference can be provided in the reactivity of the two isocyanate groups.

Among the components that form urethane (meth) acrylate, examples of the polyalkylene glycol that is the component (B2) include polyethylene glycol, polypropylene glycol, polybutylene glycol, polyhexylene glycol, and the like. Particularly preferred is glycol.
This is because polypropylene glycol can be handled without a solvent because of its low viscosity.
Moreover, if it is a polypropylene glycol, when it hardens | cures (B) component, it becomes a favorable soft segment in the said hardened | cured material, and it can improve the handling property and mounting property of a light-diffusion film effectively. is there.
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 (B2) component is 2,300-19,500 normally, Preferably it is 4,300-14,300, Most preferably, it is 6,300-12,300.

Moreover, as a hydroxyalkyl (meth) acrylate which is a (B3) component among the components which form urethane (meth) acrylate, 2-hydroxyethyl (meth) acrylate, 2-hydroxypropyl (meth) acrylate, 3 -Hydroxypropyl (meth) acrylate, 2-hydroxybutyl (meth) acrylate, 3-hydroxybutyl (meth) acrylate, 4-hydroxybutyl (meth) acrylate, etc. are mentioned.
In addition, from the viewpoint of reducing the polymerization rate of the obtained urethane (meth) acrylate and more efficiently forming a predetermined louver structure, hydroxyalkyl methacrylate is more preferable, and 2-hydroxyethyl methacrylate is particularly preferable. Is more preferable.

Moreover, the synthesis | combination of the urethane (meth) acrylate by (B1)-(B3) component can be implemented in accordance with a conventional method.
At this time, the blending ratio of the components (B1) to (B3) is preferably set to a ratio of (B1) component: (B2) component: (B3) component = 1-5: 1: 1-5 in molar ratio. .
The reason for this is that by setting such a blending ratio, one isocyanate group of the component (B1) reacts and binds to the two hydroxyl groups of the component (B2), and two more components (B1) This is because the urethane (meth) acrylate in which the hydroxyl group of the component (B3) reacts with and bonds to the other isocyanate group possessed by each can be synthesized efficiently.
Therefore, the blending ratio of the components (B1) to (B3) is preferably set to a ratio of (B1) component: (B2) component: (B3) component = 1-3: 1: 1-3 in molar ratio. Preferably, the ratio is 2: 1: 2.

(2) -2 Weight average molecular weight Moreover, it is preferable to make the weight average molecular weight of (B) component into the value within the range of 3,000-20,000.
This is because, by setting the weight average molecular weight of the component (B) within a predetermined range, a predetermined difference is caused in the polymerization rate of the component (A) and the component (B), and the copolymerizability of both components is effectively improved. This is because it can be lowered.
As a result, when photocured, a louver structure in which plate-like regions derived from the component (A) and plate-like regions derived from the component (B) extend alternately can be efficiently formed.
That is, when the weight average molecular weight of the component (B) is less than 3,000, the polymerization rate of the component (B) is increased to be close to the polymerization rate of the component (A). This is because polymerization may easily occur, and it may be difficult to efficiently form a louver structure. On the other hand, when the weight average molecular weight of component (B) exceeds 20,000, it is difficult to form a louver structure in which plate-like regions derived from component (A) and component (B) extend alternately. This is because the compatibility with the component (A) may be excessively decreased, and the component (A) may be precipitated at the coating stage.
Therefore, the weight average molecular weight of the component (B) is more preferably set to a value within the range of 5,000 to 15,000, and further preferably set to a value within the range of 7,000 to 13,000.
In addition, the weight average molecular weight of (B) component can be measured using a gel permeation chromatography (GPC).

(2) -3 Single use Moreover, although (B) component may use together 2 or more types from which molecular structure and a weight average molecular weight differ, the refractive index of the plate-shaped area | region derived from (B) component in a louver structure From the viewpoint of suppressing variations in the number, only one type is preferably used.
That is, when a plurality of (B) components are used, the refractive index in the plate-like region where the refractive index derived from the (B) component is relatively low varies or increases, and the refraction derived from the (A) component. This is because the difference in refractive index from the plate-like region having a relatively high rate may become non-uniform or excessively decrease.

(2) -4 Refractive index Moreover, it is preferable to make the refractive index of (B) component into the value within the range of 1.4-1.55.
The reason for this is that the difference between the refractive index of the plate-like region derived from the component (A) and the plate-like region derived from the component (B) is obtained by setting the refractive index of the component (B) to a value within this range. This is because the light diffusing film having the louver structure can be more efficiently obtained by adjusting the above.
That is, when the refractive index of the component (B) is less than 1.4, the difference from the refractive index of the component (A) increases, but the compatibility with the component (A) is extremely deteriorated, and the louver structure It is because there exists a possibility that it cannot form. On the other hand, when the refractive index of the component (B) exceeds 1.55, the difference from the refractive index of the component (A) becomes too small, making it difficult to obtain the desired incident angle dependency. Because there is.
Therefore, the refractive index of the component (B) is more preferably set to a value within the range of 1.45 to 1.54, and further preferably set to a value within the range of 1.46 to 1.52.
In addition, the refractive index of (B) component mentioned above means the refractive index of (B) component before hardening by light irradiation.
The refractive index can be measured, for example, according to JIS K0062.

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 for this is that a light diffusion film having a better incident angle dependency in light transmission and diffusion and a wider light diffusion incident angle region is obtained by setting the difference in refractive index to a value within a predetermined range. Because it can.
That is, when the difference in refractive index is less than 0.01, the angle range in which incident light is totally reflected in the louver structure is narrowed, so that the opening angle in light diffusion may be excessively narrowed. is there. On the other hand, if the difference in refractive index becomes an excessively large value, the compatibility between the component (A) and the component (B) is too deteriorated, and the louver structure may not be formed.
Therefore, the difference between the refractive index of the component (A) and the refractive index of the component (B) is more preferably set to a value in the range of 0.05 to 0.5, More preferably, the value is within the range.
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) -5 Content Further, the content of the component (B) in the composition for light diffusion film is within the range of 10 to 80% by weight with respect to 100% by weight of the total amount of the composition for light diffusion film. It is preferable to use a value.
The reason for this is that when the content of the component (B) is less than 10% by weight, the ratio of the component (B) to the component (A) decreases, and the width of the plate-like region derived from the component (B) However, this is because the width of the plate-like region derived from the component (A) is excessively small, and it may be difficult to obtain a louver structure having good incident angle dependency. Moreover, it is because the length of the louver in the thickness direction of the light diffusion film may be insufficient. On the other hand, when the content of the component (B) exceeds 80% by weight, the ratio of the component (B) to the component (A) increases, and the width of the plate-like region derived from the component (B) increases. This is because the width of the plate-like region derived from the component (A) is excessively large and, on the contrary, it may be difficult to obtain a louver structure having good incident angle dependency. Moreover, it is because the length of the louver in the thickness direction of the light diffusion film may be insufficient.
Therefore, it is more preferable to make content of (B) component into the value within the range of 20 to 70 weight% with respect to 100 weight% of the total amount of the composition for light diffusion films, More preferably, the value is within the range.

(3) Photopolymerization initiator Moreover, in the composition for light diffusion films in this invention, it is preferable to contain a photoinitiator as (C) component as needed.
This is because a louver structure can be formed efficiently when the composition for a light diffusing film is irradiated with active energy rays by containing a photopolymerization initiator.
Here, the photopolymerization initiator refers to a compound that generates radical species by irradiation with active energy rays such as ultraviolet rays.

Examples of the photopolymerization initiator include benzoin, benzoin methyl ether, benzoin ethyl ether, benzoin isopropyl ether, benzoin-n-butyl ether, benzoin isobutyl ether, acetophenone, dimethylaminoacetophenone, and 2,2-dimethoxy-2-phenylacetophenone. 2,2-diethoxy-2-phenylacetophenone, 2-hydroxy-2-methyl-1-phenylpropan-1-one, 1-hydroxycyclohexyl phenyl ketone, 2-methyl-1- [4- (methylthio) phenyl] 2-morpholino-propan-1-one, 4- (2-hydroxyethoxy) phenyl-2- (hydroxy-2-propyl) ketone, benzophenone, p-phenylbenzophenone, 4,4-diethyl Minobenzophenone, dichlorobenzophenone, 2-methylanthraquinone, 2-ethylanthraquinone, 2-tertiarybutylanthraquinone, 2-aminoanthraquinone, 2-methylthioxanthone, 2-ethylthioxanthone, 2-chlorothioxanthone, 2,4-dimethylthioxanthone, 2,4-diethylthioxanthone, benzyldimethyl ketal, acetophenone dimethyl ketal, p-dimethylamine benzoate, oligo [2-hydroxy-2-methyl-1- [4- (1-methylvinyl) phenyl] propane and the like Of these, one of them may be used alone, or two or more of them may be used in combination.
In addition, as content in the case of containing a photoinitiator, it is set as the value within the range of 0.2-20 weight part with respect to 100 weight part of total amounts of (A) component and (B) component. Preferably, the value is in the range of 0.5 to 15 parts by weight, and more preferably in the range of 1 to 10 parts by weight.

(4) Other Additives Additives other than the above-described compounds can be appropriately added within a range not impairing the effects of the present invention.
Examples of such additives include antioxidants, ultraviolet absorbers, antistatic agents, polymerization accelerators, polymerization inhibitors, infrared absorbers, plasticizers, diluent solvents, and leveling agents.
In general, the content of such additives is preferably set to a value in the range of 0.01 to 5 parts by weight with respect to 100 parts by weight of the total amount of the component (A) and the component (B). The value is more preferably in the range of 0.02 to 3 parts by weight, and still more preferably in the range of 0.05 to 2 parts by weight.

4). Step (b): First Application Step As shown in FIG. 4 (a), the step (b) applies the prepared light diffusion film composition to the step sheet 2, and the first application layer. It is a process of forming 1a.
Either a plastic film or paper can be used as the process sheet.
Among these, examples of the plastic film include polyester films such as polyethylene terephthalate films, polyolefin films such as polyethylene films and polypropylene films, cellulose films such as triacetyl cellulose films, and polyimide films.
Examples of the paper include glassine paper, coated paper, and laminated paper.
Moreover, when the process mentioned later is considered, as the process sheet | seat 2, it is preferable that it is a plastic film excellent in the dimensional stability with respect to a heat | fever or an active energy ray.
As such a plastic film, among those described above, a polyester film, a polyolefin film and a polyimide film are preferably exemplified.

In addition, for the process sheet, a release layer is provided on the application surface side of the composition for light diffusion film in the process sheet in order to easily peel the obtained light diffusion film from the process sheet after photocuring. Is preferred.
Such a release layer can be formed using a conventionally known release agent such as a silicone release agent, a fluorine release agent, an alkyd release agent, or an olefin release agent.
In addition, it is preferable that the thickness of the process sheet is usually a value within a range of 25 to 200 μm.

  Examples of the method for applying the light diffusing film composition on the process sheet include conventionally known methods such as knife coating, roll coating, bar coating, blade coating, die coating, and gravure coating. Can be performed.

Moreover, it is preferable to make the film thickness of a 1st application layer into the value within the range of 80-700 micrometers.
This is because the first louver structure can be formed more efficiently by setting the film thickness of the first coating layer to a value within this range.
That is, when the thickness of the first coating layer is less than 80 μm, the length of the first louver structure to be formed is insufficient and incident light that goes straight through the first louver structure increases. This is because it may be difficult to obtain the uniformity of the intensity of the diffused light within the light diffusion angle region. On the other hand, when the thickness of the first coating layer exceeds 700 μm, the first coating layer was formed in the initial stage when the first coating layer was irradiated with active energy rays to form the first louver structure. This is because the direction of photopolymerization is diffused by the louver structure, and it may be difficult to form a desired louver structure.
Therefore, the thickness of the first coating layer is more preferably set to a value within the range of 100 to 500 μm, and further preferably set to a value within the range of 120 to 300 μm.

5. Step (c): First active energy ray irradiation step In step (c), the first coating layer 1a is moved in the moving direction E with respect to the first coating layer 1a as shown in FIG. In this step, the first active energy ray irradiation 150a is performed using the linear light source 125a while moving along the first louver structure 13a.
More specifically, for example, as shown in FIG. 5A, an ultraviolet irradiation device 120 in which a condensing cold mirror 122 is provided on a linear ultraviolet lamp 125a (for example, a commercially available product is an eyepiece). By placing the heat ray cut filter 121 and the light-shielding plate 123 (123a, 123b) on a graphics (ECS-4011GX, etc.), the active energy ray 150a consisting only of direct light whose irradiation angle is controlled is taken out. The first coating layer 1a formed on the process sheet 2 is irradiated.

Moreover, as shown in FIG. 6A, when viewed from above the film, along the long axis direction of the linear light source 125a in the first active energy ray irradiation and the moving direction E of the first coating layer 1a. It is preferable to set the acute angle θ2 formed by the virtual line E ′ to a value within the range of 10 to 80 °.
The reason for this is that by defining the arrangement angle of the linear light source in this way, coupled with the arrangement angle of the linear light source in the step (e) described later, not only the direction along the longitudinal direction of the incident light, This is because it is possible to more efficiently manufacture a long light diffusion film in which the diffusion area of incident light is effectively expanded by diffusing light in the direction perpendicular to the long direction.
That is, when the value θ2 is less than 10 °, generally, the light diffusion characteristics in the direction along the longitudinal direction of the film are excessive, although depending on the arrangement angle of the linear light source in the step (e) described later. This is because the diffusion area of incident light may be excessively reduced. On the other hand, when the value θ2 exceeds 80 °, generally, the light diffusion characteristics in the direction perpendicular to the longitudinal direction of the film are excessive, depending on the arrangement angle of the linear light source in the step (e) described later. This is because the diffusion area of incident light may become excessively small.
Therefore, when viewed from above the film, the acute angle θ2 formed by the major axis direction of the linear light source in the first active energy ray irradiation and the virtual line along the moving direction of the first coating layer is 35 to 55. A value within the range of ° is more preferable, a value within the range of 40 to 50 ° is more preferable, and a value within the range of 44 to 46 ° is even more preferable.
Note that the distance between the linear light source 125a and the coating layer 1a is preferably substantially the same at any position.

Further, as the irradiation angle of the active energy ray, as shown in FIG. 5B, the irradiation angle θ6 when the angle of the normal to the surface of the first coating layer 1a is 0 ° is usually −80 to A value within the range of 80 ° is preferable.
The reason for this is that when the irradiation angle is outside the range of −80 to 80 °, the influence of reflection on the surface of the first coating layer 1a becomes large, and it is difficult to form a sufficient louver structure. This is because it may become.
The irradiation angle θ6 preferably has a width (irradiation angle width) θ6 ′ of 1 to 80 °.
This is because, when the irradiation angle width θ6 ′ is a value less than 1 °, the moving speed of the coating layer must be excessively decreased, and the production efficiency may be decreased. On the other hand, when the irradiation angle width θ6 ′ exceeds 80 °, the irradiation light is excessively dispersed and it may be difficult to form the louver structure.
Therefore, the irradiation angle width θ6 ′ of the irradiation angle θ6 is more preferably set to a value within the range of 2 to 45 °, and further preferably set to a value within the range of 5 to 20 °.
In addition, when it has irradiation angle width | variety (theta) 6 ', let the angle of the intermediate position just be irradiation angle (theta) 6.

In addition, the first active energy ray irradiation is performed through a light shielding plate having a long groove-like active energy ray transmitting portion, and the longitudinal direction of the active energy ray transmitting portion is parallel to the longitudinal direction of the linear light source. Preferably there is.
The active energy ray transmitting portion may be in any form as long as it is in a state of transmitting the active energy ray.
For example, it may be made of quartz glass, or may be a simple space where no light shielding material is present.
Specifically, as shown in FIG. 7, it is performed through a long groove-like gap (active energy ray transmitting portion) formed by two light shielding plates 123 (123a, 123b) and the length of the long groove-like gap. The direction is preferably a direction parallel to the long axis direction of the linear light source 125a.
By arranging the light shielding plate in this way, the irradiation angle θ6 of the active energy ray 150a shown in FIG. 5A is adjusted to a value within a predetermined range, and depending on each position on the surface of the first coating layer 1a, This is because the active energy ray 150a from the linear light source 125a can be effectively suppressed from being irradiated at an excessively different angle.
As a result, the inclination angle of the plate-like region in the formed louver structure can be made uniform, and as a result, the light diffusion characteristics of the obtained long light diffusion film can be made uniform.

Moreover, it is preferable to make the peak illumination intensity in the surface of the 1st application layer in 1st active energy ray irradiation into the value within the range of 0.1-50 mW / cm < ² >.
This is because the first louver structure can be formed more efficiently by setting the peak illuminance in the first active energy ray irradiation to a value within such a range.
That is, if the peak illuminance is less than 0.1 mW / cm ² , it may be difficult to clearly form the first louver structure. On the other hand, when the peak illuminance is a value exceeding 50 mW / cm ² , it is estimated that the curing speed becomes too fast, and the first louver structure may not be clearly formed.
Therefore, the peak illuminance on the surface of the first coating layer in the first active energy ray irradiation is more preferably set to a value within the range of 0.3 to 10 mW / cm ² , and 0.5 to 5 mW / cm ² . More preferably, the value is within the range.

Moreover, it is preferable to make the integrated light quantity in the surface of the 1st coating layer in 1st active energy ray irradiation into the value within the range of 5-300 mJ / cm < ² >.
The reason for this is that the first louver structure can be formed more efficiently by setting the integrated light quantity in the first active energy ray irradiation to a value within this range.
That is, when the integrated light quantity is less than 5 mJ / cm ² , it may be difficult to sufficiently extend the first louver structure from the top to the bottom. On the other hand, when the integrated light quantity exceeds 300 mJ / cm ² , the resulting light diffusion film may be colored.
Therefore, it is more preferably set to a value within the range of accumulated light amount of 10~200mJ / cm ² in the first surface of the coating layer in the first active-energy ray irradiation, a value in the range of 20~150mJ / cm ² More preferably.

Moreover, it is preferable to make the moving speed of the 1st application layer into the value within the range of 0.1-10 m / min.
This is because the first louver structure can be formed more efficiently by setting the moving speed of the first coating layer to a value within this range.
That is, when the moving speed of the first coating layer becomes a value less than 0.1 m / min, productivity may be excessively lowered. On the other hand, when the moving speed of the first coating layer exceeds 10 m / min, the first coating layer is hardened, in other words, faster than the formation of the first louver structure, and the activity on the first coating layer is increased. This is because the incident angle of the energy beam changes and the formation of the first louver structure may be insufficient.
Therefore, the moving speed of the first coating layer is more preferably set to a value within the range of 0.2 to 5 m / min, and further preferably set to a value within the range of 0.5 to 3 m / min.

It is also preferable to irradiate the upper surface of the first coating layer with active energy rays in a state where the active energy ray transmitting sheet is laminated.
The reason is that by laminating the active energy ray transmitting sheet, the influence of oxygen inhibition can be effectively suppressed and the first louver structure can be formed more efficiently.
That is, by laminating the active energy ray-transmitting sheet on the upper surface of the first coating layer, the upper surface of the first coating layer is allowed to pass through the sheet while stably preventing contact with oxygen. This is because the active energy ray can be efficiently irradiated to the first coating layer.
In addition, as an active energy ray permeable sheet, if the active energy ray can permeate | transmit among the process sheets described in the process (b) (application | coating process), it can use without a restriction | limiting in particular.

In addition to the first active energy ray irradiation as the step (c), it is preferable to further irradiate the active energy ray so that the first application layer has an integrated light amount that is sufficiently cured.
Since the active energy ray at this time is intended to sufficiently cure the first coating layer, it is preferable to use random light in any traveling direction instead of parallel light.

6). Step (d): Second Application Step As shown in FIG. 4 (c), the step (d) is a first application layer 1a ′ in which the light diffusing film composition is formed with the first louver structure 13a. Is a step of forming a laminate 1c composed of a first coating layer 1a 'and a second coating layer 1b.
When forming the first louver structure 13a, if an active energy ray transmitting sheet is used, the above operation is performed after the sheet is peeled to expose the surface of the coating layer 1a '.
Moreover, it is preferable that the composition for light diffusion films used for formation of the 2nd coating layer 1b uses the same thing as the composition for light diffusion films used for formation of the 1st coating layer 1a.
This is because by using the same composition for light diffusion film, reflection at the interface between the coating layer 1a ′ and the coating layer 1b ′ can be suppressed, and the adhesion can be improved.
Examples of the method for applying the light diffusing film composition on the first coating layer on which the first louver structure is formed include, for example, knife coating, roll coating, bar coating, blade coating, and die coating. It can carry out by the method similar to the process (b) mentioned above, such as a method and a gravure coat method.

Moreover, it is preferable to make the film thickness of a 2nd coating layer into the value within the range of 80-700 micrometers.
This is because the second louver structure can be formed more efficiently by setting the thickness of the second coating layer to a value within this range.
That is, when the thickness of the second coating layer is less than 80 μm, the length of the second louver structure to be formed is insufficient, and the incident light that goes straight through the second louver structure increases. This is because it may be difficult to obtain the uniformity of the intensity of the diffused light within the light diffusion angle region. On the other hand, when the thickness of the second coating layer exceeds 700 μm, the second coating layer was formed at the initial stage when the second coating layer was irradiated with active energy rays to form the second louver structure. This is because the direction of photopolymerization is diffused by the louver structure, and it may be difficult to form a desired louver structure.
Therefore, the thickness of the second coating layer is more preferably set to a value within the range of 100 to 500 μm, and further preferably set to a value within the range of 120 to 300 μm.

7). Step (e): Second Active Energy Ray Irradiation Step In step (e), as shown in FIG. 4D, the first louver structure 13a is formed on the second coating layer 1b. In the step of forming the second louver structure 13b by performing the second active energy ray irradiation using the linear light source 125b while moving the laminate 1c composed of the coating layer 1a 'and the second coating layer 1b. 6B, when viewed from above the film, the major axis direction of the linear light source 125a in the first active energy ray irradiation and the linear light source in the second active energy ray irradiation. This is a step of setting the acute angle θ1 formed by the major axis direction of 125b to a value in the range of 10 to 90 °.

That is, in the two active energy ray irradiation steps using the linear light source, the extending direction of the plate-like region in the first louver structure is defined by defining the relationship between the arrangement angles of the respective linear light sources within a predetermined range. And the elongate light-diffusion film which cross | intersects the extension direction of the plate-shaped area | region in a 2nd louver structure at a predetermined angle can be manufactured efficiently.
Therefore, long light that effectively spreads the diffusion area of incident light by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction orthogonal to the longitudinal direction. A diffusion film can be manufactured efficiently.
More specifically, incident light can be diffused in a direction along the longitudinal direction and in a direction orthogonal to the longitudinal direction without connecting a plurality of light diffusion films as in the prior art. A long light diffusion film can be obtained.

That is, if the acute angle θ1 shown in FIG. 6B is less than 10 °, the diffusion area of incident light may be excessively reduced.
Therefore, when viewed from above the film, the acute angle θ1 formed by the major axis direction of the linear light source in the first active energy ray irradiation and the major axis direction of the linear light source in the second active energy ray irradiation is 80. The value is more preferably in the range of -90 °, more preferably in the range of 85-90 °, and even more preferably in the range of 89-90 °.

Moreover, as shown in FIG. 6B, when viewed from above the film, the long axis direction of the linear light source 125b in the second active energy ray irradiation and the first louver structure 13a are formed. It is preferable that the acute angle θ3 formed by the virtual line E ′ along the moving direction E of the laminate 1c composed of the coating layer 1a ′ and the second coating layer 1b is set to a value in the range of 10 to 80 °.
The reason for this is that, by defining the arrangement angle of the linear light source in this way, coupled with the arrangement angle of the linear light source in the step (c) described above, not only the direction along the longitudinal direction of the incident light, This is because it is possible to more efficiently manufacture a long light diffusion film in which the diffusion area of incident light is effectively expanded by diffusing light in the direction perpendicular to the long direction.
That is, when the value θ3 is less than 10 °, generally, the light diffusion characteristics in the direction along the longitudinal direction of the film are excessive, although depending on the arrangement angle of the linear light source in the step (c) described above. This is because the diffusion area of incident light may be excessively reduced. On the other hand, when the value θ3 exceeds 80 °, generally, the light diffusion characteristics in the direction orthogonal to the longitudinal direction of the film are excessive, depending on the arrangement angle of the linear light source in the step (c) described above. This is because the diffusion area of incident light may become excessively small.
Therefore, when viewed from above the film, a virtual line along the major axis direction of the linear light source in the second active energy ray irradiation and the moving direction of the laminate composed of the first coating layer and the second coating layer Is more preferably set to a value within a range of 35 to 55 °, more preferably a value within a range of 40 to 50 °, and a value within a range of 44 to 46 °. It is more preferable.
Note that the distance between the linear light source 125b and the coating layer 1b is preferably substantially the same at any position.
In addition, the irradiation angle and irradiation angle width of the active energy ray are preferably set in the same numerical range as in the case of the first active energy ray irradiation described with reference to FIGS.

6B, when viewed from above the film, the long axis direction of the linear light source 125a in the first active energy ray irradiation and the linear light source 125b in the second active energy ray irradiation. The major axis direction is symmetrical with respect to an imaginary line E ″ perpendicular to the moving direction E of the laminate composed of the first coating layer 1a ′ and the second coating layer 1b. preferable.
This is because the incident light can be diffused more uniformly in the obtained light diffusion film by arranging the linear light source in the second active energy ray irradiation in this way.
That is, particularly in the case of θ2 = 45 °, θ3 = 45 °, or when each is a peripheral value thereof, the linear light sources are arranged so as to be symmetrical with respect to each other, and FIG. As shown in FIG. 4, the spread in the left-right direction and the spread in the vertical direction in the diffused light can be maximized.
Therefore, when such a light diffusion film is applied to a screen, the horizontal viewing angle and the vertical viewing angle can be maximized.

Here, the relationship between the arrangement angle of the linear light source (≈the extending direction of the plate-like region) and the diffusion area of the incident light will be described with reference to FIGS.
That is, FIGS. 8A to 8E show the first louver structure 13a on the left side and the diffusion state 50 'of light incident thereon, and the second louver structure 13b on the right side and incident thereon. A diffusion state 51 ′ of diffused light by the first louver structure 13a is shown.
First, FIG. 8A shows the degree of diffusion of incident light when θ1 = 90 °, θ2 = 45 °, and θ3 = 45 °, but the final incident light diffusion area becomes sufficiently wide. (51 ').
On the other hand, FIG. 8B shows the degree of diffusion of incident light when θ1 = 60 °, θ2 = 30 °, and θ3 = 30 °. Compared to the case of FIG. It turns out that the light diffusion characteristic to the direction along the elongate direction E 'of this falls, and the diffusion area of incident light becomes small (51').
FIG. 8C shows the diffusion state of incident light in the case of θ1 = 60 °, θ2 = 60 °, and θ3 = 60 °. Compared to the case of FIG. It turns out that the light diffusion characteristic to the direction orthogonal to the elongate direction E 'falls, and the diffusion area of incident light becomes small (51').
On the other hand, FIG. 8D shows the degree of diffusion of incident light when θ1 = 30 °, θ2 = 15 °, and θ3 = 15 °. Compared to the case of FIG. It can be seen that the light diffusion characteristics in the direction along the long direction E ′ of the light source are further reduced, and the diffusion area of the incident light is further reduced (51 ′).
FIG. 8 (e) shows the diffusion of incident light when θ1 = 30 °, θ2 = 75 °, and θ3 = 75 °. Compared to the case of FIG. It can be seen that the light diffusion characteristics in the direction orthogonal to the longitudinal direction E ′ of the light source are further reduced, and the diffusion area of incident light is further reduced (51 ′).
In addition, the photograph of the diffused light corresponding to Fig.8 (a)-(e) is shown to Fig.9 (a)-(e).

  Further, as shown in FIG. 7, the second active energy ray irradiation is also performed through a long groove-like gap formed by two light shielding plates for the same reason as in the case of the first active energy ray irradiation. In addition, it is preferable that the longitudinal direction of the long groove-like gap is parallel to the long axis direction of the linear light source.

Moreover, it is preferable to make the peak illumination intensity in the surface of the 2nd coating layer in 2nd active energy ray irradiation into the value within the range of 0.1-50 mW / cm < ² >.
This is because the second louver structure can be more efficiently formed by setting the peak illuminance in the second active energy ray irradiation to a value within such a range.
That is, if the peak illuminance is less than 0.1 mW / cm ² , it may be difficult to clearly form the second louver structure. On the other hand, when the peak illuminance is a value exceeding 50 mW / cm ² , it is estimated that the curing speed is too high, and the second louver structure may not be clearly formed.
Therefore, the peak illuminance on the surface of the second coating layer in the second active energy ray irradiation is more preferably set to a value within the range of 0.3 to 10 mW / cm ² , and 0.5 to 5 mW / cm ² . More preferably, the value is within the range.

Moreover, it is preferable to make the integrated light quantity in the surface of the 2nd application layer in 2nd active energy ray irradiation into the value within the range of 5-300 mJ / cm < ² >.
This is because the second louver structure can be formed more efficiently by setting the integrated light quantity in the second active energy ray irradiation to a value within this range.
That is, when the integrated light quantity becomes a value less than 5 mJ / cm ² , it may be difficult to sufficiently extend the second louver structure from above to below. On the other hand, when the integrated light quantity exceeds 300 mJ / cm ² , the resulting light diffusion film may be colored.
Therefore, it is more preferably set to a value within the range of accumulated light amount of 10~200mJ / cm ² in the second surface of the coating layer in the second active energy ray irradiation, a value in the range of 20~150mJ / cm ² More preferably.

  Also in the second active energy ray irradiation, for the same reason as in the case of the first active energy ray irradiation, a laminate composed of the first coating layer and the second coating layer on which the first louver structure is formed. The moving speed of the body is preferably set to a value within the range of 0.1 to 10 m / min, more preferably set to a value within the range of 0.2 to 5 m / min, and 0.5 to 3 m / min. More preferably, the value is within the range.

From the same viewpoint as in the case of the step (c), it is also preferable to irradiate the upper surface of the second coating layer with the active energy ray in a state where the active energy ray transmitting sheet is laminated.
In addition to the second active energy ray irradiation as the step (e), it is also preferable to further irradiate the active energy ray so that the second application layer has an integrated light amount that is sufficiently cured.
Since the active energy ray at this time is intended to sufficiently cure the second coating layer, it is preferable to use random light in any traveling direction instead of parallel light.
In addition, the process (d)-(e) mentioned above may be performed continuously with process (b)-(c) using one conveyor, and obtained by process (b)-(c). The first coating layer on which the first louver structure is formed may be collected in the form of a roll, and this may be separately placed on a conveyor to perform steps (b) to (c).
Therefore, in the former case, the linear light source in step (c) and the linear light source in step (e) are arranged separately, and in the latter case, the same linear light source is arranged at an angle of arrangement. It may be used after being changed (turned).

8). Light diffusion film Hereinafter, the light diffusion film obtained by the production method of the present invention will be described.

(1) First louver structure (1) -1 Refractive index In the first louver structure, a difference in refractive index between plate-like regions having different refractive indexes, that is, refraction of a plate-like region having a relatively high refractive index. The difference between the refractive index and the refractive index of the plate-like region having a relatively low refractive index is preferably set to a value of 0.01 or more.
This is because, by setting the difference in refractive index to a value of 0.01 or more, incident light is stably reflected in the first louver structure, and the incident angle dependency derived from the first louver structure. It is because it can improve more.
More specifically, when the difference in refractive index is less than 0.01, the angle range at which incident light is totally reflected in the first louver structure is narrowed, and the incident angle dependency is excessively reduced. It is because there is a case to do.
Therefore, the difference in refractive index between the plate-like regions having different refractive indexes in the first louver structure is more preferably 0.03 or more, and further preferably 0.05 or more.
The difference between the refractive index of the high refractive index plate-like region and the refractive index of the low refractive index plate-like region is preferably as large as possible. However, from the viewpoint of selecting a material capable of forming the first louver structure, 0.3 is preferable. The degree is considered the upper limit.

In the first louver structure, the refractive index of the plate-like region having a relatively high refractive index is preferably set to a value in the range of 1.5 to 1.7.
The reason for this is that when the refractive index of the high refractive index plate-like region is less than 1.5, the difference from the low refractive index plate-like region becomes too small, making it difficult to obtain a desired louver structure. Because there is. On the other hand, when the refractive index of the high refractive index plate-shaped region exceeds 1.7, the compatibility between the material substances in the composition for light diffusion film may be excessively lowered.
Therefore, it is more preferable to set the refractive index of the high refractive index plate-like region in the first louver structure to a value in the range of 1.52 to 1.65, and a value in the range of 1.55 to 1.6. More preferably.
In addition, the refractive index of a high refractive index plate-shaped area | region can be measured according to JISK0062, for example.

In the first louver structure, the refractive index of the plate-like region having a relatively low refractive index is preferably set to a value in the range of 1.4 to 1.5.
The reason for this is that when the refractive index of the low refractive index plate-like region is less than 1.4, the rigidity of the obtained light diffusion film may be lowered. On the other hand, when the refractive index of the low refractive index plate-like region exceeds 1.5, the difference from the refractive index of the high refractive index plate-like region becomes too small, and it is difficult to obtain a desired louver structure. This is because it may become.
Therefore, it is more preferable to set the refractive index of the low refractive index plate-like region in the first louver structure to a value in the range of 1.42 to 1.48, and to a value in the range of 1.44 to 1.46. More preferably.
In addition, the refractive index in a low refractive index plate-shaped area | region can be measured according to JISK0062, for example.

(1) -2 Width Also, as shown in FIG. 10A, in the first louver structure 13a, the widths of the high refractive index plate region 12 and the low refractive index plate region 14 having different refractive indexes (S1, S2) is preferably set to a value in the range of 0.1 to 15 μm.
The reason for this is that the width of these plate-like regions is set to a value in the range of 0.1 to 15 μm so that incident light is more stably reflected in the first louver structure, and the first louver structure. This is because the incident angle dependency derived from can be improved more effectively.
That is, if the width of the plate-like region is a value less than 0.1 μm, it may be difficult to show light diffusion regardless of the incident angle of incident light. On the other hand, when the width exceeds 15 μm, the light traveling straight in the first louver structure increases, and the uniformity of the diffused light may deteriorate.
Therefore, in the first louver structure, the width of the plate-like regions having different refractive indexes is more preferably set to a value in the range of 0.5 to 10 μm, and the value in the range of 1 to 5 μm. Further preferred.
In addition, the width | variety, length, etc. of the plate-shaped area | region which comprises a 1st louver structure can be measured by observing a film cross section with an optical digital microscope.

(1) -3 Inclination Angle As shown in FIG. 10A, in the first louver structure, a plurality of high refractive index plate regions 12 and a plurality of low refractive index plate regions 14 having different refractive indexes are provided. It is preferable that they are arranged in parallel at a constant inclination angle θa with respect to the film thickness direction.
The reason for this is that by making each inclination angle θa of the plate-like region constant, the incident light is more stably reflected in the first louver structure, and the incident angle dependency derived from the first louver structure. This is because the can be further improved.
Note that θa is 0 ° with respect to the normal of the film surface measured in a cross section when the film is cut in a plane perpendicular to the first louver structure extending in one arbitrary direction along the film surface. In this case, the inclination angle (°) of the plate-like region is meant.
More specifically, as shown in FIG. 10 (a), it means the angle on the narrow side of the angle formed between the normal line of the upper end surface of the first louver structure and the uppermost part of the plate-like region. As shown in FIG. 10A, the inclination angle when the plate-like region is inclined to the right is used as a reference, and the inclination angle when the plate-like region is inclined to the left is expressed as minus.

Further, as shown in FIG. 10B, it is also preferable that the plate-like regions (12, 14) having different refractive indexes in the first louver structure are curved from above to below along the film thickness direction. .
This is because the plate-like region is curved, so that the balance between reflection and transmission in the first louver structure can be complicated, and the opening angle of the diffused light can be effectively expanded.
In addition, it is thought that such a curved louver structure is obtained by delaying the polymerization reaction rate by ultraviolet rays in the thickness direction of the coating film.
Specifically, it can be formed by suppressing the illuminance of ultraviolet rays emitted from a linear light source and moving the coating film in an irradiated state at a low speed.

(1) -4 Thickness The thickness of the first louver structure, that is, the length L1 of the first louver structure existing portion in the normal direction of the film surface shown in FIGS. A value in the range of 50 to 500 μm is preferable.
This is because the length of the first louver structure is stably secured along the film thickness direction by setting the thickness of the first louver structure to a value within this range, and the first louver structure This is because the incident light can be more stably reflected in the inside, and the uniformity of the intensity of the diffused light within the light diffusion angle region derived from the first louver structure can be further improved.
That is, when the thickness L1 of the first louver structure becomes a value of less than 50 μm, the length of the first louver structure is insufficient, and incident light that goes straight through the first louver structure increases. This is because it may be difficult to obtain the uniformity of the intensity of the diffused light within the light diffusion angle region. On the other hand, when the thickness L1 of the first louver structure exceeds 500 μm, when the first louver structure is formed by irradiating the composition for light diffusion film with active energy rays, This is because the traveling direction of photopolymerization is diffused by the formed louver structure, and it may be difficult to form a desired first louver structure.
Therefore, the thickness L1 of the first louver structure is more preferably set to a value within the range of 70 to 300 μm, and further preferably set to a value within the range of 80 to 200 μm.

(1) -5 Stretching direction When viewed from above the film, the acute angle formed by the extending direction of the plate-like region in the first louver structure and the long direction of the film is within a range of 10 to 80 °. It is preferable to use a value.
This is because, by setting the extending direction of the plate-like region in the first louver structure to a value within this range, the incident light is coupled in the longitudinal direction in combination with the extending direction of the plate-like region in the second louver structure. This is because the diffusion area of incident light can be effectively expanded by diffusing light not only in the direction along the direction but also in the direction perpendicular to the longitudinal direction.
That is, when the acute angle is less than 10 °, generally, the light diffusion characteristic in the direction along the longitudinal direction of the film is excessively lowered although it depends on the extending direction of the plate-like region in the second louver structure. This is because the diffusion area of incident light may become excessively small. On the other hand, when the acute angle exceeds 80 °, generally, the light diffusion characteristics in the direction perpendicular to the longitudinal direction of the film is excessive, although it depends on the extending direction of the plate-like region in the second louver structure. This is because the diffusion area of incident light may be excessively reduced.
Therefore, when viewed from above the film, the acute angle formed by the extending direction of the plate-like region in the first louver structure and the longitudinal direction of the film is more preferably set to a value within the range of 35 to 55 °. The value is more preferably in the range of 40 to 50 °, and more preferably in the range of 44 to 46 °.

(2) Second louver structure Since the configuration of the second louver structure is basically the same as the configuration of the first louver structure, description thereof is omitted.

(3) Film thickness Moreover, it is preferable to make the film thickness of a light-diffusion film into the value within the range of 50-500 micrometers.
The reason for this is that when the film thickness is less than 50 μm, the length of the louver structure in the film thickness direction formed in the film becomes excessively short, and the incident light that goes straight through the louver structure increases. This is because it may be difficult to obtain sufficient incident angle dependency. On the other hand, when the film thickness exceeds 500 μm, the irradiation light is irradiated for a long time, so that the mass productivity is excessively reduced or the irradiation light is diffused by the louver structure formed in the initial stage. This is because it may be difficult to form a desired louver structure.
Therefore, the film thickness of the light diffusion film is more preferably set to a value within the range of 70 to 300 μm, and further preferably set to a value within the range of 80 to 200 μm.
In the film thickness direction of the light diffusion film, for example, there may be a portion where the louver structure does not exist in the surface layer portion or the like.
Therefore, the film thickness of the light diffusion film is equal to or greater than the sum of the thickness of the first louver structure and the thickness of the second louver structure.

(4) Shape of film Moreover, the shape of the light-diffusion film obtained by the manufacturing method of this invention is elongate.
More specifically, as shown to Fig.11 (a), it is preferable to make length L2 of the short direction in the light-diffusion film 10 into the value within the range of 0.1-3m, 0.5-2m A value within the range is more preferable.
On the other hand, the length in the longitudinal direction is not particularly limited.
That is, according to the manufacturing method of the present invention, a light diffusion film capable of diffusing incident light not only in a direction along the longitudinal direction but also in a direction orthogonal to the longitudinal direction is continuously formed. This is because it can continue to be manufactured.
Accordingly, the length L3 in the longitudinal direction is preferably 3 m or more, and more preferably 15 m or more.
This is because the film has such a shape, so that the incident light can be diffused not only in the direction along the longitudinal direction but also in the direction perpendicular to the longitudinal direction. This is because a light diffusion film having a large area can be obtained.

Moreover, as shown in FIG.11 (b), it is preferable that the light-diffusion film 20 is wound in roll shape.
The reason for this is that, by forming a roll shape, a long and large-area light diffusing film capable of diffusing incident light in a direction perpendicular to the longitudinal direction or in the vicinity thereof is obtained. Because it can.
Moreover, it is because the handleability in storage and carrying can be improved.
More specifically, in the case of a roll, workability is improved as compared with production while dropping on a sheet.
Moreover, if it is a roll shape, even if it is a case where the size of the display etc. which are going to apply a film varies widely, it can chip-cut to a required size later.
Moreover, if it is a roll shape, it can bond by another film by roll-to-roll in the next process, and productivity can be improved rather than the case where a sheet-to-sheet or a sheet-to-sheet is employ | adopted.

(5) Combination of extending directions In the light diffusion film obtained by the manufacturing method of the present invention, when viewed from above the film, the extending direction of the plate-like region in the first louver structure and the second louver structure It is preferable to set the acute angle formed by the extending direction of the plate-like region at a value within a range of 10 to 90 °.
The reason for this is that by diffusing the incident light not only in the direction along the longitudinal direction but also in the direction orthogonal to the longitudinal direction, the diffusion area of the incident light is reduced. This is because an elongated film that is effectively spread can be obtained.
That is, when the acute angle is less than 10 °, the incident light diffusion area may be excessively reduced.
Therefore, when viewed from above the film, the acute angle formed by the extending direction of the plate-like region in the first louver structure and the extending direction of the plate-like region in the second louver structure is within the range of 80 to 90 °. More preferably, the value is more preferably in the range of 85 to 90 °, and even more preferably in the range of 89 to 90 °.

(6) Adhesive layer Moreover, the light-diffusion film obtained by the manufacturing method of this invention may be equipped with the adhesive layer for laminating | stacking with respect to a to-be-adhered body in the single side | surface or both surfaces.
The pressure-sensitive adhesive constituting the pressure-sensitive adhesive layer is not particularly limited, and conventionally known pressure-sensitive adhesives such as acrylic, silicone, urethane, and rubber can be used.

  Hereinafter, with reference to an Example, the manufacturing method of the light-diffusion film of this invention is demonstrated in more detail.

[Example 1]
1. Synthesis of low refractive index polymerizable compound (B) component In a container, 1 mol of polypropylene glycol (PPG) having a weight average molecular weight of 9,200 as component (B2) is isophorone diisocyanate as component (B1). After 2 mol of (IPDI) and 2 mol of 2-hydroxyethyl methacrylate (HEMA) as component (B3) were accommodated, polymerization was performed according to a conventional method to obtain a polyether urethane methacrylate having a weight average molecular weight of 9,900.

In addition, the weight average molecular weight of polypropylene glycol and polyether urethane methacrylate is a polystyrene conversion value measured according to the following conditions by gel permeation chromatography (GPC).
GPC measurement device: manufactured by Tosoh Corporation, HLC-8020
-GPC column: manufactured by Tosoh Corporation (hereinafter, described in order of passage)
TSK guard column HXL-H
TSK gel GMHXL (× 2)
TSK gel G2000HXL
・ Measurement solvent: Tetrahydrofuran ・ Measurement temperature: 40 ° C.

2. Preparation of composition for light diffusing film Next, 100 parts by weight of polyether urethane methacrylate having a weight average molecular weight of 9,900 as the obtained component (B) is represented by the following formula (3) as the component (A). 100 parts by weight of o-phenylphenoxyethoxyethyl acrylate having a weight average molecular weight of 268 (manufactured by Shin-Nakamura Chemical Co., Ltd., NK ester A-LEN-10), and 2-hydroxy-2-methylpropiophenone as component (C) After adding 5 parts by weight, the mixture was heated and mixed at 80 ° C. to obtain a composition for a light diffusion film.
The refractive indexes of the components (A) and (B) were measured according to JIS K0062 using an Abbe refractometer (Atago Co., Ltd., Abbe refractometer DR-M2, Na light source, wavelength 589 nm). , 1.58 and 1.46, respectively.

3. First Application Step Next, the obtained composition for light diffusion film was applied to a film-like transparent polyethylene terephthalate film (hereinafter referred to as PET) as a process sheet, and a first film having a thickness of 165 μm. A coating layer was formed.

4). First active energy ray irradiation step Subsequently, an ultraviolet irradiation device (ECS-4011GX, manufactured by Eye Graphics Co., Ltd.) in which a condensing cold mirror is attached to a linear high-pressure mercury lamp as shown in FIG. ) Was prepared.
At this time, when viewed from above the film, the ultraviolet irradiation device is set so that the acute angle θ2 formed by the major axis direction of the linear light source and the virtual line along the moving direction of the first coating layer is 45 °. installed.
Next, a light shielding plate is installed on the heat ray cut filter frame, and the ultraviolet rays applied to the surface of the first coating layer are normal to the surface of the first coating layer when viewed from the long axis direction of the linear light source. When the angle was set to 0 °, the irradiation angle of direct ultraviolet rays from the linear light source (θ6 in FIG. 5B) was set to 16 °.
Further, the height from the surface of the first coating layer to the linear light source was set to 2000 mm, the peak illuminance was set to 1.26 mW / cm ² , and the integrated light amount was set to 23.48 mW / cm ² .
Further, in order to prevent the reflected light from the light shielding plate or the like from becoming stray light inside the irradiator and affecting the photocuring of the first coating layer, as shown in FIG. A plate was installed and set so that only the ultraviolet rays directly emitted from the linear light source were applied to the first coating layer.
More specifically, as shown in FIG. 7, it is arranged so that a long groove-like gap (gap width: 35 cm) formed by two light shielding plates is formed, and the longitudinal direction of the long groove-like gap is The linear light source was installed so as to be parallel to the long axis direction.
Next, the conveyor is irradiated with ultraviolet rays while moving the first coating layer in the right direction in FIG. 4B at a speed of 1.0 m / min, and the longitudinal direction (the moving direction of the first coating layer). ) Having a length of 30 m, a length in the short direction of 1.25 m, and a film thickness of 165 μm, a first coating layer having a long first louver structure was obtained.
Subsequently, in order to achieve reliable curing, on the exposed surface side of the first coating layer, as an active energy ray-transmitting sheet, a release film having a thickness of 38 μm and having UV transmittance (manufactured by Lintec Corporation, SP-PET382050; The center line average roughness 0.01 μm, haze value 1.80%, image sharpness 425, transmittance at wavelength 360 nm 84.3% on the surface on the ultraviolet irradiation side was laminated.
Next, the scattered light irradiation was performed so that the peak illuminance was 13.7 mW / cm ² and the integrated light amount was 213.6 mJ / cm ² .
The above-described peak illuminance and integrated light amount were measured by installing a UV METER (manufactured by Eye Graphics Co., Ltd., eye ultraviolet integrated illuminance meter UVPF-A1) equipped with a light receiver at the position of the first coating layer. .
Moreover, the film thickness of the 1st coating layer in which the obtained elongate 1st louver structure was formed was measured using the constant-pressure thickness measuring device (Takekku PG-02J by Takara Seisakusho Co., Ltd.). did.

5. Second Application Step Next, the active energy ray-transmitting sheet was peeled off from the first application layer on which the long first louver structure was formed.
Next, the same composition for a light diffusion film used for forming the first coating layer is applied to the exposed surface of the first coating layer on which the obtained long first louver structure is formed. Then, a second coating layer having a film thickness of 165 μm was formed.

6). Second active energy ray irradiation step Next, when viewed from above the film, the long axis direction of the linear light source in the first active energy ray irradiation and the long axis direction of the linear light source in the second active energy ray irradiation In the same manner as in the first active energy ray irradiating step, the ultraviolet ray is irradiated, and the first louver structure and the second irradiating structure are formed in the inside, except that the ultraviolet irradiation device is installed so that the acute angle θ1 formed is 90 °. Thus, a long light diffusion film having a film thickness of 330 μm having a louver structure was obtained.
When viewed from above the film, the virtual axis along the long axis direction of the linear light source and the moving direction of the laminate composed of the first coating layer and the second coating layer on which the first louver structure is formed. The acute angle θ3 formed by the line was 45 °.
In addition, after irradiating the second coating layer with ultraviolet rays, as in the case of the first coating layer, the active energy ray transmitting sheet (ultraviolet transparent release film) is laminated and irradiated with scattered light. And reliable curing was achieved.

In addition, as shown in FIG. 12, the obtained light diffusion film has an extension direction of the plate-like region in the first louver structure and an extension of the plate-like region in the second louver structure when viewed from above the film. It was confirmed that the acute angle formed by the direction was 90 °.
Further, when viewed from above the film, it was confirmed that the acute angle formed by the extending direction of the plate-like region in the first louver structure and the longitudinal direction of the film was 45 °.
Furthermore, when viewed from above the film, it was confirmed that the acute angle formed by the extending direction of the plate-like region in the second louver structure and the longitudinal direction of the film was 45 °.
Moreover, the photograph of the cross section which cut | disconnected the obtained light-diffusion film in the surface orthogonal to the elongate direction of a film was cut | disconnected in Fig.13 (a) by the surface parallel to the elongate direction of a film and orthogonal to the film surface. Cross-sectional photographs are shown in FIG.
The light diffusing film was cut using a razor, and a cross-sectional photograph was taken using an optical microscope (reflection observation).

7). Measurement As shown in FIG. 12, light was incident on the film from the direction perpendicular to the film surface from the lower side (side where the first louver structure is located) of the obtained light diffusion film.
Next, a spectrum chart of diffused light in a direction perpendicular to the longitudinal direction of the film and in a direction parallel to the longitudinal direction of the film, using a colorimeter (VC-2 manufactured by Suga Test Instruments Co., Ltd.) Got.
That is, as shown in FIG. 14A, the horizontal axis represents the light diffusion angle (°) in the diffused light diffused by the light diffusion film, and the vertical axis represents the relative intensity (−) of the diffused light. A spectrum chart was obtained.
Here, the spectrum chart A shown in FIG. 14A corresponds to the diffused light in the direction orthogonal to the longitudinal direction of the film, and the spectrum chart B represents the diffused light in the direction parallel to the longitudinal direction of the film. It corresponds to.
Moreover, the photograph of the diffused light at the time of seeing from the Z direction in FIG. 12 was obtained as shown in FIG.14 (b) using the conoscope (made by autotronic-MELCHERS GmbH).
The results shown in FIGS. 14 (a) to 14 (b) were consistent with the light diffusion characteristics expected from a film having an internal structure as shown in FIG.

[Comparative Example 1]
In Comparative Example 1, a light diffusion film was produced in the same manner as in Example 1 except that the second coating step and the second active energy ray irradiation step were not performed.

Further, as shown in FIG. 15, the obtained light diffusing film has an acute angle of 45 ° formed by the extending direction of the plate-like region in the louver structure and the longitudinal direction of the film when viewed from above the film. I confirmed that there was.
Moreover, the photograph of the cross section which cut | disconnected the obtained light-diffusion film in the surface orthogonal to the elongate direction of a film was cut | disconnected in Fig.16 (a) by the surface parallel to the elongate direction of a film, and orthogonal to the film surface. Sectional photographs are shown in FIG.

Moreover, the light diffusion condition in the case where light was incident on the film from the direction perpendicular to the film surface was measured from the lower side of the obtained light diffusion film in the same manner as in Example 1.
FIG. 17A shows a spectrum chart of the obtained diffused light, and FIG. 17B shows a photograph of the diffused light when viewed from the Z direction in FIG.
However, FIG. 17A shows a spectrum chart in the direction along the diffusion direction (major axis direction) of the diffused light shown in FIG.
The results shown in FIGS. 17 (a) to 17 (b) were consistent with the light diffusion characteristics expected from a film having an internal structure as shown in FIG.

[Comparative Example 2]
In Comparative Example 2, the acute angle formed by the longitudinal direction of the linear light source and the virtual line along the moving direction of the first coating layer when viewed from above the film in the first active energy ray irradiation step. Except for setting θ2 to 90 °, the first active energy ray irradiation step is performed on the first coating layer in the same manner as in Example 1, and the first coating layer (the first louver structure is formed inside). Obtained).
The first coating layer on which the first louver structure obtained at this time is formed, as shown in FIG. 18 (a), when viewed from above the film, the extending direction of the plate-like region in the louver structure, It was confirmed that the longitudinal direction and the acute angle formed by the longitudinal direction were 90 °.

Next, as shown in FIG. 18 (b), the long first coating layer on which the obtained first louver structure is formed is cut every 1.1 m in the long direction to obtain the first A plurality of non-long first coating layers having a louver structure were formed.
Next, as shown in FIG. 18 (c), the plurality of non-elongated first coating layers on which the first louver structure is formed are each rotated by 90 ° in the plane, They were joined together so that the distance was 0.5 mm or less.
As a result, as shown in FIG. 18 (c), the first louver having an acute angle of 0 ° formed by the extending direction of the plate-like region in the louver structure and its longitudinal direction when viewed from above the film. A long first coating layer having the structure formed thereon (with the first louver structure formed therein) was obtained.

  Next, the long coating layer shown in FIG. 18 (a) is formed into a film on the long first coating layer on which the obtained first louver structure shown in FIG. 18 (c) is formed. A light diffusing film was obtained by laminating as a long second coating layer having a second louver structure formed through an acrylic transparent adhesive layer having a thickness of 25 μm.

Further, as shown in FIG. 19, the obtained light diffusing film has an extension direction of the plate-like region in the first louver structure and a plate-like region in the second louver structure region when viewed from above the film. It was confirmed that the acute angle formed by the extending direction was 90 °.
Further, when viewed from above the film, it was confirmed that the acute angle formed by the extending direction of the plate-like region in the first louver structure and the longitudinal direction of the film was 0 °.
Furthermore, when viewed from above the film, it was confirmed that the acute angle formed by the extending direction of the plate-like region in the second louver structure and the longitudinal direction of the film was 90 °.
Moreover, the photograph of the cross section which cut | disconnected the obtained light-diffusion film in the surface orthogonal to the elongate direction of a film was cut | disconnected in FIG. 20 (a) by the surface parallel to the elongate direction of a film and orthogonal to the film surface. Sectional photographs are shown in FIG.

Moreover, the light diffusion condition in the case where light was incident on the film from the direction perpendicular to the film surface was measured from the lower side of the obtained light diffusion film in the same manner as in Example 1.
FIG. 21A shows a spectrum chart of diffused light obtained by making light incident on a seamless portion, and FIG. 21B shows a photograph of diffused light when viewed from the Z direction in FIG. Show.
The results shown in FIGS. 21A to 21B were consistent with the light diffusion characteristics expected from the film having the internal structure as shown in FIG.
However, when light is incident on the seam portion, as shown in FIGS. 22A to 22B, it is confirmed that the light diffusibility tends to be uneven due to the seam portion of the film. It was done.

As described above in detail, according to the present invention, in a predetermined manufacturing method including two active energy ray irradiation steps using a linear light source, each linear shape in the two active energy ray irradiation steps. By defining the relationship of the light source arrangement angle within a predetermined range, the incident light is diffused not only in the direction along the longitudinal direction but also in the direction perpendicular to the longitudinal direction. Thus, it has become possible to efficiently produce a long light diffusion film in which the diffusion area is effectively expanded.
Therefore, the method for producing a light diffusing film of the present invention is expected to contribute significantly to the productivity and quality improvement of a large area light diffusing film used for a projection screen, a reflective liquid crystal device and the like.

DESCRIPTION OF SYMBOLS 1a: 1st coating layer, 1a ': 1st coating layer in which the 1st louver structure was formed, 1b: 2nd coating layer, 1c: Lamination | stacking which consists of a 1st coating layer and a 2nd coating layer Body, 2: process sheet, 10: light diffusion film, 12: plate-like region having a relatively high refractive index, 13: louver structure, 13a: first louver structure, 13b: second louver structure, 13 ′: Interface surface of louver structure, 14: plate-like region having a relatively low refractive index, 20: light diffusion film obtained by the production method of the present invention, 50 ′: light diffusion condition, 51 ′: diffusion light diffusion condition, 120: UV irradiation device, 121: heat ray cut filter, 123: light shielding plate, 125: linear light source, 150: active energy ray

Claims (8)

A first louver structure and a second louver structure, in which a plurality of plate-like regions having different refractive indexes are alternately arranged in parallel in any one direction along the film surface, sequentially from below along the film thickness direction. A method for producing a long light diffusion film having
The manufacturing method of the light-diffusion film characterized by including the following process (a)-(e).
(A) Step of preparing a composition for light diffusion film containing two polymerizable compounds having different refractive indexes (b) Applying the composition for light diffusion film to a process sheet to form a first coating layer (C) A step of forming a first louver structure by irradiating the first coating layer with a first active energy ray using a linear light source while moving the first coating layer. (D) Applying the light diffusing film composition to the first coating layer on which the first louver structure is formed, and forming a laminate composed of the first coating layer and the second coating layer. Step (e) Forming a second active energy ray using a linear light source while moving the laminate composed of the first coating layer and the second coating layer with respect to the second coating layer And forming a second louver structure, comprising: When viewed from above, the acute angle θ1 formed by the major axis direction of the linear light source in the first active energy ray irradiation and the major axis direction of the linear light source in the second active energy ray irradiation is 10 The process which makes it the value within the range of -90 degrees   In the step (c), when viewed from above the film, a major axis direction of the linear light source in the first active energy ray irradiation and an imaginary line along the moving direction of the first coating layer are: The acute angle θ2 to be made is a value within the range of 10 to 80 °, and when viewed from above the film in the step (e), the major axis direction of the linear light source in the second active energy ray irradiation, The acute angle θ3 formed by a virtual line along the moving direction of the laminate composed of the first coating layer and the second coating layer is set to a value within a range of 10 to 80 °. The manufacturing method of the light-diffusion film of description. In the step (e), when viewed from above the film, the long axis direction of the linear light source in the first active energy ray irradiation and the long axis direction of the linear light source in the second active energy ray irradiation The line is symmetrical with respect to an imaginary line orthogonal to the moving direction of the laminate composed of the first coating layer and the second coating layer. A method for producing a light diffusion film.   In the step (c) and the step (e), the first active energy ray irradiation and the second active energy ray irradiation are performed through a light shielding plate having a long groove-like active energy ray transmitting portion, and the active energy The method for producing a light diffusing film according to any one of claims 1 to 3, wherein a longitudinal direction of the line transmitting portion is a direction parallel to a major axis direction of the linear light source. In the step (c), the peak illuminance on the surface of the first coating layer in the first active energy ray irradiation is set to a value within a range of 0.1 to 50 mW / cm ² , and the first coating is performed. the method of manufacturing an optical diffusion film as described in any one of claims 1 to 4, characterized in that a value within the range of accumulated light amount of 5~300mJ / cm ² at the surface of the layer. In the step (e), the peak illuminance on the surface of the second coating layer in the second active energy ray irradiation is set to a value within a range of 0.1 to 50 mW / cm ² , and the second coating is performed. the method of manufacturing an optical diffusion film as described in any one of claims 1 to 5, characterized in that a value within the range of accumulated light amount of 5~300mJ / cm ² at the surface of the layer.   In the step (b), the thickness of the first coating layer is set to a value in the range of 80 to 700 μm, and in the step (d), the thickness of the second coating layer is set to 80 to 700 μm. It is set as the value within a range, The manufacturing method of the light-diffusion film as described in any one of Claims 1-6 characterized by the above-mentioned.   The moving speed of the first coating layer in the step (c) and the moving speed of the laminate composed of the first coating layer and the second coating layer in the step (e) are respectively 0.1 to 10 m / It is set as the value within the range of minutes, The manufacturing method of the light-diffusion film as described in any one of Claims 1-8 characterized by the above-mentioned.