1. Field of the Invention
The present invention is related to an integrated light guide plate, and more particularly to an integrated light guide plate applied to a backlight module to enhance axial luminosity with microstructures formed on the plate.
2. Description of the Related Art
A backlight module plays a critical role in an active matrix light crystal display. With reference to
Light-emitting luminance distribution of the LGP 51 could become uneven as a result of the geometrical design of the microstructures. The lower diffuser sheet 53b serves to modify the emitting light into a Lambertian distribution. To improve the axial luminous intensity of a backlight module of a handheld display or personal display with limited luminance, a conventional measure uses the two orthogonally-distributed prism sheets 54a, 54b to collimate the emitting light axially. The collimated light further passes through the upper diffuser sheet 53a to smoothen minor uniformity imperfections or possible Moiré fringes of back light.
According to the manufacturing methods, LGPs (51) can be classified into printed light guide plates and non-printed light guide plates. Printed LGPs are formed by printing a diffusive dot matrix onto plain polymer plates. Non-printed light guide plates are integrally formed with the microstructures by injection molding or hot embossing. Non-printed LGPs usually have a prominent optical performance, in comparison with printed LGPs using dot matrices, since the microstructures of the non-printed LGP do not turn yellowish as a result of prolonged exposure to light. Hence, non-printed LGPs have dominated small-to-medium back light modules (BLMs).
Usually, LGPs have a microstructure taking a form of V-cuts formed on a bottom surface thereof. As such microstructures can vary in density or size along one-dimensional direction, the LGPs having such microstructures are suitable for a CCFL light source. If LED is used as a light source, the distribution of the microstructures has to be varied in two dimensions as the illumination distribution of LEDs is similar to a point light source with a limited emitting angle. Hence, spherical dots and short V-slots become the most common microstructures for LED lit LGPs.
With reference to
Certain optical elements such as prisms, convex and concave lens are designed on the edge-lit surface of the LGP to modify the emitting angle and intensity distribution of light sources. With reference to
With further reference to
With reference to
With reference to
Keeping abreast with the market demand, backlight modules tend to be slim, and light, and head for a goal of low power consumption and low cost. However, as disclosed earlier, conventional LGPs must be additionally equipped with the reflector sheet, the diffuser sheet and prism sheets to acquire more satisfactory emitting luminance. Besides, additional components cause a drop of light efficiency and run counter to the demands of lowering size, weight and cost of the backlight modules.
An objective of the present invention is to provide an integrated light guide plate having enhanced axial luminosity, which enhances axial directional luminance with microstructure formed thereon.
To achieve the foregoing objective, the integrated light guide plate has a substrate, a plurality of V-cuts and a plurality of pyramidal recesses.
The substrate has a light incident plane, a light emission plane and a bottom surface opposite to the light emission plane.
The plurality of V-cuts are formed on the light incident plane and serve as prisms, and each V-cut has a first angle ranging from 85° to 105°.
The plurality of pyramidal recesses are formed in the bottom surface of the substrate.
A reference line passing through one vertex of one of the pyramidal recesses is normal to one side of the substrate, and a second angle is defined between the reference line and an edge of a base of the pyramidal recess and ranges between 43° to 47°.
Given the combination and distribution of the V-cuts and the pyramidal recesses, the integrated light guide plate can provide emitting light with high intensity axially without requiring additional diffuser sheets and prism sheets.
With reference to
With reference to
An angle between the reference line L1 and one edge of the base of the pyramidal recess 30 is defined as θ2. The θ2 ranges from 43° to 47°. In the present embodiment, the pyramidal recess 30 is a truncated regular pyramidal recess fabricated by using anisotropic wet etching defined by the [100] crystal plane and an etch stop.
Given the first angle θ1 being 90° and the second angle θ2 being 45°, a light effect can be observed in the view angles α and β as shown in
Followed by the vertical view angle β, the corresponding axial luminous intensity curve is C1. Similar to the interpretation for the horizontal view angle α, when the first angle θ1 of the V-cuts is 90°, the light energy loss due to the side lobes located around angle β=±70° is minimized, and thus the light focusing effect is more noticeable, which produces a highest axial luminous intensity.
With reference to Table 1, the first angle θ1 is incremented from 70° to 110° by 5° at a time. According to the simulation data listed in Table 1, when the first angle θ1 is gradually incremented from 70° to 110°, the axial luminous intensity is demonstrated as a curve, and the highest value is about 11.4. Varying the first angle has minor influence on the axial luminous intensity and the average luminance. Hence, an apex angle of incident light or the first angle θ1 can be determined by the values of the axial luminous intensity. The acceptable range of the first angle θ1 is 85° to 105°.
With reference to Table 2, observe the simulation data of the table by incrementing the rotation angle θ2 of the pyramidal recess 30 from 35° to 45° by 2° at a time. As the rotation angles θ2 from 35° to 43° are not symmetrical relative to an LED lighting plane, the light intensity distribution leans to one side to lower the axial luminous intensity values. Varying the rotation angle θ2 has minor influence on the light efficiency and the average luminance. According to the variation of the axial luminous intensity, the best rotation angles θ2 of the pyramidal recess 30 is between 43° to 47° (45°±2°).
Instead of additionally requiring the upper and lower diffuser sheets and two prism sheets, the present invention employs the range of the rotation angle (θ2) of the pyramidal recess 30, 43°˜47°, in collaboration with the first angle (θ1) of the V-cuts to enhance the axial luminous intensity. The goal of the integrated LGP is achieved and the production cost and the module thickness are also reduced. Meanwhile, as the integrated LGP of the present invention eliminates the use of the lower diffuser sheet and the two prism sheets, the loss of the light efficiency resulting from the use of optical sheets can be avoided.
With reference to Table 3, after comparing the simulation data of the LGP of the present invention and conventional LGPs without having any optical sheets, the axial luminous intensity of the integrated LGP of the present invention is about 2.6 times of that of the conventional LGPs without the optical sheets and is similar to that of the conventional LGPs equipped with the optical sheets.
In sum, the integrated LGP not only avoids the use of optical sheets causing the drop of the light efficiency of LGPs, but also provides axial directional light luminance. To reduce the thickness and cost and enhance the light efficiency of LGPs, the integrated single-sheet LGP can be a better alternative to replace the conventional LGPs equipped with two more prism sheets.
Even though numerous characteristics and advantages of the present invention have been set forth in the foregoing description, together with details of the structure and function of the invention, the disclosure is illustrative only. Changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed.
Number | Name | Date | Kind |
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20100142225 | Kurihara et al. | Jun 2010 | A1 |
Number | Date | Country | |
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20120081926 A1 | Apr 2012 | US |