11: liquid crystal display panel
13: cathode ray tube (light source)
19: sheet back surface
21: sheet substrate surface
22: sheet front surface
23: prism portion
29: sheet end face
31: mirror reflection layer (optical function part)
33: light diffusing layer (optical function part)
41: inclined surface (optical function part)
100, 100A: prism sheet (optical sheet)
200: illumination device
300: flat panel display
θ: included angle
Preferred embodiments of an optical sheet and an illumination device and a flat panel display utilizing the same will now be described with reference to the drawings.
A flat panel display 300 according to the invention includes an illumination device 200 provided such that a light-emitting surface of the device faces a back surface of a liquid crystal display panel 11. The illumination device 200 includes a light source unit 15 provided by arranging a plurality of linear cathode ray tubes 13 serving as light sources side by side, a light diffusing sheet 17 provided on a light exit side of the light source unit 15, and two prism sheets 100 which are optical sheets provided on a light exit side of the light diffusing sheet 17.
Since the two prism sheets 100 are identical, the description will address only one of the sheets. A prism sheet 100 allows light emitted from the illumination device 200 to enter the sheet itself through a sheet back surface 19 that is shown in
An optical function part is provided on a sheet end face 29 of the prism sheet 100. A prism end face 29 is an end face extending between a circumferential edge of the sheet back surface 19 and a circumferential edge of the sheet front surface 22. In the present embodiment, the optical function part is constituted by a mirror reflection layer 31 which reflects light leaking through the sheet end face 29 to prevent it from exiting the sheet. For example, let us discuss light passing through a point A as shown in
The optical function part may be a light diffusing layer 33 which prevents light from exiting the sheet end face 29 by causing diffuse reflection of the light which can otherwise leak out through the sheet end face. The light diffusing layer 33 may be a layer formed on the sheet end face 29 shown in
As shown in
The mirror reflection layer 31 and the light diffusing layer 33 may be formed by a process in which an optical sheet is fabricated using a material roll 35 and a product roll 37 and in which, for example, coating 36 is performed according to the above-described method on a roll end face 37a of the product roll 37 after the sheet is taken up. Alternatively, coating 38 may be performed according to the above-described method on the material roll 35 prior to the fabrication of the sheet, and a prism sheet 100 may be thereafter fabricated. After the roll sheet is cut, coating 40 is further performed to form mirror reflection layers 31 and light diffusing layers 33 on end faces of the cut sheets. Alternatively, the mirror reflection layers 31 may be formed on sheet end faces 29 by coating them with metal paste as described above at a handling step that is arbitrarily provided.
In particular, the mirror reflection layers 31 or light diffusing layers 33 may be formed on the sheet end faces 29 when the sheets are in the rolled state according to any of the above-described methods if the sheet end faces 29 are vertical. However, when the sheet end faces 29 constitute a surface at an angle offset from the vertical, it is difficult to form the layers according to the above-described methods because each sheet forms an irregularity at the end face of the roll when the sheets are in the rolled state. Therefore, the mirror reflection layers 31 or light diffusing layers 33 may alternatively be formed by immersing the sheet end faces 29 in a solution for forming the layers while keeping the sheets vertical at a step for conveying the sheets in an unrolled state (at a roll conveying path which is not shown in
In the case of the prism sheet 100 having such optical function part on the sheet end face 29 thereof, light is returned back into the sheet by the optical function part at the sheet end face 29 where the light will otherwise be dissipated out of the sheet. Therefore, the light can be reused and can exit the sheet through the front surface thereof. When luminance is kept constant, the emission intensity of light sources or the number of the light sources can be reduced.
A second embodiment of an optical sheet according to the invention will now be described.
A sheet end face 29 of a prism sheet 100A according to the present embodiment is constituted by an inclined surface 41 which meets sheet surfaces (a sheet back surface 19 and a sheet substrate surface 21 in the present embodiment) at an included angle (hereinafter also referred to as “end face angle”) θ of 90° or less to the sheet surfaces.
As shown in
That is, when light traveling in the sheet along the sheet surfaces reaches the sheet end face 29, the angle of the light is changed by the inclined surface 41 to return the light back into the sheet, thereby preventing the light from being transmitted and dissipated out of the sheet. The light is then repeatedly transmitted, refracted, and reflected in the sheet to increase the quantity of light exiting the sheet front surface 22.
The inclined surface 41 (an end face of a transparent substrate constituted by plastic or a film) of the prism sheet 100A is preferably a smooth surface which can cause mirror reflection (a mirror reflection layer 31). The inclined surface 41 may be a light diffusing layer 33 having diffusing properties. The included angle θ of the inclined surface 41 is set at an appropriate and optimum value according to the thickness and size the optical sheet (the sheet size being the length of a side of the sheet or the surface area of the same).
Preferably, the sheet end face 29 meets sheet surfaces (the sheet back surface 19 and the sheet substrate surface 21 in the present embodiment) of the optical sheet 100 at an included angle within the range of 90° plus and minus 20° or the range from 70° to 110°. The reason is that frontal luminous intensity is substantially the same when the included angle θ of the sheet end face 29 is 85° and 90° and is slightly lower when the angle is 75°. Frontal luminous intensity having high peaks can be maintained by keeping the end face angle within the range of 90° plus and minus 20°.
The prism sheet 100A returns light which has been transmitted and dissipated lost out of the sheet according to the related art, back into the sheet. The light returned into the sheet travels in the sheet in the opposite direction. Light rays in parallel with the sheet substrate surface 21 travel toward another sheet end face 29 on the opposite side. Light rays which are offset from the parallelism impinge upon a sheet back surface 19 and a prism portion 23 however small the offsets are. The light rays are repeatedly refracted, reflected, and transmitted, and the quantity of light exiting the prism portion 23 is thereby increased.
In an idealistic system in which the substrate of the prism sheet 100A is completely flat and in which the sheet end faces 29 are perfectly vertical, light rays traveling in perfect parallelism with the sheet substrate surface 21 are reflected by the sheet end face 29, and they reach the sheet end face 29 on the opposite side to be reflected repeatedly. The percentage of the light rays in perfect parallelism is small, and light rays offset from the parallelism impinge upon the sheet back surface 19 and the prism portion 23 as a result of reflection at the end face however small the offsets are.
In practice, there are microscopic curves and irregularities on the surface of the prism sheet 100A. The end faces also have an angular offset from the vertical, and there are also curves and irregularities on the sheet end faces 29. Therefore, most of light rays reflected by the sheet end faces 29 impinge upon either sheet back surface 19 or prism portion 23. When the sheet end face 29 is formed to define an included angle θ that is different from the vertical, light rays traveling in the sheet substantially in parallel with the same are reflected by the sheet end face 29 with their angles changed, and the light rays then impinge upon the sheet back surface 19 and the prism portion 23 to be refracted, reflected, and transmitted.
For example, let us assume that the sheet back surface 19 is a surface inclined from the perpendicularity to the sheet substrate surface 21 as shown in
The inclined surface 41 of the prism sheet 100A is a smooth surface which allows mirror reflection to take place. Although the inclined surface 41 is preferably constituted by a smooth mirror reflection layer 31, the purpose of preventing transmission and dissipation of light from the sheet end face 29 can be achieved by a surface having irregularities as long as the surface reflects light. Similarly, the inclined surface may be a light diffusing layer 33 having diffusing properties.
The sheet end face 29 of the prism sheet 100A may be constituted by a plurality of inclined surfaces 41a, 41b, and 41c at different angles of inclination θa, θb, and θc as shown in
With a prism sheet 100A formed with a sheet end faces having a plurality of angles of inclination different from each other as described above, when light at a certain inclination to the sheet substrate surface 21 is reflected at the sheet end face 29 to eventually exit the sheet front surface 22, the light can be reflected at a wider range of angles of inclination to the sheet front surface 22 and can therefore exit the sheet front surface 22 with higher efficiency.
Referring now to means for inclining the sheet end face 29 of the prism sheet 100A at an angle other than 90° or the method of forming the sheet end face 29 at an arbitrary angle to the sheet substrate surface 21 other than perpendicularity, an oblique cutting process may be employed, which is performed at different cutting angles with cutting means that is commonly used.
Even when the sheet end face is set at an angle of inclination other than perpendicularity as described above, the dissipation of light out of the sheet can be reliably prevented by providing the mirror reflection layer 31 or the light diffusing layer 33 on the sheet end face 29.
An analysis was carried out on the effect of a prism sheet according to the embodiment by way of example. Referring to
Referring to the result of the simulation carried out by varying the angle of the sheet end face shown in
In the above-described optical sheet, an optical function part (the mirror reflection layer 31, light diffusing layer 33, or inclined surface 41) is provided on the sheet end face 29 extending between a circumferential edge of the sheet back surface 19 and a circumferential edge of the sheet front surface 22 to prevent light from leaking out of the sheet through the sheet end face and to return the light back into the sheet. Thus, the light which can be otherwise dissipated out of the sheet through the sheet end face 29 can be reused and caused to exit the front of the sheet, which makes it possible to achieve improved frontal luminance. When luminance is kept unchanged, it is possible to reduce the emission intensity of light sources or to reduce the number of light sources. Thus, power consumption can be reduced.
The illumination device 200 includes the optical sheet and a light source disposed to face the sheet back surface 19 of the optical sheet. When light emitted from the light source enters the sheet from a sheet back surface 19 and the light which has entered the sheet is about to leak out through the sheet end face 29, the light is prevented from exiting by the optical function part provided on the sheet end face 29 and returned back into the sheet as return light. As a result, the quantity of light rays exiting forward through the prism portion 23 is increased, which allows improved frontal luminance to be achieved with the same level of power consumption as that in the related art.
The flat panel display 300 includes the illumination device 200 and a liquid crystal display panel 11 disposed to face a sheet surface of the optical sheet in parallel with the same. A backlight source for the liquid crystal display panel 11 can be constituted by the illumination device 200 which achieves high utilization of light. Therefore, display at high luminance can be achieved with the same power consumption as that of a flat panel display according to the related art. When display is to be achieved with only the same luminance as in the related art, power consumption can be reduced by reducing the emission intensity of light sources or reducing the number of light sources.
This application is based on Japanese Patent application JP 2006-238655, filed Sep. 4, 2006, the entire content of which is hereby incorporated by reference, the same as if fully set forth herein.
Although the invention has been described above in relation to preferred embodiments and modifications thereof, it will be understood by those skilled in the art that other variations and modifications can be effected in these preferred embodiments without departing from the scope and spirit of the invention.
Number | Date | Country | Kind |
---|---|---|---|
2006-238655 | Sep 2006 | JP | national |