Some displays use backlighting to illuminate the display surface. The light used to backlight the display is typically coupled into an edge of the display.
Displays are devices used to display electronic images to users. Some displays produce light used to create the image, for example a cathode ray tube (CRT). Other displays produce light to illuminate the elements in the display that create the image, for example liquid crystal displays (LCD). Some displays use back lighting to illuminate the surface of the display, for example touch screens. Backlit displays typically couple one or more light beams into the backplane of the display through a side edge of the backplane. The backplane is the layer in the display that channels or directs the light along the surface of the display.
When coupling a light beam into the backplane of a display through a side edge, the refracted beam angle and the beam height inside the backplane of the display determines when the backplane is uniformly illuminated. The refracted beam angle inside the backplane is dependent on the angle the beam makes with the top surface of the backplane, the angle the edge surface makes with the top surface of the backplane and the index of refraction of the backplane material. When the edge surface of the backplane is at a 90 degree angle with respect to the top surface of the backplane, the refracted angle of the beam inside the backplane cannot be adjusted such that the back plane is uniformly illuminated. By angling the side edge with respect to the top surface, the refracted angle of the beam inside the backplane can be adjusted such that the back plane is uniformly illuminated.
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Backplane 108 typically has a thickness in the range between 1 and 10 mm. Backplane 108 has a top surface 102, a bottom surface and an edge surface 104. The bottom surface of the backplane is parallel with the top surface. The edge surface makes a non-ninety degree angle (also called a wedge angle) with the top surface. Optical system 107 produces the collimated beam of light 106 using one or more lenses and/or mirrors. In some examples, optical system has a single light source (as shown). In other examples multiple light sources may be used to create the beam of collimated light 106. The collimated beam of light enters the backplane though edge surface 104. The collimated beam of light substantially fills the edge surface 104.
When β′ equal to α, distance d1 will equal distance d2 because the two triangles are equal (triangle ABC is equal to triangle A′B′C′). Therefore when β′ is equal to α, the edges of the beam inside the backplane will just meet along the top surface of the backplane as the beam propagates down the backplane. Therefore the backplane 308 will have uniform illumination along the top surface 302.
When β′ is smaller than α, the beam will have gaps in illumination as it travels down the backplane. These gaps form dark areas in the illumination of the top surface of the backplane. The gaps in illumination form a non-uniform illumination along the top surface of backplane 308. When β′ greater than α, the beam will overlap along the top surface of the backplane as it travels down the backplane.
Angle β and β′ are related by Snell's law, the index of refractive of the two materials and angle α. In this case the first material is air, which has a refractive index of 1. Setting β′ equal to α and using N as the index of refraction of the backplane 308, we can solve for β.
sin β=cos α√{square root over (1−(N cos 2α)2)}−N cos 2α*sin α Equation 1
In addition the angle β′ (which equals angle α) must be kept small enough to satisfy the total internal reflection constraint. The refracted beam angle measured with respect to a line perpendicular to the top surface (i.e. 90−β′) should be larger than the critical angle for total internal reflection. The critical angle is measured with respect to a line perpendicular to the top surface. The critical angle θc is equal to arcsin (1/N), where N is the index of refraction of the backplane. Therefore β′ set less than 90−θc.
Point 532 is where the beam angle β is zero (i.e. the beam is parallel with the top surface of the backplane). The wedge angle α for point 532 is 26 degrees. Because the beam enters the backplane parallel with the top surface of the backplane, a display can be fabricated using planer geometry (i.e. all the components can be manufactured/assembled in the same plane). Point 534 is where both the beam angle β and the wedge angle α are at 45 degrees. This allows the beam to enter the side surface of the backplane at a 90 degree angle (i.e. no refraction of the beam as it enters the backplane). When the wedge angle α of the edge surface is equal to 90 degrees, there is no angle β that can be chosen such that angle β′ is greater than or equal to angle α.