Present infrared cameras can be very expensive. A lower cost camera would open up new markets and provide increased sales volume. Present un-cooled bolometer camera designs are very sophisticated, achieving high performance but at a high cost. Much of the cost is the cost of the array, the readout electronics, the addressing CMOS in the array, the display electronics, and various other electronics systems such as non uniformity correction. These features are all included to achieve high performance image but at a high cost.
An infrared camera includes a lens to receive infrared radiation from an image to be viewed. A thermal detector is positioned to receive the infrared radiation from the lens and vary the amount of light transmitted through the thermal detector responsive to the infrared radiation.
In the following description, reference is made to the accompanying drawings that form a part hereof, and in which is shown by way of illustration specific embodiments which may be practiced. These embodiments are described in sufficient detail to enable those skilled in the art to practice the embodiments, and it is to be understood that other embodiments may be utilized and that structural, logical and electrical changes may be made. The following description of example embodiments is, therefore, not to be taken in a limited sense, and the scope is defined by the appended claims.
The functions or algorithms described herein may be implemented in software or a combination of software and human implemented procedures in one embodiment. The software may consist of computer executable instructions stored on computer readable media such as memory or other type of storage devices. Further, such functions correspond to modules, which are software, hardware, firmware or any combination thereof. Multiple functions may be performed in one or more modules as desired, and the embodiments described are merely examples. The software may be executed on a digital signal processor, ASIC, microprocessor, or other type of processor operating on a computer system, such as a personal computer, server or other computer system.
Various embodiments, the invention utilize a transducer that has a thermo-optical effect that causes transitions from transparent to opaque to selected frequencies of light responsive to temperature changes. By focusing infrared light, such as long wavelength infrared light (LWIR) on the transducer, the transitions may be representative of images generating the infrared light. The transducer may be directly viewed by a user where transitions are in a visible light range without the need for much of the expensive features of prior infrared cameras. In further embodiments, the transitions may be wavelengths that are not directly visible, but may be detected by a sensor such as a CMOS CCD (charge coupled device) detectors and converted to a signal which can be used to drive a user viewable display.
In one embodiment, infrared light strikes an array of an array of pixels that have an absorbing film (Si3N4) and a VO2-based optical transducer. The absorbing film is a thermo-optical responsive film, such that its transmissivity to selected ranges of light changes responsive to IR radiation. Crystalline VO2 undergoes a semiconductor metal transition at 67° C. which transforms the material from transparent to reflective and opaque. By adding other metals to VO2 the transition temperature may be lowered to 20° C., lowering the temperature of the reflective-transparent transition. The slope of the transition may also be modified to provide visual changes in the transducer representative of a wider or narrower range of temperatures.
Infrared light striking the array that is in this transition region, will heat up pixels individually depending on the intensity of light coming from the viewed target. The absorbed heat from the IR light causes the reflectance and transmission of each pixel to change in a desired wavelength range of light in response to the level of IR power received. This change can be viewed directly by a user or via an image sensor, and may be enhanced by using a backlight system similar to those used for LCD displays that projects onto a screen or eyepiece. Such a backlight should transmit list in the desired wavelength range. The array in one embodiment may be totally passive.
The array 230 may be directly viewed by a user via an eyepiece or view screen when the transmission changes are in the visible spectrum. In one embodiment, the eyepiece 235 is positioned opposite the beam splitter 225 from the array 230 such that visible light from the array 230 passes through the beam splitter 225 to the eyepiece 235.
In a further embodiment, a backlight 240 may be positioned below the array 230 and emit light 243 that is collimated via a cold lens 245 to illuminate the array 230. The collimated light passes through the array 230 to enhance the light transmitted through the beam splitter 225 to the eyepiece 235. The backlight 240 may be a DLP-like backlight and is optional. If the backlight 240 is used, it is an active element, but may utilize very little power. The rest of the IR detection system 200 may remain passive in various embodiments.
In one embodiment, the eyepiece 235 may include a CMOS CCD array to convert the light to an electronic output, which may be transmitted to a display device, also represented by block 235. The CMOS CCD array may operate in the visible range of light, or may be optimized to operate in a range corresponding to the spectrum at which transmission changes of detector array 230 are most prevalent, such as about 1.1 μm to 1.5 μm, or other wavelength ranges. One example array at these wavelengths include Germanium CMOS arrays pushed to 1.2 μm or a pushed CMOS CCD made by hitting the array with a laser beam to increase quantum efficiency at desired wavelengths.
The VO2 film may be doped in one embodiment to change transmission at RT based on Si3N4 temperature change generated by IR. The RT operation and steepness of transition depend on doping VO2 with metals such as W, Re, and Mo for example. VO2 has a Mott semiconductor-metal transition of about 67° C. Doping with metal can reduce the edge to RT (293° K). Other dopants may also affect such transition characteristics. In one embodiment, the thermal properties may be optimized with the use of an integral vacuum package.
In one embodiment, the IR absorber layer 430 has a 90 to 95% fill factor to efficiently absorb LWIR radiation and change temperature accordingly. The metal pixel body 415 is fairly thin to provide low mass and high thermal conductance to the transducer elements 425, which may be formed of VOx in one embodiment. The metal pixel body 415 may be reflective for shielding pixels from being adversely affected by backlight heating. Posts 340, also referred to as vias, may be formed of low conductance Si3N4, as may be the legs, for providing pixel thermal isolation.
In summary, an IR detector is based on the absorption of LWIR radiation by a pixellated thermal structure. A lens projects the LWIR radiation emitted from a scene onto the pixellated array. Each pixel is heated by the absorbed IR radiation to a degree proportional to the focused LWIR intensity. High efficiency thermally isolated pixels that form the array are designed to efficiently convert the absorber LWIR power into heat and raise the pixel temperature at rates consistent with normal video frame rates.
The temperature at the pixel causes an optical transmission or reflection change in a thermo-optical material located on the pixel. The transmission change is proportional to the amount of IR radiation absorbed by each pixel in the array. The transmission change can be sensed by viewing the change directly with the naked eye when the pixel is back-illuminated with visible light. It can also be sensed by a CMOS array when the pixellated array is backlit at wavelengths where the thermal-optical effect is greatest and where the CMOS detector array has adequate sensitivity. In the latter case the CMOS array provides the ability for non-uniformity correction and for electronic readout of the converted LWIR image. One desirable thermo-optical material is VO2 which exhibits a large transmission change at slightly elevated temperatures or a variety of VO2 films doped with a range of dopants (W, Ti, Re) that can be used to lower the transition temperature.
This application claims priority to U.S. Provisional Application Ser. No. 61/334,490 (entitled Passive Infrared Imager, filed May 13, 2010) which is incorporated herein by reference.
Number | Date | Country | |
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61334490 | May 2010 | US |