The invention relates to a surface light source device, in particular a surface light source device used as a backlight in an image display device such as a liquid crystal display device or the like.
Surface light source devices are conventionally used in image display devices such as liquid crystal display devices to illuminate the display panel. These surface light source devices generally comprise a light-emitting unit, a light guide, a reflector, a prism sheet and the like. A conventional surface light source device will now be described with reference to the drawings.
With these conventional surface light source devices, light output from light-emitting unit 1 is diffused upwards by the reflector or the diffusion pattern disposed below the light guide either after being reflected at upper surface 2a or rear surface 2b of the light guide, or without being reflected at all. The angles of the prism, the uneven angles of the diffusion pattern, the dot printing of the diffuse reflectance ink and the like are optically designed to ensure that brightness is increased in the surface direction and that the whole surface is uniformly illuminated with light condensed to an extremely narrow angle on the other surface by the condensing effect of the prisms on light reaching the prism sheet.
However although a light-emitting diode such as a chip-type LED or the like is employed as the point light source in conventional light-emitting units, this type of light-emitting diode has a directionality, as shown in
Now, when using a surface light source device which employs this kind of point light source as the back light for a liquid crystal panel, the effective viewing angle for a screen on the liquid crystal display panel is normally around 30° (±15°). However, with the surface light source device shown in
Thus the purpose of invention is to provide a surface light source device which, as a surface light source device employing a single point light source as the source of light, is capable of outputting light efficiently with little visible unevenness in brightness, particularly with little visible unevenness in brightness when the display screen is viewed from an oblique direction, and moreover which is bright when the screen is observed from front on.
Having made a detailed study of the difficulty, the inventors have found that it can be resolved by positioning a light-diffusing film with directionality beside the light-outputting surface of said light guide. Directionality here means that the degree of diffusion differs with the direction, and unevenness in brightness can be prevented by causing the direction of diffusion of the light-diffusing sheet to appropriately correspond with the direction in which unevenness in brightness occurs.
In other words, the invention relates to the surface light source device cited in (1)-(7) below:
(1) In a surface light source device having a light-emitting unit comprising a point light source and a light guide, a reflecting surface being provided on the reverse side of the light guide and also having a prism pattern, a surface light source characterised in that a directional light-diffusing film which diffuses and allows light to pass, comprising two phases with differing refractive indices, and which in addition to the phase with the greater refractive index including a plurality of regions with a columnar structure extending in the direction of the thickness of the film, has said columnar structure inclined at an angle of more than 5° and less than 60° to the normal direction of the film, is provided beside the light-outputting surface of the light guide in such a way that the direction of diffusion of the directional light-diffusing film is in the same direction as the direction of the unevenness in brightness.
(2) The surface light source device claimed in Claim (1), characterised in that said directional light-diffusing film is made to adhere to said light guide or prism sheet with prism pattern using a light-diffusing adhesion agent containing microparticles with a diameter of 0.1-50 μm.
(3) The surface light source device claimed in Claim (2), characterised in that said light-diffusing adhesion agent contains minute particles with diameters in the range of 1-100 nm whose refractive index is 1.8 or greater.
(4) The surface optical source device claimed in Claims (2) and (3), characterized in that the refractive index of said light-diffusing adhesion agent is 1.55 or greater.
(5) The surface optical source device claimed in any of Claims (1)-(4), characterized in that said columnar structure has a structure such that the refractive index varies gradually along the axis line of said columnar structure.
(6) The surface light source device claimed in any of Claims (1)-(5), characterized in that said light-emitting unit is positioned facing the centre of the end surface of the light guide, the direction of diffusion of said directional light-diffusing film being parallel to the other end.
(7) The surface light source device claimed in any of Claims (1)-(6), characterized in that said light-emitting unit is positioned facing the angled end surface of the light guide, the direction of diffusion of said directional light-diffusing film being directed towards the angle facing the light-emitting unit.
(
(
(
(
(
(
(
(
(
(
(
(
(
(
(
(
(
The invention will now be described in further detail with reference to the drawings.
First of all, the light-emitting unit in an image display device such as a liquid crystal display device or the like may be of any kind as long as it is point light source 11 of the type used as the light source for a conventional backlight. A light-emitting diode (LED) is used which may comprise a variety of materials such as GaP, GaAlAs, and InGaAlP and their variants. In the invention, the light-emitting unit is a point light source comprising a single LED lamp. As shown in
Light guide 12 is a plate-shaped member comprising transparent material with a large refractive index. Any materials used as the material for a conventional light guide will be suitable as materials for the structure of the light guide, but polycarbonate resin and metacrylic resin are particularly preferable from the point of view of their transparency and refractive index. The configuration of the light guide may also be similar to that of conventional ones, and the rear surface (lower surface) 12b of the light guide may also be provided where necessary with an uneven configuration or printed diffusion pattern 12d. Furthermore, as shown in
Any type of reflector may be used providing that it is of a light-reflecting type. Preferred types of reflector include a metal sheet such as aluminium foil or the like, a metal plate or sheet of synthetic resin or the like, or a sheet with vacuum-deposited metal on which a light-reflecting surface of silver, aluminium or the like can be formed on the plate or sheet, but are not limited to these, and any type of reflector used as a reflector in a conventional surface light source device may be used. Where necessary a white diffusion plate may also be used as a reflector. Furthermore, as shown in
The light-diffusing phenomena occurring in this directional light-diffusing film will now be explained with reference to
As described above, with the directional light-diffusing film shown in
It should be noted that it is possible to define the AOV (Angle of View) as a parameter for light diffusion. The smaller the AOV, the less the diffusion characteristics, and light is seen to be transmitted. When a laser light is directed at the film experimentally, light intensity can be measured through 180° by rotating the light-emitting unit. The AOV is defined as the angle of the half width of the profile of the light intensity. The AOV of the light-diffusing film shown in
There is no limitation on the size of the columnar structures in the light-diffusing film, but it is preferable that the range of the diameter be between 10 nm and 100 μm. There is no limitation on the thickness of the film either, but it is generally in the range of approximately 2-100 μm. Moreover, the shape of the columnar structure is not limited to a cylindrical shape, but may of oval or other configuration, and there is no limitation on the size of these shapes. In addition, each of the columnar structures may be positioned regularly or irregularly.
There is no particular limitation on the method of forming the columnar structure for the light-diffusing film, which may be selected from any of the existing conventional methods, but the preferred method is a method which selectively irradiates a radiation-sensitive polymer film to form columnar structures with a high refractive index. Prior to radiation the polymer film and may be a pre-polymer or a monomer, and it may be polymerized where necessary after the radiation using a method such as heating. At this time the preferred method is a method whereby the radiation-sensitive polymer film is irradiated with the radiation at a set angle via a mask with the desired pattern formed on it, and using this method it is possible to form a columnar structure with a gradually varying refractive index at the interface between the columnar structure and the base film. The method of forming the mask may be any method conventionally used. As another method of forming the columnar structure, the radiation beam may be irradiated onto the radiation-sensitive polymer film at a set angle with only the required parts exposed, thus polymerizing the radiation-sensitive polymer film directly without using a mask. There is also a method whereby apertures are formed in the polymer film using a laser beam or another method, with material of a high refractive index being filled into the apertures thereafter. There is no particular limitation on the material for the radiation-sensitive polymer film, but it may for example be a type that employs commercially available material such as DuPont's OMNIDEX (registered trademark) sold as HRF 150 and HRF 600.
The refractive index of lower refractive index region 21 which comprises the base material of the polymer film and the refractive index of the high refractive index region 22 are not limited by the invention, and may be selected as appropriate to the light-diffusing characteristics required, but are preferably in the range of 1.2-1.8, and more preferably in the range 1.35-1.8. Material with a double refractive index is undesirable due to the coloration effect, but material which exhibits double refraction may be used where the double refractive index falls within an acceptable range. It is preferable that the actual material for the base polymer film and high refractive index regions have a high rate of light transmission. The difference between the refractive index of the base material of the polymer film and the high refractive index regions is generally set to be within the range of 0.005-0.2. With a reflective index of less than 0.05, it is not easy to achieve adequate diffusion characteristics. More preferably, it is in the range of 0.005-0.1. The refractive indices of the polymer film base and high refractive index regions may be a so-called step index type which rapidly changes at the interface between the two phases, but the so-called graded index type which form columnar structures having refractive indices that gradually vary is preferable due to the desirable diffusion characteristics.
The three main characteristics of said light-diffusing film can be summarised as follows:
The light-diffusing adhesive agent used in the invention containing microparticles with diameters of 0.1-50 μm will now be described. In the invention, the light-diffusing adhesive agent causes the light-diffusing film and the light guide to adhere together, and is used as it forms light-diffusing adhesive layer 16 in which light is diffused uniformly between the light-diffusing film and the light guide. This kind of light-diffusing adhesive agent can be manufactured using conventional methods known to the art, and is generally manufactured by including a filler within the base resin of the adhesive agent.
Examples of the base resin of the light-diffusing adhesive agent include polyester resins, epoxy resins, polyurethane resins, silicon resins, acrylic resins and the like. These may be used singly or in compounds of two or more. Acrylic resins in particular are superior for their reliable resistance to water, heat and light, have good adhesive power and transparency, being preferable as it is easy to adjust their refractive index to suit the liquid crystal display. Examples of acrylic adhesive agents include acrylic acid and its esters, metacrylic acid and its esters, acrylamide, homopolymers of acryl monomers such as acrylonitrile or copolymers of these, and further copolymers of at least one of said acryl monomers and aromatic vinyl monomers such as vinyl acetate, anhydrous maleic acid and styrene. In particular, with main monomers such as ethylene acrylate, butyl acrylate, 2-ethylhexyl acrylate which express adhesive properties, monomers such as vinyl acetate, acyrlonitrile, acrylamide, styrene, metacrylate, and methyl acrylate which act as cohesive components, copolymers comprising functional monomers such as metacrylic acid, acrylic acid, itaconic acid, hydroxy ethyl acrylate, hydroxy propyl metacrylate, dimethyl amino ethyl metacrylate, acrylamide, methylol acrylamide, glycidyl metacrylate, anhydrous maleic acid which further improve adhesion and provide a starting point for bridging, Tg (the glass transition point) is between −60° C. and −15° C., compounds with a weighted average molecular weight of between 200,000 and 1,000,000 being preferable.
At the same time, as a hardening agent for the light-diffusing adhesive agent, bridging compounds such as metal chelates, isocyanates and epoxies can be used singly or in compounds of two or more as necessary. When containing a filler to be described later, this kind of acrylic adhesive agent will preferably be mixed so as to have an adhesive force in the range of 100-2000 g/25 mm. With an adhesive force of less than 100/25 mm resistance to the environment is impaired, and in particular there is the danger that separation will occur at high temperatures and humidities, yet when greater than 2000 g/25 mm there is the disadvantage that the film cannot be removed and reaffixed, or where it can that the adhesive agent will remain behind. The refractive index of acrylic adhesive agents should preferably be in the range of 1.45-1.70, and in particular in the range of 1.5-1.65.
General examples of the filler which included in the structure of the light-diffusing adhesive agent to diffuse light include white inorganic pigments such as silica, calcium carbonate, aluminium hydrocarbonate, magnesium hydrocarbonate, clay, talc, and titanium dioxide, and transparent or white organic pigments such as acrylic resin, polystyrene resin, epoxy resin, and silicon resin. When selecting an acrylic adhesive agent, silicon beads, epoxy resin beads are preferred as they exhibit superior dispersal with respect to the acrylic adhesive agent, and a uniform and high quality light diffusion can be obtained. The shape of the filler should preferably be round, which permits a uniform diffusion of light.
The diameters of the microparticles of this filler should be in the range of 0.1-50 μm, and preferably between 0.1-20 μm, and more preferably in the range of 0.5 to 10 μm. The range of 0.1-10 μm is particularly preferred. If the diameter of the microparticles is less than 0.1 μm the filler does not have the desired effect, the diffusion of the light suffers and the background of the image is liable to become tinged with an aluminium colour. At the same time it is necessary to disperse the light as finely as possible to ensure paper-white quality, and if the diameter of the microparticles exceeds 50 μm, the particles are too coarse and the background of the image acquires a satin finish, reducing the paper-white effect and causing the contrast of the image to deteriorate.
The difference between the refractive index of the filler in the invention and the refractive index of the adhesive agent needs to be between 0.05-0.5, and preferably within the range of 0.05-0.3. If the difference in the refractive index is less than 0.05, light is not diffused, and a satisfactory paper-white effect cannot be obtained. Moreover, if the difference in the refractive index exceeds 0.5, the internal diffusion is too large, the overall light transmission rate deteriorates and the paper-white effect cannot be obtained. Furthermore, it is preferable that the refractive index of the filler be lower than the refractive index of the adhesive agent because it is easier to adjust, and improves productivity.
The quantity of filler to be included in the base resin of the adhesive agent will preferably be in the range of 1-40% by weight, and particularly between 2-20% by weight. If there is less than 1% of filler by weight, it is difficult for the filler to achieve the effect of diffusing the light and light-diffusing deteriorates, making it difficult to achieve improved screen brightness and visibility over a wide viewing angle, the effect of the invention. At the same time if the amount of filler included exceeds 40% by weight, the adhesion of the light-diffusing layer is decreased and it is liable to peel off, with the danger that durability will be reduced and it will not performed its function as a light-diffusing layer.
The optimal filler for inclusion in the light-diffusing film is plastic beads, ones with good transparency and a refractive index whose difference from that of the matrix resin is within the above-mentioned range being preferable. Preferred types of such plastic include melamine beads (refractive index; 1.57), acrylic beads (refractive index; 1.49), acryl-styrene beads (refractive index; 1.54) polycarbonate beads, polyethylene beads, and vinyl chloride beads. Inorganic fillers such as celium oxide (CeO2; refractive index 1.63) may also be used. In the case of celium oxide, microparticles with a diameter of around 5 nm can be obtained, but as explained above those with a diameter in the range of 0.1 μm-50 μm are the optimal choice.
In a comparison of the refractive indices of filler, where the refractive index of the resin used is low, microparticles with a high refractive index such as inorganic microparticles of TiO2 (refractive index; 2.3-2.7), Y2O3 (refractive index; 1.87), La2O3 (refractive index; 1.95), ZrO2 (refractive index; 2.05) with a particle diameter of 1-100 nm and preferably within the range of a few nm to several dozen nm are added to the light-diffusing adhesive agent to the extent required to maintain the diffusion properties of the film, and can be used to adjust the refractive index upwards. The greater the refractive index of the microparticles the better, being normally 1.8 or greater, and preferably 1.9 or greater and more preferably 2.0 or greater. It is undesirable to have the diameter of the microparticles greater than 100 nm, as this interferes with transparency. And although no limit is particularly specified, diameters of around 1 nm or more are preferable, for example 5 nm or more is preferred from the point of view of availability and ease of dispersal. By adding inorganic microparticles with a high refractive index as described to a light-diffusing adhesive agent with a low refractive index, and raising the refractive index of the base material of the adhesive agent, it is possible to form a light-diffusing adhesive agent with a refractive index greater than the refractive index of the light guide of between 1.45-1.7, and using this light-diffusing adhesive agent with its high refractive index to bond the directional light-diffusing film and the light guide, the critical angle at the interface between the light guide and the light-diffusing adhesive agent is eliminated, and total reflection is prevented. Thus light which escapes laterally due to total reflection under normal circumstances can be efficiently extracted from the light guide, allowing the light to be effectively used.
It should be noted that
Furthermore, where the surface light source device of the invention is positioned as a backlight behind the liquid crystal display panel, the surface light source device will be positioned below the lower polarising plate of the liquid crystal display panel, with the result that optical films such as the directional light-diffusing film and prism sheets are positioned far away from the liquid crystal display panel. Thus even if faults should be present in an optical film such as the directional light-diffusing film and prism sheet, not only will the faults be difficult to observe, but because a directional light-diffusing film device which does not have a regularly repeating optical structure is easily obtained it is unlikely that Moire fringes will be generated between the liquid crystal display panel and the optical sheet when such a device is employed.
Optimal Configurations for Embodying the Invention
The invention will now described with specific reference to embodiments, although the invention is not limited to the following embodiments.
Embodiment 1
The surface light source device of the first embodiment of the invention will now be described with reference to
The directional light-diffusing film used in embodiment 1 was manufactured in the following fashion. In other words, a polyethylene terephthalate film was coated with 50 μm of light sensitive polymer using DuPont's OMNIDEX that HRF600 or 150, a mask having a plurality of round perforation patterns being made to adhere closely to the surface of this light-sensitive polymer using the hard contact method. However, the round perforations in the mask were within the range of 500 nm to 30 μm, with the average diameter being 2 μm. Ultraviolet light from a mercury lamp was condensed to a parallel beam using a lens system, and irradiated onto the mask at an angle of 30° to the normal direction. The length of the irradiation varies from several seconds to several minutes. Thereafter it was subject to thermal processing for one hour at 120° C. As a result, a light-diffusing film having a regions of high refractive index with a columnar structure angled at 30° to the normal direction of the film was obtained with a cross-sectional structure matching the perforated pattern of the mask. The refractive index of the polymer matrix of the light-diffusing film was 1.47, and the refractive index of the regions with a high refractive index 1.52. The diffusion characteristics of the directional light-diffusing film thus obtained were as shown in
When a single LED light is positioned as the light source at the centre of the light guide as in the first embodiment, there is a large quantity of light in the direction of the line A-A , as shown in
Incidentally, with the surface light source device of Embodiment 1 it was possible to efficiently eliminate unevenness in brightness with a light-diffusing film having a maximum diffusion of between 10-30°, and when using a directional light-diffusing film where the slope of the columnar structures is in the range of 5-60°, it was possible to eliminate unevenness in brightness in every case.
Embodiment 2
A second embodiment of the invention is shown in
Embodiment 3
The surface light source device of embodiment 3 has an identical structure to that of Embodiment 1 apart from the fact that directional light-diffusing film 14 of the surface light source device of embodiment 1 is positioned on prism sheet 15 instead of being positioned on light guide 12. When this surface light source device was used to light a liquid crystal panel as a back light, there was no unevenness in brightness even when seen from an angle, and the degree of brightness seen from the front was high, resulting in a bright image display device.
Embodiment 4
The surface light source device of Embodiment 4 is shown in
In the above embodiment, a light-diffusing adhesive agent with a HAZE value of 15 was obtained using a 2% inclusive volume of silicon resin beads, and used to form a surface light source device in the same way as above, and when this surface light source device was used to light a liquid crystal panel as a back light, there was no unevenness in brightness even when seen from an angle, and the degree brightness seen from the front was high, resulting in a bright image display device in the same way as for the surface light source device of Embodiment 4.
Embodiment 5
The surface light source device of Embodiment 5 was manufactured in the same way as that of Embodiment 4 apart from the fact that the following was used as the light-diffusing adhesive agent. In other words filler was added to a base coating with 1.5 parts of isocyanate hardener (D-90; manufactured by Soken Kagaku) for 100 parts of acrylic adhesive agent with a refractive index of 1.50, and a dispersal liquid of TiO2 or ZrO2 butanol or MEK (methyl ethyl ketone) with a particle diameter size of several nm further added, and then mixed in an agitator for one hour, producing a light-diffusing adhesive agent. This light-diffusing adhesive agent was coated onto a 8 μm thick parting sheet 2 (PET3801, made by Rintech) to reach a thickness of 25 μm after drying, and with the forming of a diffusing adhesive layer after drying, a parting sheet (K-14, manufactured by Teijin) was bonded onto the diffusing adhesive layer to obtain a diffusing adhesive sheet. The filler used was silicon epoxy beads (refractive index 1.43, average particle diameter 1.0 μm) with an inclusive volume of 3%. The HAZE value of the light-diffusing adhesive agent thus obtained was 25. It should be noted that the refractive index of this light diffusing adhesive agents can be adjusted to the desired refractive index by adding in the appropriate quantity of microparticles of TiO2 or ZrO2 butanol or MEK dispersal agent. For example, where wishing to bring the refractive index of the light-diffusing adhesive agent to 1.6, it is sufficient to adjust the proportions so that TiO2 or ZrO2 are present in 35 units per weight in solid measure, with the base resin (including filler) at 65 parts per weight. This light-diffusing adhesive agent was made to adhere to said light-diffusing film, and bonded to light guide 12 by pressure adhesion using a roller to obtain the surface light source device. When this surface light source device was used to light a liquid crystal panel as a back light, there was no unevenness in brightness even when seen from an angle, and the degree of brightness seen from the front was high, resulting in a bright image display device.
In the above embodiment, a light-diffusing adhesive agent with a HAZE value of 15 was obtained using a 2% inclusive volume of silicon resin beads, and used to form a surface light source device in the same way as above, and when this surface light source device was used to illuminate a liquid crystal panel, a bright image display device with no unevenness in brightness was obtained in the same way as for the surface light source device of Embodiment 5.
Embodiment 6
In this embodiment, the surface light source device has the structure shown in
Embodiment 7
The surface light source device of Embodiment 7 will now be described with reference to
At the same time in this embodiment, directional light-diffusing film 14 is positioned on said light guide as shown in
Effect of the Invention
As has been described above, according to the surface light source device of the invention, since the directional light-diffusing film or the optical film comprising said directional light-diffusing film and a light-diffusing adhesive layer which selectively diffuses the unevenness in brightness of light output diagonally to the rear surface of the light guide is positioned facing the rear surface of the light guide, it is possible to provide a surface light source device which eliminates unevenness in the brightness of the light leaking diagonally from the surface of the light guide, and which has uniform brightness and a high degree of brightness seen from the front, and also an image display device with this built in.
Furthermore with the surface light source device of the invention, where the surface light source device is placed behind the image display panel, since the optical sheet which is the directional light-diffusing film, light prism sheet or the like is positioned far away from the image display panel, even where faults are present in the optical sheet not only are the faults difficult to see, Moire fringes are unlikely to be generated between the image display panel and the optical sheet due to the fact that the columnar structures of the directional light-diffusing film are positioned randomly, or due to changes in the diameter of the columnar structures.
Number | Date | Country | Kind |
---|---|---|---|
2003-281211 | Jul 2003 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/JP04/10123 | 7/15/2004 | WO | 8/8/2006 |