CN106199535B - It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction - Google Patents
It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction Download PDFInfo
- Publication number
- CN106199535B CN106199535B CN201610517141.XA CN201610517141A CN106199535B CN 106199535 B CN106199535 B CN 106199535B CN 201610517141 A CN201610517141 A CN 201610517141A CN 106199535 B CN106199535 B CN 106199535B
- Authority
- CN
- China
- Prior art keywords
- induced
- pulse
- signal
- laser
- radar 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.)
- Active
Links
- 238000000034 method Methods 0.000 title abstract description 11
- 230000003287 optical effect Effects 0.000 claims abstract description 33
- 230000006698 induction Effects 0.000 claims abstract description 24
- 230000001939 inductive effect Effects 0.000 claims abstract description 18
- 239000004065 semiconductor Substances 0.000 claims description 9
- 230000008878 coupling Effects 0.000 claims description 8
- 238000010168 coupling process Methods 0.000 claims description 8
- 238000005859 coupling reaction Methods 0.000 claims description 8
- 230000004044 response Effects 0.000 claims description 7
- 230000001052 transient effect Effects 0.000 claims description 6
- 230000001934 delay Effects 0.000 claims description 4
- 238000004519 manufacturing process Methods 0.000 claims 1
- 238000001514 detection method Methods 0.000 abstract description 17
- 230000003044 adaptive effect Effects 0.000 abstract 1
- 230000000149 penetrating effect Effects 0.000 description 14
- 239000000463 material Substances 0.000 description 13
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 10
- 238000005516 engineering process Methods 0.000 description 9
- 230000008859 change Effects 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000007274 generation of a signal involved in cell-cell signaling Effects 0.000 description 4
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 4
- 229910052753 mercury Inorganic materials 0.000 description 4
- 238000004088 simulation Methods 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 230000005684 electric field Effects 0.000 description 3
- 230000035515 penetration Effects 0.000 description 3
- 230000007704 transition Effects 0.000 description 3
- 238000013461 design Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 238000012795 verification Methods 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000003116 impacting effect Effects 0.000 description 1
- 230000008676 import Effects 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- 230000003071 parasitic effect Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 239000000243 solution Substances 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
- G01S7/28—Details of pulse systems
- G01S7/282—Transmitters
-
- 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
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/88—Radar or analogous systems specially adapted for specific applications
- G01S13/885—Radar or analogous systems specially adapted for specific applications for ground probing
-
- 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
- G01S17/88—Lidar systems specially adapted for specific applications
-
- 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
- G01S7/484—Transmitters
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Computer Networks & Wireless Communication (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Radar Systems Or Details Thereof (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Abstract
本发明公开了一种基于光诱导开关产生高压脉冲雷达信号的方法及装置。所述方法包括:1)产生诱导激光脉冲信号,通过光耦合器后分为两路;2)通过光诱导开关使两路诱导激光脉冲信号产生正向波与反向波;3)通过延时控制模块调节正向波与反向波的相对时间延迟,产生脉宽可调的雷达信号。所述装置包括:诱导激光控制电路,将产生的诱导激光脉冲输出为两路诱导激光脉冲信号;脉冲发生电路,产生两个方向相反的脉冲,输出脉宽可调的雷达信号。本发明具有更高的稳定性和可重复性,使产生的雷达信号具有更好的质量和更小的波形拖尾,实际探测中可自动或手动地调整探地雷达信号脉宽,实现具有高度适应性和针对性的最佳分辨率探测。
The invention discloses a method and a device for generating a high-voltage pulse radar signal based on an optical induction switch. The method includes: 1) generating an induced laser pulse signal, which is divided into two paths after passing through an optical coupler; 2) making the two paths of induced laser pulse signal generate a forward wave and a reverse wave through an optical inductive switch; 3) passing a time delay The control module adjusts the relative time delay between the forward wave and the reverse wave to generate a radar signal with adjustable pulse width. The device includes: an induction laser control circuit, which outputs the generated induction laser pulses as two induction laser pulse signals; a pulse generation circuit, which generates two pulses in opposite directions, and outputs a radar signal with adjustable pulse width. The invention has higher stability and repeatability, so that the generated radar signal has better quality and smaller waveform tailing. In actual detection, the pulse width of the ground-penetrating radar signal can be adjusted automatically or manually to achieve a high Adaptive and targeted optimal resolution detection.
Description
技术领域technical field
本发明属于探地雷达技术领域,具体涉及一种基于光诱导开关产生高压脉冲雷达信号的方法及装置。The invention belongs to the technical field of ground penetrating radar, and in particular relates to a method and a device for generating high-voltage pulse radar signals based on an optical induction switch.
背景技术Background technique
利用探地雷达设备和技术进行地下目标探测的机理是通过发射高频电磁脉冲波,利用地下目标与周围介质电性参数的差异,根据回波信号振幅与时间、频率特征等参数来分析和推断地下目标的空间位置、深度与尺寸等信息。探地雷达是一种高效的浅层地球物理探测技术,与探空雷达不同,探地雷达使用的频率一般低于前者,其理论研究主要是电磁波在有耗介质中的传播,由于介质的不均匀性、各向异性、强衰减性等,其复杂程度较之探空雷达要大得多。与传统的地球物理方法相比,探地雷达具有快捷、操作简单、抗干扰和场地适应能力强、探测分辨率高等方面的优势,因而该技术一面世就受到工程物探界的普遍重视。特别是自20世纪70年代以来,随着计算机和微电子技术的飞速发展,探地雷达无论是在仪器设备,还是数据处理等方面都得到了普遍提高,其应用范围不断扩大,目前已广泛应用于地质、工程、资源、环境、军事等方面。The mechanism of ground-penetrating radar equipment and technology for underground target detection is to analyze and infer according to the echo signal amplitude, time, frequency characteristics and other parameters by emitting high-frequency electromagnetic pulse waves, using the difference in electrical parameters between the underground target and the surrounding medium. Information such as the spatial position, depth and size of underground targets. GPR is an efficient shallow geophysical detection technology. Different from airsonde radar, the frequency used by GPR is generally lower than that of the former. Its theoretical research is mainly on the propagation of electromagnetic waves in lossy media. Uniformity, anisotropy, strong attenuation, etc., its complexity is much greater than that of sounding radar. Compared with traditional geophysical methods, ground penetrating radar has the advantages of quickness, simple operation, strong anti-interference and site adaptability, and high detection resolution. Especially since the 1970s, with the rapid development of computer and microelectronic technology, ground penetrating radar has been generally improved in terms of equipment and data processing, and its application range has been continuously expanded. In geology, engineering, resources, environment, military and other aspects.
探地雷达一般由电磁脉冲信号产生电路、收发天线、信号采集电路以及数据处理等部分构成。其中的电磁脉冲信号产生电路部分是探地雷达的核心模块之一,对于产生纳秒级的电磁脉冲信号而言,电性的脉冲产生方式主要有气体放电、隧道二极管、水银开关和雪崩三极管等。其中,气体放电和水银开关结合的电磁脉冲信号产生原理是利用水银开关管的瞬间放电击穿和恢复特性,产生前沿和宽度为纳秒级,幅度高达千伏的高压窄脉冲;而水银开关则是一种高性能的高压开关,所产生的脉冲对称性较好;隧道二极管脉冲发生器由于其脉冲宽度较宽且幅度不高所以并不是非常常用;雪崩三极管的重复率可达几兆赫,响应时间快产生的脉冲幅度可达上百伏特。常见的电磁脉冲信号电路产生电路一半利用半导体雪崩二极管、阶跃二极管等多级串接来实现高压雷达波脉冲信号,然而其产生的脉冲波形脉冲宽度是固定的,同时多级串接时由于多个器件之间存在参数差异性、延迟的不同步以及寄生参数的影响,将引起雷达脉冲波形的脉宽展宽,同时还会产生高压脉冲信号的拖尾。Ground penetrating radar is generally composed of electromagnetic pulse signal generation circuit, transceiver antenna, signal acquisition circuit and data processing and other parts. The electromagnetic pulse signal generation circuit part is one of the core modules of ground penetrating radar. For generating nanosecond electromagnetic pulse signals, the electrical pulse generation methods mainly include gas discharge, tunnel diode, mercury switch and avalanche triode, etc. . Among them, the principle of electromagnetic pulse signal generation combined with gas discharge and mercury switch is to use the instantaneous discharge breakdown and recovery characteristics of the mercury switch tube to generate a high-voltage narrow pulse with a leading edge and a width of nanoseconds and an amplitude of up to kilovolts; while the mercury switch is It is a high-performance high-voltage switch, and the pulse symmetry generated is better; the tunnel diode pulse generator is not very commonly used because of its wide pulse width and low amplitude; the repetition rate of the avalanche triode can reach several MHz, and the response The amplitude of the pulse generated by the fast time can reach hundreds of volts. Half of the common electromagnetic pulse signal circuit generation circuit uses semiconductor avalanche diodes, step diodes and other multi-stage series connections to realize high-voltage radar wave pulse signals. There are parameter differences, delay out-of-sync, and parasitic parameters among individual devices, which will cause the pulse width of the radar pulse waveform to widen, and at the same time cause the tail of the high-voltage pulse signal.
目前国内应用于实际工程的绝大多数探地雷达设备是依赖于国外进口,但从目前的应用情况来看,探地雷达在工程探测中的应用还存在很大的问题与技术瓶颈,首先是设备价格昂贵限制了探地雷达设备和探测技术的推广和普及,另一个非常重要的原因是设备的应用和选择非常依赖于探测的目标特征,如不同目标探测深度、不同目标尺寸应选择不同系列或不同频段的雷达;从技术上讲,具有一定重复频率的高压短脉冲产生技术是基于脉冲信号的探地雷达探测技术的重要关键,不同型号、不同频段的探地雷达其特征对应特定的发射雷达波脉宽,如500MHz波段冲击雷达,其对应的脉宽接近1纳秒;再者,雷达探测分辨率与探测范围存在固有的矛盾,高频段的雷达虽然具有较高的分辨率,但其穿透深度却非常有限,一般400MHz透深度为4米,而典型的1.6GHz雷达穿透深度只有0.5米。At present, the vast majority of ground penetrating radar equipment used in actual engineering in China relies on foreign imports, but judging from the current application situation, there are still big problems and technical bottlenecks in the application of ground penetrating radar in engineering detection, first of all The high price of equipment limits the promotion and popularization of ground penetrating radar equipment and detection technology. Another very important reason is that the application and selection of equipment are very dependent on the characteristics of the target to be detected. For example, different target detection depths and different target sizes should choose different series. Or radars of different frequency bands; technically speaking, the high-voltage short pulse generation technology with a certain repetition frequency is an important key to the ground-penetrating radar detection technology based on pulse signals, and the characteristics of ground-penetrating radars of different models and different frequency bands correspond to specific emission The pulse width of radar waves, such as the 500MHz band impacting the radar, corresponds to a pulse width close to 1 nanosecond; moreover, there is an inherent contradiction between the radar detection resolution and the detection range. Although the high-frequency radar has a higher resolution, its The penetration depth is very limited, generally 400MHz penetration depth is 4 meters, while the typical 1.6GHz radar penetration depth is only 0.5 meters.
就目前情况来看,对于雷达电磁脉冲信号产生模块,如何产生具有更快上升时间、以及更高的稳定性与重复性,如何使产生的雷达脉冲信号具有更好的质量以及更小的波形拖尾是目前高分辨率雷达电磁脉冲产生技术所面临的问题之一;如何提高单个探地雷达的多种对象探测能力,即实现单一雷达设备具备频段可调的功能,以在实际探测中实现面向具体目标对象的最佳分辨率探测,也是当下探地雷达技术所面临的关键问题之一。As far as the current situation is concerned, for the radar electromagnetic pulse signal generation module, how to generate faster rise time, higher stability and repeatability, and how to make the generated radar pulse signal have better quality and smaller waveform drag Tail is one of the problems faced by high-resolution radar electromagnetic pulse generation technology; The optimal resolution detection of specific target objects is also one of the key issues faced by current ground penetrating radar technology.
发明内容Contents of the invention
针对上述技术所存在的问题,本发明提供了一种基于光诱导开关产生高压脉冲雷达信号的方法,实现输出的高压脉冲雷达信号具有脉宽可调的功能。Aiming at the problems existing in the above-mentioned technologies, the present invention provides a method for generating high-voltage pulse radar signals based on optically induced switches, and realizes that the output high-voltage pulse radar signals have the function of adjustable pulse width.
一种基于光诱导开关产生高压脉冲雷达信号的方法,包括步骤:A method for generating a high-voltage pulse radar signal based on an optically induced switch, comprising the steps of:
1)产生诱导激光脉冲信号,通过光耦合器后分为两路;1) Generate an induced laser pulse signal, which is divided into two paths after passing through an optical coupler;
2)通过光诱导开关使两路诱导激光脉冲信号产生正向波与反向波;2) Through the optical induction switch, the two induction laser pulse signals generate forward wave and reverse wave;
3)通过延时控制模块调节正向波与反向波的相对时间延迟,产生脉宽可调的雷达信号。3) The relative time delay between the forward wave and the reverse wave is adjusted by the delay control module to generate a radar signal with adjustable pulse width.
本发明还提供了一种基于光诱导开关产生高压脉冲雷达信号的装置,能产生具有更快上升时间、更高稳定性与重复性的高压电磁脉冲信号,并且能够很好地解决单一雷达设备无产生多频段可调的探地雷达功能,应用于面向探测对象的脉宽可调探地雷达系统,以实现不同深度下的高分辨率探测。The present invention also provides a device for generating a high-voltage pulse radar signal based on an optically induced switch, which can generate a high-voltage electromagnetic pulse signal with a faster rise time, higher stability and repeatability, and can well solve the problem of no single radar device. Generate multi-band adjustable ground penetrating radar function, which is applied to the pulse width adjustable ground penetrating radar system for detection objects to achieve high-resolution detection at different depths.
一种基于光诱导开关产生高压脉冲雷达信号的装置,包括:A device for generating high-voltage pulse radar signals based on an optically induced switch, comprising:
1)诱导激光控制电路,将产生的诱导激光脉冲输出为两路诱导激光脉冲信号;1) The induced laser control circuit outputs the generated induced laser pulses as two induced laser pulse signals;
2)脉冲发生电路,产生两个方向相反的脉冲,输出脉宽可调的雷达信号。2) The pulse generating circuit generates two pulses in opposite directions, and outputs a radar signal with adjustable pulse width.
所述诱导激光控制电路包括诱导信号激光源、光耦合器和两个延时控制模块;所述诱导信号激光源产生诱导激光脉冲,经光耦合器后分为两路,通过两个延时控制模块分别控制这两路诱导激光脉冲的时间延迟,最后输出两路诱导激光脉冲信号。The induced laser control circuit includes an induced signal laser source, an optical coupler and two delay control modules; the induced signal laser source generates an induced laser pulse, which is divided into two paths through the optical coupler, and is controlled by two delays. The module separately controls the time delay of the two induced laser pulses, and finally outputs two induced laser pulse signals.
所述脉冲发生电路,包括高压偏置输入模块、两个光诱导开关、负载匹配模块、输出耦合模块;所述高压偏置输入模块产生高电平的脉冲信号,为两个光诱导开关提供能量,两个光诱导开关接收诱导激光控制电路输出的诱导激光脉冲信号,产生暂态响应,负载匹配模块用于匹配负载,脉冲输出耦合模块输出脉宽可调的高压脉冲雷达信号。The pulse generation circuit includes a high-voltage bias input module, two photo-induced switches, a load matching module, and an output coupling module; the high-voltage bias input module generates a high-level pulse signal to provide energy for the two photo-induced switches The two optical induction switches receive the induction laser pulse signal output by the induction laser control circuit to generate a transient response, the load matching module is used to match the load, and the pulse output coupling module outputs a high-voltage pulse radar signal with adjustable pulse width.
所述高压偏置输入模块通过微带线连接到两个光诱导开关的公共端,提供电路所需的高压能量,产生高电平的脉冲信号,并提供光诱导开关中光敏部分发生光电效应所需的强电场条件。The high-voltage bias input module is connected to the common end of the two photo-induced switches through a microstrip line to provide the high-voltage energy required by the circuit, generate a high-level pulse signal, and provide the photoelectric effect generated by the photosensitive part of the photo-induced switch. required strong electric field conditions.
所述两个光诱导开关以推挽式结构相互连接,以产生方向相反的脉冲信号。The two light-induced switches are connected to each other in a push-pull structure to generate pulse signals with opposite directions.
所述两个光诱导开关接收诱导激光控制电路输出的诱导激光脉冲信号,在极短时间内诱导激光脉冲信号照射光诱导开关的光敏部分,光诱导开关的开闭状态将在极短时间内发生改变,使电路在极短时间内产生暂态响应。在诱导激光脉冲照射下,两个光诱导开关可以先后输出两个方向相反的脉冲波(即正向波与反向波),通过延时控制模块可以控制输出的正向波与反向波的相对时间延迟,进而调节高压脉冲雷达信号的脉宽。The two photo-induced switches receive the induced laser pulse signal output by the induced laser control circuit, and the induced laser pulse signal irradiates the photosensitive part of the photo-induced switch in a very short time, and the on-off state of the photo-induced switch will occur in a very short time Change, so that the circuit produces a transient response in a very short time. Under the irradiation of induced laser pulses, the two optically induced switches can successively output two pulse waves in opposite directions (that is, forward wave and reverse wave), and the delay control module can control the output of forward wave and reverse wave. Relative time delay, and then adjust the pulse width of the high-voltage pulse radar signal.
所述光诱导开关选用半导体光诱导开关。其构成材料为III-V族化合物半导体材料。该半导体材料具有暗态电阻高、载流子寿命短、载流子迁移率大的特性。相对于传统的雪崩二极管或阶跃二极管,采用光诱导开关的雷达脉冲发生电路产生的雷达信号具有更快的上升时间以及更高的稳定性与重复性,并且具有更好的质量以及更小的波形拖尾。The photo-induced switch is a semiconductor photo-induced switch. Its constituent materials are III-V compound semiconductor materials. The semiconductor material has the characteristics of high dark state resistance, short carrier lifetime and high carrier mobility. Compared with the traditional avalanche diode or step diode, the radar signal generated by the radar pulse generation circuit using the light-induced switch has a faster rise time, higher stability and repeatability, and has better quality and smaller Waveforms smear.
作为优选,所述光诱导开关选用基于GaAs材料的光诱导开关。当具有一定能量的光子注入GaAs材料的半导体时,半导体内部被吸收的光子会产生电子空穴对,其内部电阻将发生随激光注入的迅速改变。Preferably, the light-induced switch is a light-induced switch based on GaAs material. When photons with a certain energy are injected into the semiconductor of GaAs material, the photons absorbed inside the semiconductor will generate electron-hole pairs, and its internal resistance will change rapidly with the laser injection.
进一步优选,选择光子能量为1.16eV的1064nm激光作为基于GaAs材料的光诱导开关的控制光信号。本发明中输入端为偏置高压,提供高压电场条件,使禁带宽度为1.42eV的GaAs材料的有效能隙减小,因此使用光子能量为1.16eV的1064nm激光作为基于GaAs材料的光诱导开关的光诱导控制信号。Further preferably, a 1064nm laser with a photon energy of 1.16eV is selected as the control optical signal of the light-induced switch based on GaAs material. In the present invention, the input end is a bias high voltage, which provides a high voltage electric field condition, so that the effective energy gap of the GaAs material with a band gap of 1.42eV is reduced, so a 1064nm laser with a photon energy of 1.16eV is used as a light-induced switch based on the GaAs material light-induced control signals.
所述基于光诱导开关产生高压脉冲雷达信号的装置工作时,诱导信号激光光源产生诱导激光脉冲信号,经光耦合器后分为两路,两路诱导激光脉冲信号分别由两个延时控制模块控制并调节时间延迟,所形成的两路诱导激光脉冲信号分别控制两个光诱导开关的开闭状态。光诱导开关的光敏区在诱导激光脉冲信号的照射下发生光电效应,使电路产生暂态响应。在延时控制模块的控制下,两个诱导激光脉冲信号之间的相对时间延迟达到亚纳秒级别,从而实现反向波与正向波之间的相对时间延迟达到亚纳秒级精度。通过调节反向波与正向波之间的相对时间延迟,信号波形由反向极小值至正向极大值之间的上升过渡时间将发生改变,合成的暂态波波形以及合成的雷达脉冲信号的中心频段将发生变化。经过调节,可以将形成的雷达脉冲波形调节精度控制在亚纳秒精度。When the device for generating high-voltage pulse radar signals based on an optical inductive switch is in operation, the inductive signal laser light source generates an inductive laser pulse signal, which is divided into two paths after being passed through an optical coupler, and the two inductive laser pulse signals are controlled by two delay control modules respectively. The time delay is controlled and adjusted, and the two induced laser pulse signals formed respectively control the opening and closing states of the two optically induced switches. The photosensitive area of the photoinducible switch has a photoelectric effect under the irradiation of the inductive laser pulse signal, which makes the circuit produce a transient response. Under the control of the delay control module, the relative time delay between the two induced laser pulse signals reaches the sub-nanosecond level, so that the relative time delay between the reverse wave and the forward wave reaches the sub-nanosecond level precision. By adjusting the relative time delay between the reverse wave and the forward wave, the rising transition time of the signal waveform from the reverse minimum value to the forward maximum value will change, the synthesized transient wave waveform and the synthesized radar The center frequency band of the pulse signal will change. After adjustment, the adjustment accuracy of the formed radar pulse waveform can be controlled at sub-nanosecond accuracy.
通过方案设计和仿真,确定两个方向相反的脉冲波之间的时间延迟和与之相对应的合成雷达信号的脉宽之间的关系。在实际测量场景中,通过诱导激光控制电路调节诱导激光的延时进行光诱导开关触发延时的控制,进而调节雷达信号的脉宽,从而使形成的雷达信号于当前应用场景保证最佳的测量分辨率。Through scheme design and simulation, the relationship between the time delay between two opposite pulse waves and the corresponding pulse width of the synthesized radar signal is determined. In the actual measurement scene, the delay of the induced laser is adjusted by the induced laser control circuit to control the trigger delay of the light-induced switch, and then adjust the pulse width of the radar signal, so that the formed radar signal can ensure the best measurement in the current application scenario resolution.
与传统探地雷达系统相比,本发明能够产生的脉宽可调雷达信号,能够产生具有更快上升时间、更高稳定性与重复性的高压电磁脉冲信号,并且很好地解决单一雷达设备无产生多频段可调的探地雷达功能,应用面向探测对象的脉宽可调探地雷达系统,实现不同深度下的高分辨率探测。Compared with the traditional ground penetrating radar system, the pulse width adjustable radar signal that the present invention can generate can generate high-voltage electromagnetic pulse signals with faster rise time, higher stability and repeatability, and can solve the problem of single radar equipment well. Without the function of generating multi-band adjustable ground penetrating radar, the pulse width adjustable ground penetrating radar system for detection objects is applied to realize high-resolution detection at different depths.
附图说明:Description of drawings:
图1为本发明基于光诱导开关产生高压脉冲雷达信号的装置示意图。Fig. 1 is a schematic diagram of a device for generating high-voltage pulse radar signals based on an optical inductive switch according to the present invention.
图2为本发明装置输出的正反两个脉冲波示意图。Fig. 2 is a schematic diagram of two positive and negative pulse waves output by the device of the present invention.
图3为本发明装置改变时间延迟所形成的雷达信号的示意图。Fig. 3 is a schematic diagram of the radar signal formed by changing the time delay of the device of the present invention.
图4为本发明装置改变时间延迟所形成的雷达信号的频谱示意图。Fig. 4 is a schematic diagram of the frequency spectrum of the radar signal formed by changing the time delay of the device of the present invention.
具体实施方式:Detailed ways:
为了更为具体地描述本发明,下面将结合附图及具体实施方式对本发明的技术方案进行详细说明。In order to describe the present invention more specifically, the technical solution of the present invention will be described in detail below in conjunction with the accompanying drawings and specific embodiments.
基于光诱导开关产生高压脉冲雷达信号的方法,包括步骤:A method for generating a high-voltage pulse radar signal based on an optically induced switch, comprising the steps of:
1)产生诱导激光脉冲信号,通过光耦合器分为两路;1) Generate an induced laser pulse signal, which is divided into two paths through an optical coupler;
2)通过光诱导开关使两路诱导脉冲信号产生正向波与反向波;2) Through the optical induction switch, the two induction pulse signals generate forward wave and reverse wave;
3)通过延时控制模块调节正向波与反向波的相对时间延迟,产生脉宽可调的雷达信号。3) The relative time delay between the forward wave and the reverse wave is adjusted by the delay control module to generate a radar signal with adjustable pulse width.
如图1所示,基于光诱导开关产生高压脉冲雷达信号的装置包括诱导激光控制电路和脉冲发生电路;诱导激光控制电路包括诱导信号激光源1、光耦合器2、延时控制模块3a和延时控制模块3b;脉冲发生电路包括光诱导开关5a、光诱导开关5b、负载匹配模块6、高压偏置输入模块8、输出耦合模块9、连接各模块的微带线10、信号地7a和信号地7b。As shown in Figure 1, the device for generating high-voltage pulse radar signals based on an optical inductive switch includes an inductive laser control circuit and a pulse generation circuit; the inductive laser control circuit includes an inductive signal laser source 1, an optical coupler 2, a delay control module 3a and a delay Timing control module 3b; pulse generating circuit includes light induction switch 5a, light induction switch 5b, load matching module 6, high voltage bias input module 8, output coupling module 9, microstrip line 10 connecting each module, signal ground 7a and signal Land 7b.
具体工作时,诱导信号激光源1产生诱导激光脉冲信号,经过光耦合器2分路为两路,两路诱导激光脉冲各自经过延时控制模块3a、3b后分别输出两个具有相对时间延迟的诱导激光脉冲信号4a、4b,诱导激光脉冲信号4a用于控制光诱导开关5a,诱导激光脉冲信号4b用于控制光诱导开关5b;高压偏置输入模块8由微带线10接到两个光诱导开关5a、5b的公共端;光诱导开关5a、5b以推挽式结构相互连接;光诱导开关5a另一端经微带线10连接信号地7a,光诱导开关5b另一端连接负载匹配模块6,同时经输出耦合模块9输出雷达信号。During specific work, the induced signal laser source 1 generates an induced laser pulse signal, which is divided into two paths through the optical coupler 2, and the two induced laser pulses respectively pass through the delay control modules 3a and 3b and then output two signals with relative time delays. The induced laser pulse signal 4a, 4b, the induced laser pulse signal 4a is used to control the optically induced switch 5a, and the induced laser pulse signal 4b is used to control the optically induced switch 5b; the high voltage bias input module 8 is connected to two optical The common end of the inductive switch 5a, 5b; the optical inductive switch 5a, 5b is connected to each other in a push-pull structure; the other end of the optical inductive switch 5a is connected to the signal ground 7a through the microstrip line 10, and the other end of the optical inductive switch 5b is connected to the load matching module 6 , and output the radar signal through the output coupling module 9 at the same time.
两个光诱导开关选用基于GaAs材料的光诱导开关,当具有一定能量的光子注入GaAs材料的半导体时,半导体内部被吸收的光子就会产生电子空穴对,其内部电阻将发生随激光注入的迅速改变。本方案中输入端为偏置高压,提供高压电场条件,使禁带宽度为1.42eV的GaAs材料的有效能隙减小,可以使用光子能量为1.16eV的1064nm激光作为GaAs材料的光诱导开关的光诱导控制信号。The two photoinduced switches are based on GaAs material. When photons with a certain energy are injected into the semiconductor of GaAs material, the photons absorbed inside the semiconductor will generate electron-hole pairs, and the internal resistance will change with the laser injection. change quickly. In this scheme, the input end is a bias high voltage, which provides high voltage electric field conditions to reduce the effective energy gap of the GaAs material with a bandgap width of 1.42eV. The 1064nm laser with photon energy of 1.16eV can be used as the light-induced switch of the GaAs material. Light-induced control signals.
光诱导开关5a、5b的光敏区分别在诱导激光脉冲信号4a、4b的照射下,电路将产生暂态响应,具体过程如下:当诱导激光脉冲4a对光诱导开关5a有效时,诱导激光脉冲4b对光诱导开关5b无效,此时光诱导开关5a开启,光诱导开关5b关闭,光诱导开关5a接通短路负载,即直接连接信号地7a,在输出耦合模块9输出反向波;当诱导激光脉冲4a对光诱导开关5a无效时,诱导激光脉冲4b对光诱导开关5b有效,此时光诱导开关5a关闭,光诱导开关5b开启,光诱导开关5b接通负载匹配模块6,并在输出耦合模块9输出正向波。如图2所示,11和12分别为产生的反方向波和正向波,13为正向波12相对于反向波11的时间延迟。The photosensitive areas of the photoinduced switches 5a and 5b are respectively irradiated by the induced laser pulse signals 4a and 4b, and the circuit will produce a transient response. The specific process is as follows: When the induced laser pulse 4a is effective for the photoinduced switch 5a, the induced laser pulse 4b It is invalid for the photo-induced switch 5b. At this time, the photo-induced switch 5a is turned on, and the photo-induced switch 5b is closed. When 4a is invalid for the photo-induced switch 5a, the induced laser pulse 4b is effective for the photo-induced switch 5b. At this time, the photo-induced switch 5a is closed, the photo-induced switch 5b is opened, and the photo-induced switch 5b is connected to the load matching module 6, and the output coupling module 9 Output positive wave. As shown in FIG. 2 , 11 and 12 are the generated reverse wave and forward wave respectively, and 13 is the time delay of the forward wave 12 relative to the reverse wave 11 .
诱导激光控制电路的调节使产生的两个诱导激光脉冲信号4a、4b之间的时间延迟达到亚纳秒级别,采用基于GaAs材料的光诱导开关时,光诱导开关具有非常高的速度、动态范围大、耐压高及响应稳定等特点,使产生的脉冲宽度可以达到皮秒精度,完全可以满足本方案设计要求。The adjustment of the induction laser control circuit makes the time delay between the generated two induction laser pulse signals 4a and 4b reach the sub-nanosecond level. When the optical induction switch based on GaAs material is used, the optical induction switch has a very high speed and dynamic range. Large, high withstand voltage and stable response, the generated pulse width can reach picosecond precision, which can fully meet the design requirements of this scheme.
通过改变两个诱导激光脉冲信号4a、4b的相对时间延迟,使得诱导激光脉冲信号产生的反向波与正向波之间的相对时间延迟也发生改变,将两个具有相对时间延迟输出的反向波进行部分重叠,通过控制诱导激光脉冲信号的时间延迟来控制两个反向波的重叠部分时间宽度,即控制合成的雷达信号波形由反向极小值到正向极大值的过渡时间,从而控制输出的雷达信号脉冲的宽度,即实现了输出高压脉冲雷达信号的脉宽可调。By changing the relative time delay of the two induced laser pulse signals 4a, 4b, the relative time delay between the reverse wave and the forward wave generated by the induced laser pulse signal is also changed, and the two reverse waves with relative time delay output Partially overlap the wave, and control the time width of the overlapping part of the two reverse waves by controlling the time delay of the induced laser pulse signal, that is, control the transition time of the synthesized radar signal waveform from the reverse minimum value to the positive maximum value , so as to control the pulse width of the output radar signal, that is, to realize the adjustable pulse width of the output high-voltage pulse radar signal.
为了进一步验证本发明所提出的技术方案可以实现所合成的雷达信号的脉宽可调,进行了该方案的仿真验证:In order to further verify that the technical scheme proposed by the present invention can realize the adjustable pulse width of the synthesized radar signal, the simulation verification of the scheme has been carried out:
如图2所示,通过调节两个脉冲之间的时间延迟13,在不同的时间延迟下,将反向波和正向波以一定的延迟合成,可以形成如图3所示的雷达信号波形,得到的雷达信号波形由反向极小值至正向极大值之间的过渡时间也相应的改变,对应频谱如图4所示。图3中,选用脉冲宽度τ=0.2ns的高斯脉冲作为模拟本实施方式所产生的高斯脉冲信号,控制正反两个高斯脉冲之间的相对时延分别为tshift=0.1ns,tshift=0.6ns,tshift=0.7ns。其中,图3中的编号与图4中编号一一对应,即图4中的各频谱波形分别是图3中的各个雷达信号的频谱。调节正向波与反向波之间的相对时间延迟,可以调节输出的雷达信号波形的中心频率。As shown in Figure 2, by adjusting the time delay 13 between the two pulses, under different time delays, the reverse wave and the forward wave are synthesized with a certain delay, and the radar signal waveform as shown in Figure 3 can be formed. The transition time between the obtained radar signal waveform from the reverse minimum value to the positive maximum value also changes accordingly, and the corresponding frequency spectrum is shown in Figure 4. In Fig. 3, select the Gaussian pulse of pulse width τ=0.2ns as the Gaussian pulse signal that this embodiment of simulation produces, control the relative time delay between two positive and negative Gaussian pulses respectively as t shift =0.1ns, t shift = 0.6 ns, t shift = 0.7 ns. Wherein, the numbers in FIG. 3 correspond to the numbers in FIG. 4 one by one, that is, each spectrum waveform in FIG. 4 is the spectrum of each radar signal in FIG. 3 . By adjusting the relative time delay between the forward wave and the reverse wave, the center frequency of the output radar signal waveform can be adjusted.
仿真验证结果证明,通过改变时间延迟可以很好地实现所合成的雷达信号波形的中心频率在一定频段范围内可调,从而使单一的探地雷达设备适应更多的探测场景。The simulation verification results prove that the center frequency of the synthesized radar signal waveform can be adjusted within a certain frequency range by changing the time delay, so that a single ground-penetrating radar device can adapt to more detection scenarios.
Claims (4)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610517141.XA CN106199535B (en) | 2016-07-04 | 2016-07-04 | It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610517141.XA CN106199535B (en) | 2016-07-04 | 2016-07-04 | It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106199535A CN106199535A (en) | 2016-12-07 |
CN106199535B true CN106199535B (en) | 2018-10-02 |
Family
ID=57465981
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201610517141.XA Active CN106199535B (en) | 2016-07-04 | 2016-07-04 | It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106199535B (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108519593B (en) * | 2018-03-22 | 2021-07-02 | 电子科技大学 | An asynchronous positioning method based on single-station dual-frequency continuous wave radar |
CN112666566B (en) * | 2021-01-14 | 2025-01-17 | 深圳市杉川机器人有限公司 | Laser radar ranging method and device, electronic equipment and storage medium |
CN115085700B (en) * | 2022-07-01 | 2024-04-19 | 中国人民解放军63660部队 | Solid-state pulse source output waveform delay control device and method |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3846645A (en) * | 1973-10-17 | 1974-11-05 | Westinghouse Electric Corp | Bi-polar pulse generator |
CN201528322U (en) * | 2009-09-25 | 2010-07-14 | 安徽华东光电技术研究所 | Full solid wide pulse floating-deck modulator |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100612820B1 (en) * | 2005-07-28 | 2006-08-21 | 한국전기연구원 | Unipolar and Bipolar Pulse Generators |
-
2016
- 2016-07-04 CN CN201610517141.XA patent/CN106199535B/en active Active
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3846645A (en) * | 1973-10-17 | 1974-11-05 | Westinghouse Electric Corp | Bi-polar pulse generator |
CN201528322U (en) * | 2009-09-25 | 2010-07-14 | 安徽华东光电技术研究所 | Full solid wide pulse floating-deck modulator |
Non-Patent Citations (2)
Title |
---|
"Ground penetrating radar enabled by high gain GaAs photoconductive semiconductor switches";GM Loubriel等;《Office of scientific and technical information technical reports》;19971231;第17-24页 * |
"雪崩晶体管在探底雷达中的应用";张瑜等;《微计算机信息》;20081231;第24卷(第14期);第270-272页 * |
Also Published As
Publication number | Publication date |
---|---|
CN106199535A (en) | 2016-12-07 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN106199535B (en) | It is a kind of to switch the method and device for generating high-voltage pulse radar signal based on photoinduction | |
CN102121983A (en) | Ultra-wideband radar pulse transmitter and method | |
Çetin et al. | An experimental study of high precision TOA based UWB positioning systems | |
Pi et al. | A Marx-based Gaussian monocycle pulse generator with low ringing level for ground penetrating radar applications | |
Tajfar et al. | A 20 a sub-nanosecond integrated CMOS laser diode driver for high repetition rate SPAD-based direct Time-of-Flight measurements | |
Lalande et al. | An ultra wideband impulse optoelectronic radar: RUGBI | |
CN207318704U (en) | A kind of high-amplitude picosecond micropower UWB radar clock generates system | |
CN117254792A (en) | Gaussian monopulse generation circuit based on SRD | |
Xia et al. | A monocycle pulse generator with variable capacitance diodes for radar target detecting application | |
Ameri et al. | Balanced pulse generator for UWB radar application | |
Wang et al. | Design of Impulse Ground Penetrating Radar Signal Source Based on Power Synthesis | |
Li et al. | Design of Nanosecond Pulse Laser Diode Array Driver Circuit for LiDAR. | |
CN108872716B (en) | Device and method for enhancing laser-induced air plasma microwave radiation by external magnetic field | |
Hu et al. | Radiation simulation on satellite navigation antenna by strong electromagnetic pulse | |
CN107329118A (en) | A kind of high-amplitude picosecond micropower UWB radar detection system | |
CN106953619A (en) | Subperiod Microwave Pulse Sequence Generator for Cold Atom Quantum State Manipulation | |
Zhao et al. | Design of picosecond level short pulse based on dual NOT gates structure | |
CN203135817U (en) | High power ultra wideband signal generator | |
Labate et al. | High-speed photoconductive switches at high voltage bias in radar systems | |
Zhi-yuan et al. | A digital pulse drive circuit for continuously modulated semiconductor laser | |
Gao et al. | Performance improvement for sub-nanosecond Marx generator based on avalanche transistors by considering the traveling wave process | |
Dou | The design of radiating circuit for ultra-wideband ground penetrating radar | |
Kumar et al. | A review on impulse RADAR | |
Tian et al. | Impulse generator using UWB pulse forming network | |
Li et al. | The interval modulation system for the ultra-wideband vehicular radar |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |