The present invention relates to solid-state image sensors and, specifically to CCD image sensor charge detection amplifiers with positive feedback in the first stage of the amplifier.
A typical image sensor senses light by converting impinging photons into electrons that are integrated (collected) in sensor pixels. After completion of integration cycle, charge is usually transported, using the charge coupled device (CCD) process, into an on-chip analog memory and from the memory it is scanned into an output amplifier that is located adjacent to the pixel array. The signal from each pixel is processed in a serial fashion through the same amplifier, which results in high pixel-to-pixel uniformity, however the amplifier requires high speed. With increasing array size the pixel size, and consequently, the amount of signal in each pixel is reduced while the speed increases. This places more stringent demands on performance of the charge detection amplifiers that need to have higher sensitivity (conversion gain), lower noise, and operate at higher speeds. A typical charge detection amplifier consists of a floating diffusion that is reset by a reset transistor and that is connected to a gate of a Source Follower (SF) that is typically an NMOS transistor. More details about such circuits can be found for example in the book: Albert J. P. Theuwissen “Solid-State Imaging with Charge-Coupled Devices” Kluwer Academic Publishers, Boston 1995 pp.76-79, or in the article: J. Hynecek “Design and Performance of a Low-Noise Charge Detection Amplifier for VPCCD Devices”, IEEE Transactions on Electron Devices, vol. ED-31, No. 12 Dec. 1984. When charge is transferred on the floating diffusion the transistor senses the resulting potential change and this change is then transferred either directly to the output terminals of the chip or to other on on-chip signal processing circuits. When the signal is transferred directly to the output terminals another buffer SF is usually necessary to increase the chip output driving power. For achieving a high conversion gain the first SF stage needs to be very small in order not to load the FD charge detection node by excessively large transistor gate input capacitance. The small transistor size also increases noise. On the other hand, for high frequency operation, it is necessary that the first SF stage has a reasonable size to drive the large input capacitance of the next stages with high speed. These are contradictory requirements that can be solved, for example, by using three SF stages. However, this solution results in an unacceptable loss of voltage signal and the resulting sensor charge conversion factor and thus overall sensor sensitivity.
It is an object of the present invention to overcome limitations in prior art. It is further object of the disclosed invention to provide a practical charge detection amplifier that has larger first transistor source follower stage size for high frequency operation and low noise without loading the floating diffusion node with large input capacitance. Incorporating another transistor connected in series with the first stage source follower transistor and biasing it from the second stage introduces a small positive feedback into the circuit, which accomplishes this goal and other objects of the invention.
In the drawings:
In
As mentioned previously, this circuit suffers from the lack of the high frequency response and has a low conversion gain. The low conversion gain is a result of the large capacitive loading of the FD charge detection node caused by the first SF stage transistor that has a large gate-source capacitance.
A preferred embodiment solution to these problems is presented in the circuit diagram 200 shown in
The described charge detection amplifier has therefore three SF stages, which provide the desired high frequency response. The high conversion gain is due to the small positive feedback that minimizes loading effect of the FD charge detection node without increasing noise.
The advantages of the present invention are provided by connecting another MOS transistor in series with the first SF stage. Biasing its source from the output node of the second stage introduces a small positive feedback into the circuit. As a result the first stage transistor input capacitance that normally undesirably loads the FD detection node changes from positive to negative value. This is due to the Miller feedback effect of the source-gate capacitance. This now reduces the detection node loading without increasing noise. As a result the first SF stage now has a small voltage gain, which makes it possible to use two or more SF stages for achieving high speed.
While this invention has been described with reference to illustrative embodiments, this description is not intended to be construed in a limiting sense. Various modifications and combinations of the illustrative embodiments, as well as other embodiments of the invention, will be apparent to persons skilled in the art upon reference to the description. It is therefore intended that the appended claims encompass any such modifications or embodiments.
Number | Name | Date | Kind |
---|---|---|---|
4649430 | Hynecek | Mar 1987 | A |
4716356 | Vyne et al. | Dec 1987 | A |
5192920 | Nelson et al. | Mar 1993 | A |
5274687 | Hirama | Dec 1993 | A |
5600451 | Maki | Feb 1997 | A |
5872484 | Hynecek | Feb 1999 | A |
5905256 | Nakano | May 1999 | A |
6153453 | Jimenez | Nov 2000 | A |
6201270 | Chen | Mar 2001 | B1 |
6288613 | Bennett | Sep 2001 | B1 |
20020008574 | Mathe et al. | Jan 2002 | A1 |
20020088975 | Furumiya | Jul 2002 | A1 |
20050285957 | Mutoh et al. | Dec 2005 | A1 |
Number | Date | Country | |
---|---|---|---|
20070090273 A1 | Apr 2007 | US |