CN105258795B - A kind of electric capacity trans-impedance amplifier circuit with pure digi-talization output for faint light detection - Google Patents

A kind of electric capacity trans-impedance amplifier circuit with pure digi-talization output for faint light detection Download PDF

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CN105258795B
CN105258795B CN201510665728.0A CN201510665728A CN105258795B CN 105258795 B CN105258795 B CN 105258795B CN 201510665728 A CN201510665728 A CN 201510665728A CN 105258795 B CN105258795 B CN 105258795B
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CN105258795A (en
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赵毅强
李雪民
辛睿山
王佳
张赟
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Tianjin University
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Abstract

本发明属于光探测领域,尤其涉及一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,包括信号产生电路、基于CTIA的光探测电路和两级反相器,并依次连接,信号产生电路包括采样信号SELECT电路和方波复位信号RESET电路,采样信号SELECT电路的输入端输入初始方波信号,初始方波信号经过第一延迟单元后送给异或门的一个输入端,异或门另一个输入端则为初始方波信号,异或门输出的脉冲信再与初始方波信号作与运算得到采样信号SELECT,方波复位信号RESET由初始方波信号经过三级延迟单元得到。本发明的有益效果:通过该新型CTIA结构,在探测微弱光时,可以实现纯数字化输出,便于后续电路进行处理。

The invention belongs to the field of light detection, in particular to a capacitive transimpedance amplifier circuit with pure digital output for weak light detection, including a signal generation circuit, a CTIA-based light detection circuit and a two-stage inverter, which are connected in sequence, The signal generation circuit includes a sampling signal SELECT circuit and a square wave reset signal RESET circuit. The input terminal of the sampling signal SELECT circuit inputs an initial square wave signal, and the initial square wave signal is sent to an input end of an exclusive OR gate after passing through the first delay unit. The other input terminal of the OR gate is the initial square wave signal, and the pulse signal output by the XOR gate is ANDed with the initial square wave signal to obtain the sampling signal SELECT, and the square wave reset signal RESET is obtained from the initial square wave signal through the three-stage delay unit . Beneficial effects of the present invention: through the novel CTIA structure, pure digital output can be realized when weak light is detected, which is convenient for subsequent circuits to process.

Description

一种用于微弱光探测的带纯数字化输出的电容跨阻放大器 电路A Capacitive Transimpedance Amplifier with Purely Digital Output for Faint Light Detection circuit

技术领域technical field

本发明属于光探测领域,尤其涉及一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路。The invention belongs to the field of light detection, in particular to a capacitive transimpedance amplifier circuit with pure digital output for weak light detection.

背景技术Background technique

随着微电子技术的日趋成熟,面向集成电路与信息系统敏感信息获取方法日渐增多,一般可分为非入侵式攻击和入侵式攻击。其中,入侵式攻击通过开盖、钻孔、腐蚀等手段实现对芯片封装的破坏,利用拍照和微探针等技术,提取版图、密码等重要信息,而封装的破坏则会使芯片置于光照之下。因此,为了增强芯片或者系统的抗攻击能力,往往会设计微弱光探测器感测开盖、钻孔等信息,为芯片或系统提供预警信号。With the maturity of microelectronics technology, there are more and more ways to acquire sensitive information for integrated circuits and information systems, which can generally be divided into non-invasive attacks and intrusive attacks. Among them, the intrusive attack destroys the chip package by opening the cover, drilling, corrosion and other means, and uses technologies such as photography and microprobes to extract important information such as layout and passwords, and the destruction of the package will expose the chip to light. under. Therefore, in order to enhance the anti-attack capability of chips or systems, weak light detectors are often designed to sense information such as cover opening and drilling, and provide early warning signals for chips or systems.

考虑到开盖、钻孔等可能发生在微弱光强之下,因此所设计的光探测器须实现在光照强度大于某一微弱光强时发出报警信号。而在微弱光照下,产生的光生电流较小,暗电流对其影响较大,因此考虑使用电容跨阻放大器(CTIA)结构实现对光照强度的检测。Considering that opening the cover and drilling may occur under weak light intensity, the designed photodetector must realize an alarm signal when the light intensity is greater than a certain weak light intensity. However, under weak light, the generated photocurrent is small, and the dark current has a great influence on it. Therefore, the structure of capacitive transimpedance amplifier (CTIA) is considered to realize the detection of light intensity.

常见的基于CTIA的光探测电路如图1,它是由运放和反馈电容以及开关构成的一种复位积分型光探测电路,探测器利用半导体的光生福特效应,即当PN结用一定波长的光照射时,由于内建电势场在PN结内部产生光生电压,如果将PN结接入回路中,即会出现光生电流的现象。其原理简述如下:当RESET信号为高时,开关S0导通,进入复位模式,电容C0被复位,此时SELECT为低,开关S1断开,C1上保存着上一个积分时期的积分值;当RESET信号为低时,开关S0断开,SELECT信号为高,开关S0闭合,进入积分模式,C1上的电压持续上升,直到下一个复位周期开始为止,常见的基于CTIA的光探测电路的输出波形如图2。为了将该波形转换成高低电平式的信号,通常在开关S1后面加两级反相器如图3,光强大小体现在PWM信号的占空比上,占空比越大说明光照强度越强。该结构在临界光强时输出为占空比50%的方波,而在临界光强之下时输出为低电平,输出波形如图4。A common CTIA-based photodetection circuit is shown in Figure 1. It is a reset-integral photodetection circuit composed of an operational amplifier, a feedback capacitor, and a switch. When light is irradiated, since the built-in electric potential field generates a photo-generated voltage inside the PN junction, if the PN junction is connected to the circuit, a phenomenon of photo-generated current will appear. The principle is briefly described as follows: when the RESET signal is high, the switch S 0 is turned on and enters the reset mode, and the capacitor C 0 is reset. At this time, the SELECT is low, the switch S 1 is turned off, and the previous integration period is saved on C 1 When the RESET signal is low, the switch S 0 is disconnected, the SELECT signal is high, the switch S 0 is closed, and enters the integral mode, and the voltage on C 1 continues to rise until the next reset cycle begins. Common based on The output waveform of the photodetection circuit of CTIA is shown in Fig. 2 . In order to convert the waveform into a high-low level signal, two - stage inverters are usually added behind the switch S1 as shown in Figure 3. The light intensity is reflected in the duty cycle of the PWM signal. The larger the duty cycle, the greater the light intensity. stronger. The output of this structure is a square wave with a duty ratio of 50% at the critical light intensity, and the output is low level when the light intensity is below the critical light intensity. The output waveform is shown in Fig. 4 .

相比基于CTIA的光探测电路,加两级反相器后的电路结构具有输出信号为数字化PWM的优点。但由于该电路的用途为探测微弱光,为了便于后续电路对报警信号的处理,理想的输出报警信号为纯数字化输出,而PWM信号则需要使用计数器等将占空比信息转换成高电平或者低电平信号,而这样做一方面增加了系统复杂性,另一方面增加了系统功耗。因此需要一种用于微弱光探测的新型带纯数字化输出的CTIA结构。Compared with the CTIA-based light detection circuit, the circuit structure after adding two-stage inverter has the advantage that the output signal is digital PWM. However, since the purpose of this circuit is to detect weak light, in order to facilitate the processing of the alarm signal by the subsequent circuit, the ideal output alarm signal is a pure digital output, while the PWM signal needs to use a counter to convert the duty ratio information into a high level or Low-level signals, while doing so increases the complexity of the system on the one hand, and increases the power consumption of the system on the other hand. Therefore, there is a need for a new CTIA structure with purely digital output for weak light detection.

发明内容Contents of the invention

为要解决的上述问题,本发明提供一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路。To solve the above problems, the present invention provides a capacitive transimpedance amplifier circuit with pure digital output for weak light detection.

本发明的技术方案:一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,其特征在于包括信号产生电路、基于CTIA的光探测电路和两级反相器,所述信号产生电路、所述基本CTIA的光探测电路和所述两级反相器依次连接,所述信号产生电路包括用于产生尖脉冲式的采样信号SELECT电路和方波复位信号RESET电路。Technical scheme of the present invention: a capacitive transimpedance amplifier circuit with pure digital output for weak light detection, characterized in that it includes a signal generation circuit, a CTIA-based light detection circuit and a two-stage inverter, the signal generation The circuit, the photodetection circuit of the basic CTIA and the two-stage inverter are connected in sequence, and the signal generation circuit includes a SELECT circuit for generating a spike-like sampling signal and a RESET circuit for a square-wave reset signal.

所述采样信号SELECT电路的输入端输入初始方波信号,所述初始方波信号经过第一级延时单之后送给异或门的一个输入端,所述异或门另一个输入端则为所述初始方波信号,所述异或门输出为脉冲信号,所述脉冲信号的频率为所述初始方波信号的2倍,所述脉冲信号的脉冲宽度由所述第一延时单元决定;所述脉冲信号再与所述初始方波信号作与运算得到采样信号SELECT,所述采样信号SELECT具有和所述初始方波信号同频率,所述采样信号SELECT与所述初始方波信号的上升沿同时到达。The input terminal of the sampling signal SELECT circuit inputs an initial square wave signal, and the initial square wave signal is sent to an input terminal of an XOR gate after passing through a first-stage delay sheet, and the other input terminal of the XOR gate is The initial square wave signal, the output of the XOR gate is a pulse signal, the frequency of the pulse signal is twice that of the initial square wave signal, and the pulse width of the pulse signal is determined by the first delay unit Described pulse signal and described initial square wave signal do and operation again and obtain sampling signal SELECT, and described sampling signal SELECT has the same frequency with described initial square wave signal, described sampling signal SELECT and described initial square wave signal The rising edges arrive at the same time.

所述方波复位信号RESET电路输入端输入所述初始方波信号,所述初始方波信号经过第一延时单元、第二延时单元和第三延时单元产生方波复位信号RESET信号,所述方波复位信号RESET的上升沿与所述采样信号SELECT的下降沿的时间差第二延时单元和第三延时单元引起的延时。The input terminal of the square wave reset signal RESET circuit inputs the initial square wave signal, and the initial square wave signal generates a square wave reset signal RESET signal through the first delay unit, the second delay unit and the third delay unit, The time difference between the rising edge of the square wave reset signal RESET and the falling edge of the sampling signal SELECT is the delay caused by the second delay unit and the third delay unit.

所述第一延时单元、所述第二延时单元和所述第三延时单元为相同单元或不同单元。本发明的有益效果:通过该新型CTIA结构,在探测微弱光时,可以实现纯数字化输出,便于后续电路进行处理。The first delay unit, the second delay unit and the third delay unit are the same unit or different units. Beneficial effects of the present invention: through the novel CTIA structure, pure digital output can be realized when weak light is detected, which is convenient for subsequent circuits to process.

附图说明Description of drawings

图1是常见基于CTIA的光探测电路的结构示意图。Figure 1 is a schematic diagram of the structure of a common CTIA-based photodetection circuit.

图2是图1的输出波形。Figure 2 is the output waveform of Figure 1.

图3是带两级反相器的CTIA结构的结构示意图。FIG. 3 is a schematic structural diagram of a CTIA structure with two stages of inverters.

图4是图3的输出波形。FIG. 4 is the output waveform of FIG. 3 .

图5是本发明电路的结构示意图。Fig. 5 is a structural schematic diagram of the circuit of the present invention.

图6是本发明强光下的时序图。Fig. 6 is a timing diagram of the present invention under strong light.

图7是本发明弱光下的时序图。Fig. 7 is a timing diagram of the present invention under weak light.

图8是本发明无光下的时序图。Fig. 8 is a timing diagram of the present invention in the absence of light.

图9是本发明的信号产生电路的结构示意图。FIG. 9 is a schematic structural diagram of the signal generating circuit of the present invention.

图10是图9中延迟单元的结构示意图。FIG. 10 is a schematic structural diagram of the delay unit in FIG. 9 .

具体实施方式detailed description

下面结合附图1对本发明的一种具体实施方式做出说明。A specific embodiment of the present invention will be described below in conjunction with accompanying drawing 1 .

本发明涉及一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,其特征在于包括信号产生电路、基于CTIA的光探测电路和两级反相器,信号产生电路、基本CTIA的光探测电路和两级反相器依次连接。The invention relates to a capacitive transimpedance amplifier circuit with pure digital output for weak light detection, which is characterized in that it includes a signal generation circuit, a CTIA-based light detection circuit and a two-stage inverter, a signal generation circuit, and a basic CTIA The light detection circuit and the two-stage inverters are connected in sequence.

信号产生电路包括用于产生尖脉冲式的采样信号SELECT电路和方波复位信号RESET电路。采样信号SELECT电路的输入端输入初始方波信号,初始方波信号经过第一级延时单之后送给异或门的一个输入端,异或门另一个输入端则为初始方波信号,异或门输出为脉冲信号,脉冲信号的频率为初始方波信号的2倍,脉冲信号的脉冲宽度由第一延时单元决定;脉冲信号再与初始方波信号作与运算得到采样信号SELECT,采样信号SELECT具有和初始方波信号同频率,采样信号SELECT与初始方波信号的上升沿同时到达。The signal generating circuit includes a sampling signal SELECT circuit and a square wave reset signal RESET circuit for generating sharp pulses. The input terminal of the sampling signal SELECT circuit inputs the initial square wave signal, and the initial square wave signal is sent to one input terminal of the XOR gate after passing through the first stage of delay, and the other input terminal of the XOR gate is the initial square wave signal. The output of the OR gate is a pulse signal, the frequency of the pulse signal is twice that of the initial square wave signal, and the pulse width of the pulse signal is determined by the first delay unit; the pulse signal is ANDed with the initial square wave signal to obtain the sampling signal SELECT, and the sampling The signal SELECT has the same frequency as the original square wave signal, and the sampling signal SELECT arrives at the same time as the rising edge of the original square wave signal.

方波复位信号RESET电路输入端输入初始方波信号,初始方波信号经过第一延时单元、第二延时单元和第三延时单元产生方波复位信号RESET信号,方波复位信号RESET的上升沿与采样信号SELECT的下降沿的时间差第二延时单元和第三延时单元引起的延时。第一延时单元、第二延时单元和第三延时单元为相同单元或不同单元。The square wave reset signal RESET circuit input input the initial square wave signal, the initial square wave signal passes through the first delay unit, the second delay unit and the third delay unit to generate a square wave reset signal RESET signal, the square wave reset signal RESET The time difference between the rising edge and the falling edge of the sampling signal SELECT is the delay caused by the second delay unit and the third delay unit. The first delay unit, the second delay unit and the third delay unit are the same unit or different units.

具体地,图5是本发明电路的结构示意图,用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,包括信号产生电路、基于CTIA的光探测电路和两级反相器,信号产生电路用于产生一个尖脉冲式的采样信号SELECT电路和经过延迟的方波复位信号RESET电路。其中第一级反相器的翻转电压为VTHSpecifically, Fig. 5 is a structural schematic diagram of the circuit of the present invention, a capacitive transimpedance amplifier circuit with a pure digital output for weak light detection, including a signal generation circuit, a CTIA-based light detection circuit and a two-stage inverter, and the signal generation The circuit is used to generate a sharp pulse sampling signal SELECT circuit and a delayed square wave reset signal RESET circuit. The flipping voltage of the first-stage inverter is V TH .

图6是本发明强光下的时序图,图7是本发明弱光下的时序图,图8是本发明无光下的时序图。在T1时刻,复位信号RESET变为高,开关S0闭合,电容C0两端电压复位,均为VREF,此时S1处于断开状态,C1保持上个时刻的电压值,因而输出值VOUT在复位阶段将保持不变;在T2时刻,复位信号RESET由高电平变为低电平,复位开关S0断开,进入积分阶段,由于运放A1的虚短虚断特性,由PN结产生的光电流将通过C0积分,导致A1输出端电压VC0上升,此时由于开关S1断开,C1上的电压VC1仍然保持原值;在T3时刻,采样信号SELECT变为高电平,开关S1闭合,电容C0和C1发生电荷的重新分配,使得瞬间VC0和VC1相等,并等于介于原来二者之间的一个值;在T4时刻,采样信号SELECT变低,开关S1断开,由于复位信号RESET仍然为低,光电流继续对C0充电,因此VC0继续上升,而VC1则停止上升并保持T4时刻的值不变。到T5时刻,复位信号RESET变高,VC0又变为VREF,而VC1仍然保持。如果光生电流足够大,T4之前,VC1将大于A2的阈值电压VTH,使得输出VOUT为高电平,并保持整个周期。结构遵循I*T/2=Q=C*U,其中,I为由光电二极管产生的光电流的大小,其大小由光强和二极管的面积决定,T/2为积分时间,也就是半周期,Q是电容两端的电荷量变化,C为电容C0的容值,U为电容C0两端电压差的变化。当公式中的I为阈值光强产生的光电流时,U为VTH-VREF。C的大小与光探测器的灵敏度有密切的关系,U和T一定时,C越小,I越小,探测器越灵敏。通过调节积分电容的大小、PN结面积、VTH-VREF以及RESET方波信号的周期可以调节PN结产生的光电流的大小,使该结构得以对微弱临界光进行探测。Fig. 6 is a timing diagram of the present invention under strong light, Fig. 7 is a timing diagram of the present invention under weak light, and Fig. 8 is a timing diagram of the present invention under no light. At the time T1, the reset signal RESET becomes high, the switch S0 is closed, the voltage across the capacitor C0 is reset, both are V REF , at this time S1 is in the disconnected state, and C1 maintains the voltage value at the previous moment, so The output value V OUT will remain unchanged during the reset phase; at T 2 time, the reset signal RESET changes from high level to low level, the reset switch S 0 is turned off, and enters the integration phase. The photocurrent generated by the PN junction will be integrated through C 0 , causing the output voltage V C0 of A 1 to rise. At this time, because the switch S 1 is disconnected, the voltage V C1 on C 1 still maintains the original value; at T 3 At this moment, the sampling signal SELECT becomes high level, the switch S 1 is closed, and the charges of the capacitors C 0 and C 1 are redistributed, so that the instantaneous V C0 and V C1 are equal and equal to a value between the two; At T4 moment, the sampling signal SELECT becomes low, the switch S1 is turned off, since the reset signal RESET is still low, the photocurrent continues to charge C0 , so V C0 continues to rise, while V C1 stops rising and remains at T4 moment The value of is unchanged. At time T5, the reset signal RESET becomes high, V C0 becomes V REF again, and V C1 remains. If the photogenerated current is large enough, V C1 will be greater than the threshold voltage V TH of A 2 before T 4 , making the output V OUT a high level and maintaining the whole cycle. The structure follows I*T/2=Q=C*U, where I is the size of the photocurrent generated by the photodiode, which is determined by the light intensity and the area of the diode, and T/2 is the integration time, that is, the half cycle , Q is the change of the charge at both ends of the capacitor, C is the capacitance of the capacitor C 0 , and U is the change of the voltage difference between the two ends of the capacitor C 0 . When I in the formula is the photocurrent generated by the threshold light intensity, U is V TH -V REF . The size of C is closely related to the sensitivity of the photodetector. When U and T are constant, the smaller C is, the smaller I is, and the more sensitive the detector is. The size of the photocurrent generated by the PN junction can be adjusted by adjusting the size of the integrating capacitor, the area of the PN junction, V TH -V REF and the period of the RESET square wave signal, so that the structure can detect weak critical light.

如图9本发明的信号产生电路的结构示意图,采样信号SELECT输入为初始方波信号,初始方波信号经过第一级延时单元之后送给异或门的一个输入端,异或门另一个输入端则为该初始方波信号,异或门输出为一个频率为初始方波信号频率2倍的脉冲信号,脉冲宽度由延时单元决定。脉冲信号与初始方波信号作与运算,得到的便是具有和初始方波信号同频率的采样信号SELECT,采样信号SELECT与初始方波信号的上升沿同时到达;方波复位信号RESET电路为初始方波信号经过第一延时单元、第二延时单元、第三延时单元三级延时单元产生方波复位信号RESET,方波复位信号RESET的上升沿与采样信号SELECT的下降沿的时间差为两个延时单元引起的延时。如图10所示延时单元,起主要延时作用的元件为R和C,延时τ≈R*C,通过合理设置R与C的值,便可得到一定的延时时间。图9中示出的三级延时单元相同,但是在实际情况中,三级延时单元中的R和C值可以不同,通过合理调整各级延时单元的R和C的值,可以获得预设的尖脉冲宽度T4-T3以及尖脉冲下降沿与RESET信号上升沿之间的时间间距T5-T4As shown in Figure 9, the structural schematic diagram of the signal generating circuit of the present invention, the sampling signal SELECT input is an initial square wave signal, and the initial square wave signal is sent to one input end of the XOR gate after passing through the first stage delay unit, and the other side of the XOR gate The input end is the initial square wave signal, and the output of the XOR gate is a pulse signal whose frequency is twice the frequency of the initial square wave signal, and the pulse width is determined by the delay unit. The pulse signal and the initial square wave signal are ANDed, and the sampling signal SELECT with the same frequency as the initial square wave signal is obtained, and the sampling signal SELECT arrives at the same time as the rising edge of the initial square wave signal; the square wave reset signal RESET circuit is the initial The square wave signal passes through the first delay unit, the second delay unit, and the third delay unit to generate a square wave reset signal RESET, and the time difference between the rising edge of the square wave reset signal RESET and the falling edge of the sampling signal SELECT Delay caused by two delay units. As shown in the delay unit in Figure 10, the main delay elements are R and C, and the delay time τ≈R*C. By setting the values of R and C reasonably, a certain delay time can be obtained. The three-level delay units shown in Figure 9 are the same, but in actual situations, the R and C values in the three-level delay units can be different, and by reasonably adjusting the R and C values of the delay units at all levels, it can be obtained The preset spike width T 4 -T 3 and the time interval T 5 -T 4 between the falling edge of the spike pulse and the rising edge of the RESET signal.

在具体工作过程中,需要外界提供一个CLK时钟信号和VREF基准电压。在实际测试微弱临界光时,可以通过调节CLK信号的频率、VREF的大小来调节微弱临界光的阈值光强。CLK的频率应选取合适,太大的话会增加系统功耗,太小的话则会增大光探测器的响应时间。在设置好临界阈值光强后进行测试时,光强超过阈值光强会输出高电平,光强小于阈值光强则会输出低电平。In a specific working process, a CLK clock signal and a V REF reference voltage need to be provided from the outside. When actually testing the weak critical light, the threshold light intensity of the weak critical light can be adjusted by adjusting the frequency of the CLK signal and the size of V REF . The frequency of CLK should be selected properly, if it is too large, it will increase the power consumption of the system, if it is too small, it will increase the response time of the photodetector. When testing after setting the critical threshold light intensity, if the light intensity exceeds the threshold light intensity, it will output a high level, and if the light intensity is less than the threshold light intensity, it will output a low level.

以上对本发明的一个实例进行了详细说明,但所述内容仅为本发明的较佳实施例,不能被认为用于限定本发明的实施范围。凡依本发明申请范围所作的均等变化与改进等,均应仍归属于本发明的专利涵盖范围之内。An example of the present invention has been described in detail above, but the content described is only a preferred embodiment of the present invention and cannot be considered as limiting the implementation scope of the present invention. All equivalent changes and improvements made according to the application scope of the present invention shall still belong to the scope covered by the patent of the present invention.

Claims (2)

1.一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,其特征在于包括信号产生电路、基于CTIA的光探测电路和两级反相器,所述信号产生电路、所述基于CTIA的光探测电路和所述两级反相器依次连接,所述信号产生电路包括用于产生尖脉冲式的采样信号SELECT电路和方波复位信号RESET电路;1. A capacitive transimpedance amplifier circuit with pure digital output for faint light detection, characterized in that it comprises a signal generation circuit, a CTIA-based light detection circuit and a two-stage inverter, the signal generation circuit, the The CTIA-based photodetection circuit is sequentially connected to the two-stage inverter, and the signal generation circuit includes a sampling signal SELECT circuit and a square wave reset signal RESET circuit for generating sharp pulses; 所述采样信号SELECT电路的输入端输入初始方波信号,所述初始方波信号经过第一延时单元之后送给异或门的一个输入端,所述异或门另一个输入端则为所述初始方波信号,所述异或门输出为脉冲信号,所述脉冲信号的频率为所述初始方波信号的2倍,所述脉冲信号的脉冲宽度由所述第一延时单元决定;所述脉冲信号再与所述初始方波信号作与运算得到采样信号SELECT,所述采样信号SELECT具有和所述初始方波信号相同频率,所述采样信号SELECT与所述初始方波信号的上升沿同时到达;The input terminal of the sampling signal SELECT circuit inputs an initial square wave signal, and the initial square wave signal is sent to an input terminal of an exclusive OR gate after passing through the first delay unit, and the other input terminal of the exclusive OR gate is the input terminal of the exclusive OR gate. The initial square wave signal, the XOR gate output is a pulse signal, the frequency of the pulse signal is twice that of the initial square wave signal, and the pulse width of the pulse signal is determined by the first delay unit; The pulse signal is then ANDed with the initial square wave signal to obtain a sampling signal SELECT, the sampling signal SELECT has the same frequency as the initial square wave signal, and the rising of the sampling signal SELECT and the initial square wave signal arrive at the same time; 所述方波复位信号RESET电路输入端输入所述初始方波信号,所述初始方波信号经过第一延时单元、第二延时单元和第三延时单元产生方波复位信号RESET信号,所述方波复位信号RESET的上升沿与所述采样信号SELECT的下降沿的时间差为所述第二延时单元和所述第三延时单元引起的延时。The input terminal of the square wave reset signal RESET circuit inputs the initial square wave signal, and the initial square wave signal generates a square wave reset signal RESET signal through the first delay unit, the second delay unit and the third delay unit, The time difference between the rising edge of the square wave reset signal RESET and the falling edge of the sampling signal SELECT is the delay caused by the second delay unit and the third delay unit. 2.根据权利要求1所述的一种用于微弱光探测的带纯数字化输出的电容跨阻放大器电路,其特征在于所述第一延时单元、所述第二延时单元和所述第三延时单元为相同单元或不同单元。2. A capacitive transimpedance amplifier circuit with a pure digital output for weak light detection according to claim 1, characterized in that the first delay unit, the second delay unit and the first delay unit The three delay units are the same unit or different units.
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