Electronic image sensors are typically comprised of pixel arrays of a large number of very small light detectors, together called “pixel arrays”. These sensors typically generate electronic signals that have amplitudes that are proportional to the intensity of the light received by each of the detectors in the array. Electronic cameras comprise imaging components to produce an optical image of a scene onto the pixel array. The electronic image sensors convert the optical image into a set of electronic signals. These electronic cameras typically include components for conditioning and processing the electronic signals to allow images to be converted into a digital format so that the images can be processed by a digital processor and/or transmitted digitally. Various types of semiconductor devices can be used for acquiring the image. These include charge couple devices (CCDs), photodiode arrays and charge injection devices. The most popular electronic image sensors utilize arrays of CCD detectors for converting light into electrical signals. These detectors have been available for many years and the CCD technology is mature and well developed. One big drawback with CCD's is that the technique for producing CCD's is incompatible with other integrated circuit technology such as MOS and CMOS technology, so that processing circuits and the CCD arrays must be produced on chips separate from the CCD's.
Another currently available type of image sensors is based on metal oxide semiconductor (MOS) technology or complementary metal oxide semi-conductor (CMOS) technology. These sensors are commonly referred to as CMOS sensors. CMOS sensors have multiple transistors within each pixel. The most common CMOS sensors have photo-sensing circuitry and active circuitry designed in each pixel cell. They are called active pixel sensors. The active circuitry consists of multiple transistors that are inter-connected by metal lines; as a result, this area is opaque to visible light and cannot be used for photo-sensing. Thus, each pixel cell typically comprises a photosensitive region and a non-photosensitive region. In addition to circuitry associated with each pixel cell, CMOS sensors have other digital and analog signal processing circuitry, such as sample-and-hold amplifiers, analog-to-digital converters and digital signal processing logic circuitry, all integrated as a monolithic device. Both pixel arrays and other digital and analog circuitry are fabricated using the same basic process sequence.
Small cameras which utilize CCD arrays to convert an optical image to an electronic image have been commercially available for many years. Also, attempts have been made to produce small visible light cameras using CMOS sensors on the same chip with processing circuits. One such attempt is described in recently issued U.S. Pat. No. 6,486,503.
Small cameras using CCD sensors consume large amounts of energy (as compared to cameras with CMOS sensors) and require high rail-to-rail voltage swings to operate CCD. This can pose problems for today's mobile appliances, such as Cellular Phone and Personal Digital Assistant. On the other hand, small cameras using CMOS sensors may provide a solution for energy consumption; but the traditional CMOS-based small cameras suffer low light sensing performance, which is intrinsic to the nature of CMOS active pixel sensors caused by shallow junction depth in the silicon substrate and its active transistor circuitry taking away the real estate preciously needed for photo-sensing. U.S. Pat. Nos. 5,528,043 5,886,353, 5998,794 and 6,163,030 are examples of prior art patents utilizing CMOS circuits for imaging which have been licensed to Applicants' employer. U.S. Pat. No. 5,528,043 describes an X-ray detector utilizing a CMOS sensor array with readout circuits on a single chip. In that example image processing is handled by a separate processor (see FIG. 4 which is FIG. 1 in the '353 patent. U.S. Pat. No. 5,886,353 describes a generic pixel architecture using a hydrogenated amorphous silicon layer structure, either p-i-n or p-n or other derivatives, in conjunction with CMOS circuits to for the pixel arrays. U.S. Pat. Nos. 5,998,794 and 6,163,030 describe various ways of making electrical contact to the underlying CMOS circuits in a pixel. All of the above US patents are incorporated herein by reference.
A need exists for improved camera technology which can provide cameras with cost, quality and size improvements over prior art cameras.
The present invention provides a novel MOS or CMOS based active sensor array for producing electronic images from electron-hole producing light. Each pixel of the array includes a layered photodiode for converting the light into electrical charges and MOS and/or CMOS pixel circuits located under the layered photodiodes for collecting the charges. The present invention also provides additional MOS or CMOS circuits in and/or on the same crystalline substrate for processing the collected charges for the purposes of producing images. The layered photodiode of each pixel is fabricated as continuous layers of charge generating material on top of the MOS and/or CMOS pixel circuits so that extremely small pixels are possible with almost 100 percent packing factors. In preferred embodiments, pixel crosstalk is minimized by careful design of the bottom photodiode layer with the addition of carbon to the doped amorphous silicon N or P layer to increase the electrical resistivity. The increased electrical resistivity also helps avoid adverse electrical effects at the edge of the pixel array where the pixel electrodes may be in close proximity to the material used for a top transparent electrode layer.
In a first preferred embodiment the sensor is a 0.3 mega pixel (3.2 mm×2.4 mm, 640×480) array of 5 micron square pixels which is compatible with a lens of {fraction (1/4.5)} inch optical format. In a preferred embodiment the sensor along with focusing optics is incorporated into a cellular phone camera or a camera attachment the cellular phone to permit transmission of visual images along with the voice communication. All of the camera circuits are incorporated on or in a single crystalline substrate along with the sensor pixel circuits. The result is an extremely low cost camera at high volume production that can be made extremely small (e.g., smaller than the human eye). High volume production costs for the above 0.3 mega-pixel camera are projected to be less than $10 per camera.
In a second preferred embodiment the sensor includes a two-million pixel array of 5-micron wide pixels. This sensor is especially useful for a high-definition television camera.
In the following description of preferred embodiments, reference is made to the accompanying drawings, which form a part hereof, and which show by way of illustration a specific embodiment of the invention. It is to be understood by those of working skill in this technological field that other embodiments may be utilized, and structural, electrical, as well as procedural changes may be made without departing from the scope of the present invention.
A preferred embodiment of the present invention is a single chip camera with a sensor consisting of a photodiode array consisting of photoconductive layers on top of an active array of CMOS circuits. (Applicants refer to this sensor as a “POAP Sensor” the “POAP” referring to “Photoconductor On Active Pixel”.) In this sensor there are 307,200 pixels arranged in as a 640×480 pixel array and there is a transparent electrode on top of the photoconductive layers. The pixels are 5 microns×5 microns and the packing fraction is approximately 100 percent. The active dimensions of the sensor are 3.2 mm×2.4 mm and a preferred lens unit is a standard lens with a {fraction (1/4.5)} inch optical format. A preferred application of the camera is as a component of a cellular phone as shown in
The sensor section is implemented with a photoconductor on active pixel array, readout circuitry, readout timing/control circuitry, sensor timing/control circuitry and analog-to-digital conversion circuitry. The sensor includes:
The sensor array is similar to the visible light sensor array described in U.S. Pat. No. 5,886,353 (see especially text at columns 19 through 21 and FIG. 27) that is incorporated by reference herein. Details of various sensor arrays are also described in the parent patent applications referred to in the first sentence of this specification all of which have also been incorporated herein by reference.
The sensor array is coated with color filters and each pixel is coated with only one color filter to define only one component of the color spectrum. The preferred color filters set is comprises three broadband color filters with peak transmission at 450 nm (B), 550 nm (G) and 630 nm (R). The full width of half maximum of the color filters is about 50 nm for Blue and Green filters. The Red filter typically has transmission all the way into near infrared. For visible image application, an IR cut-off filter needs to be used to tailor the Red response to be peaked at 630 nm with about 50 nm full width of half maximum. These filters are used for visible light sensing applications. Four pixels are formed as a quadruplet, as shown in
Carbon atoms or molecules are preferably added to bottom P-doped layer 114 to increase electrical resistance. This minimizes the lateral crosstalk among pixels and avoids loss of spatial resolution. It also avoids any adverse electrical effects at the edge of the pixel array where the transparent electrical layer makes contact with the bottom layer 114 as shown in
In this preferred embodiment, as shown in
Environmental Analyzer Circuits:
The data out of the sensor section is fed into an environmental analyzer circuit 140 where image's statistics is calculated. The sensor region is preferably partitioned into separate sub-regions, with the average or mean signal within the region being compared to the individual signals within that region in order to identify characteristics of the image data. For instance, the following characteristics of the lighting environment are measured:
The measured image characteristics are provided to decision and control circuits 144. The image data passing through an environmental analyzer circuit 140 are preferably not be modified by it at all. In this embodiment, the statistics include the mean of the first primary color signal among all pixels, the mean of the second primary color signal, the mean of the third primary color signal and the mean of the luminance signal. This circuit will not alter the data in any way but calculate the statistics and pass the original data to image manipulation circuits 142. Other statistical information, such as maximum and minimum will be calculated as well. They can be useful in terms of telling the range of the object reflectance and lighting condition. The statistics for color information is on full image basis, but the statistics of luminance signal is on a per sub-image regions basis. This implementation permits the use of a weighted average to emphasize the importance of one selected sub-image, such as the center area.
Decision & Control Circuits:
The image parameter signals received from the environmental analyzer 140 are used by the decision and control circuits 144 to auto-exposure and auto-white-balance controls and to evaluate the quality of the image being sensed, and based on this evaluation, the control module (1) provide feedback to the sensor to change certain modifiable aspects of the image data provided by the sensor, and (2) provide control signals and parameters to image manipulation circuits 142. The change can be sub-image based or full-image based. Feedback from the control circuits 144 to the sensor 100 provides active control of the sensor elements (substrate, image absorption layer, and readout circuitry) in order to optimize the characteristics of the image data. Specifically, the feedback control provides the ability to program the sensor to change operation (or control parameters) of the sensor elements. The control signals and parameters provided to the image manipulation circuits 142 may include certain corrective changes to be made to the image data before outputting the data from the camera.
Image Manipulation Circuits:
Image manipulation circuit 142 receives the image data from the environmental analyzer and, with consideration to the control signals received from the control module, provides an output image data signal in which the image data is optimized to parameters based on the control algorithm. In these circuits, pixel-by-pixel image data are processed so each pixel is represented by three color-primaries. Color saturation, color hue, contrast, brightness can be adjusted to achieve desirable image quality. The image manipulation circuits provide color interpolation between each pixel and adjacent pixels with color filters of the same kind so each pixel can be represented by three-color components. This provides enough information with respect to each pixel so that the sensor can mimic human perception with color information for each pixel. It further does color adjustment so the difference between the color response of sensors and human vision can be optimized.
Communication Protocol Circuits:
Communication protocol circuits 146 rearrange the image data received from image manipulation circuits to comply with communication protocols, either industrial standard or proprietary, needed for a down-stream device. The protocols can be in bit-serial or bit-parallel format. Preferably, communication protocol circuits 146 convert the process image data into luminance and chrominance components, such as described in ITU-R BT.601-4 standard. With this data protocol, the output from the image chip can be readily used with other components in the market place. Other protocols may be used for specific applications.
Input & Output Interface Circuits:
Input and output interface circuits 148 receive data from the communication protocol circuits 146 and convert them into the electrical signals that can be detected and recognized by the down-stream device. In this preferred embodiment, the input & output Interface circuits 148 provide the circuitry to allow external to get the data from the image chip, read and write information from/to the image chip's programmable parametric section.
Chip Package:
The image chip is packaged into an 8 mm×8 mm plastic chip carrier with glass cover. Depending upon the economics and applications, other type and size of chip carrier can be used. Glass-cover can be replaced by other type of transparent materials as well. The glass cover can be coated with anti-reflectance coating, and/or infrared cut-off filter. In an alternative embodiment, this glass cover is not needed if the module is hermetically sealed with a substrate on which the image chip is mounted, and assembled in a high quality clean room with lens mount as the cover.
Lens 4 shown in
Camera Exposure Control:
Sensor 100 can be used as a photo-detector to determine the lighting condition. Since the sensor signal is directly proportional to the light sensed in each pixel, one can calibrate the camera to have a “nominal” signal under desirable light. When the signal is lower than the “nominal” value, it means that the ambient “lighting level” is lower than desirable. To bring the electrical signal back to “nominal” level, the pixel exposure time to light and/or the signal amplification factor in sensor or in the image manipulation module are automatically adjusted. The camera may be programmed to partition the full image into sub-regions is to be sure the change of operation can be made on a sub-region basis or to have the effect weighted more on a region of interest.
Camera White Balance Control:
The camera may be used under all kind of “light sources”. Each light source has different spectral distribution. As a result, the signal out of the sensor will vary under different “light source”. However, one would like to make the image visualized similarly when displayed on a visualizing device, such as print paper or CRT display. It means that a typical light source (day light, flash light, tungsten light bulb, etc) needs to be perceived as a white object more or less. Since the sensor has pixels covered with primary color filters, one can then determine the relative intensity of the light source from the image data. The environmental analyzer is to get the statistics of the image and determine the spectral composition and make necessary parametric adjustment in sensor operation or Image Manipulation to create a signal that can be displayed as “white object” when perceived by human.
A second preferred embodiment of the present invention, which includes a two million pixels sensor array, can be described by reference to
The two million pixels cell array and related circuitry is shown in
The array includes an interconnect structure 115 comprised of dielectric layers providing insulation and electrical interconnections of various elements of the pixel cell array. These interconnections include a set of vias 135 and metalized regions 136 for each pixel connecting diffusion region 130 with a patterned electrode pad 116 formed on top of the interconnect structure 115. Interconnect structure 115, and metalized regions 136 and vias 135 are produced using standard CMOS fabrication techniques. In the standard CMOS fabrication process, metal lines are formed of a stack of Titanium Nitride (TiN) and Aluminum layers, where Aluminum line is stacked on top of TiN line and TiN is making contact with vias. Because Aluminum has very high diffusivity with amorphous silicon, Applicants' embodiment has 116 made of Titanium Nitride without the top Aluminum layer. This finding is essential to make Applicants' sensor work. Of course other metals, such as Titanium, Tungsten, Titanium-Tungsten alloy and Tungsten Nitride, can be used as well. But Titanium Nitride is readily available in a typical CMOS process, therefore, it is Applicants' preferred material.
Each pixel includes a N-I-P photodiode portion formed by continuous layers laid down on top of the interconnect structure 115 and patterned electrode pads 116. The lowest of the photodiode layers, layer 114, is about 0.01 micron thick and is comprised of P-doped hydrogenated amorphous silicon. As in the first preferred embodiment, carbon is preferably added to this layer at concentrations between about 5 to 35 percent. (Carbon concentrations as high as 50 percent could be used. In prototype devices actually built and tested by Applicants, the carbon concentration was about 30 percent.) Applicants have discovered that carbon doping at this concentration does not significantly adversely affect the quality of this layer as a p-type semiconductor but does substantially increase the electrical resistivity of the layer. This issue is discussed in more detail below. The next higher layer, layer 112 is the intrinsic layer of the N-I-P photodiode region of the array. It is hydrogenated amorphous silicon and no doping and is in this embodiment about 0.5 to 1.0 micron thick. The top photodiode layer 110 is N-doped hydrogenated amorphous silicon and is about 0.005 to 0.01 micron thick. A transparent electrode layer 108 is a layer of indium tin oxide deposited on top of N-layer 108 about 0.06 micron thick. This material is electrically conductive and also transparent to visible light.
The electronic components of each pixel in this embodiment are shown in
A block diagram of the sensor array circuitry for the two millions pixel array is shown in
With the basic design of the present invention where the photodiode layers are continuous layers covering pixel electrodes, the potential for crosstalk between adjacent pixels is an issue. For example, when one of two adjacent pixels is illuminated with radiation that is much more intense than the radiation received by its neighbor, the electric potential difference between the surface electrode and the pixel electrode of the intensely radiated pixel will become substantially reduced as compared to its less illuminated neighbor. Therefore, there could be a tendency for charges generated in the intensely illuminated pixel to drift over to the neighbor's pixel electrode.
In the case of a three-transistor unit cell design, the photo-generated charge is collected on a capacitor at the unit cell. As this capacitor charges, the voltage at the pixel contact swings from the initial reset voltage to a maximum voltage, which occurs when the capacitor has been fully charged. A typical voltage swing is 1.4V. Due to the continuous nature of Applicant's coating, there is the potential for charge leakage between adjacent pixels when the sense nodes of those pixels are charged to different levels. For example, if a pixel is fully charged and an adjacent pixel is fully discharged, a voltage differential of 1.4V will exist between them. There is a need to isolate the sense nodes among pixels so crosstalk can be minimized or eliminated.
As explained in Applicant's parent patent application Ser. No. 10/072,637 that has been incorporated herein by reference, a gate-biased transistor can be used to isolate the pixel sense nodes while maintaining all of the pixel electrodes at substantially equal potential so crosstalk is minimized or eliminated. However, an additional transistor in each pixel adds complexity to the pixel circuit and provides an additional means for pixel failure. Therefore, a less complicated means of reducing crosstalk is desirable.
Applicants have discovered that crosstalk between pixel electrodes can be significantly reduced or almost completely eliminated in preferred embodiments of the present invention through careful control of the design of the bottom photodiode layer without a need for a gate-biased transistor. The key elements necessary for the control of pixel crosstalk are the spacing between pixel contacts and the thickness and resistivity of the photodiode layers. These elements are simultaneously optimized to control the pixel crosstalk, while maintaining all other sensor performance parameters. The key issues related to each variation are described below.
1. Pixel Contact Spacing
The growth of a high-resistivity amorphous silicon based film can be achieved by alloying the silicon with another material resulting in a wider band gap and thus higher resistivity. It is also necessary that the material not act as a dopant providing free carriers within the alloy. The elements known to alloy with amorphous silicon are germanium, tin, oxygen, nitrogen and carbon. Of these, alloys of germanium and tin result in a narrowed band gap and alloys of oxygen, nitrogen and carbon result in a widened band gap. Alloying of amorphous silicon with oxygen and nitrogen result in very resistive, insulating materials. However, silicon-carbon alloys allow controlled increase of resistivity as a function of the amount of incorporated carbon. Furthermore, silicon-carbon alloy can be doped both N-type and P-type by use of phosphorus and boron, respectively.
Amorphous silicon based films are typically grown by plasma enhanced chemical vapor deposition (PECVD). In this deposition process the film constituents are supplied through feedstock gasses that are decomposed by means of a low-power plasma. Silane or di-silane are typically used for silicon feedstock gasses. The carbon for silicon-carbon alloys is typically provided through the use of methane gas, however ethylene, xylene, dimethyl-silane (DMS) and trimethyl-silane (TMS) have also been used to varying degrees of success. Doping may be introduced by means of phosphene or diborane gasses.
The thickness of the indium tin oxide (ITO) layer (the transparent surface electrode) is preferably thick enough so that (1) it can hold the characteristics of a homogenous film, (2) it can result in negligible voltage drop across the ITO layer vertically, (3) it also provides negligible voltage drop in the ITO layer in the horizontal directions. These three considerations are mainly to achieve good electrical properties. However, this transparent surface electrode layer is also the front surface of the sensor in the optical path. Therefore, one needs to optimize its properties so it also provides the desirable optical properties. In addition to using the transparent nature of the material for incoming light of wavelength within the range of interest, the thickness also is preferably chosen to achieve minimum front surface reflection and maximum transmission into photodiode layers, for light at wavelengths within the range of interest. For cameras that are designed for viewing with visible light the wavelength near the center of the visible spectrum is about 550 nm. Thin film techniques for minimizing reflection are well known and optics programs are available for designing thin films for minimizing surface reflection based on known values of index of refraction and film thicknesses. Absorption in the ITO layer increases with film thickness. Therefore, designs that provide maximum transmission of light into the photo diode layers typically will involve a tradeoff involving considerations of reflection and absorption as well as conduction across the pixel array surface. One can change ITO thickness to move this reflection/transmission optimum throughout the entire visible spectrum, from 400 nm to 700 μm, for application-specific needs.
In our current practice for a N-I-P diode, the P-layer, which is making contact with the pixel electrode, has a thickness of about 0.01 microns. The pixel size is 5 microns×5 microns. Because of the aspect ratio between the thickness and pixel width (or length) is much smaller than 1, within the P-layer the resistance along the lateral (along the pixel width/length direction) is substantially higher than the vertical direction, based upon Equation 1. Because of this, the electrical carriers prefer to flow in the vertical direction than in the lateral direction. This alone may not be sufficient to ensure that the crosstalk is low enough. Therefore, Applicants prefer to increase the resistivity by introducing carbon atoms into P-layer to make it become a wider band-gap material. Our P-layer is a hydrogenated amorphous silicon layer with carbon concentration about 1022 atoms/cc. The hydrogen content in this layer is in the order of 1021-1022 atoms/cc, and the P-type impurity (Boron) concentration in the order of 1020-1021 atoms/cc. This results in a film resistivity of about 1010 ohm-cm. For a 5 um×5 um pixel, we have found out that negligible pixel crosstalk can be achieved even when the P-layer resistivity is down to the range of a few 106 ohm-cm. Like what is described above, there is a need of engineering trade-off among P-layer thickness, carbon concentration, boron concentration and pixel size to achieve the required overall sensor performance. Therefore, the resistivity requirement may vary for other pixel sizes and configurations. For this N-I-P diode with 5 um×5 um pixel, our I-layer is an intrinsic hydrogenated amorphous silicon with a thickness about 0.5-1 um. The N-layer is also a hydrogenated amorphous silicon layer with N-type impurity (Phosphorous) concentration in the order of 1020 to 1021 atoms/cc.
For applications where the polarity of the photodiode layers are reversed and the N-layer is adjacent to the pixel electrode, the carbon atoms/molecules are added to the N-layer to reduce crosstalk and to avoid adverse electrical effects at the edge of the pixel array.
As explained above since we have carbon in the bottom layer of our photodiode to make it very resistive, contact with top transparent electrode layer 108 at the edge of the pixel array as shown at 125 in
106 (ohm-cm)×0.01 cm/(1 cm×10−6 cm)=1×1010 ohm
This is as resistive as most known insulators. As a result of, the image quality would not be affected.
The photodiode layers of the present invention are laid down in situ without any photolithography/etch step in between. (Some prior art sensor fabrication processes incorporate a photolithography/etch step after laying down the bottom photodiode layer in order to prevent or minimize cross talk.) An important advantage of the present process is to avoid any contamination at the junction between the bottom and intrinsic layers of the photodiode that could result from this photolithography/etch step following the laying down of the bottom layer. Contamination at this junction may result in electrical barrier that would prevent the photo-generated carriers being detected as electrical signal. Furthermore, it could trap charges so deep that cannot be recombined with opposite thermally-generated charges resulting in permanent damage to the sensor. Once the photodiode layers are put on the CMOS wafer, a photolithography/etch step is used to open up TEL contact pads and I/O bonding pads as shown at 127 and 129 in
Below is a summary of the steps we make our POAP sensors on a wafer based process:
Steps 2, 3, 4 and 5 in the order presented are special steps developed to fabricate chips according to the present invention. The other listed steps are processes regularly used in integrated circuit sensor fabrication. Variations in these steps can be made based on established practices of different fabrication facilities.
Applicants have built and tested a prototype two-million pixel sensor as shown in
Two preferred embodiment of the present invention have been described in detail above. However, many variations from that description may be made within the scope of the present invention. For example, the three-transistor pixel design described above could be replaced with more elaborate pixel circuits (including 4, 5 and 6 transistor designs) described in detail the parent applications. The additional transistors provide certain advantages as described in the referenced applications at the expense of some additional complication. The photoconductive layers described in detail above could be replaced with other electron-hole producing layers as described in the parent application or in the referenced '353 patent. The photodiode layer could be reversed so that the p-doped layer is on top and the n-doped layer is on the bottom in which case the charges would flow through the layers in the opposite direction. The transparent layer could be replaced with a grid of extremely thin conductors. The readout circuitry and the camera circuits 140-148 as shown in
This invention provides a camera potentially very small in size, potentially very low in fabrication cost and potentially very high in quality. Naturally there will be some tradeoffs made among size, quality and cost, but with the high volume production costs in the range of a few dollars, a size measured in millimeters and image quality measured in mega-pixels or fractions of mega-pixels, the possible applications of the present invention are enormous. Some potential applications in addition to cell phone cameras are listed below:
Since the camera can be made smaller than a human eyeball, one embodiment of the present invention is a camera fabricated in the shape of a human eyeball. Since the cost will be low the eyeball camera can be incorporated into many toys and novelty items. A cable may be attached as an optic nerve to take image data to a monitor such as a personal computer monitor. The eyeball camera can be incorporated into dolls or manikins and even equipped with rotational devices and a feedback circuit so that the eyeball could follow a moving feature in its field of view. Instead of the cable the image data could be transmitted wirelessly using cell phone technology.
The small size of these cameras permits them along with a cell phone type transmitter to be worn (for example) by professional football players installed in their helmets. This way TV fans could see the action of professional football the way the players see it. In fact, the camera plus a transmitter could even be installed in the points of the football itself that could provide some very interesting action views. These are merely examples of thousands of potential applications for these tiny, inexpensive, high quality cameras.
While there have been shown what are presently considered to be preferred embodiments of the present invention, it will be apparent to those skilled in the art that various changes and modifications can be made herein without departing from the scope and spirit of the invention. For example, this camera can be used without the lens to monitor the light intensity profile and output the change of intensity and profile. This is crucial in optical communication application where beam profile needs to be monitored for highest transmission efficiency. This camera can be used to extend light sensing beyond visible spectrum when the amorphous-Silicon is replaced with other light sensing materials. For example, one can use microcrystalline-Silicon to extend the light sensing toward near-infrared range. Such camera is well suitable for night vision. In the preferred embodiment, we use a package where senor is mounted onto a chip carrier on which is clicked onto a lens housing. One can also change the assembly sequence by solder the sensor onto a sensor board first, then put the lens holder with lens to cover the sensor and then mechanically fasten onto the PCB board to make a camera. This is a natural variation from this invention to those skilled in the art.
Thus, the scope of the invention is to be determined by the appended claims and their legal equivalents.
This application is a continuation in part of U.S. patent application Ser. Nos. 10/229,953 filed Aug. 27, 2002; Ser. No. 10/229,954 filed Aug. 27, 2002; Ser. No. 10/229,955 filed Aug. 27, 2002; Ser. No. 10/229,956 filed Aug. 27, 2002; Ser. No. 10/648,129 filed Aug. 26, 2003; Ser. No. 10/746,529 filed Dec. 23, 2003 and claims the benefit of Provisional Application Ser. No. 60/584,523, filed Jun. 30, 2004, all incorporated herein by reference. The present invention relates to cameras and in particular to cameras with MOS or CMOS sensors.
Number | Date | Country | |
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60584523 | Jun 2004 | US |
Number | Date | Country | |
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Parent | 10229953 | Aug 2002 | US |
Child | 10921387 | Aug 2004 | US |
Parent | 10229954 | Aug 2002 | US |
Child | 10921387 | Aug 2004 | US |
Parent | 10229955 | Aug 2002 | US |
Child | 10921387 | Aug 2004 | US |
Parent | 10229956 | Aug 2002 | US |
Child | 10921387 | Aug 2004 | US |
Parent | 10648129 | Aug 2003 | US |
Child | 10921387 | Aug 2004 | US |
Parent | 10746529 | Dec 2003 | US |
Child | 10921387 | Aug 2004 | US |