1. Field of the Invention
The present invention pertains to liquid crystal on silicon (LCOS) displays, and more particularly to improved temperature and color temperature control and compensation method for the microdisplay systems.
2. Description of the Prior Art
Since microdislay systems, especially the liquid crystal on silicon (LCOS) Microdisplay frequently operate in the hot interior of a projection device, the microdisplay technology is still challenged by the need to effectively control the temperature and compensate for the color balancing under the circumstances of temperature increase such that the quality of display would not be impaired by uncontrolled high temperatures. The difficulties of color balancing are compounded because the display from each color element has its own individual temperature variations and each color element also has different temperature sensitivities. Meanwhile, it is imperative to control and proper compensate the color balancing operated under temperature variations because the color balance of a projection system is an important feature of its performance.
In a well-designed system, the color balance is determined by the respective power levels of the primary colors and by the spectral bandwidths of those colors. Various techniques have long been known in the art that can be used to achieve color balance in a projection display system where the intensities of the three colors can be modulated separately. In the application of such techniques to projection systems based on microdisplays and spatial light modulator, some problems arise. First, the microdisplays most often operate in the hot interior of a projection device. As will be further discussed below, all components within such devices have thermal sensitivities of some sort. The birefringence of the liquid crystal material within such a display normally becomes lower with elevated temperature and thus the electro-optical (EO) curve for such a device is highly temperature dependent. In a system using three separate microdisplays the situation often arises where each of the microdisplays operates at a different temperature than the others. When the unit is first turned on after having previously reached ambient temperature the microdisplays are all operating at lower than normal temperature. While the rise in temperature begins immediately it may take 30 minutes to reach a new, stable set of operating temperatures. The voltage transfer curve has been shown to vary with temperature. Additionally, the voltage-transfer curves for each color device at a given temperature differ because of the differences in the materials. A technical challenge is faced by the microdisplay system to provide a method of determining the temperature of the liquid crystal to develop and implement control methods that mitigate the effects of high or low temperature through temperature control or other compensation and that simultaneously maintain proper color balance.
There are several prior art approaches taken in attempt to solve the problems caused by temperature variations in a microdisplay system including disclosures made by 1) U.S. Pat. No. 6,304,243, Kondo, et al, “Light Valve Device” Oct. 16, 2001, column 28, line 62 through column 29, line 37, for a discussion of one approach to the implementation of cooling of a microdisplay; 2) U.S. Pat. No. 4,338,600, Leach, “Liquid Crystal Display System Having Temperature Compensation” Jul. 6, 1982, and 3) U.S. Pat. No. 4,460,247, Hilsum et al, “Temperature Compensated Liquid Crystal Displays”, Jul. 17, 1984. Another disclosure was reported by Kurogane et al to use an electro-optic mode that does not exhibit noticeable thermal variation in the linear region of interest. However, the availability of the materials employed and special manufacture processes and mode of operations would significantly restrict the usefulness of the proposed microdisplay systems. Another is the approach taken in U.S. Pat. No. RE 37056, Wortel, et al, where the inventors disclose a method to manufacture the cell in such a manner that the slopes of the electro-optic curves measured at different temperatures in the same liquid crystal device are quite close. A simple temperature measurement system is employed to provide information to a system that can adjust the column drive voltage and thus effect the compensation. However, this particular approach is of limited usefulness because the method requires a very specific approach to the design and manufacture of the cell.
In view of the current state of the art of microdisplay temperature control, there is an ever-increasing demand for new methods and system configurations that can effectively control the temperature and to compensate the performance variations caused by the temperature changes due to the temperature sensitivities of the microdisplay systems. There are several reasons for such increased demand. First, it is observed from operations of microdisplay systems that a liquid crystal experiences a rise in temperature from ambient over a period of 20 to 30 minutes after a system is turned on. This rise in temperature is attributable in part to a rise in ambient temperature within the product case due to heating of the air within by such items as the lamp and by other electronic components. A second major source of heating is the heat generated from the thermal characteristics of the silicon in the LCOS microdisplay itself. A third major source is heat caused by the illumination from the lamp falling on the microdisplay itself. The degree of temperature increase depends on the thermal design of the product and the environment in which it operates. A second reason for the increasing demand to control and compensate temperature effect for a microdisplay system is a observation that the system performance of a microdisplay is strongly temperature dependent. A first sensitivity of LCOS microdisplays is the reduction of the birefringence of the liquid crystal material with elevated temperature within such a display with thus the electro-optic (EO) curve for such a device is highly temperature dependent. One particular aspect of this temperature driven effect is that the dark state rises as temperature deviates from the design temperature and therefore the contrast of such a system suffers.
Referring to the LC curves of
Thus from the above it is clear that temperature is an important factor in the performance of a liquid crystal device. It is also clear that knowledge of the temperature of a liquid crystal device can enable several commonly known control mechanisms in the electro-optical-mechanical design of a product using such devices. In order to control the microdisplay operational temperature, traditional measures includes the use of fan controlled by a thermostat for activating a fan to increase the air circulation of a microdisplay system. Alternatively the thermostat may be position to measure the heat at a set of heat sinks mounted to the back of the microdisplays. Additionally, the knowledge of several control mechanisms in the electro-optical-mechanical design embodied in different products using such mechanisms can be implemented to further exploit such knowledge to achieve optimal performance. However, as of now, the conventional technologies in microdisplay temperature control still have not fully take advantage of the availability of different control mechanisms to improve and enhance the temperature control and compensation for microdisplay systems operated under widely varying temperatures. Particularly, temperature compensations for adjusting color contrast in response to temperature variations to achieve improved color balancing become more important when the microdisplay systems are subject to greater degree of temperature variations.
Color balance in a system has two important aspects. The first is the range of colors that can be created in a system. This is referred to as the color gamut of the system. It is determined by the spectrum of the color used to create the primary colors of the system. This information is commonly presented as an x-y plot of the color coordinates of the three primaries; the most common system being the CIE 1931 color plots. Colors that can be created by these primaries will have color coordinates that fall within the triangle formed by the three primaries. The x-y coordinates of colors that fall outside the triangle cannot be represented by such colors. The primary colors themselves, in a three-panel projection system, are determined by the spectral characteristics of the lamp, by the various optical filters and the pass characteristics of the optical elements, and by the efficiency and spectral response characteristics of the light modulators. A CIE 1931 plot with indicates of regions associated with particular colors, from page 7 of Hazeltine Corporation Report No. 7128, “Colorimetry”, dated Jun. 10, 1952, which in turn cites D. B. Judd, “Color in Business, Science and Industry” John Wiley and Sons, 1952, is shown As
The second important aspect of color balance is the color temperature of the white point of the system. In its simplest form the white point of a system is determined by the color coordinates when all three channels are turned on to their maximum intended brightness. This can be measured reliably using instruments such as those used to measure the color coordinates of the primaries. The determination of color temperature requires assessment of the color coordinates against an overlay of the black body curve. A useful version of the curve, presented in
The color coordinates of the white point of the system are determined not only by the color coordinates of the individual primaries, but by the relative power of the primaries. The relative power of the primaries is normally determined in large part during the design phase when a new projection device is made. It requires a comprehensive assessment of the filtering function of each component within a system, including the microdisplays.
Given a set of performance characteristics, the color coordinates for each spectral channel can be predicted; although it is often preferable to measure the color coordinates experimentally to take into account component variance from the nominal specifications. Similarly, the white point can be predicted from measured data or calculated data, although a direct measurement is a more reliable method. Regardless of the origins of the data, it is clear that changes to the efficiency of the individual color channels will change the relative intensity of portion of the spectrum and therefore will change the color coordinates of the white color point, hence the color temperature of white.
As discussed above, the spectral band-pass limits are normally designed into the system early in its development. While changes can be made, this normally requires the replacement of a spectrally important component, such as a dichroic trim filter or the like. In some cases, dichroic filters are designed and then mounted to facilitate rapid modification of a design.
Furthermore, since the microdisplays are sensitive to variations from the design temperature. In the instances presented, the voltage required to reach maximum efficiency drops as temperature rises. Additionally, it is experimentally proven that the microdisplay for each color may be operating at different liquid crystal temperatures. It is also well known that the curve of voltage versus efficiency is normally different for each color, even in those instances where the liquid crystal cells are identical. This is because the longer wavelengths interact differently with a given cell configuration.
Managing a constant white point under such circumstances is challenging but can be accomplished if the ambient conditions are those predicted by the designers. However, there are always circumstances where the ambient cannot match the exact circumstances predicted. One example is that of a system that has just been turned on and is going through a warm-up period. A second likely circumstance is that the room temperature is hotter or colder than the nominal design temperature for the mechanical design of the system, resulting in the introduction of air into the system that differs from the design expectation to some degree.
For these reasons, there is still need and great challenge in the art of microdisplay such as a three-panel liquid crystal on silicon (LCOS) display to provide improved system architecture and methods of temperature control and color-balancing and compensation to improve the system performance under wide ranges of temperature variations such that the above-mentioned limitations and difficulties can be overcome.
It is therefore an object of the present invention to provide new and improved means to adjust the white point of a liquid crystal on silicon display while that display operates in a temperature regime outside the nominal design point or while that display encounters a temperature change normally experienced at power on, or similar circumstances. The purpose of the invention is to keep the appearance of the display stable over a range of environmental conditions.
These and other objects and advantages of the present invention will no doubt become obvious to those of ordinary skill in the art after having read the following detailed description of the preferred embodiment, which is illustrated in the various drawing figures.
Referring to
For better understanding of this invention, another co-pending application Ser. No. 10/329,645 submitted by a co-inventor of this patent application is also incorporated herein as reference. The co-pending patent application Ser. 10/329,645 discloses a microdisplay controller and the microdisplay design that deliver voltages to the pixels based on a pulse width modulation scheme. Each pixel circuit has two voltage supplies deliverable to it, termed V0 and V1 that correspond to dark state and light state voltages. The voltages are relatively fixed and do not vary with data. A new data load modulates the display when this new data load overwrites the previous data load. The pixel switches to the other supply when the data on the pixel is changed. To DC balance the liquid crystal associated with the pixel electrode, a multiplex signal is sent to each pixel that switches a pixels voltage selection to the other supply and simultaneously switches the counter electrode to a new value that mains the symmetric nature of the liquid crystal drive voltage. The DC balancing of the display need not be accomplished synchronously with the switching of data. The modulation of the liquid crystal occurs because the pixels of the microdisplay switch between the two voltage supplies at a sufficiently rapid rate so as to appear as a voltage waveform. When this switching speed takes place at a very fast rate, the liquid crystal will appear to be responding to the RMS of the waveform. Thus switching between two voltages—one at or near the peak of the “white” region and the other at the “black” point, the liquid crystal will respond as if driven by a switching DC waveform at some intermediate point between the two voltages. The RMS voltage over the time scale of the liquid crystal reaction determines the exact point of reflectivity and that is the points to which the liquid crystal device is driven.
In the case of the normally black mode previously described, it is possible to present the curves in a different manner. Rather than display voltage versus throughput, the classic voltage-transfer curve, it is possible to plot a “digital drive-transfer” curve where the throughput is plotted as a function of the digital word that is used to create the drive voltage in the scheme under consideration. The digital word corresponds to a gray level in the drive scheme. Gray levels may range from 2 (full on or full off) to as many as are practical. In modern color display systems gray levels may vary from 6 bits per color in some inexpensive flat panel displays to as high as 12 or 14 bits per color (36 to 42 bits) in some very expensive high end displays.
Referring to
The output of the temperature sensor transmitted back to the counter-timer circuit 140 contains data available for to be further processed by the system processor 300. The counter time circuit 140 on the Control Circuits 100 is optional in that it is needed for circuits of a specific implementation. Alternatively, if the temperature sensor output were an analog voltage then the device could be replaced by an Analog to Digital converter (ADC). If the output were digital, then the block could be dispensed with and the output could be fed directly to the System Processor and Memory. The System Processor and Memory 300 loads digital words into the VITO
There is a normal relationship between the various voltages referenced as that shown in
One function of the system microprocessor 400 is to set the voltages that drive the microdisplays. The digital words to command the different voltages are loaded into the Control Registers on the controllers, one for each channel to control the microdisplay. The correct loads for each color channel are then transferred to each of the DACs 420-R, 420-G and 420-B. The DACs values are inputted to the corresponding voltage terminals 430-R, 430-G and 430-B respectively to set the voltages, which are then scaled to operating voltage by a set of Op-Amps. This establishes the voltages for Vwhite and Vblack as well as the two Vito voltages. In the descriptions of this invention, for reasons for clarity, the term Vwhite, Vblack and Vito may be used interchangeably with the terms V0, V1, Vito_0 and Vito_1. The exact relationship for a normally black mode can be better understood according to following tables:
The exact relationship for a normally white mode is as follows:
Another function of the microprocessor is to control the operation of the temperature sensor system and interpret the temperature readings measured by the temperature sensor modules 440-R, 440-G, 440-B from the individual microdisplay panels 450-R, 450-G, and 450-B respectively. The microprocessor 400 sets the digital word on the Control Registers on each Microdisplay Controller 415-R, 415-G, and 415-B. The Microdisplay Controller in turn passes the control signals to the Microdisplay via the Serial Input/Output line 445-R, 445-G, and 445-B to and from the set I/O registers 435-R, 435-B, and 435-B in each color panel 450-R, 450-B, and 450-B respectively. The Temperature Module function is in turn set from the Serial I/O registers 435-R, 435-B, and 435-B. The output of the Temperature Module is passed back to the Microdisplay Controller, which in turn passes the data back to the System Microprocessor and Control Unit. Alternatively a state machine within the Microdisplay Controller 415-R, 415-B, and 415-G can preprocess the information received from the Microdisplay Temperature Modules 440-R, 440-G, and 440B. The allocation of functions among the various components is not so important as the accomplishment of the function.
The process used to assess the state of the system and then make the necessary adjustments requires first of all that the system temperatures be measured and assessed. The assessment of temperature may include reasonability assessments to be certain that the data is anomalous. It may also include data smoothing measures such as averaging or Kalman filtering. The present invention assumes that the data is assessed to be reasonable or that the temperature sensor is known to be otherwise trustworthy by excellence of design or proven reliability.
Referring to
Once the wait loop time has expired, the full assessment process begins. As previously stated, the temperature assessment systems for each microdisplay provide measured temperature data from the microdisplay sensors for use by the system (step 512). This may be one of the integral temperature sensors previously discussed, or alternatively a PID device or thermocouple or some other sensor known in the art.
The next step is to take the received temperature information and determine from that information which color channel is most limited in the sense that the maximum efficiency of that channel at its operating temperature limits its maximum contribution to achieve the required color balance less than what the other color channels are capable of (step 515). The data for the color channels versus temperature may be stored in a lookup table LUT1, or alternatively it may be stored in a series of lookup tables. While it is possible that a mathematical description might be found using curve fit processes, this hardly seems necessary.
The structure of LUT1 is of interest. LUT1 may be divided into three pages, each page corresponding to a color channel in the device. The entry index for the pages in the table is a temperature. The temperature may be stored at reasonable intervals, such as 1° C. or 5° C., or even at variable intervals. The resulting value may be the result of interpolation between two values following a linear or other rule. This value is a maximum relative efficiency value. The maximum relative efficiency value is an arbitrary constructed value that may be based on the best efficiency at the design point (color temperature) of the system in which the displays are operated, or on some other point of operation. These may not reflect the peak intensity of the system but rather the efficiencies at the desired color point. More than one set of tables may be needed if the system is further designed to support more than one color temperature set point, as is often the case with CRT and LCD monitors commonly available as of this writing.
Referring to
An illustration of one form of the second lookup table (LUT2) follows the Table LUT1 is shown in
Entries for both LUT1 and LUT2 are both best determined experimentally, although once a system is characterized, knowledge of color science and an understanding of the E-O curves for a particular set of microdisplays can permit extension of the data into regions beyond the scope of the data. The predictive arts may be applied subject to an assessment of the deviation of the particular system under inquiry from the statistical mean.
Although the present invention has been described in terms of the presently preferred embodiment, it is to be understood that such disclosure is not to be interpreted as limiting. Various alternations and modifications will no doubt become apparent to those skilled in the art after reading the above disclosure. Accordingly, it is intended that the appended claims be interpreted as covering all alternations and modifications as fall within the true spirit and scope of the invention.
This Application is a Continuation-in-Part (CIP) Application and claim a Priority Date of Oct. 11, 2002 benefited from a Provisional Patent Application 60/417,786 file by one common inventor of this patent application.
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