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CN115134541A - High dynamic CMOS image sensor with high and low gains and logarithmic response, time sequence control method and reading mode - Google Patents

High dynamic CMOS image sensor with high and low gains and logarithmic response, time sequence control method and reading mode Download PDF

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CN115134541A
CN115134541A CN202210699481.4A CN202210699481A CN115134541A CN 115134541 A CN115134541 A CN 115134541A CN 202210699481 A CN202210699481 A CN 202210699481A CN 115134541 A CN115134541 A CN 115134541A
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transistor
point
charge
voltage
charge compensation
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常玉春
娄珊珊
曲杨
钟国强
程禹
张为森
孔祥和
孙汉蔚
周义喆
李技烨
牛仕泽
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Dalian University of Technology
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Abstract

A high dynamic CMOS image sensor with high and low gain and logarithmic response, a time sequence control method and a reading mode belong to the field of semiconductor photoelectric direction image sensors. The invention utilizes the principle that charge compensation elements respectively work in a cut-off region and a subthreshold region under different light intensities: the charge compensation element is positioned in a cut-off region under weak light and strong light, and no conducting current exists, so that the pixel structure has the same technical function as a high-dynamic pixel with a high-low gain structure, and has strong detection capability under the weak light; under super-strong light or long integration time, the charge compensation element works in a sub-threshold region, and the charge compensation of the over-flash light is realized by utilizing the characteristic that the current and the voltage of the transistor in the sub-threshold region are in logarithmic relation, so that the image can be formed under super-high light intensity. The invention can obtain a plurality of images with the same integral time under one exposure, and the plurality of images can be synthesized into an image with an ultrahigh dynamic range corresponding to weak light, strong light and ultrahigh light.

Description

一种同时具有高低增益和对数响应的高动态CMOS图像传感器 及时序控制方法和读取方式A high dynamic CMOS image sensor with both high and low gain and logarithmic response and timing control method and reading method

技术领域technical field

本发明属于半导体光电方向图像传感器领域,具体为一种同时具有高低增益和对数响应的高动态CMOS图像传感器,以及与其相对应的时序控制方法和读取方式。The invention belongs to the field of semiconductor photoelectric directional image sensors, in particular to a high dynamic CMOS image sensor with both high and low gain and logarithmic response, as well as a timing control method and a reading method corresponding thereto.

背景技术Background technique

动态范围是评价CMOS图像传感器的一项重要指标,表示CMOS图像传感器能够在同一帧图像中同时探测到的最大光强信号和最小光强信号的范围,动态范围越大所获得图像的灰度细节等级就越高。随着集成电路技术的不断发展,CMOS图像传感器已经被广泛应用于图像传感领域。普通的CMOS图像传感器动态范围只能达到60~70dB,然而在汽车影像、安防监控、军事、自动化光学检测等领域中,环境光的范围可达到100dB以上,普通的CMOS图像传感器已经无法满足实际场景成像要求。The dynamic range is an important indicator for evaluating CMOS image sensors, which indicates the range of the maximum light intensity signal and the minimum light intensity signal that the CMOS image sensor can detect simultaneously in the same frame of image. The larger the dynamic range, the grayscale details of the obtained image. The higher the level. With the continuous development of integrated circuit technology, CMOS image sensors have been widely used in the field of image sensing. The dynamic range of ordinary CMOS image sensors can only reach 60-70dB. However, in the fields of automotive imaging, security monitoring, military, and automated optical detection, the range of ambient light can reach more than 100dB, and ordinary CMOS image sensors can no longer meet the actual scene. Imaging requirements.

得到广泛应用的高动态CMOS图像传感器采用的是具有高低增益的像素结构,如图1所示。该像素结构由钳位光电二极管1、电荷转移控制晶体管2、复位晶体管3、高动态范围晶体管4、源极跟随器5、行选晶体管6组成,2-6均为标准NMOS晶体管。工作时序如图2所示,首先进行复位操作,2、3、4晶体管全部导通一次;然后像素进入积分阶段,积分结束之前再对FD点进行一次复位操作,分别读取低增益复位值RST_L和高增益复位值RST_H;接下来,积分结束,电荷转移控制晶体管2导通,将钳位光电二极管1产生的光生电荷转移到FD点,得到高增益信号电压SIG_H;然后电荷转移控制晶体管2和高动态范围晶体管4再同时导通,此时读取低增益信号值SIG_L。在高动态范围晶体管4导通期间,FD点与FDL点相连,相当于增大了FD点的电容,可以容纳更多来自于钳位光电二极管1的光生电荷,从而提高了像素的动态范围。通过两次电荷转移分别获得高低增益的方法可以使得像素的动态范围扩大20~30dB,从而总动态范围接近或达到90dB。The widely used high dynamic CMOS image sensor adopts the pixel structure with high and low gain, as shown in Figure 1. The pixel structure is composed of a clamp photodiode 1, a charge transfer control transistor 2, a reset transistor 3, a high dynamic range transistor 4, a source follower 5, and a row select transistor 6. 2-6 are standard NMOS transistors. The working sequence is shown in Figure 2. First, the reset operation is performed, and transistors 2, 3, and 4 are all turned on once; then the pixel enters the integration stage, and the FD point is reset again before the integration ends, and the low gain reset value RST_L is read respectively. and the high gain reset value RST_H; next, the integration ends, the charge transfer control transistor 2 is turned on, and the photogenerated charge generated by the clamp photodiode 1 is transferred to the FD point to obtain the high gain signal voltage SIG_H; then the charge transfer control transistor 2 and The high dynamic range transistor 4 is turned on again at the same time, and the low gain signal value SIG_L is read at this time. During the conduction period of the high dynamic range transistor 4, the FD point is connected to the FDL point, which is equivalent to increasing the capacitance of the FD point, which can accommodate more photo-generated charges from the clamping photodiode 1, thereby improving the dynamic range of the pixel. The method of obtaining high and low gains through two charge transfers can expand the dynamic range of the pixel by 20 to 30 dB, so that the total dynamic range is close to or reaches 90 dB.

具有高低增益结构的高动态像素,虽然通过两次电荷转移提高了动态范围,但由于像素面积、填充比的限制,钳位光电二极管阱容量有限,当光强过强,或者积分时间较长时,积分时间内钳位光电二极管达到满阱,将不能容纳更多的电荷,从而限制了图像传感器的动态范围。High dynamic pixels with high and low gain structure, although the dynamic range is improved by two charge transfer, but due to the limitation of pixel area and filling ratio, the well capacity of the clamped photodiode is limited, when the light intensity is too strong, or when the integration time is long , the clamped photodiode reaches full well during the integration time and will not be able to hold more charges, thus limiting the dynamic range of the image sensor.

此外,还有采用多级横向溢出栅、双光电二极管、二极管连接的对数模式等扩展动态范围的方式,以上方法存在需要特殊工艺制造大电容、电路结构复杂、像素面积大且不适用于大面阵图像传感器、弱光下暗电流大信噪比差等缺点。In addition, there are also ways to extend the dynamic range, such as multi-level lateral overflow gates, dual photodiodes, and diode-connected logarithmic modes. The above methods require special processes to manufacture large capacitors, complex circuit structures, and large pixel areas, and are not suitable for large Disadvantages of area array image sensor, large dark current under low light, and poor signal-to-noise ratio.

发明内容SUMMARY OF THE INVENTION

本发明涉及一种同时具有高低增益和对数响应的高动态CMOS图像传感器,以及与之相应的时序控制方法和读取方式。本发明的目的在于在传统基于高低增益的高动态像素结构基础上,对复位晶体管和高动态范围晶体管额外进行一次离子注入,调整这两个NMOS管的阈值电压低于正常值,这两个晶体管共同构成了本发明所提出的电荷补偿元件。电荷补偿元件在超强光照下或者超长积分时间时工作在亚阈值区域,可向FD点注入电荷,用以补偿钳位光电二极管溢出到FD点的光生电荷,避免因钳位光电二极管达到满阱而导致的信号饱和,从而实现拓展动态范围。本发明利用了在不同光强下电荷补偿元件分别工作在截止区和亚阈值区的原理:在一定积分时间下(如10ms),在弱光(0.0001lux到0.1lux)和强光(0.1lux~10lux)下电荷补偿元件处于截止区,无导通电流,此时本发明的像素结构与具有高低增益结构的高动态像素技术功能相同,因此在弱光下具有很强的探测能力;在超强光(超过10lux)下电荷补偿元件工作在亚阈值区,利用亚阈值区晶体管电流电压为对数关系的特性实现对光生电荷的补偿,因此可在超高光强下成像。本发明在一次曝光下可以获得多幅相同积分时间的图像,对应弱光、强光和超强光,多幅图像即可合成一幅具有超高动态范围的图像。本发明同样利用了不同积分时间下电荷补偿元件分别工作在截止区和亚阈值区的原理:当像素结构处于一定光强(如10lux)下,当积分时间很短时(如100μs),电荷补偿元件处于截止区,无导通电流,此时本发明的像素结构与前述技术功能相同,因此在一定光强下积分时间较短时仍具有很强的成像能力;当积分时间很长时(如10ms),钳位光电二极管达到满阱,电荷补偿元件工作在亚阈值区,利用亚阈值区晶体管的电流电压为对数关系的特性实现对光生电荷的补偿。此时,输出信号与光强的对数成正比,与积分时间无关。The invention relates to a high dynamic CMOS image sensor with high and low gain and logarithmic response at the same time, and a timing control method and reading method corresponding to it. The purpose of the present invention is to perform an additional ion implantation on the reset transistor and the high dynamic range transistor on the basis of the traditional high and low gain based high dynamic pixel structure to adjust the threshold voltage of the two NMOS transistors to be lower than the normal value. Together they constitute the charge compensation element proposed by the present invention. The charge compensation element works in the sub-threshold region under super strong illumination or super long integration time, and can inject charges into the FD point to compensate for the photo-generated charge overflowing from the clamp photodiode to the FD point to avoid the clamp photodiode reaching full capacity. signal saturation caused by the trap, thus achieving extended dynamic range. The invention utilizes the principle that the charge compensation element works in the cut-off region and the sub-threshold region respectively under different light intensities: under a certain integration time (such as 10ms), under weak light (0.0001lux to 0.1lux) and strong light (0.1lux) ~10lux), the charge compensation element is in the cut-off region, and there is no on-current. At this time, the pixel structure of the present invention has the same function as the high-dynamic pixel technology with high and low gain structure, so it has strong detection ability under weak light; Under strong light (over 10 lux), the charge compensation element works in the sub-threshold region, and the photo-generated charge can be compensated by using the characteristic that the transistor current and voltage in the sub-threshold region have a logarithmic relationship, so imaging can be performed under ultra-high light intensity. The present invention can obtain multiple images with the same integration time under one exposure, corresponding to weak light, strong light and super strong light, and the multiple images can be synthesized into an image with ultra-high dynamic range. The invention also utilizes the principle that the charge compensation elements work in the cut-off region and the sub-threshold region respectively under different integration times: when the pixel structure is under a certain light intensity (such as 10 lux), when the integration time is very short (such as 100 μs), the charge compensation The element is in the cut-off region and has no on-current. At this time, the pixel structure of the present invention has the same function as the aforementioned technology, so it still has a strong imaging ability when the integration time is short under a certain light intensity; when the integration time is very long (such as 10ms), the clamping photodiode reaches full well, the charge compensation element works in the sub-threshold region, and the compensation of the photo-generated charge is realized by using the characteristic that the current and voltage of the transistor in the sub-threshold region are logarithmic. At this time, the output signal is proportional to the logarithm of the light intensity and has nothing to do with the integration time.

本发明的技术方案:Technical scheme of the present invention:

一种同时具有高低增益和对数响应的高动态CMOS图像传感器,结构如图3所示。像素结构包括钳位光电二极管1、电荷转移控制晶体管2、新型复位晶体管7、新型高动态范围晶体管8、源极跟随器5和行选晶体管6。新型复位晶体管7、新型高动态范围晶体管8共同构成本发明所述电荷补偿元件9。A high dynamic CMOS image sensor with both high and low gain and logarithmic response, the structure is shown in Figure 3. The pixel structure includes a clamped photodiode 1 , a charge transfer control transistor 2 , a novel reset transistor 7 , a novel high dynamic range transistor 8 , a source follower 5 and a row select transistor 6 . The new reset transistor 7 and the new high dynamic range transistor 8 together constitute the charge compensation element 9 of the present invention.

钳位光电二极管1作为光电探测元件,能够把接收的光信号转换为电信号并积累光生电荷,钳位光电二极管1的P端接GND,N端接电荷转移控制晶体管2的源极。电荷转移控制晶体管2用于将钳位光电二极管1中积累的光生电荷转移到FD点,电荷转移控制晶体管2的栅极的控制信号TX来自于图像传感器系统中的行控制模块,漏极连接到FD点。电荷补偿元件9包括新型复位晶体管7、新型高动态范围晶体管8,其中新型复位晶体管7的漏极接Vpix电位,源极连接到新型高动态范围晶体管8的漏极,新型高动态范围晶体管8的源极连接到FD点。新型复位晶体管7和新型高动态范围晶体管8共同构成的电荷补偿元件9的栅极控制信号RST和HDR来自于行控制模块,该元件弱光和强光下工作在截止区,超强光或者超长积分时间时工作在亚阈值区,以此来增加图像传感器的动态范围。源极跟随器5和行选晶体管6用于将像素信号输出到后续读出电路,源极跟随器5的栅极与FD点相连,漏极接至VDD,源极与行选晶体管6的漏极相连。行选晶体管6的栅端的控制信号SEL来自于行控制模块,源极与列总线相连,用于将像素的信号值输出到图像传感器系统的后续读出电路中。The clamping photodiode 1 is used as a photodetecting element, which can convert the received optical signal into an electrical signal and accumulate photo-generated charges. The P terminal of the clamping photodiode 1 is connected to GND, and the N terminal is connected to the source of the charge transfer control transistor 2 . The charge transfer control transistor 2 is used to transfer the photogenerated charge accumulated in the clamp photodiode 1 to the FD point. The control signal TX of the gate of the charge transfer control transistor 2 comes from the row control module in the image sensor system, and the drain is connected to FD point. The charge compensation element 9 includes a new type of reset transistor 7 and a new type of high dynamic range transistor 8, wherein the drain of the new type of reset transistor 7 is connected to the Vpix potential, and the source is connected to the drain of the new type of high dynamic range transistor 8. The source is connected to the FD point. The gate control signals RST and HDR of the charge compensation element 9 composed of the new reset transistor 7 and the new high dynamic range transistor 8 come from the row control module. Operating in the subthreshold region for long integration times increases the dynamic range of the image sensor. The source follower 5 and the row selection transistor 6 are used to output the pixel signal to the subsequent readout circuit. The gate of the source follower 5 is connected to the FD point, the drain is connected to VDD, and the source is connected to the drain of the row selection transistor 6. extremely connected. The control signal SEL of the gate terminal of the row selection transistor 6 comes from the row control module, and the source is connected to the column bus for outputting the signal value of the pixel to the subsequent readout circuit of the image sensor system.

所述的电荷转移控制晶体管2、源极跟随器5和行选晶体管6均采用标准NMOS晶体管工艺制造而成。The charge transfer control transistor 2 , the source follower 5 and the row selection transistor 6 are all manufactured by standard NMOS transistor technology.

所述的新型复位晶体管7、新型高动态范围晶体管8是在标准工艺基础上进行了一次额外的离子注入,用来调整晶体管的阈值电压,使其阈值电压低于正常值,故二者共同构成了所述的电荷补偿元件9。该元件在超强光下或者长时间积分时工作在亚阈值区域,可以向FD点注入电荷补偿钳位光电二极管1溢出到FD点的光生电荷,避免因钳位光电二极管达到满阱而导致信号饱和。利用亚阈值区晶体管电流电压为对数关系的特性,从而在弱光和强光的线性响应基础上获得对数响应,极大的扩展了图像传感器的动态范围。The new reset transistor 7 and the new high dynamic range transistor 8 are based on an additional ion implantation based on the standard process to adjust the threshold voltage of the transistor, so that the threshold voltage is lower than the normal value, so the two together constitute The described charge compensation element 9 is obtained. The device works in the sub-threshold region under super strong light or when integrating for a long time. It can inject the photo-generated charge from the charge compensation clamp photodiode 1 overflowing to the FD point to the FD point, so as to avoid the signal caused by the clamp photodiode reaching the full well. saturation. Using the characteristic that the transistor current and voltage in the sub-threshold region have a logarithmic relationship, the logarithmic response is obtained based on the linear response of weak light and strong light, which greatly expands the dynamic range of the image sensor.

一种同时具有高低增益和对数响应的高动态CMOS图像传感器的时序控制方法和读取方式如图4所示,具体步骤如下:A timing control method and reading method of a high dynamic CMOS image sensor with both high and low gain and logarithmic response are shown in Figure 4, and the specific steps are as follows:

步骤一,复位操作。Step 1, reset operation.

首先像素进入复位状态,电荷转移控制晶体管2、电荷补偿元件9同时导通一次,钳位光电二极管1中的电荷被清空,FD点电压被复位到Vpix。First, the pixel enters the reset state, the charge transfer control transistor 2 and the charge compensation element 9 are turned on at the same time, the charge in the clamping photodiode 1 is emptied, and the FD point voltage is reset to Vpix.

步骤二,积分操作。Step 2, integral operation.

复位操作结束后,电荷转移控制晶体管2和电荷补偿元件9的栅极控制信号电压分别下降到VTXL和VRL,像素进入积分阶段,钳位光电二极管1内开始积累光生电荷。After the reset operation, the gate control signal voltages of the charge transfer control transistor 2 and the charge compensation element 9 drop to VTXL and VRL respectively, the pixel enters the integration stage, and the clamp photodiode 1 begins to accumulate photo-generated charges.

1)弱光或者强光下曝光时间不够长时,钳位光电二极管1中产生的光生电荷小于等于钳位光电二极管1的满阱容量,光生电荷全部积累在钳位光电二极管1中,不会有多余的光生电荷通过电荷转移控制晶体管2流向FD点,因此积分时间内FD点电压不会发生变化。电荷补偿元件9的栅源电压VGS远远小于阈值电压,因此电荷补偿元件9工作于截止区,没有电流流向FD点。1) When the exposure time is not long enough under weak light or strong light, the photo-generated charge generated in the clamp photodiode 1 is less than or equal to the full well capacity of the clamp photodiode 1, and the photo-generated charge is all accumulated in the clamp photodiode 1. The excess photogenerated charges flow to the FD point through the charge transfer control transistor 2, so the voltage at the FD point will not change during the integration time. The gate-source voltage V GS of the charge compensation element 9 is much smaller than the threshold voltage, so the charge compensation element 9 works in the cut-off region, and no current flows to the FD point.

2)随着光强的增加或者积分时间的延长,积分过程中钳位光电二极管1中积累的光生电荷会超过自身的满阱容量,多余的光生电荷会通过电荷转移控制晶体管2流到FD点,构成过溢电流IOV,该电流与钳位光电二极管1所生成的光生电流Iph相等,2) With the increase of the light intensity or the extension of the integration time, the photo-generated charges accumulated in the clamp photodiode 1 during the integration process will exceed its full well capacity, and the excess photo-generated charges will flow to the FD point through the charge transfer control transistor 2. , which constitutes the overflow current I OV , which is equal to the photo-generated current I ph generated by the clamp photodiode 1,

IOV=Iph=ηRPin I OV =I ph =ηRP in

其中,η、R、Pin分别是钳位光电二极管1的量子效率、响应率和入射光功率;该电流使得FD点的电压下降,电压变化值ΔVFD与积分时间t成正比,Among them, η, R, and P in are the quantum efficiency, responsivity and incident light power of the clamped photodiode 1, respectively; the current causes the voltage at the FD point to drop, and the voltage change value ΔV FD is proportional to the integration time t,

ΔVFD=ηRPin·tΔV FD =ηRP in ·t

由于此时光强不够大,因此一定积分时间内,流到FD点的光生电荷有限,FD点的电压不会下降很多,电荷补偿元件9内部两个晶体管都处于关闭状态,工作状态不发生改变。此时体现为FD点电压变化与光强成正比。FD的电压值通过源极跟随器5、行选晶体管6及后续电路读出,作为对数模式的线性信号值LOG_S1。Since the light intensity is not large enough at this time, the photogenerated charge flowing to the FD point is limited within a certain integration time, and the voltage at the FD point will not drop a lot. At this time, it is reflected that the voltage change at the FD point is proportional to the light intensity. The voltage value of the FD is read out through the source follower 5, the row selection transistor 6 and the subsequent circuits as the linear signal value LOG_S1 in logarithmic mode.

3)当光强过强,或者积分时间较长时,钳位光电二极管1中积累的光生电荷远远超过自身的满阱容量,过多的光生电荷会通过电荷转移控制晶体管2流到FD点并且积累在FD点,产生持续的光生过溢电流IOV,导致FD点电压持续下降,使得电荷补偿元件9的VGS持续增高。由于电荷补偿元件9内部晶体管是在标准工艺的基础上进行了一次额外的离子注入,其阈值电压低于正常值,此时VGS值接近该阈值电压,使得电荷补偿元件9从截止区进入到亚阈值工作区域,导致有电流从Vpix流入FD点。该电流可以抵消从钳位光电二极管1流入到FD点的过溢电流IOV,因此被称为电荷补偿电流IC。如果光强足够强或者积分时间足够长时,光生过溢电流IOV与电荷补偿电流IC达到平衡状态,则FD点电压将不再随积分时间变化。此时,电荷补偿元件9工作在亚阈值区,电荷补偿电流IC如下式:3) When the light intensity is too strong or the integration time is long, the photo-generated charge accumulated in the clamp photodiode 1 far exceeds its full well capacity, and the excess photo-generated charge will flow to the FD point through the charge transfer control transistor 2. And accumulated at the FD point, a continuous photo-generated overflow current I OV is generated, which causes the voltage at the FD point to continuously drop, so that the V GS of the charge compensation element 9 continues to increase. Since the internal transistor of the charge compensation element 9 has undergone an additional ion implantation on the basis of the standard process, its threshold voltage is lower than the normal value, and the VGS value is close to the threshold voltage at this time, so that the charge compensation element 9 enters from the cut-off region to the Sub-threshold operating region, resulting in a current flowing from Vpix to the FD point. This current can cancel the overflow current I OV flowing from the clamp photodiode 1 to the FD point, so it is called the charge compensation current I C . If the light intensity is strong enough or the integration time is long enough, the photo-generated overflow current I OV and the charge compensation current IC reach a balance state, then the voltage at the FD point will no longer change with the integration time. At this time, the charge compensation element 9 works in the sub-threshold region, and the charge compensation current I C is as follows:

Figure BDA0003703432530000051
Figure BDA0003703432530000051

其中,IS是具有电流量纲的常量、VRST是电荷补偿元件9的栅极电压、VFD是FD点的电压、VTH是电荷补偿元件9的阈值电压、m是亚阈值斜率因子、VT是热电压。where IS is a constant having a current dimension, V RST is the gate voltage of the charge compensation element 9, V FD is the voltage at point FD, V TH is the threshold voltage of the charge compensation element 9, m is the subthreshold slope factor, V T is the thermal voltage.

在平衡后,电荷补偿电流与光生过溢电流相等,After balancing, the charge compensation current is equal to the photogenerated overflow current,

IOV=IC=ηRPin I OV = I C = ηRP in

可以得到VFD表达式: The VFD expression can be obtained:

Figure BDA0003703432530000052
Figure BDA0003703432530000052

根据上式可知,此时FD点的电压值变化与入射光强的对数成正比。该电压可通过源极跟随器5、行选晶体管6及后续电路读出,作为对数模式的信号值LOG_S2。According to the above formula, the change of the voltage value at the FD point at this time is proportional to the logarithm of the incident light intensity. This voltage can be read out by the source follower 5, the row select transistor 6 and subsequent circuits as the signal value LOG_S2 in logarithmic mode.

积分结束之前,再对FD点进行一次复位操作,电荷补偿元件9内部新型复位晶体管7、新型高动态范围晶体管8分别导通,在新型高动态范围晶体管8的栅极控制信号HDR为高电平VHDRH时,FD点电压作为低增益的复位值RST_L,可通过源极跟随器5、行选晶体管6及后续电路读出;随后HDR信号电压降为VRL,FD点电压作为高增益的复位值RST_H,可通过源极跟随器5、行选晶体管6及后续电路读出。至此像素电路积分阶段结束。Before the integration ends, perform a reset operation on the FD point again, the new reset transistor 7 and the new high dynamic range transistor 8 inside the charge compensation element 9 are turned on respectively, and the gate control signal HDR of the new high dynamic range transistor 8 is high level. When VHDRH, the FD point voltage is used as the low gain reset value RST_L, which can be read out through the source follower 5, row select transistor 6 and subsequent circuits; then the HDR signal voltage drops to VRL, and the FD point voltage is used as the high gain reset value RST_H , can be read out through source follower 5, row select transistor 6 and subsequent circuits. At this point, the integration phase of the pixel circuit ends.

步骤三,第一次电荷转移过程。Step 3, the first charge transfer process.

首先,电荷转移控制晶体管2导通,在电势差的作用下,钳位光电二极管1中积累的光生电荷通过电荷转移控制晶体管2转移到FD点。此时读取FD点的高增益信号值SIG_H,该电压可通过源极跟随器5、行选晶体管6及后续电路读出。First, the charge transfer control transistor 2 is turned on, and under the action of the potential difference, the photogenerated charges accumulated in the clamp photodiode 1 are transferred to the FD point through the charge transfer control transistor 2. At this time, the high-gain signal value SIG_H of the FD point is read, and the voltage can be read out through the source follower 5, the row selection transistor 6 and subsequent circuits.

步骤四,第二次电荷转移过程。Step 4, the second charge transfer process.

第一次电荷转移之后将新型高动态范围晶体管8开启,FD和FDL点短接,期间电荷转移控制晶体管2再次导通,钳位光电二极管1中剩余的光生电荷通过电荷转移控制晶体管2继续转移到FD和FDL点。读取FD点电压值为低增益的信号值SIG_L,该电压可通过源极跟随器5、行选晶体管6及后续电路读出。After the first charge transfer, the new high dynamic range transistor 8 is turned on, and the FD and FDL points are short-circuited. During this period, the charge transfer control transistor 2 is turned on again, and the remaining photo-generated charges in the clamp photodiode 1 continue to be transferred through the charge transfer control transistor 2. to FD and FDL points. The read voltage value of the FD point is the signal value SIG_L with a low gain, and the voltage can be read out through the source follower 5 , the row select transistor 6 and subsequent circuits.

本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器,其像素的输入光强与输出信号的关系如图5所示。在一定积分时间下,根据入射光强大小,高动态像素可分为4种工作状态:状态1(HG)和状态2(LG)为线性区域,二者的差别在于状态1对应输入光强最弱,这时由于像素的新型高动态范围晶体管8关闭,FD点电容值很小,像素的CVG(电荷-电压转换增益)较大,从而在弱光下可以得到非常高的信噪比。状态2对应强光,此时新型高动态范围晶体管8开启,像素的CVG较小,增大了满阱容量。状态3为状态2和状态4的过渡部分,此时输出信号仍与光强成正比。超强光下像素工作在状态4,电荷补偿元件9工作在亚阈值区,从钳位光电二极管流向FD的电流与电荷补偿元件9形成的补偿电流达到平衡,使输出信号与输入光强的对数成正比,从而扩大了动态范围。在一定积分时间下(如10ms),状态1对应光强范围为0.0001lux量级~0.1lux量级,状态2的光强范围为0.1lux量级~10lux量级,状态3的光强范围仍维持10lux量级,状态4的光强范围为10lux量级~10000lux量级以上。由此可见,采用本发明所述的电荷补偿元件9以及控制时序和信号读取方式,可在一帧成像下输出具有相同曝光时间的4幅图片,分别针对弱光、强光和超强光。与传统采用高低增益提高动态范围的方法相比,本发明除对应弱光和强光的状态1和状态2,还增加了状态3和4,其中状态3是过渡状态,输入光强变化不超过1个数量级,而状态4对应超强光,此时由于本发明所述的电荷补偿元件9工作在亚阈值,使得像素输出信号与光强对数成正比,极大地提高了图像传感器的动态范围,可在传统采用高低增益提高动态范围的基础上,再增加至少60dB的动态范围。For the high dynamic CMOS image sensor with both high and low gain and logarithmic response according to the present invention, the relationship between the input light intensity of the pixel and the output signal is shown in FIG. 5 . Under a certain integration time, according to the intensity of incident light, high dynamic pixels can be divided into four working states: state 1 (HG) and state 2 (LG) are linear regions, the difference between them is that state 1 corresponds to the highest input light intensity At this time, since the new high dynamic range transistor 8 of the pixel is turned off, the capacitance value of the FD point is small, and the CVG (charge-voltage conversion gain) of the pixel is large, so that a very high signal-to-noise ratio can be obtained in low light. State 2 corresponds to strong light, when the new high dynamic range transistor 8 is turned on, the CVG of the pixel is smaller, and the full well capacity is increased. State 3 is the transition between state 2 and state 4, and the output signal is still proportional to the light intensity at this time. Under super strong light, the pixel works in state 4, and the charge compensation element 9 works in the sub-threshold region. The current flowing from the clamping photodiode to the FD and the compensation current formed by the charge compensation element 9 reach a balance, so that the output signal and the input light intensity match. is proportional to the number, thereby expanding the dynamic range. Under a certain integration time (such as 10ms), the corresponding light intensity range of state 1 is in the order of 0.0001 lux to 0.1 lux, the light intensity range of state 2 is in the order of 0.1 lux to 10 lux, and the light intensity range of state 3 is still Maintaining the order of 10 lux, the light intensity of state 4 ranges from the order of 10 lux to the order of 10,000 lux or more. It can be seen that, by using the charge compensation element 9 and the control timing and signal reading method of the present invention, 4 pictures with the same exposure time can be outputted under one frame of imaging, respectively for weak light, strong light and super strong light. . Compared with the traditional method of using high and low gain to improve the dynamic range, the present invention adds states 3 and 4 in addition to states 1 and 2 corresponding to weak light and strong light. 1 order of magnitude, and state 4 corresponds to super-intensive light. At this time, since the charge compensation element 9 of the present invention works at a sub-threshold value, the pixel output signal is proportional to the logarithm of the light intensity, which greatly improves the dynamic range of the image sensor. , which can increase the dynamic range by at least 60dB on the basis of the traditional use of high and low gain to improve the dynamic range.

本发明的有益效果:Beneficial effects of the present invention:

(1)与传统的基于高低增益的高动态图像传感器像素结构相比较,本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器,不改变像素电路结构,通过电荷补偿元件增加一次额外的离子注入,降低构成电荷补偿元件的复位晶体管和高动态范围晶体管的阈值电压,使得在光强过强或积分时间过长时电荷补偿元件工作在亚阈值区域。此时,电荷补偿元件产生的补偿电流,与栅源电压成指数关系,会补偿经电荷转移控制晶体管流到FD点的光生过溢电流。随着光强的加大或积分时间的增加,两个电流会达到平衡,这时FD点电压将不再随积分时间变化,其电压值与入射光强的对数成正比,从而极大地拓展了图像传感器的动态范围。(1) Compared with the traditional high-low gain based high-dynamic image sensor pixel structure, the high-dynamic CMOS image sensor with high and low gain and logarithmic response described in the present invention does not change the pixel circuit structure, and increases through the charge compensation element. An additional ion implantation reduces the threshold voltage of the reset transistor and the high dynamic range transistor that constitute the charge compensation element, so that the charge compensation element operates in the sub-threshold region when the light intensity is too strong or the integration time is too long. At this time, the compensation current generated by the charge compensation element has an exponential relationship with the gate-source voltage, which will compensate the photo-generated overflow current flowing to the FD point through the charge transfer control transistor. With the increase of the light intensity or the increase of the integration time, the two currents will reach a balance. At this time, the voltage at the FD point will no longer change with the integration time, and its voltage value is proportional to the logarithm of the incident light intensity, thus greatly expanding the the dynamic range of the image sensor.

(2)与现有的图像传感器提高动态范围的方式相比,本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器像素结构,电路结构简单,通过阈值调整注入,使电荷补偿元件在超强光下或长时间曝光下工作在亚阈值区域,实现输入光强与输出信号的对数响应。可以在一帧下对具有不同光强照度的物体同时获取对数模式、高增益、低增益等多幅图像,这几幅图像具有相同的曝光时间,实现了基于双光电二极管结合不同积分时间技术的高动态图像传感器所无法探测的LED闪烁效应。(2) Compared with the way of improving the dynamic range of the existing image sensor, the pixel structure of the high dynamic CMOS image sensor with both high and low gain and logarithmic response described in the present invention has a simple circuit structure. The compensation element works in the sub-threshold region under super-intensive light or long-time exposure, and realizes the logarithmic response of the input light intensity and the output signal. Multiple images in logarithmic mode, high gain, low gain, etc. can be simultaneously acquired for objects with different light intensities under one frame. These images have the same exposure time, realizing the technology based on dual photodiodes combined with different integration times. LED flickering effect that cannot be detected by the high dynamic image sensor.

(3)与传统的实现高动态范围的图像传感器像素结构相比,本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器像素结构,在弱光和强光时为线性响应,信噪比与基于钳位光电二极管的传统4T像素结构相同,具有超强的弱光探测能力;同时在超强光时具有对数响应,输出信号不随光强变大而饱和,可将动态范围拓展3~4个数量级。(3) Compared with the traditional image sensor pixel structure that realizes high dynamic range, the high dynamic CMOS image sensor pixel structure with both high and low gain and logarithmic response according to the present invention has a linear response in weak light and strong light , the signal-to-noise ratio is the same as that of the traditional 4T pixel structure based on the clamp photodiode, and it has super weak light detection ability; at the same time, it has a logarithmic response under super strong light, and the output signal does not saturate with the increase of light intensity, which can change the dynamic The range is extended by 3 to 4 orders of magnitude.

(4)与传统的实现高动态范围的图像传感器像素结构相比,本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器像素结构根据入射光强区间可以分为4个工作状态,分别是线性高增益、线性低增益、对数线性和对数响应,分别对应弱光、强光、强光与超强光过渡,以及超强光。经后续读出电路对信号放大和模数转换后,4个状态的数字输出信号都包含了充足的信息量。将这4个状态的输出结果进行融合,可得到同时保留从弱光到超强光下图像所有细节的高动态范围图像。(4) Compared with the traditional image sensor pixel structure that realizes high dynamic range, the high dynamic CMOS image sensor pixel structure with both high and low gain and logarithmic response according to the present invention can be divided into 4 tasks according to the incident light intensity interval The states are linear high gain, linear low gain, log linear and log response, respectively corresponding to weak light, strong light, transition between strong light and super strong light, and super strong light. After signal amplification and analog-to-digital conversion by subsequent readout circuits, the digital output signals of the four states contain sufficient information. The output results of these four states are fused to obtain a high dynamic range image that retains all the details of the image from low light to super bright light.

附图说明Description of drawings

图1是高低增益高动态像素电路结构;Fig. 1 is the circuit structure of high and low gain high dynamic pixel;

图2是高低增益高动态像素工作时序;Figure 2 is the working timing of high and low gain and high dynamic pixels;

图3是同时具有高低增益和对数响应的高动态像素电路结构;Fig. 3 is a high dynamic pixel circuit structure with both high and low gain and logarithmic response;

图4是同时具有高低增益和对数响应的高动态像素工作时序及读取方式;Figure 4 is a high dynamic pixel working sequence and reading method with high and low gain and logarithmic response at the same time;

图5是同时具有高低增益和对数响应的高动态像素输入光强与输出信号关系曲线;Fig. 5 is a high dynamic pixel input light intensity and output signal relationship curve with both high and low gain and logarithmic response;

图6是实施例1工作时序及读取方式;Fig. 6 is working sequence and reading mode of embodiment 1;

图7是实施例2工作时序及读取方式;Fig. 7 is working sequence and reading mode of embodiment 2;

图8是实施例3同时具有单增益线性响应及对数响应的高动态像素电路结构;8 is a high dynamic pixel circuit structure having both a single-gain linear response and a logarithmic response in Embodiment 3;

图9是实施例3工作时序及读取方式;Fig. 9 is working sequence and reading mode of embodiment 3;

图中:1钳位光电二极管,2电荷转移控制晶体管,3复位晶体管,4高动态范围晶体管,5源极跟随器,6行选晶体管,7新型复位晶体管,8新型高动态范围晶体管,9电荷补偿元件。In the figure: 1 clamp photodiode, 2 charge transfer control transistors, 3 reset transistors, 4 high dynamic range transistors, 5 source followers, 6 row select transistors, 7 new reset transistors, 8 new high dynamic range transistors, 9 charge Compensation element.

具体实施方式Detailed ways

实施例1Example 1

实施例1所述的同时具有高低增益和对数响应的高动态CMOS图像传感器像素电路结构如图3所示。像素结构由钳位光电二极管1、电荷转移控制晶体管2、新型复位晶体管7、新型高动态范围晶体管8、源极跟随器5、行选晶体管6组成,像素中的电荷转移控制晶体管2、源极跟随器5、行选晶体管6均采用标准NMOS晶体管工艺制造而成,新型复位晶体管7、新型高动态范围晶体管8共同构成本发明所述电荷补偿元件9,是在标准工艺基础上进行了一次额外的离子注入,用来调整晶体管的阈值电压,使其阈值电压为-0.3V。电荷补偿元件9在超强光下或者长时间积分时工作在亚阈值区域,向FD点注入电荷,用以补偿钳位光电二极管1阱溢出到FD点的光生电荷,避免因钳位光电二极管达到满阱而导致的信号饱和。其中,钳位光电二极管1作为光电探测元件,可以把接收的光信号转换为电信号,P端接0V,N端接电荷转移控制晶体管2的源极。电荷转移控制晶体管2的栅极的控制信号TX来自于图像传感器系统中的行控制模块,漏极连接到FD点。电荷补偿元件9包括新型复位晶体管7、新型高动态范围晶体管8,其中新型复位晶体管7的漏极接Vpix电位3.3V,栅极控制信号RST来自于行控制模块,源极连接到新型高动态范围晶体管8的漏极,新型高动态范围晶体管8的栅极控制信号HDR来自于行控制模块,源极连接到FD点。源极跟随器5的栅极与FD点相连,漏极接至3.3V,源极与行选晶体管6的漏极相连。行选晶体管6的栅端的控制信号SEL来自于行控制模块,源极与列总线相连用于将像素的信号值输出到图像传感器系统的后续读出电路中。The pixel circuit structure of the high-dynamic CMOS image sensor with both high and low gain and logarithmic response described in Embodiment 1 is shown in FIG. 3 . The pixel structure consists of a clamp photodiode 1, a charge transfer control transistor 2, a new reset transistor 7, a new high dynamic range transistor 8, a source follower 5, and a row select transistor 6. The charge transfer control transistor 2 in the pixel, the source The follower 5 and the row selection transistor 6 are all manufactured by standard NMOS transistor process. The new reset transistor 7 and the new high dynamic range transistor 8 together constitute the charge compensation element 9 of the present invention, which is an additional process based on the standard process. The ion implantation is used to adjust the threshold voltage of the transistor so that its threshold voltage is -0.3V. The charge compensation element 9 works in the sub-threshold region under super strong light or when integrating for a long time, and injects charge into the FD point to compensate for the photo-generated charge overflowing from the clamp photodiode 1 well to the FD point, so as to avoid reaching the FD point due to the clamp photodiode. Signal saturation due to full well. Among them, the clamping photodiode 1 is used as a photodetection element, which can convert the received optical signal into an electrical signal. The P terminal is connected to 0V, and the N terminal is connected to the source of the charge transfer control transistor 2 . The control signal TX of the gate of the charge transfer control transistor 2 comes from the row control module in the image sensor system, and the drain is connected to the FD point. The charge compensation element 9 includes a new reset transistor 7 and a new high dynamic range transistor 8. The drain of the new reset transistor 7 is connected to the Vpix potential of 3.3V, the gate control signal RST comes from the row control module, and the source is connected to the new high dynamic range. The drain of the transistor 8, the gate control signal HDR of the new high dynamic range transistor 8 comes from the row control module, and the source is connected to the FD point. The gate of the source follower 5 is connected to the FD point, the drain is connected to 3.3V, and the source is connected to the drain of the row selection transistor 6 . The control signal SEL of the gate terminal of the row selection transistor 6 comes from the row control module, and the source is connected to the column bus for outputting the signal value of the pixel to the subsequent readout circuit of the image sensor system.

本发明所述的同时具有高低增益和对数响应的高动态CMOS图像传感器的具体时序控制方法和读取方式如图4所示,具体步骤如下:The specific timing control method and reading method of the high dynamic CMOS image sensor with high and low gain and logarithmic response according to the present invention are shown in FIG. 4 , and the specific steps are as follows:

步骤一,复位操作。Step 1, reset operation.

首先像素进入复位状态,电荷转移控制晶体管2、电荷补偿元件9同时导通一次,钳位光电二极管1中的电荷被清空,FD点电压被复位到3.3V。First, the pixel enters the reset state, the charge transfer control transistor 2 and the charge compensation element 9 are turned on at the same time, the charge in the clamping photodiode 1 is emptied, and the voltage at the FD point is reset to 3.3V.

步骤二,积分操作。Step 2, integral operation.

复位操作结束后,电荷转移控制晶体管2和电荷补偿元件9的栅极控制信号电压都下降到0V,像素进入积分阶段,钳位光电二极管1内开始积累光生电荷。After the reset operation, the gate control signal voltages of the charge transfer control transistor 2 and the charge compensation element 9 both drop to 0V, the pixel enters the integration stage, and the clamp photodiode 1 begins to accumulate photo-generated charges.

1)弱光或者强光下曝光时间不够长时,钳位光电二极管1中产生的光生电荷小于等于钳位光电二极管1的满阱容量,光生电荷全部积累在钳位光电二极管1中,不会有多余的光生电荷通过电荷转移控制晶体管2管流向FD点,因此积分时间内FD点电压不会发生变化。电荷补偿元件9的栅源电压VGS远远小于阈值电压-0.3V,因此电荷补偿元件9工作于截止区,没有电流流向FD点。1) When the exposure time is not long enough under weak light or strong light, the photo-generated charge generated in the clamp photodiode 1 is less than or equal to the full well capacity of the clamp photodiode 1, and all the photo-generated charges are accumulated in the clamp photodiode 1, which will not The excess photogenerated charges flow to the FD point through the charge transfer control transistor 2, so the voltage at the FD point will not change during the integration time. The gate-source voltage V GS of the charge compensation element 9 is much smaller than the threshold voltage -0.3V, so the charge compensation element 9 works in the cut-off region, and no current flows to the FD point.

2)随着光强的增加或者积分时间的延长,积分过程中钳位光电二极管1中积累的光生电荷会自身的满阱容量,多余的光生电荷会通过电荷转移控制晶体管2流到FD点,构成过溢电流IOV,该电流与钳位光电二极管1所生成的光生电流Iph相等,该电流使得FD点的电压下降,电压变化值与积分时间成正比。2) With the increase of the light intensity or the extension of the integration time, the photo-generated charges accumulated in the clamping photodiode 1 during the integration process will have its own full well capacity, and the excess photo-generated charges will flow to the FD point through the charge transfer control transistor 2, An overflow current I OV is formed, which is equal to the photo-generated current I ph generated by the clamping photodiode 1 , and this current causes the voltage at the FD point to drop, and the voltage change value is proportional to the integration time.

由于此时光强不够大,因此一定积分时间内,流到FD点的光生电荷有限,FD点的电压不会下降很多,电荷补偿元件内部两个晶体管都处于关闭状态,工作状态不发生改变。此时体现为FD点电压与光强成正比。积分结束前读取一次FD的电压值,作为对数模式的线性信号值LOG_S1。Since the light intensity is not large enough at this time, the photogenerated charge flowing to the FD point is limited within a certain integration time, and the voltage at the FD point will not drop a lot. At this time, it is reflected that the voltage at the FD point is proportional to the light intensity. Before the integration ends, read the voltage value of FD once as the linear signal value LOG_S1 in logarithmic mode.

3)当光强过强,或者积分时间较长时,钳位光电二极管1中积累的光生电荷远远超过自身的满阱容量,过多的光生电荷会通过电荷转移控制晶体管2流到FD点并且积累在FD点,产生持续的光生过溢电流IOV,导致FD点电压持续下降,使得电荷补偿元件的VGS持续增高。由于电荷补偿元件9内部两个晶体管的阈值电压被调整为-0.3V,此时VGS值接近该阈值电压,使得这两个晶体管从截止区进入到亚阈值工作区域,导致有电流从Vpix流入FD点。该电流可以抵消从钳位光电二极管1流入到FD点的光生过溢电流IOV,因此被称为电荷补偿电流IC。如果光强足够强或者积分时间足够长时,光生过溢电流IOV与电荷补偿电流IC达到平衡状态,则FD点电压将不再随积分时间变化。此时,电荷补偿元件9工作在亚阈值区,在平衡后,电荷补偿电流与光生过溢电流相等,可以得到此时FD点的电压值与入射光强的对数成正比。该电压可通过源极跟随器5、行选晶体管6及后续电路读出,作为对数模式的信号值LOG_S2。3) When the light intensity is too strong or the integration time is long, the photo-generated charge accumulated in the clamp photodiode 1 far exceeds its full well capacity, and the excess photo-generated charge will flow to the FD point through the charge transfer control transistor 2. And accumulated at the FD point, a continuous photo-generated overflow current I OV is generated, which causes the voltage at the FD point to continue to drop, so that the V GS of the charge compensation element continues to increase. Since the threshold voltage of the two transistors inside the charge compensation element 9 is adjusted to -0.3V, the VGS value is close to the threshold voltage at this time, so that the two transistors enter the sub-threshold working region from the cut-off region, resulting in a current flowing from Vpix FD point. This current can cancel the photo-overflow current I OV flowing from the clamp photodiode 1 to the FD point, so it is called the charge compensation current I C . If the light intensity is strong enough or the integration time is long enough, the photo-generated overflow current I OV and the charge compensation current IC reach a balance state, then the voltage at the FD point will no longer change with the integration time. At this time, the charge compensation element 9 works in the sub-threshold region. After balancing, the charge compensation current is equal to the photo-generated overflow current. It can be obtained that the voltage value at the FD point is proportional to the logarithm of the incident light intensity. This voltage can be read out by the source follower 5, the row select transistor 6 and subsequent circuits as the signal value LOG_S2 in logarithmic mode.

积分结束之前,再对FD点进行一次复位操作,电荷补偿元件内部晶体管7和8分别导通,在新型高动态范围晶体管8的栅极控制信号HDR为高电平4V时,图像传感器读出电路读取低增益的复位值RST_L,随后HDR信号电压降为0V,图像传感器的读出电路读取高增益的复位值RST_H,最后新型高动态范围晶体管8的栅极控制信号HDR降为低电平0V。至此像素电路积分阶段结束。Before the integration ends, perform a reset operation on the FD point again, and the internal transistors 7 and 8 of the charge compensation element are turned on respectively. When the gate control signal HDR of the new high dynamic range transistor 8 is at a high level of 4V, the image sensor readout circuit. The low gain reset value RST_L is read, then the HDR signal voltage drops to 0V, the readout circuit of the image sensor reads the high gain reset value RST_H, and finally the gate control signal HDR of the new high dynamic range transistor 8 drops to a low level 0V. At this point, the integration phase of the pixel circuit ends.

步骤三,第一次电荷转移过程。Step 3, the first charge transfer process.

首先,电荷转移控制晶体管2导通,在电势差的作用下,钳位光电二极管1中积累的光生电荷通过电荷转移控制晶体管2转移到FD点。此时读取FD点的高增益信号值SIG_H。First, the charge transfer control transistor 2 is turned on, and under the action of the potential difference, the photogenerated charges accumulated in the clamp photodiode 1 are transferred to the FD point through the charge transfer control transistor 2. At this time, the high gain signal value SIG_H of the FD point is read.

步骤四,第二次电荷转移过程。Step 4, the second charge transfer process.

第一次电荷转移之后将新型高动态范围晶体管8开启,FD和FDL点短接,期间电荷转移控制晶体管2再次导通,钳位光电二极管1中剩余的光生电荷通过电荷转移控制晶体管2继续转移到FD和FDL点。读取FD点电压值为低增益的信号值SIG_L。After the first charge transfer, the new high dynamic range transistor 8 is turned on, and the FD and FDL points are short-circuited. During this period, the charge transfer control transistor 2 is turned on again, and the remaining photo-generated charges in the clamp photodiode 1 continue to be transferred through the charge transfer control transistor 2. to FD and FDL points. Read the signal value SIG_L with the low gain voltage value at the FD point.

实施例2Example 2

实施例2所述的高动态范围图像传感器像素电路结构如图3所示。实施例2所述的高动态范围CMOS图像传感器像素结构的时序和读取方式如图7所示。实施例2与实施例1工作过程基本相同,不同点在于在积分过程中电荷补偿元件的栅电压值,不是降低到0V,而是到1V,目的是提高电荷补偿元件源极电压,即FD点的电压,使其更容易被图像传感器中像素之后的读出电路进行信号处理和读出。The pixel circuit structure of the high dynamic range image sensor described in Embodiment 2 is shown in FIG. 3 . The timing sequence and reading method of the pixel structure of the high dynamic range CMOS image sensor described in Embodiment 2 are shown in FIG. 7 . The working process of Example 2 is basically the same as that of Example 1. The difference is that the gate voltage value of the charge compensation element is not reduced to 0V, but to 1V during the integration process. The purpose is to increase the source voltage of the charge compensation element, that is, the FD point. voltage, making it easier for signal processing and readout by the readout circuitry after the pixel in the image sensor.

实施例3Example 3

本发明前述的同时具有高低增益和对数响应的高动态CMOS图像传感器像素中的电荷补偿元件由两个晶体管构成,在本实施例中还可以将电荷补偿元件中的新型复位晶体管和新型高动态范围晶体管合并为一个晶体管,构成同时具有单增益线性响应及对数响应的高动态范围像素,其电路结构如图8所示。The aforementioned charge compensation element in the high-dynamic CMOS image sensor pixel with both high and low gain and logarithmic response of the present invention is composed of two transistors. In this embodiment, the new reset transistor in the charge compensation element and the new high dynamic The range transistors are combined into one transistor to form a high dynamic range pixel with both a single-gain linear response and a logarithmic response. The circuit structure is shown in Figure 8.

实施例3所述像素电路结构的工作时序和读取方式如图9所示。像素电路工作仍然分为复位阶段、积分阶段和电荷转移阶段。复位阶段电荷补偿元件9和电荷转移控制晶体管2同时导通一次,将钳位光电二极管1内电荷清空同时将FD点复位到3.3V,积分结束前读出电路采样一次对数信号LOG_SIG,之后再对FD点进行一次复位操作,读出电路读取线性复位信号值LIN_RST,然后电荷转移控制晶体管2导通一次,将钳位光电二极管1内的光生电荷转移到FD点,读出电路读取线性信号值LIN_SIG。The working timing and reading method of the pixel circuit structure described in Embodiment 3 are shown in FIG. 9 . The pixel circuit work is still divided into a reset phase, an integration phase and a charge transfer phase. In the reset stage, the charge compensation element 9 and the charge transfer control transistor 2 are turned on at the same time, the charge in the clamp photodiode 1 is emptied and the FD point is reset to 3.3V. Before the integration ends, the readout circuit samples the logarithmic signal LOG_SIG once, and then Perform a reset operation on the FD point, the readout circuit reads the linear reset signal value LIN_RST, and then the charge transfer control transistor 2 is turned on once to transfer the photogenerated charge in the clamp photodiode 1 to the FD point, and the readout circuit reads the linearity. Signal value LIN_SIG.

Claims (4)

1. A high dynamic CMOS image sensor with both high and low gain and logarithmic response is characterized in that the pixel structure comprises a clamping photodiode (1), a charge transfer control transistor (2), a charge compensation element (9), a source follower (5) and a row selection transistor (6);
the clamp photodiode (1) is used as a photoelectric detection element and can convert a received optical signal into an electric signal and accumulate photo-generated charges, the P end of the clamp photodiode (1) is connected with GND, and the N end of the clamp photodiode is connected with the source electrode of the charge transfer control transistor (2); the charge transfer control transistor (2) is used for transferring the photo-generated charge accumulated in the clamping photodiode to an FD point, a control signal TX of a grid electrode of the charge transfer control transistor (2) comes from a row control module in the image sensor system, and a drain electrode of the charge transfer control transistor is connected to the FD point; the charge compensation element (9) comprises a novel reset transistor (7) and a novel high dynamic range transistor (8), wherein the drain electrode of the novel reset transistor (7) is connected with the Vpix potential, the source electrode of the novel reset transistor is connected to the drain electrode of the novel high dynamic range transistor (8), and the source electrode of the novel high dynamic range transistor (8) is connected to the FD point; grid control signals RST and HDR of a charge compensation element 9 formed by the novel reset transistor (7) and the novel high dynamic range transistor (8) come from a row control module, the element works in a cut-off region under weak light and strong light, and works in a subthreshold region under super-strong light or super-long integration time, so that the dynamic range of the image sensor is increased; the source follower (5) and the row selection transistor (6) are used for outputting pixel signals to a subsequent readout circuit, the grid electrode of the source follower (5) is connected with an FD point, the drain electrode is connected to VDD, and the source electrode is connected with the drain electrode of the row selection transistor (6); a control signal SEL of a grid end of the row selection transistor (6) is from a row control module, and a source electrode of the control signal SEL is connected with a column bus and used for outputting a signal value of a pixel to a subsequent reading circuit of the image sensor system;
the charge transfer control transistor (2), the source follower (5) and the row selection transistor (6) are all manufactured by adopting a standard NMOS transistor process;
the novel reset transistor (7) and the novel high dynamic range transistor (8) are subjected to one additional ion implantation on the basis of a standard process to adjust the threshold voltage of the transistors to be lower than a normal value, so that the two transistors jointly form the charge compensation element 9; the element works in a sub-threshold region under super-strong light or long-time integration, photogenerated charges overflowing to an FD point of a charge compensation clamping photodiode (1) can be injected into the FD point, and signal saturation caused by the fact that the clamping photodiode reaches a full well is avoided; the characteristic that the current and the voltage of the transistor in the sub-threshold region are in logarithmic relation is utilized, so that logarithmic response is obtained on the basis of linear response of weak light and strong light, and the dynamic range of the image sensor is greatly expanded.
2. The timing control method and reading method of the high dynamic CMOS image sensor having both high and low gains and logarithmic response according to claim 1, wherein the specific steps are as follows:
step one, resetting operation;
firstly, the pixel enters a reset state, the charge transfer control transistor (2) and the charge compensation element (9) are simultaneously conducted once, the charge in the clamping photodiode (1) is cleared, and the FD point voltage is reset to Vpix;
step two, integral operation;
after the reset operation is finished, the grid control signal voltages of the charge transfer control transistor (2) and the charge compensation element (9) are respectively reduced to VTXL and VRL, the pixel enters an integration stage, and the clamp photodiode (1) starts to accumulate photo-generated charges;
1) when the exposure time under weak light or strong light is not long enough, the photo-generated charge generated in the clamping photodiode (1) is less than or equal to the full-well capacity of the clamping photodiode (1), the photo-generated charge is completely accumulated in the clamping photodiode (1), and no redundant photo-generated charge flows to an FD point through the charge transfer control transistor (2), so that the voltage of the FD point does not change within the integration time; gate-source voltage V of charge compensation element (9) GS Much smaller than the threshold voltage, so that the charge compensation element (9) operates in the cut-off region, with no current flowing to the FD point;
2) with the increase of light intensity or the extension of integration time, the photo-generated charge accumulated in the clamping photodiode (1) in the integration process can exceed the full-well capacity of the clamping photodiode, and the redundant photo-generated charge can flow to an FD point through the charge transfer control transistor (2) to form an over-current I OV The current is in parallel with a photo-generated current I generated by the clamped photodiode (1) ph The number of the first and the second antennas is equal,
I OV =I ph =ηRP in
wherein eta, R, P in The quantum efficiency, the responsivity and the incident optical power of the clamping photodiode (1) respectively; the current causes the voltage at FD point to drop by a voltage change value DeltaV FD In proportion to the integration time t,
ΔV FD =ηRP in ·t
because the light intensity is not large enough at the moment, the photo-generated charges flowing to the FD point are limited within a certain integration time, the voltage of the FD point cannot be reduced greatly, two transistors in the charge compensation element (9) are both in a closed state, and the working state is not changed; the voltage change of the FD point is directly proportional to the light intensity; the voltage value of FD is read out through a source follower (5), a row selection transistor (6) and a subsequent circuit and is used as a linear signal value LOG _ S1 of a logarithmic mode;
3) when the intensity of the light is too strong,or when the integration time is longer, the photo-generated charge accumulated in the clamping photodiode (1) far exceeds the full-trap capacity of the clamping photodiode, the excessive photo-generated charge flows to an FD point through the charge transfer control transistor (2) and is accumulated at the FD point, and continuous photo-generated over-current I is generated OV Causing the voltage at the FD point to continuously decrease, so that the V of the charge compensation element (9) GS Continuously increasing height; since the transistor in the charge compensation element (9) is subjected to an additional ion implantation based on the standard process, the threshold voltage is lower than the normal value, and V is the value GS A value close to the threshold voltage such that the charge compensation element (9) enters the sub-threshold working region from the cut-off region, resulting in a current flowing from Vpix to the FD point; this current can cancel an excessive current I flowing from the clamp photodiode (1) to the FD point OV And is therefore referred to as charge compensation current I C (ii) a If the light intensity is strong enough or the integration time is long enough, the light-generated excessive current I OV And a charge compensation current I C When the balance state is reached, the voltage of the FD point does not change along with the integration time any more; in this case, the charge compensation element (9) operates in the subthreshold region, and the charge compensation current I C The following formula:
Figure FDA0003703432520000021
wherein, I S Is a constant, V, having a current dimension RST Is the gate voltage, V, of the charge compensation element (9) FD Is the voltage, V, of the FD point TH Is the threshold voltage of the charge compensation element (9), m is the sub-threshold slope factor, V T Is a thermal voltage;
after balancing, the charge compensation current is equal to the photo-generated overflow current,
I OV =I C =ηRP in
can obtain V FD Expression:
Figure FDA0003703432520000031
according to the above formula, the voltage value change of the FD point is directly proportional to the logarithm of the incident light intensity; the voltage can be read out through a source follower (5), a row selection transistor (6) and a subsequent circuit and is used as a LOG mode signal value LOG _ S2;
before the integration is finished, resetting operation is carried out on the FD point once again, a novel reset transistor (7) and a novel high dynamic range transistor (8) in the charge compensation element (9) are respectively conducted, when a grid control signal HDR of the novel high dynamic range transistor (8) is a high level VHDRH, the voltage of the FD point is used as a reset value RST _ L of low gain and can be read out through a source follower (5), a row selection transistor (6) and a subsequent circuit; then the voltage of the HDR signal is reduced to VRL, and the voltage of the FD point serves as a reset value RST _ H with high gain and can be read out through a source follower (5), a row selection transistor (6) and a subsequent circuit; ending the integration stage of the pixel circuit;
step three, a first charge transfer process;
firstly, a charge transfer control transistor (2) is conducted, and photo-generated charges accumulated in a clamping photodiode (1) are transferred to an FD point through the charge transfer control transistor (2) under the action of potential difference; reading a high-gain signal value SIG _ H of the FD point, wherein the voltage can be read out through a source follower (5), a row selection transistor (6) and a subsequent circuit;
step four, a second charge transfer process;
after the first charge transfer, the novel high dynamic range transistor (8) is started, the FD and the FDL points are in short circuit, the charge transfer control transistor (2) is conducted again in the period, and the rest photo-generated charges in the clamping photodiode (1) are continuously transferred to the FD and FDL points through the charge transfer control transistor (2); the voltage value at the FD point is read as a signal value SIG _ L with low gain, and the voltage can be read out through a source follower (5), a row selection transistor (6) and a subsequent circuit.
3. The timing control method and reading method according to claim 2, wherein the high dynamic pixel is divided into 4 working states according to the incident light intensity under a certain integration time: the states 1-HG and 2-LG are linear regions, the difference between the states is that the input light intensity corresponding to the state 1 is the weakest, at this time, because the novel high dynamic range transistor (8) of the pixel is closed, the capacitance value of the FD point is very small, and the CVG of the pixel is relatively large, so that a very high signal-to-noise ratio can be obtained under weak light; the state 2 corresponds to strong light, at the moment, the novel high dynamic range transistor (8) is started, the CVG of the pixel is small, and the full-well capacity is increased; state 3 is the transition between state 2 and state 4, where the output signal is still proportional to the light intensity; under the ultra-strong light, the pixel works in a state 4, the charge compensation element works in a subthreshold region, the current flowing to the FD from the clamping photodiode and the compensation current formed by the charge compensation element reach balance, so that the output signal is in direct proportion to the logarithm of the input light intensity, and the dynamic range is expanded; under a certain integration time, the light intensity range corresponding to the state 1 is 0.0001lux magnitude to 0.1lux magnitude, the light intensity range corresponding to the state 2 is 0.1lux magnitude to 10lux magnitude, the light intensity range corresponding to the state 3 still maintains 10lux magnitude, and the light intensity range corresponding to the state 4 is more than 10lux magnitude to 10000lux magnitude; therefore, 4 pictures with the same exposure time can be output under one frame of imaging by adopting the charge compensation element (9) and a control time sequence and signal reading mode, and the 4 pictures are respectively used for weak light, strong light and ultra-strong light.
4. The CMOS image sensor with high dynamic range and high gain simultaneously as claimed in claim 1, wherein the charge compensation device 9 formed by the novel reset transistor (7) and the novel high dynamic range transistor (8) can be replaced by combining the novel reset transistor and the novel high dynamic range transistor in the charge compensation device into one transistor to form a high dynamic range pixel with single gain linear response and logarithmic response simultaneously; the pixel circuit still comprises a reset stage, an integration stage and a charge transfer stage; the charge compensation element (9) and the charge transfer control transistor (2) are simultaneously conducted once in the reset stage, charges in the clamping photodiode (1) are emptied, the FD point is reset to Vpix, a readout circuit samples a logarithmic signal LOG _ SIG once before integration is finished, then the FD point is reset once again, the readout circuit reads a linear reset signal value LIN _ RST, then the charge transfer control transistor (2) is conducted once, photo-generated charges in the clamping photodiode (1) are transferred to the FD point, and the readout circuit reads the linear signal value LIN _ SIG.
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CN102752560A (en) * 2012-06-21 2012-10-24 吉林大学 Ultra-wide dynamic range image sensor based on pixel charge compensation technology
CN114640808A (en) * 2022-03-09 2022-06-17 大连理工大学 High Dynamic Range Image Sensor Based on Reset Transistor Multiplexing Technology

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CN102752560A (en) * 2012-06-21 2012-10-24 吉林大学 Ultra-wide dynamic range image sensor based on pixel charge compensation technology
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