Abstract:
A structure for reducing internal reflections in an optical system includes a stack of layers including a first layer having a first refractive index, a second layer having a second refractive index, a third layer having a third refractive index, a fourth layer having a fourth refractive index, and a fifth layer having a fifth refractive index. The second layer is arranged between the first layer and the third layer, and the fourth layer is arranged between the third layer and fifth layer. Further, the third refractive index is greater than the second and fourth refractive indexes, the second refractive index is greater than the first refractive index, and the fourth refractive index is greater than the fifth refractive index.

Description:
TECHNICAL FIELD 
     The present invention relates generally to optical systems and, more particularly, to a display structure that uses destructive interference of light to cost-effectively reduce reflections at higher-refractive index layers within an optical system. 
     BACKGROUND OF THE INVENTION 
     Many optical systems contain layers of contrasting refractive index, n. This gives rise to reflections within the system, diverting incident light from its designed path, decreasing efficiency and increasing noise. More particularly, several systems contain a higher-refractive index medium surrounded by two lower-refractive index media. In some such systems the higher-index medium is thin enough so that interference between reflections at the two surfaces of the higher-index layer can take place, constructively or destructively, depending on the optical path difference. 
     One such system illustrated in  FIG. 1  is a liquid crystal display (LCD), where one indium-tin-oxide (ITO) electrode,  102 , with n≈1.95, lies between layers of liquid crystal (LC),  104 , with n≈1.53, and glass or color filter (CF),  101 , with n≈1.53, and the other lies between LC,  104  and a planarizing resin,  108 , with n≈1.59. There is also a thin layer of polyimide (PI),  103 , with n≈1.70, between the LC and each ITO electrode. There are also layers of silicon nitride,  105 , with n≈2.04, between layers of silica,  106 , with n≈1.55 and/or the planarizing resin. The silica and silicon nitride layers are used as dielectric and for passivation in and around the thin-film transistor (TFT) system. Glass,  107 , supports the structure. This is one typical structure in use in the industry. 
     Reflection of ambient light at a display device undesirably reduces the contrast of the image seen by a viewer. Anti-reflection coatings (ARCs) are used on the front surface of displays, which can reduce its reflectivity to less than 1%. However, reflections arise within the device, particularly at the ITO electrodes and silicon nitride layers, which also contribute to the degradation of the image in a brightly lit room. ARCs for the outer surfaces of optical systems have been studied in detail. One is described, for example, in U.S. Pat. No. 6,207,263. 
     Concerning interfaces within an optical system, that which has received most attention is a single interface, between a lower-refractive index medium and a higher-refractive index medium. 
     U.S. Pat. No. 5,061,874 describes a layer introduced between two media, together with a roughening of the interfaces, to reduce specular reflection. 
     Within the field of LCDs, several specific situations have been investigated, with a view to reducing reflections. Reducing reflections at a glass-semiconductor interface is the subject of US Patent Application No. 2006/0197096A. A structure which uses destructive interference of light to make a ‘black matrix’ effective as an absorber is claimed in U.S. Pat. No. 7,167,221. US Patent Application No. 2004/0109305A describes ARCs used on the elements of an LCD backlight which are in contact with air. 
     WO 2004/044998 describes a design for an organic light emitting diode (OLED). All of the layers, an outermost layer and the internal, light-emitting layers, have thicknesses chosen, according to their refractive index, to result in destructive interference of ambient light in reflection. 
     Finally, U.S. Pat. No 7,215,075 describes a structure that reduces reflections at the cathode of an OLED, which has a higher refractive index than its surrounding media. The method according to U.S. Pat. No. 7,215,075 is to replace the single cathode layer with an even number of layers, which have alternating high and low refractive indices. 
     SUMMARY OF THE INVENTION 
     A device and method in accordance with the present invention can be used in an optical system, such as a liquid crystal display, to minimize internal reflections. More particularly, the device and method in accordance with the present invention provide a structure that includes a first layer formed between a second and third layer, wherein a refractive index of the first layer is greater than a refractive index of the second and third layers. Further, a fourth layer is formed on one side of the second layer, and a fifth layer is formed on one side of the third layer, wherein the fourth and fifth layers have a lower refractive index than the second and third layers, respectively. The device and method in accordance with the present invention reduce internal reflections of an optical device while utilizing fewer layers relative to conventional optical devices. Additionally, a display device, such as an LCD, employing principles in accordance with the present invention is less costly to produce relative to conventional LCD devices. 
     According to one aspect of the invention, a structure for reducing internal reflections in an optical system includes a stack of layers including a first layer having a first refractive index, a second layer having a second refractive index, a third layer having a third refractive index, a fourth layer having a fourth refractive index, and a fifth layer having a fifth refractive index, wherein the second layer is arranged between the first layer and the third layer, and the fourth layer is arranged between the third layer and fifth layer, and wherein the third refractive index is numerically greater than the second and fourth refractive indexes, the second refractive index is numerically greater than the first refractive index, and the fourth refractive index is numerically greater than the fifth refractive index. 
     According to one aspect of the invention, the second refractive index is different from fourth refractive index. 
     According to one aspect of the invention, the first refractive index is different from the fifth refractive index. 
     According to one aspect of the invention, at least one layer comprises liquid crystal layer. 
     According to one aspect of the invention, the first layer comprises a color filter, the second layer comprises a polymide, the third layer comprises an indium-tin-oxide electrode, the fourth layer comprises a polymide and the fifth layer comprises a liquid crystal layer. 
     According to one aspect of the invention, the first layer comprises a liquid crystal material, the second layer comprises a polymide, the third layer comprises an indium-tin-oxide electrode, the fourth layer comprises a polymide and the fifth layer comprises a planarizing layer. 
     According to one aspect of the invention, the first layer comprises a planarizing layer, the second layer comprises a polymide, the third layer comprises a silicon nitride layer, the fourth layer comprises a polymide and the fifth layer comprises a silica layer layer. 
     According to one aspect of the invention, the respective layers are optimized to minimize total reflectivity by destructive interference. 
     According to one aspect of the invention, the structure further includes at least one of silica or silicon nitride arranged in the stack, and a light transmission path through the stack, wherein the at least one of silica or silicon nitride are arranged outside of the light transmission path. 
     According to one aspect of the invention, the second and/or fourth layers comprise at least one of polycarbonate, polystyrene, or indium zinc oxide. 
     According to one aspect of the invention, a display device includes a support, and the structure in accordance with the invention is arranged over the support. 
     According to one aspect of the invention, the support comprises glass. 
     According to one aspect of the invention, the display device is at least one of a liquid crystal display, an organic light emitting diode display, or an electrowetting display. 
     According to one aspect of the invention, a method for minimizing internal reflections in an optical device is provided, the optical device including a stack of layers, the stack comprising a first layer having a first refractive index, a second layer having a second refractive index, and a third layer having a third refractive index, the second layer formed between the first and third layer, wherein the second refractive index is numerically greater than the first refractive index and third refractive index, the method includes: forming a fourth layer having a fourth refractive index between the first and second layers, and forming a fifth layer having a fifth refractive index between the second and third layers, wherein the second refractive index is numerically greater than the fourth refractive index and the fifth refractive index, the fourth refractive index is numerically greater than the first refractive index, and the fifth refractive index is numerically greater than the third refractive index. 
     According to one aspect of the invention, the method includes selecting the fourth layer and fifth layer such that the fourth layer&#39;s refractive index is different from fifth layer&#39;s refractive index. 
     According to one aspect of the invention, the method includes optimizing the respective layers of the stack to minimize total reflectivity in the optical device by destructive interference. 
     According to one aspect of the invention, the method includes forming the second layer to a thickness such that an amplitude of total light reflected at the second layer depends on a phase difference between waves reflected from different surfaces of the second layer. 
     To the accomplishment of the foregoing and related ends, the invention, then, comprises the features hereinafter fully described and particularly pointed out in the claims. The following description and the annexed drawings set forth in detail certain illustrative embodiments of the invention. These embodiments are indicative, however, of but a few of the various ways in which the principles of the invention may be employed. Other objects, advantages and novel features of the invention will become apparent from the following detailed description of the invention when considered in conjunction with the drawings. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  illustrates an exemplary optical structure of an LCD system. 
         FIG. 2  illustrates an exemplary optical structure that includes a higher-refractive index layer between two lower-refractive index media. 
         FIG. 3  illustrates an exemplary optical structure that includes intermediate-refractive index layers to reduce reflections in the optical system in accordance with an embodiment of the present invention. 
         FIG. 4  illustrates a conventional two-layer optical system designed to reduce reflections relative to the one-layer system of  FIG. 2 . 
         FIG. 5  illustrates a conventional four-layer optical system with alternating layers designed to reduce reflections relative to the one-layer system of  FIG. 2 . 
         FIG. 6  illustrates an exemplary LCD structure that includes intermediate-refractive index layers in accordance with an embodiment of the present invention. 
         FIG. 7  illustrates an alternative LCD structure to the structure of  FIG. 1   
         FIG. 8  illustrates the LCD structure of  FIG. 7  with intermediate-refractive index layers in accordance with an embodiment of the present invention. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     The principles of the invention will now be described with reference to the drawings. Because the invention was conceived and developed for use in liquid crystal display systems, it will be herein described chiefly in this context. However, the principles of the invention in their broader aspects can be adapted to other types of optical systems, such as, for example, organic light emitting diode (LED) display systems and electrowetting display systems. 
     Referring to  FIG. 2 , there is shown an exemplary optical structure to which principles in accordance with the present invention can be applied. As shown in  FIG. 2 , a higher-refractive index layer (e.g., media having a refractive index that is numerically greater than the refractive index of other media), HI, is surrounded by lower-refractive index layers (e.g., media having a refractive index that is numerically less than the refractive index of HI), LI 1  and LI 2 , which may have the same or different refractive indices. The thickness of the higher-refractive index layer is such that the total reflected power is a result of interference between the two reflections at the surfaces of the higher-refractive index layer (there is a maximum thickness of the HI layer for which this is true, dependent on the coherence of the light). 
     Moving to  FIG. 3 , layers of intermediate refractive index, MI 1  and MI 2 , are applied to each side of the higher-refractive index layer HI, in between the higher refractive index layer and the lower-refractive index surrounding media LI 1  and LI 2 . MI 1  and MI 2  may have the same or different refractive indices. 
     The device in accordance with  FIG. 3  reduces reflections at a higher-refractive index layer, surrounded by lower-refractive index media in an optical system. Further, the device in accordance with  FIG. 3  reduces reflections more effectively than 2-, 4- and 6-layer systems, such as those described in U.S. Pat. No. 7,215,075. This will now be demonstrated below. 
     The following results have been obtained using a downhill simplex, numerical method of multidimensional minimization, as described in Press, W. H., et al., ‘Numerical recipes in C: the art of scientific computing’, second edition (Cambridge University Press, 1992), pages 408-412. The reflectivities are calculated for light at normal incidence, using a calculation as found in Smith, W. J., ‘Modern Optical Engineering’, third edition (McGraw-Hill, 2000), pages 205-207 (equation 7.32 has been corrected to agree with equations 7.30 and 7.31). They are averaged for a flat spectrum from 450 nm to 750 nm. Average reflectivity (hereafter referred to as ‘reflectivity’) is minimized with respect to refractive indices, where they are unknown, and thicknesses of the layers. The above-referenced portions of both Press and Smith are hereby incorporated by reference.
         a) Referring to  FIG. 2 , consider the case of a layer, HI, with n=1.95, surrounded by media, LI 1  and LI 2 , both with n=1.50. The minimum reflectivity at HI, with respect to its thickness, is then 0.013. HI is 148 nm thick in this case. The reflectivity is so low, despite the refractive index contrast between HI and LI 1  and LI 2 , due to destructive interference of light reflected at the two surfaces of HI.       

     In accordance with the present invention, and as noted above, two extra layers of intermediate refractive index can be added to the system of  FIG. 2 . These are MI 1  and MI 2  as shown in  FIG. 3 . The reflectivity of the new, three-layer system (Hi, MI 1  and MI 2  form the three layers) can be minimized to 0.00005, i.e., reflectivity is reduced by a factor of 3000 relative to the device of  FIG. 2 . The refractive indices of MI 1  and MI 2  in this case are both 1.66 and their thicknesses are 85 nm. HI (with n=1.95) is 145 nm thick. 
     In a method related to that of U.S. Pat. No. 7,215,075, a single extra layer, E, could instead be added to the system, as shown in the conventional optical structure of  FIG. 4 . In this two-layer case (HI and E form the two layers), the minimum possible reflectivity is 0.0084 and the extra layer has refractive index 1.61. Comparing the above results obtained with respect to the two layer system of  FIG. 4  to the results for the device in  FIG. 3 , the reduction in reflectivity of a two-layer solution is improved by a factor of 170 in this case.
         b) To make a comparison with the next simplest embodiment of U.S. Pat. No. 7,215,075, the materials used in the examples of U.S. Pat. No. 7,215,075 are examined. This is a four-layer system, with alternating higher and lower refractive indices, and is shown in  FIG. 5  (layers Y, X, Y, and X form the four layers). L 1  and L 2  are the media surrounding the four layers. Each alternating layer is composed of either medium X or Y.       

     The examples in U.S. Pat. No. 7,215,075 use X and Y with refractive index 1.8 and 2.2. L 1  and L 2  are not specified, so this configuration cannot be compared fully with the embodiment shown in  FIG. 3 . L 1  and L 2  are here taken to be 1.50. Using the multi-dimensional minimization algorithm to vary the thicknesses in this four-layer structure, the reflectivity at these layers (surrounded by media L 1  and L 2 ) can be minimized to 0.018. 
     The same materials used in the above example can be used in the device in accordance with the present invention, e.g. in a three-layer system as described herein. The refractive index of HI is 2.2 in this case, those of MI 1  and MI 2  are both 1.8, and those of LI 1  and LI 2  are both 1.50. The reflectivity at the three layers can be minimized, with respect to thicknesses of the layers, to 0.0017. 
     Thus, using the same materials with the device in accordance with the present invention as opposed to the four-layer embodiment of U.S. Pat. No. 7,215,075, the reflectivity is reduced by an order of magnitude.
         c) Referring to  FIG. 5 , a four-layer system is now considered having the refractive indices of L 1  being 1.50, that of L 2  being 1.60 and those of X and Y being 1.70 and 1.95, respectively. The four-layer system then has a minimum reflectivity of 0.0039.       

     The three-layer system in accordance with the present invention, using the same materials, i.e., refractive indices of 1.70, 1.95 and 1.70 for MI 1 , HI and MI 2  in  FIG. 3 , allows a minimum reflectivity of 0.00056. The reflectivity is again reduced, this time by a factor of 7, compared with the use of the same materials according to the four-layer embodiment of U.S. Pat. No. 7,215,075. 
     A six-layer alternating system (also an embodiment of U.S. Pat. No. 7,215,075), using refractive indices 1.70 and 1.95 allows a minimum reflectivity of 0.0037. 
     Considering all of these results, it can be seen that when a higher-refractive index layer is surrounded by lower-refractive index media, the device in accordance with the present invention offers superior reduction of reflections when compared to solutions according to U.S. Pat. No. 7,215,075. 
     The device in accordance with the present invention will be described more fully hereinafter with reference to the accompanying drawings. The principles in accordance with the present invention, however, may be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. 
     Embodiment One 
     Referring to  FIG. 1 , there is shown an example of an optical structure embodied as a liquid crystal display (LCD), where one ITO electrode,  102 , with n≈1.95, lies between layers of liquid crystal (LC),  104 , with n≈1.53, and glass or color filter (CF),  101 , with n≈1.53, and the other lies between LC,  104  and a planarizing resin,  108 , with n≈1.59. There is also a thin layer of polyimide (PI),  103 , with n≈1.70, between the LC and each ITO electrode. There are also layers of silicon nitride,  105 , with n≈2.04, between layers of silica,  106 , with n≈1.55 and/or the planarizing resin. The silica and silicon nitride layers are used as dielectric and for passivation in and around the TFT system. Glass,  107 , supports the structure. This is one typical structure in use in the industry, and is also described in Table 1, with thickness also given for each layer. 
     
       
         
               
               
               
               
               
             
           
               
                   
                 TABLE 1 
               
               
                   
                   
               
               
                   
                   
                 Label in 
                 Refractive index 
                   
               
               
                   
                 Material 
                 FIG. 1 
                 (approximate) 
                 Thickness 
               
               
                   
                   
               
             
             
               
                   
                 Color filter (CF) 
                 101 
                 1.50 
                 &gt;10 μm 
               
               
                   
                 ITO 
                 102 
                 1.95 
                 138 nm 
               
               
                   
                 Polyimide (PI) 
                 103 
                 1.70 
                  70 nm 
               
               
                   
                 LC 
                 104 
                 1.53 
                  3 μm 
               
               
                   
                 Polyimide (PI) 
                 103 
                 1.70 
                  76 nm 
               
               
                   
                 ITO 
                 102 
                 1.95 
                 138 nm 
               
               
                   
                 Planarizing resin 
                 108 
                 1.59 
                  2.5 μm 
               
               
                   
                 Silicon nitride 
                 105 
                 2.04 
                 330 nm 
               
               
                   
                 Silica 
                 106 
                 1.55 
                 700 nm 
               
               
                   
                 Silicon nitride 
                 105 
                 2.04 
                 300 nm 
               
               
                   
                 Silica 
                 106 
                 1.55 
                 380 nm 
               
               
                   
                 Glass 
                 107 
                 1.53 
                 &gt;10 μm 
               
               
                   
                   
               
             
          
         
       
     
     The structure described in Table 1 has thicknesses of PI and ITO optimized to minimize total reflectivity by destructive interference. (These thicknesses are within the typical manufacturing range.) The total reflectivity of this structure is 0.104; 10.4% of incident light is reflected by this internal structure. 
     Referring now to  FIG. 6 , extra layers of intermediate refractive index,  601 ,  602 ,  603 ,  604 ,  605  and  606 , can be placed between higher- and lower-refractive index layers. For example,  601  is inserted between the ITO and CF, forming the structure of  FIG. 3  in accordance with the invention, together with the LC and PI. Table 2 describes the case where the layers  601 ,  602 ,  603 ,  604 ,  605  and  606  are polyimide, with n≈1.70. 
     The structure described in Table 2 has thicknesses of PI and ITO optimized to minimize total reflectivity by destructive interference. The total reflectivity of this structure is 0.0091; 0.91% of incident light is reflected by this internal structure. Therefore, using a device in accordance with the invention, wherein polyimide is used as the intermediate-refractive index material, has reduced the reflectivity of this LCD structure by a factor of 11. 
     
       
         
               
               
               
               
             
           
               
                   
                 TABLE 2 
               
               
                   
                   
               
               
                   
                   
                 Refractive index 
                   
               
               
                   
                 Material 
                 (approximate) 
                 Thickness 
               
               
                   
                   
               
             
             
               
                   
                 Color filter (CF) 
                 1.50 
                 &gt;10 μm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  81 nm 
               
               
                   
                 ITO 
                 1.95 
                 138 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  81 nm 
               
               
                   
                 LC 
                 1.53 
                  3 μm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  80 nm 
               
               
                   
                 ITO 
                 1.95 
                 138 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  82 nm 
               
               
                   
                 Planarizing resin 
                 1.59 
                  2.5 μm 
               
               
                   
                 Polimide (PI) 
                 1.70 
                  84 nm 
               
               
                   
                 Silicon nitride 
                 2.04 
                 330 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  77 nm 
               
               
                   
                 Silica 
                 1.55 
                 700 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  75 nm 
               
               
                   
                 Silicon nitride 
                 2.04 
                 300 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  80 nm 
               
               
                   
                 Silica 
                 1.55 
                 380 nm 
               
               
                   
                 Glass 
                 1.53 
                 &gt;10 μm 
               
               
                   
                   
               
             
          
         
       
     
     If the refractive index of layers  601 ,  602 ,  603 ,  604 ,  605  and  606  can be freely chosen, as well as their thickness, the structure of Table 3 results (the question marks in table 3 indicate that materials having appropriate refractive index can be freely chosen). 
     The structure described in Table 3 has refractive indices of layers  601 ,  602 ,  603 ,  604 ,  605  and  606  and thicknesses of PI, ITO and layers  601 ,  602 ,  603 ,  604 ,  605  and  606  optimized to minimize total reflectivity by destructive interference. The total reflectivity of this structure is 0.0050; 0.50% of incident light is reflected by this internal structure. Therefore, using a device in accordance with the invention, wherein polyimide is used as the intermediate-refractive index material, has reduced the reflectivity of this LCD structure by a factor of 21. 
                                     TABLE 3                           Refractive index               Material   (approximate)   Thickness                           Color filter (CF)   1.50   &gt;10 μm           ?   1.68    81 nm           ITO   1.95   139 nm           Polyimide (PI)   1.70    80 nm           LC   1.53    3 μm           Polyimide (PI)   1.70   81 nm           ITO   1.95   142 nm           ?   1.73    82 nm           Planarizing resin   1.59    2.5 μm           ?   1.77    81 nm           Silicon nitride   2.04   330 nm           ?   1.70    86 nm           Silica   1.55   700 nm           ?   1.79    70 nm           Silicon nitride   2.04   300 nm           ?   1.76    75 nm           Silica   1.55   380 nm           Glass   1.53   &gt;10 μm                        
Embodiment 2
 
     It is also possible to remove the silica and/or silicon nitride from the areas through which light is transmitted in an LCD. This is because they are only required around the TFT and circuitry in the device. Light is not transmitted through these regions (it is either reflected by metal or absorbed in the commonly used black mask), and so they can be considered irrelevant for purposes of reducing internal reflections. The silica and silicon nitride can in principle be patterned so that they are only found in these opaque regions, not in the transparent part of the pixel. In this case, the structure is as given in Table 4 and  FIG. 7 . 
     The structure described in Table 3 has the thicknesses of PI and ITO optimized to minimize total reflectivity by destructive interference. The total reflectivity of this structure is 0.015; 1.5% of incident light is reflected by this internal structure. 
     
       
         
               
               
               
               
               
             
           
               
                   
                 TABLE 4 
               
               
                   
                   
               
               
                   
                   
                 Label in 
                 Refractive index 
                   
               
               
                   
                 Material 
                 FIG. 7 
                 (approximate) 
                 Thickness 
               
               
                   
                   
               
             
             
               
                   
                 Color filter (CF) 
                 101 
                 1.50 
                 &gt;10 μm 
               
               
                   
                 ITO 
                 102 
                 1.95 
                 134 nm 
               
               
                   
                 Polyimide (PI) 
                 103 
                 1.70 
                  49 nm 
               
               
                   
                 LC 
                 104 
                 1.53 
                  3 μm 
               
               
                   
                 Polyimide (PI) 
                 103 
                 1.70 
                  60 nm 
               
               
                   
                 ITO 
                 102 
                 1.95 
                 134 nm 
               
               
                   
                 Planarizing resin 
                 108 
                 1.59 
                  2.5 μm 
               
               
                   
                 Silica 
                 106 
                 1.55 
                 380 nm 
               
               
                   
                 Glass 
                 107 
                 1.53 
                 &gt;10 μm 
               
               
                   
                   
               
             
          
         
       
     
     Referring to  FIG. 8 , extra layers of intermediate refractive index,  801  and  802  can be placed between higher- and lower-refractive index layers of the system of  FIG. 7 . For example,  801  can be inserted between the ITO and CF, forming the structure of  FIG. 3  in accordance with the present invention, together with the LC and PI. Table 5 describes the case where  801  and  802  are polyimide layers, with n≈1.70. 
     
       
         
               
               
               
               
             
           
               
                   
                 TABLE 5 
               
               
                   
                   
               
               
                   
                   
                 Refractive index 
                   
               
               
                   
                 Material 
                 (approximate) 
                 Thickness 
               
               
                   
                   
               
             
             
               
                   
                 Color filter (CF) 
                 1.50 
                 &gt;10 μm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  74 nm 
               
               
                   
                 ITO 
                 1.95 
                 122 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  74 nm 
               
               
                   
                 LC 
                 1.53 
                  3 μm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  81 nm 
               
               
                   
                 ITO 
                 1.95 
                 142 nm 
               
               
                   
                 Polyimide (PI) 
                 1.70 
                  83 nm 
               
               
                   
                 Planarizing resin 
                 1.59 
                  2.5 μm 
               
               
                   
                 Silica 
                 1.55 
                 380 nm 
               
               
                   
                 Glass 
                 1.53 
                 &gt;10 μm 
               
               
                   
                   
               
             
          
         
       
     
     The structure described in Table 5 has thicknesses of PI and ITO optimized to minimize total reflectivity by destructive interference. The total reflectivity of this structure is 0.00080; 0.50% of incident light is reflected by this internal structure. Therefore, using the device in accordance with the invention, wherein polyimide is used as the intermediate-refractive index material, has reduced the reflectivity of this LCD structure by a factor of 19. 
     Other Intermediate-Refractive Index Materials AND Embodiments 
     For such use in an LCD, or other system, other materials, organic and inorganic may be found which have an appropriate refractive index. Polycarbonate (n≈1.59), polystyrene (n≈1.59) are two examples of polymers which may be used between some layers. Indium zinc oxide can be deposited with a refractive index of 1.8 (according to U.S. Pat. No. 7,215,075). Additionally, the structure in accordance with the present invention can be utilized in liquid crystal display systems, as well as organic light emitting diode (OLED) display systems and electrowetting display systems. 
     Although the invention has been shown and described with respect to certain preferred embodiments, it is obvious that equivalents and modifications will occur to others skilled in the art upon the reading and understanding of the specification. The present invention includes all such equivalents and modifications, and is limited only by the scope of the following claims.