CN104579640A - Real-time delay tracking device and method of quantum communication system - Google Patents
Real-time delay tracking device and method of quantum communication system Download PDFInfo
- Publication number
- CN104579640A CN104579640A CN201410837187.0A CN201410837187A CN104579640A CN 104579640 A CN104579640 A CN 104579640A CN 201410837187 A CN201410837187 A CN 201410837187A CN 104579640 A CN104579640 A CN 104579640A
- Authority
- CN
- China
- Prior art keywords
- delay
- control device
- time
- real
- tracking
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Landscapes
- Optical Communication System (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
量子通信系统的实时延时跟踪装置,包括控制装置、延时装置和单光子探测器,其中,控制装置用于控制延时装置产生一定步长的延时;延时装置用于产生延时,并将该延时作用于单光子探测器的时钟,使得由时钟延时产生的门脉冲触发单光子探测器对入射单光子信号进行探测;单光子探测器用于将探测到的单光子信号计数反馈到控制装置中;控制装置将预定时间内的所述计数累积值Y与预先存储的所述预定时间内的单光子信号的计数累积值X进行比较,根据比较结果寻找正确的延时方向,进行下一步的延时跟踪。
The real-time delay tracking device of the quantum communication system includes a control device, a delay device and a single photon detector, wherein the control device is used to control the delay device to generate a certain step-length delay; the delay device is used to generate a delay, And the delay is applied to the clock of the single photon detector, so that the gate pulse generated by the clock delay triggers the single photon detector to detect the incident single photon signal; the single photon detector is used to count and feed back the detected single photon signal In the control device; the control device compares the count accumulation value Y within the predetermined time with the pre-stored count accumulation value X of the single photon signal within the predetermined time, and finds the correct delay direction according to the comparison result, and performs Time-lapse tracking for the next step.
Description
技术领域technical field
本发明涉及量子保密通信,具体而言是在量子保密通信系统中,针对单光子探测器中时钟和信号存在的延迟漂移问题,用一种“短步长、长积分”的实时延迟跟踪方法扫描定位最佳延时点,从而保证单光子探测器获得最大的计数,确保量子密钥成码率。The invention relates to quantum secure communication, specifically, in a quantum secure communication system, aiming at the problem of delay drift in the clock and signal in a single photon detector, a real-time delay tracking method of "short step size and long integration" is used to scan Locate the best delay point, so as to ensure the maximum count of the single photon detector and ensure the coding rate of the quantum key.
背景技术Background technique
量子保密通信是近三十多年来迅速发展起来的一个热门研究领域,是目前公认的能够实现无条件安全的通信方式。量子密钥分发技术自从1984年由Bennett.C.H和G.Brassard提出以后,得到了科学界的广泛关注。如今许多国家都看好量子保密通信的前景,欧美等发达国家已经开始了高速量子通信和大规模保密通信网络的探索,我国也将其列为重点科研项目进行研究。Quantum secure communication is a hot research field that has developed rapidly in the past 30 years, and it is currently recognized as a communication method that can achieve unconditional security. Since the quantum key distribution technology was proposed by Bennett.C.H and G.Brassard in 1984, it has received extensive attention from the scientific community. Nowadays, many countries are optimistic about the prospects of quantum secure communication. Developed countries such as Europe and the United States have begun to explore high-speed quantum communication and large-scale secure communication networks. my country has also listed it as a key scientific research project for research.
量子保密通信系统的实施方案有很多种,包括偏振、相位、纠缠态方案等。在量子密钥分发过程中,信息被加载到单光子上,利用其量子特性实现信息的传递,并通过后期的基比对等操作筛选出密码。在整个密钥产生的过程中,一个重要的环节就是对单光子的检测,因为单光子的能量极低,仅为10-19J量级,因此在实用化的量子通信系统中需要使用超灵敏的单光子探测设备进行检测,而且单光子探测器的性能好坏直接决定了量子通信系统中成码率和误码率等核心参数的优劣。There are many implementation schemes for quantum secure communication systems, including polarization, phase, and entanglement schemes. In the quantum key distribution process, information is loaded onto a single photon, and its quantum properties are used to realize the transmission of information, and the password is screened out through the later base-by-peer operation. In the entire key generation process, an important link is the detection of single photons, because the energy of single photons is extremely low, only on the order of 10-19J, so it is necessary to use ultra-sensitive photons in practical quantum communication systems. Single-photon detection equipment is used for detection, and the performance of single-photon detectors directly determines the quality of core parameters such as coding rate and bit error rate in quantum communication systems.
就目前而言,量子通信系统中最常用到的单光子探测器件为基于InGaAs的雪崩光电二极管(APD)。当其工作在“盖革模式”下时,只有当探测门脉冲出现的时间段内,APD才进入雪崩模式,实现对单光子的探测;而在没有门脉冲时,APD工作在线性区内,不发生雪崩。这种模式可以有效的使APD淬灭,并且提升了探测器的信噪比。For now, the most commonly used single-photon detection devices in quantum communication systems are InGaAs-based avalanche photodiodes (APDs). When it works in the "Geiger mode", only when the detection gate pulse appears, the APD enters the avalanche mode to realize the detection of single photons; when there is no gate pulse, the APD works in the linear region, No avalanche occurs. This mode can effectively quench the APD and improve the signal-to-noise ratio of the detector.
基于这种工作模式,单光子探测器只在门脉冲的时间内响应入射光子,因此在进行系统设计时,必须确保门脉冲和单光子脉重合,才可获得最佳的探测效率和成码率。但是在实际情况下,门脉冲和单光子脉冲往往由不同的信道提供,由于环境温度、机械振动等原因导致的光纤长度和折射率的变化,都会引起门脉冲和单光子脉冲的相对延迟发生漂移,这种漂移将直接导致计数率的下降(从而导致成码率下降),甚至使密钥分发过程失败。Based on this working mode, the single-photon detector only responds to the incident photon within the time of the gate pulse. Therefore, when designing the system, it is necessary to ensure that the gate pulse and the single-photon pulse coincide to obtain the best detection efficiency and coding rate. . However, in practical situations, gate pulses and single-photon pulses are often provided by different channels, and changes in fiber length and refractive index due to environmental temperature, mechanical vibration, etc., will cause the relative delay of gate pulses and single-photon pulses to drift. , this drift will directly lead to a decrease in the counting rate (thereby causing a decrease in the coding rate), and even cause the key distribution process to fail.
目前,解决这一问题的常用方案是中断通信,对门脉冲和单光子脉冲的相对延时重新进行扫描,以找到最佳的延时点。此方案弊端在于通信会被中断,降低系统的工作效率。本发明提出了一种新的寻找最佳延时点的方案,克服了前述方案的缺点。At present, the common solution to this problem is to interrupt the communication and re-scan the relative delay of the gate pulse and the single photon pulse to find the best delay point. The disadvantage of this solution is that the communication will be interrupted and the working efficiency of the system will be reduced. The present invention proposes a new scheme for finding the best delay point, which overcomes the disadvantages of the foregoing schemes.
发明内容Contents of the invention
本发明的目的是:提出实时延时跟踪装置和方法,其能够实现不用中断通信即可实时找到最佳延时点。The object of the present invention is to provide a real-time delay tracking device and method, which can realize the optimal delay point in real time without interrupting communication.
本发明建立了一套在量子密钥分发中实时控制单光子探测器门脉冲延时的方案,利用环境变化通常为慢变过程的特点,对扫描过程采用“短步长,长积分”的方案,可以在不中断通信的条件下对探测器门脉冲的延时进行扫描,寻找出最佳延时点,这种方式不仅可以使单光子探测器的计数值始终保持在较高的水平,并且具有实时跟踪的特点。The present invention establishes a set of schemes for real-time control of single-photon detector gate pulse delay in quantum key distribution, utilizes the characteristics that environmental changes are usually slow-changing processes, and adopts a scheme of "short step length, long integration" for the scanning process , the delay of the detector gate pulse can be scanned without interrupting the communication to find the best delay point. This method can not only keep the count value of the single photon detector at a high level, but also It has the characteristics of real-time tracking.
本发明目的实现由以下技术方案完成:The object of the present invention is realized by the following technical solutions:
在量子保密通信探测模块中,利用FPGA控制延时芯片对单光子探测器门脉冲的相位延时进行“短步长”的扫描。因每一步延时改变很小,探测计数值的变化控制在很小的范围内,对通信成码影响十分微小。同时,由于单光子探测器的探测效率有一定范围的波动,加上“短步长”的延时改变不易区分出探测计数的变化,因此本发明中还采用了“长积分”的计数方法,将较长时间内的光子计数值累积保存于FPGA中,用做反馈判断。长时间的累积计数能有效减小噪声抖动带来的误差,准确的区分出延时改变前后计数大小的改变。FPGA对前后两次数据进行比较,按照相应的算法判断延迟调节的方向,从而实现对最大计数值的实时跟踪。In the quantum secure communication detection module, the phase delay of the gate pulse of the single photon detector is scanned in a "short step" by using the FPGA to control the delay chip. Because the change of the delay in each step is very small, the change of the detection count value is controlled in a small range, and the influence on the communication coding is very small. Simultaneously, since the detection efficiency of the single photon detector fluctuates within a certain range, and it is difficult to distinguish the change of the detection count due to the delay change of the "short step size", the counting method of "long integral" is also adopted in the present invention, The photon count value accumulated and stored in the FPGA for a long period of time is used for feedback judgment. Long-term cumulative counting can effectively reduce the error caused by noise and jitter, and accurately distinguish the change in counting size before and after the delay change. FPGA compares the two data before and after, and judges the direction of delay adjustment according to the corresponding algorithm, so as to realize the real-time tracking of the maximum count value.
一种量子通信系统的实时延时跟踪装置,包括控制装置、延时装置和单光子探测器,其中,A real-time delay tracking device for a quantum communication system, including a control device, a delay device and a single photon detector, wherein,
控制装置用于控制延时装置产生一定步长的延时;The control device is used to control the delay device to generate a certain step-length delay;
延时装置用于产生延时,并将该延时作用于单光子探测器的时钟,使得由时钟延时产生的门脉冲触发单光子探测器对入射单光子信号进行探测;The delay device is used to generate a delay, and the delay is applied to the clock of the single photon detector, so that the gate pulse generated by the clock delay triggers the single photon detector to detect the incident single photon signal;
单光子探测器用于将探测到的单光子信号计数反馈到控制装置中;The single photon detector is used to count and feed back the detected single photon signal to the control device;
控制装置将预定时间内的所述计数累积值Y与预先存储的所述预定时间内的单光子信号的计数累积值X进行比较,根据比较结果寻找正确的延时方向,进行下一步的延时跟踪。The control device compares the count accumulation value Y within the predetermined time with the pre-stored count accumulation value X of the single photon signal within the predetermined time, finds the correct delay direction according to the comparison result, and performs the next delay track.
如上所述的实时延时跟踪装置,其特征在于:The above-mentioned real-time delay tracking device is characterized in that:
控制装置首先把预定时间内的单光子信号计数累积后存入变量X中,然后控制延时装置产生一定步长的延时,并把之后单光子探测器在所述预定时间内探测到的单光子信号计数累积后存入变量Y中;The control device first accumulates the single-photon signal counts within a predetermined time and stores them in the variable X, and then controls the delay device to generate a delay of a certain step length, and then stores the single-photon signal detected by the single-photon detector within the predetermined time. The photon signal counts are accumulated and stored in the variable Y;
控制装置对X和Y进行比较,如果Y>X,重复前面的延时过程继续进行延时跟踪;如果Y<X,将延时方向调转,进行反方向的延时跟踪。The control device compares X and Y, and if Y>X, repeats the previous delay process to continue delay tracking; if Y<X, reverses the delay direction and performs reverse delay tracking.
如上所述的实时延时跟踪装置,其特征在于:The above-mentioned real-time delay tracking device is characterized in that:
所述控制装置是FPGA。The control device is FPGA.
如上所述的实时延时跟踪装置,其特征在于:The above-mentioned real-time delay tracking device is characterized in that:
所述延时装置是延时芯片。The delay device is a delay chip.
如上所述的实时延时跟踪装置,其特征在于:The above-mentioned real-time delay tracking device is characterized in that:
控制装置产生的延时可为正向或反向。The time delay generated by the control device can be forward or reverse.
一种量子通信系统的实时延时跟踪方法,其特征在于包括如下步骤:A real-time delay tracking method for a quantum communication system, characterized in that it comprises the following steps:
控制装置预先存储单光子探测器在预定时间内探测到的入射单光子信号计数累积值X;The control device pre-stores the cumulative value X of counting incident single-photon signals detected by the single-photon detector within a predetermined time;
控制装置控制延时装置产生一定步长的延时;The control device controls the delay device to generate a certain step-length delay;
延时装置产生延时,并将该延时作用于单光子探测器的时钟,使得由时钟延时产生的门脉冲触发单光子探测器对入射单光子信号进行探测;The delay device generates a time delay, and applies the time delay to the clock of the single-photon detector, so that the gate pulse generated by the clock delay triggers the single-photon detector to detect the incident single-photon signal;
单光子探测器将探测到的单光子信号计数反馈到控制装置中;The single photon detector counts the detected single photon signal and feeds it back to the control device;
控制装置将预定时间内的所述计数累积值Y与预先存储的所述计数累积值X进行比较,根据比较结果寻找正确的延时方向,进行下一步的延时跟踪。The control device compares the count accumulation value Y within a predetermined time with the pre-stored count accumulation value X, finds the correct delay direction according to the comparison result, and performs the next delay tracking.
如上所述的实时延时跟踪方法,其特征在于:The real-time delay tracking method as described above is characterized in that:
控制装置首先把预定时间内的单光子信号计数累积后存入变量X中,然后控制延时装置产生一定步长的延时,并把之后单光子探测器在所述预定时间内探测到的单光子信号计数累积后存入变量Y中;The control device first accumulates the single-photon signal counts within a predetermined time and stores them in the variable X, and then controls the delay device to generate a delay of a certain step length, and then stores the single-photon signal detected by the single-photon detector within the predetermined time. The photon signal counts are accumulated and stored in the variable Y;
控制装置对X和Y进行比较,如果Y>X,重复前面的延时过程继续进行延时跟踪;如果Y<X,将延时方向调转,进行反方向的延时跟踪。The control device compares X and Y, and if Y>X, repeats the previous delay process to continue delay tracking; if Y<X, reverses the delay direction and performs reverse delay tracking.
如上所述的实时延时跟踪方法,其特征在于:The real-time delay tracking method as described above is characterized in that:
所述控制装置是FPGA。The control device is FPGA.
如上所述的实时延时跟踪方法,其特征在于:The real-time delay tracking method as described above is characterized in that:
所述延时装置是延时芯片。The delay device is a delay chip.
如上所述的实时延时跟踪方法,其特征在于:控制装置产生的延时可为正向或反向。The above-mentioned real-time delay tracking method is characterized in that the delay generated by the control device can be forward or reverse.
附图说明Description of drawings
图1为本发明量子通信系统的实时延时跟踪装置示意图;Fig. 1 is the schematic diagram of the real-time delay tracking device of the quantum communication system of the present invention;
图2为本发明量子通信系统的实时延时跟踪方法示意图。Fig. 2 is a schematic diagram of the real-time delay tracking method of the quantum communication system of the present invention.
具体实施方式Detailed ways
以下结合附图通过实施例对本发明特征及其它相关特征作进一步详细说明。The features of the present invention and other related features will be further described in detail below through embodiments in conjunction with the accompanying drawings.
如图1所示,实时延时跟踪装置由FPGA、延时芯片和单光子探测器构成。FPGA可以控制延时芯片产生正反向一定步长的延时(延时的选择需考虑探测器门脉冲的宽度,太宽会导致光子计数急剧减小,太窄会导致区分度不够,结合到本系统中,门脉冲宽度1ns,所以选取了0.01ns),延时作用于时钟后产生的门脉冲触发单光子探测器对入射单光子信号进行探测,单光子探测器将探测计数反馈到FPGA中,FPGA将较长时间内的计数累积后进行比较,寻找正确的延时方向,进行下一步的延时跟踪。As shown in Figure 1, the real-time delay tracking device is composed of FPGA, delay chip and single photon detector. The FPGA can control the delay chip to generate a certain step-length delay in forward and reverse directions (the choice of delay should consider the width of the detector gate pulse, too wide will cause the photon count to decrease sharply, and too narrow will lead to insufficient discrimination, combined with In this system, the gate pulse width is 1ns, so 0.01ns is selected), and the gate pulse generated after the delay acts on the clock triggers the single photon detector to detect the incident single photon signal, and the single photon detector feeds back the detection count to the FPGA , the FPGA will accumulate the counts in a long period of time and then compare them to find the correct delay direction and carry out the next delay tracking.
图2是实时延时跟踪装置的工作流程图,具体如下:Fig. 2 is the working flowchart of real-time delay tracking device, specifically as follows:
当外部产生一个实时延时跟踪请求输入FPGA,整个系统开始工作。FPGA首先把一定时间(积分时间的选择需考虑延时漂移的速度,以及探测器本身的探测效率抖动范围,结合到本系统,选择3分钟的积分时间)内的光子计数累积后存入变量X中,然后将延时方向向后延0.01ns,并计下之后3分钟内的光子计数存入变量Y中,FPGA片内对X和Y进行比较,如果Y>X,说明最大探测计数点在此时的延时方向以后,当前采用的延时方向是正确的,重复前面的延时过程向后继续延时即可逼近最佳的延时点;一旦发现Y<X,说明最大探测计数点在原先延时方向的反向,当前采用的延时方向是错误,因此将延时方向调转,并延时0.01ns。When an external real-time delay tracking request is input into FPGA, the whole system starts to work. FPGA first accumulates the photon counts within a certain period of time (the selection of the integration time needs to consider the speed of delay drift, and the detection efficiency jitter range of the detector itself, combined with this system, and the integration time of 3 minutes is selected) and then stored in the variable X , and then delay the delay direction by 0.01ns, and count the photon count within 3 minutes and store it in the variable Y, and compare X and Y in the FPGA chip. If Y>X, it means that the maximum detection count point is at After the delay direction at this time, the current delay direction is correct. Repeat the previous delay process and continue to delay backward to approach the best delay point; once Y<X is found, it means the maximum detection count point In the reverse direction of the original delay direction, the current delay direction is wrong, so reverse the delay direction and delay by 0.01ns.
最佳延时点是一个理论值,即时钟和信号相对偏差为0的点,在这个点上探测器可以获得一个最大的计数。但是由于时钟和信号的相对时间漂移是一个动态过程,本发明实现的功能是通过对不等式的判断,使时钟和信号的相对偏差不断变小,直至趋近最小偏差值(即最佳值),最后的结果是,偏差值会在0点(即最佳值)附近振荡。The optimal delay point is a theoretical value, that is, the point at which the relative deviation between the clock and the signal is 0, and the detector can obtain a maximum count at this point. But because the relative time drift of the clock and the signal is a dynamic process, the function realized by the present invention is to make the relative deviation of the clock and the signal continuously decrease until approaching the minimum deviation value (i.e. the optimum value) by judging the inequality. The final result is that the deviation value will oscillate around 0 point (ie the optimal value).
因最佳延时点是实时变化的,所以在整个跟踪过程需要不断的进行延时调整,最终探测器的门脉冲延时将在实际的最佳延时点附近左右震荡,并在最佳延时点发生漂移时进行跟踪,从而实现单光子探测器始终保持良好的探测计数率,确保量子密钥分发过程的成码稳定性。Because the optimal delay point changes in real time, it is necessary to continuously adjust the delay during the whole tracking process. Finally, the gate pulse delay of the detector will oscillate around the actual optimal delay point, and at the optimal delay point Tracking is carried out when the time point drifts, so that the single photon detector can always maintain a good detection count rate and ensure the coding stability of the quantum key distribution process.
Claims (10)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201410837187.0A CN104579640A (en) | 2014-12-24 | 2014-12-24 | Real-time delay tracking device and method of quantum communication system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201410837187.0A CN104579640A (en) | 2014-12-24 | 2014-12-24 | Real-time delay tracking device and method of quantum communication system |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN104579640A true CN104579640A (en) | 2015-04-29 |
Family
ID=53094927
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201410837187.0A Pending CN104579640A (en) | 2014-12-24 | 2014-12-24 | Real-time delay tracking device and method of quantum communication system |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN104579640A (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105049202A (en) * | 2015-08-19 | 2015-11-11 | 安徽问天量子科技股份有限公司 | Method and device for dynamically adjusting defector drift in quantum key distribution system |
| JP2017157998A (en) * | 2016-03-01 | 2017-09-07 | 沖電気工業株式会社 | Quantum key delivery system and time synchronization method |
| CN108827477A (en) * | 2018-06-27 | 2018-11-16 | 中国人民解放军战略支援部队信息工程大学 | A kind of single-photon detector detection efficient self-checking device and method |
| CN109617685A (en) * | 2018-12-28 | 2019-04-12 | 北京中创为南京量子通信技术有限公司 | A kind of high speed bit synchronization method and device generating system for quantum key |
| CN111510284A (en) * | 2019-01-31 | 2020-08-07 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111510208A (en) * | 2019-01-31 | 2020-08-07 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111896096A (en) * | 2020-06-30 | 2020-11-06 | 太原理工大学 | A device for precise measurement of mechanical vibrations using a photon counter |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20030169880A1 (en) * | 2002-02-22 | 2003-09-11 | Nec Corporation | Quantum cryptography key distribution system and method |
| US20070133799A1 (en) * | 2003-11-12 | 2007-06-14 | Magiq Technologies, Inc | Detector autocalibration in qkd systems |
| US20080144823A1 (en) * | 2004-07-12 | 2008-06-19 | Mitsubishi Denki Kabushiki Kaisha | Photon Detecting Device and Optical Communication System |
| CN101558590A (en) * | 2005-04-20 | 2009-10-14 | Magiq技术公司 | QKD system detector autocalibration based on bit-error rate |
-
2014
- 2014-12-24 CN CN201410837187.0A patent/CN104579640A/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20030169880A1 (en) * | 2002-02-22 | 2003-09-11 | Nec Corporation | Quantum cryptography key distribution system and method |
| US20070133799A1 (en) * | 2003-11-12 | 2007-06-14 | Magiq Technologies, Inc | Detector autocalibration in qkd systems |
| US20080144823A1 (en) * | 2004-07-12 | 2008-06-19 | Mitsubishi Denki Kabushiki Kaisha | Photon Detecting Device and Optical Communication System |
| CN101558590A (en) * | 2005-04-20 | 2009-10-14 | Magiq技术公司 | QKD system detector autocalibration based on bit-error rate |
Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105049202A (en) * | 2015-08-19 | 2015-11-11 | 安徽问天量子科技股份有限公司 | Method and device for dynamically adjusting defector drift in quantum key distribution system |
| CN105049202B (en) * | 2015-08-19 | 2018-05-22 | 安徽问天量子科技股份有限公司 | The method and device of dynamic adjustment detector drift in quantum key dispatching system |
| JP2017157998A (en) * | 2016-03-01 | 2017-09-07 | 沖電気工業株式会社 | Quantum key delivery system and time synchronization method |
| CN108827477A (en) * | 2018-06-27 | 2018-11-16 | 中国人民解放军战略支援部队信息工程大学 | A kind of single-photon detector detection efficient self-checking device and method |
| CN109617685A (en) * | 2018-12-28 | 2019-04-12 | 北京中创为南京量子通信技术有限公司 | A kind of high speed bit synchronization method and device generating system for quantum key |
| CN111510284A (en) * | 2019-01-31 | 2020-08-07 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111510208A (en) * | 2019-01-31 | 2020-08-07 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111510208B (en) * | 2019-01-31 | 2021-04-23 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111510284B (en) * | 2019-01-31 | 2021-07-02 | 北京中创为南京量子通信技术有限公司 | Real-time bit synchronization correction method for quantum key generation system |
| CN111896096A (en) * | 2020-06-30 | 2020-11-06 | 太原理工大学 | A device for precise measurement of mechanical vibrations using a photon counter |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN104579640A (en) | Real-time delay tracking device and method of quantum communication system | |
| CN103148950B (en) | Integrated gating active quenching/restoring circuit | |
| Kosaka et al. | Single-photon interference experiment over 100 km for quantum cryptography system using balanced gated-mode photon detector | |
| US10132921B2 (en) | Light communications receiver and decoder with time to digital converters | |
| KR101740263B1 (en) | Single photon detector in the near infrared using an InGaAs/InP avalanche photodiode operated with a bipolar rectangular gating signal. | |
| US8949300B2 (en) | Circuit and method for controlling quality of random numbers | |
| JP5751649B2 (en) | Apparatus and method for detecting attacks attempting to control a single photon detector of a quantum cryptography device by randomly changing the efficiency | |
| CN103759840B (en) | A kind of semiconductor infrared single-photon detector avalanche signal screening device and method | |
| Walenta et al. | Sine gating detector with simple filtering for low-noise infra-red single photon detection at room temperature | |
| JP7160027B2 (en) | Single-photon detector timing adjustment method, device, and program in quantum key distribution system | |
| Huang et al. | Real-time and high-speed underwater photon-counting communication based on SPAD and PPM symbol synchronization | |
| KR101685494B1 (en) | Apparatus for Detecting Single Photon and Method for the same | |
| CN109443555A (en) | Based on the single-photon detection system that active restoring circuit is actively quenched | |
| CN204886965U (en) | Wireless Optical Communication System Based on Photon Counting | |
| CN116961775A (en) | Signal processing method, signal processing device and quantum communication receiving end | |
| WO2021031667A1 (en) | Single-photon detection apparatus and method | |
| JP2007147472A (en) | Data processing method and apparatus for characteristics measurement of photon detection device and photon receiver using it | |
| KR102368114B1 (en) | Avalanche Photodiode that can Operate as One of Single Photon Detection Devices Operating in Two Different Modes | |
| CN110726483B (en) | Device and method for resisting avalanche transition region attack | |
| Lee et al. | The impact of spot‐size on single‐photon avalanche diode timing‐jitter and quantum key distribution | |
| KR101966652B1 (en) | Method and Apparatus for Detecting Single Photon by Reverse Counting | |
| KR20220158962A (en) | Method for Aligning the Avalanche Photodiode to an Optimal Position for Detecting Photons | |
| CN107147441B (en) | Signal detection method and device | |
| Jin et al. | The influence of stochastic dispersion on quantum key distribution system | |
| CN222321554U (en) | Quantum key distribution system and gated detector dead time defense circuit |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| RJ01 | Rejection of invention patent application after publication |
Application publication date: 20150429 |
|
| RJ01 | Rejection of invention patent application after publication |