1. Field of the Invention
The present invention relates generally to a liquid crystal display (LCD) module, and more particularly to a direct-light illuminating unit, in which a sheet of light diffuser is designated by a surface function to meet the very requirement of the illuminating unit.
2. Description of the Related Art
Liquid crystal displays (LCDs) have been applied to computer monitors, video devices, consumer electronics and the like. A conventional LCD module is mainly composed of a liquid crystal panel and an illuminating backlight unit. The backlight unit provides illumination to the liquid crystal panel so that the panel can show predetermined images. The conventional illuminating backlight unit is typically classified into so called direct-light illuminating unit and so called edge-light illuminating unit.
Typically, the direct-light illuminating unit has a case on which a reflector, lamps and a sheet of diffuser are configured in order. The lamps radiate light onto both of the diffuser and the reflector. The reflector reflects the backward directed rays from the lamps toward the diffuser in the front and the diffuser allows the rays both from the lamps and from the reflector transmitting through and diffuses the light that consequently forms a diffusive light-emitting surface for the liquid crystal panel.
The conventional diffuser has a transparent substrate in which organic fillers are uniformly distributed in the substrate to deflect or reflect the light. In consequence, random and complex light transmitting passages are formed along the thickness of the substrate. The fillers in the substrate deflect the directions of light that prevent light from going through straight and thus diffuse the light, as well as reflect part of the incident light back to the cavity between the reflector and diffuser. The result is a uniform transmitting light emit from the diffuser. Unfortunately, this ray averaging process also decades the amount of light that could be possibly transmitted through, by means of absorption mechanisms due to quantum effects.
The primary objective of the present invention is to provide a direct-light illuminating unit as a LCD backlight, which has higher light emitting efficiency.
According to the objective of the present invention, a direct-light illuminating unit comprises a case on which a reflector, at least a lamp and a sheet of diffuser are configured in order. The diffuser comprises of a transparent substrate, onto which, either side of the surfaces may have predetermined optical patterns being formed into a specific profile. The optical pattern is composed of a plurality of optical transform units. The specific surface profile alters the onward direction and strength of incident rays and result in redistributed emitting light across the illuminating area with uniform luminosity.
As shown in
A case 10 is consisted of a back cover plate 12 and a upper frame 14 and in the center of the upper frame 14 is a window opening 16.
Three lamps 18 are Cold Cathode Fluorescent Lamps (CCFLs). Such lamps have advantages of smaller diameter, longer life and higher illuminating performance and so on. Each lamp 18 is bent from a straight tube of lamp into a substantial U-shape. The lamps 18 are firmly mounted on the back cover plate 12 of the case 10 and electrically connected to transformers or transformer output channels of an inverter (not shown), which is mounted on the case 10, to provide the lamps 18 with high-voltage AC electricity. In practice, the numbers and the specification of the lamps and the transformers are determined according to the requirements of the illuminating backlight unit.
A reflector film 22 is attached on the back cover plate 12 of the case 10 below the lamps 18.
A diffuser sheet 24 is mounted on the back cover plate 12 of the case above the lamps 18.
Two side frames 26 are mounted at opposite ends of the lamps 18 to fix the lamps 18.
As shown in
The surface profile 30 has a predetermined pattern and the pattern is determined from a predetermined surface function. The parameters of the function are the positions of the diffuser sheet 24 related to the lamps 18 and the reflector film 22 etc. and the given constrains, such as the specification of luminance and viewing angle etc. These parameters are calculated via numerical analysis, namely, Project on Convex Set (POCS) method, and are optimized by adjusting the weighting factor of transfer function through recursion.
The surface profile 30 of the diffuser sheet 24 is designated to change the propagation of the light. The surface profile 30 is provided with a plurality of cavities with various depths and widths, called optical transform units 31, on the surface of the substrate 28. The degree of change of light propagation profile through the diffuser sheet is related to the size of optical transform units.
If the pixels of the optical transform units 31 of the surface profile 30 are smaller than a certain characteristic size (relative to the wavelength of light), the propagation of light is a non-linear behavior rather than linear behavior, which can be governed by geometric rules. The governing equations of non-linear optics can be solved by Fourier Transfer method.
Because the optical components of the illuminating backlight unit are nottime dependent, so that all optical components are integrated in design and in fabrication to reduce the space of system and the difficulty of assembly. And the efficiency of light transmittance is high while the light diffusion capability is also high, without scarifying transmittance.
According to our study, the Y-G Algorithm gives a surface profile, which approximates the real phase as possible. The ways of fabrication of the surface profile 30 could be done by etching method, printing method, electroforming method and other suitable methods.
The surface profile 30 of the diffuser sheet 24 has phases with various depths and widths. The conventional method averages the phases to approximate the real phases, so that there are only a few of constant depths of the phases. The present invention assumes that each order has individual depth and width, so that it would get a well far-field diffraction under a predetermined depth and width. The formula for calculation the phase is hereunder:
As shown in