An improved video display system

FIELD OF THE INVENTION

The present invention relates generally to video display devices and more particularly to an improved video display system employing an active matrix LCD in conjunction with projection optics.

BACKGROUND OF THE INVENTION

Video displays using cathode-ray tubes (CRTs) have been widely used for several decades, although many problems in CRT technology still remain. Picture size is still limited, making group viewing difficult. The actual display units with a picture size of at least 19" (measured diagonally), about the smallest "comfortable" size for family home viewing, remain large and cumbersome, hovering ominously over the room, collecting dust, consuming valuable floor space and creating an aesthetic eyesore. Additionally, a television convenient to watch sitting up becomes inconvenient, to watch from a bed. In addition to these mere inconveniences, health hazards from X-rays emanating from color sets, eye strain related to flicker rate and the dangers of high voltage and possible picture-tube implosion remain problems which have not been adequately addressed.

Image quality problems of CRT-based video displays include color distortion, lowered resolution from the influences of the earth's magnetic field, convergence error, age or misadjustment and decreased resolution due to visual artifacts such as scanning lines, phosphor stripes, and phosphor dots which are inherent in all such TV displays and are particularly visible when viewing at close range. These visual artifacts provide a poorer image quality than images in movie theaters.

"Projection televisions" have been developed and commercialized in recent years. Although such televisions have solved the small viewing screen problem, other existing problems have been exacerbated and new problems have been created. Projection televisions are more expensive than standard, direct-view televisions and are more cumbersome, heavier and larger so that portability is impractical. Two types of projection televisions systems have become popular: one using three CRTs with projection lenses and the other using an oil film scanned by an electron beam.

The CRT-based system remains very dim, requiring a dimly-lit viewing environment and a costly special screen which provides a very limited viewing angle. The three CRTs produce images in the primary colors: blue, green, and red. The oilbased system, often referred to as an Eidophor System has three "scanned oil elements" which have a relatively short life and uses an external light source. In either system, these images must be converged onto the screen to form one color picture. Due to the curvature of the lenses and variations in the performance of the circuits in either system, proper convergence is not easily achieved and sometimes requires up to a half hour of additional setup time. If the projector or screen is moved, the convergence procedure must be repeated. The CRTs are driven with a high anode voltage to obtain as much brightness out of them as possible. Increasing the anode voltage further increases the X-ray hazard and lowers tube life and other problems associated with high voltage. The three tubes increase the danger of tube implosion.

Many attempts have been made through the years to solve the above-mentioned problems by using a "light valve" based system. This type of system uses an external light source which can be as bright as desired, with a light valve to modulate the light carrying the picture information. The research and experimentation to develop a workable light valve has been focused upon using different optical effects, coupled with physical effects and finding or producing various materials to accomplish the desired effects in a light valve. With the exception of the oil scanning type of system, no other light valve system has proven feasible or economically viable. Experimentation has also been performed on a laser system which scans out an image on a viewing screen in the same way an electron beam scans the image onto the face of a CRT. The laser system is much too large to be portable, very complex to use and maintain, extremely expensive, very dangerous and has proven too dim for large images. The various light-valve system attempts have mainly utilized: crystals, such as quartz, Potassium Di-Hydrogen Phosphate, Lithium Niobate, Barium Strontium Niobate, Yttrium Aluminum Garnet, or Chromium Oxide; or liquids such as Nitro Benzene; or liquid crystals of the smectic or nematic type; or a suspension of particles such as iodoquinine sulphate in a liquid carrier. These and other similar materials have been used to capitalize on one or more optical effects including: electro-optical effects such as creating a rotated plane of polarization or altering the index of refraction of the material due to an applied electric field, magneto-optical effects using an applied magnetic field, electro-striction effects, piezo-optical effects, electrostatic particle orientation, photo-conductivity, acousto-optical effects, photochromic effects, laser-scan-induced secondary electron emission, and various combinations of these effects. Unfortunately, such light valves have proven impossible to manufacture inexpensively, in large quantities and with a large aperture and have often been toxic, dangerous and inconsistent in production quality.

In all light valves, different areas must be supplied different information so that a different amount of light would emerge through each area, adding up to a complete picture across the total beam of light. This required the materials to be scanned by a laser or electron beam or for a tiny criss-cross of electrically conductive paths in the form of a matrix to be deposited on or adjacent the material to be addressed. In scanning beam systems, problem included outgassing, erosion of material and image information loss due to the bright and hot illuminating light. The electrical matrix system has proved difficult to engineer, requiring good conductivity characteristics with extremely fast switching circuits, which were impractical at the high voltages required to activate a given area of material. The main system (developed to address small areas) which has shown promise is often referred to as electronic multiplexing.

Electronic multiplexing only works with low voltage requiring materials such as liquid crystals. With this method, all pixel addresses are x and y coordinates on the conductive grid. To activate a given pixel area a specific amount, different voltages must be applied to the x and y conductors so that, where they meet, they together exceed a threshold and modulate the area. A major drawback to such multiplexing is crosstalk, where surrounding areas are affected by the local electric field, causing false data to influence surrounding pixels. Crosstalk is also a problem with electron and laser scanned materials and reduces contrast and resolution as well as color saturation and accuracy. Since these light valves have very little persistence and one pixel area is activated at a time, substantially less light passes through the screen to ultimately arrive at the viewer since all pixels are "off" most of the time which wastes light, produces a dimmer image with poorer contrast, and generates more heat because of the brighter source necessary to compensate. High refresh rates are impractical because that would require faster switching times and faster responding material.

"Pocket TVs" are constructed today using the electronic multiplexing technique, but because the picture is small, the light source bright and the ambient conditions restricted, these defects are not very noticeable. However, when an image is projected, the defects are greatly magnified and become unacceptably noticeable as the large pixels form very noticeable squares and rows detracting from image quality. Contrast is then also noticeably very low - ie. no "black" is possible. To further decrease contrast, the bright, hot lamp could heat up the LCD, causing a "hot spot" in the center of the image, spreading out in a Gaussian-like pattern. This lowers contrast further. Color rendition is also measurably poorer in pocket TVs than with a CRT.

JP-A-60 179 723 discloses a liquid crystal projection device comprising an LCD having a plurality of pixels arranged in a matrix for forming an image; a solid state pixel control element associated with each pixel for storing a respective pixel control signal; and means for projecting the image formed by the LCD onto a viewing area.

SID International Symposium, Digest of Technical Papers, Vol. XVIII, May 1987, pages 75 to 78, discloses a high-resolution full-colour video projector with poly-Si TFT array light valves.

According to the present invention there is provided a light valve display system, comprising: <ul id="ul0001" list-style="none" compact="compact"><li>a light source; and at least one light valve,</li></ul>    characterized in that <ul id="ul0002" list-style="none" compact="compact"><li>the system further comprises an optical system for eliminating the appearance of disjointed red, blue and green areas and of spaces between adjacent pixels in the displayed image formed by said at least one light valve, and that said optical system includes a plurality of optical elements located downstream of said light valve and acting on the pixels in such a way that the disjointed red, blue and green areas disappear and the dead spaces between the adjacent pixels are eliminated.</li></ul>

The present invention makes it possible to provide an adjustable size video image which can be very large, yet possess high quality and sufficient brightness to be visible in a normally lit room. A display is possible which has high resolution and contrast, with more accurate color rendition approaching that of a CRT, while reducing the strain associated with flicker and eliminating the appearance of stripes or pixels.

The system of the invention preferably uses an "active matrix" for electronically addressing and activating each of the liquid crystal elements in the matrix. The matrix is "active" in that a separate transistor or other suitable semiconductor is deposited adjacent to each picture element or "pixel" to store the respective pixel control signal.

The method of eliminating the clear spaces between adjacent pixels is to fill them using a 4-mirror system, in which a first striped mirror pair duplicates each pixel and the image is shifted horizontally into the spaces which previously existed between pixels. A second mirror pair duplicates the newly created rows of pixels and shifts the original and the duplicated pixel images vertically to fill the remaining spaces between pixels.

Other methods are described of filling spaces between adjacent pixels through the use of an expanding lens array and a collimating lens or a second collimating lens array to expand and collimate individual images of the pixels.

The invention will be better understood by the Detailed Description of the Preferred Embodiment in conjunction with the appended drawings, of which:

Brief Description of the Drawings

<dl id="dl0001"><dt><u>Figure 1</u></dt><dd>is a schematic view of an arrangement for causing disjointed red, blue and green areas to disappear, for use in the invention, the arrangement comprising three LCDs projecting their image onto one common screen;</dd><dt><u>Figure 2</u></dt><dd>is a schematic view of a modified form of the arrangement of Figure 1, in which the images of three LCDs are internally superposed and projected onto a common screen employing one set of projection optics;</dd><dt><u>Figure 3</u></dt><dd>is a schematic view of various pixels with reduced spaces between them, and is not according to the invention;</dd><dt><u>Figure 4</u></dt><dd>is a schematic view of a projected image of superposed "full color pixels";</dd><dt><u>Figure 5</u></dt><dd>is a schematic view of four-mirror system depicting a method of filling in spaces between adjacent pixels, for use in the invention;</dd><dt><u>Figure 6</u></dt><dd>is a schematic view depicting the filling of spaces between pixels by the first two mirrors (a "striped-mirror pair") of the four-mirror system of Figure 5;</dd><dt><u>Figure 7</u></dt><dd>is an enlarged schematic view of a "striped-mirror pair" of the four-mirror system of Figure 5;</dd><dt><u>Figures 8a and 8b</u></dt><dd>are schematic views of embodiments of lens-systems for eliminating dead spaces between adjacent pixels, for use in the present invention;</dd><dt><u>Figure 9a</u></dt><dd>is a schematic view of a dichroic mirror system of the preferred embodiment of the present invention;</dd><dt><u>Figure 9b</u></dt><dd>is a schematic view of the embodiment of the dichroic mirror system of Figure 9, modified to include an additional light path;</dd><dt><u>Figure 10</u></dt><dd>is a graphical plot of transmitted light intensity over the visible spectrum through two full color LCDs, one with a constant LCD cavity thickness contrasted with a "stepped thickness" LCD cavity;</dd><dt><u>Figures 11a and 11b</u></dt><dd>are graphical plots of transmitted light intensity vs. applied voltage for three wavelengths used in two full-color LCDs, one for a constant thickness LCD cavity and one for a "stepped thickness" LCD cavity;</dd><dt><u>Figure 12</u></dt><dd>is a magnified schematic view of a "stepped thickness" LCD cavity showing the different thicknesses of LCD that red, green, and blue light traverse through;</dd><dt><u>Figure 13</u></dt><dd>is a CIE chromaticity diagram comparing color ranges of a CRT display, a conventional color LCD display with a fixed cavity thickness and a "stepped thickness" LCD cavity;</dd><dt><u>Figure 14</u></dt><dd>is a schematic view of a rear-screen projection system utilizing the present invention with a venetian-blind type of rear-projection screen;</dd><dt><u>Figure 15a</u></dt><dd>is a schematic view of color filters on corresponding color-pixel areas in a full-color LCD;</dd><dt><u>Figure 15b</u></dt><dd>is a schematic view of an alternate arrangement of pixels in which three pixels of a color triad are indicated by a triangle; and</dd><dt><u>Figure 16</u></dt><dd>is an open perspective view of a sound suppression system which may incorporated in the system of the present invention.</dd><dt><u>Figure 17</u></dt><dd>is a schematic diagram of the preferred embodiment of the invention.</dd></dl>

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

Of all video display systems researched and operated thus far, the one that shows the greatest potential for solving the above-mentioned problems is an LCD display system, utilized in transmissive or reflective mode, taking advantage of the polarization/rotation or scattering capabilities of liquid crystals, with a conductive matrix for addressing. Various changes must be made to current video display designs, which use electronic multiplexing, to eliminate the current problems.

Although present LCD TV displays using electronic multiplexing produce a satisfactory small image, when such images are projected to a large picture, the transmitted light never reaches to zero, causing low contrast. Additionally, with electronic multiplexing, crosstalk and electronic "bleed through" to neighboring pixels reduces resolution and color fidelity. If a picture is to be a mosaic of red, blue and green pixels, each pixel must acquire a precise amount of current to reproduce the brightness of each picture element's originally broadcast brightness, as well as its color rendition. Additionally, light is wasted and the picture appears dim with each pixel being turned on for only part of a scanning field. The image cannot be refreshed and so flicker, as well as brightness efficiency, is dependent on the persistence of the LCD, which is not adjustable.

Consequently, applicant has proposed a new idea for a light valve projection element. This idea involves the deposition of a thin film transistor next to each pixel, creating an "active" rather than "passive" matrix. Instead of present day multiplexing, each transistor would receive a voltage level which can be stored there until changed, creating a simple "transistor memory" for each pixel. This way, each pixel can be addressed, turned on (to transmit or reflect light) and will remain on until data for the next frame is presented. With this system, no interlaced scanning need be used and flicker can be eliminated. Each pixel will be on for the entire length of a frame, immediately changing to the appropriate level of transmissivity or reflectivity for the pixel in the next frame. Each pixel will be on (the desired amount) all the time, allowing the highest throughput of light from the external light source.

This "active matrix" will allow more brightness and less heat for a a given level of brightness. Addressing each transistor separately and letting the transistor determine the current to each pixel, in addition to introducing some "dead space" between pixels, assures that each pixel receives the correct amount of current without any crosstalk from neighboring pixels. By allowing for a "dead space" between pixels, necessary for the placement of the transistor (in the area of liquid crystal "overlap" where electric fields from neighboring pixels could co-mingle and produce false data, reducing contrast and distorting the color mix) eliminates the crosstalk problem. Placing an opaque black covering over these areas serves at least two purposes: it stops passage of improperly modulated and un-modulated light from passage to the screen; and protects the transistor from damage due to irradiation from the intense light and heat. This area may be a fraction of the size of a pixel. The 5 use of such a thin film transistor active matrix modulation system eliminates many of the problems concerning contrast, brightness, flicker, and color rendition. State of the art methods of deposition of semi-conductor material can be utilized to mass-produce this system.

This new LCD light valve is used in conjunction with projection optics. In the preferred embodiment of the invention, depicted in Figure 17, a light source 1700 is collimated by collimating optics 1710, which 5 could comprise a spherical or parabolic reflector 1720, a condensing lens 1730, and collimating lenses 1740. The LCD light valve 1750 is illuminated by this collimated light, creating a full-color optical image thereupon. Projection optics 1780 then focusses this image on a viewing surface, 1790. To improve the quality of the projected image as explained further herein, subsystem 1760 is used to superpose pixels of color triads forming full-color pixels with spaces between them. Further, subsystem 1770, also explained herein is then used to fill in the spaces between pixels. A source of lowered resolution, contrast, and the fidelity of color and gray levels is heat generated by the required projection bulb. The heat, like the light, irradiates the LCD in a Gaussian-like pattern, causing a "hot spot" in the center of the LCD. Excessive heat could damage the LCD. If the damage threshold is not reached, image degradation, as just described, could still occur because the LCD expands, increasing the distance light must travel through the LCD. This increases the scattering on the rotation of the plane of polarization of the light passing through, throwing off contrast, resolution, color and gray rendition in a Gaussian-like pattern.

Several steps may be taken to deal with the detrimental effects of heating of the LCD. First, all optics, including the LCD, should be mounted with good contact to large heat sinks, as is done, for instance, with power transistors. Additionally, all optics can be coated with material of proper thickness, such as is done for dichroic reflectors, to reflect the infrared (IR) spectrum. IR reflecting mirrors and heat absorbing glass can also be used in the optical path. Additionally, a fluid means such as a liquid or gas in a container, allowing large bodies of index-matched high-boiling-point fluid (liquid or gas), circulating within a contained area or static can be used for further cooling. Alternatively, instead of transmissive optics, metal reflective optics can be utilized for further heat sinking and to suppress reflection at IR wavelengths (with anti-reflection coating for the IR).

The simplest measure that can be taken to cool the LCD, as well as the other components of the system, is the use of a cooling fan or fans. However, a fan can pose a noise problem when the audio volume of the system is at a very low level, particularly in a small room. To suppress the noise, an "air baffle" may be used between the fan and the outlet of the housing of the invention. Figure 16 shows the sound suppression system, comprising fan 1600 resting on platform 1620. The addition of airflow blocker 1630 forces the air to traverse a curved path with deflection prior to exiting the housing through outlet 1640. The surfaces from which the air reflects are covered with sound absorbing materials, greatly reducing the noise entering the listening environment. Since some noise will still be present at outlet 1640, a further measure may be taken for noise reduction. This measure comprises microphone 1650 which picks up the remaining noise, sends it to an amplifier which inverts the phase of the noise by 180 degrees. The inverted noise is played back through speaker 1660. By properly adjusting the volume and phasing of the amplifier, the remaining perceived fan noise could be substantially reduced and made practically inaudible.

Depending upon the brightness of the source utilized and the physical and economic constraints of a given system, some significant Gaussian-like heat pattern could remain at the LCD and could change with time as overall heat builds up during operation. Consequently, an electronic approach can be utilized in addition to eliminate the problem and lower the magnitude of the other remedies recited. Since the degree of rotation of the plane of polarization of the light is not only dependent on the thickness of the LCD that it passes through, but also upon the amount of applied electric field, modifying the electric field in opposition to temperature effects will cancel the distortion, resulting in uniform performance across the LCD. This amounts to a bias voltage, applied differently to different pixels which is distributed in a Gaussian-like pattern and is controlled by the individual transistors and/or the addressing circuitry. A thermistor or other temperature-sensing device, placed at the LCD, can monitor overall average LCD temperature, adjusting the Gaussian-like bias voltage distribution as the temperature fluctuates, using an electronic servo-circuit. For even more accurate temperature control, a thermistor-type device can be deposited next to each pixel transistor in the space between the pixels, to independently control the heat-compensating bias of each pixel.

A simple, compact, and inexpensive, full-color television projection system, may be constructed using a single "full-color" LCD. Full-color, direct-view-video image display, not using projection, has been accomplished with a single "full-color" LCD. When this image is enlarged by projection however, several problems become very apparent.

In a standard CRT based TV system, red, blue and green pixel data are sent to adjacent red, blue and green phosphor spots on the CRT face. Analogously, in a direct-view LCD TV system, red, blue and green pixel data are sent to adjacent areas of the LCD. These areas are then covered by red, blue and green filters to appropriately color the light passing through those LCD pixel elements. Figure 15a depicts a simple arrangement of color filters on corresponding color-pixel areas in which pixels of a given color are located above one another creating vertical color stripes. Three horizontally adjacent pixel areas make up a triad which represents a single color pixel from the actual image. Figure 15b depicts an alternate arrangement of pixels in which the three pixels of a color triad are arranged to form a triangle. Such small, closely packed red, blue and green spots of light create the illusion of color in a scene as they are supposed to appear. However, when this image is magnified by projection, each adjacent red, blue and green pixel no longer merges to produce properly colored areas. Instead, they appear as disjointed red, blue and green areas, detracting from the appearance of a naturally colored image. Furthermore, the spaces between adjacent pixel areas in the LCD which allow for the deposition of thin film transistors necessary to create an "active matrix" are magnified as well, further creating a disjointed, disruptive, unnatural looking image.

The elimination of the appearance of disjointed red, blue and green spots instead of actual colors, which is one of the features of the optical system used in the present invention, can be achieved by the use of a dichroic mirror system as depicted in Figure 9a. Assuming the pixel arrangement of Figure 15a, individual red, blue and green pixels can be made to overlap by the following arrangement. Collimated light 901 passes through the full-color LCD 902 and hits dichroic mirror 903 which reflects only the blue image. The remaining red and green images pass through dichroic mirror 903, hitting dichroic mirror surface 904 which reflects only the red image, allowing the green image to pass through. The blue image reflects off front surface mirrors 910 and 911 and then off dichroic mirror surface 905 which reflects only blue light. Here the blue image rejoins the green image. By adjusting front surface mirrors 910 and 911, the blue pixels can be made to overlap the green pixels. The red image reflects off front surface mirrors 920 and 921 and then off dichroic mirror 906, which only reflects red light. At this point, the red image rejoins the blue and green images and by adjusting front surface mirrors 920 and 921, the red pixels can be made to overlap the already joined blue and green pixels. At this juncture, we have a full color image with large spaces between pixels as illustrated in Figure 4.

If individual colored pixels are arranged on the LCD as shown by Figure 15b, in which a color triad forms a triangle, bringing the red and blue pixels together as just described will not allow them to superimpose on top of the green pixels since the green pixels are vertically displaced from their corresponding red and blue pixels. Consequently, this type of pixel arrangement requires an additional dichroic mirror path similar to the paths used by the red and blue light. This is depicted more clearly in Figure 9b, which is a side view of the system in Figure 9a modified to include an additional light path.

Collimated light 901 passes through full-color LCD 902 as before. However, the distance between LCD 902 and dichroic mirror 903 is increased to allow for the insertion of dichroic mirror 950 which reflects green light and transmits red and blue light. As before, 903 reflects blue light and transmits red light. Now, mirror surfaces 904 and 905 are front surface mirrors. Mirror 906 reflects red light and transmits blue light. As before, mirrors 910, 911, 920 and 921 are front surface mirrors. In addition, mirrors 960 and 970 are also front surface mirrors. Mirror 980 is a dichroic mirror which reflects green light and transmits red and blue light. By this modified arrangement, proper separation of mirror 910 from mirror 911 and separation of mirror 920 from mirror 921 will still cause the overlap of the red and blue pixels. Additionally, proper separation of mirrors 960 and 970 will cause the green pixels to overlap the already joined red-blue pixel pair. This overhead mirror arrangement may also be used with the color LCD whose pixel arrangement is as depicted in Figure 15a with the spacing between mirrors 960 and 970 adjusted to prevent vertical displacement of the green pixels since they are already in line with the red and blue pixels. The separate mirror path for the green light makes the distance traversed by each color through the system equal, which is important because the light, although collimated, still expands somewhat with distance traveled. Consequently, if different color components traversed different distances, then when they are rejoined into full-color pixel images, the color component with the shorter path would create an image of a pixel that smaller than the image of the other colored pixels, creating a poorer quality color image. Now (and this is true of both Figure 9a and Figure 9b) the image can pass through 930 which is either the "striped mirror pair" system or the lens array system described hereafter to fill the spaces between pixels for final projection by projection optics 940. This is another feature of the optical system used in the present invention.

This combined system to superimpose corresponding color pixels to form "full-color pixels" and then filling in spaces between pixels by enlargement or duplication of pixels could also be equally useful on a CRT-based video projector to improve the subjective resolution.

Various other combinations should now be obvious such as using three full color LCDs in a projection system where the red pixels of one LCD overlap the green pixels of a second LCD which overlaps the blue pixels of a third LCD. This also creates full-color pixels, eliminating the need for the mirror system of Figure 9. The 3 LCD system allows three light sources (although one could be used) for triple the brightness and is depicted in Figure 1.

Figure 1 shows three LCDs, one displaying red 110, one green 111 and one blue 112 picture data, each illuminated with light of the appropriate color (100, 101, 102). The red light from source 100 is collected by condenser 120 and collimated by collimating optics 130. Projection optic 140 focuses a red picture on screen 150. Similarly the green and blue images are projected and made to converge on the screen, forming a full color image. The disadvantage of the full color system employing 3 LCDs is that adjustments must be made to the optics to converge the images whenever the projector or screen is moved. This problem is eliminated by the use of dichroic mirrors and a single projection lens as shown by Figure 2. Red image information from LCD 200 reflects off front-surface mirror 201 to dichroic mirror 204 which reflects red light but passes blue and green light. Blue image information from LCD 220 reflects off front surface mirror 202 and then off dichroic mirror 203, which reflects blue but permits green light to pass, and then passes through dichroic mirror 204. Green image information from LCD 210 passes through dichroic mirrors 203 and 204. Thus, a totally registered full-color image is projected by projection optics 205 to form an image on screen 206. Convergence is always perfect, regardless of repositioning of the projector or screen. Of course, a plurality of monochrome and/or full color LCDs could be used to produce a video display. The disadvantage of using a plurality of LCDs to the increased cost of the multiple LCDs.

With either one lens or three, the three images can be slightly offset to fill the spaces between pixels. As an example, see Figure 3 wherein blue pixel 301 may be slightly higher than red pixel 302 and green pixel 303 can be slightly to the left of each red pixel 302. Many other arrangements of offsets of the different colored pixels are possible and all serve to decrease black spaces in the image, but at the same time, the individual colors become more visible at close range (Figure 3 and such other arrangements are not within the scope of the claimed invention.) Although such an image may be acceptable, a better solution, whether one or more LCDs are used, is to have all pixels exactly superimposed in triads (red, green and blue together forming "full-color pixels") with spacing between such pixel triads (arranged by proper LCD manufacture), preferably, although not necessarily, to be equal to the dimensions of a pixel. Then the pixel images can be duplicated or expanded to fill the spaces exactly, creating a "continuous image". In Figure 4, each pixel 401 is a superposition of a corresponding red, blue and green pixel. 402 represents spaces which need to be filled.

Whether a "full-color" LCD or multiple "mono-color" LCDs are used, the use of an "active matrix" could increase the space between pixels. A preferred method of filling the spaces is by the proper use of mirrors. To make a mirror system that duplicates the pixels in the proper places with minimum waste of light, a special "striped-mirror system" can be used. One such configuration is shown in Figure 5. Light containing full color image information 501 (laid out as indicated in Figure 4) hits a "striped mirror pair" labeled as 502 and 503. This causes the entire image to be duplicated and shifted horizontally the width of one pixel with approximately one-half the brightness of the original image (which is also reduced to one half of its original brightness), filling the spaces between pixels in the horizontal rows as shown by Figure 6. Vertical rows 601A, 602A, and 603A are duplications of vertical rows 601, 602 and 603 respectively. The combined (original and duplicated) image existing in space 504 of Figure 5, then passes through a second "striped mirror pair" 505 and 506, which duplicates the image but shifts it vertically the height of one pixel, producing two images of equal brightness, one above the other, filling in the horizontal rows indicated in Figure 6 as 610, 611, and 612. Thus a "solid" image is created with no blank spaces. Eliminating blank spaces, separately colored pixels and the distinction between pixels improves image resolution even above today's CRT images at close range, since CRTs have discernable lines, pixels, and spaces.

A "striped mirror pair" is better understood by reviewing Figure 7. Light from a single pixel 701, impinges upon a "clear" space 720 on the first mirror 702 of the mirror pair. This first mirror is made of glass, plastic, or other suitable material which is AR coated over the visible spectrum and coated on its opposite side in stripes of a suitable reflective material such as aluminum or silver. The striped coating may be accomplished by, for instance, vacuum deposition with a "striped mask over the glass". Alternatively, the glass can be coated with photo-resist and exposed to a projected image of stripes of the desired size. After development, the glass will be exposed for metal vacuum deposition only in the desired stripes. After deposition, the remaining resist could be peeled or dissolved away, leaving the required clear stripes.

The second mirror 703 of the pair also has alternating clear and reflective stripes. On this mirror however, the reflective coating is thinner, creating partial mirrors instead of full mirrors. The percentage of reflectivity is adjusted so that the two pixel images which emerge are of equal brightness.

Light from pixel 701, after passing through space 720, impinges on partial mirror 730, creating a transmitted beam 710 and a reflected beam which hits mirrored surface 740 on first mirror 702. This reflects light through clear space 750 on mirror 703 creating a second beam 710a which is an exact duplicate of beam 710, except that it is contiguously displaced from beam 710. If the spacing between pixels is not equal to the dimensions of a pixel, the mirrored areas 740 on mirror 702 as well as clear spaces 750 on mirror 703 may be adjusted to the dimensions of the space between pixels.

The overhead view of Figure 5 shows that "striped mirror pair" (502, 503) which has vertical stripes, is tilted with reference to beam 501 around a "vertical tilt axis" to create a horizontally displaced duplicate image, and "striped mirror pair" (505-506) which has horizontal stripes, is tilted around a "horizontal tilt axis" (which is perpendicular to the tilt axis of the first "striped mirror pair" and to the beam 501), so as to create a vertically displaced duplicate image.

An alternate method of elimination of spaces between pixels, using lenses instead of mirrors, may be used. The alternate method would be especially useful if the spacing between pixels were any different from the dimensions of the pixels. For example, assume that the spacing between pixels was a little larger than the dimensions of a pixel. A lens array 801 (as shown in Figures 8a and 8b) constructed with the same number of lenses as there are "full color" pixels (the number of color "triads" on the LCDs arranged with the center of each lens over each pixel, 802) could be used to magnify each pixel as depicted in Figures 8a and 8b. Then, either a collimating lens array 803 as depicted in Figure 8a or a large collimating optic 804 as depicted in Figure 8b could be used to re-collimate the now enlarged and contiguous pixels for projection by suitable projection optics.

If the spacing between pixels varies from the pixel dimensions differently in the vertical than the horizontal, anamorphic lenses would be needed to fill the spaces properly. Although fabrication of small lens arrays is within the state of the art, it is far simpler and less expensive to use more readily available lenticular lenses. These cylindrical lens arrays can be overlapped with their axes perpendicular to one another to accomplish the same goal. The separation of lens function for each orthogonal dimension eliminates the need for anamorphic lenses which are difficult to reproduce accurately and consistently in such small sizes.

Making a "full-color" LCD creates another problem which, although not very noticeable on small displays, creates major problems on a large display. This problem results in a poor contrast ratio and poor color fidelity. To understand and correct the resulting deficiencies, the working of a full-color LCD display must be carefully analyzed.

The following discussion explains the nature of the problem. The transmitted light intensity (TI) from a twisted nematic liquid crystal device, under no applied voltage, with a crystal thickness (d) for any given wavelength (λ) is dependent on the refraction anisotropy (Δn) and the liquid crystal twist angle (θ). TI can only equal zero for a few unique simultaneous combinations of values for these parameters. This means that, except for very specific combinations of wavelength (λ) and thickness (d) for any given crystal, zero transmitted intensity or true "black" will not occur. Thus, if the anisotropy, twist angle, and crystal thickness are fixed, as they are in a conventional LCD (consisting of liquid crystal between two flat plates), only one color can go to black at a time. If a voltage is applied, changing the twist angle, then a different color can go to black. This nonlinearity eliminates the possibility of true contrast in all colors simultaneously; and since perceived color is produced by addition, this eliminates true color fidelity. To further illustrate, the dashed curve of Figure 10 shows the transmitted intensity over the visible spectrum of a standard full-color LCD with a given thickness. Figure llA shows the non-linear transmittance variations for the three wavelengths used in a full-color LCD of uniform thickness plotted against the voltage. When red transmission is at a minimum, for instance, blue transmission is over 10 percent and green transmission is about 5%. Having no true black results in a low contrast ratio, which is one of the main problems with today's LCDs. To solve this problem, the crystal thickness (the space between the plates encasing the liquid crystal) can be selected under each color filter such that at exactly zero volts, the proper rotation is imposed on the polarized light for the specific wavelength transmitted by that color filter. By doing this for each of the 3 sets of color filters used, the minimum amount of light for each color will be transmitted with no voltage applied. This will provide a blacker black and thus, a higher contrast. This result is accomplished if stepped deposition or etching of one plate is done to produce steps as illustrated in Figure 12.

By using an LCD cavity with such a "stepped thickness" cavity, the crystal thickness-wavelength combination will allow true black for all three colors simultaneously and a linear relationship between applied voltage and transmitted intensity for all colors simultaneously. This is demonstrated by Figure 10 (solid line) where transmission is nearly zero for all colors simultaneously with no voltage applied; and in Figure 11b where the transmission for all colors vary with voltage simultaneously.

In applicant's demonstration model, using a "stepped thickness" cavity results in a contrast ratio as high as 100:1 and color fidelity approaching that of a CRT. This high color fidelity can be seen in the CIE diagram of Figure 13 in which the dashed line represents the chromaticity of conventional multi-color LC displays, the dotted line represents the chromaticity of an LC color display with varying crystal thicknesses and the solid line represents the chromaticity of a conventional CRT.

Many projection formats can be used in conjunction with the disclosed video display systems. In addition to curved, direction-sensitive, high reflectance screens, less expensive, more widely dispersive screens can be used with this system. A regular movie screen or even a wall proves adequate with a system of such high brightness. By vertical mounting of the unit or the attachment to the projection lens of a front-surface mirror, the image can be displayed on a bedroom ceiling, for instance. This technique, never before possible, allows for convenient viewing of video imagery while lying in bed, without causing neck or back strain.

Rear-screen projection can be achieved as well. Conventional rear-screen television requires a lenticular lens and a Fresnel lens for adequate brightness. This adds a discernable pattern to the image and produces a limited angle of viewing horizontally and vertically. This type of screen, like a conventional CRT, reflects ambient light to the viewer, creating glare which adds to the viewer's eye strain. With the present system, brightness is much higher, allowing for less stringent screens as well as more streamlined, lightweight and aestheically pleasing display units.

An example of a more artistic and futuristic projection system is illustrated by Figure 14. The video projector 1401 can be mounted to an upright 1402 projecting an image onto a mirror 1403. Mirror 1403 can reflect the image to focus onto a special rear screen 1404 mounted in a frame which appears to be "hanging in space". The screen itself can be made of extremely thin slats 1405 of almost any rear projection material. By mounting an axle onto the ends of each slat with a gear on each, a motor drive can be used to open (lie flat, parallel to the floor) and close the slats (perpendicular to the floor, creating a solid, rear-screen for projection). In the open position the screen will appear as a transparent window in space. When the projection unit is turned on, by remote control, for instance, the slats can simultaneously and quickly close, creating a "video image in space".

Whatever projection method is used, two other important problems exist. Unless the surface being projected upon is perpendicular to the optical axis of the projection beam, the image will suffer from keystoning and blurring of the parts of the picture not precisely focussed on the screen surface. This problem is inherent if the projector is mounted on the floor, on a low table or on the ceiling and the screen is centered on a wall. CRT systems handle keystoning by varying the electromagnetic scan line deflection. The disclosed LCD based system however has pre-defined pixel locations, and thus cannot utilize this technique.

Consequently, a type of anamorphic lens system can be constructed. A zoom lens normally changes the size of a projected image by changing the relative positions between the elements of the projection optics. However, this could also be accomplished if lens elements of different curvatures were used. In the present application, a lens is proposed which has added to it two varying focal length lenses, one above and one below the standard lens, all molded into one lens. The central area of the lens, large enough to magnify the entire LCD, creates a square projected image. But if this lens is raised or lowered with respect to the LCD, the magnification varies, causing a trapezoidal image magnification with either the top or bottom of the image of the LCD being the largest side of the trapezoid. Thus, the lens is adjusted up or down, depending on the angle the video projector is making with the screen and thereby the keystone effect is cancelled.

The variable focus problem can be corrected by a little-known photographic technique known as "Scheimflug correction." If a scene to be photographed has a large depth and a fairly large aperture is used, the only way to get all elements of the scene in focus is to tilt the lens and film plane such that a line drawn through all objects in the scene intersects the line drawn through the film plane at the same point that it intersects a line drawn through the lens plane. Using the same logic, a mechanical adjustment that tilts the LCD plane and the plane of the projection optics, creating an intersection with a line passing through the screen plane, will cause the entire image to be in focus, even though the projector's beam is not perpendicularly aimed at the screen.

The present invention lends itself to three-dimensional video projection. One method of accomplishing 3-D projection is to use two projection systems with the polarizers of one LCD system perpendicular to the polarizers of the other LCD system. Sending stereoscopic video signals, derived from two displaced cameras for instance, and projecting onto a non-depolarizing screen will allow viewers wearing polarized glasses to see full color 3-D video. A single lens 3-D video projection system can be constructed by placing both LCD systems in one enclosure. Instead of using the second mirror 503 of the first "striped mirror pair" 502 and 503 of Figure 5, the horizontally displaced spaces between the pixels of one LCD can be filled by the pixels of the other LCD through a simple beam splitter setup, creating a horizontally interlaced, orthogonally polarized 3-D image pair for projection through the single projection lens. Striped mirror 502 can be tilted at a 45° angle with respect to the axis of the light coming from the first LCD. The light from the pixels of this LCD will pass through the clear areas of the striped mirror. The second LCD, whose axis is perpendicular to the axis of the first LCD, reflects its light from the mirrored areas of the striped mirror, causing an interlaced composite image made from both images, with orthogonal polarization.

Another method of 3-D projection which can be used is rear-screen auto-stereoscopic 3-D projection. This method doesn't require any special glasses for 3-D viewing. Two identical lenticular lens screens, placed backto back with a thin translucent screen between them are projected upon at different angles by two or more such video projectors, bearing stereo or multiple-angles-of-view information. The images can be viewed from the opposite side of the screen at various locations in space. As one moves to various locations, around the screen, the images are viewable, one at a time, without image overlap. This creates several orthoscopic as well as pseudoscopic viewing zones in space. If one positions his eyes in an orthoscopic viewing zone such that one image goes to each eye, a 3-D view will be visible. Many viewers will be able to view an orthoscopic 3-D video image from several angles at once.

The systems disclosed in this application all use discrete, individually addressed and maintained (electrically) pixels. This approach provides the basis for true digital television, which does not exist today. Presently, both audio and video signals are digitized and stored as digital bits on laser disks and "CSs." This digitization preserves the exact values of the signal from micro-second to micro-second. Distortions in the systems such as amplifier noise and non-linearity, scratches, dropout, and other defects on the recording material, ghost signals, and so on can be completely ignored by a system only looking at each bit to see if it is on or off- a "0" or a "1", and not caring if it varies in strength or clarity. However, once the digital data is read, and amplifiers and the heart of today's video systems - the CRT - must utilize an analog signal, reintroducing noise and false data, degrading the quality of the image. The basis of a CRT is an electron beam scanning a phosphor, varying its strength in an analog fashion as it goes. By contrast, the present invention is actually a digital computer on each pixel, best operating in a digital mode. This will result in more precise, higher quality television and video display. The upcoming thrust toward High Definition Television should move the field toward this type of a digital display device as the system of choice. To increase resolution, one only needs to increase the number of pixels just as a computer RAM is increased by adding more chips. In summary, the present invention makes possible a viable basis for implementation of digital and High Definition TV, regardless of the format convention selected.

While the preferred embodiment of the invention have been illustrated in detail, modifications and adaptations of such embodiments will be apparent to those skilled in the art.