CN201159766Y - High-precision speed-measuring and ranging laser radar system - Google Patents
High-precision speed-measuring and ranging laser radar system Download PDFInfo
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- CN201159766Y CN201159766Y CNU2008200560037U CN200820056003U CN201159766Y CN 201159766 Y CN201159766 Y CN 201159766Y CN U2008200560037 U CNU2008200560037 U CN U2008200560037U CN 200820056003 U CN200820056003 U CN 200820056003U CN 201159766 Y CN201159766 Y CN 201159766Y
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Abstract
Disclosed is a high accuracy laser radar system for measuring speed and distance, which is composed of a laser device, a linear chirp modulator, a pseudo-random code modulator, an acoustooptic modulator, an arbitrary waveform generator, an acoustooptic modulator driving device, a first coupler, a second coupler, a circulator, a telescope, a coherent detection and pulse compression device, a single-photon detector, a single-photon counter and a computer. The utility module has the advantage of accurately obtaining the speed and distance information of the target.
Description
Technical field
The utility model patent relates to laser radar, particularly a kind of high precision speed-measuring range laser radar system, it is a kind of system that utilizes pseudo-random code modulation technique, photon counting technique, coherent detection technology and pulse compression technique that unites, and can high precision obtains the speed and the range information of target.
Background technology
Aircraft needs accurate speed and the positional information that must know oneself when landing.Like this safe landing had key effect.Especially the landing face that has remarkable uncontinuity, for example moon.And commonly used pass through the method that measuring distance obtains range derivative speed again, because the uncontinuity of distance can not obtain correct velocity information.And echoed signal is cut into a plurality of little time periods, obtain velocity information by the Doppler shift of measuring each time period, again according to the time period moment corresponding come computed range information method, can not obtain high-resolution range information.
Summary of the invention
The problem that the utility model patent will solve is to overcome the deficiency of above existing method, and a kind of high precision speed-measuring range laser radar system is provided, and this system can provide high-accuracy speed information and range information.
Ultimate principle of the present utility model is that laser is modulated through linear chrip modulation and pseudo-random code, and the laser overwhelming majority after the modulation is launched by telescope as shoot laser; Sub-fraction is used for coherent detection as local oscillator light; Laser echo signal is divided into two parts: a part obtains range information by carrying out related calculation with original pseudo-random code; Another part carries out pulse compression by doing coherent detection with local oscillator light, obtains local oscillator light and the echoed signal light frequency is poor, and this difference on the frequency comprises range information and Doppler shift simultaneously; Obtain Doppler shift by mathematical operation, thereby can high precision obtain the speed and the range information of target.
Technical solution of the present utility model is as follows:
A kind of high precision speed-measuring range laser radar system, comprise laser instrument and telescope, be characterized on the optical axis of the output beam of described laser instrument, being provided with the linear chrip modulator successively, the pseudo-random code modulator and first coupling mechanism, first output terminal of this first coupling mechanism links to each other with first port of circulator, the outbound course of second port of this circulator is a telescope, second output terminal of first coupling mechanism links to each other through the first input end of acousto-optic modulator with coherent detection and compression device, the 3rd port of described circulator connects the input end of second coupling mechanism, this second coupling mechanism, first output terminal links to each other with second input end of described coherent detection and compression device, second output terminal of this second coupling mechanism connects behind single-photon detector and single photon counter has signals collecting, handle, control, the computing machine of calculating and Presentation Function, the described computing machine of output termination of described coherent detection and compression device, three output terminals of one AWG (Arbitrary Waveform Generator) connect described linear chrip modulator respectively, pseudo-random code modulator and computing machine, for described linear chrip modulator provides drive signal, for described pseudo-random code modulator and computing machine provide pseudo-random code, an acoustooptic modulator driver provides the acousto-optic modulator drive signal for acousto-optic modulator and described coherent detection and compression device.
Described coherent detection and compression device are by the 3rd coupling mechanism, the balance detection device, 90 ° of phase shifters, first multiplier, second multiplier, first low-pass filter, second low-pass filter is formed, described the 3rd coupling mechanism is the 3dB photo-coupler, have two input ends, two output terminals, two input ends are respectively the first input end and second input end of this coherent detection and compression device, two input ends of the described balance detection device of described two output terminations, the electric signal of this balance detection device output and the drive signal of described acoustooptic modulator driver are mixed in described first multiplier, and the output signal of described first multiplier obtains signal I through behind described first low-pass filter; The drive signal of described acoustooptic modulator driver is after 90 ° of described 90 ° of phase shifter phase shifts, mix in second multiplier with the electric signal of described balance detection device output, the output signal of described second multiplier obtains signal Q through behind described second low-pass filter, and the spectrum peak expression formula of signal I and signal Q is f
0=kt-f
d, wherein: k is the linear chrip modulation rate, unit is a hertz per second, f
dBe Doppler frequency.
Described laser instrument is a single-longitudinal-mode fiber laser.
Described linear chrip modulator is the lithium niobate intensity modulator.
Described described pseudo-random code modulator is a high-speed electro-optic modulator.
Described described telescope is the telescopic system that transmits and receives common optical axis.
Advantage of the present utility model is
1, adopt fiber laser, ripe optical fibre device and full optical fiber optical optical road to connect, electrical efficiency height, power consumption are little, light weight, be easy to connect, system stability is reliable
2, adopted modulation of high speed pseudo-random code and photon counting technique, enough signal to noise ratio (S/N ratio)s have been arranged even under low peak power echoed signal, also can guarantee each the measurement.Modulation rate can reach 1GHz, and promptly the pseudo-random code Baud Length is 1ns, and range resolution can reach 15cm like this.
3, coherent detection and pulse compression mechanism have been adopted.Adopt coherent detection, amplified the power of echoed signal effectively, make this part of system's coherent detection can be operated in the quantum noise limit, obtain more high s/n ratio than direct detection; Pulse compression mechanism again with the concentration of energy of broadband signal on simple signal, promptly on frequency domain, realized pulse compression.Coherent detection mechanism and pulse compression mechanism are used simultaneously and can be made velocity resolution reach the 1cm/s magnitude.
4, local oscillation signal and telescope outgoing signal have all passed through linear chrip modulation and pseudo-random code modulation, separate timing at coherent detection like this, have saved this step of demodulation of warbling, and have simplified system.
5, range sensing and speed detection are not discrete two-way, and these two parts are related, and the utility model can obtain the speed and the range information of target simultaneously accurately.。
Description of drawings
Fig. 1 is the utility model high precision speed-measuring range laser radar entire system structured flowchart
Fig. 2 is the utility model Coherent Detection, pulse compression part-structure block diagram
Among the figure: the 1-laser instrument, 2-linear chrip modulator, 3-pseudo-random code modulator, 4-first coupling mechanism, the 5-circulator, the 6-telescope, the 7-acousto-optic modulator, 8-second coupling mechanism, 9-coherent detection and compression device, the 10-single-photon detector, the 11-single photon counter, the 12-computing machine, the 13-acousto-optic modulator drives, the 14-AWG (Arbitrary Waveform Generator), 91-the 3rd coupling mechanism, 92-balance detection device, 93-90 ° of phase shifter, the 94-multiplier, the 95-multiplier, the 96-low-pass filter, the 97-low-pass filter;
Embodiment
The utility model is described in further detail below in conjunction with embodiment and accompanying drawing, but should not limit protection domain of the present utility model with this.
At first please refer to Fig. 1, Fig. 1 is the utility model high precision speed-measuring range laser radar entire system structured flowchart.As seen from Figure 1, the utility model high precision speed-measuring range laser radar system is by laser instrument 1, linear chrip modulator 2, pseudo-random code modulator 3, acousto-optic modulator 7, AWG (Arbitrary Waveform Generator) 14, acoustooptic modulator driver 13, first coupling mechanism, 4, the second coupling mechanisms 8, circulator 5, telescope 6, coherent detection and compression device 9, single-photon detector 10, single photon counter 11, and the computing machine 12 with signal Processing, control, calculating, collection, Presentation Function is formed.Its position relation is: be provided with linear chrip modulator 2, pseudo-random code modulator 3, first coupling mechanism 4 on the output beam optical axis of described laser instrument 1 successively.Described first coupling mechanism 4 is divided into two laser: wherein most of light is gone out Laser emission through circulator 5 and telescope 6; Another fraction light is used for coherent detection through acousto-optic modulator 7 as local oscillator light.Described telescope 6 is collected echoed signal, and echoed signal enters second coupling mechanism 8 through circulator 5.This second coupling mechanism 8 is two with the echoed signal portion: wherein sub-fraction obtains comprising the mixed information of distance and speed through coherent detection and compression device 9; Another is most of through entering computing machine 12 behind single-photon detector 10, the single photon counter 11, and the original pseudo-random code that provides with AWG (Arbitrary Waveform Generator) 14 in computing machine 12 carries out related calculation.Related operation peak value moment corresponding has been represented range information.Comprehensive this two parts information can obtain range information and velocity information respectively.
The concrete device that present embodiment adopts is: described laser instrument 1 is single-longitudinal-mode fiber laser; Described linear chrip modulator 2 is the lithium niobate intensity modulator; Described pseudo-random code modulator 3 is a high-speed electro-optic modulator; Described AWG (Arbitrary Waveform Generator) 14 contains two output channels, and linear chrip modulator 2 and pseudo-random code modulator 3 provide drive signal respectively.For described computing machine 12 provides pseudo-random code; Described first coupling mechanism 4 is 1: 99 a photo-coupler.Wherein 1% light is as local oscillator light; 99% light passes through telescope 6 with laser emitting; Described second coupling mechanism 8 is 20: 80 photo-couplers.Output is divided into two-way, and wherein 20% as coherent detection and pulse compression, and 80% as related operation; Described telescope 6 is the telescopic systems that transmit and receive common optical axis.
Described coherent detection and compression device 9 are by the 3rd coupling mechanism 91, balance detection device 92,90 ° of phase shifters 93, first multiplier 94, second multiplier 95, first low-pass filter 96, second low-pass filter 97 is formed, described the 3rd coupling mechanism 91 is the 3dB photo-coupler, have two input ends, two output terminals, two input ends are respectively the first input end and second input end of this coherent detection and compression device 9,90 ° of the phase phasic differences of two output signals, two input ends of the described balance detection device 92 of described two output terminations, the electric signal of these balance detection device 92 outputs and the drive signal of described acoustooptic modulator driver 13 are mixed in described first multiplier 94, and the output signal of described first multiplier 94 obtains signal I through behind described first low-pass filter 96; The drive signal of described acoustooptic modulator driver 13 is after 90 ° of described 90 ° of phase shifters, 93 phase shifts, mix in second multiplier 95 with the electric signal of described balance detection device 92 outputs, the output signal of described second multiplier 95 obtains signal Q through behind described second low-pass filter 97, and the spectrum peak expression formula of signal I and signal Q is f
0=kt-f
d, wherein: k is the linear chrip modulation rate, unit is a hertz per second, f
dBe Doppler frequency.
The utility model embodiment high precision speed-measuring range laser radar system test the speed the range finding detailed process be:
1. laser instrument 1 output laser is divided into two parts through linear chrip modulator 2 and pseudo-random code modulator 3 modulation backs by first photo-coupler 4 successively: 99% laser by first output terminal of first photo-coupler 4 through described circulator 5 first ports enter described circulator 5 and through second port output of this circulator 5 by described telescope 6 emissions, 1% laser through behind described acousto-optic modulator 7 shift frequencies as local oscillator light;
2. described telescope 6 receiving target echoed signal light, enter described circulator 5 and enter second coupling mechanism 8 by described circulator 5 the 3rd port through the 3rd port of this circulator 5, second coupling mechanism 8 is divided into two echoed signal light: the signal of the second defeated end output 80% of second coupling mechanism (8) enters computing machine 12 behind single-photon detector 10 and single photon counter 11, the original pseudo-random code that provides with AWG (Arbitrary Waveform Generator) 14 in computing machine 12 carries out related calculation, and the corresponding relation of related operation peak value moment corresponding t and target distance L of living in is
Wherein c is the light velocity;
3. the signal of first output terminal of second coupling mechanism 8 output 20% is used for doing coherent detection and pulse compression with local oscillator light at coherent detection and compression device 9, forms signal I and signal Q;
4. 12 couples of signal I of described computing machine and signal Q gather and do Fourier transform respectively, obtain FFTI, FFTQ, the signal behind these two Fourier transforms are combined into a way word signal FFTI again
2+ FFTQ
2The frequency of this digital signal peak value correspondence has comprised range information and velocity information.This digital signal FFTI
2+ FFTQ
2Crest frequency f=2 (kt-f
d), wherein k is the linear chrip modulation rate, unit is a hertz per second, f
dBe Doppler frequency, Doppler frequency and be parallel to aircraft and the target velocity v of target link between corresponding relation be
λ is the output wavelength of laser instrument;
5. described computing machine 12 comprehensive above-mentioned the 2. with the 4. result in step, obtain target velocity:
Claims (5)
1, a kind of high precision speed-measuring range laser radar system, comprise laser instrument (1) and telescope (6), it is characterized in that on the optical axis of the output beam of described laser instrument (1), being provided with linear chrip modulator (2) successively, pseudo-random code modulator (3) and first coupling mechanism (4), first output terminal of this first coupling mechanism (4) links to each other with first port of circulator (5), the outbound course of second port of this circulator (5) is telescope (6), second output terminal of first coupling mechanism (4) links to each other with the first input end of coherent detection with compression device (9) through acousto-optic modulator (7), the 3rd port of described circulator (5) connects the input end of second coupling mechanism (8), these second coupling mechanism (8) first output terminals link to each other with second input end of described coherent detection with compression device (9), second output terminal of this second coupling mechanism (8) connects behind single-photon detector (10) and single photon counter (11) has signals collecting, handle, control, the computing machine (12) of calculating and Presentation Function, the described computing machine of output termination (12) of described coherent detection and compression device (9), three output terminals of one AWG (Arbitrary Waveform Generator) (14) connect described linear chrip modulator (2) respectively, pseudo-random code modulator (3) and computing machine (12), for described linear chrip modulator (2) provides drive signal, for described pseudo-random code modulator (3) and computing machine (12) provide pseudo-random code, an acoustooptic modulator driver (13) provides the acousto-optic modulator drive signal for acousto-optic modulator (7) and described coherent detection and compression device (9).
2, high precision speed-measuring range laser radar according to claim 1 system, it is characterized in that described coherent detection and compression device (9) are by the 3rd coupling mechanism (91), balance detection device (92), 90 ° of phase shifters (93), first multiplier (94), second multiplier (95), first low-pass filter (96), second low-pass filter (97) is formed, described the 3rd coupling mechanism (91) is the 3dB photo-coupler, have two input ends, two output terminals, two input ends are respectively the first input end and second input end of this coherent detection and compression device (9), two input ends of the described two output described balance detection devices of termination (92), the electric signal of this balance detection device (92) output and the drive signal of described acoustooptic modulator driver (13) are mixed in described first multiplier (94), obtain signal I behind output signal described first low-pass filter of process (96) of described first multiplier (94); The drive signal of described acoustooptic modulator driver (13) is after 90 ° of described 90 ° of phase shifters (93) phase shifts, mix in second multiplier (95) with the electric signal of described balance detection device (92) output, obtain signal Q behind output signal described second low-pass filter of process (97) of described second multiplier (95), the spectrum peak expression formula of signal I and signal Q is f
0=kt-f
d, wherein: k is the linear chrip modulation rate, unit is a hertz per second, f
dBe Doppler frequency.
3, high precision speed-measuring range laser radar according to claim 1 system is characterized in that described laser instrument (1) is a single-longitudinal-mode fiber laser.
4, high precision speed-measuring range laser radar according to claim 1 system is characterized in that described linear chrip modulator (2) is the lithium niobate intensity modulator.
5, high precision speed-measuring range laser radar according to claim 1 system is characterized in that described described pseudo-random code modulator (3) is a high-speed electro-optic modulator.
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| CNU2008200560037U CN201159766Y (en) | 2008-03-07 | 2008-03-07 | High-precision speed-measuring and ranging laser radar system |
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| CNU2008200560037U CN201159766Y (en) | 2008-03-07 | 2008-03-07 | High-precision speed-measuring and ranging laser radar system |
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Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101788671B (en) * | 2010-02-09 | 2012-08-01 | 中国科学院上海技术物理研究所 | Multicycle modulation method applied to laser ranging device using chirp amplitude modulation based on heterodyne detection |
| CN103472458A (en) * | 2013-09-16 | 2013-12-25 | 中国科学院上海光学精密机械研究所 | Three-dimensional video laser radar system based on acousto-optic scanning |
| CN105425244A (en) * | 2015-12-16 | 2016-03-23 | 哈尔滨工业大学 | Front mixing chirp modulation photon counting laser radar |
| CN105438912A (en) * | 2016-01-28 | 2016-03-30 | 中国人民解放军信息工程大学 | Position monitoring method and system |
| CN106093962A (en) * | 2016-08-03 | 2016-11-09 | 中国工程物理研究院流体物理研究所 | A kind of interference velocity-measuring system and method |
| CN108089194A (en) * | 2017-12-15 | 2018-05-29 | 中国科学院光电技术研究所 | A kind of photon counting laser radar based on compound pseudorandomcode |
| RU2690990C2 (en) * | 2017-06-09 | 2019-06-07 | Общество с ограниченной ответственностью НаноРельеф Дисплей | Lidar without moving parts |
| CN110161520A (en) * | 2019-06-11 | 2019-08-23 | 中国科学院光电技术研究所 | A kind of photon counting coherent laser radar based on compression sampling technology |
| CN110471079A (en) * | 2019-09-25 | 2019-11-19 | 浙江缔科新技术发展有限公司 | A kind of light quantum tests the speed telescope and speed-measuring method |
| CN111198378A (en) * | 2019-12-27 | 2020-05-26 | 深圳市优必选科技股份有限公司 | Boundary-based autonomous exploration method and device |
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- 2008-03-07 CN CNU2008200560037U patent/CN201159766Y/en not_active Expired - Fee Related
Cited By (16)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN101788671B (en) * | 2010-02-09 | 2012-08-01 | 中国科学院上海技术物理研究所 | Multicycle modulation method applied to laser ranging device using chirp amplitude modulation based on heterodyne detection |
| CN103472458A (en) * | 2013-09-16 | 2013-12-25 | 中国科学院上海光学精密机械研究所 | Three-dimensional video laser radar system based on acousto-optic scanning |
| CN103472458B (en) * | 2013-09-16 | 2015-04-15 | 中国科学院上海光学精密机械研究所 | Three-dimensional video laser radar system based on acousto-optic scanning |
| CN105425244B (en) * | 2015-12-16 | 2018-04-27 | 哈尔滨工业大学 | The chirped modulation photon counting laser radar of preposition mixing |
| CN105425244A (en) * | 2015-12-16 | 2016-03-23 | 哈尔滨工业大学 | Front mixing chirp modulation photon counting laser radar |
| CN105438912B (en) * | 2016-01-28 | 2018-07-13 | 中国人民解放军信息工程大学 | A kind of position monitoring method and system |
| CN105438912A (en) * | 2016-01-28 | 2016-03-30 | 中国人民解放军信息工程大学 | Position monitoring method and system |
| CN106093962A (en) * | 2016-08-03 | 2016-11-09 | 中国工程物理研究院流体物理研究所 | A kind of interference velocity-measuring system and method |
| RU2690990C2 (en) * | 2017-06-09 | 2019-06-07 | Общество с ограниченной ответственностью НаноРельеф Дисплей | Lidar without moving parts |
| CN108089194A (en) * | 2017-12-15 | 2018-05-29 | 中国科学院光电技术研究所 | A kind of photon counting laser radar based on compound pseudorandomcode |
| CN110161520A (en) * | 2019-06-11 | 2019-08-23 | 中国科学院光电技术研究所 | A kind of photon counting coherent laser radar based on compression sampling technology |
| CN110161520B (en) * | 2019-06-11 | 2022-11-08 | 中国科学院光电技术研究所 | Photon counting coherent laser radar based on compressive sampling technology |
| CN110471079A (en) * | 2019-09-25 | 2019-11-19 | 浙江缔科新技术发展有限公司 | A kind of light quantum tests the speed telescope and speed-measuring method |
| CN110471079B (en) * | 2019-09-25 | 2023-07-11 | 浙江缔科新技术发展有限公司 | Light quantum speed measuring telescope and speed measuring method |
| CN111198378A (en) * | 2019-12-27 | 2020-05-26 | 深圳市优必选科技股份有限公司 | Boundary-based autonomous exploration method and device |
| CN111198378B (en) * | 2019-12-27 | 2022-06-28 | 深圳市优必选科技股份有限公司 | Boundary-based autonomous exploration method and device |
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