Source: https://patents.google.com/patent/JP5338319B2/en
Timestamp: 2020-01-21 02:50:03
Document Index: 454269701

Matched Legal Cases: ['arts 22', 'arts 22', 'arts 22', 'in fine', 'in fine', 'in fine', 'art 22', 'art 22']

JP5338319B2 - Optical sheet, surface light source device, display device, and optical sheet manufacturing method - Google Patents
Optical sheet, surface light source device, display device, and optical sheet manufacturing method Download PDF
JP5338319B2
JP5338319B2 JP2008553082A JP2008553082A JP5338319B2 JP 5338319 B2 JP5338319 B2 JP 5338319B2 JP 2008553082 A JP2008553082 A JP 2008553082A JP 2008553082 A JP2008553082 A JP 2008553082A JP 5338319 B2 JP5338319 B2 JP 5338319B2
JP2008553082A
JPWO2008084744A1 (en
聡 浜田
純一 澤登
2007-01-09 Priority to JP2007000961 priority Critical
2007-01-09 Priority to JP2007000961 priority
2007-12-28 Application filed by 大日本印刷株式会社 filed Critical 大日本印刷株式会社
2007-12-28 Priority to PCT/JP2007/075299 priority patent/WO2008084744A1/en
2007-12-28 Priority to JP2008553082A priority patent/JP5338319B2/en
2010-04-30 Publication of JPWO2008084744A1 publication Critical patent/JPWO2008084744A1/en
2013-11-13 Publication of JP5338319B2 publication Critical patent/JP5338319B2/en
An optical sheet is structured to have a translucent substrate 12, an optical element 16 provided on one surface S1 of the translucent substrate 12, on which a plurality of unit prisms 14 or unit lenses are arranged, and a light diffusion layer provided between the one surface S1 and the optical element 16 and/or on another surface S2 of the translucent substrate 12, and at least one of the light diffusion layer 18 includes gap parts 22 as a light diffusion element. At this time, the gap parts 22 is preferably in an approximately oval shape oriented in a uniaxial direction in plan view.
The present invention relates to an optical sheet, a surface light source device, and a display device. More specifically, an optical sheet suitably used for a backlight surface light source device that illuminates a translucent display body from the back, such as a liquid crystal display device or an advertising board, a surface light source device having the optical sheet, And a display device having the surface light source device.
In recent liquid crystal display devices, surface light source devices for illuminating a liquid crystal display device from the back are required to be thin and light as required for low power consumption, thinning and lightening. The light from the light source is effectively used to reduce the power consumption of the light source. As a surface light source device used for such a liquid crystal display device, an edge light type surface light source device and a direct type surface light source device are known.
An edge-light type surface light source device usually enters light source light from one end face of a plate-shaped light guide such as a transparent acrylic resin, and a liquid crystal panel or the like from a light exit surface as one surface of the light guide. The light is emitted to the back surface. In this surface light source device, a light reflecting plate or a light reflecting film is provided on the surface opposite to the light exit surface of the light guide to improve the light utilization efficiency. In addition, a light diffusion sheet is provided on the light exit surface side of the light guide to make the emitted light uniform. On the other hand, a direct type surface light source device is configured by disposing a liquid crystal panel and a reflection plate in a state in which a light source is sandwiched. Usually, the light source light is reflected by the reflection plate to the back surface of the liquid crystal panel, and the front surface of the liquid crystal panel. The light is diffused by the light diffusing sheet disposed on the substrate to make the emitted light uniform.
In such edge light type and direct type surface light source devices, an optical sheet comprising a plurality of unit prisms is arranged on the light exit surface of the light guide, and the optical sheet transmits light from the surface light source device to the liquid crystal panel. Refracted and transmitted to the display body side. However, such an optical sheet may cause luminance nonuniformity such as uneven luminance fringes due to the light from the surface light source device, luminance unevenness due to visual recognition of the light source image, or repeated patterns of light and dark. However, the liquid crystal display device provided with the above has a problem that the image is likely to be disturbed due to the non-uniform brightness.
In order to solve such a problem, the following Patent Document 1 proposes an optical sheet having minute irregularities on a smooth surface opposite to a plurality of unit prism surfaces, and this optical sheet receives light from a surface light source device. There arises a problem that the original function of the optical sheet, which improves the luminance by condensing in the normal direction of the light exit surface, is deteriorated. Therefore, Patent Documents 2 and 3 below propose an optical sheet, a surface light source device, and a transmissive display device that can suppress the generation of interference fringes without causing a decrease in luminance on the light exit surface side. This optical sheet is obtained by arranging a plurality of unit prisms on the surface of a translucent substrate and covering the back surface with a coating layer made of a translucent material. Many micro hill-like projections are provided on the surface opposite to the material, and in Patent Document 3, spherical beads are included in the coating layer to provide a micro-projection shape. This suppresses uneven brightness.
Japanese Patent Laid-Open No. 7-151909 Japanese Patent Laid-Open No. 10-300908 JP-A-11-133214
However, in the current situation in which development competition for recent high-quality liquid crystal display devices is intensifying, even if any of the optical sheets of Patent Documents 2 and 3 is used, there is a decrease in luminance. However, the problem of improving the degree of “blurring” and suppressing nonuniform luminance due to the occurrence of interference fringes or the like is not necessarily sufficient, and further improvement is required.
The present invention has been made to solve the above-described problems, and its purpose is to improve the degree of “blurring” in a state in which a decrease in luminance is suppressed as much as possible, and to reduce the luminance caused by occurrence of interference fringes and the like. It is in providing the optical sheet which can suppress nonuniformity. Another object of the present invention is to provide a surface light source device having such an optical sheet and a display device including the surface light source device.
An optical sheet of the present invention for solving the above-mentioned problems is provided with a light-transmitting substrate, and an optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the light-transmitting substrate. A light diffusing layer provided between the one surface and the optical element and / or on the other surface of the translucent substrate, and at least one surface of the light diffusing layer. The provided light diffusion layer has a gap as a light diffusion element.
According to this invention, it is provided on at least one surface of the light diffusion layers provided between one surface of the translucent substrate and the optical element and / or on the other surface of the translucent substrate. Since the light diffusion layer thus formed has a gap as a light diffusion element, the light incident on the light diffusion layer is refracted or reflected at the interface of the gap acting as the light diffusion element. Since the refractive index of the gap is approximately 1, diffusion of light occurs effectively due to refraction or reflection at the interface of the gap, and the degree of “blurring” can be increased as a whole. “Brightness nonuniformity” such as uneven brightness fringes due to light from the apparatus, uneven brightness due to visual recognition of the light source image, or repeated patterns of light and darkness can be suppressed.
Further, the optical sheet according to the present invention includes a translucent base material in which a gap as a light diffusing element is formed in the vicinity of one surface or from one surface to the other surface, and the translucent material An optical sheet configured to include an optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the substrate may be used.
As a preferred embodiment of the optical sheet of the present invention, the light diffusion layer having the void portion is formed by extending a transparent resin layer in which fine particles are dispersed uniaxially or biaxially. The optical sheet is configured to have a flat shape extending in a direction perpendicular to the normal line of the optical sheet.
According to the present invention, the void portion has a flat shape extending in a direction perpendicular to the normal line of the optical sheet in a cross-sectional view. This shape is obtained by uniaxial or biaxially forming the transparent resin layer in which fine particles are dispersed. It can be obtained by stretching on the axis. In addition, since the gap portion is a flattened flat shape extending in a direction perpendicular to the normal line of the optical sheet, for example, the radius of curvature (R) of the end portion of the gap portion is smaller than that of a non-crushed spherical shape. It is a small form. At the interface at these end portions, the light incident on the light diffusion layer can be diffused greatly. As a result, an optical sheet with high diffusibility is obtained.
If the fine particles at this time are translucent particles, the void formed around the fine particles is also made of transparent air, so that the light incident on the light diffusion layer is the fine particles and the It penetrates without being absorbed by the surrounding voids. As a result, the incident light on the optical sheet can be transmitted to the optical element side without being attenuated, and the optical element is deflected to the viewer side, so that a decrease in luminance can be suppressed as much as possible.
As a preferred embodiment of the optical sheet of the present invention, the gap portion may be configured to have a substantially elliptical shape oriented in a uniaxial direction in plan view, or the gap portion may be substantially circular in plan view. It may be configured.
According to the present invention, the gap portion of any form can improve the light diffusibility in the gap portion (particularly the end portion of the gap portion) as described above, and becomes an optical sheet with high diffusibility.
As another preferred embodiment of the optical sheet of the present invention, light of the transmitted light that is incident on the optical sheet excluding the optical element parallel to the normal line of the optical sheet and that is transmitted through the optical sheet. When diffusivity is measured, the light diffusivity measured on a plurality of virtual lines orthogonal to the normal line of the optical sheet is configured to be anisotropic.
According to the present invention, since the light diffusibility measured on a plurality of virtual lines orthogonal to the normal line of the optical sheet is anisotropic, when the optical sheet is combined with an arbitrary light source, the anisotropic property is obtained. Therefore, it is possible to solve the conventional problem of non-uniform brightness by utilizing the diffusion characteristics.
In the other aspect, when the light diffusibility of the anisotropic optical sheet is represented by a light diffusion curve represented by a luminance and a diffusion angle, a half width obtained from the light diffusion curve is obtained. Of these, the direction in which the imaginary line showing the maximum half-value width extends is a direction orthogonal to the major axis direction of the substantially elliptical cavity oriented in a uniaxial direction in plan view.
According to the present invention, the extending direction of the imaginary line showing the maximum half-value width among the half-value widths obtained from the light diffusion curve (that is, the direction in which the maximum diffusion characteristic is exhibited) is aligned in a uniaxial direction in plan view. Although the direction is perpendicular to the major axis direction of the substantially elliptical void portion, the coincidence or approximate coincidence of these directions is caused by the shape of the substantially elliptical void portion. Specifically, the substantially elliptical void portion achieves high diffusibility at the end portion having a small radius of curvature (R), but the ratio of the end portion is that of the substantially elliptical void portion 22 oriented in the uniaxial direction. This is due to the fact that the direction perpendicular to the longitudinal direction is larger than the case parallel to the long axis direction.
Further, in the other aspect, when the light diffusibility of the anisotropic optical sheet is represented by a light diffusion curve represented by luminance and a diffusion angle, the half width obtained from the light diffusion curve It is preferable that the direction in which an imaginary line showing the maximum half-value width extends and the ridge line direction of the unit prism or unit lens constituting the optical element are orthogonal or substantially orthogonal.
When a direct-type backlight unit is configured by arranging a plurality of cold cathode tubes on the back surface of the optical sheet, the longitudinal direction of the cold cathode tubes and the ridge line direction of the unit prism or unit lens included in the optical element are usually parallel. Alternatively, although arranged so as to be substantially parallel, according to the present invention, the direction in which the light diffusion layer exhibits the maximum diffusion characteristic (the direction in which the virtual line indicating the maximum half-value width extends) and the above-described ridge line direction are Since it is configured to be orthogonal or substantially orthogonal, it is possible to prevent the occurrence of stripe-like luminance unevenness derived from the direct type backlight unit. This aspect is an aspect in which the ridge line direction of the unit prism or unit lens is parallel or substantially parallel to the major axis direction of the substantially elliptical cavity oriented in one axis direction.
Further, in the other aspect, when the light diffusibility of the anisotropic optical sheet is represented by a light diffusion curve represented by luminance and a diffusion angle, the half width obtained from the light diffusion curve It is preferable that the direction in which an imaginary line showing the maximum half-value width extends and the ridge line direction of the unit prism or unit lens constituting the optical element are parallel or substantially parallel.
Unlike the above aspect, when an edge light type backlight unit is provided in which a light guide is disposed on the back surface of an optical sheet and a linear light source is provided on the side end surface of the light guide, the longitudinal direction of the linear light source is usually used. Are arranged so that the ridge line direction of the unit prism or unit lens included in the optical element is parallel or substantially parallel. According to the present invention, the direction in which the light diffusion layer exhibits the maximum diffusion characteristics (maximum half The illuminating line in the width direction of the linear light source derived from the edge-light type backlight unit is generated since the ridge line direction) and the ridge line direction are configured to be parallel or substantially parallel to each other. Can be prevented. This aspect is an aspect in which the ridge line direction of the unit prism or unit lens is orthogonal or substantially orthogonal to the major axis direction of the substantially elliptical cavity oriented in one axis direction.
As still another preferred embodiment of the optical sheet of the present invention, linear light is incident on the optical sheet excluding the optical element in parallel to the normal line of the optical sheet, and the linear light is transmitted through the optical sheet. When the light diffusivity is measured, the light diffusivity measured on a plurality of virtual lines orthogonal to the normal line of the optical sheet is isotropic.
According to the present invention, the light diffusibility measured on a plurality of virtual lines orthogonal to the normal line of the optical sheet is isotropic. Therefore, when this optical sheet is combined with an arbitrary light source, the isotropic diffusion is performed. It becomes possible to solve the conventional problem of non-uniform luminance by utilizing the characteristics.
In the optical sheet of the present invention, the image sharpness value measured by the method defined in JIS K 7374 of the optical sheet excluding the optical elements is 15 or less at a slit pitch of 0.5 mm, and in JIS K 7361-1. The haze value measured by the prescribed method is preferably 20% or more and 95% or less.
According to the present invention, since the light diffusion layer having the void portion as the light diffusion element is provided, the optical sheet in the form excluding the optical element (that is, the light diffusion having the void portion on the translucent substrate) The image sharpness value of the layer formed) is 15 or less at a slit pitch of 0.5 mm, and the haze value of the optical sheet in an aspect excluding the light diffusion element is 20% or more and 95% or less. Can be configured. Such an optical sheet can suppress the non-uniformity of luminance described above in a state in which a decrease in luminance is suppressed as much as possible.
A surface light source device according to a first aspect of the present invention for solving the above-described problems is made of a light-transmitting material, and guides light introduced from at least one side end surface from a light emission surface that is one surface. An optical sheet that is provided on a light emitting surface of the light guide, is provided on the light emitting surface of the light guide, and transmits light emitted from the light emitting surface. A light source device comprising: a light-transmitting base material; and an optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the light-transmitting base material. An element, and a light diffusion layer provided between the one surface and the optical element and / or on the other surface of the translucent substrate, and at least one of the light diffusion layers The light diffusion layer provided on the surface has a gap as a light diffusion element, That.
A surface light source device according to a second aspect of the present invention for solving the above-described problem includes a translucent substrate and a plurality of unit prisms or unit lenses provided on one surface of the translucent substrate. An optical element, and a light diffusion layer provided between the one surface and the optical element and / or on the other surface of the translucent substrate, The light diffusion layer provided on at least one of the surfaces, an optical sheet having a void as a light diffusion element,
A light source that emits light from the back side of the optical sheet;
And a reflector disposed on a side opposite to the optical sheet of the light source and reflecting light from the light source toward the optical sheet.
According to the first and second aspects of the present invention, light is transmitted between one surface of the translucent substrate constituting the optical sheet and the optical element and / or on the other surface of the translucent substrate. Since a light diffusion layer having a gap as a diffusion element is provided, light from the light source enters the optical sheet from the light emission surface of the light guide, and is refracted at the interface of the gap in the light diffusion layer. reflect. Since the refractive index of the air gap is approximately 1, diffusion of light refracted or reflected at the interface of the air gap occurs effectively, and the degree of “blurring” is improved as a whole, resulting in uneven brightness. Can be suppressed.
In addition, in the case where fine particles are used for forming the void portion of the light diffusion layer, if the fine particles are translucent particles, the light incident on the light diffusion layer is not absorbed by the fine particles. Since the light is transmitted, the light incident on the optical sheet can be transmitted to the optical element side without being attenuated. As a result, the transmitted light is deflected to the viewer side by the optical element, so that a decrease in luminance can be suppressed as much as possible.
In the surface light source device according to the first and second aspects of the present invention, the optical element constituting the optical sheet may be provided on the light emission side of the light source, or the light source It may be configured so as to be provided on the light incident side from.
Instead of the optical sheet according to the first and second aspects, the surface light source device according to the present invention has a gap as a light diffusing element in the vicinity of one of the surfaces or from one surface to the other surface. An optical sheet having a formed translucent base material and an optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the translucent base material is used. It may be.
The display device of the present invention for solving the above-described problems is a planar light-transmitting display body and the book that is disposed on the back surface of the light-transmitting display body and that irradiates light from the back surface. A surface light source device according to the invention.
According to the present invention, since the surface light source device according to the present invention is used as the light source of the display device, the light source image and the interference fringes are visually recognized, and the light output unevenness from the light source and the light guide is visually recognized. It is possible to suppress the non-uniformity of the luminance distribution on the display surface caused by the above, and to supply high-luminance illumination light with high uniformity to the display panel side. As a result, it is possible to realize a display device in which the degree of image quality is improved without lowering the luminance, particularly a recent high-quality liquid crystal display device.
According to the optical sheet of the present invention, since the light diffusion can be effectively caused by the presence of the gap as the light diffusing element of the light diffusing layer, the degree of “blurring” of the optical sheet can be reduced as a whole. For example, it is possible to suppress “non-uniform luminance” such as uneven luminance fringes caused by light from the surface light source device, luminance unevenness due to visual recognition of the light source image, or repeated bright and dark patterns.
According to the surface light source device of the present invention, since the optical sheet having the above-described effect is provided, it is particularly preferable as a surface light source device for a recent high-quality liquid crystal display device, and the above-described non-uniform luminance is not accompanied by a decrease in luminance. It is possible to provide a surface light source device that suppresses the conversion.
According to the display device of the present invention, since the surface light source device having the above-described effects is provided, the display caused by the fact that the light source image and the interference fringes are visually recognized, or the unevenness in light emission from the light source and the light guide is visually recognized. Since the luminance distribution on the surface can be suppressed and high-luminance illumination light with high uniformity can be supplied to the display panel, the image quality can be reduced without lowering the luminance. An improved display device, particularly a recent high-quality liquid crystal display device can be realized.
Hereinafter, embodiments of an optical sheet, a surface light source device, and a display device of the present invention will be described in detail with reference to the drawings. However, the present invention is not limited to the following description and drawings, and is within the scope of the gist of the present invention. Various modifications can be made.
First, the optical sheet will be described. 1 to 3 are schematic perspective views showing examples of the optical sheet of the present invention. The optical sheet 10 (10A, 10B, 10C) of the present invention is provided on the translucent base material 12 and one surface S1 of the translucent base material 12, as shown in FIGS. An optical element 16 in which a plurality of unit prisms 14 or unit lenses (see reference numerals 16A and 16B in FIG. 12) are arranged, and between the one surface S1 and the optical element 16, and / or a translucent substrate. 12 and the light diffusion layer 18 provided on the other surface S2. And the light-diffusion layer 18 provided in at least one surface (S1 or S2) among the light-diffusion layers 18 has many space | gap parts 22 as a light-diffusion element. Hereinafter, the components of the optical sheet 10 of the present invention will be described in detail.
The translucent substrate 12 is a main constituent member of the optical sheet 10 and functions as a substrate of the optical element 16 described in detail later, and transmits most of the light from the light source to the optical element 16 side. Act on. The light-transmitting substrate 12 may be a light-transmitting substrate made of a material such as resin, glass, ceramics, and a substrate having a transmittance of 85% or more as a single substrate is particularly preferably used. In addition, the transmittance | permeability here is the value measured, for example with the light transmittance meter (model: HM-150) by Murakami Color Research Laboratory Co., Ltd. etc. Although the thickness of the translucent base material 12 is not specifically limited, Usually, it exists in the range of 50 micrometers-500 micrometers.
Examples of the translucent substrate 12 made of a resin material include polyester resins such as polyethylene terephthalate, polybutylene terephthalate, and polyethylene naphthalate, acrylic resins such as polymethyl methacrylate, polycarbonate resins, polystyrene resins, and polymethylpentene resins. Consists of a resin obtained by curing an ionizing radiation curable resin comprising an oligomer such as a thermoplastic resin, polyester acrylate, urethane acrylate, epoxy acrylate and / or an acrylate monomer with electromagnetic radiation such as ultraviolet rays or electron beams, etc. A transparent base material can be mentioned preferably. Further, as the translucent substrate 12 made of glass, soda glass, borosilicate glass, or the like is used.
The translucent substrate 12 may be produced by coextrusion together with a light diffusion layer 18 described later, or may be produced by other methods. The translucent base material 12 produced by coextrusion or the translucent base material 12 produced by other methods is stretched in a state having the light diffusion layer 18. The stretching process may be a biaxial stretching process or a uniaxial stretching process. By subjecting the translucent substrate 12 having the light diffusion layer 18 to stretching treatment, the void portion 22 which is a characteristic configuration of the present invention can be formed, and details thereof will be described later.
(Light diffusion layer)
FIG. 4 is an enlarged cross-sectional view of the optical sheet shown in FIG. FIG. 5 is an enlarged cross-sectional view of the light diffusion layer, and FIG. 6 is an enlarged plan view of the light diffusion layer. The light diffusing layer 18 is a characteristic configuration of the present invention, and as shown in FIGS. 5 and 6, is a layer having a large number of voids 22 as light diffusing elements. Such a light diffusion layer 18 may be provided between one surface S1 of the translucent substrate 12 and the optical element 16 as in the optical sheet 10A shown in FIG. Like the sheet 10B, it may be provided on the other surface S2 of the translucent substrate 12, or like the optical sheet 10C shown in FIG. It may be provided both between the element 16 and on the other surface S2 of the translucent substrate 12. 6A is an example in the case where the planar view shape of the gap portion 22 included in the light diffusion layer 18 is substantially elliptical, and FIG. 6B is a plan view of the void portion 22 included in the light diffusion layer 18. It is an example in case a visual shape is substantially circular.
As the resin material 19 constituting the light diffusion layer 18, the same transparent resin material as that of the translucent substrate 12 can be preferably exemplified. Specifically, polyester resins such as polyethylene terephthalate, polybutylene terephthalate, polyethylene naphthalate, ethylene-terephthalate-isophthalate copolymer, ethylene glycol-1,4-cyclohexanedimethanol-terephthalic acid copolymer, polymethyl (meta ) Acrylic resin such as acrylate, polybutyl (meth) acrylate, methyl (meth) acrylate-butyl (meth) acrylate copolymer, methyl (meth) acrylate-styrene copolymer (here, “(meth) acrylate” And acrylate or methacrylate.), Polycarbonate resins, polystyrene resins, polymethylpentene resins, thermoplastic urethane resins and other thermoplastic resins, polyester (meth) acrylates, urethane Ionizing radiation curable resins comprising oligomers such as (meth) acrylates and epoxy (meth) acrylates and / or (meth) acrylate monomers such as trimethylolpropane tri (meth) acrylate and dipentaerythritol hexa (meth) acrylate And resins cured with electromagnetic radiation such as ultraviolet rays or electron beams. In particular, the use of a resin material that can be coextruded with the above-described translucent substrate 12 is convenient in production. The refractive index of the resin material 19 constituting the light diffusion layer 18 is usually about 1.45 to 1.60.
The light diffusion layer 18 illustrated in FIGS. 5 and 6 is configured to have fine particles 20 and voids 22 existing around the fine particles 20 in the resin material 19. The light diffusing layer 18 having such a form is formed by, for example, coextruding a transparent resin in which fine particles 20 are dispersed together with the resin material forming the light transmissive substrate 12 or on the light transmissive substrate 12. Then, they can be formed by stretching uniaxially or biaxially. The large number of voids 22 can represent the degree of formation with a density per unit area when viewed in plan. Based on the results of examples described later, for example, 10 to 3000 per cm 2 in plan view It can be said that it is preferable.
In the case where a large number of voids 22 are formed by stretching, the fine particles 20 are blended so as to be almost uniformly dispersed in the resin material constituting the light diffusion layer 18. The fine particles 20 may be light-transmitting fine particles that are generally used for optical sheets. Examples of the fine particles 20 include styrene resin fine particles, silicone resin fine particles, acrylic resin fine particles, and MS resin (methacryl-styrene copolymer resin) fine particles. Examples thereof include inorganic fine particles such as organic fine particles, glass fine particles, and glass beads, and one or more of these can be contained in the resin.
The fine particles 20 preferably have a refractive index equal to or lower than that of the resin material 19 constituting the light diffusion layer 18. If the material of the fine particles 20 is selected, the refractive index can be set to an arbitrary value. However, the refractive index of the fine particles 20 is set to be equal to or less than the refractive index of the resin material 19 constituting the light diffusion layer 18. By forming the light diffusion layer 18, it is possible to effectively cause light diffusion when light incident on the light diffusion layer 18 passes through the fine particles 20. Note that the refractive index of the fine particles 20 may be about 1.45 to 1.60, or less, similar to the resin material 19 constituting the light diffusion layer 18.
The shape of the fine particles 20 is not particularly limited, but generally, a spherical shape such as a spherical shape, a spheroid, or a polyhedron with rounded corners is advantageous in terms of availability. The average particle diameter of the fine particles 20 is preferably 3 μm to 20 μm. The average particle size at this time is obtained by observing the cross section of the light diffusion layer 18 with a microscope, and is represented by an average value of 50 or more measurement samples.
In the present invention, it is preferable that the surface of the fine particles 20 be treated so as not to be compatible with the resin material constituting the light diffusion layer 18. The resin material which comprises the fine particle 20 and the light-diffusion layer 18 by extending | stretching after forming the translucent base material 12 and the light-diffusion layer 18 by coextrusion by giving such a process to the surface of the fine particle 20 is carried out. It is considered that peeling occurs at the interface with the gap 22 and the gap 22 is easily formed. As a result, it is possible to easily form the above-described predetermined gap portion 22 in the light diffusion layer 18.
Next, the shape of the gap 22 will be described in more detail.
The plan view shape of the gap portion 22 may be a substantially elliptical shape oriented in a uniaxial direction as shown in FIG. 6 (A), or oriented in a specific direction as shown in FIG. 6 (B). However, as shown in FIG. 5, the cross-sectional shape of the gap portion 22 is orthogonal to the normal line Y of the optical sheet 10, regardless of whether it is uniaxially stretched or biaxially stretched. It has a flat shape that is crushed and extended in the direction X. Here, the “sectional view shape” is a cross-sectional shape of the optical sheet viewed from a direction orthogonal to the normal direction of the optical sheet observing the planar view shape. Further, the “planar shape” means a planar shape obtained by projecting a three-dimensional shape onto a plane orthogonal to the line-of-sight direction.
The voids 22 shown in FIGS. 5 and 6 exist around the fine particles 20. The void portion 22 may exist around the entire circumference of the fine particle 20 or may exist around a part of the fine particle 20. It is preferable that the gap portion 22 exists in as wide a part as possible. Since the gap 22 acts as an air layer, the refractive index thereof is approximately 1. Therefore, the light incident on the light diffusion layer 18 is easily refracted or reflected at the interface between the resin material 19 constituting the light diffusion layer 18 and the gap 22, and light diffusion occurs effectively. Therefore, this gap 22 acts as a result of making the optical sheet 10 as a “blurred state” as a whole, improving the degree of blurring and, for example, equal thickness interference fringes due to light from the surface light source device In addition, it is possible to suppress “brightness non-uniformity” such as luminance unevenness due to visual recognition of a light source image or a repeated pattern of light and dark.
The shape of the gap 22 is not particularly limited, but when formed by a stretching process after coextruding the light transmissive substrate 12 and the light diffusion layer 18, the gap 22 is, as shown in FIG. The contour shape in plan view is substantially elliptical (see FIG. 6A) or substantially circular (see FIG. 6B). The substantially elliptical void 22 shown in FIG. 6A is oriented in a uniaxial direction in a plan view and has a so-called anisotropic (anisotropic) form. On the other hand, the substantially circular gap 22 shown in FIG. 6B is not oriented in a specific direction in plan view, and has a so-called isotropic form. The stretching process is performed in the longitudinal direction and the lateral direction of the sheet. Usually, since stretching in either direction is large, the outline of the gap portion 22 is generally approximately elliptical in a plan view shape as described above. Many of them are as shown in FIG.
FIG. 7 is a schematic diagram for explaining the light diffusibility in the gap included in the light diffusion layer, taking a spherical gap as an example, and FIG. 8 shows the light diffusibility in the fine particles included in the light diffusion layer. FIG. 2 is a schematic diagram illustrating a spherical fine particle as an example. As shown in FIG. 7, the light incident on the light diffusion layer 18 from the normal direction of the translucent substrate (corresponding to the direction from the bottom to the top in FIGS. 7 and 8) has a refractive index of about A large amount of light is refracted at the interface between the resin material 19 of about 1.56 and the gap 22 having a refractive index of about 1.0. On the other hand, in the light diffusion layer that does not have the void portion 22, the refractive index of the resin material 19 is about 1.56 and the refractive index of the fine particles 20 is about 1.49. In addition, it does not refract very much. Therefore, the gap 22 provided in the optical sheet 10 of the present invention can effectively diffuse the light incident on the light diffusion layer 18 from the normal direction.
FIG. 9 is a schematic diagram of a plan view shape of a gap that actually appears after the stretching process. 10 is a cross-sectional view taken along the line AA in FIG. 9, and FIG. 11 is a cross-sectional view taken along the line BB in FIG. The gap 22 that appears after the stretching treatment usually extends in the stretching direction of the translucent substrate 12, has a flat cross section as shown in FIG. 5, and has a plan view shape as shown in FIG. Is substantially elliptic or circular. As shown in FIG. 9, when the length in the major axis direction is “a” and the length in the minor axis direction is “b” when the gap portion 22 is viewed in plan, “a / b” of the gap portion 22 is obtained. "Can be arbitrarily changed depending on the conditions of the stretching treatment. For example, when the void portion 22 is formed by uniaxial stretching, by performing only longitudinal stretching or transverse stretching at a predetermined magnification, the substantially elliptical shape extends in the uniaxial direction as shown in FIG. 6A and is strong. The gap 22 having anisotropy (non-isotropic) can be formed. In addition, it is preferable that the draw ratio at the time of uniaxial stretching is larger than 1 time and about 10 times. On the other hand, when the void portion 22 is formed by biaxial stretching, by performing longitudinal stretching and lateral stretching in that order, transverse stretching and longitudinal stretching in that order, or simultaneously performing longitudinal stretching and transverse stretching at a predetermined magnification, As shown in FIG. 6B, an isotropic substantially circular gap 22 can be formed. In biaxial stretching, the shape of the gap portion 22 can be adjusted by adjusting the stretching ratio in the longitudinal direction and the stretching ratio in the lateral direction, and can be adjusted in a wide range from a circular shape to a substantially circular shape. . In addition, it is preferable that the draw ratio at the time of biaxial stretching is larger than 1 time and about 10 times.
In particular, the light diffusibility of the light diffusing layer 18 is improved by forming the cavity 22 having an approximately elliptic shape that is anisotropic and anisotropic as shown in FIG. 6A in the light diffusing layer 18. Anisotropy can be imparted. As shown in FIG. 10, the substantially elliptical void portion 22 viewed from the major axis direction has a configuration in which the central portion of the upper and lower surfaces (surfaces in the normal direction Y of the translucent substrate) is relatively flat. It has become. Therefore, most of the light that is incident from the normal direction and is refracted and transmitted at the interface of the gap 22 is slightly refracted on the upper and lower surfaces of the relatively flat and long central portion and escapes to the optical element 16 side. On the other hand, the refraction of the light incident on the interface at an angle close to the normal direction y of the optical sheet is large at both ends of the substantially elliptical gap portion 22, and as shown in FIG. Idemitsu. That is, both end portions include the end portion of the gap portion 22 and have a form with a small curvature radius (R), so that incident light is refracted and diffused greatly. Therefore, as shown in FIG. 10, in the major axis direction of the gap portion 22, the light diffusion in the central portion that occupies most is not strong, and can transmit a lot of light without diffusing so much. There is a feature that a certain luminance can be secured.
On the other hand, as shown in FIG. 11, the substantially elliptical void portion 22 as viewed from the minor axis direction has a short central portion on the upper and lower surfaces (surfaces in the normal direction Y of the translucent substrate). It is not flat compared to the case. And the ratio for which the both ends which the refraction of the light which injected into the interface of the angle near the normal line direction y of an optical sheet becomes large occupies becomes relatively large. Therefore, as shown in FIG. 11, the light that is incident from the normal direction and is refracted and transmitted through the gap portion 22 is largely refracted at the end portion, and becomes a large diffused light, and the ratio of light emitted to the left and right is increased. Therefore, as shown in FIG. 11, there is a characteristic that relatively strong light diffusion occurs in the minor axis direction of the gap 22.
When these characteristics are arranged, as shown in FIG. 10, when light is incident on the long-axis cross section of the flat and elliptical gap portion 22, the light is refracted in the long axis direction of the gap portion 22 at both ends. However, it can be said that the length of both end portions contributing to one gap portion 22 is substantially proportional to the length of the short axis. Similarly, as shown in FIG. 11, when light is incident on the short-axis cross section of the flat and elliptical gap portion 22, it contributes to the refraction of light in the short-axis direction of the gap portion 22 at both ends thereof. However, it can be said that the lengths of both end portions contributing to one gap portion 22 are substantially proportional to the length of the major axis. From this, when the shape of the gap portion 22 is elliptical, the component in the minor axis direction of the transmitted light is diffused more strongly, and the light diffusibility can be made anisotropic, in other words, It becomes possible to give anisotropy to the light diffusibility. The anisotropy of the light diffusibility can be controlled by controlling the ratio a / b of the major axis a and the minor axis b of the void portion 22 having an elliptical shape. As the ratio a / b is increased, the diffusible anisotropy can be increased.
The number, shape, size, capacity, and the like of the voids 22 are not particularly limited, but can be arbitrarily adjusted in consideration of desired normal luminance, image sharpness value, haze value, and the like. For example, when it is desired to reduce the value of image definition and increase the degree of blurring, the number, shape, size, capacity, etc. of the gaps 22 can be increased to adjust the light diffusion, When it is desired to increase the value of image definition and reduce the degree of blurring, the number, shape, size, capacity, etc. of the gaps 22 can be reduced to reduce light diffusion. The number of the voids 22 can be adjusted by the number of fine particles 20 to be included in the light diffusion layer 18, and the shape and size of the voids 22 are, for example, when the voids 22 are generated by a stretching process. Depending on whether the stretching process is performed uniaxially or biaxially, the degree of stretching (referred to as the stretching ratio and the degree of stretching) can be adjusted and set. The capacity of the gap 22 can be adjusted by the size of the fine particles 20 and the degree of stretching (stretching degree).
Although the thickness of the light-diffusion layer 18 which consists of such a structure is not specifically limited, Usually, it exists in the range of 5 micrometers-30 micrometers.
The light diffusion layer 18 can be produced by various methods. Preferably, as described above, a resin material in which the fine particles 20 are dispersed is prepared, and the resin material is coextruded with the extrusion material of the translucent substrate 12, or It can apply | coat and can produce the obtained sheet | seat by performing extending | stretching processes, such as uniaxial stretching or biaxial stretching. By this stretching treatment, the interface between the fine particles 20 and the constituent resin of the light diffusion layer 18 is peeled off to form the voids 22.
The optical element 16 is provided on one surface S1 of the translucent substrate 12, and is formed by arranging a plurality of unit prisms 14 or unit lenses (see reference numerals 16A and 16B in FIG. 12 described later). As shown in FIGS. 1 to 3, the optical element 16 may be a prism group in which unit prisms 14 having a triangular prism shape are arranged so that the ridges thereof are parallel to each other, as shown in FIG. As shown in FIG. 12B, the lens group may be formed by arranging a large number of unit lenses 14A having a cylindrical shape with a substantially hemispherical cross section. Alternatively, as shown in FIG. 14B may be an eyelid lens 16B in which a large number are arranged two-dimensionally. These unit prisms 14 or unit lenses 14A and 14B may have a cross-sectional shape such as a circle, ellipse, cardioid, Rankine egg, cycloid, involute curve, or the like, or a triangle, quadrangle, pentagon, or six. Examples thereof include those using a part or the whole of a polygon such as a square. The unit lenses 14A and 14B may be convex lenses as shown in FIG. 12, or concave lenses (not shown).
The optical sheet 10 having the optical element 16 can be used in a single-sheet configuration, but has an optical element 16 in order to control the light diffusion angle in two directions (vertical direction and horizontal direction) using a columnar lens. Two optical sheets 10 may be laminated so that their ridge lines are orthogonal. In this case, it is most preferable that the lens surfaces are oriented in the same direction for both lenses, but the optical element 16 side may be configured to face each other.
As a constituent material of the optical element 16, a homopolymer of (meth) acrylate ester such as poly (meth) acrylate methyl, poly (meth) acrylate butyl, or methyl (meth) acrylate- (meth) acrylic Copolymers of (meth) acrylic acid esters such as acid butyl copolymer (here, “(meth) acrylic acid” means acrylic acid or methacrylic acid), polyethylene terephthalate, polybutylene Polyesters such as terephthalate, thermoplastic resins such as polycarbonate, polystyrene, polymethylpentene, etc., or (meth) acrylates such as polyfunctional urethane (meth) acrylates and polyester (meth) acrylates that are crosslinked with ultraviolet rays or electron beams, unsaturated For transparent resin such as polyester, transparent glass, transparent ceramics, etc. It is. In addition, the thickness from the lens top part of the optical element 16 to the plane part is usually about 20 μm to 1000 μm.
As a method for forming the optical element 16, for example, a known hot press method (Japanese Patent Laid-Open No. 56-157310), an embossing of the shape of a unit prism or unit lens with a roll emboss plate on an ultraviolet curable thermoplastic resin film. After that, the film is cured by irradiating with ultraviolet rays (Japanese Patent Laid-Open No. 61-156273), and the ultraviolet or electron beam curable resin liquid is applied on the rotating roll intaglio engraved with the shape of the unit prism or unit lens. After applying and filling the recesses, the film-shaped translucent substrate is coated on the roll intaglio via the resin liquid and cured by irradiation with ultraviolet rays or electron beams, and then they are released from the roll intaglio, A method of forming the shape of a roll intaglio unit prism or unit lens on a film-like translucent substrate (JP-A-3-223388, US Pat. No. 45) Mention may be made of the 6850 issue, etc.), and the like.
The translucency required for the optical element 16 may be a level that does not hinder the use of each application and is preferably colorless and transparent. However, depending on the application, it may be colored and transparent or matte translucent. Here, the matte transparency refers to a property that diffuses and transmits transmitted light almost uniformly and isotropically in all directions within a half solid angle, and is used as a synonym for light isotropic diffusibility.
According to the optical sheet 10 of the present invention composed of such components, between the one surface S1 of the translucent substrate 12 and the optical element 16 and / or on the other surface S2 of the translucent substrate 12. Since the light diffusion layer 18 having the gap portion 22 as a light diffusion element is provided, the light incident on the light diffusion layer 18 is refracted or reflected at the interface of the gap portion 22. Since the refractive index of the air gap portion 22 is approximately 1, the presence of the air gap portion 22 effectively diffuses light, resulting in an overall “blurred state” and uneven brightness due to interference fringes and the like. Can be suppressed.
When the light diffusing layer 18 includes translucent fine particles 20, the light incident on the light diffusing layer 18 is transmitted without being absorbed by the fine particles 20. As a result, incident light can be transmitted to the optical element 16 side without being attenuated as much as possible, so that a reduction in luminance can be suppressed as much as possible.
(Relationship between light diffusivity of light diffusion layer and optical elements)
In the optical sheet of the present invention, the gap 22 having the form shown in FIG. 6A can be formed to make the light diffusion property anisotropic, or the gap having the form shown in FIG. The portion 22 may be formed to make the light diffusibility isotropic.
Here, as shown in FIG. 6 (A), “anisotropic light diffusibility” means that the light diffusion layer 18 having a substantially elliptical shape in which the plan view shape of the gap portion 22 is oriented in a uniaxial direction is used. It is a characteristic that appears when it is provided. This anisotropic light diffusibility can be confirmed by measuring the optical sheet 10 excluding the optical element 16. Specifically, the optical element 16 constituting the optical sheet 10 of the present invention is scraped to eliminate the function of the optical element 16, or the same material as that of the optical element 16 or a transparent material having the same refractive index is applied onto the optical element 16. An optical sheet after the function of the optical element 16 is eliminated (hereinafter, such an optical sheet is referred to as a “base sheet”), linear light is incident in parallel to the normal line of the base sheet, and the linear light is incident. The light diffusibility can be confirmed by measuring the light diffusibility of the transmitted light transmitted through the base sheet. In this case, the base sheet having the light diffusing layer 18 having a substantially elliptical shape in which the plan view shape of the gap portion 22 is aligned in the uniaxial direction is a light diffusivity measured on a plurality of imaginary lines orthogonal to the normal line. Is higher in a certain direction and is anisotropic.
If the light diffusivity at this time is represented by a light diffusion curve represented by luminance and diffusion angle, the direction in which the imaginary line indicating the maximum half-value width of the half-value width obtained from the light diffusion curve extends (that is, the maximum The direction in which the diffusion characteristic is exhibited) coincides with or substantially coincides with the direction orthogonal to the major axis direction of the gap portion 22 formed of a substantially elliptical shape oriented in one axis direction in plan view. The coincidence or substantially coincidence of these directions is caused by the shape of the gap portion 22 having a substantially elliptical shape. Specifically, as described above, the substantially elliptical gap portion 22 has a small curvature radius (R). The end portion (contour portion) achieves high diffusibility, but the proportion of the end portion is orthogonal to the case of being parallel to the major axis direction of the substantially elliptical void portion 22 oriented in one axis direction. This is due to the fact that is growing.
On the other hand, “isotropic light diffusibility” refers to a light diffusion layer 18 having a substantially circular shape in which the plan view shape of the gap 22 does not extend significantly in a specific direction, as shown in FIG. This is a characteristic that appears when This isotropic light diffusibility can be confirmed by measuring the optical sheet 10 excluding the optical element 16. Specifically, as described above, the optical element 16 constituting the optical sheet 10 of the present invention is scraped to eliminate the function of the optical element 16, or the same material as that of the optical element 16 or a transparent material having the same refractive index is applied onto the optical element 16. For example, a base material sheet after the function of the optical element 16 is eliminated is formed, linear light is incident parallel to the normal line of the base material sheet, and the transmitted light is transmitted through the base material sheet. By measuring the diffusibility, the light diffusibility can be confirmed. In this case, the base sheet having the light diffusing layer 18 in which the shape of the gap 22 in plan view is a substantially circular shape is isotropic with no significant difference in light diffusibility measured on a plurality of virtual lines orthogonal to the normal line. It has become.
If the light diffusivity at this time is represented by a light diffusion curve represented by luminance and diffusion angle, the half width obtained from the light diffusion curve is not significantly different in each virtual line. This is due to the shape of the substantially circular gap portion 22. Specifically, even in the substantially circular gap portion 22, the end portion (contour portion) having a small curvature radius (R) realizes high diffusibility. However, this is because the ratio of the end portions is isotropic.
13 and 14 are configuration diagrams illustrating the relationship between the optical element and the light diffusion layer provided in the optical sheet of the present invention and the light source combined with the optical sheet of the present invention. FIG. 13 is a configuration diagram in the case of combining a direct type backlight unit as a light source, and FIG. 14 is a configuration diagram in the case of combining an edge light type backlight unit as a light source. Since the optical sheet 10 of the present invention can have light diffusibility anisotropy (isotropic light diffusibility), the types of light sources to be combined as shown in FIGS. 13 and 14 It can be arbitrarily applied depending on the case. For example, when the light source has directional brightness unevenness, the unevenness of brightness can be canceled by applying the optical sheet 10 of the present invention to increase the diffusivity in the direction of the brightness unevenness of the light source. Unevenness can be blurred efficiently.
As shown in FIG. 13, when a direct-type backlight unit is configured by arranging a light source 34 composed of a plurality of cold cathode tubes on the back surface of the optical sheet 10, the longitudinal direction H of the cold cathode tubes and the optical elements are usually The unit prism 14 (or unit lens) included in 16 is arranged so that the ridge line direction G is parallel or substantially parallel. In such a case, as shown in FIG. 13, when the light diffusibility of the base sheet 13 having the anisotropic light diffusion layer 18 is represented by a light diffusion curve represented by luminance and diffusion angle, The direction F of the imaginary line showing the maximum half-value width among the half-value widths obtained from the light diffusion curve and the ridge line direction G of the unit prism 14 (or unit lens) constituting the optical element 16 are orthogonal or substantially orthogonal. It is preferable to configure so as to.
The direct type backlight unit configured as described above has a direction F in which the light diffusion layer 18 exhibits the maximum diffusion characteristics (that is, a direction in which an imaginary line indicating the maximum half-value width extends) and a ridge line direction of the unit prism 14. Since G is configured to be orthogonal or substantially orthogonal, it is possible to more effectively prevent the occurrence of striped luminance unevenness derived from the light source 34 including a cold cathode tube or the like that constitutes the direct type backlight unit. it can.
On the other hand, as shown in FIG. 14, when the light guide 32 is arranged on the back surface of the optical sheet 10 and the linear light source 34 is provided on the side end face 32A of the light guide 32, an edge light type backlight unit is configured. Usually, the linear light source 34 is arranged so that the longitudinal direction H of the linear light source 34 and the ridge line direction G of the unit prism 14 (or unit lens) included in the optical element 16 are parallel or substantially parallel. In such a case, as shown in FIG. 14, when the light diffusibility of the base sheet 13 having the anisotropic light diffusion layer 18 is represented by a light diffusion curve represented by luminance and diffusion angle, The extending direction F of the imaginary line showing the maximum half width among the half widths obtained from the light diffusion curve and the ridge line direction G of the unit prism 14 (or unit lens) constituting the optical element 16 are parallel or substantially parallel. It is preferable to constitute so that.
The edge light type backlight unit configured as described above includes a direction F in which the light diffusion layer 18 exhibits the maximum diffusion characteristic (that is, a direction in which an imaginary line indicating the maximum half-value width extends), and a ridge line of the unit prism 14. Since the direction G is configured to be parallel or substantially parallel, it is possible to prevent luminance unevenness generated in the width direction (longitudinal direction H) of the linear light source 34 derived from the light source structure of the edge light type backlight unit.
As described above, the positional relationship between the light diffusing layer 18 having anisotropic light diffusibility and the optical element 16 is arranged corresponding to the light source to be used, so that the luminance nonuniformity derived from the light source structure is uneven. It becomes possible to solve the problem of conversion.
In the above description, the ridge line direction G of the unit prisms 14 is a direction orthogonal to the arrangement direction J of the unit prisms 14. In addition, in the above, the direction F in which the light diffusion layer 18 exhibits the maximum diffusion characteristic (that is, the direction in which the imaginary line indicating the maximum half-value width extends) is the gap 22 made of a substantially elliptical shape oriented in the uniaxial direction. It is a direction orthogonal to the major axis direction. Further, in the above, the light diffusibility is measured by removing the optical element 16 from the completed optical sheet 10, but in the manufacturing process of the optical sheet 10, as shown in the examples described later, the optical element 16 The light diffusibility of the base material sheet 71 (the sheet that has been stretched and also formed with the voids 22) is measured to confirm the light diffusibility anisotropy and isotropy.
(Characteristics of optical sheet)
The optical sheet 10 of the present invention composed of the above components is an optical sheet excluding the optical element 16 (that is, a “base sheet in which a light diffusion layer 18 having a gap 22 is formed on a light-transmitting base 12”. 13 ”(see FIG. 13 and FIG. 14). The image sharpness value measured by the method defined in JIS K 7374 is 15 or less, preferably 10 or less at a slit pitch of 0.5 mm, and JIS K 7361. It is preferable that the haze value measured by the method prescribed | regulated by -1 is 20% or more and 95% or less. Since the optical sheet 10 of the present invention and the substrate sheet 13 constituting the optical sheet 10 include the light diffusion layer 18 having the gap portion 22 as a light diffusion element, the optical sheet 10 should have optical characteristics within the above range. The obtained optical sheet 10 is a bright and sufficiently bright optical sheet. The value of image definition and the haze value can be adjusted mainly by the size of the gap 22 constituting the light diffusion layer 18 and the like. Further, the normal luminance will be described later in Examples, but it was obtained by comparison as a relative value with respect to the conventional optical sheet, and preferably 96% when the conventional optical sheet is 100%. The above is preferable.
The value of the image definition is not a value obtained by measuring the obtained optical sheet 10, but a base sheet (that is, a base formed by forming the light diffusion layer 18 having the gap portion 22 on the translucent substrate 12. The base material sheet 13 or the base material sheet 13 after the optical element 16 is removed from the optical sheet 10 is measured by a method defined in JIS K 7374, for example, 0.125 mm, 0.5 mm. , 1.0 mm, 2.0 mm, and other slit plates with slits of arbitrary width are arranged in front of the light receiving unit, and the light emitted from the light source is transmitted through the slit plate out of the light passing through the measurement object. It is the result of having measured the ratio of the light which did. The smaller the image sharpness value, the better the degree of blurring and the occurrence of brightness non-uniformity due to interference fringes, etc., but the greater the value, the lower the degree of blurring and the luminance due to interference fringes etc. Inhomogeneity occurs. Moreover, haze value uses the light transmittance meter (Murakami Color Research Laboratory Co., Ltd. make, model: HM-150) about the test piece which cut out the center part of the base material sheet 13 by 60 mm square, and is JIS-K-. It is the result measured according to 7361-1. Further, the normal luminance is a result measured by a minute declination luminance meter which is a device for measuring the luminance for each light emission angle, and the larger the value, the brighter it looks.
In the above description, the optical sheet excluding the optical element 16 is the same as the base sheet 13 or the optical element 16 after the optical element 16 constituting the optical sheet 10 is scraped to eliminate the function of the optical element 16. The base sheet 13 after the function of the optical element 16 is eliminated by applying a material or a transparent material having the same refractive index onto the optical element 16 can be exemplified.
In the optical sheet 10, a light diffusion layer (not shown) may be provided on the surface opposite to the optical element 16 (sometimes referred to as the other surface S2). For example, when the light diffusion layer 18 as shown in FIG. 3 is formed on both surfaces S1 and S2 of the optical sheet 10, a mode in which a light diffusion layer is provided instead of the light diffusion layer 18 on the back surface S2 side can be exemplified. Such a light diffusion layer only needs to have an action of diffusing light, and is formed on a general light diffusion sheet. For example, a layer in which light diffusing fine particles having a particle diameter of 1 μm to 30 μm are dispersed in a resin, for example, the same one proposed in Patent Documents 2 and 3 can be applied.
The light diffusing layer is formed by applying a paint in which light diffusing fine particles are dispersed in a translucent binder resin by spray coating, roll coating, or the like. As the material for the light diffusing fine particles, polymethyl methacrylate (acrylic) beads, polybutyl methacrylate beads, polycarbonate beads, polyurethane beads, calcium carbonate beads, silica beads and the like are used. As the translucent binder resin, a transparent material such as acrylic, polystyrene, polyester, or vinyl polymer is used. The thickness of the light diffusion layer is usually in the range of 1 μm to 20 μm.
The optical sheet 10 can be manufactured by various methods. For example, after preparing the sheet-like translucent base material 12, the light diffusion layer 18 is formed on one side or both sides thereof, or they are simultaneously formed by two-layer extrusion or the like, and then the optical element 16 is formed. Can be obtained. When the translucent substrate 12 and the light diffusing layer 18 are formed separately, for example, after the sheet-like translucent substrate 12 is extruded, a light diffusion layer forming resin liquid is applied to one or both sides thereof. The light diffusion layer 18 can be formed by drying, and then stretched to form the light diffusion layer 18 having the voids 22 around the fine particles 20, and then the optical element 16 can be formed and manufactured. Moreover, when forming the translucent base material 12 and the light-diffusion layer 18 simultaneously, for example, after extruding two sheet-like translucent base materials 12 and the light-diffusion layer 18 and forming simultaneously, extending process is carried out. Thus, the light diffusion layer 18 having the voids 22 around the fine particles 20 can be formed, and then the optical element 16 can be formed and manufactured.
The optical element 16 is, for example, a thermoplastic resin hot press method, an injection molding method, or a cast molding method of a curable resin by ultraviolet rays or heat, as disclosed in JP-A-56-157310. Can be manufactured. As another manufacturing method, for example, an ionizing radiation curable resin liquid is applied to a shaping roll having a shaping mold of the optical element 16 having a desired lens arrangement as disclosed in JP-A-5-1699015. The light transmissive base material 12 on which the light diffusion layer 18 after the stretching treatment is formed is layered thereon and irradiated with ionizing radiation such as ultraviolet rays and electron beams as it is from the light transmissive base material 12 side. The ionizing radiation curable resin liquid is cured. Then, the optical sheet 10 in which the optical element 16 made of the cured ionizing radiation curable resin is formed can be manufactured by peeling them from the shaping roll.
(Other aspects of optical sheet)
In the above description, as a representative form of the optical sheet 10 of the present invention, the translucent substrate 12 and the light diffusion layer 18 are clearly separate layers as shown in FIGS. . Moreover, the example which forms the translucent base material 12 and the light-diffusion layer 18 as a separate layer by methods, such as a melt coextrusion method, also illustrates the manufacturing method. However, the present invention is not limited to such a form. That is, the above-mentioned "providing a light diffusion layer on one surface and / or the other surface of the translucent substrate" means that at least one surface and / or the other surface of the translucent substrate. This means that at least the vicinity of the surface may be a light diffusion layer specific to the present invention.
Therefore, in the originally single-layer translucent base material, a void portion may be included in the vicinity of one of the surfaces. Furthermore, in the originally single-layer translucent base material, a void portion may be continuously contained from one surface to the other surface. In this case, in other words, it can be said that the optical element is directly laminated on any one surface of the single light diffusion layer.
In summary, the optical sheet according to the present invention includes a translucent base material in which a gap as a light diffusing element is formed in the vicinity of one surface or from one surface to the other surface, and the transparent substrate. An optical sheet configured to have an optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the optical base material may be used. Also in the optical sheet of this aspect, the constituent elements are the same as the constituent elements of the optical sheet already described with reference to FIGS. 1 to 4, and have the same effects as the optical sheet.
FIG. 15 is a perspective view showing an example of the surface light source device according to the first aspect of the present invention. The surface light source device 30 according to the first aspect of the present invention is a so-called edge light type surface light source device, and guides light introduced from at least one side end surface 32A from a light emitting surface 32B as one surface. A light source 32, a light source 34 for allowing light to enter the inside from at least one side end surface 32A of the light guide 32, and a light emission surface 32B of the light guide 32, are emitted from the light emission surface 32B. It has the optical sheet 10 according to the present invention that transmits light.
The light guide 32 is a plate-like body made of a translucent material, and is configured to emit light introduced from the left side end surface 32A in FIG. 15 from the upper light emission surface 32B. The light guide 32 is made of a light-transmitting material similar to the material of the optical sheet 10, but is usually made of acrylic or polycarbonate resin. The thickness of the light guide 32 is usually about 1 μm to 10 mm, and the thickness may be constant over the entire range, or as shown in FIG. 15, it is the thickest at the position of the side end face 32A on the light source 34 side. The taper shape may be gradually thinned in the opposite direction.
In order to emit light from a wide surface (light emission surface 32B), the light guide 32 preferably has a light scattering function added to the inside or the surface thereof.
The light source 34 causes light to enter the inside from at least one side end face 32 </ b> A of the light guide 32, and is disposed along the side end face 32 </ b> A of the light guide 32. The light source 34 is not limited to a linear light source as shown in FIG. 15, and point light sources such as incandescent bulbs and LEDs (light emitting diodes) may be arranged in a line along the side end face 32A. . A plurality of small flat fluorescent lamps may be arranged along the side end face 32A.
The light emitting surface 32B of the light guide 32 is provided with the above-described optical sheet 10 according to the present invention. Normally, the optical sheet 10 is provided on the light emitting surface 32B, but the form is not particularly limited. The optical sheet 10 is provided so that the opposite surface of the optical element 16 becomes the light emission surface 32 </ b> B of the light guide 32. The details of the optical sheet 10 have already been described and will not be described here.
The light reflecting plate 36 is provided on a surface opposite to the light emitting surface 32B of the light guide 32 and is provided on a side end surface other than the left side end surface 32A, and reflects and guides light emitted from these surfaces. This is for returning to the light body 32. As the light reflection plate 36, a thin metal plate deposited with aluminum or the like, or white foamed PET (polyethylene terephthalate) is used.
FIG. 16 is a perspective view showing an example of a surface light source device according to the second aspect of the present invention. The surface light source device 40 according to the second aspect of the present invention is a direct-type surface light source device, and irradiates light from the optical sheet 10 according to the present invention and the opposite surface of the optical sheet 10 on the optical element 16 side. The light source 34 has a concave reflector 44 that is disposed on the opposite side of the optical sheet as viewed from the light source 34 and reflects the light from the light source 34 toward the optical sheet 10. The details of the optical sheet 10 have already been described and will not be described here.
The light from the light source 34 is transmitted through the optical sheet 10 toward the light emitting surface 42 on the optical sheet 10 side, and the light transmitted through the optical sheet 10 toward the light emitting surface 42 after being reflected by the reflector 44. is there.
The light reflecting plate 44 is formed by depositing aluminum or the like on a thin metal plate, white foamed PET (polyethylene terephthalate), or the like, as in the surface light source device of the first aspect. The shape of the light reflection plate 44 is not particularly limited as long as the light from the light source 34 can be uniformly reflected as a parallel light beam, and a concave arc shape, a parabolic columnar shape, a hyperbolic columnar shape, an elliptical columnar shape, or the like is selected.
FIG. 17 is a perspective sectional view showing another example of the surface light source device according to the first and second aspects of the present invention. FIG. 17A shows another example of the surface light source device according to the first aspect. B) shows another example of the surface light source device according to the second aspect. The surface light source device 30 ′ shown in FIG. 17A is different from the surface light source device 30 of FIG. 15 described above in the direction of the optical element 16 constituting the optical sheet 10, and the optical element 16 is a light source 34. Alternatively, it may be provided on the side from which light is emitted toward the optical sheet 10, that is, on the light emission surface 32 </ b> B side of the light guide 32. Further, the surface light source device 40 ′ shown in FIG. 17B is different from the surface light source device 40 in FIG. 16 described above in the direction of the optical element 16 constituting the optical sheet 10, and constitutes the optical sheet 10. The optical element 16 may be provided on the side from which light is emitted from the light source 34 toward the optical sheet 10, that is, on the light emission surface 42 side on the optical sheet 10 side.
In addition, as another aspect of the surface light source device according to the present invention, for example, instead of the optical sheet 10 according to the aspect shown in FIGS. 1 to 4, either near one surface or from one surface to the other surface. A translucent base material in which a gap portion as a light diffusing element is formed, and an optical element provided on one surface of the translucent base material, in which a plurality of unit prisms or unit lenses are arranged. A surface light source device using an optical sheet may be used.
18 and 19 are schematic perspective views showing examples of a liquid crystal display device as a display device of the present invention. A liquid crystal display device 50 shown in FIG. 18 includes a liquid crystal panel 52 that is a flat light-transmitting display, and an edge according to the present invention that is disposed on the back surface of the liquid crystal panel 52 and that irradiates light from the back surface. And a light-type surface light source device 30. Similarly, the liquid crystal display device 60 shown in FIG. 19 is also arranged on the back surface of the liquid crystal panel 62 that is a flat light-transmitting display body, and the book that irradiates the liquid crystal panel 62 with light from the back surface. And a direct-type surface light source device 40 according to the invention. The liquid crystal display devices 50 and 60 are transmissive liquid crystal display devices including backlight surface light source devices 30 and 40, and each pixel forming a liquid crystal screen is illuminated from the back side by light emitted from the surface light source devices 30 and 40. Is configured to do. Note that as the surface light source device, the surface light source devices 30 ′ and 40 ′ having the modes shown in FIGS. 17A and 17B may be applied.
The liquid crystal display devices 50 and 60 have the surface light source devices 30 and 40 according to the present invention as constituent members, and the surface light source devices 30 and 40 have a normal line having a base sheet with a small image definition value. The optical sheet 10 with high brightness is provided. As a result, the liquid crystal display devices 50 and 60 can obtain good luminance and can form a good image because luminance nonuniformity due to interference fringes does not occur.
A polyethylene terephthalate (hereinafter referred to as “PET”) resin having a refractive index of 1.56 is used as an extruded resin for forming a light-transmitting substrate, and a PET resin having a refractive index of 1.56 is used as an extruded resin for forming a light diffusion layer. The two layers were put into a co-extrusion apparatus and subjected to two-layer extrusion. The extruded resin for forming the light diffusion layer is obtained by dispersing 20 parts by weight of fine particles 20 made of a polyester resin having an average particle diameter of 20 μm and a refractive index of 1.56 in the above-mentioned PET resin material. The obtained sheet was subsequently stretched by a stretching apparatus, and the thickness after the treatment was 163 μm for the PET resin base material as the translucent base material 12 and 25 μm for the light diffusion layer 18. In this way, a base sheet 71 including the light diffusion layer 18 in which the predetermined gap portion 22 was formed was produced. In addition, the extending | stretching process used the extending | stretching apparatus, and biaxially extended with the degree of extending | stretching (8/4) in the elongate direction and the width direction of the bilayer extrusion sheet | seat. The average dimension of the formed gap portion 22 is 160 μm in the length a in the major axis direction when the gap portion 22 is viewed in plan, and is 80 μm in the length b in the minor axis direction when the gap portion is viewed in plan view. It was.
The base material sheet 71 thus manufactured is put into the manufacturing apparatus 70 shown in FIG. 20, and the optical element 16 is formed on the surface (referred to as “back surface” in Table 1) on the side where the light diffusion layer 18 is not provided ( (See FIG. 2). First, a winding roll 72 for the base sheet 71 obtained as described above was prepared. On the other hand, a shaping roll 73 in which a triangular unit prism shaping die 76 is formed on the surface of a metal cylinder is prepared, and an ultraviolet curable resin liquid is fed from a T-die nozzle 74 while rotating around the central axis. 80 was supplied to the shaping roll surface and filled in the shaping die 76 of the unit prism. Next, the base sheet 71 is unwound from the winding roll 72 at a speed synchronized with the rotational peripheral speed of the shaping roll 73, and the base sheet 71 is placed on the shaping roll 73 by the pressing roll 81. In this state, ultraviolet rays from the ultraviolet irradiation devices 82 and 82 are irradiated from the substrate sheet 71 side, and the resin liquid 80 is crosslinked and cured in the shaping mold 76 at the same time. The sheet 71 was adhered. Next, the base sheet 71 traveling using the peeling roll 83 was peeled off together with the optical element 16 adhered thereto to obtain the optical sheet 10 having the form shown in FIG. 1 in which a plurality of triangular unit prisms were arranged. The unit prism has a triangular shape. Specifically, the unit prism is an isosceles triangle having a pitch of 50 μm and a cross section of the unit prism having an apex angle of 85 °, and is arranged adjacently so that the ridge lines are parallel to each other. It formed so that it might become. Further, in Example 1, the optical element 16 was formed by arranging the shaping roll so that the ridge line direction G of the unit prism and the major axis direction of the gap portion 22 were parallel to each other.
As shown in Table 1 described later, the obtained optical sheet 10 had a normal luminance of 96.4% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 45.9%, and the value of the image definition was 3.1 when measured with a 0.5 mm slit. The normal luminance is a value obtained by measuring the obtained optical sheet, but the haze value and the image sharpness value are not values obtained by measuring the obtained optical sheet. A material sheet 71 (that is, a base material sheet 71 formed by forming a light diffusion layer on a translucent base material) is measured.
The optical sheet of Example 2 was produced in the same manner as Example 1. The optical sheet of Example 2 was produced so as to improve the normal luminance while maintaining the same image definition value as that of Example 1. The normal luminance of the obtained optical sheet was 97.2% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 36.2%, and the value of the image definition was 3.2 when measured with a 0.5 mm slit. Such adjustment of the characteristics was performed by adjusting the size of the gap 22 and the particle size and content of the fine particles 20 in the light diffusion layer 18.
The optical sheet of Example 3 was produced in the same manner as Example 1. The optical sheet of Example 3 was prepared so as to make the image definition value larger than that of Example 1 and to further improve the normal luminance. The normal luminance of the obtained optical sheet was 99.7% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 20.1%, and the value of the image definition was 8.9 when measured with a 0.5 mm slit. Such adjustment of the characteristics was performed by adjusting the size of the gap 22 and the particle size and content of the fine particles 20 in the light diffusion layer 18.
In the same manner as in Example 1 , the optical sheet of Reference Example 1 was produced. The optical sheet of Reference Example 1 was prepared so as to make the value of image definition the same as that of Example 1 and to make the space 22 is circular and to make light diffusivity isotropic. The normal luminance of the obtained optical sheet was 99.7% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 14.2%, and the value of the image definition was 9.2 as measured with a 0.5 mm slit. The shape and characteristics of the void portion 22 were adjusted by adjusting the longitudinal / lateral stretching ratio and the particle size and content of the fine particles 20 in the light diffusion layer 18. In addition, as for the average dimension of the space | gap part 22, when the space | gap part 22 was planarly viewed, all the orthogonal length was 24 micrometers, and it was substantially circular shape.
The optical sheet of Reference Example 1 has a circular shape of the gap portion 22 and shows isotropic light diffusivity as in Comparative Examples 1 to 4 described later, but it can also be seen from the results in Table 1 below. In particular, the image sharpness was good.
An optical sheet of Example 4 was produced in the same manner as Example 1. In the optical sheet of Example 4 , unit prisms are arranged on the surface opposite to Example 1 of the base sheet 71 produced in Example 1 (that is, the surface on which the light diffusion layer 18 is formed). (See FIG. 1). The normal brightness of the obtained optical sheet was 96.3% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%.
An optical sheet of Example 5 was produced in the same manner as Example 1. The optical sheet of Example 5 is obtained by rotating the arrangement direction of the unit prisms of the base sheet 71 produced in Example 1 by 90 degrees. In order to obtain this optical sheet, a shaping roll 73 in which the direction of the shaping pattern on the surface was rotated by 90 degrees was prepared and used. The normal brightness of the obtained optical sheet was 95.3% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%.
In the same manner as in Example 1, an optical sheet of Reference Example 2 was produced. The optical sheet of Reference Example 2 was prepared by making the shape of the gap portion 22 circular to make the light diffusibility isotropic, and making the gap portion 22 larger than that of Reference Example 1 . The normal brightness of the obtained optical sheet was 98.5% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 23.3%, and the value of the image definition was 12.8 as measured with a 0.5 mm slit.
(Example 6 )
An optical sheet of Example 6 was produced in the same manner as Example 1. The optical sheet of Example 6 is manufactured by making the value of image definition the same as that of Example 1 and changing the shape of the gap portion 22 to be elongated. The normal luminance of the obtained optical sheet was 99.2% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet 71 was 22.8%, and the value of the image definition was 3.5 when measured with a 0.5 mm slit.
An optical polyethylene terephthalate film (Toyobo, A4300) having a refractive index of 1.56 and a thickness of 188 μm is coated with mat ink (polyester resin mixed with acrylic fine particles having a particle size of 5 μm) and a mat layer having a thickness of 8 μm. The base material sheet which has this was produced. The base sheet thus prepared was put into the manufacturing apparatus 70 shown in FIG. 20 in the same manner as in Example 1, and the optical element 16 was formed on the surface opposite to the side on which the mat layer was formed. Was made. In preparing the base sheet, the manufacturing conditions were adjusted so that the haze value was about 28% to 32%. The haze value of the obtained base material sheet was 29.3%, and the image sharpness value of the base material sheet was 22.5 as measured with a 0.5 mm slit.
A base sheet was prepared by coating in the same manner as in Comparative Example 1. The base material sheet of Comparative Example 2 was prepared so that a haze value equivalent to that of Example 1 was obtained. The haze value was adjusted by increasing the content of acrylic fine particles contained in the mat ink (see Table 1). In the same manner as in Example 1, the base material sheet thus prepared was put into the manufacturing apparatus 70 shown in FIG. 20, and the optical element 16 was formed on the surface opposite to the side on which the mat layer was formed, so that the optical sheet of Comparative Example 2 was manufactured. did. The haze value of the obtained base material sheet was 46.2%, and the image sharpness value of the base material sheet was 17.2 when measured with a 0.5 mm slit.
In the same manner as Comparative Example 1, an optical sheet of Comparative Example 3 was produced. The optical sheet of Comparative Example 3 was prepared using 20 μm acrylic fine particles to be included in the mat ink, and the density of particles per unit area was approximately the same as the density of the voids in Example 1. . The normal luminance of the obtained optical sheet was 93.4% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Moreover, the haze value of the base material sheet was 12.7%, and the image sharpness value was 42.1 as measured with a 0.5 mm slit.
In the same manner as in Comparative Example 1, an optical sheet of Comparative Example 4 was produced. The optical sheet of Comparative Example 4 was prepared by using 80 μm acrylic fine particles to be included in the mat ink, and the density of particles per unit area was approximately the same as the density of the voids in Example 1. . The normal luminance of the obtained optical sheet was 94.8% as a relative value when the optical sheet of Comparative Example 1 was taken as 100%. Further, the haze value of the base sheet was 10.8%, and the image sharpness value was 59.8 as measured with a 0.5 mm slit.
The light diffusion layer 18 constituting the obtained optical sheet is observed in plan view with a micrograph, and the density per unit area of the voids 22 in the light diffusion layer 18 (pieces / cm 2 ) and the size of the voids 22. (Short axis diameter μm / Long axis diameter μm) was measured.
The normal luminance is a device that measures the luminance at each light emission angle, using a small declination luminance meter (manufactured by Topcon, model: BM-7), using a light table that emits isotropic diffused light as a light source, The measurement was performed under the measurement condition of a viewing angle of 1 degree. At this time, the normal luminance of the optical sheet of Comparative Example 1 was set to 100% based on the luminance values measured for the optical sheets of Examples 1 to 6, Reference Examples 1 and 2, and Comparative Examples 1 to 4. The normal brightness of the optical sheets of Examples 1 to 6, Reference Examples 1 and 2, and Comparative Examples 2 to 4 were calculated as relative values. The results are shown in Table 1. The normal luminances of the optical sheets of Examples 1 to 6 and Reference Examples 1 and 2 were all 95% or higher (relative to Comparative Example 1). In addition, the total light transmittance in Table 1 was measured using a light transmittance meter (manufactured by Murakami Color Research Co., Ltd., model: HM-150).
The haze value was measured using the optical sheet 10 excluding the optical element 16, that is, the base material sheet 71 in which the light diffusion layer 18 having the gap 22 was formed on the translucent base material 12. Is. About the test piece which cut out the center part of the base material sheet 71 by 60 mm square, it measured according to JIS-K-7361-1 using the light transmittance meter (Murakami Color Research Laboratory make, model: HM-150). . The results are shown in Table 1.
The value of the image definition is measured on the optical sheet 10 excluding the optical element 16, that is, the base material sheet 71 in which the light diffusion layer 18 having the gap 22 is formed on the translucent base material 12. It is a sample. For measurement, using a image clarity measuring instrument (manufactured by Suga Test Instruments Co., Ltd., model: ICM-1DP), according to JIS-K-7374, transmission measurement, measurement angle 0 °, optical comb (slit width: 2.0 mm, 1.0 mm, 0.5 mm, and 0.125 mm). If the evaluation of the image sharpness value is described in the case of a slit width of 0.5 mm, for example, if the value is 15 or less, the degree of blurring is large, and the occurrence of luminance unevenness due to interference fringes or the like can be suppressed. When the value is in the range of 20 to 40, the degree of blurring is moderate, and uneven brightness due to interference fringes or the like may be visually recognized. When the value exceeds 50, the degree of blurring is low, and the interference fringes are low. Luminance non-uniformity due to etc. is visually recognized. Moreover, it measured similarly about the optical sheet of Comparative Examples 1-4. The results are shown in Table 1.
For light diffusivity, a three-dimensional gonio system (manufactured by Optec) was used to measure the diffusion characteristics when the incident light angle was changed from 0 ° to ± 10 °. As for the vertical angle of view (γV), the diffusion characteristics in the vertical direction of the respective base material sheets 71 produced in Example 1, Reference Example 2 and Comparative Example 4 were measured. 1, the diffusion property in the horizontal direction of each base sheet 71 produced in Reference Example 2 and Comparative Example 4 was measured. The results are shown in FIG. 21 and FIG.
21 and 22 show the relative luminance in the vertical and horizontal directions with the base sheet 71 produced in Example 1, Reference Example 2 and Comparative Example 4 as samples, and the front luminance of each as 100%. The relationship between angle and angle is shown. The “diffusion characteristic” here refers to the light diffusibility in the vertical direction and the horizontal direction represented by a light diffusion curve composed of luminance and diffusion angle. The diffusion characteristics shown in FIG. 21 indicate the light diffusibility in the vertical direction. The term “vertical direction” here refers to a substantially elliptical shape oriented so as to extend long in one axial direction when the substrate sheet 71 is viewed in plan view. This is a direction parallel to the long axis direction of the gap portion formed in the shape. On the other hand, the diffusion characteristic of FIG. 22 shows the light diffusibility in the horizontal direction. The “horizontal direction” here is oriented so as to extend long in one axial direction when the base sheet 71 is viewed in plan. This is a direction orthogonal to the major axis direction of the substantially elliptical void.
As can be seen from Table 1, the base material sheet used in Comparative Example 4 contains fine particles having a particle size of 80 μm and does not contain voids. On the other hand, the base material sheet 71 used in Reference Example 2 has an isotropic gap of 80 μm, and the base material sheet 71 used in Example 1 is anisotropic with a short diameter / long diameter = 80 μm / 160 μm. It has a gap. 21 and 22 show the light diffusibility of each of these base material sheets, the light diffusion curve (also referred to as a relative luminance distribution curve) in the base material sheet of Comparative Example 4 is the vertical direction shown in FIG. Both the horizontal curve shown in FIG. 22 and the horizontal curve shown in FIG. 22 show diffusion characteristics having a narrow angle range (small half-value width). The light diffusion curve in the base material sheet of Reference Example 2 shows both the vertical curve shown in FIG. 21 and the horizontal curve shown in FIG. ing. On the other hand, the light diffusion curve in the base material sheet of Example 1 shows diffusion characteristics having an aspect of a wider angle range (large half width) in the vertical curve shown in FIG. The horizontal curve shows the diffusion characteristic having an aspect of an angle range narrower than that of the reference example 2 . The reason for this is that although Reference Example 2 containing isotropic voids shows better light diffusibility than Comparative Example 4 containing isotropic particles, the voids of Reference Example 2 and the particles of Comparative Example 4 are used. Since both are isotropic shapes, the diffusion characteristics are almost the same in both vertical and horizontal directions. On the other hand, in Example 1 including an anisotropic gap, the difference in diffusion characteristics between the vertical direction and the horizontal direction was very significant. This indicates that, as already described, it depends on the relationship between the direction in which the substantially elliptical void portion is oriented and the diffusion characteristics.
In addition, in this application, the half value width obtained from the light diffusion curve is the width of the diffusion angle when the relative luminance is 50% in FIG. 21, and thus, for example, in the base material sheet of Example 1 The horizontal direction that is the measurement direction of the diffusion characteristics shown in FIG. 22 is the “direction in which the imaginary line showing the maximum half-value width among the half-value widths obtained from the light diffusion curve extends” in the present invention, and “plane The direction perpendicular to the major axis direction of the substantially elliptical void portion oriented in the uniaxial direction when viewed.
The optical sheets 10 of Examples 1 to 6 and Reference Examples 1 and 2 according to the present invention have a clear image with a haze value in the range of 20% to 95% from the results of Table 1 and the diffusion characteristics of FIGS. When the value of the degree was, for example, a 0.5 mm slit, the value was 15 or less. Further, the normal luminance was 95% or more (relative value to Comparative Example 1), which was a high value. As a result, if a surface light source device having an optical sheet is used as a backlight member of a liquid crystal display device, uneven brightness due to interference fringes or the like can be suppressed while maintaining sufficient brightness for an observer.
Table 2 shows a case where a direct type backlight unit and an edge light type backlight unit are prepared, and the optical sheets of Example 1, Example 5 and Comparative Example 2 are mounted on the respective backlight units. It is an evaluation result of luminance unevenness appearance.
At this time, in both cases of using the direct type backlight unit and the edge light type backlight unit, the ridge line direction of the unit prism of each optical sheet and the cold cathode tube as the light source of each backlight unit Was set to be parallel to the longitudinal direction (see FIGS. 13 and 14). On the other hand, the major axis direction of the substantially elliptical shape of the gap portion 22 of the light diffusion layer 18 and the ridge line direction of the unit prism of each optical sheet are parallel to each other when the direct type backlight unit is used. In the case where the light unit was used, they were arranged so as to be orthogonal.
From the results of Table 2, the brightness unevenness was clearly confirmed in all cases where the optical sheet of Comparative Example 2 was used, but the brightness unevenness was improved when the optical sheets of Examples 1 and 5 were used. In particular, when the optical sheet of Example 1 is applied to a direct type backlight unit and when the optical sheet of Example 5 is applied to an edge light type backlight unit, the effect of improving luminance unevenness is the highest. confirmed.
It is a typical perspective view which shows an example of the optical sheet of this invention. It is a typical perspective view which shows another example of the optical sheet of this invention. It is a typical perspective view which shows another example of the optical sheet of this invention. It is an expanded sectional view of the optical sheet shown in FIG. It is an expanded sectional view of a light diffusion layer. It is an enlarged plan view of a light diffusion layer. It is a schematic diagram explaining the light diffusibility in the space | gap part contained in a light-diffusion layer by taking the spherical space | gap part as an example. It is a schematic diagram explaining the light diffusibility in the fine particle contained in a light-diffusion layer by using a spherical fine particle as an example. It is a schematic diagram of the planar view shape of the space | gap part which actually appears after extending | stretching process. It is AA sectional drawing of FIG. It is BB sectional drawing of FIG. It is a typical perspective view which shows the other example of a form of an optical element. It is a block diagram explaining the relationship between the optical element with which the optical sheet of this invention is equipped, a light-diffusion layer, and the light source combined with the optical sheet of this invention. It is a block diagram explaining the relationship between the optical element and the light-diffusion layer with which the optical sheet of this invention is equipped, and the other light source combined with the optical sheet of this invention. It is a perspective view which shows an example of the surface light source device which concerns on the 1st aspect of this invention. It is a perspective view which shows an example of the surface light source device which concerns on the 2nd aspect of this invention. It is a perspective sectional view showing other examples of the surface light source device concerning the 1st and 2nd modes of the present invention. It is a schematic perspective view which shows an example of the liquid crystal display device as a display apparatus of this invention. It is a schematic perspective view which shows another example of the liquid crystal display device as a display apparatus of this invention. It is a typical block diagram which shows an example of the manufacturing apparatus for forming an optical element on a base material sheet. It is a measurement result of the diffusion characteristic of the perpendicular direction of a substrate sheet. It is a measurement result of the spreading | diffusion characteristic of the horizontal direction of a base material sheet.
DESCRIPTION OF SYMBOLS 10, 10A, 10B, 10C ... Optical sheet 12 ... Translucent base material 13, 71 ... Base material sheet 14 ... Unit prism 14A, 14B ... Unit lens 16, 16B, 16C ... Optical element 18 ... Light-diffusion layer 19 ... Resin Material 20 ... Fine particles 22 ... Gaps 30, 30 ', 40, 40' ... Surface light source device 32 ... Light guide 32A ... Side end surface 32B ... Light emitting surface 34 ... Light source 36, 44 ... Light reflectors 50, 60 ... Liquid crystal display device 52, 62 ... Liquid crystal panel S1 ... One surface of translucent substrate S2 ... Other surface of translucent substrate X ... Direction orthogonal to normal of optical sheet Y ... Normal of optical sheet a ... the length in the major axis direction when the gap portion is viewed in plan b ... the length in the minor axis direction when the gap portion is seen in plan view F ... the direction in which the virtual line showing the maximum half-value width extends G ... the unit prism or unit Lens ridge direction H ... Linear Light source width direction (longitudinal direction)
J: Unit prism arrangement direction
A translucent base material, an optical element provided on one surface of the translucent base material, in which a plurality of unit prisms are arranged, and between the one surface and the optical element, and / or A light diffusion layer provided on the other surface of the translucent substrate,
The light diffusion layer provided on at least one surface of the light diffusion layer has fine particles and voids as light diffusion elements formed around the fine particles,
The gap is substantially oval oriented in a uniaxial direction in plan view,
The substantially elliptical shape has a short axis diameter and a long axis diameter,
The minor axis diameter is 1.2 times or more and 4.0 times or less with respect to the average particle diameter of the fine particles, and the major axis diameter is 4.0 times or more with respect to the average particle diameter of the fine particles, 8.0 times or less, and the average particle size of the fine particles is in the range of 3 μm to 20 μm,
An optical sheet characterized in that the image sharpness measured by the method defined in JIS K 7374 of the optical sheet excluding the optical element is 15 or less at a slit pitch of 0.5 mm.
A translucent base material having fine particles in the vicinity of one surface or from one surface to the other surface and voids as light diffusing elements formed around the fine particles, and the translucent material An optical element formed by arranging a plurality of unit prisms or unit lenses provided on one surface of the conductive substrate;
The light diffusing layer having the void is formed by extending a uniaxial or biaxial transparent resin layer in which fine particles are dispersed, and the void is perpendicular to the normal line of the optical sheet in a sectional view. a flat shape extending in the optical sheet according to claim 1 or 2.
When the optical sheet excluding the optical element is incident with linear light parallel to the normal line of the optical sheet, and the light diffusivity of the transmitted light transmitted through the optical sheet is measured, the optical sheet The optical sheet according to any one of claims 1 to 3 , wherein light diffusivity measured on a plurality of virtual lines orthogonal to the normal is anisotropic.
When the light diffusibility of the anisotropic optical sheet is represented by a light diffusion curve represented by luminance and diffusion angle, it indicates the maximum half-value width among the half-value widths obtained from the light diffusion curve. 5. The optical sheet according to claim 4 , wherein the direction in which the imaginary line extends is a direction orthogonal to the major axis direction of the gap portion formed of a substantially elliptical shape oriented in a uniaxial direction in plan view.
When the light diffusibility of the anisotropic optical sheet is represented by a light diffusion curve represented by luminance and diffusion angle, it indicates the maximum half-value width among the half-value widths obtained from the light diffusion curve. The direction in which the virtual line extends;
The optical sheet according to claim 4 or 5 , wherein the ridge line direction of the unit prism or unit lens constituting the optical element is configured to be orthogonal or substantially orthogonal.
The optical sheet according to claim 4 or 5 , wherein the optical sheet is configured such that a ridge line direction of a unit prism or a unit lens constituting the optical element is parallel or substantially parallel.
The optical sheet according to any one of claims 1 to 7 , wherein the optical sheet excluding the optical element has a haze value measured by a method defined in JIS K 7361-1 of 20% or more and 95% or less.
A light guide made of a light-transmitting material and emitting light introduced from at least one side end surface from a light emission surface which is one surface; and light from the at least one side end surface of the light guide to the inside. A light source to be incident and an optical sheet according to any one of claims 1 to 8 , which is provided on a light emission surface of the light guide and transmits light emitted from the light emission surface. A surface light source device.
When the light diffusibility of the optical sheet is represented by a light diffusion curve represented by luminance and diffusion angle, a direction in which an imaginary line showing the maximum half-value width among the half-value widths obtained from the light diffusion curve extends The surface light source device according to claim 9 , wherein a longitudinal direction of the light source is parallel or substantially parallel.
The optical sheet according to any one of claims 1 to 8 ,
A surface light source device, comprising: a reflector disposed on a side opposite to the optical sheet of the light source and reflecting light from the light source toward the optical sheet.
When the light diffusibility of the optical sheet is represented by a light diffusion curve represented by luminance and diffusion angle, a direction in which an imaginary line showing the maximum half-value width among the half-value widths obtained from the light diffusion curve extends The surface light source device according to claim 11 , wherein a longitudinal direction of the light source is orthogonal or substantially orthogonal.
The surface light source device according to any one of claims 9 to 12 , wherein an optical element constituting the optical sheet is provided on a light emission side of the light from the light source.
The optical elements constituting the optical sheet is provided on the incident side of light from the light source, surface light source device according to any one of claims 9-12.
The planar light-transmitting display body and the surface light source device according to any one of claims 9 to 14 , which is disposed on a back surface of the light-transmitting display body and irradiates light from the back surface. A display device comprising:
It is a manufacturing method of an optical sheet given in any 1 paragraph of Claims 1 and 3-8 ,
And the resin for the transparent base formation, a step of co-extruding a resin for forming a light diffusion layer obtained by dispersing fine particles,
And a step of stretching the co-extruded resin to form the void portion.
JP2008553082A 2007-01-09 2007-12-28 Optical sheet, surface light source device, display device, and optical sheet manufacturing method Expired - Fee Related JP5338319B2 (en)
JP2007000961 2007-01-09
PCT/JP2007/075299 WO2008084744A1 (en) 2007-01-09 2007-12-28 Optical sheet, planar light source device, and display device
JP2008553082A JP5338319B2 (en) 2007-01-09 2007-12-28 Optical sheet, surface light source device, display device, and optical sheet manufacturing method
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JP2008553082A Expired - Fee Related JP5338319B2 (en) 2007-01-09 2007-12-28 Optical sheet, surface light source device, display device, and optical sheet manufacturing method
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WO (1) WO2008084744A1 (en)
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TWI468744B (en) 2015-01-11
WO2008084744A1 (en) 2008-07-17
US20100271840A1 (en) 2010-10-28
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