1. Field of the Invention
The present invention relates to CMOS sensors, and more particularly, to a method and apparatus for providing simultaneous electronic shutter action (SESA) frame storage and correlated double sampling (CDS) simultaneously in the CMOS sensors.
2. Description of the Prior Art
Digital cameras are commonly used today. Typically, a digital camera contains image sensors for converting light into electrical charges. Generally, image sensors can be divided into two broad categories according to the applied manufacturing process: CCD (charge-coupled device) sensors and CMOS (Complementary Metal Oxide Semiconductor) image sensors, where the CMOS image sensors (CIS) are based on the CMOS technologies.
For CMOS image sensors, a pixel is an element of an image sensor implemented for generating a differentiable strength output signal; the differentiable strength output signal is proportional to the strength of incident light. Each pixel within the image sensor is also implemented for detecting, storing, and outputting a signal. Typically, CMOS sensors use an “active pixel” for image sensing rather than use a “passive pixel” within. In brief, a pixel with an amplifier or signal buffer is called an “active pixel”, while a pixel with only a photo detector and a switch is defined as a “passive pixel”. With regards to a typical “active pixel” CMOS image sensor, each active pixel contains a photodiode for sensing light and a parasitic capacitor for holding the received signal.
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For CMOS image sensors with active pixels, correlated double sampling (CDS) is often adopted to eliminate a low-frequency noise within the CMOS image sensors. The operating scheme of the CDS operation is described as follows.
For the CDS operation, at time t=t1, a first voltage signal readout vout1=vn1 is obtained, where Vn1 illustrates noise at the sampling node (i.e., the node 105). At time t=t2=t1+Δt, a signal is added to the sampling node (i.e., the node 105), and then a second signal readout, i.e., vout2=vn2+vsig is obtained immediately. That is, in the CDS operation, the first readout is for capturing noise, and the second readout is for capturing both the undesired noise (Vn2) and the demanded signal (Vsig).
Thereafter, the CDS operation extracts the demanded signal by subtracting the first sampled value derived from the first signal readout from the second sampled value derived from the second signal readout. The extracted signal ΔVout hence can be represented as below:
Δvout=vout2−vout1=(vn2+vsig)−(vn1)=(vn2−vn1)+vsig
In a case where the low-frequency noise dominates and Δt is small enough, a value (vn2−vn1) at this time will be close to zero, thus achieving a desired output: Δvout≅vsig.
That is, the CDS operation acts as a high-pass filter for filtering out undesired low-frequency noise. The smaller the value of Δt; the higher the cutoff frequency, which further suppresses noise. The Δt between two readouts should be as small as possible. Typically, for an effective CDS in an image sensor with active pixels, Δt should be in the order of a few microseconds or smaller. However, for an active pixel to perform the CDS function, two separated storing nodes for signal storage are necessary, although one of the storing nodes may simultaneously have other functions, e.g., signal detecting or sampling. In addition, a complete CDS readout also requires CDS operation in the readout circuitry, which adds its own noise to the data.
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In face, it is preferable in most cases to perform a snapshot operation and a simultaneous electronic shutter action (SESA) operation. The “snapshot” function synchronizes all pixels in an image sensor to simultaneously start and stop exposure. The process to achieve higher shutter speed in an electronic image sensor by controlling the start and stop of integration (exposure) is called “Simultaneous Electronic Shutter Action (SESA)”. The SESA operation ensures that all pixels capture the image of a scene at the very same moment. Unfortunately, the designs of the existing CMOS image sensors can not provide both a complete CDS function and the SESA functionality simultaneously. As mentioned above, there are a plurality of different structures of APS pixel, such as 3T APS pixel, 4T APS pixel (e.g., a photogate APS), 5T APS pixel, etc. depending on design requirements. Descriptions for these different APS pixels are as follows.
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Step 1: For the row 1 as shown in
Step 2: The CMOS image sensor executes a first readout operation for the row 1 to sample (signal+noise) level, thereby extracting a rudimentary output voltage Vout1: vout1=v1(2)=vreset1+vn1+vsig. The voltage Vout1 (i.e., V1(2)) represents an extracted voltage when turning on the row select transistor 306 (a pulse 2 of the row select signal 306A in
Step 3: A second reset operation is executed for the node 308 via turning on the reset transistor 310 (i.e., a pulse 3 of the reset signal 310A occurs) to thereby extracts a voltage: v1(3)=vreset2+vn2, where the voltage V1(3) represents the extracted voltage at this time.
Step 4: A second readout operation is executed for completing an operation cycle of one particular row (e.g., the row 1 in this case). The second reset level is sampled in the second readout operation, hence: vout2=vreset2+vn2, where the voltage Vout2 represents an extracted voltage via turning on the row select transistor 306 (i.e., a pulse 4 of the row select signal 306A occurs in
The above four steps complete an operation cycle for one certain row in one frame. With the execution of aforementioned steps 1-4, an output of a pixel can be extracted as:
v
out
=v
out1
−v
out2
=v
sig+(vreset1−vreset2)+(vn1−vn2).
In general, vreset1−vreset2≈0, but (vn1−vn2)=√{square root over (2)}·{tilde over (v)}n ({tilde over (v)}n is the root-mean-square noise value), due to the fact that two samples (readouts) are not correlated to each other. Therefore, a final output of non correlated double sampling functionality in
The 3T APS pixel 300 has some unwelcome drawbacks due to no true CDS (correlated double sampling) operation. This is because there being only one node 308 for signal detection, storage and sampling; once a charge integration of pixels in a row ends at the first readout, the subsequent second reset then destroys the signal.
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During the first read out operation, a noise is sampled accordingly as: vout1=vreset+vn1. Then, a voltage of the transmit signal 503A rises to turn on the transfer transistor 503 and a voltage of the photodiode signal 502A falls, and the charges stored underneath the photodiode 502 are transferred to the sampling node 504. The second readout (i.e., signal+noise) is sampled as: vout2=vsig+vreset+vn1. In this way, the output can be extracted from the two corrected samples (readouts) as: vout=vout2−vout1=vsig.
By applying the 4T APS pixels 500 with the CDS operation to the CMOS image sensor, the low-frequency noise hence is removed. However, the CMOS image sensor with a pixel array of a plurality of 4T APS pixels 500 still lack SESA operation since the same node is used for both signal detecting and storing.
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Generally, for achieving the aforementioned SESA operation, an APS pixel has to hold “exposure data” until it is read out. Nevertheless, a required data holding time could be as long as tens of milliseconds. Because electronic imaging systems do not have a mechanical shutter, the incoming light continues to generate charges during this period. A simple charge sink commonly seen in a pixel consists of a high-voltage source as a drain for electrons (or low-voltage source for holes), and a switch that connects this voltage source to a sensing node.
Yet another prior art structure of an APS pixel with the SESA operation is disclosed in U.S. Pat. No. 6,369,853 (Merrill et al.). In Merrill's disclosure, a reset switch and a reset voltage reset the photodiode before integration, and serve as a charge sink while holding signal. However, the structure taught by Merrill again lacks CDS capability.
As discussed above, the conventional systems have drawbacks. Therefore, there is a demand for providing a process and a system that allows both efficient CDS and SESA operation in the CMOS environment for digital cameras for better performances.
In one exemplary embodiment of the present invention, an electronic image sensor with a pixel array of a plurality of active pixels is provided. Each of the active pixels includes: a photo detector, providing a sensing node for producing a signal based on an amount of light incident thereon; a storing node for storing a plurality of photo-generated charges according to the signal; a first controllable potential barrier between the sensing node and the storing node; a outputting node; and a second controllable potential barrier between the storing node and the outputting node, wherein each of the sensing node, the storing node and the outputting node is not overlapped.
In another exemplary embodiment of the present invention, a method for correlated double sampling (CDS) in an electronic image sensor with a pixel array of a plurality of active pixels where each active pixel has a photo detector for producing a signal based on an amount of light incident on the pixel array is provided. The method includes: integrating a plurality of photo-generated charges according to the signal; resetting a signal sampling node; sampling noise at a first readout; transferring the photo-generated charges to the signal sampling node; and obtaining a second read out with charge sampling to extract a signal accordingly.
In yet another exemplary embodiment of the present invention, a method is provided for correlated double sampling and “snapshot and simultaneous electronic shutter action (SESA)” in an electronic image sensor with a pixel array of a plurality of active pixels where each active pixel has a photo detector for producing a signal based on an amount of light incident on the pixel array. The method includes: integrating a plurality of photo-generated charges according to the signal; holding the photo-generated charges until a readout; turning on a charge sink for draining a plurality of incoming photo-generated charges; resetting a signal sampling node; sampling noise at a first readout; transferring the photo-generated charges to the signal sampling node; and turning off a charge sink for pre-resetting a plurality of nodes.
In yet another exemplary embodiment of the present invention, an
imaging system with an electronic image sensor having a pixel array of a plurality of active pixels is provided. Each of the active pixels includes: a photo detector, providing a sensing node for producing a signal based on an amount of light incident thereon; a storing node for storing a plurality of photo-generated charges according to the signal; a first controllable potential barrier between the sensing node and the storing node; an outputting node; and a second controllable potential barrier between the storing node and the outputting node, wherein each of the sensing node, the storing node and the outputting node is not overlapped.
According to one aspect of the present invention, a pixel with a plurality of separated nodes for signal detecting, storing and sampling, and further with a charge sink is provided. The pixel is capable of efficiently performing SESA in the CMOS sensor.
According to another aspect of the present invention, a pixel capable of performing Correlated Double Sampling (CDS) by using a “spill well” structure is provided. The photo detector of the present invention has higher quantum efficiency than those employing CCD and photogate types of pixels.
According to yet another aspect of the present invention, a pixel and an area-array of such a pixel as an image sensor capable of performing both SESA and CDS at the same time are provided. Also, the spill well structure that uses a photodiode as the photo detector helps to achieve higher quantum efficiency than those employing CCD and photogate pixels. Furthermore, the present invention is compatible with a standard CMOS process.
These and other objectives of the present invention will no doubt become obvious to those of ordinary skill in the art after reading the following detailed description of the preferred embodiment that is illustrated in the various figures and drawings.
The foregoing features and other features of the present invention will now be described with reference to the drawings of a preferred embodiment. In the drawings, the same components have the same reference numerals. The illustrated embodiment is intended to illustrate, but not to limit, the invention. The drawings include the following figures:
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In this embodiment, the active pixel 900 includes a charge sink 910, wherein the charge sink 910 contains a transistor 911 (TX3) that creates a potential barrier between a photo detecting node 914A and a charge drain 915. The active pixel 900 further includes a spill well structure 906 that contains a transistor 912 (TX2) implemented for creating a potential barrier between the photo detecting node 914A and a storing node 917. A transistor 918 (TX1) forms a potential barrier between the storing node 917 and a outputting node 922; and a transistor 919, serving as a reset transistor, switches between the outputting node 922 and a reset voltage Va. In addition, a transistor 905 is implemented to act as a source-follower amplifier for signal buffering. In
In
In this embodiment, the voltage Va is set to be less than or identical to a voltage VDD, and a voltage Vsink is preferably greater than a voltage applied to the transistor 911 (TX3). In one aspect, the voltage Vsink is at least one transistor threshold voltage greater than the voltage applied to the transistor 911 (TX3). That is, the voltage Vsink can be set as a high voltage VDD since it is used as a charge sink.
In different embodiments, the active pixel 900 may be constructed using n-type or p-type semiconductor transistors with appropriate adjustments according to the design requirements. It is noteworthy that the polarity described above (
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In step S1002, a plurality of photo-generated charges are integrated. The reset transistor 919 is turned off and the voltage VSTO (i.e., the voltage at the gate of the storing transistor 913) pulls up. In this step, a potential well is formed to store the charges collected by the fully depleted photodiode 914. As shown in
In
In step S1005 in
The gate of the transfer transistor 918(TX1) may be held at a specified constant voltage V1, and the gate of the second transfer transistor 912 may be held at another specified constant voltage V2, for minimizing any switching noise. However, in another embodiment shown in
In the descriptions above, the active pixel 900 operates with CDS when no SESA required is disclosed, In other words, the foregoing operation may be conducted in a “row-rolling” manner, since there is no SESA function.
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Steps S1201, S1202, S1204, S1205, and S1206 in
In brief, at step S1201, the reset transistor 919 turns on for a first resetting, and before the step S1202 the reset transistor 919 turns off. In step S1202 the storing transistor 913 turns on and the photodiode 914 in this embodiment is fully depleted photodiode so that the generated charges will successfully store in the storing node 913. In a preferred embodiment, at the end of the integration, the voltage applied on the transfer transistor 912 (TX2) is slightly heaved to further enhance the barrier between the sensing node 914A and the storing node 917. in step 1203, since the pixel 900 is operated with both SESA and CDS, the voltage signal 911A of the transfer transistor 911 (TX3) is down during the data holding for drain out the remnant charges at the sensing node 914A. Since the voltage signal 912A of the second transfer transistor is heaved at step S1203 and the photodiode 914 is shorted to a voltage Vsink since the third transfer transistor 911 is on, any additional photo-generated charges are drained by the voltage Vsink. Data associated with any captured exposure is stored under the gate of the storing transistor 913. The potential barrier created by the transfer 912(TX2) and the light shield 909 prevents the stored data from being interfered with by any incoming signal, and the charge sink 910 formed by the third transfer transistor 911 (TX3) and the voltage Vsink. This combination allows all pixels in an area array to stop integration simultaneously, and hold the data until readout and hence efficiently facilitates SESA operation.
In step S1204, the reset transistor 919 turns on again for reset. In step S1205, after the reset transistor 919 turns off, the row select transistor 904 turns on for achieve first read out. At step S1206, the transfer transistor 918 turns on and the storing transistor 913 turns off for transferring the charges from the storing node 917 to the outputting node 922; after the charge transfer the transfer transistor 918(TX1) turns off and then the row select transistor 904 turns on for the second readout. It is noteworthy that steps S1204-S1206 (also steps S1003-S1005) are performed in a “rolling” manner, i.e., sequentially row after row, until the last row is reached.
Operations for one row of the pixel array are finished from the aforementioned steps. After the readout operations of all the rows within the pixel array end (a readout operation of a frame), the transfer transistor 911 (TX3) is turned off and the reset transistor 919 is turned on for the follow-up frames. Since the photodiode 914 is a fully depleted photodiode in this embodiment; this ensures that all incoming charges are transferred to the storage node 917, instead of staying in the photodiode 914.
It should be noted that the present invention is not limited to the foregoing implementations. Various modifications may be used to implement the foregoing techniques. For example, the potential barrier formed by the transfer transistors 918(TX1), the transfer transistor 912(TX2), and the transfer transistor 911 (TX3) may be operated differently than as described above. An example of such a variation is provided with respect to the diagram shown in
The steps S1401-S1407 of
In step S1402, the voltage applied on the gate of the first transfer transistor 918(TX!) is biased at a voltage V13
As for the applied voltage on the transfer transistor 912(TX2), the gate of the transfer transistor 912(TX2) is biased at a voltage V13-tx2 lower than a voltage V11
According to one aspect of the present invention, an active pixel with a plurality of separate nodes for signal detecting, storing and outputting, a charge sink, and an area-array is provided. The active pixel is capable of efficiently performing SESA in the CMOS area.
According to another aspect of the present invention, an active pixel can perform Correlated Double Sampling (CDS) by using a “spill well” structure. The photo detector of the present invention has higher quantum efficiency than those using CCD and photogate types of pixels.
According to yet another aspect of the present invention, an active pixel and an area-array of such a pixel can perform both SESA and CDS simultaneously. The spill well structure which uses a photodiode as the photo detector helps to achieve higher quantum efficiency than those using CCD and photogate types of pixels. In a preferred embodiment, the photodiode is a fully depleted photodiode. Furthermore, the present invention is compatible with standard CMOS process.
Those skilled in the art will readily observe that numerous modifications and alterations of the device and method may be made while retaining the teachings of the invention.