CN110161522A - A kind of Gao Zhongying single-photon laser radar for eliminating range ambiguity - Google Patents
A kind of Gao Zhongying single-photon laser radar for eliminating range ambiguity Download PDFInfo
- Publication number
- CN110161522A CN110161522A CN201910501221.XA CN201910501221A CN110161522A CN 110161522 A CN110161522 A CN 110161522A CN 201910501221 A CN201910501221 A CN 201910501221A CN 110161522 A CN110161522 A CN 110161522A
- Authority
- CN
- China
- Prior art keywords
- laser
- pulse
- time
- photon
- signal
- 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.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 claims abstract description 19
- 238000009825 accumulation Methods 0.000 claims abstract description 14
- 238000001161 time-correlated single photon counting Methods 0.000 claims abstract description 8
- 238000005259 measurement Methods 0.000 claims description 16
- 230000000875 corresponding effect Effects 0.000 claims description 5
- 238000002592 echocardiography Methods 0.000 claims description 4
- 230000001276 controlling effect Effects 0.000 claims 2
- 210000001367 artery Anatomy 0.000 claims 1
- 238000004080 punching Methods 0.000 claims 1
- 230000002123 temporal effect Effects 0.000 claims 1
- 210000003462 vein Anatomy 0.000 claims 1
- 238000000034 method Methods 0.000 description 9
- 230000035508 accumulation Effects 0.000 description 6
- 238000001514 detection method Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000035945 sensitivity Effects 0.000 description 3
- 230000002596 correlated effect Effects 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000001960 triggered effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
- G01S17/02—Systems using the reflection of electromagnetic waves other than radio waves
- G01S17/06—Systems determining position data of a target
- G01S17/08—Systems determining position data of a target for measuring distance only
- G01S17/10—Systems determining position data of a target for measuring distance only using transmission of interrupted, pulse-modulated waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
- G01S7/483—Details of pulse systems
- G01S7/486—Receivers
- G01S7/487—Extracting wanted echo signals, e.g. pulse detection
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02A—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
- Y02A90/00—Technologies having an indirect contribution to adaptation to climate change
- Y02A90/10—Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Computer Networks & Wireless Communication (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Electromagnetism (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Abstract
本发明公开了一种可消除距离模糊的高重频单光子激光雷达,包括控制模块、激光器、分束器、发射光学系统、光电二极管、事件计时器、接收光学系统、单光子探测器、信号处理模块。利用控制模块产生重复频率可调的脉冲信号,将其作为激光器的主控信号,用于控制激光脉冲的发射时刻。利用事件计时器分别记录参考光脉冲和回波光脉冲时刻,并由信号处理模块进行时间相关单光子计数处理,由于激光脉冲频率不断变化,使得累积过程中只有本次触发时刻的回波光脉冲才能累积起来,非本次触发时刻的回波光脉冲被离散化处理,最终使得单光子激光雷达能够在高重频条件下消除距离模糊问题。
The invention discloses a high-repetition-frequency single-photon laser radar capable of eliminating distance ambiguity, comprising a control module, a laser, a beam splitter, an emission optical system, a photodiode, an event timer, a receiving optical system, a single-photon detector, a signal processing module. The control module is used to generate a pulse signal with adjustable repetition frequency, which is used as the main control signal of the laser to control the emission time of the laser pulse. The event timer is used to record the reference light pulse and echo light pulse time respectively, and the signal processing module performs time-correlated single-photon counting processing. Due to the constant change of the laser pulse frequency, only the echo light pulse at this trigger time can be accumulated during the accumulation process. Finally, the echo light pulses not at the current trigger time are discretized, which finally enables the single-photon lidar to eliminate the distance ambiguity problem under the condition of high repetition frequency.
Description
技术领域technical field
本发明属于激光雷达技术领域,特别涉及一种可消除距离模糊的高重频单光子激光雷达。The invention belongs to the technical field of laser radar, and in particular relates to a high-repetition-frequency single-photon laser radar capable of eliminating distance ambiguity.
背景技术Background technique
单光子激光雷达利用单光子探测器接收光子量级回波信号,通过时间相关单光子计数(Time-Correlated Single Photon Counting,TCSPC)技术将时间飞行测距的光信号探测灵敏度提高到量子极限,极大地提高了激光雷达的作用距离。单光子激光雷达虽然具有很高的探测灵敏度,但是其采用的TCSPC技术需要进行多次累积来提取目标的距离信息。在重复频率一定的条件下,增加累积次数会造成了测距时间过长,无法适用运动目标的激光测距场合。因此,提高激光脉冲的重复频率是提高单光子激光雷达数据更新率的有效途径。Single-photon LiDAR uses a single-photon detector to receive photon-level echo signals, and uses Time-Correlated Single Photon Counting (TCSPC) technology to improve the optical signal detection sensitivity of time-of-flight ranging to the quantum limit. Greatly improves the range of lidar. Although the single-photon lidar has high detection sensitivity, the TCSPC technology it adopts requires multiple accumulations to extract the distance information of the target. Under the condition of a certain repetition frequency, increasing the accumulation times will cause the ranging time to be too long, and it cannot be applied to the laser ranging of moving targets. Therefore, increasing the repetition frequency of laser pulses is an effective way to improve the data update rate of single-photon lidar.
然而,重复频率的提高会造成缩短最大不模糊距离,限制了单光子激光雷达在远距离目标测距中的应用。为了解决激光脉冲重频与最大不模糊距离之间的矛盾,目前大体存在以下方法:其中一种是基于相关运算的伪随机编码技术,该方法将激光发射的长脉冲进行编码,通过将探测器接收到的回波脉冲跟发射脉冲进行相关运算提取出回波脉冲中目标信号,从而实现远距离的运动目标探测,同时通过对各个脉冲施加不同的编码方式,能够有效解决了高重频条件下的距离模糊问题。然而,这种方法存在的问题是单光子探测器的死时间会降低发射脉冲与回波脉冲之间的相关性,进而降低回波探测的灵敏度。另外一种方法是双频或多频调制技术,即利用两种或者固定频率(对应的周期分别为T1、T2、…、Tn)对激光脉冲进行调制,则其可探测的最大不模糊距离为dmax=c[T1、T2、…、Tn]/2,这里的[T1、T2、…、Tn]为T1、T2、…、Tn的最小公倍数。然而,当相邻两个回波信号的时间间隔很短(小于单光子探测器的死时间)时,单光子探测器的死时间会影响回波回波信号的探测概率。However, the increase of repetition rate will shorten the maximum unambiguous distance, which limits the application of single-photon lidar in long-distance target ranging. In order to solve the contradiction between the laser pulse repetition frequency and the maximum unambiguous distance, there are generally the following methods: one of them is the pseudo-random coding technology based on correlation operation, which encodes the long pulse emitted by the laser, The received echo pulse is correlated with the transmitted pulse to extract the target signal in the echo pulse, so as to realize long-distance moving target detection. At the same time, by applying different coding methods to each pulse, it can effectively solve the problem of high repetition frequency distance blur problem. However, the problem with this method is that the dead time of the single-photon detector reduces the correlation between the transmitted pulse and the echo pulse, which in turn reduces the sensitivity of echo detection. Another method is dual-frequency or multi-frequency modulation technology, that is, using two or fixed frequencies (corresponding periods are T 1 , T 2 , ..., T n ) to modulate the laser pulse, the maximum detectable frequency is The fuzzy distance is d max =c[T 1 , T 2 ,..., T n ]/2, where [T 1 , T 2 ,..., T n ] is the least common multiple of T 1 , T 2 ,..., T n . However, when the time interval between two adjacent echo signals is very short (less than the dead time of the single photon detector), the dead time of the single photon detector will affect the detection probability of the echo signals.
发明内容SUMMARY OF THE INVENTION
为了克服现有技术的缺点和不足,本发明提出了一种可消除距离模糊的高重频单光子激光雷达,能够以较高的重复频率实现远距离的运动目标探测。In order to overcome the shortcomings and deficiencies of the prior art, the present invention proposes a high-repetition-frequency single-photon laser radar capable of eliminating distance ambiguity, which can realize long-distance moving target detection with a high repetition frequency.
为了实现上述目的,本发明采用的技术方案为:一种可消除距离模糊的高重频单光子激光雷达,该激光雷达包括控制模块、激光器、分束器、发射光学系统、光电二极管、第一事件计时器、接收光学系统、单光子探测器、第二事件计时器以及信号处理模块,其中:In order to achieve the above purpose, the technical solution adopted in the present invention is: a high-repetition-frequency single-photon laser radar that can eliminate distance ambiguity, the laser radar includes a control module, a laser, a beam splitter, an emission optical system, a photodiode, a first An event timer, a receiving optical system, a single photon detector, a second event timer, and a signal processing module, wherein:
所述的控制模块用于产生重复频率可调的触发脉冲信号,将其作为激光器的主控信号,用于控制激光脉冲的发射时刻;The control module is used to generate a trigger pulse signal with adjustable repetition frequency, which is used as the main control signal of the laser to control the emission time of the laser pulse;
所述的激光器用于产生激光脉冲信号,脉冲频率由控制模块控制;The laser is used to generate laser pulse signals, and the pulse frequency is controlled by the control module;
所述的分束器将激光器发射的激光信号一分为二,其中的大部分激光传输至发射光学系统作为信号光,而小部分激光传输至光电二极管作为参考光;The beam splitter divides the laser signal emitted by the laser into two parts, most of the laser light is transmitted to the emission optical system as signal light, and a small part of the laser light is transmitted to the photodiode as reference light;
所述的发射光学系统用于对信号光进行准直和扩束并发射至被测目标上;The transmitting optical system is used for collimating and beam expanding the signal light and transmitting it to the measured target;
所述的光电二极管用于探测分束器分出的参考光,以此作为计时基准信号;The photodiode is used to detect the reference light separated by the beam splitter, and use it as a timing reference signal;
所述的第一事件计时器用于精确记录参考光脉冲的时刻,以此作为脉冲飞行时间测量的起点;The first event timer is used to accurately record the time of the reference light pulse, which is used as the starting point for measuring the time of flight of the pulse;
所述的接收光学系统用于接收被测目标反射/散射的激光回波信号;The receiving optical system is used for receiving the laser echo signal reflected/scattered by the measured target;
所述的单光子探测器用于响应光子量级的微弱回波光脉冲信号;The single-photon detector is used to respond to a weak echo light pulse signal of the photon level;
所述的第二事件计时器用于精确记录回波光脉冲的时刻,以此作为脉冲飞行时间测量的终点;The second event timer is used to accurately record the time of the echo light pulse as the end point of the pulse flight time measurement;
所述的信号处理模块用于进行时间相关单光子计数处理,从而获得直方图,计算脉冲飞行时间,最终实现目标距离的测量。The signal processing module is used for time-correlated single-photon counting processing, so as to obtain a histogram, calculate the pulse flight time, and finally realize the measurement of the target distance.
其中,采用控制模块产生重复频率可调的触发脉冲信号作为激光器的主控信号,用于控制激光脉冲的发射时刻,使得激光器输出的相邻两个脉冲之间的时间间隔各不相同。Among them, the control module is used to generate a trigger pulse signal with adjustable repetition frequency as the main control signal of the laser, which is used to control the emission timing of the laser pulse, so that the time interval between two adjacent pulses output by the laser is different.
其中,采用了事件计时器对参考光和回波光的脉冲时刻进行精确记录,既能实现皮秒量级的时间分辨率,又能实现大量程的测时范围,克服了时间分辨率与测时范围之间的矛盾。Among them, the event timer is used to accurately record the pulse timing of the reference light and the echo light, which can not only realize the time resolution of picosecond level, but also realize the time measurement range of a large range, which overcomes the time resolution and time measurement. inconsistencies between ranges.
其中,相邻两个激光脉冲之间的时间间隔各不相同,使得累积过程中只有本次触发时刻对应的回波光脉冲才能累积起来,非本次触发时刻的回波光脉冲将被离散化处理而无法累积起来,使得发射的高重频激光脉冲在大量程的测时范围条件下也不会出现多个回波。Among them, the time interval between two adjacent laser pulses is different, so that in the accumulation process, only the echo light pulses corresponding to the current trigger time can be accumulated, and the echo light pulses not at the current trigger time will be discretized and processed. It cannot be accumulated, so that the emitted high repetition frequency laser pulse will not have multiple echoes under the condition of a large range of time measurement range.
其中,采用了高重频的脉冲频率调制形式,高的重复频率既解决了光子计数体制的多次累积问题,又能适应运动条件下的测距场合,而脉冲频率调制可消除距离模糊实现远距离目标测距。Among them, the pulse frequency modulation form of high repetition frequency is adopted. The high repetition frequency not only solves the multiple accumulation problem of the photon counting system, but also adapts to the occasion of ranging under motion conditions. ranging from the target.
与现有技术相比,本发明所述的可消除距离模糊的高重频单光子激光雷达的优势在于:Compared with the prior art, the advantages of the high-repetition-frequency single-photon laser radar that can eliminate the distance ambiguity according to the present invention are:
(1)该高重频单光子激光雷达,采用了参考光和回波光均采用事件计时器精确记录脉冲时刻,既能实现皮秒量级的时间分辨率,又能实现大量程的测时范围。(1) This high-repetition single-photon lidar uses both the reference light and the echo light to accurately record the pulse time using an event timer, which can not only achieve a time resolution of the order of picoseconds, but also a large-scale time measurement range .
(2)该高重频单光子激光雷达,采用了相邻两个激光脉冲之间的时间间隔各不相同,使得累积过程中只有本次触发时刻对应的回波光脉冲才能累积起来,非本次触发时刻的回波光脉冲将被离散化处理而无法累积起来,使得发射的高重频激光脉冲在大的测时范围条件下也不会出现多个回波。(2) The high repetition frequency single-photon lidar uses different time intervals between two adjacent laser pulses, so that only the echo light pulses corresponding to the current trigger moment can be accumulated during the accumulation process, not the current time. The echo light pulse at the trigger time will be discretized and cannot be accumulated, so that the emitted high repetition frequency laser pulse will not have multiple echoes under the condition of a large time measurement range.
(3)该高重频单光子激光雷达,采用了高重频的频率调制激光脉冲,既解决了光子计数体制的多次累积问题,又能适应运动条件下的测距场合,还能消除距离模糊实现远距离目标测距。(3) The high repetition frequency single-photon lidar adopts high repetition frequency frequency modulated laser pulses, which not only solves the multiple accumulation problem of the photon counting system, but also adapts to ranging occasions under motion conditions, and can also eliminate the distance Fuzzy to achieve long-distance target ranging.
附图说明Description of drawings
图1为本发明一种可消除距离模糊的高重频单光子激光雷达的结构示意图。FIG. 1 is a schematic structural diagram of a high-repetition-frequency single-photon laser radar capable of eliminating distance ambiguity according to the present invention.
图2为本发明的脉冲频率调制波形图。FIG. 2 is a pulse frequency modulation waveform diagram of the present invention.
图3为本发明的回波信号提取原理图。FIG. 3 is a schematic diagram of the echo signal extraction of the present invention.
具体实施方式Detailed ways
为了使本发明的目的、方案和优点更加清楚明白,以下结合具体实施例,并参照附图对本发明作进一步的详细说明。In order to make the objects, solutions and advantages of the present invention more clearly understood, the present invention will be further described in detail below in conjunction with specific embodiments and with reference to the accompanying drawings.
本发明一种可消除距离模糊的高重频单光子激光雷达,该高重频单光子激光雷达包括控制模块1、激光器2、分束器3、发射光学系统4、光电二极管5、第一事件计时器6、接收光学系统7、单光子探测器8、第二事件计时器9和信号处理模块10,所述的控制模块1用于产生重复频率可调的触发脉冲信号,将其作为激光器的主控信号,用于控制激光脉冲的发射时刻;所述的激光器2用于产生激光脉冲信号,脉冲频率由控制模块1控制;所述的分束器3将激光器发射的激光信号一分为二,其中的大部分激光传输至发射光学系统4作为信号光,而小部分激光传输至光电二极管5作为参考光;所述的发射光学系统4用于对信号光进行准直和扩束并发射至被测目标上;所述的光电二极管5用于探测分束器3分出的参考光,以此作为计时基准信号;所述的第一事件计时器6用于精确记录参考光脉冲的时刻,以此作为脉冲飞行时间测量的起点;所述的接收光学系统7用于接收被测目标反射/散射的激光回波信号;所述的单光子探测器8用于响应光子量级的微弱回波光脉冲信号;所述的第二事件计时器9用于精确记录回波光脉冲的时刻,以此作为脉冲飞行时间测量的终点;所述的信号处理模块10用于进行时间相关单光子计数处理,从而获得直方图,计算脉冲飞行时间,最终实现目标距离的测量。The present invention is a high repetition frequency single photon laser radar capable of eliminating distance ambiguity. The high repetition frequency single photon laser radar comprises a control module 1, a laser 2, a beam splitter 3, an emission optical system 4, a photodiode 5, a first event A timer 6, a receiving optical system 7, a single-photon detector 8, a second event timer 9 and a signal processing module 10, the control module 1 is used to generate a trigger pulse signal with adjustable repetition frequency, which is used as a laser pulse signal. The main control signal is used to control the emission time of the laser pulse; the laser 2 is used to generate the laser pulse signal, and the pulse frequency is controlled by the control module 1; the beam splitter 3 divides the laser signal emitted by the laser into two , most of the laser light is transmitted to the emission optical system 4 as the signal light, and a small part of the laser light is transmitted to the photodiode 5 as the reference light; the emission optical system 4 is used to collimate and expand the signal light and emit it to on the measured target; the photodiode 5 is used to detect the reference light separated by the beam splitter 3 as a timing reference signal; the first event timer 6 is used to accurately record the time of the reference light pulse, Take this as the starting point of pulse time-of-flight measurement; the receiving optical system 7 is used to receive the laser echo signal reflected/scattered by the measured target; the single-photon detector 8 is used to respond to the weak echo light of the photon level Pulse signal; the second event timer 9 is used to accurately record the time of the echo light pulse as the end point of the pulse flight time measurement; the signal processing module 10 is used to perform time-correlated single-photon counting processing, thereby Obtain the histogram, calculate the pulse flight time, and finally realize the measurement of the target distance.
如图1所示,本发明提出的可消除距离模糊的高重频单光子激光雷达,包括控制模块1、激光器2、分束器3、发射光学系统4、光电二极管5、第一事件计时器6、接收光学系统7、单光子探测器8、第二事件计时器9、信号处理模块10。利用控制模块1产生重复频率可调的触发脉冲信号,将其作为激光器2的主控信号,用于控制激光脉冲的发射时刻。利用第一、第二事件计时器分别记录参考光脉冲和回波光脉冲时刻,并由信号处理模块10进行时间相关单光子计数处理,由于激光脉冲频率不断变化,使得累积过程中只有本次触发时刻的回波光脉冲才能累积起来,非本次触发时刻的回波光脉冲被离散化处理,最终使得单光子激光雷达能够在高重频条件下对远距离目标进行测距。As shown in FIG. 1 , the high-repetition single-photon lidar proposed by the present invention that can eliminate distance ambiguity includes a control module 1, a laser 2, a beam splitter 3, an emission optical system 4, a photodiode 5, and a first event timer 6. A receiving optical system 7 , a single photon detector 8 , a second event timer 9 , and a signal processing module 10 . The trigger pulse signal with adjustable repetition frequency is generated by the control module 1, which is used as the main control signal of the laser 2 to control the emission time of the laser pulse. The first and second event timers are used to record the time of the reference light pulse and the echo light pulse respectively, and the signal processing module 10 performs time-correlated single-photon counting processing. Since the frequency of the laser pulse changes continuously, only this trigger time is in the accumulation process. The echo light pulses can be accumulated, and the echo light pulses not at the current trigger time are discretized, which finally enables the single-photon lidar to measure the distance of long-distance targets under the condition of high repetition frequency.
控制模块1产生的重复频率可调制的脉冲信号,作为激光器2的主控信号,用于控制激光脉冲的发射时刻,脉冲频率调制波形图如图2所示。只要合理控制激光脉冲重频的变化量,就能够确保脉冲触发计时过程中只有本次触发时刻对应的回波光脉冲在规定的目标相对运动速度条件下均落在同一个距离门内,因而能够累积起来;而非本次触发时刻的回波光脉冲将被离散化处理而无法累积起来,使得发射的高重频激光脉冲在很大的测时范围条件下也不会出现多个回波。如此使得单光子激光雷达既不会出现距离模糊问题,又能够以较高的重频发射激光脉冲以实现运动目标的激光测距。The pulse signal with a modulated repetition frequency generated by the control module 1 is used as the main control signal of the laser 2 to control the emission timing of the laser pulse. The pulse frequency modulation waveform diagram is shown in FIG. 2 . As long as the variation of the repetition frequency of the laser pulse is reasonably controlled, it can be ensured that only the echo light pulse corresponding to the current trigger moment falls within the same distance gate under the specified relative motion speed of the target during the pulse trigger timing process, so it can accumulate The echo light pulses not at this trigger time will be discretized and cannot be accumulated, so that the emitted high repetition frequency laser pulse will not have multiple echoes under the condition of a large timing range. In this way, the single-photon lidar does not have the problem of distance ambiguity, and can emit laser pulses at a high repetition frequency to achieve laser ranging of moving targets.
为了更详细地说明可消除距离模糊的高重频单光子激光雷达基本原理,这里对回波信号提取方法进行说明,具体如图3所示。在一个时间测量周期中,ti时刻触发计时后采集到的脉冲只有ri是该时刻发射的激光脉冲产生的回波,ri与ti之间的时间间隔代表了真实的激光脉冲往返飞行时间,可以用于计算目标距离;而rj(i≠j)是其他时刻发射的激光脉冲产生的回波,rj与ti之间的时间间隔并不是真实的激光脉冲往返飞行时间,不能用于计算目标距离。In order to explain in more detail the basic principle of the high-repetition-frequency single-photon lidar that can eliminate distance ambiguity, the method for extracting echo signals is described here, as shown in Figure 3. In a time measurement cycle, only ri is the echo generated by the laser pulse emitted at the time t i of the pulses collected after the timing is triggered, and the time interval between ri and ti represents the real round-trip flight of the laser pulse time, which can be used to calculate the target distance; and r j (i≠j) is the echo generated by the laser pulses emitted at other times. The time interval between r j and t i is not the real round-trip flight time of the laser pulse, which cannot be Used to calculate the target distance.
另外,为了使得ti时刻触发计时后采集到的rj(i≠j)脉冲在多次累积过程中不会叠加起来,必须将这些脉冲离散分布开来,而不出现在同一个距离门内。为了达到这个效果,触发计时的时刻ti必须满足如下关系:In addition, in order to prevent the r j (i≠j) pulses collected after the trigger timing at time t i from being superimposed during multiple accumulation processes, these pulses must be discretely distributed and not appear in the same distance gate . In order to achieve this effect, the time t i that triggers the timing must satisfy the following relationship:
这里的Tbin为距离门时间,V为目标相对运动速度,c为光速。也就是说,在进行多次累积过程中,两个激光脉冲之间的时间间隔应满足如下条件:Here T bin is the distance gate time, V is the relative motion speed of the target, and c is the speed of light. That is to say, in the process of multiple accumulation, the time interval between two laser pulses should satisfy the following conditions:
只要确保激光脉冲的周期差异一个距离门时间Tbin,就可以使得ti时刻触发计时后采集到的rj(i≠j)脉冲在多次累积过程中不会出现在相同的距离门内,因而不会叠加起来。As long as the period of the laser pulses is different by a distance gate time T bin , the r j (i≠j) pulses collected after the trigger timing at time t i will not appear in the same distance gate in the multiple accumulation process, So they don't stack up.
本发明一种基于脉冲频率调制的高重频激光测距方法,既能消除距离模糊实现远距离目标测距,又能解决光子计数体制的多次累积问题,适应运动条件下的测距场合。同时,采用了事件计时器对参考光和回波光的脉冲时刻进行精确记录,既能实现皮秒量级的时间分辨率,又能实现大量程的测时范围,克服了时间分辨率与测时范围之间的矛盾。The present invention is a high repetition frequency laser ranging method based on pulse frequency modulation, which can not only eliminate distance ambiguity to achieve long-distance target ranging, but also solve the multiple accumulation problem of the photon counting system, and is suitable for ranging occasions under motion conditions. At the same time, an event timer is used to accurately record the pulse timing of the reference light and the echo light, which can not only achieve a time resolution of the order of picoseconds, but also a large range of time measurement, which overcomes the need for time resolution and time measurement. inconsistencies between ranges.
Claims (5)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910501221.XA CN110161522B (en) | 2019-06-11 | 2019-06-11 | High-repetition-frequency single-photon laser radar capable of eliminating range ambiguity |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910501221.XA CN110161522B (en) | 2019-06-11 | 2019-06-11 | High-repetition-frequency single-photon laser radar capable of eliminating range ambiguity |
Publications (2)
Publication Number | Publication Date |
---|---|
CN110161522A true CN110161522A (en) | 2019-08-23 |
CN110161522B CN110161522B (en) | 2022-11-11 |
Family
ID=67628344
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201910501221.XA Active CN110161522B (en) | 2019-06-11 | 2019-06-11 | High-repetition-frequency single-photon laser radar capable of eliminating range ambiguity |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN110161522B (en) |
Cited By (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110632578A (en) * | 2019-08-30 | 2019-12-31 | 深圳奥锐达科技有限公司 | System and method for time-coded time-of-flight distance measurement |
CN110687545A (en) * | 2019-09-27 | 2020-01-14 | 电子科技大学中山学院 | A high-precision lidar system |
CN110749898A (en) * | 2019-10-18 | 2020-02-04 | 深圳奥锐达科技有限公司 | Laser radar ranging system and ranging method thereof |
CN110850428A (en) * | 2019-12-12 | 2020-02-28 | 北京万集科技股份有限公司 | Laser radar ranging method, device, equipment and storage medium |
CN112130163A (en) * | 2020-11-26 | 2020-12-25 | 南京天朗防务科技有限公司 | Laser ranging system and method based on single photon detection |
WO2021035695A1 (en) * | 2019-08-30 | 2021-03-04 | 深圳奥锐达科技有限公司 | System and method for measuring distance by time of flight based on time codes |
CN112731428A (en) * | 2020-12-25 | 2021-04-30 | 中国科学技术大学 | Distance measuring device and active three-dimensional imaging system |
CN112731429A (en) * | 2020-12-10 | 2021-04-30 | 四川九洲空管科技有限责任公司 | Phase type laser radar range unit based on pulse position modulation |
CN113514850A (en) * | 2021-04-16 | 2021-10-19 | 山东省科学院海洋仪器仪表研究所 | Self-adaptive distance gating underwater laser imager and imaging method thereof |
CN113567959A (en) * | 2020-07-27 | 2021-10-29 | 北京一径科技有限公司 | Detection method and device of repetition frequency signal, processing equipment and storage medium |
WO2023279755A1 (en) * | 2021-07-07 | 2023-01-12 | 奥比中光科技集团股份有限公司 | Method and apparatus for masking ambiguity distance values of ranging system, and device |
WO2023279618A1 (en) * | 2021-07-07 | 2023-01-12 | 奥比中光科技集团股份有限公司 | Distance measurement system, and method for shielding fuzzy distance value |
CN117970347A (en) * | 2024-02-18 | 2024-05-03 | 中国电子科技集团公司第三十八研究所 | Single-photon laser radar ranging method using pulse period modulation |
CN118534474A (en) * | 2024-04-15 | 2024-08-23 | 深圳市慧脑智芯科技有限公司 | Target Radar Detection Method Based on Spiking Neural Network |
Citations (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4151415A (en) * | 1977-10-31 | 1979-04-24 | Varo, Inc. | Active imaging system using variable gate width time programmed dwell |
CN101722888A (en) * | 2008-10-29 | 2010-06-09 | 中国科学院半导体研究所 | A method for realizing anti-jamming large field of view distance gating car night vision |
CN203909297U (en) * | 2014-01-20 | 2014-10-29 | 华东师范大学 | Laser range finder based on high-speed single-photon detection |
CN104977571A (en) * | 2015-06-25 | 2015-10-14 | 西安电子科技大学 | Distance blur clutter suppression method based on pitch frequency diversity STAP |
CN105607073A (en) * | 2015-12-18 | 2016-05-25 | 哈尔滨工业大学 | A Photon Counting Imaging LiDAR Using Adjacent Pixel Thresholding Method to Filter Noise in Real Time |
US20160209498A1 (en) * | 2012-02-16 | 2016-07-21 | Reilly Daniel R | System and method for measuring optical delay using a single photon detector with pulsed optical signals |
CN106526608A (en) * | 2016-12-29 | 2017-03-22 | 中科和光(天津)应用激光技术研究所有限公司 | VCSEL-based laser radar ranging device |
CN107144834A (en) * | 2017-05-23 | 2017-09-08 | 哈尔滨工业大学 | A kind of Gao Zhongying pulse radar extends the waveform design method of finding range |
CN108089194A (en) * | 2017-12-15 | 2018-05-29 | 中国科学院光电技术研究所 | Photon counting laser radar based on composite pseudorandom coding |
CN108168717A (en) * | 2017-12-13 | 2018-06-15 | 中国科学院光电技术研究所 | photon number resolution balance detector |
CN108603758A (en) * | 2015-11-30 | 2018-09-28 | 卢米诺技术公司 | The pulse laser of laser radar system and laser radar system with distribution type laser device and multiple sensor heads |
US20180284240A1 (en) * | 2017-03-29 | 2018-10-04 | Luminar Technologies, Inc. | Using Detectors with Different Gains in a Lidar System |
CN109343069A (en) * | 2018-08-24 | 2019-02-15 | 南京理工大学 | Photon counting lidar capable of combined pulse ranging and its ranging method |
-
2019
- 2019-06-11 CN CN201910501221.XA patent/CN110161522B/en active Active
Patent Citations (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4151415A (en) * | 1977-10-31 | 1979-04-24 | Varo, Inc. | Active imaging system using variable gate width time programmed dwell |
CN101722888A (en) * | 2008-10-29 | 2010-06-09 | 中国科学院半导体研究所 | A method for realizing anti-jamming large field of view distance gating car night vision |
US20160209498A1 (en) * | 2012-02-16 | 2016-07-21 | Reilly Daniel R | System and method for measuring optical delay using a single photon detector with pulsed optical signals |
CN203909297U (en) * | 2014-01-20 | 2014-10-29 | 华东师范大学 | Laser range finder based on high-speed single-photon detection |
CN104977571A (en) * | 2015-06-25 | 2015-10-14 | 西安电子科技大学 | Distance blur clutter suppression method based on pitch frequency diversity STAP |
CN108603758A (en) * | 2015-11-30 | 2018-09-28 | 卢米诺技术公司 | The pulse laser of laser radar system and laser radar system with distribution type laser device and multiple sensor heads |
CN105607073A (en) * | 2015-12-18 | 2016-05-25 | 哈尔滨工业大学 | A Photon Counting Imaging LiDAR Using Adjacent Pixel Thresholding Method to Filter Noise in Real Time |
CN106526608A (en) * | 2016-12-29 | 2017-03-22 | 中科和光(天津)应用激光技术研究所有限公司 | VCSEL-based laser radar ranging device |
US20180284240A1 (en) * | 2017-03-29 | 2018-10-04 | Luminar Technologies, Inc. | Using Detectors with Different Gains in a Lidar System |
CN107144834A (en) * | 2017-05-23 | 2017-09-08 | 哈尔滨工业大学 | A kind of Gao Zhongying pulse radar extends the waveform design method of finding range |
CN108168717A (en) * | 2017-12-13 | 2018-06-15 | 中国科学院光电技术研究所 | photon number resolution balance detector |
CN108089194A (en) * | 2017-12-15 | 2018-05-29 | 中国科学院光电技术研究所 | Photon counting laser radar based on composite pseudorandom coding |
CN109343069A (en) * | 2018-08-24 | 2019-02-15 | 南京理工大学 | Photon counting lidar capable of combined pulse ranging and its ranging method |
Non-Patent Citations (4)
Title |
---|
张河辉等: "光子技术激光测深系统", 《红外与激光工程》, vol. 48, no. 1, 16 October 2018 (2018-10-16), pages 100 - 104 * |
李飞: "相位编码合成孔径激光雷达关键技术研究", 《中国优秀博硕士学位论文全文数据库(博士)信息科技辑》 * |
李飞: "相位编码合成孔径激光雷达关键技术研究", 《中国优秀博硕士学位论文全文数据库(博士)信息科技辑》, 15 November 2016 (2016-11-15), pages 136 - 5 * |
陈臻: "基于偏振调制的激光三维成像方法研究", 《中国优秀博硕士学位论文全文数据库(博士)信息科技辑》, 15 September 2017 (2017-09-15), pages 136 - 55 * |
Cited By (20)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110632578B (en) * | 2019-08-30 | 2022-12-09 | 深圳奥锐达科技有限公司 | System and method for time-encoded time-of-flight distance measurement |
CN110632578A (en) * | 2019-08-30 | 2019-12-31 | 深圳奥锐达科技有限公司 | System and method for time-coded time-of-flight distance measurement |
WO2021035695A1 (en) * | 2019-08-30 | 2021-03-04 | 深圳奥锐达科技有限公司 | System and method for measuring distance by time of flight based on time codes |
CN110687545A (en) * | 2019-09-27 | 2020-01-14 | 电子科技大学中山学院 | A high-precision lidar system |
CN110687545B (en) * | 2019-09-27 | 2022-03-25 | 电子科技大学中山学院 | High-precision laser radar system |
CN110749898A (en) * | 2019-10-18 | 2020-02-04 | 深圳奥锐达科技有限公司 | Laser radar ranging system and ranging method thereof |
CN110850428A (en) * | 2019-12-12 | 2020-02-28 | 北京万集科技股份有限公司 | Laser radar ranging method, device, equipment and storage medium |
CN110850428B (en) * | 2019-12-12 | 2021-11-23 | 北京万集科技股份有限公司 | Laser radar ranging method, device, equipment and storage medium |
CN113567959A (en) * | 2020-07-27 | 2021-10-29 | 北京一径科技有限公司 | Detection method and device of repetition frequency signal, processing equipment and storage medium |
CN112130163B (en) * | 2020-11-26 | 2021-02-05 | 南京天朗防务科技有限公司 | Laser ranging system and method based on single photon detection |
CN112130163A (en) * | 2020-11-26 | 2020-12-25 | 南京天朗防务科技有限公司 | Laser ranging system and method based on single photon detection |
CN112731429A (en) * | 2020-12-10 | 2021-04-30 | 四川九洲空管科技有限责任公司 | Phase type laser radar range unit based on pulse position modulation |
CN112731429B (en) * | 2020-12-10 | 2024-05-14 | 四川九洲空管科技有限责任公司 | Phase type laser radar ranging device based on pulse position modulation |
CN112731428A (en) * | 2020-12-25 | 2021-04-30 | 中国科学技术大学 | Distance measuring device and active three-dimensional imaging system |
CN112731428B (en) * | 2020-12-25 | 2023-11-28 | 中国科学技术大学 | A distance measuring device and active three-dimensional imaging system |
CN113514850A (en) * | 2021-04-16 | 2021-10-19 | 山东省科学院海洋仪器仪表研究所 | Self-adaptive distance gating underwater laser imager and imaging method thereof |
WO2023279755A1 (en) * | 2021-07-07 | 2023-01-12 | 奥比中光科技集团股份有限公司 | Method and apparatus for masking ambiguity distance values of ranging system, and device |
WO2023279618A1 (en) * | 2021-07-07 | 2023-01-12 | 奥比中光科技集团股份有限公司 | Distance measurement system, and method for shielding fuzzy distance value |
CN117970347A (en) * | 2024-02-18 | 2024-05-03 | 中国电子科技集团公司第三十八研究所 | Single-photon laser radar ranging method using pulse period modulation |
CN118534474A (en) * | 2024-04-15 | 2024-08-23 | 深圳市慧脑智芯科技有限公司 | Target Radar Detection Method Based on Spiking Neural Network |
Also Published As
Publication number | Publication date |
---|---|
CN110161522B (en) | 2022-11-11 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN110161522B (en) | High-repetition-frequency single-photon laser radar capable of eliminating range ambiguity | |
CN110161519B (en) | Macro-pulse photon counting laser radar | |
CN109343069B (en) | Photon counting laser radar capable of realizing combined pulse ranging and ranging method thereof | |
CN110741281B (en) | LiDAR system and method using late lock cover mode detection | |
CN108828616B (en) | Photon counting laser radar capable of realizing monopulse ranging and constant false alarm control method | |
CN103148744B (en) | Method for resisting backward dispersion for laser semi-active seeker | |
CN203909297U (en) | Laser range finder based on high-speed single-photon detection | |
CN109597057A (en) | A kind of return laser beam distance measuring method and range unit | |
CN107907885B (en) | Underwater target detection device based on single photon counting method | |
CN109613506A (en) | A Random Frequency Hopping Repeated Frequency Agility Radar Target Echo Signal Detection Method | |
CN110488241A (en) | A kind of laser radar multiple echo information extraction element and method | |
CN112526536B (en) | Single photon ranging system and method based on pulse train technology | |
CN111505658B (en) | Pulse group type laser ranging method with adjustable repetition frequency | |
CN1831561A (en) | Apparatus and method for chaotic laser distance measurement of LD pumped solid-state laser | |
CN109870702A (en) | A kind of distant-range high-precision laser ranging system and distance measuring method based on TDC | |
WO2020083780A1 (en) | Time-of-flight ranging using modulated pulse trains of laser pulses | |
CN114185057B (en) | A detection method, device and terminal | |
US4153366A (en) | Rangefinding system | |
CN104111450B (en) | A kind of method and system utilizing dipulse detection target micro-Doppler feature | |
Zhu et al. | High anti-interference 3D imaging LIDAR system based on digital chaotic pulse position modulation | |
CN107015235B (en) | High-precision Gm-APD laser radar system based on multi-gate full-waveform response and ranging method thereof | |
CN117590418A (en) | A laser echo ranging method and system based on spread spectrum system | |
CN116148815A (en) | True random coding single-photon laser radar and target position determining method | |
Lyu et al. | Signal flux and time-of-flight estimation based on waveform optimization for single-photon LiDAR | |
CN111521991B (en) | Proximity detection device and method |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |