The present invention relates to the field of CMOS image sensors and, more particularly, to reducing dark current and hot pixels in CMOS image sensors.
Image sensors, including complimentary metal oxide semiconductor (CMOS) image sensors and charge-coupled devices (CCD), may be used in many different digital imaging applications to capture scenes. An image sensor may include an array of pixels. Each pixel in the array may include at least a photosensitive element for outputting a signal having a magnitude proportional to the intensity of incident light contacting the photosensitive element. When exposed to incident light to capture a scene, each pixel in the array may output a signal having a magnitude corresponding to an intensity of light at one point in the scene. The signals output from each photosensitive element may be processed to form an image representing the captured scene.
As pixels are made smaller, pixel elements may be located closer together in the pixel, resulting in increased risk of cross-talk between adjacent pixels. Further, the supply voltage node must be located close to the photodiode. Shallow trench isolation (STI) regions, which may be dielectric-filled trenches formed in the substrate of the image sensor, may be used to isolate pixels and pixel elements from each other.
While helping to electrically isolate pixels and pixel elements, the STI regions may also create problems in the operation of the pixel cell. For example, STI boundaries may have a higher defect density than the substrate, creating a higher density of “trap sites” along the STI boundaries as compared to the silicon/gate oxide interface or silicon surface that can “trap” electrons or holes. Trap sites may result from defects along the silicon dioxide/silicon interface between the STI boundaries and the silicon substrate. For example, dangling bonds or broken bonds along the silicon dioxide/silicon interface may trap electrons or holes.
Trapped electrons or holes may generate a proportional current at the trap site. The current generation from trap sites inside or near the photosensor may contribute to dark current (i.e., electrical current in the photosensor in the absence of light) in CMOS image sensors since a constant charge may be leaking in the photodiode. Because the readout circuitry of the image sensor may not distinguish between sources of charge in the photosensitive element, dark current may be added to the magnitude of the signal output from the pixel, thus making the pixel appear brighter in the produced image than that point actually appeared in the scene. Such a pixel may be referred to as a hot pixel.
In conventional image sensors, a supply voltage may be applied to the photodiode and the floating diffusion during reset to deplete the photodiode of charge, returning the photodiode to its pinned voltage, and to reset the floating diffusion region. It may be desirable to maintain the supply voltage at a high voltage level (e.g., 2.8 v for mobile applications and 3.3 v for digital camera applications) to reset the floating diffusion to a high voltage and to fully deplete the photodiode. The high supply voltage applied to the supply voltage node may deplete the active area connected to the supply voltage node and may also deplete the photodiode to its pinned voltage (e.g., 1.5 V). When this occurs, a field may be generated between the supply voltage node and the photodiode, which may pull the photodiode depletion region close to the STI edge. Accordingly, dark current may increase at photodiode and STI interface.
Included in the drawing are the following figures:
The present invention may reduce dark current at photodiode and STI interfaces due to the electrical field generated between the supply voltage node and the photodiode. This is achieved by reducing the supply voltage so that it is closer to, equal to, or lower than the pinned voltage of the photodiode during column readout. When the supply voltage equals the pinned voltage of the photodiode, no field is generated. Accordingly, the present invention may reduce dark current at the photodiode and STI interface by reducing or eliminating the electrical field between the supply voltage node and the photodiode.
A pixel 10, according to the present invention, is shown in
A cross-sectional view of the structure of pixel 10 is shown in
Pixel 10 further includes shallow trench isolation regions (STIs) 110. STIs 110 may be formed by etching trenches into substrate 210 and filling the trenches with a dielectric. As shown in
All the pixels in the same row may be sampled at the same time by applying a row select line signal RS to row select transistor 70 of the selected row. Specific pixels in each column may be selectively output by respective column select lines (e.g., column readout line 90 of
As shown in
An example of a sequence by which row and column lines may be activated is referred to as a global shutter. In a global shutter, all rows in the array are reset and integrated concurrently. After an integration period, individual rows may be read out sequentially, one row at a time.
Another example sequence by which rows of pixels may be reset is referred to as a rolling shutter. In a rolling shutter, the reset and integration process occurs one row at a time. That is, a first row in the array may be reset and integrated. After the first row meets the integration time, it may be read. The process continues to reset, integrate and read sequential rows as they meet the integration time. Therefore, during the rolling shutter, one row may be integrating while another row is being read.
In
During pixel to column readout period I, row n is selected by applying a signal RS to the row select line corresponding to row n, thereby turning on a row select transistor 70 for each pixel in row n. Next, reset signal RST is applied to reset transistor 40, applying VAA_pix to floating diffusion region 50 of each pixel in row n, thereby resetting respective floating diffusion region 50. Next, the SHR command causes sampling of Vrst from each pixel in row n to sample and hold circuitry 370. Thereafter, TX may be applied to transfer gates 30, transferring a signal representing the level of respective photodiode 20 to respective floating diffusion 50, for each pixel in row n. Then, the SHS command causes sampling of Vsig from each pixel in row n to sample and hold circuitry 370. Throughout period I, VAA_pix may remain at a relatively high voltage (e.g., 2.8v) to allow respective floating diffusion regions 50 to reset to a relatively high voltage.
During period II, floating diffusion region 50 and photodiode 20 of each pixel in row (n+m) is reset. To accomplish this, the RST signal is applied to a respective reset transistor 40 and the TX signal is applied to a respective transfer gate 30, thereby applying VAA_pix to a respective photodiode 20 and floating diffusion region 50. Throughout period II, Vaa_pix remains at a relatively high voltage (e.g., 2.8v) to allow a respective floating diffusion region 50 to reset to a relatively high voltage and to allow a respective photodiode 20 to be fully depleted. When photodiode 20 is fully depleted, the photodiode returns to its respective pinned voltage (e.g., 1.5v).
At the end of pixel to column readout during period I for the (n)th row, Vrst and Vsig for each pixel in the (n)th row may be stored in column sample and hold capacitors in sample and hold circuitry 370. During period III for the (n)th row, column readout may take place. Here, the signals on sample and hold capacitors for each pixel in the row may be transferred to differential amplifier 380. As described above, differential amplifier 380 may provide signal (Vsig−Vrst) to ADC 390, which may convert signals (Vsig−Vrst) for each read out pixel into digital signals.
In a conventional imager, VAA_pix remains relatively high throughout all three periods described above. For example, in one conventional imager, the VAA_pix may remain at 2.8v for mobile applications and at 3.3v for digital camera applications. Maintaining VAA_pix at a voltage higher than the pinned voltage of the photodiode (e.g., 1.5v), however, may generate an electrical field between the VAA_pix node and the photodiode. This may cause the photodiode depletion region to be pulled closer to the STI edge, as shown in the example provided in
In the embodiment of the present invention, shown in
When VAA_pix is reduced to a relatively low voltage during column readout period III, the electrical field between the VAA_pix node and the photodiode is substantially reduced as compared to conventional imagers. When VAA_pix is set to equal the pinned voltage of the photodiode (e.g., VAA_pix=1.5v), the electrical field is substantially reduced. With a weak electrical field or with no electrical field, as the case may be, the depletion region of the photodiode remains spaced apart from the STI edge, as shown in
This embodiment also permits high voltage reset of the floating diffusion region during pixel to column readout period I and reset period II and a full depletion of the photodiode to its pinned voltage during reset period II. This is so because VAA_pix remains relatively high (e.g., 2.8v) throughout both periods. Because VAA_pix is not used to reset the floating diffusion region or photodiode during column readout period III, however, VAA_pix may be reduced during the column readout period III without significantly affecting the operation of the image sensor. This results in reduced dark current in the photodiode.
In one embodiment, VAA_pix may be reduced during column readout period III to a lower voltage, for example, in the range of 1.0v to 1.5v. This voltage range during period III may be desirable for at least one reason. As VAA_pix approaches 0v, the electrical field between the VAA_pix node and the photodiode changes such that the relatively low potential VAA_pix node acts as a hot electron generator. That is, the VAA_pix node injects a relatively large amount of hot electrons into the photodiode. Accordingly, it may be desirable to reduce VAA_pix to a voltage between 1.0v and 1.5v during column readout period III to reduce dark current in the photodiode and to prevent injection of hot electrons into the photodiode.
While the above-described embodiments describe reducing VAA_pix during period III, it is within the scope of the embodiments of the present invention to maintain VAA_pix at a lower voltage whenever possible, except during reset of the photodiode or when signal readout is occurring. By way of example, VAA_pix may be maintained at a lower voltage during column readout (as previously described) or during integration of the photodiode whenever possible (such as during longer integration times when neither signal readout or reset of the pixel is taking place).
Although the invention is illustrated and described herein with reference to specific embodiments, the invention is not intended to be limited to the details shown. Rather, various modifications may be made in the details within the scope and range of equivalents of the claims and without departing from the invention.
Number | Name | Date | Kind |
---|---|---|---|
5831675 | Ueno | Nov 1998 | A |
6232626 | Rhodes | May 2001 | B1 |
6611037 | Rhodes | Aug 2003 | B1 |
6809359 | Yamada | Oct 2004 | B2 |
7064406 | Mouli | Jun 2006 | B2 |
7115855 | Hong | Oct 2006 | B2 |
7119322 | Hong | Oct 2006 | B2 |
7187020 | Mabuchi | Mar 2007 | B2 |
7279395 | Mouli | Oct 2007 | B2 |
20020009824 | Maeda | Jan 2002 | A1 |
20050248673 | Fowler | Nov 2005 | A1 |
20060033129 | Mouli | Feb 2006 | A1 |
20060082667 | Rhodes | Apr 2006 | A1 |
20060146158 | Toros et al. | Jul 2006 | A1 |
20060169870 | Silsby et al. | Aug 2006 | A1 |
20060180741 | Agranov et al. | Aug 2006 | A1 |
20060231733 | Boemler | Oct 2006 | A1 |
20060279649 | Cole | Dec 2006 | A1 |
20070012966 | Park | Jan 2007 | A1 |
20070020791 | Hsu et al. | Jan 2007 | A1 |
20070031987 | Mouli et al. | Feb 2007 | A1 |
20070045679 | McKee et al. | Mar 2007 | A1 |
20070064137 | Kanbe | Mar 2007 | A1 |
20070097241 | Mabuchi | May 2007 | A1 |
20070158771 | Hynecek | Jul 2007 | A1 |
Number | Date | Country |
---|---|---|
2006093815 | Apr 2006 | JP |
2007081358 | Mar 2007 | JP |
20050018512 | Feb 2005 | KR |
WO 03054922 | Jul 2003 | WO |
WO 2004044989 | May 2004 | WO |
WO 2007066996 | Jun 2007 | WO |
Number | Date | Country | |
---|---|---|---|
20090127437 A1 | May 2009 | US |