Method for removing moiré
A technology of Moore interference and cylindrical lens, applied in the field of optics, can solve problems such as the generation of cylindrical lens devices, affecting the display effect, affecting viewing comfort, etc., and achieve the effect of solving technical constraints
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specific Embodiment approach 1
[0018] Specific implementation mode one: the following combination Figure 3 to Figure 6 Describe this embodiment mode, the method for eliminating moiré fringe described in this embodiment mode, the 3D display that this method is aimed at includes cylindrical lens grating 101, PET base material 102, OCA optical adhesive 103 and liquid crystal screen, and liquid crystal screen comprises color filter glass 109, TFT glass 111, the upper surface of color film glass 109 and the lower surface of TFT glass 111 are respectively provided with a polarizer 108. The color film glass 109 and TFT glass 111 are provided with a display screen core layer 110, and the display screen core layer 110 includes three Layer structure: upper glass, lower glass and liquid crystal with a thickness of only about 4 microns between them; The lower glass is provided with a circuit layer, which is made of conductive metal or metal oxide such as ITO or molybdenum-aluminum-molybdenum. The circuit layer include...
specific Embodiment approach 2
[0026] Specific implementation mode two: the following combination Figure 5 with Image 6 Describe this embodiment mode. This embodiment mode will further explain Embodiment 1. The cylindrical lens grating can adopt two structural modes:
[0027] The first structure: such as Figure 5 As shown, the cylindrical lens adopts a single convex grating structure. n1 is the refractive index of the prism; n2 is the refractive index of the cylindrical lens embedded in the prism; and n2<n1;
[0028] The second structure, such as Image 6 As shown, the cylindrical lens adopts a combined grating; the combined grating is composed of a concave grating with a refractive index of n2 and a convex grating with a refractive index of n3, and the combined grating is equivalent to an ordinary convex lens. n1 is the refractive index of the prism; n2<n1;
specific Embodiment approach 3
[0029] Embodiment 3: This embodiment further explains Embodiment 2. The height of the triangular prism does not exceed 1 / 3 of the height of the cylindrical lens embedded in it. If it exceeds this value, it is adjusted by increasing the thickness of the base of the cylindrical lens.
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