The present invention relates generally to displays and, in particular embodiments, to a rear projection display using laser excited photoluminescence.
A conventional CRT display uses a raster scanned electron beam to excite individual phosphors on a screen. A plasma display uses individually addressed cells in which an electric discharge (plasma) is used to excite a red, green, or blue phosphor. The plasma display generates images of exceptional saturation and brightness but suffers from poor energy efficiency relative to other display technologies. An LCD display uses individually addressed light valves to deliver red, green, or blue illumination to each pixel from a backlight. Each of these technologies uses a means to illuminate an individual subpixel within an image.
A MEMS device uses individually addressed mirrors or transmissive elements to project the pixels on the display surface. In one embodiment, the entire MEMS device is illuminated sequentially with either red, green or blue, and individual pixels are addressed to project a specific color pattern. The illumination source can either be white light, such as from a high pressure gas discharge source; red, green, and blue LEDs; or red, green, and blue lasers.
The MEMS device is generally much more energy efficient than other technologies, and is highly cost effective in larger screen sizes. However, lower manufacturing costs have favored the LCD technology in the most popular screen sizes.
In one aspect, the present invention provides a novel display technology using a scanning infrared laser to excite individual red, green, and blue subpixels in a rear projection architecture.
In a first embodiment, a display system includes an optical light source, such as a laser, and a display panel with an array of optically excitable pixels. Optics are positioned between the optical light source and the display panel so as to direct light from the optical light source toward the display panel to cause the optically excitable pixels to emit a visible image.
For a more complete understanding of the present invention, and the advantages thereof, reference is now made to the following descriptions taken in conjunction with the accompanying drawings, in which:
The making and using of the presently preferred embodiments are discussed in detail below. It should be appreciated, however, that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed are merely illustrative of specific ways to make and use the invention, and do not limit the scope of the invention.
The present invention will be described with respect to preferred embodiments in a specific context, namely a rear projection display, such as for a television. The invention may also be applied, however, to other display systems.
One embodiment of the architecture is shown in
In a preferred embodiment, the display panel 104 includes a display surface that is composed of a rare earth containing glass, such as Pr:Yb that exhibits red, green, and blue fluorescence simultaneously, depending on the composition of the glass and ratios of rare earths in the glass. One example of a material with such properties is described in Dwivedi, et al., “Intense white upconversion emission in Pr/Er/Yb codoped tellurite glass,” Journal of Applied Physics 104. 043509 (2008), four pages.
Individual subpixels are produced by red, green, and blue filters that pass only the fluorescence of the desired wavelength. One possible arrangement of the filters is shown in
While, the subpixels are described as being the primary colors, it is understood that the complementary colors could alternatively be used. In addition, a white, e.g., unfiltered or transparent, subpixel could be included to increase the brightness of the display.
In another embodiment, conventional glass is used, and individual red, green, and blue phosphors are applied to individual red, green, and blue subpixels so that the laser beam can individually and sequentially address each subpixel to produce the desired image.
The wavelength of the laser to be used will depend on the phosphor. For example, Pr:Yb can be excited to produce red, green, and blue using one or more infrared lasers. Other embodiments will be individual phosphors optimized for each color. The laser can be used with either an upconversion phosphor (e.g., two photons of infrared light to produce visible colors) or downconversion (e.g., excitation wavelength shorter than the fluorescence). If one or more infrared lasers are used to excite photoluminescence, the process is upconversion. On the other hand, if the laser is of shorter wavelength than the red, green, or blue, then it is downconversion. The optimum will be determined by minimizing the quantum defect for the system as well as maximizing the photoluminescence efficiency. By increasing the number of subpixels beyond three, a false color hyperspectral image could also be displayed, or the gamut in the visible could be increased.
The system can operate in a number of modes. For subtractive color formation, an infrared laser excites a rare earth doped host material (such as Er/Pr/Yb co-doped glass) to produce white light. Each pixel is composed of individual red, green, and blue subpixels formed by filters. As discussed above, a white subpixel could also be included. The color filters subtract the unwanted portions of the white light to produce the individual RGB. The spatial light modulator (SLM) directs the exciting laser beam to the appropriate subpixel.
An example of a display panel 104 is shown in
In one example, the subpixels are excited by light reflected (or transmitted) by a spatial light modulator. For example, a DMD could include at least two rows, each with twice as many minors as there are subpixels in a row. The display panel 104 could then be imaged one row at a time. In an alternate embodiment, each DMD row could include less than all the subpixels and the light beam could be moved to alternately illuminate different color sets.
In direct color formation, each pixel has red, green and blue subpixels. The laser light is directed to the appropriate subpixel by a SLM, which is composed of a phosphor designed to emit at the appropriate color under IR laser excitation. This requires an upconversion phosphor. The fluorescence can also be excited by downconversion, where a blue or UV laser is used to excite a phosphor. Fluorescent lamps and plasma display panels use UV photon excitation of phosphors to excite red, green, and blue emission.
In another example, laser 102 is scanned in a manner similar to a cathode ray tube. This embodiment is illustrated in
In this embodiment, the color filters are incorporated as strips 116 along the panel 104. In one example, the strip 116b has a high reflection for blue, the strip 116r has a high reflection for red and the strip 116g has a high reflection for green. These strips can be excited, for example, by a spatially modulated beam or by a scanned laser that is turned off and on as it traverses each color row 116b, r or g. In addition, a broad band high reflection layer 118 is formed on a back surface of the substrate 114 to direct the photoluminescence forward. This layer is preferably transparent to the wavelength of the impinging light, e.g., transparent for infrared when an infrared laser is used.
The previous embodiment describes a white phosphor that is filtered to absorb the undesired primary colors and to let the desired primary color through. While this embodiment can have advantages, it can also be inefficient. In other embodiments, each subpixel (e.g., laser or phosphor) produces the desired primary, which leads to a more efficient solution.
Another embodiment includes a matrix of individually addressed optically pumped solid state lasers in a large area display panel, where each individual subpixel is a red, green, or blue laser. This embodiment can be envisioned with reference to
In the preferred embodiment, the display panel is a Yb:Er:Pr glass with a broad band high reflectivity coating on the back side. It is understood that other rare-earth dopants could alternatively be used. The backside coating 118 is highly reflective for red, green, and blue, but is transmissive for IR. The IR from the pump laser is directed to the individual subpixels on the glass. Each subpixel forms a resonant cavity by having a front side coating with partial reflectivity for either R, G, or B, and transmissive for the other two colors. Directing the IR to the subpixel causes resonant emission (lasing) at the desired color. Each laser therefore provides an individual color pixel for a digital picture.
This embodiment would have one laser per subpixel. In other words, a full HD display would include several million lasers (e.g., 1920×1080=2,073,600 pixels×3 subpixels/pixel=6,220,800 subpixels). A fourth subpixel would increase the number proportionately. In this case, the display panel with solid state laser subpixels would be made monolithically using semiconductor fabrication techniques, and would include the glass substrate containing the rare earth ions and cavities defined by the front and rear surface minors.
The scope of the present application is not intended to be limited to the particular embodiments of the process, machine, manufacture, composition of matter, means, methods and steps described in the specification. As one of ordinary skill in the art will readily appreciate from the disclosure of the present invention, processes, machines, manufacture, compositions of matter, means, methods, or steps, presently existing or later to be developed, that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized according to the present invention. Accordingly, the appended claims are intended to include within their scope such processes, machines, manufacture, compositions of matter, means, methods, or steps.
This application is a continuation of co-pending International Application No. PCT/US2010/032996, filed Apr. 29, 2010, which claims the benefit of U.S. Provisional Application No. 61/173,860, entitled “Rear Projection Display using Laser Excited Photoluminescence,” filed on Apr. 29, 2009, both of which are incorporated herein by reference.
Number | Name | Date | Kind |
---|---|---|---|
6501590 | Bass et al. | Dec 2002 | B2 |
6900916 | Okazaki et al. | May 2005 | B2 |
6986581 | Sun et al. | Jan 2006 | B2 |
7090355 | Liu et al. | Aug 2006 | B2 |
7537346 | Liu et al. | May 2009 | B2 |
8384625 | Hajjar et al. | Feb 2013 | B2 |
20040070551 | Walck et al. | Apr 2004 | A1 |
20050174635 | Bruegl et al. | Aug 2005 | A1 |
Number | Date | Country |
---|---|---|
2002-0024408 | Mar 2002 | KR |
WO 9520811 | Aug 1995 | WO |
Entry |
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Dwivedi., Y, et al., “Intense white upconversion emission in Pr/Er/Yb codoped tellurite glass,” Journal of Applied Physics, 104, 043509, 2008, pp. 043509-1 to 043509-4. |
Number | Date | Country | |
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20120195021 A1 | Aug 2012 | US |
Number | Date | Country | |
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61173860 | Apr 2009 | US |
Number | Date | Country | |
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Parent | PCT/US2010/032996 | Apr 2010 | US |
Child | 13284517 | US |