Light control film and backlight unit using the same

Abstract

A light control film enabling improvement in front luminance, having appropriate light diffusing property and free from problems of interference pattern, glare etc. is provided.

Description

TECHNICAL FIELD

The present invention relates to a light control film used for backlight units such as those for liquid crystal displays and so forth, and a backlight unit using the same.

BACKGROUND ART

For liquid crystal displays and so forth, backlight units of the edge light type or direct type are conventionally used. Since backlight units of the edge light type themselves can be manufactured with a small thickness, they are used for notebook computers etc., whereas backlight units of the direct type are used for large-sized liquid crystal television etc. in many cases.

Lights emitted from these conventional backlight units contain components projected along directions significantly inclined from the direction the front direction. Lights emitted from backlight units of the edge light type, in particular, contain a lot of components projected along directions significantly inclined from the front direction, and thus it is difficult to obtain high front luminance.

In the conventional backlight units, two or more optical films such as prism sheets and light diffusive films are used in combination in order to improve front luminance so that directions of lights should be directed to the front direction (see, for example, Patent document 1).

Although prism sheets can generally increase the ratio of lights emerging along the front direction (direction perpendicular to film surface) by surface design based on geometric optics. However, they have drawbacks that they are likely to suffer from an interference pattern due to regularly arranged convex portions, and that they cause glare if they are used alone and thus they impair visibility of image. Moreover, they unduly concentrate lights along the front direction, and therefore they cannot provide a wide viewing angle.

On the other hand, if diffusion films are used alone, the front luminance becomes insufficient, although the aforementioned problems are not caused.

In the technique disclosed in Patent document 1, a prism sheet and a light diffusive film are used in combination. However, the front luminance enhanced by the prism sheet is reduced by the use of the light diffusive film. Moreover, the films place in layers may generate Newton rings between the members, or scratches and so forth may be generated due to the contact of the members as the case may be.

[Patent document 1] Japanese Patent Unexamined Publication (KOKAI) No. 9-127314 (claim 1, paragraph 0034)

DISCLOSURE OF THE INVENTION

Problems to be Solved by the Invention

Therefore, an object of the present invention is to provide a light control film that can surely improve front luminance when it is used alone or in combination with a prism sheet, has an appropriate light diffusing property, and does not suffer from the problems of interference pattern and glare, and a backlight unit using the same.

Means for Achieving the Object

In order to achieve the aforementioned object, the inventor of the present invention conducted various researches on various factors defining surface profile of light control film such as shapes, slopes with respect to film surface (base plane), heights and pitches of convexoconcaves (protrusion and recess) and so forth, and as a result, he found that the front luminance could be improved by appropriately controlling the slopes of the curved surface constituting the rough surface with respect to the base plane and thereby efficiently directing lights entered into the film to the front direction (projection direction).

More specifically, they found that superior front luminance could be achieved if average (θ_nv (degree)) of slopes of the curved surface of the rough surface with respect to the standard surface (the surface opposite to the surface on which convexoconcaves are formed), which slopes are henceforth referred to as “slopes of a curved surface”, obtained for an area of a particular size or larger (1 mm² or larger) was within a predetermined range, as defined in the first to fourth embodiments of the present invention.

It was further found that if the average of slopes of the curved surface (θ_nv (degree)) was used as an index of slope of the rough surface, and a ratio of an area (A1) of an approximately square region on the rough surface (area of orthogonal projection of the rough surface) and a surface area (A2) of a curved surface constituting the rough surface (A_r=A2/A1) was used as an index of height of convexoconcaves, relations of these indexes with change of front luminance could be described by particular relational equations, and when the values of the indexes were within specific ranges, superior front luminance could be achieved, and thus accomplished the first to fourth embodiments of the present invention.

That is, the light control film according to the first embodiment of the present invention is a light control film having a rough surface, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees at substantially any position on the light control film (a condition providing θ_nv not less than 27 degrees and not more than 70 degrees is called “condition 1” hereafter).

The light control film according to the second embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees at any position on the light control film (a condition providing θ_nv not less than (59-20 n) degrees and not more than 70 degrees is called “condition 2” hereafter).

Further, the light control film according to the third embodiment of the present invention is a light control film having a rough surface, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film and a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) satisfy the following equation (1) or (2) at substantially any position on the light control film (a condition providing θ_nv and A_r that satisfy “θ_nv÷A_r≧22” or “30≦θ_nv×A_r≦140” is called “condition 3” hereafter). θ_nv÷A_r≧22  (1) 30≦θ_nv×A_r≦140  (2)

The light control film according to the fourth embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film and a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) satisfy the following equation (3) or (4) at substantially any position on the light control film (a condition providing θ_nv and A_r that satisfy “θ_nv÷A_r×n²≧35” or “60≦θ_nv×A_r×n²≦350” is called “condition 4” hereafter). θ_nv÷A_r×n²≧35  (3) 60≦θ_nv×A_r×n²≦350  (4)

Aiming at achieving the aforementioned object, it was also found that if average (θ_nv (degree)) of slopes of a curved surface of the rough surface with respect to the standard surface (the surface opposite to the surface on which convexoconcaves are formed), which slopes are henceforth referred to as “slopes of a curved surface”, obtained for an area of a particular size or larger (1 mm² or larger) was within a predetermined range, and a numerical value A_sk [equation (5)] representing an index of asymmetry of a probability density function for the height direction obtained from all the surface height data for the aforementioned area, or a numerical value A_ku [equation (6)] representing as an index of sharpness of the probability density function for the height direction obtained from all the surface height data was within a predetermined range, as defined in the fifth to eighth embodiments of the present invention, superior front luminance could be achieved. $\begin{array}{cc}\left[\mathrm{\#1}\right]& \\ A_{\mathrm{sk}}=\frac{\sum _{i=1}^m{z}_i^3}{m}/{\sqrt{\frac{\sum _{i=1}^m{z}_i^2}{m}}}^3& \left(5\right)\end{array}$ [In the equation (5), z_i represents a value obtained by subtracting a height of average plane of the rough surface from a measured surface height, and m represents a number of measurement points.] $\begin{array}{cc}\left[\mathrm{\#2}\right]& \\ A_{\mathrm{ku}}=\frac{\sum _{i=1}^m{z}_i^4}{m}/{\sqrt{\frac{\sum _{i=1}^m{z}_i^2}{m}}}^4& \left(6\right)\end{array}$ [In the equation (6), z_i represents a value obtained by subtracting a height of average plane of the rough surface from a measured surface height, and m represents a number of measurement points.]

That is, the light control film according to the fifth embodiment of the present invention is a light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees, and an absolute value of a numerical value (A_sk) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film (the condition providing θ_nv not less than 27 degrees and not more than 70 degrees and an absolute value of A_sk not more than 1.2 is called “condition 5” hereafter).

The light control film according to the sixth embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees, and an absolute value of a numerical value (A_sk) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film (the condition providing θ_nv not less than (59-20 n) degrees and not more than 70 degrees and an absolute value of A_sk not more than 1.2 is called “condition 6” hereafter).

Further, the light control film according to the seventh embodiment of the present invention is a light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees, and a numerical value (A_ku) calculated by using all the height data of the rough surface in accordance with the aforementioned equation (6) is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film (the condition providing θ_nv not less than 27 degrees and not more than 70 degrees and A_ku not less than 1.5 and not more than 5.0 is called “condition 7” hereafter).

Furthermore, the light control film according to the eighth embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θ_nv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees, and a numerical value (A_ku) calculated by using all the height data of the rough surface in accordance with the aforementioned equation (6) is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film (the condition providing θ_nv not less than (59-20 n) degrees and not more than 70 degrees and a value of A_ku not less than 1.5 and not more than 5.0 is called “condition 8” hereafter).

Aiming at achieving the aforementioned object, it was also found that if a ratio (A_r=A2/A1, referred to as a surface area ratio hereafter) of a surface area (A2) of a curved surface constituting the rough surface and an area (A1) of an approximately square region on the rough surface (area of orthogonal projection of the rough surface) was within a predetermined range, and a numerical value A_sk [equation (5)] representing an index of asymmetry of a probability density function for the height direction obtained from all the surface height data for the area (A1), or a numerical value A_ku [equation (6)] representing an index of sharpness of the probability density function for the height direction obtained from all the surface height data was within a predetermined range, as defined in the ninth to twelfth embodiments of the present invention, superior front luminance could be achieved. $\begin{array}{cc}\left[\mathrm{\#3}\right]& \\ A_{\mathrm{sk}}=\frac{\sum _{i=1}^m{z}_i^3}{m}/{\sqrt{\frac{\sum _{i=1}^m{z}_i^2}{m}}}^3& \left(5\right)\end{array}$ [In the equation (5), z_i represents a value obtained by subtracting a height of average plane of the rough surface from a measured surface height, and m represents a number of measurement points.] $\begin{array}{cc}\left[\mathrm{\#4}\right]& \\ A_{\mathrm{ku}}=\frac{\sum _{i=1}^m{z}_i^4}{m}/{\sqrt{\frac{\sum _{i=1}^m{z}_i^2}{m}}}^4& \left(6\right)\end{array}$ [In the equation (6), z_i represents a value obtained by subtracting a height of average plane of the rough surface from a measured surface height, and m represents a number of measurement points.]

Thus, the light control film according to the ninth embodiment of the present invention is a light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) is not less than 1.2 and not more than 2.5, and absolute value of a numerical value (A_sk) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film (the condition providing A_r not less than 1.2 and not more than 2.5 and an absolute value of A_sk not more than 1.2 is called “condition 9” hereafter).

The light control film according to the tenth embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) is not less than (2-0.5 n) and not more than 2.5, and absolute value of a numerical value (A_sk) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film (the condition providing A_r not less than (2-0.5 n) and not more than 2.5 and an absolute value of A_sk not more than 1.2 is called “condition 10” hereafter).

Further, the light control film according to the eleventh embodiment of the present invention is a light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) is not less than 1.2 and not more than 2.5, and a numerical value A_ku calculated in accordance with the equation (6) mentioned above by using all the surface height data is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film (the condition providing A_r not less than 1.2 and not more than 2.5 and A_ku not less than 1.5 and not more than 5.0 is called “condition 11” hereafter).

The light control film according to the twelfth embodiment of the present invention is a light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm² or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (A_r=A2/A1) is not less than (2-0.5 n) and not more than 2.5, and a numerical value A_ku calculated in accordance with the equation (6) mentioned above by using all the surface height data is not less than 1.5 and not more than 5.0 at substantially any position on the light control film (the condition providing A_r not less than (2-0.5 n) and not more than 2.5 and A_ku not less than 1.5 and not more than 5.0 is called “condition 12” hereafter).

In the first to twelfth embodiments of the present invention, the area of the approximately square region on the rough surface means an area of the orthogonal projection of the rough surface.

In the first to twelfth embodiments of the present invention, the base plane of the film means a plane of the film regarded substantially planar, and when the face of the light control film of the present invention opposite to the face on which convexoconcaves are formed is smooth, the plane of this face can be regarded as the base plane. When the opposite face is not smooth but a rough surface, a plane including the central lines of two different directions thereof can be regarded as the base plane.

In the first to eighth embodiments of the present invention, the average of slopes of a curved surface (θ_nv (degree)) is used. In general, if a curved surface of a rough surface can be represented with a common function z=ƒ(x, y), an average of slopes of the curved surface (C_fc) constituting the rough surface with respect to the aforementioned base plane can be represented by the following equation (7) wherein D is a region for which the average is calculated. $\begin{array}{cc}\left[\mathrm{\#5}\right]& \\ C_{\mathrm{fc}}=\int {\int }_D^{}\left(\frac{\partial z}{\partial x}+\frac{\partial z}{\partial y}\right)dxdy/\int {\int }_D^{}dxdy& \left(7\right)\end{array}$

Further, the average of slopes of the curved surface wherein the slopes are indicated with angle (θ_fc (degree)) can be represented by the following equation (8). θ_fc=tan⁻¹C_fc  (8)

However, although it is possible to use such a function for product designing, it is almost impossible to describe a rough surface with a general function for an actual product, and average of slopes of a curved surface (θ_fc (degree)) can hardly be obtained, either. Therefore, in the first to eighth embodiments of the present invention, a value calculated as follows is defined as an average of slopes of a curved surface (θ_nv (degree))

First, surface height data of a rough surface are measured by using a surface profiler at positions defined by dividing an approximately square region of an area larger than a particular area (1 mm² or larger) at an arbitrary position on the rough surface in a lattice pattern with predetermined intervals (Δd_L, Δd_H) for the longitudinal and transverse directions. When the surface height data for the approximately square region on the base plane are measured at points in numbers of r for the longitudinal direction and s for the transverse direction, the height data correspond to those of points in a number of (r×s), and the respective data points are represented as {(H₁₁, H₁₂, H₁₃, . . . H_1s), (H₂₁, H₂₂, H₂₃, . . . H_2s), . . . (H_r1, H_r2, H_r3, . . . H_rs)}. The numbers of the measurement points for the longitudinal and transverse directions, r and s, may be the same or different, so long as the region is approximately square. Further, the measurement intervals for the longitudinal and transverse directions, Δd_L and Δd_H, may also be the same or different.

Then, one diagonal line is drawn in each unit lattice having side lengths of Δd_L and Δd_H for the longitudinal and transverse directions on the base plane to divide the lattice into two triangles. From height data at the positions of three apexes of each of these two triangles on the base plane, “one triangle plane (henceforth referred to as “minute triangle plane”)” is uniquely defined for each triangle on the base plane, and slope of this minute triangle plane with respect to the base plane can be obtained by obtaining the angle between the normal of the minute triangle plane and the normal of the base plane through calculation. If Δd_L and Δd_H are sufficiently small, it can be regarded that the curved surface constituting the rough surface is approximated with planes of the minute triangles. Therefore, the average of slopes of the curved surface (θ_nv (degree)) can be obtained by applying this method to all the unit lattices in the approximate square for which the height data are measured to approximate the curved surface constituting the rough surface with planes of minute triangles, obtaining slopes of the minute triangle planes and averaging the slopes.

The lengths of the measurement intervals (Δd_L and Δd_H) mentioned above are such lengths that the profile of the rough surface included in the measurement region can be sufficiently correctly reflected, and both are specifically intervals of about 1.0 μm or shorter.

On the other hand, in the third, fourth and ninth to twelfth embodiments of the present invention, the surface area of a curved surface constituting the rough surface (A2) is used. In general, if a curved surface of a rough surface can be represented with a common function z=ƒ(x, y), the surface area of the curved surface constituting the rough surface (A2) can be represented by the following equation (9) wherein D is a region for which the average is calculated. $\begin{array}{cc}\left[\mathrm{\#7}\right]& \\ A2=\int {\int }_D^{}\sqrt{1+{\left(\frac{\partial z}{\partial x}\right)}^2+{\left(\frac{\partial z}{\partial y}\right)}^2}dxdy& \left(9\right)\end{array}$

However, although it is possible to use such a function for product designing, it is almost impossible to describe a rough surface with a general function for an actual product, and therefore the surface area (A2) can hardly be obtained, either. Therefore, in the third, fourth and ninth to twelfth embodiments of the present invention, a value calculated as follows is defined as the surface area of a curved surface (A2).

First, surface height data of the rough surface are measured by using a surface profiler at positions defined by dividing an approximately square region of an area larger than a particular area (1 mm² or larger) at an arbitrary position on the rough surface in a lattice pattern with predetermined intervals (Δd_L, Δd_H) for the longitudinal and transverse directions. When the surface height data for the approximately square region on the base plane are measured at points in numbers of r for the longitudinal direction and s for the transverse direction, the total data correspond to those of points in a number of (r×s), and the respective data points are represented as {(H₁₁, H₁₂, H₁₃, . . . H_1s), (H₂₁, H₂₂, H₂₃, . . . H_2s), . . . (H_r1, H_r2, H_r3, . . . H_rs)}. The numbers of the measurement points for the longitudinal and transverse directions, r and s, may be the same or different, so long as the region is approximately square. Further, the measurement intervals for the longitudinal and transverse directions, Δd_L and Δd_H, may also be the same or different.

Then, one diagonal line is drawn in each unit lattice having lengths of Δd_L and Δd_H for the longitudinal and transverse directions on the base plane to divide the lattice into two triangles. From height data at the positions of three apexes of each of these two triangles on the base plane, “one triangle plane (henceforth referred to as “minute triangle plane”)” is uniquely defined for each triangle on the base plane, and area of this minute triangle plane can be obtained by calculation. If Δd_L and Δd_H are sufficiently small, it can be regarded that the curved surface constituting the rough surface is approximated with planes of minute triangles. Therefore, the curved surface area (A2) can be obtained by applying this method to all the unit lattices in the approximate square for which the height data are measured to approximate the curved surface constituting the rough surface with planes of minute triangles, obtaining areas of the minute triangle planes and summing the areas.

The lengths of the measurement intervals (Δd_L and Δd_H) mentioned above are such lengths that the profile of the rough surface included in the measurement region can be sufficiently correctly reflected, and both are specifically intervals of about 1.0 μm or shorter.

Further, the light control film according to the thirteenth embodiment of the present invention is the light control film according to any one of the first to twelfth embodiments mentioned above, wherein absolute value of average (φ_ave) of angles (φ, −180 degrees<φ≦180 degrees) between orthogonal projections of normals of the curved surface of the rough surface projected on the base plane and one side of the approximately square region is not more than 5 degrees irrespective of the direction along which the approximately square region is defined in the rough surface (the condition providing an absolute value of the average (φ_ave) not more than 5 is referred to as “conditions 13” hereafter). If the condition 13 for φ_ave is satisfied for the approximately square region defined along an arbitrary direction within the rough surface, glare of the light control film can further be prevented. In order to obtain such a light control film satisfying the condition 13, multiple convex portions constituting the rough surface preferably substantially independent from one another, and each convex portion preferably consists of such a revolution body as shown in FIG. 2-2 as described later.

A backlight unit according to the fourteenth embodiment of the present invention is a backlight unit comprising a light guide plate equipped with a light source end portion thereof and having a light emergent surface approximately perpendicular to the end portion and a light control film provided on the light emergent surface of the light guide plate, wherein the aforementioned light control film is used as the light control film. A backlight unit according to the fifteenth embodiment of the present invention is the aforementioned backlight unit, wherein a prism sheet is used between the light control film and the light guide plate.

A backlight unit according to the sixteenth embodiment of the present invention is a backlight unit comprising a light source, a light diffusive plate provided on one side of the light source and a light control film provided on the side of the light diffusive plate opposite to the light source side, wherein the aforementioned light control film is used as the light control film.

EFFECT OF THE INVENTION

The light control film according to any one of the first to thirteenth embodiments of the present invention can increase components of lights of the front direction, in particular, those in the range of emergent angle of 0 to 30 degrees, for lights entered from the surface opposite to the rough surface and emerging from the rough surface, and thus it can attain markedly higher front luminance compared with usual diffusing films. In addition, it also has appropriate light diffusing property and does not generate glare and interference pattern.

Further, the backlight unit according to the fourteenth or fifteenth embodiment of the present invention is a backlight unit providing high front luminance, having appropriate light diffusing property, and not generating glare and interference pattern, because it uses the particular light control film. Moreover, it can prevent generation of scratches on a prism sheet due to contact with other members and so forth.

BEST MODE FOR CARRYING OUT THE INVENTION

Hereafter, the light control film and backlight unit of the present invention will be explained in detail with reference to the drawings. The sizes (thickness, width, height etc.) of the elements illustrated in the drawings used for explanation of the present invention are enlarged or reduced as required for explanation and do not reflect actual sizes of the elements of actual light control film and backlight unit.

FIGS. 1(a) to (c) schematically show examples of the light control film of the present invention. As shown in the drawings, the light control film of the present invention has fine convexoconcaves formed on one face of a substantially planar film and has a characteristic profile of the convexoconcaves. The convexoconcaves may be formed on a layer provided on one face of a film used as a substrate as shown in (a) and (b), or the light control film may be constituted with a single layer on which convexoconcaves are formed as shown in (c).

When lights enter into the light control film of the present invention from the surface opposite to the surface on which convexoconcaves are formed and emerge from the rough surface, the light control film of the present invention controls direction of the lights so that components of lights emerging with an angle with respect to the front direction within a predetermined range should increase to enhance front luminance, and light diffusing property which can prevent glares should be provided. Although the surface opposite to the surface on which convexoconcaves are formed is typically a smooth surface, it is not limited to a smooth surface. For example, matting may be performed or a predetermined dot pattern etc. may be formed on the surface.

Hereafter, the conditions concerning the profile of the convexoconcaves for controlling direction of lights described above will be explained.

In the present invention, conditions for obtaining optimum emergent lights were first investigated for a single convex portion (FIG. 2-2) consisting of a revolution body formed by rotating such an arbitrary curve as shown in FIG. 2-1 on a xy-plane as a base plane around a z-axis perpendicular to the xy-plane by simulating relationship between incident lights and emergent lights in a three-dimensional space with changing the convex shape, height thereof, angle of incident light and so forth. And distribution of lights emerging from the convex side (emergent angle characteristics) was obtained by calculation for the case where lights having the same distribution as that of lights emerging from a light guide plate in an actual backlight unit enter from the bottom face side of the convex portion. The calculation was performed by assuming that the refractive index of the inside of the convex portion was 1.5, which is the refractive index of a common acrylic resin.

FIG. 3 shows a graph representing distribution of emergent lights, which is a result of simulation performed for the convex portion having the shape shown in FIG. 2-2. In the graph, the solid line represents distribution of emergent lights, and the dotted line represents distribution of incident lights. In order to provide favorable front luminance and light scattering property of a certain degree, it is desirable that components of lights emerging with an angle within the range of the front direction (0 degree)±30 degrees should be abundant.

Then, in order to find conditions for obtaining emergent light characteristics satisfying such conditions for a rough surface on which multiple convex portions are formed, change of emergent light distribution was simulated while the shape of the convex portions and height thereof was variously changed for a system having a multiple number of the convex portions mentioned above. Specifically, by using, for the convex portion, a constant bottom area, 5 to 6 kind of heights, and about 100 kinds of curve shapes for each height, 500 to 600 kinds in total of shapes of the convex portion were defined, and distribution of emergent lights was simulated for 500 to 600 kinds of samples each having multiple convex portions of a single shape on a plane. The results are shown in the graph of FIG. 4. In the graph, the horizontal axis represents average of slopes of the curved surface (θ_nv), and the vertical axis represents energy of emergent lights. In the graph, among the points represented by Δ, □ and ◯, those of the first group 601 represented by Δ indicate energies of emergent lights within the range of 6 degrees about the z axis (henceforth referred to as “emergent lights₆”) for the samples, those of the second group 602 represented by □ indicate energies of emergent lights within the range of 18 degrees about the z axis (henceforth referred to as “emergent lights₁₈”) for the samples, and those of the third group 603 represented by ◯ indicate energies of emergent lights within the range of 30 degrees about the z axis (henceforth referred to as “emergent lights₃₀”) for the samples.

From the simulation results shown in FIG. 4, it was found that if the average of slopes of the curved surface (θ_nv) was not less than 27 degrees and not more than 70 degrees, preferably not less than 27 degrees and not more than 65 degrees, more preferably not less than 27 degrees and not more than 60 degrees, the ratio of the emergent light₃₀ increased.

Moreover, in the simulation results shown in FIG. 4, there was observed a tendency that the ratio of the emergent light₃₀ increased as the average of slopes of the curved surface (θ_nv) became larger, but when it became further larger exceeding a certain level, the ratio conversely decreased. Therefore, a comprehensive index of convexoconcave profile providing correlation with the emergent light₃₀ was investigated. As a result, it was found that if a quotient or product of the average of slopes of the curved surface (θ_nv) and a ratio of a surface area of the curved surface constituting the rough surface (A2) to an area of an approximately square region on the rough surface (A1, area of the orthogonal projection of the rough surface) (A_r=A2/A1, henceforth referred to as “surface area ratio”) was used, the relation with the emergent light₃₀ can be best described. A2 can be obtained by totaling the areas of planes in a minute triangle shape obtained from height data.

FIGS. 5 and 6 show graphs representing the simulation data of FIG. 4 by using the indexes of θ_nv and A_r. FIG. 5 represents change of the emergent light energy with change of a value obtained by dividing the average of slopes of the curved surface (θ_nv) with the surface area ratio (A_r) plotted in the horizontal axis, and FIG. 6 represents change of the emergent light energy with change of a value obtained by multiplying the average of slopes of the curved surface (θ_nv) with the surface area ratio (A_r) plotted in the horizontal axis.

From the results shown in FIGS. 5 and 6, it was found that when the value obtained by dividing the average of slopes of the curved surface (θ_nv) with the surface area ratio (A_r) (quotient) was not less than 22, or when the value obtained by multiplying the average of slopes of the curved surface (θ_nv) with the surface area ratio (A_r) (product) was not less than 30 and not more than 140, the energy of emergent lights having an emergent angle of 30 degrees or less sharply increased. That is, it can be seen that when either one of the following conditions (equation (1) or equation (2)) is satisfied, a light control film exhibiting high front luminance and moderate light diffusion property is constituted. θ_nv÷A_r≧22  (1) 30≦θ_nv×A_r≦140  (2)

The value obtained by dividing the average of slopes of the curved surface (θ_nv) with the surface area ratio (A_r) in the formula (1) is more preferably not less than 25. As for the lower limit of the product of the average of slopes of the curved surface (θ_nv) and the surface area ratio (A_r) in the formula (2) is more preferably not less than 35, and as for the upper limit, the product is more preferably not more than 130.

Such conditions must be satisfied at substantially any position. The expression “substantially any position” is used to mean that it is sufficient that the conditions should be satisfied at almost all observation positions when observation is performed at multiple measurement positions for a certain specific light control film, and it include a case that the conditions are not satisfied at one or two positions.

In the aforementioned simulation for finding the conditions which the rough surface of the present invention must satisfy, the convex portions were assumed to consist of a material having a refractive index of 1.5. However, materials generally used for optical films can be used for the patterned layer of the light control film of the present invention, and the refractive index thereof is not limited to 1.5. In order to generalize the conditions in consideration of the refractive index n, the aforementioned simulation was repeated with changing the refractive index within a predetermined range. As a result, it was found that when the average of slopes of the curved surface (θ_nv) is not less than (59-20 n) degrees and not more than 70 degrees, the aforementioned effect could be obtained.

If the aforementioned formulas (1) and (2) are similarly generalized in consideration of the refractive index n, they can be represented as the following formulas (3) and (4). θ_nv÷A_r×n²≧35  (3) 60≦θ_nv×A_r×n²≦350  (4)

The value of the left side of the formula (3) is more preferably not less than 40. As for the lower limit of the value of the center portion of the formula (4), it is not less than more preferably 70, and as for the upper limit, the value is more preferably not more than 340. By designing the convexo-concave profile in consideration of the refractive index of the material constituting the convexoconcaves as described above, the luminance for the front direction can be more improved.

Another comprehensive index of the convexo-concave profile that could provide correlation with the emergent light₃₀ was further investigated on the basis of the results of the aforementioned simulation, and as a result, it was found that if a numerical value A_sk representing an index of asymmetry of a probability density function for the height direction obtained from all the surface height data used for obtaining the average of slopes of the curved surface, or a numerical value A_ku representing an index of sharpness of the probability density function for the height direction obtained from all the surface height data is used, the correlation with the emergent light₃₀ could be described better.

FIGS. 7 and 8 show graphs representing the simulation data of FIG. 4 by using the index of θ_nv, and the both represent change of the emergent light energy with change of the average of slopes of the curved surface (θ_nv) plotted in the horizontal axis. In FIG. 7, the points of 704 represent the data of the samples showing a value of 1.2 or less as an absolute value of A_sk represented by the aforementioned formula (5). In FIG. 8, the points of 804 represent the data of the samples showing a value of not less than 1.5 and not more than 5.0 as A_ku represented by the aforementioned formula (6).

From the results shown in FIGS. 7 and 8, it was found that the energy of emergent lights having an projected angle of 30 degrees or less tended to sharply increase when the average of slopes of the curved surface (θ_nv) was not less than 27 degrees and not more than 70 degrees, whereas the rate of the emergent light₃₀ did not become high in some cases even if the average of slopes of the curved surface (θ_nv) was within the aforementioned range (the points of 703 in FIG. 7, and the points of 803 in FIG. 8). However, it was found that if only the results where the absolute value of A_sk represented by the aforementioned formula (5) was not more than 1.2 (points of 704 in FIG. 7) were observed, the rate of the emergent light₃₀ was always high. Moreover, it was found that if only the results where A_ku represented by the aforementioned formula (6) was not less than 1.5 and not more than 5.0 (points of 804 in FIG. 6) were observed, the rate of the emergent light₃₀ was always high.

When the average of slopes of the curved surface (θ_nv) is not less than 27 degrees and not more than 70 degrees, preferably not less than 27 degrees and not more than 65 degrees, more preferably not less than 27 degrees and not more than 60 degrees, and the absolute value of A_sk represented by the formula (5) is not more than 1.2, preferably not more than 1.1, or A_ku represented by the formula (6) is not less than 1.5 and not more than 5.0, preferably not less than 1.5 and not more than 4.5, particularly superior effect can be obtained.

Such conditions must be satisfied at substantially any position. The expression “substantially any position” is used to mean that it is sufficient that the conditions should be satisfied at almost all observation positions when observation is performed at multiple measurement positions for a certain specific light control film, and it include a case that the conditions are not satisfied at one or two positions.

In the aforementioned simulation for finding the conditions which the rough surface of the present invention must satisfy, the convex portions were assumed to consist of a material having a refractive index of 1.5. However, materials generally used for optical films can be used for the patterned layer of the light control film of the present invention, and the refractive index thereof is not limited to 1.5. If the condition is generalized in consideration of the refractive index n, when the average of slopes of the curved surface (θ_nv) is not less than (59-20 n) degrees and not more than 70 degrees, the aforementioned effect can be obtained.

By designing the convexo-concave profile in consideration of the refractive index of the material constituting the patterned layer as described above, the luminance for the front direction can be further improved.

FIGS. 9 and 10 show graphs representing the simulation data of FIG. 4 by using the surface area ratio (A_r), and both the graphs represent change of the emergent light energy with change of the surface area ratio (A_r) plotted in the horizontal axis. In FIG. 9, the points of 904 represent the data of the samples showing a value not more than 1.2 as an absolute value of A_sk represented by the aforementioned formula (5). In FIG. 10, the points of 1004 represent the data of the samples showing a value not less than 1.5 and not more than 5.0 as A_ku represented by the aforementioned formula (6).

From the results shown in FIGS. 9 and 10, it was found that the energy of emergent lights of an emergent angle of 30 degrees or less tended to sharply increase when the surface area ratio (A_r) is not less than 1.2 and not more than 2.5, whereas the rate of the emergent light₃₀ did not become high in some cases even if the surface area ratio (A_r) was within the aforementioned range (the points of 903 in FIG. 9, and the points of 1003 in FIG. 10). However, it was found that if only the results where the absolute value of A_sk represented by the aforementioned formula (5) was not more than 1.2 (points of 904 in FIG. 9) were observed, the rate of the emergent light₃₀ was always high. Moreover, it was found that if only the results where A_ku represented by the aforementioned formula (6) was not less than 1.5 and not more than 5.0 (points of 1004 in FIG. 10), the rate of the emergent light₃₀ was always high.

When this surface area ratio (A_r) is not less than 1.2 and not more than 2.5, preferably not less than 1.3 and not more than 2.4, more preferably not less than 1.4 and not more than 2.3, and the absolute value of A_sk represented by the formula (5) is not more than 1.2, preferably not more than 1.1, or A_ku represented by the formula (6) is not less than 1.5 and not more than 5.0, preferably not less than 1.5 and not more than 4.5, particularly superior effect can be obtained.

Such conditions must be satisfied at substantially any position. The expression “substantially any position” is used to mean that it is sufficient that the conditions should be satisfied at almost all observation positions when observation is performed at multiple measurement positions for a certain specific light control film, and it include a case that the conditions are not satisfied at one or two positions.

In the aforementioned simulation for finding the conditions which the rough surface of the present invention must satisfy, the convex portions were assumed to consist of a material having a refractive index of 1.5. However, materials generally used for optical films can be used for the patterned layer of the light control film of the present invention, and the refractive index thereof is not limited to 1.5. If the conditions are generalized in consideration of the refractive index n, the aforementioned effect can be obtained when the surface area ratio (A_r) is not less than (2-0.5 n) and not more than 2.5.

By designing the profile of the rough surface in consideration of the refractive index of the material constituting the patterned layer as described above, the luminance for the front direction can be more improved.

By designing the rough surface so that it should satisfy the aforementioned conditions, the light control film of the present invention can exhibit high front luminance, and have a light diffusing property of a certain degree. The light control film of the present invention having such characteristics is disposed, for example, directly on a light guide plate of a backlight unit of the edge light type, or via a light diffusing material on a light source of a backlight unit of the direct type, and used as a film for controlling the direction of emergent lights of the backlight unit.

So long as “the average of slopes of the curved surface (θ_nv) of the rough surface” or “the surface area ratio (A_r)” of the light control film of the present invention satisfies any one of the aforementioned conditions 1 to 12, the shape and arrangement of the convex portions are not particularly limited. That is, the convex portions and concave portions may be randomly or regularly arranged. However, if a random arrangement is used, generation of an interference pattern can be easily prevented even if another member having a regular pattern is used in combination. Individual convex portions and concave portions may have the same shape or different shapes, and they may be arrange so that they should overlap with one another, or a part or all of the convex portions and concave portions should overlap with one another. The height of the convex portions and depth of the concave portions are both about 3 to 100 μm, and arrangement density of the convex portions or the concave portions is preferably about 10 to 200,000 portions/mm². A typical rough surface of the light control film satisfying the aforementioned conditions is shown in FIG. 11.

Hereafter, specific configurations for producing the light control film having the aforementioned rough surface will be explained.

As the material constituting the substrate 11 and the patterned layer 12 of the light control film 10 of the present invention, materials generally used for optical films can be used. Specifically, the material for the substrate 11 is not especially limited so long as a material exhibiting favorable light transmission property is chosen, and plastic films such as those of polyethylene terephthalate, polybutylene terephthalate, polyethylene naphthalate, polycarbonate, polyethylene, polypropylene, polystyrene, triacetyl cellulose, polyacrylate, polyvinyl chloride, and so forth can be used.

The material for constituting the patterned layer 12 is not also especially limited so long as a material exhibiting favorable light transmission property is chosen, and glass, polymer resins, and so forth can be used. Examples of the glass include oxide glass such as silicate glass, phosphate glass, and borate glass. Examples of the polymer resins include thermoplastic resins, thermosetting resins, and ionizing radiation curable resins such as polyester resins, acrylic resins, acrylic urethane resins, polyester acrylate resins, polyurethane acrylate resins, epoxy acrylate resins, urethane resins, epoxy resins, polycarbonate resins, cellulose resins, acetal resins, vinyl resins, polyethylene resins, polystyrene resins, polypropylene resins, polyamide resins, polyimide resins, melamine resins, phenol resins, silicone resins, and fluorocarbon resins, and so forth.

Among these materials, polymer resins are preferred in view of workability and handling property, and those having a refractive index (JIS K7142:1996) of about 1.3 to 1.7 are especially preferably used. Even if a material having a refractive index n out of the aforementioned range is used as a material constituting the patterned layer, favorable luminance can be realized so long as the condition 1, 3, 5, 7, 9 or 11 is satisfied. However, by using a material having a refractive index within such a range, high luminance can be obtained. In particular, by designing the rough surface so that it should satisfy the condition 2, 4, 6, 8, 10 or 12 depending on the refractive index of the material, front luminance can be further improved.

Although the patterned layer 12 may comprise light diffusing agents such as beads of organic materials and inorganic pigments, like general light diffusive sheets, they are not indispensable. The light control film of the present invention can exert light diffusing effect to a certain degree by the rough surface itself, even if it does not comprise light diffusing agents. If light diffusing agents are not used, other members are not damaged by light diffusing agents, or light diffusing agents do not separate and fall to generate dusts.

As the method for forming the patterned layer 12, 1) a method of using an embossing roller, 2) a method of using an etching treatment, and 3) a method of using molding with a mold can be employed. However, a production method of using a mold is preferred, because it enables production of light control films having a predetermined patterned layer with good reproducibility. Specifically, the production can be attained by preparing a mold having a profile complementary to that of the rough surface, casting a material constituting the patterned layer such as polymer resins into the mold, curing the material, and taking out the cured material from the mold. When a substrate is used, the production can be attained by casting a polymer resin or the like into the mold, superimposing a transparent substrate thereon, curing the polymer resin or the like, and taking out the cured material together with the transparent substrate from the mold.

Although the method of forming a profile complementary to the rough surface in the mold is not particularly limited, the following method can be employed. For example, convex portions having a specific shape are formed on a plate so that the arrangement density of the portions should be several thousands portions/mm² by a laser microprocessing technique, and this plate is used as a male mold to prepare a mold for molding (female mold). The convex portions having a specific shape means such convex portions that when height data thereof are measured with equal intervals of a length that allows correct reflection of the shape of one whole convex portion (1.0 μm or shorter), the convex portions should satisfy the condition 1 or 3. Alternatively, resin plates having a convex-concave layer are prepared by curing a resin containing particles of a predetermined particles size dispersed therein, the surfaces of the patterned layers are measured by using a surface profiler to choose a resin plate satisfying the aforementioned conditions, and a mold for molding (female mold) is prepared by using the chosen plate as a male mold.

Although the surface of the light control film opposite to the rough surface may be smooth, it may be subjected to a fine matting treatment in order to prevent generation of Newton rings when the film is brought into contact with a light guide plate or resin plate, or an antireflection treatment in order to improve light transmittance.

Moreover, in order to obtain favorable front luminance, as an optical characteristic of the light control film, the film desirably has a haze of 60% or more, preferably 70% or more. The haze referred to herein is a value of the haze defined in JIS K7136:2000, and is a value obtained in accordance with the equation: Haze (%)=[(τ₄/τ₂)−τ₃(τ₂/τ₁)]×100 (τ₁: flux of incident light, τ₂: total light flux transmitted through a test piece, τ₃: light flux diffused in a unit, τ₄: light flux diffused in the unit and test piece).

Although the total thickness of the light control film is not particularly limited, it is usually about 20 to 300 μm.

The light control film of the present invention explained above is mainly used as a member of a backlight constituting a liquid crystal display, illumination signboard, and so forth.

Hereafter, the backlight of the present invention will be explained. The backlight of the present invention consists at least of a light control film and a light source. As the light control film, the aforementioned light control film is used. Although the direction of the light control film arranged in the backlight is not particularly limited, it is preferably used so that the rough surface should serve as a light emergent surface side. For the backlight, a configuration called edge light type or direct type is preferably employed.

A backlight of the edge light type consists of a light guide plate, a light source disposed on at least one end of the light guide plate, a light control film disposed on the light emergent surface side of the light guide plate, and so forth. The light control film is preferably used so that the rough surface should serve as the light emergent surface. Further, a prism sheet is preferably used between the light guide plate and the light control film. With such a configuration, a backlight unit exhibiting superior balance of front luminance and a view angle and not exhibiting glare, which is a problem peculiar to a prism sheet, can be provided.

The light guide plate has a substantially plate-like shape at least one of which sides serves as a light incident surface and one of which surfaces perpendicular to the side serves as a light emergent surface, and mainly consists of a matrix resin selected from highly transparent resins such as polymethyl methacrylate. Resin particles having a refractive index different from that of the matrix resin may be added as required. Each surface of the light guide plate may not be a uniform plane, but has a complicated surface profile, or may be subjected to diffusion printing for a dot pattern or the like.

The light source is disposed end of the light guide plate, and a cold-cathode tube is mainly used. Examples of the shape of the light source include a linear shape, L-shape, and so forth.

Besides the aforementioned light control film, light guide plate, and light source, the backlight of the edge light type may be equipped with a light reflector, a polarization film, an electromagnetic interference shield film etc. depending on the purpose.

One embodiment of the backlight of the edge light type according to the present invention is shown in FIG. 12. This backlight 140 has a configuration that light sources 142 are provided on the both sides of a light guide plate 141, and a light control film 143 is placed on the upside of the light guide plate 141 so that a rough surface should be exposed to the outside. The light sources 142 are covered with light source rear reflectors 144 except for the parts facing the light guide plate 141 so that lights from the light source should efficiently enter into the light guide plate 141. Moreover, a light reflector 146 stored in a chassis 145 is provided under the light guide plate 141. By this configuration, lights projected on the side of the light guide plate 141 opposite to the projecting side are returned into the light guide plate 141 again to increase lights emerging from the projection surface of the light guide plate 141.

A backlight of the direct type consists of a light control film, and a light diffusive material and a light source disposed in this order on a surface of the light control film opposite to the light emergent surface, and so forth. The light control film is preferably used so that the rough surface should serve as the light emergent surface. Moreover, a prism sheet is preferably used between the light diffusing material and the light control film. With such a configuration, a backlight unit exhibiting superior balance of front luminance and view angle and not exhibiting glare, which is a problem peculiar to a prism sheet, can be provided.

The light diffusive material is for erasing a pattern of the light source, and a milky resin plate, a transparent substrate on which a dot pattern is formed on a portion corresponding to the light source (lighting curtain) as well as a so-called light diffusive film having a convexo-concave light diffusing layer on a transparent film, and so forth can be used individually or in a suitable combination.

As the light source, a cold-cathode tube is mainly used. Examples of the shape of the light source include a linear shape, L-shape, and so forth. Besides the aforementioned light control film, light diffusing material, and light source, the backlight of the direct type may be equipped with a light reflector, a polarization film, an electromagnetic wave shield film, etc. depending on the purpose.

One embodiment of the backlight of the direct type according to the present invention is shown in FIG. 13. This backlight 150 has a configuration that plural light sources 152 are provided above a light reflector 156 stored in a chassis 155, and a light control film 153 is placed thereon via a light diffusive material 157 as shown in the drawing.

Because the backlight of the present invention utilizes a light control film having a specific rough surface as a light control film that controls direction of lights emerging from a light source or a light guide plate, it can improve front luminance compared with conventional backlights, and suffers from the problem of glare and generation of scratches in less degrees compared with the case of using a prism sheet alone.

EXAMPLES

Hereafter, the present invention will be further explained with reference to examples.

Examples 1 to 4

Four kinds of molds (1) to (4) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (1) to (3), and a silicone resin having a refractive index of 1.40 was poured into the mold (4). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (1) to (4) having a size of 23 cm (for the direction perpendicular to the light source)×31 cm (for the direction parallel to the light source) (light control film of Examples 1 to 4).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (1) to (4) were measured by using a laser microscope (VK-9500, KEYENCE CORP.) with an objective lens of magnification ×50. The measurement interval in the plane was about 0.26 μm. Since one field of the objective lens of magnification ×50 is 270 μm×202 μm, an automatic connecting function was used to obtain surface height data of a region of 1 mm×1 mm. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes of the curved surfaces to base planes (θ_nv, unit is degree) were calculated by using these surface height data. The results obtained for the light control films (1) to (4) are shown in Table 1. Further, by using a turbidimeter (NDH2000, Nippon Denshoku), hazes of the light control films (1) to (4) were measured according to JIS K7136:2000. The measurement results are also shown in Table 1.

	TABLE 1
	θnv	haze
	(degree)	(%)
Example 1	43.0	82.7
	43.0
	43.7
	41.4
	41.9
Example 2	34.1	82.6
	35.6
	33.8
	34.8
	32.7
Example 3	29.6	79.1
	28.2
	28.4
	28.3
	31.0
Example 4	33.4	79.7
	34.4
	32.8
	34.9
	33.7

As seen from the results shown in Table 1, the averages of slopes of the curved surfaces of the light control films of Examples 1 to 4 were not less than 27 degrees and not more than 70 degrees at all the measurement points. Moreover, all the light control films of Examples 1 to 4 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (1) to (4) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (1) to (4) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (1) to (4) are shown in Table 2 (unit is “cd/m²”).

	TABLE 2
	luminance (cd/m2)
	Example 1	Example 2	Example 3	Example 4
parallel	left 45	1050	1130	1150	1140
direction	degree
	left 30	2100	1730	1630	1680
	degree
	0	2300	1810	1680	1740
	degree
	right30	2070	1710	1620	1660
	degree
	right45	1060	1130	1150	1140
	degree
per-	up 45	1040	1240	1290	1270
pendicular	degree
direction	up 30	2370	1950	1840	1890
	degree
	0	2300	1810	1680	1740
	degree
	down 30	2350	1940	1830	1880
	degree
	down 45	1010	1230	1290	1260
	degree

It was demonstrated by the results shown in Table 2 that, for the light control films of Examples 1 to 4, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Examples 5 to 8

Four kinds of molds (5) to (8) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (5) to (7), and a silicone resin having a refractive index of 1.40 was poured into the mold (8). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (5) to (8) having a size of 23 cm×31 cm (light control films of Examples 5 to 8).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (5) to (8) were measured in the same manner as that used in Examples 1 to 4. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes to base planes of the curved surfaces (θ_nv, unit is degree) were calculated by using the obtained surface height data. Further, surface areas of the rough surfaces (A2) were obtained from the same surface height data, the ratios thereof to the orthogonal projections of the measured rough surfaces (A1) (A_r=A2/A1) were calculated, and products or quotients were obtained by using the averages of slopes of the curved surface (θ_nv), and the surface area ratios (A_r). The results obtained for the light control films (5) to (8) are shown in Table 3 (unit of slope is “degree”). Further, by using a turbidimeter (NDH2000, Nippon Denshoku), hazes of the light control films (5) to (8) were measured according to JIS K7136:2000. The measurement results are also shown in Table 3.

	TABLE 3
	θnv				haze
	(degree)	Ar	θnv ÷ Ar	θnv × Ar	(%)
	Example 5	42.6	1.552	27.4	66.1	82.7
		42.2	1.573	26.9	66.4
		41.1	1.613	25.5	66.3
		43.1	1.500	28.8	64.7
		43.6	1.594	27.3	69.4
	Example 6	50.9	2.080	24.5	105.9	82.6
		52.4	2.046	25.6	107.2
		51.7	2.168	23.9	112.2
		53.1	2.032	26.2	108.0
		48.9	2.022	24.2	98.9
	Example 7	36.5	1.389	26.3	50.7	82.0
		36.7	1.393	26.4	51.2
		35.0	1.399	25.0	48.9
		35.7	1.427	25.0	50.9
		36.9	1.414	26.1	52.2
	Example 8	44.0	1.735	25.4	76.3	82.1
		44.8	1.809	24.7	81.0
		44.6	1.713	26.1	76.5
		42.0	1.732	24.2	72.7
		43.8	1.749	25.1	76.7

As shown in Table 3, in the light control films of Examples 5 to 8, fluctuation of the average of slopes of the curved surface and the surface area ratio was small at all the measurement points, and thus the films had a uniform roughness characteristic as the whole films. Moreover, all the light control films of Examples 5 to 8 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (5) to (8) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (5) to (8) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (5) to (8) are shown in Table 4 (unit is “cd/m²”).

	TABLE 4
	luminance (cd/m2)
	Example 5	Example 6	Example 7	Example 8
parallel	left 45	1060	1100	1130	1110
direction	degree
	left 30	2040	1850	1710	1800
	degree
	0	2220	1970	1780	1900
	degree
	right 30	2020	1830	1690	1780
	degree
	right 45	1080	1110	1140	1120
	degree
per-	up 45	1070	1170	1250	1200
pendicular	degree
direction	up 30	2310	2090	1930	2030
	degree
	0	2220	1970	1780	1900
	degree
	down 30	2280	2070	1910	2010
	degree
	down 45	1040	1160	1240	1190
	degree

It was demonstrated by the results shown in Table 4 that, for the light control films of Examples 5 to 8, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Comparative Examples 1 to 3

For commercially available light diffusive sheets (Comparative Examples 1 to 3), surface profiles of rough surfaces (light emergent surfaces) were measured at 5 points on each film in the same manner as that used in the examples, and averages of slopes of the curved surface (θ_nv) were calculated. The results obtained for the light diffusive sheets of Comparative Examples 1 to 3 are shown in Table 5 in order.

	TABLE 5
	θnv	haze
	(degree)	(%)
	Comparative	25.2	89.2
	Example 1	25.3
		25.0
		26.2
		26.0
	Comparative	16.8	85.7
	Example 2	16.3
		17.2
		16.7
		16.1
	Comparative	10.7	65.5
	Example 3	10.3
		10.6
		10.7
		11.2

As seen from the results shown in Table 5, all the light diffusive sheets of Comparative Examples 1 to 3 were those that could not provide an average of slopes of the curved surface (θ_nv) not less than 27 degrees and not more than 70 degrees at all the measurement points.

Then, the light diffusive sheets of Comparative Examples 1 to 3 were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light diffusive sheets of Comparative Examples 1 to 3 were each disposed on a light guide plate so that the rough surface of the light diffusive sheet should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results are shown in Table 6.

	TABLE 6
	luminance (cd/m2)
	Comparative	Comparative	Comparative
	Example 1	Example 2	Example 3
parallel direction	left 45	1170	1310	1250
	degree
	left 30	1540	1310	1170
	degree
	0	1560	1220	1070
	degree
	right 30	1510	1310	1170
	degree
	right 45	1170	1310	1240
	degree
perpendicular	up 45	1340	1620	1540
direction	degree
	up 30	1740	1500	1320
	degree
	0	1560	1220	1070
	degree
	down 30	1700	1470	1370
	degree
	down 45	1340	1580	1600
	degree

As seen from the results shown in Table 6, when the conventional light diffusive sheets were incorporated into the backlight unit, favorable front luminance could not be obtained.

As clearly seen from the results of the aforementioned examples, the light control films of the examples were those exhibiting superior front luminance and appropriate light diffusing property, because the rough surfaces thereof were designed to satisfy the specific configuration. Moreover, by incorporating such light control films into a backlight unit, backlight units exhibiting strong front luminance and not suffering from glare and generation of an interference pattern could be provided.

Examples 9 to 12

Four kinds of molds (9) to (12) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (9) to (11), and a silicone resin having a refractive index of 1.40 was poured into the mold (12). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (9) to (12) having a size of 23 cm (for the direction perpendicular to the light source)×31 cm (for the direction parallel to the light source) (light control film of Examples 9 to 12).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (9) to (12) were measured by using a laser microscope (VK-9500, KEYENCE CORP.) with an objective lens of magnification ×50. The measurement interval in the plane was about 0.26 μm. Since one field of the objective lens of magnification ×50 is 270 μm×202 μm, an automatic coupling function was used to obtain surface height data of a region of 1 mm×1 mm. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes of the curved surfaces to base planes (θ_nv) were calculated by using these surface height data. Further, A_sk was calculated in accordance with the aforementioned formula (5) by using the same surface height data. The results obtained for the light control films (9) to (12) are shown in Table 1 (unit of slope is “degree”). Further, by using a turbidimeter (NDH2000, Nippon Denshoku), hazes of the light control films (9) to (12) were measured according to JIS K7136:2000. The measurement results are also shown in Table 1.

	TABLE 7
	θnv		haze
	(degree)	| Ask |	(%)
	Example 9	42.0	0.661	82.5
		43.8	0.655
		41.0	0.644
		40.9	0.652
		41.0	0.631
	Example 10	34.1	0.661	82.6
		35.2	0.667
		35.6	0.683
		35.6	0.671
		33.9	0.654
	Example 11	29.6	0.010	79.1
		28.2	0.038
		28.6	0.104
		30.5	0.098
		29.7	0.103
	Example 12	36.5	0.366	82.0
		34.9	0.369
		35.9	0.368
		35.7	0.351
		38.1	0.370

As seen from the results shown in Table 7, the averages of slopes of the curved surfaces (θ_nv) of the light control films of Examples 9 to 12 were not less than 27 degrees and not more than 70 degrees at all the measurement points. Further, all the absolute values of A_sk were not more than 1.2. Moreover, all the light control films of Examples 9 to 12 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (9) to (12) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (9) to (12) were each disposed on a light guide plate so that the rough surfaces should serve as the light emergent surfaces, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (9) to (12) are shown in Table 8 (unit is “cd/m²”).

	TABLE 8
	luminance (cd/m2)
	Example	Example	Example	Example
	9	10	11	12
	parallel	left 45	1040	1120	1150	1130
	direction	degree
		left 30	1960	1740	1650	1720
		degree
		0	2110	1810	1680	1780
		degree
		right 30	1930	1720	1630	1700
		degree
		right 45	1060	1130	1150	1130
		degree
	per-	up 45	903	1150	1250	1170
	pendicular	degree
	direction	up 30	2070	1870	1790	1850
		degree
		0	2110	1810	1680	1780
		degree
		down 30	2060	1870	1800	1860
		degree
		down 45	948	1170	1270	1200
		degree

It was demonstrated by the results shown in Table 8 that, for the light control films of Examples 9 to 12, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Examples 13 to 16

Four kinds of molds (13) to (16) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (13) to (15), and a silicone resin having a refractive index of 1.40 was poured into the mold (16). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (13) to (16) having a size of 23 cm×31 cm.

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (13) to (16) were measured in the same manner as that used in Examples 9 to 12. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes of the curved surfaces to base planes (θ_nv) were calculated by using the obtained surface height data. Further, A_ku was calculated in accordance with the aforementioned formula (6) by using the same surface height data. The results obtained for the light control films (13) to (16) are shown in Table 9 (unit of slope is “degree”). Further, by using a turbidimeter (NDH2000, Nippon Denshoku), hazes of the light control films (13) to (16) were measured according to JIS K7136:2000. The measurement results are also shown in Table 9.

	TABLE 9
	θnv		haze
	(degree)	Aku	(%)
	Example 13	49.6	2.072	82.8
		48.2	2.018
		44.9	2.151
		45.8	2.113
		46.7	2.044
	Example 14	40.1	4.023	76.2
		41.1	3.910
		38.2	4.005
		38.5	4.102
		38.9	4.146
	Example 15	34.0	2.063	82.7
		35.2	2.034
		32.8	1.990
		33.0	2.131
		34.2	2.150
	Example 16	41.5	1.710	82.6
		42.3	1.661
		40.4	1.723
		42.9	1.774
		43.0	1.726

As seen from the results shown in Table 9, the averages of slopes of the curved surfaces (θ_nv) of the light control films of Examples 13 to 16 were not less than 27 degrees and not more than 70 degrees at all the measurement points. Further, all the values of A_ku were not less than 1.5 and not more than 5.0. Moreover, all the light control films of Examples 13 to 16 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (13) to (16) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (13) to (16) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (13) to (16) are shown in Table 10 (unit is “cd/m²”).

	TABLE 10
	luminance (cd/m2)
	Example	Example	Example	Example
	13	14	15	16
parallel	left 45	1050	1130	1150	1120
direction	degree
	left 30	1950	1690	1630	1740
	degree
	0	2100	1740	1650	1810
	degree
	right 30	1920	1670	1610	1720
	degree
	right 45	1060	1140	1160	1130
	degree
per-	up 45	911	1200	1270	1150
pendicular	degree
direction	up 30	2070	1830	1770	1870
	degree
	0	2100	1740	1650	1810
	degree
	down 30	2050	1830	1780	1880
	degree
	down 45	956	1220	1300	1170
	degree

It was demonstrated by the results shown in Table 10 that, for the light control films of Examples 13 to 16, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Comparative Examples 4 to 6

Three kinds of molds (17) to (19) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, and an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds. Subsequently, the poured resin was cured, and then taken out from the molds to obtain light control films (17) to (19) having a size of 23 cm×31 cm (light control films of Comparative Examples 4 to 6).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (17) to (19) were measured in the same manner as that used in Examples 9 to 12. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes of the curved surfaces to base planes (θ_nv) were calculated by using the obtained surface height data. Further, A_sk was calculated in accordance with the aforementioned formula (5) by using the same surface height data. The results obtained for the light control films (17) to (19) are shown in Table 11 (unit of slope is “degree”).

	TABLE 11
	θnv		haze
	(degree)	| Ask |	(%)
	Comparative	33.8	1.272	81.2
	Example 4	33.0	1.258
		35.5	1.286
		34.8	1.269
		32.2	1.269
	Comparative	41.5	1.479	81.3
	Example 5	40.2	1.435
		42.1	1.452
		40.8	1.450
		40.2	1.456
	Comparative	47.7	1.408	74.5
	Example 6	45.7	1.398
		50.1	1.388
		49.8	1.429
		48.5	1.404

As seen from the results shown in Table 11, the averages of slopes of the curved surfaces (θ_nv) of the light control films (17) to (19) were not less than 27 degrees and not more than 70 degrees at all the measurement points. However, all the values of A_sk were more than 1.2.

Then, the light control films (17) to (19) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (17) to (19) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (17) to (19) are shown in Table 12 (unit is “cd/m²”).

	TABLE 12
	luminance (cd/m2)
	Comparative	Comparative	Comparative
	Example 4	Example 5	Example 6
parallel	left 45	1230	1210	1200
direction	degree
	left 30	1420	1460	1500
	degree
	0	1370	1420	1480
	degree
	right 30	1420	1450	1500
	degree
	right 45	1220	1210	1200
	degree
perpendicular	up 45	1500	1460	1420
direction	degree
	up 30	1590	1620	1660
	degree
	0	1370	1420	1480
	degree
	down 30	1600	1630	1670
	degree
	down 45	1500	1470	1420
	degree

From the results shown in Table 12, it was found that when the light control films of Comparative Examples 4 to 6 were incorporated into a backlight unit, front luminance was insufficient.

Comparative Examples 7 to 9

Three kinds of molds (20) to (22) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, and an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds. Subsequently, the poured resin was cured, and then taken out from the molds to obtain light control films (20) to (22) having a size of 23 cm×31 cm (light control films of Comparative Examples 7 to 9).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (20) to (22) were measured in the same manner as that used in Examples 9 to 12. The measurement was performed at arbitrary 5 positions on each light control film, and averages of slopes of the curved surfaces to base planes (θ_nv) were calculated by using the obtained surface height data. Further, A_ku was calculated in accordance with the aforementioned formula (6) by using the same surface height data. The results obtained for the light control films (20) to (22) are shown in Table 13 (unit of slope is “degree”).

	TABLE 13
	θnv		haze
	(degree)	Aku	(%)
	Comparative	28.3	1.312	70.3
	Example 7	28.8	1.258
		29.0	1.281
		27.7	1.338
		29.2	1.361
	Comparative	33.4	1.395	76.9
	Example 8	34.6	1.302
		33.6	1.391
		34.8	1.400
		34.9	1.393
	Comparative	38.7	7.198	70.6
	Example 9	37.4	7.270
		39.6	7.165
		39.9	7.053
		38.6	7.197

As seen from the results shown in Table 13, the averages of slopes of the curved surfaces (θ_nv) of the light control films (20) to (22) were not less than 27 degrees and not more than 70 degrees at all the measurement points. However, all the values of A_ku were less than 1.5 or more than 5.0.

Then, the light control films (20) to (22) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (20) to (22) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (20) to (22) are shown in Table 14 (unit is “cd/m²”).

	TABLE 14
	luminance (cd/m2)
	Comparative	Comparative	Comparative
	Example 7	Example 8	Example 9
parallel	left 45	1270	1220	1240
direction	degree
	left 30	1310	1450	1390
	degree
	0	1210	1400	1320
	degree
	right 30	1310	1440	1390
	degree
	right 45	1260	1210	1230
	degree
perpendicular	up 45	1630	1480	1550
direction	degree
	up 30	1480	1610	1550
	degree
	0	1210	1400	1320
	degree
	down 30	1500	1620	1570
	degree
	down 45	1620	1480	1540
	degree

From the results shown in Table 14, it was found that when the light control films of Comparative Examples 7 to 9 were incorporated into a backlight unit, front luminance was insufficient.

Comparative Examples 10 and 11

For commercially available light diffusive sheets (Comparative Examples 10 and 11), surface height data of rough surfaces (light emergent surfaces) were measured in the same manner as in Examples at arbitrary 5 positions on each sheet, and averages of slopes of the curved surfaces (θ_nv) were obtained. Further, A_sk and A_ku were calculated in accordance with the aforementioned formulas (5) and (6), respectively, by using the same surface height data. The results obtained for the light diffusive sheets of Comparative Examples 10 and 11 are shown in Table 15.

	TABLE 15
	θnv
	(degree)	| Ask |	Aku
	Comparative	25.3	0.131	3.321
	Example 10	26.3	0.134	3.282
		26.3	0.128	3.409
		24.8	0.125	3.259
		24.2	0.135	3.353
	Comparative	16.8	0.730	3.661
	Example 11	16.6	0.733	3.803
		17.4	0.741	3.823
		17.5	0.759	3.808
		17.0	0.704	3.688

As seen from the results shown in Table 15, the light diffusive sheets of Comparative Examples 10 and 11 were those that could not provide an average of slopes of the curved surface (θ_nv) not less than 27 degrees and not more than 70 degrees at all the measurement points.

Then, the light diffusive sheets of Comparative Examples 10 and 11 were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light diffusive sheets of Comparative Examples 7 and 8 were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) at the center of the backlight unit (1 inch=2.54 cm). The results are shown in Table 16.

	TABLE 16
	luminance(cd/m2)
	Comparative	Comparative
	Example 10	Example 11
	parallel	left 45	1180	1260
	direction	degree
		left 30	1560	1330
		degree
		0	1560	1240
		degree
		right30	1550	1330
		degree
		right45	1180	1250
		degree
	perpendicular	up 45	1350	1610
	direction	degree
		up 30	1710	1500
		degree
		0	1560	1240
		degree
		down 30	1720	1520
		degree
		down 45	1360	1600
		degree

As seen from the results shown in Table 16, when the conventional light diffusive sheets were incorporated into a backlight unit, favorable front luminance could not be obtained.

As clearly seen from the results of the aforementioned examples, the light control films of the examples exhibited superior front luminance and appropriate light diffusing property, because the rough surfaces thereof were designed so that they should satisfy the specific configuration. Further, by incorporating such light control films into a backlight unit, backlight units exhibiting high front luminance and not suffering from glare and generation of a interference pattern could be obtained.

Examples 17 to 20

Four kinds of molds (23) to (26) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (23) to (25), and a silicone resin having a refractive index of 1.40 was poured into the mold (26). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (23) to (26) having a size of 23 cm (for the direction perpendicular to the light source)×31 cm (for the direction parallel to the light source) (light control film of Examples 17 to 20).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (23) to (26) were measured by using a laser microscope (VK-9500, KEYENCE CORP.) with an objective lens of magnification ×50. The measurement interval in the plane was about 0.26 μm. Since one field of the objective lens of magnification ×50 is 270 μm×202 μm, an automatic connecting function was used to obtain surface height data of a region of 1 mm×1 mm. The measurement was performed at arbitrary 5 positions on each light control film, surface areas of the rough surfaces (A2) were obtained by using the obtained surface height data, and the ratios (A_r=A2/A1) to the orthogonal projections of the measured rough surfaces (A1) were calculated. Further, A_sk was calculated in accordance with the aforementioned formula (5) by using the same surface height data. The results obtained for the light control films (23) to (26) are shown in Table 17. Further, measurement results of hazes of the light control films (23) to (26) measured by using a turbidimeter (NDH2000, Nippon Denshoku) according to JIS K7136:2000 are also shown in Table 17.

	TABLE 17
			haze
	Ar	|Ask|	(%)
	Example 17	2.239	0.097	82.8
		2.144	0.124
		2.241	0.109
		2.306	0.049
		2.208	0.117
	Example 18	1.780	0.792	82.8
		1.834	0.820
		1.705	0.761
		1.708	0.798
		1.801	0.826
	Example 19	1.432	0.260	81.0
		1.489	0.255
		1.389	0.248
		1.423	0.260
		1.500	0.254
	Example 20	1.843	0.020	81.7
		1.773	0.028
		1.816	0.027
		1.894	0.018
		1.823	0.012

As seen from the results shown in Table 17, the surface area ratios A_r of the light control films (23) to (26) of Examples 17 to 20 were not less than 1.2 and not more than 2.5 at all the measurement points. Further, all the absolute values of A_sk were not more than 1.2. Moreover, all the light control films of Examples 17 to 20 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (23) to (26) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (23) to (26) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (23) to (26) are shown in Table 18 (unit is “cd/m²”).

	TABLE 18
	luminance (cd/m2)
	Example	Example	Example	Example
	17	18	19	20
	parallel	left 45	1110	1100	1070	1110
	direction	degree
		left 30	1750	1790	1870	1760
		degree
		0	1830	1880	1990	1840
		degree
		right 30	1740	1770	1850	1740
		degree
		right 45	1120	1110	1090	1120
		degree
	per-	up 45	1130	1090	1000	1120
	pendicular	degree
	direction	up 30	1890	1920	1990	1890
		degree
		0	1830	1880	1990	1840
		degree
		down 30	1890	1920	1990	1900
		degree
		down 45	1160	1120	1040	1150
		degree

It was demonstrated by the results shown in Table 18 that, for the light control films (23) to (26) of Examples 17 to 20, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Examples 21 to 24

Four kinds of molds (27) to (30) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds (27) to (29), and a silicone resin having a refractive index of 1.40 was poured into the mold (30). Subsequently, the poured resins were cured, and then taken out from the molds to obtain light control films (27) to (30) having a size of 23 cm×31 cm (light control films of Examples 21 to 24).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (27) to (30) were measured in the same manner as that used in Examples 17 to 20. The measurement was performed at arbitrary 5 positions on each light control film, and surface areas of the rough surfaces (A2) were obtained by using the obtained surface height data, and the ratios (A_r=A2/A1) to the orthogonal projections of the measured rough surfaces (A1) were calculated. Further, A_ku was calculated in accordance with the aforementioned formula (6) by using the same surface height data. The results obtained for the light control films (27) to (30) are shown in Table 19 (unit of slope is “degree”). Further, by using a turbidimeter (NDH2000, Nippon Denshoku), hazes of the light control films (27) to (30) were measured according to JIS K7136:2000. The measurement results are also shown in Table 19.

	TABLE 19
			haze
	Ar	Aku	(%)
	Example 21	1.452	1.594	78.4
		1.403	1.536
		1.446	1.590
		1.500	1.548
		1.408	1.593
	Example 22	1.622	1.925	82.6
		1.686	1.946
		1.683	1.837
		1.554	1.960
		1.584	1.890
	Example 23	2.239	1.747	82.0
		2.229	1.728
		2.179	1.787
		2.217	1.783
		2.257	1.830
	Example 24	1.780	2.590	82.8
		1.727	2.562
		1.848	2.638
		1.863	2.592
		1.861	2.480

As seen from the results shown in Table 19, the surface area ratios A_r of the light control films of Examples 21 to 24 were not less than 1.2 and not more than 2.5 at all the measurement points. Further, all the values of A_ku were not less than 1.5 and not more than 5.0. Moreover, all the light control films (27) to (30) of Examples 21 to 24 had a haze of 70% or higher, and thus satisfied the optical characteristics required for obtaining favorable front luminance.

Then, the light control films (27) to (30) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (27) to (30) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (27) to (30) are shown in Table 20 (unit is “cd/m²”).

	TABLE 20
	luminance (cd/m2)
	Example	Example	Example	Example
	21	22	23	24
parallel	left 45	1060	1100	1110	1100
direction	degree
	left 30	1890	1790	1740	1780
	degree
	0	2030	1880	1830	1860
	degree
	right 30	1870	1770	1730	1760
	degree
	right 45	1080	1110	1120	1110
	degree
per-	up 45	968	1090	1130	1110
pendicular	degree
direction	up 30	2020	1920	1890	1900
	degree
	0	2030	1880	1830	1860
	degree
	down 30	2010	1900	1890	1910
	degree
	down 45	1000	1110	1160	1120
	degree

It was demonstrated by the results shown in Table 20 that, for the light control films of Examples 21 to 24, only by incorporating one sheet of light control film into the backlight unit, the luminance for emergent angles of 30 degrees or less could be increased, and thus strong emergent lights could be obtained for the front direction.

Comparative Examples 12 to 14

Three kinds of molds (31) to (33) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, and an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds. Subsequently, the poured resin was cured, and then taken out from the molds to obtain light control films (31) to (33) having a size of 23 cm×31 cm (light control films of Comparative Examples 12 to 14).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (31) to (33) were measured in the same manner as that used in Examples 17 to 20. The measurement was performed at arbitrary 5 positions on each light control film, surface areas of the rough surfaces (A2) were obtained by using the obtained surface height data, and the ratios (A_r=A2/A1) to the orthogonal projections of the measured rough surfaces (A1) were calculated. Further, A_sk was calculated in accordance with the aforementioned formula (5) by using the same surface height data. The results obtained for the light control films (31) to (33) are shown in Table 21 (unit of slope is “degree”).

	TABLE 21
			haze
	Ar	|Ask|	(%)
	Comparative	1.413	2.159	78.7
	Example 12	1.386	2.246
		1.434	2.146
		1.462	2.091
		1.448	2.056
	Comparative	1.658	1.479	81.2
	Example 13	1.625	1.518
		1.578	1.493
		1.716	1.456
		1.639	1.447
	Comparative	2.401	1.755	70.4
	Example 14	2.469	1.637
		2.294	1.749
		2.498	1.824
		2.342	1.758

As seen from the results shown in Table 21, the surface area ratios A_r of the light control films (31) to (33) of Comparative Examples 12 to 14 were not less than 1.2 and not more than 2.5 at all the measurement points. However, all the absolute values of A_sk were more than 1.2.

Then, the light control films (31) to (33) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (31) to (33) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (31) to (33) are shown in Table 22 (unit is “cd/m²”).

	TABLE 22
	luminance (cd/m2)
	Comparative	Comparative	Comparative
	Example 12	Example 13	Example 14
parallel	left 45	1240	1210	1220
direction	degree
	left 30	1380	1470	1430
	degree
	0	1320	1430	1380
	degree
	right 30	1380	1460	1420
	degree
	right 45	1230	1210	1210
	degree
perpendicular	up 45	1540	1450	1490
direction	degree
	up 30	1550	1620	1590
	degree
	0	1320	1430	1380
	degree
	down 30	1570	1630	1600
	degree
	down 45	1540	1450	1490
	degree

From the results shown in Table 22, it was found that when the light control films of Comparative Examples 12 to 14 were incorporated into a backlight unit, front luminance was insufficient.

Comparative Examples 15 to 17

Three kinds of molds (34) to (36) on which predetermined convexo-concave profiles were formed by a laser microprocessing technique were prepared, and an ultraviolet curing resin having a refractive index of 1.50 was poured into the molds. Subsequently, the poured resin was cured, and then taken out from the molds to obtain light control films (34) to (36) having a size of 23 cm×31 cm (light control films of Comparative Examples 15 to 17).

Then, height data of the rough surfaces (light emergent surfaces) of the light control films (34) to (36) were measured in the same manner as that used in the examples. The measurement was performed at arbitrary 5 positions on each light control film, surface areas of the rough surfaces (A2) were obtained by using the obtained surface height data, and the ratios (A_r=A2/A1) to the orthogonal projections of the measured rough surfaces (A1) were calculated. Further, A_ku was calculated in accordance with the aforementioned formula (6) by using the same surface height data. The results obtained for the light control films (34) to (36) are shown in Table 23 (unit of slope is “degree”).

	TABLE 23
			haze
	Ar	Aku	(%)
	Comparative	2.034	7.270	71.0
	Example 15	2.025	7.576
		2.003	7.249
		2.042	6.935
		2.118	7.475
	Comparative	1.565	1.351	72.8
	Example 16	1.519	1.301
		1.571	1.334
		1.595	1.403
		1.612	1.307
	Comparative	1.392	1.312	72.2
	Example 17	1.441	1.310
		1.348	1.319
		1.413	1.349
		1.404	1.250

As seen from the results shown in Table 23, the surface area ratios A_r of the light control films of Comparative Examples 15 to 17 were not less than 1.2 and not more than 2.5 at all the measurement points. However, all the values of A_ku were less than 1.5 or more than 5.0.

Then, the light control films (34) to (36) were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light control films (34) to (36) were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results obtained for the light control films (34) to (36) are shown in Table 24 (unit is “cd/m²”).

	TABLE 24
	luminance (cd/m2)
	Comparative	Comparative	Comparative
	Example 15	Example 16	Example 17
parallel	left 45	1220	1210	1270
direction	degree
	left 30	1460	1480	1310
	degree
	0	1410	1440	1210
	degree
	right 30	1450	1470	1310
	degree
	right 45	1220	1210	1260
	degree
perpendicular	up 45	1480	1450	1640
direction	degree
	up 30	1620	1640	1480
	degree
	0	1410	1440	1210
	degree
	down 30	1630	1650	1510
	degree
	down 45	1470	1450	1630
	degree

From the results shown in Table 24, it was found that when the light control films of Comparative Examples 15 to 17 were incorporated into a backlight unit, front luminance was insufficient.

Comparative Examples 18 and 19

For commercially available light diffusive sheets (Comparative Examples 18 and 19), surface height data of rough surfaces (light emergent surfaces) were measured in the same manner as in Examples at arbitrary 5 positions on each sheet, areas of the rough surfaces (A2) were obtained, and the ratios (A_r=A2/A1) to the orthogonal projections of the measured rough surfaces (A1) were calculated. Further, A_sk and A_ku were calculated in accordance with the aforementioned formulas (5) and (6), respectively, by using the same surface height data. The results obtained for the light diffusive sheets of Comparative Examples 18 and 19 are shown in Table 25.

	TABLE 25
	Ar	|Ask|	Aku
	Comparative	1.157	0.178	3.441
	Example 18	1.107	0.170	3.559
		1.166	0.179	3.578
		1.117	0.184	3.584
		1.156	0.186	3.309
	Comparative	1.069	0.722	3.671
	Example 19	1.029	0.707	3.721
		1.081	0.748	3.697
		1.109	0.718	3.508
		1.098	0.724	3.740

As seen from the results shown in Table 25, the light control films of Comparative Examples 18 and 19 did not have a surface area ratio A_r not less than 1.2 and not more than 2.5 at all the measurement points.

Then, the light diffusive sheets of Comparative Examples 18 and 19 were each incorporated into a 15-inch edge light type backlight unit (one cold-cathode tube was provided for each of upside and downside), and front luminance was measured. That is, the light diffusive sheets of Comparative Examples 18 and 19 were each disposed on a light guide plate so that the rough surface should serve as the light emergent surface, and the luminance was measured at each emergent angle for the parallel and perpendicular directions with respect to the light source (cold-cathode tubes) positioned at the center of the backlight unit (1 inch=2.54 cm). The results are shown in Table 26.

	TABLE 26
	luminance (cd/m2)
	Comparative	Comparative
	Example 18	Example 19
	parallel	left 45	1180	1260
	direction	degree
		left 30	1560	1330
		degree
		0	1560	1240
		degree
		right 30	1550	1330
		degree
		right 45	1180	1250
		degree
	perpendicular	up 45	1350	1610
	direction	degree
		up 30	1710	1500
		degree
		0	1560	1240
		degree
		down 30	1720	1520
		degree
		down 45	1360	1600
		degree

As seen from the results shown in Table 26, when the conventional light diffusive sheets were incorporated into a backlight unit, favorable front luminance could not be obtained.

Moreover, for the light control films of Examples 1 to 24, absolute values of averages (φ_ave) of angles (φ, −180 degrees<φ≦180 degrees) between orthogonal projections of normals of curved surfaces of the rough surfaces projected on base planes and one side of predetermined approximately square regions were calculated. Specifically, for a square region (1 mm×1 mm) determined at one arbitrary position on each of the light control films of Examples 1 to 24, surface profile was measured in the same manner as that used in Examples 1 to 24, and curved surface of the rough surface was approximated on the basis of the measured height data. The angles φ between orthogonal projections of normals at predetermined multiple points of the curved surfaces projected on a base plane and one side of the predetermined square region were obtained, the average thereof, φ_ave, was calculated, and the absolute value thereof was obtained. As a result, the absolute value of φ_ave was 5 or less for all the light control films of Examples 1 to 24. Furthermore, also with height data obtained by rotating the square region within the film around the center of the region as a rotation axis, the absolute value of φ_ave was 5 or less irrespective of the direction of the square region.

For the light control films of Examples 1, 9 and 17 as typical examples, change of the absolute value of φ_ave observed when the direction of the determined square was turned by 10 degrees at a time for 360 degrees is shown in the graph of FIG. 14. In FIG. 14, the vertical axis represents the absolute value of φ_ave, the horizontal axis represents the direction (degree) based on the original position of the square region, the thick line 1401 represents the result for the light control film of Example 1, thin line 1402 represents that of Example 9, and the dashed line 1403 represents that of Example 17. As seen from the results shown in the graph of FIG. 14, all the absolute values of φ_ave of the light control films of Examples 1, 9 and 17 were less than 0.5 degree even at the maximum, and the absolute value of φ_ave was not more than 5 degree.

Since the absolute value of φ_ave was not more than 5 degree for any direction of the determined square region in the light control films of Examples 1 to 24 as described above, they did not cause glare when they were incorporated into backlight units.

As clearly seen from the results of the aforementioned examples, the light control films of the examples were those exhibiting superior front luminance and appropriate light diffusing property, because the rough surfaces thereof were designed to satisfy the specific configuration. Moreover, by incorporating such light control films into a backlight unit, backlight units exhibiting strong front luminance and not suffering from glare and generation of an interference pattern could be provided.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 Sectional views showing embodiments of the light control film of present invention

FIG. 2-1 Sectional view of a three-dimensional shape of a convex portion used in the present invention for simulating difference in emergent angle characteristics caused by the shape

FIG. 2-2 Drawing showing an example of three-dimensional shape of a convex portion used in the present invention for simulating difference in emergent angle characteristics caused by the shape

FIG. 3 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 4 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 5 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 6 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 7 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 8 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 9 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 10 Drawing showing results of three-dimensional simulation performed by changing shape of convex portion in an embodiment of the invention

FIG. 11 Drawing showing an example of the rough surface of the light control film of present invention

FIG. 12 Drawing showing an embodiment of the backlight unit of the present invention

FIG. 13 Drawing showing an embodiment of the backlight unit of the present invention

FIG. 14 Graph showing relations between the absolute values of φave measured for the light control films of Examples 1, 9 and 17 and direction of the determined square region.

DESCRIPTION OF NOTATIONS

• 10 . . . Light control film
• 11 . . . Substrate
• 12 . . . Convexo-concave layer
• 140 . . . Backlight unit of edge light type
• 150 . . . Backlight unit of direct type

Claims

1. A light control film having a rough surface, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees at substantially any position on the light control film.

2. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees at any position on the light control film.

3. A light control film having a rough surface, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film and a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) satisfy the following equation (1) or (2) at substantially any position on the light control film.

4. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film and a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) satisfy the following equation (3) or (4) at substantially any position on the light control film.

5. A light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees, and an absolute value of a numerical value (Ask) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film.

6. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees, and an absolute value of a numerical value (Ask) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film.

7. A light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than 27 degrees and not more than 70 degrees, and a numerical value (Aku) calculated in accordance with the equation (6) by using all the height data of the rough surface is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film.

8. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, an average of slopes of the curved surface (θnv (degree)) of the rough surface with respect to a base plane of the film is not less than (59-20 n) degrees and not more than 70 degrees, and a numerical value (Aku) calculated in accordance with the equation (6) by using all the height data of the rough surface is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film.

9. A light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) is not less than 1.2 and not more than 2.5, and absolute value of a numerical value (Ask) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film.

10. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) is not less than (2-0.5 n) and not more than 2.5, and absolute value of a numerical value (Ask) calculated in accordance with the equation (5) by using all the height data of the rough surface is not more than 1.2 is satisfied at substantially any position on the light control film.

11. A light control film having a rough surface, wherein a condition that, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) is not less than 1.2 and not more than 2.5, and a numerical value Aku calculated in accordance with the equation (6) by using all the surface height data is not less than 1.5 and not more than 5.0 is satisfied at substantially any position on the light control film.

12. A light control film having a rough surface formed by a patterned layer comprising a material having a refractive index n, wherein, for a curved surface of the rough surface approximated in an approximately square region having an area of 1 mm2 or larger defined at an arbitrary position on the rough surface by using height data of the rough surface measured with predetermined intervals for the longitudinal and transverse directions in the approximately square region, a ratio of an area of the approximately square region (A1) and a surface area of the approximated curved surface of the rough surface (A2) (Ar=A2/A1) is not less than (2-0.5 n) and not more than 2.5, and a numerical value Aku calculated in accordance with the equation (6) by using all the surface height data is not less than 1.5 and not more than 5.0 at substantially any position on the light control film.

13. The light control film according to claim 1, wherein absolute value of average (φave) of angles (φ, −180 degrees<φ 180 degrees) between orthogonal projections of normals of the curved surface of the rough surface projected on the base plane and one side of the approximately square region is not more than 5 degrees irrespective of the direction along which the approximately square region is defined in the rough surface.

14. A backlight unit comprising a light guide plate equipped with a light source on at least one end portion thereof and having a light emergent surface approximately perpendicular to the end portion and a light control film provided on the light emergent surface of the light guide plate, wherein the light control film according to claim 1 is used as the light control film.

15. The backlight unit according to claim 14, wherein a prism sheet is used between the light control film and the light guide plate.

16. A backlight unit comprising a light source, a light diffusive plate provided on one side of the light source and a light control film provided on the side of the light diffusive plate opposite to the light source side, wherein the light control film according to claim 1 is used as the light control film.