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CN110098556A - A kind of 828nm atmosphere vapour detection differential absorption lidar transmitter system - Google Patents

A kind of 828nm atmosphere vapour detection differential absorption lidar transmitter system Download PDF

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CN110098556A
CN110098556A CN201910414302.6A CN201910414302A CN110098556A CN 110098556 A CN110098556 A CN 110098556A CN 201910414302 A CN201910414302 A CN 201910414302A CN 110098556 A CN110098556 A CN 110098556A
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water vapor
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洪光烈
李嘉唐
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Shanghai Institute of Technical Physics of CAS
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO 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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/483Details of pulse systems
    • G01S7/484Transmitters
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/081Construction or shape of optical resonators or components thereof comprising three or more reflectors
    • H01S3/083Ring lasers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1303Stabilisation of laser output parameters, e.g. frequency or amplitude by using a passive reference, e.g. absorption cell
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/1305Feedback control systems

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  • Radar, Positioning & Navigation (AREA)
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  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Abstract

本发明公开了一种828nm大气水汽探测差分吸收激光雷达发射机系统,包括828nm连续波种子激光器,单纵模窄线宽脉冲Nd:YAG激光器,KTP环形腔光参量振荡器,基于水汽吸收的多通道吸收池的PDH种子激光波长稳定单元,基于扫描保持技术的光参量振荡器谐振腔腔长锁定单元。本发明能够产生适用于大气水汽探测的单频激光脉冲,是差分吸收激光雷达的核心结构。

The invention discloses an 828nm atmospheric water vapor detection differential absorption laser radar transmitter system, which includes an 828nm continuous wave seed laser, a single longitudinal mode narrow line width pulse Nd:YAG laser, a KTP ring cavity optical parametric oscillator, and a multi-channel laser based on water vapor absorption. The PDH seed laser wavelength stabilization unit of the channel absorption cell, and the optical parametric oscillator resonator cavity length locking unit based on scan-and-hold technology. The invention can generate single-frequency laser pulses suitable for atmospheric water vapor detection, and is the core structure of the differential absorption laser radar.

Description

一种828nm大气水汽探测差分吸收激光雷达发射机系统An 828nm Atmospheric Water Vapor Detection Differential Absorption LiDAR Transmitter System

技术领域technical field

本发明涉及激光雷达遥感测量领域,也涉及一种地基或车载的大气水汽遥感仪器,尤其是一种探测大气水汽分布、工作在828nm波段的差分吸收激光雷达的发射机系统。The invention relates to the field of laser radar remote sensing measurement, and also relates to a ground-based or vehicle-mounted atmospheric water vapor remote sensing instrument, in particular to a differential absorption laser radar transmitter system that detects atmospheric water vapor distribution and works in the 828nm band.

背景技术Background technique

激光雷达是以发射激光束来探测目标特征量的光学主动遥感设备,目前已成为探测大气成分及其垂直分布的最有效的手段之一。发射机发出5至200ns的超短激光脉冲,进入大气后在行进过程中不断与大气中的待测物质发生相互作用,其后向Raman散射、后向Mie散射和后向Rayleigh散射均可作为回波信号被望远镜接收,由光电探测器检测转换成电压信号送给模数转换器件以便于后续的信号处理与反演工作。Lidar is an optical active remote sensing device that emits laser beams to detect target feature quantities. It has become one of the most effective means to detect atmospheric composition and its vertical distribution. The transmitter emits ultra-short laser pulses of 5 to 200 ns, and after entering the atmosphere, it continuously interacts with the substances to be measured in the atmosphere during its travel, and the back Raman scattering, back Mie scattering and back Rayleigh scattering can all be used as echoes. The wave signal is received by the telescope, detected by the photodetector and converted into a voltage signal, which is sent to the analog-to-digital conversion device for subsequent signal processing and inversion.

上世纪80年代以来,国际上相继建立基于多种平台探测对流层大气水汽廓线的差分吸收激光雷达。因为大气水汽主要集中在大气边界层,根据国际经验,机载和空间应用的差分吸收激光雷达,发射激光束由高层大气向低层大气传输,光束下行的路径上水汽浓度由低到高,对激光的吸收由弱到强,一般认为此时水汽对发射激光的吸收截面相对大些更为适宜;地基和车载差分吸收激光雷达探测由地表起至对流层顶的大气水汽含量,一般采用吸收截面相对小的815-820nm附近或720-730nm附近波段。Since the 1980s, differential absorption lidars based on various platforms to detect tropospheric atmospheric water vapor profiles have been successively established internationally. Because atmospheric water vapor is mainly concentrated in the atmospheric boundary layer, according to international experience, the differential absorption lidar for airborne and space applications transmits the laser beam from the upper atmosphere to the lower atmosphere, and the water vapor concentration on the downward path of the beam changes from low to high. The absorption ranges from weak to strong. It is generally believed that it is more appropriate for water vapor to absorb a larger cross-section of the emitted laser light at this time; the ground-based and vehicle-mounted differential absorption lidar detects the atmospheric water vapor content from the surface to the tropopause, and generally uses a relatively small absorption cross-section. near 815-820nm or near 720-730nm.

国际上已经建立的探测对流层水汽的地基差分吸收激光雷达发射机系统主要分为两大类,一类以低重复频率、大脉冲能量构建,如使用钛宝石激光器或翠绿宝石激光器。钛宝石激光器发射机采用了种子注入和谐振腔主动稳频技术,发射机的光谱性能较稳定,波长一般靠近钛宝石增益较高的波长815-820nm;翠绿宝石激光器一般工作在720-730nm的水汽吸收区,但在720-730nm波段大气分子后向散射产生的谱线展宽严重,反演误差增大。另一类使用重复频率高,脉冲能量很低的发射机,以二极管激光器和半导体放大器为核心,工作波长为823、828nm,这类激光雷达称之为微脉冲差分吸收激光雷达。The ground-based differential absorption lidar transmitter systems that have been established internationally to detect tropospheric water vapor are mainly divided into two categories. One is built with low repetition rate and large pulse energy, such as using titanium sapphire laser or alexandrite laser. The Ti:Sapphire laser transmitter adopts seed injection and resonant cavity active frequency stabilization technology. The spectral performance of the transmitter is relatively stable. The wavelength is generally close to the wavelength of 815-820nm with higher Ti:Sapphire gain; the alexandrite laser generally works in the water vapor of 720-730nm However, in the 720-730nm band, the spectral line broadening caused by the backscattering of atmospheric molecules is serious, and the inversion error increases. Another type of transmitter uses a high repetition rate and low pulse energy, with a diode laser and a semiconductor amplifier as the core, and an operating wavelength of 823 and 828nm. This type of lidar is called a micropulse differential absorption lidar.

随着光参量振荡器技术不断进步和窄线宽单纵模Nd:YAG激光器的不断成熟,基于种子注入的光参量振荡器方法可以产生优良的828nm-828nm激光束,覆盖水汽的一个吸收光谱区,因而可以用作地基或车载差分吸收激光雷达探测大气对流层水汽廓线的激光发射机。With the continuous advancement of optical parametric oscillator technology and the continuous maturity of narrow linewidth single longitudinal mode Nd:YAG lasers, the optical parametric oscillator method based on seed injection can generate excellent 828nm-828nm laser beams, covering an absorption spectral region of water vapor , so it can be used as a laser transmitter for ground-based or vehicle-mounted differential absorption lidar to detect the water vapor profile of the atmospheric troposphere.

发明内容Contents of the invention

本发明旨在提出一种工作在820~830nm波段的差分吸收激光雷达的发射机系统,这样做的目的在于进一步丰富用于水汽探测的差分吸收激光雷达构建手段,增强差分吸收激光雷达应用的普遍性。The purpose of this invention is to propose a transmitter system for differential absorption lidar operating in the 820-830nm band. The purpose of doing so is to further enrich the construction means of differential absorption lidar for water vapor detection and enhance the universality of differential absorption lidar applications. sex.

所述激光雷达发射机系统包括单频泵浦激光器1、主动稳频的828nm种子激光器2、环形腔光参量振荡器3以及必要的光学镜片4~7,整体结构如图1所示。其中,采用种子注入的Nd:YAG激光器作为泵浦源,包括1064nm Nd:YAG光放大器1-1、二倍频晶体1-2、1064nmNd:YAG主振荡器1-3、1064nm种子源1-4。单频泵浦激光器1产生泵浦激光,到达R1064T532介质膜双色镜4时的泵浦激光同时包含1064nm成分和532nm成分。R1064T532介质膜双色镜4镀532nm减反射膜和1064nm高反射膜,使得532nm激光透过4进入环形腔光参量振荡器3,1064nm反射至1064nm反射镜5,并被5再次反射至R532T1064介质膜双色镜6。R532T1064介质膜双色镜6镀1064nm减反射膜和532nm高反射膜,使得1064nm透过6被释放掉。由环形腔光参量振荡器3出射的激光同时包含828nm成分和532nm成分,R532T828介质膜双色镜7镀828nm减反射膜和532nm高反射膜,使得828nm激光透过7进行发射,532nm激光被7反射至R532T1064介质膜双色镜6,并被6再次反射释放。The lidar transmitter system includes a single-frequency pump laser 1, an active frequency-stabilized 828nm seed laser 2, a ring cavity optical parametric oscillator 3, and necessary optical lenses 4-7. The overall structure is shown in FIG. 1 . Among them, the seed-injected Nd:YAG laser is used as the pump source, including 1064nm Nd:YAG optical amplifier 1-1, double frequency crystal 1-2, 1064nm Nd:YAG main oscillator 1-3, 1064nm seed source 1-4 . The single-frequency pump laser 1 generates pump laser light, and the pump laser light when it reaches the R1064T532 dielectric film dichroic mirror 4 contains both 1064nm components and 532nm components. R1064T532 dielectric film dichroic mirror 4 is coated with 532nm antireflection film and 1064nm high reflection film, so that 532nm laser light passes through 4 and enters ring cavity optical parametric oscillator 3, 1064nm is reflected to 1064nm mirror 5, and is reflected by 5 again to R532T1064 dielectric film bichromatic Mirror 6. The R532T1064 dielectric film dichroic mirror 6 is coated with 1064nm antireflection coating and 532nm high reflection coating, so that 1064nm can be released through 6. The laser emitted by the ring cavity optical parametric oscillator 3 contains both 828nm and 532nm components. R532T828 dielectric film dichroic mirror 7 is coated with 828nm anti-reflection film and 532nm high-reflection film, so that 828nm laser is emitted through 7, and 532nm laser is reflected by 7 to the R532T1064 dielectric film dichroic mirror 6, and is reflected by 6 again for release.

所述激光雷达发射机系统使用主动稳频的828nm种子激光器2作为光参量振荡器注入种子源,如图3,包括828nm DFB激光器2-1、95:5光纤分路器2-2、水汽吸收池2-3、气体池光电探测器2-4、种子光控制电子单元2-5。种子光的波长以水汽标准吸收池的光吸收率曲线中心极小值频率ω0作为参照标准,如图2,使用PDH(Pound–Drever–Hall)稳频技术稳定种子源波长。The laser radar transmitter system uses an active frequency-stabilized 828nm seed laser 2 as an optical parametric oscillator to inject the seed source, as shown in Figure 3, including 828nm DFB laser 2-1, 95:5 fiber splitter 2-2, water vapor absorption Cell 2-3, gas cell photodetector 2-4, seed light control electronics unit 2-5. The wavelength of the seed light is based on the minimum value frequency ω 0 in the center of the light absorptivity curve of the water vapor standard absorption cell as a reference standard, as shown in Figure 2, using the PDH (Pound–Drever–Hall) frequency stabilization technology to stabilize the seed source wavelength.

对连续波种子激光频率ω进行电光相位调制,入射到水汽多通道吸收池之前被相位调制的电场变为Electro-optic phase modulation is performed on the continuous wave seed laser frequency ω, and the phase-modulated electric field before entering the water vapor multi-channel absorption cell becomes

Einc=E0ei(ωt+msinδt)≈E0[J0(m)eiωt+J1(m)ei(ω+δ)t-J1(m)ei(ω-δ)t] (1)E inc =E 0 e i(ωt+msinδt) ≈E 0 [J 0 (m)e iωt +J 1 (m)e i(ω+δ)t -J 1 (m)e i(ω-δ) t ] (1)

其中m是相位调制的深度,δ调制波的频率,msinδt即为相位调制项。被调制的连续激光分裂成三个频谱,分别为中心频率分量载波J0(m)eiωt,以及分布在中心频率两侧、幅度相等且相位相反的两个边带。当种子光频率ω对准参考水汽多通道吸收池的中心频率ω0时,水汽吸收之后的上下边带与载波拍频电流大小相等且相位相反,探测器输出Pcoherent为零;反之,种子光频率ω与水汽多通道吸收池的中心频率ω0不等时,两侧边带经过水汽多通道吸收池的吸收之后其反对称性被破坏,上下边带与载波拍频电流不再抵消,此时探测器输出Pcoherent与原射频调制信号sinδt相混频,并进行低通滤波之后,即得到含有种子激光频率与水汽多通道吸收池的中心频率偏差信息。后级PID伺服控制系统根据此偏差信息反馈控制种子激光器的注入电流和压电电压,从而实现种子激光器的频率ω向水汽多通道吸收池的中心频率ω0逼近。Among them, m is the depth of phase modulation, the frequency of δ modulation wave, and msinδt is the phase modulation term. The modulated CW laser is split into three frequency spectra, namely the center frequency component carrier J 0 (m)e iωt , and two sidebands distributed on both sides of the center frequency with equal amplitude and opposite phase. When the seed light frequency ω is aligned with the center frequency ω 0 of the reference water vapor multi-channel absorption cell, the upper and lower sidebands after water vapor absorption are equal in size and opposite to the carrier beat frequency current, and the detector output P coherent is zero; otherwise, the seed light When the frequency ω is not equal to the center frequency ω 0 of the water vapor multi-channel absorption cell, the antisymmetry of the sidebands on both sides is destroyed after being absorbed by the water vapor multi-channel absorption cell, and the upper and lower sidebands and the carrier beat frequency current no longer cancel each other out. When the detector output P coherent is mixed with the original radio frequency modulation signal sinδt, and after low-pass filtering, the center frequency deviation information containing the seed laser frequency and the water vapor multi-channel absorption cell is obtained. The post-stage PID servo control system feeds back and controls the injection current and piezoelectric voltage of the seed laser according to the deviation information, so that the frequency ω of the seed laser approaches the center frequency ω 0 of the water vapor multi-channel absorption pool.

所述激光雷达发射机系统使用的产生单频828nm波长激光的工作光路如图4所示。由单频泵浦激光器1产生的532nm泵浦激光经过泵浦光缩束镜组17和半波-2 16后,由532nm反射镜14反射,通过腔镜M2 3-2进入谐振腔;由主动稳频的828nm种子激光器2产生的种子激光经过整形棱镜8和光隔离器9后,通过光纤耦合-1 10-1进入单模保偏光纤10-2,再由光纤耦合器-2 10-3输出,经过准直镜11和半波-1 12后,由828nm反射镜13反射,通过腔镜M33-3进入谐振腔。环形腔光参量振荡器3采用了四镜环形腔结构,其中腔镜M4 3-4紧贴压电陶瓷3-5。由环形腔光参量振荡器3出射的激光同时包含828nm成分和532nm成分,其中532nm由R828T532介质膜双色镜18透射泄漏,828nm由18反射,经过828nm反射镜21进行发射。同时,通过光束取样镜20取样少部分发射激光至谐振腔光电探测器23获得腔长调制信号,再通过谐振腔控制电子单元24和LV放大器25获得锁腔信号反馈至压电陶瓷3-5进行谐振腔腔长锁定。The working optical path used by the lidar transmitter system to generate a single-frequency 828nm wavelength laser is shown in FIG. 4 . The 532nm pump laser light produced by the single-frequency pump laser 1 passes through the pump light beam shrinker group 17 and the half-wave-2 16, is reflected by the 532nm mirror 14, and enters the resonant cavity through the cavity mirror M2 3-2; The seed laser generated by the frequency-stabilized 828nm seed laser 2 passes through the shaping prism 8 and the optical isolator 9, enters the single-mode polarization-maintaining fiber 10-2 through the fiber coupling-1 10-1, and is output by the fiber coupler-2 10-3 , after passing through the collimating mirror 11 and the half-wave-1 12, it is reflected by the 828nm mirror 13, and enters the resonant cavity through the cavity mirror M33-3. The ring cavity optical parametric oscillator 3 adopts a four-mirror ring cavity structure, wherein the cavity mirror M4 3-4 is closely attached to the piezoelectric ceramic 3-5. The laser emitted by the ring cavity optical parametric oscillator 3 contains both 828nm and 532nm components, of which 532nm is transmitted and leaked by the R828T532 dielectric film dichroic mirror 18, and 828nm is reflected by 18 and emitted by the 828nm mirror 21. At the same time, a small part of the emitted laser light is sampled by the beam sampling mirror 20 to the resonant cavity photodetector 23 to obtain a cavity length modulation signal, and then the cavity-locked signal is obtained through the resonant cavity control electronic unit 24 and LV amplifier 25 and fed back to the piezoelectric ceramics 3-5 for further processing. The resonant cavity is long locked.

所述激光雷达发射机系统在差分吸收激光雷达工作的时候,需要输出在828nm附近的窄带λon激光和宽带λoff激光之间以5-25Hz的速度快速切换。为此,采用光纤输出的半导体激光器作为注入种子,通过快速光开关选通方式注入OPO的谐振腔。在种子注入的同时,压电陶瓷3-5扫描OPO腔长,并以谐振腔光电探测器23监测OPO输出端泄漏出的种子光信号,当扫描到OPO谐振波长与注入种子光波长的整数倍恰好一致时,种子信号会处于极小值的位置,记录此位置。待整个扫描周期完成后,谐振腔控制电子单元24产生控制电压,经过LV放大器25放大后驱动压电陶瓷3-5将OPO腔长调至所记录的极小值获得点并保持在此位置,即可使得在泵浦脉冲到来时OPO能振荡输出与注入种子光频率一致的单频脉冲激光。整个流程时序如图5所示。为提高系统的长时间稳定性和可重复性,每一发脉冲在输出前均经历扫描—保持的过程。When the lidar transmitter system is working on the differential absorption lidar, it needs to switch between the narrowband λ on laser and the broadband λ off laser near 828nm at a speed of 5-25Hz. To this end, the semiconductor laser output from the fiber is used as the injection seed, and injected into the resonant cavity of the OPO through a fast optical switch gating method. While the seed is injected, the piezoelectric ceramic 3-5 scans the length of the OPO cavity, and uses the resonant cavity photodetector 23 to monitor the seed light signal leaked from the OPO output. When they coincide exactly, the seed signal will be at the position of the minimum value, and record this position. After the entire scanning period is completed, the resonant cavity control electronic unit 24 generates a control voltage, which is amplified by the LV amplifier 25 and drives the piezoelectric ceramics 3-5 to adjust the length of the OPO cavity to the recorded minimum value to obtain a point and keep it at this position. That is to say, when the pump pulse comes, the OPO can oscillate and output a single-frequency pulse laser that is consistent with the frequency of the injected seed light. The timing sequence of the whole process is shown in Fig. 5 . In order to improve the long-term stability and repeatability of the system, each pulse undergoes a scan-hold process before being output.

附图说明Description of drawings

图1 828nm水汽探测差分吸收激光雷达发射机框图。图中标号:1-单频泵浦激光光源,其中1-1是1064nm Nd:YAG光放大器、1-2是二倍频器、1-3是1064nm Nd:YAG主振荡器、1-4是1064nm种子源;2是主动稳频的828nm种子激光器、3是环形腔光参量振荡器、4是R1064T532介质膜双色镜、5是1064nm反射镜、6是R532T1064介质膜双色镜、7是R532T828介质膜双色镜。Fig.1 Block diagram of 828nm water vapor detection differential absorption lidar transmitter. Labels in the figure: 1-Single-frequency pump laser light source, 1-1 is 1064nm Nd:YAG optical amplifier, 1-2 is frequency doubler, 1-3 is 1064nm Nd:YAG main oscillator, 1-4 is 1064nm seed source; 2 is 828nm seed laser with active frequency stabilization; 3 is ring cavity optical parametric oscillator; 4 is R1064T532 dielectric film dichromatic mirror; 5 is 1064nm mirror; 6 is R532T1064 dielectric film dichromatic mirror; 7 is R532T828 dielectric film dichroic mirror.

图2水汽标准吸收池吸收光谱特性及调制频率示意。Figure 2 Schematic diagram of the absorption spectrum characteristics and modulation frequency of the water vapor standard absorption cell.

图3主动稳频的828nm种子激光器结构框图。图中标号:2-1是828nm DFB激光器、2-2是95:5光纤分路器、2-3是水汽吸收池、2-4是气体池光电探测器、2-5是种子光控制电子单元。Figure 3 is a block diagram of the active frequency-stabilized 828nm seed laser. Numbers in the figure: 2-1 is 828nm DFB laser, 2-2 is 95:5 fiber splitter, 2-3 is water vapor absorption pool, 2-4 is gas pool photodetector, 2-5 is seed light control electronics unit.

图4种子注入的光参量振荡器示意图。图中标号:2是主动稳频的828nm种子激光器、3是环形腔光参量振荡器,3-1是腔镜M1,3-2是腔镜M2,3-3是腔镜M3,3-4是腔镜M4、3-5是压电陶瓷、3-6是KTP晶-1、3-7是KTP晶-2、8是整形棱镜、9是光隔离器、10-1是光纤耦合-1、10-2是光纤、10-3是光纤耦合器-2、11是准直镜、12是半波-1、13是828nm反射镜、14是532nm反射镜、15是光挡-1、16是半波-2、17是泵浦光缩束镜组、18是R828T532介质膜双色镜,19是光挡-2、20是光束取样镜、21是828nm反射镜、22是光阑、23是谐振腔光电探测器、24是谐振腔控制电子单元、25是LV放大器。Figure 4. Schematic diagram of the seed-injected optical parametric oscillator. Numbers in the figure: 2 is the 828nm seed laser with active frequency stabilization, 3 is the ring cavity optical parametric oscillator, 3-1 is the cavity mirror M1, 3-2 is the cavity mirror M2, 3-3 is the cavity mirror M3, 3-4 M4 is cavity mirror, 3-5 is piezoelectric ceramic, 3-6 is KTP crystal-1, 3-7 is KTP crystal-2, 8 is shaping prism, 9 is optical isolator, 10-1 is fiber coupling-1 , 10-2 is optical fiber, 10-3 is fiber coupler-2, 11 is collimating mirror, 12 is half-wave-1, 13 is 828nm reflector, 14 is 532nm reflector, 15 is light barrier-1, 16 It is half-wave-2, 17 is the pump light reducer group, 18 is the R828T532 dielectric film dichroic mirror, 19 is the light barrier-2, 20 is the beam sampling mirror, 21 is the 828nm mirror, 22 is the diaphragm, 23 is The resonant cavity photodetector, 24 is the resonant cavity control electronic unit, and 25 is the LV amplifier.

图5扫描保持方法锁腔时序图。Fig. 5 The timing diagram of the cavity lock in the scan and hold method.

具体实施方式Detailed ways

1.所述激光雷达发射机系统使用种子注入的Nd:YAG激光器的二倍频532nm激光脉冲作为泵浦源,如法国Quantel公司YG980系列产品搭配1064nm连续波种子激光器(SI-2000)、美国Continuum公司PowerliteTM系列搭配1064nm连续波种子激光器(SI-2000)、德国InnoLas Laser GmbH公司SpitLight系列搭配1064nm连续波种子激光器、美国Spectra-Physics公司Quanta-Ray系列搭配1064nm连续波种子激光器(Model 6350),以及中国镭宝光电技术有限公司单纵模Nd:YAG激光器;1064nm的种子源可以是连续波掺镱分布反馈半导体激光器,也可以是单块Nd:YVO4晶体的连续波激光器。1. The laser radar transmitter system uses the double frequency 532nm laser pulse of the seed injected Nd:YAG laser as the pump source, such as the French Quantel company YG980 series product collocation 1064nm continuous wave seed laser (SI-2000), the U.S. Continuum The company's Powerlite TM series is equipped with a 1064nm continuous wave seed laser (SI-2000), the German InnoLas Laser GmbH company's SpitLight series is equipped with a 1064nm continuous wave seed laser, and the American Spectra-Physics company's Quanta-Ray series is equipped with a 1064nm continuous wave seed laser (Model 6350). And the single longitudinal mode Nd:YAG laser of China Leibao Optoelectronics Technology Co., Ltd.; the 1064nm seed source can be a continuous wave ytterbium-doped distributed feedback semiconductor laser, or a continuous wave laser of a single Nd:YVO 4 crystal.

2.所述激光雷达发射机系统使用KTP晶体作为非线性工作物质。KTP被切割成8mm×8mm×12mm,晶体表面镀宽频带减反射膜,xy平面内晶体沿x轴被切割θ=62°,满足Ⅱ类临界相位匹配。晶体被精确定位使泵浦束穿过晶体中心。泵浦光缩束镜组17被用以调整进入谐振腔的泵浦光束直径。2. The laser radar transmitter system uses KTP crystal as the nonlinear working substance. KTP is cut into 8mm×8mm×12mm, the surface of the crystal is coated with broadband anti-reflection coating, and the crystal is cut along the x-axis in the xy plane at θ=62°, which meets the critical phase matching of type II. The crystal is precisely positioned so that the pump beam passes through the center of the crystal. The pump beam shrinker group 17 is used to adjust the diameter of the pump beam entering the resonant cavity.

3.所述激光雷达发射机系统谐振腔3包括四块平面镜,腔镜M2 3-2对信号光有高的反射率和对泵浦光高的透过率,反射角45°;腔镜M3 3-3对信号光有70%反射率,对泵浦光有高的透过率,入射角45°;腔镜M4 3-4对于828nm信号光和532nm泵浦光都有高的反射率;腔镜M1 3-1对于泵浦光有高的透过率,对于信号光有高的反射率。所有腔镜对于空闲光都有较高透过率,空闲光由谐振腔各个腔镜泄露出去,只有信号光被正反馈而在谐振腔内振荡。3. The resonant cavity 3 of the laser radar transmitter system includes four planar mirrors, the cavity mirror M2 3-2 has a high reflectivity to the signal light and a high transmittance to the pump light, and the reflection angle is 45 °; the cavity mirror M3 3-3 has 70% reflectivity for signal light, high transmittance for pump light, and an incident angle of 45°; cavity mirror M4 3-4 has high reflectivity for 828nm signal light and 532nm pump light; The cavity mirror M1 3-1 has a high transmittance for the pump light and a high reflectivity for the signal light. All the cavity mirrors have high transmittance for the idle light, and the idle light leaks out from each cavity mirror of the resonator, and only the signal light is positively fed back to oscillate in the resonator.

4.所述激光雷达发射机系统引入由DFB激光器或者ECDL激光器或者DBR激光器产生的828nm种子光作为光参量振荡器谐振腔注入种子;使用充有水汽多通道吸收池与外腔调谐半导体激光器形成PDH(Pound–Drever–Hall)反馈伺服系统,使种子激光的波长位于水汽吸收线的中心波长。4. The lidar transmitter system introduces the 828nm seed light produced by the DFB laser or the ECDL laser or the DBR laser as an optical parametric oscillator resonator injection seed; use a multi-channel absorption pool filled with water vapor and an external cavity tuned semiconductor laser to form a PDH (Pound–Drever–Hall) feedback servo system, so that the wavelength of the seed laser is located at the center wavelength of the water vapor absorption line.

Claims (3)

1. a kind of 828nm atmosphere vapour detects differential absorption lidar transmitter system, including single-frequency pump laser (1), The 828nm seed laser (2) and annular cavity optical parametric oscillator (3) of active frequency stabilization, it is characterised in that:
Annular cavity optical parametric oscillator (3) are passed through by the 532nm pumping laser pulse that the single-frequency pump laser (1) emits The exploring laser light pulse of 828nm is converted to, conversion process needs the kind for generating the 828nm seed laser (2) of active frequency stabilization Sub- laser injects annular cavity optical parametric oscillator (3).
2. 828nm atmosphere vapour as described in claim 1 detects differential absorption lidar transmitter system, feature exists In the 828nm seed laser (2) of the active frequency stabilization module includes 828nm Distributed Feedback Laser (2-1), 95:5 optical fiber point Road device (2-2), water vapor absorption pond (2-3), gas cell photodetector (2-4), seed photocontrol electronic unit (2-5).By The seed laser that 828nm Distributed Feedback Laser (2-1) generates is divided into two-way by 95:5 optical fiber splitter (2-2), and 95% is sent to ring Shape chamber optical parametric oscillator (3), 5% is sent to water vapor absorption pond (2-3);By gas cell photodetector (2-4) after water vapor absorption Absorption signal is obtained, seed photocontrol electronic unit (2-5) carries out 828nm Distributed Feedback Laser (2-1) according to absorption signal anti- Feedback control.
3. 828nm atmosphere vapour as described in claim 1 detects differential absorption lidar transmitter system, it is characterised in that The annular cavity optical parametric oscillator (3) includes hysteroscope M1 (3-1), hysteroscope M2 (3-2), hysteroscope M3 (3-3), hysteroscope M4 (3- 4), piezoelectric ceramics (3-5), ktp crystal 1 (3-6), ktp crystal 2 (3-7);By the 532nm pump of single-frequency pump laser (1) transmitting Pu laser pulse enters ring resonator, the 828nm laser arteries and veins that annular cavity optical parametric oscillator (3) generates by hysteroscope M2 (3-2) Punching leaves resonant cavity via hysteroscope M3 (3-3), and the annular cavity optical parametric oscillator (3) has used resonant cavity stable mode simultaneously Block, including Resonant Cavity Photodetectors (23), resonant cavity control electronic unit (24) and LV amplifier (25), and resonant cavity photoelectricity is visited It surveys the chamber long modulated signal that device (23) obtain and the calculating of electronic unit (24) and putting for LV amplifier (25) is controlled by resonant cavity Piezoelectric ceramics (3-5) is fed back to after big.
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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110888118A (en) * 2019-11-18 2020-03-17 中国科学院上海技术物理研究所 Differential absorption laser radar transmitter for detecting atmospheric pressure
CN112285674A (en) * 2020-09-25 2021-01-29 中国科学院上海技术物理研究所 Micro-pulse differential absorption laser radar transmitter for detecting atmospheric water vapor
CN113267777A (en) * 2020-02-17 2021-08-17 上海禾赛科技有限公司 Laser radar
CN113640831A (en) * 2021-08-19 2021-11-12 中国科学院上海技术物理研究所 Micropulse lidar and method for detecting atmospheric water vapor, temperature and pressure
WO2023274351A1 (en) * 2021-06-30 2023-01-05 The Chinese University Of Hong Kong Pump-probe photothermal spectroscopy having passive phase detection and an optical waveguide
CN115980710A (en) * 2023-03-21 2023-04-18 南京信息工程大学 Differential absorption laser radar transmitting device based on electro-optical modulation and laser radar

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103513490A (en) * 2012-06-21 2014-01-15 中国科学院大连化学物理研究所 Single-longitudinal-mode optical parametric oscillation amplifier and automatic locking method thereof
WO2015022148A1 (en) * 2013-08-12 2015-02-19 Cnrs - Centre National De La Recherche Scientifique Multifrequency pulsed laser emitter and differential absorption lidar employing such a laser emitter
CN109301687A (en) * 2018-11-26 2019-02-01 中国人民解放军国防科技大学 A laser automatic frequency stabilization system based on saturable absorption spectrum intelligent identification technology
CN109655843A (en) * 2019-01-16 2019-04-19 武汉大学 A Pulsed Infrared Differential Absorption Lidar System for Detecting Carbon Dioxide Concentration Profiles
CN210074417U (en) * 2019-05-17 2020-02-14 中国科学院上海技术物理研究所 828nm atmospheric water vapor detection differential absorption laser radar transmitter system

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103513490A (en) * 2012-06-21 2014-01-15 中国科学院大连化学物理研究所 Single-longitudinal-mode optical parametric oscillation amplifier and automatic locking method thereof
WO2015022148A1 (en) * 2013-08-12 2015-02-19 Cnrs - Centre National De La Recherche Scientifique Multifrequency pulsed laser emitter and differential absorption lidar employing such a laser emitter
CN109301687A (en) * 2018-11-26 2019-02-01 中国人民解放军国防科技大学 A laser automatic frequency stabilization system based on saturable absorption spectrum intelligent identification technology
CN109655843A (en) * 2019-01-16 2019-04-19 武汉大学 A Pulsed Infrared Differential Absorption Lidar System for Detecting Carbon Dioxide Concentration Profiles
CN210074417U (en) * 2019-05-17 2020-02-14 中国科学院上海技术物理研究所 828nm atmospheric water vapor detection differential absorption laser radar transmitter system

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
洪光烈: "水汽差分吸收激光雷达发射机935nm高功率光参量振荡器", 红外与激光工程, vol. 47, no. 12, pages 1 - 3 *
洪光烈;李嘉唐;孔伟;葛烨;舒嵘;: "935nm差分吸收激光雷达系统及对流边界层水汽廓线探测", 光学学报, vol. 37, no. 02 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110888118A (en) * 2019-11-18 2020-03-17 中国科学院上海技术物理研究所 Differential absorption laser radar transmitter for detecting atmospheric pressure
CN110888118B (en) * 2019-11-18 2023-05-05 中国科学院上海技术物理研究所 A Differential Absorption LiDAR Transmitter for Detecting Atmospheric Pressure
CN113267777A (en) * 2020-02-17 2021-08-17 上海禾赛科技有限公司 Laser radar
CN112285674A (en) * 2020-09-25 2021-01-29 中国科学院上海技术物理研究所 Micro-pulse differential absorption laser radar transmitter for detecting atmospheric water vapor
CN112285674B (en) * 2020-09-25 2022-11-11 中国科学院上海技术物理研究所 A Transmitter for Micropulse Differential Absorption Lidar for Detecting Atmospheric Water Vapor
WO2023274351A1 (en) * 2021-06-30 2023-01-05 The Chinese University Of Hong Kong Pump-probe photothermal spectroscopy having passive phase detection and an optical waveguide
CN113640831A (en) * 2021-08-19 2021-11-12 中国科学院上海技术物理研究所 Micropulse lidar and method for detecting atmospheric water vapor, temperature and pressure
CN113640831B (en) * 2021-08-19 2024-03-08 中国科学院上海技术物理研究所 Micropulse laser radar and method for detecting atmospheric water vapor, temperature and pressure
CN115980710A (en) * 2023-03-21 2023-04-18 南京信息工程大学 Differential absorption laser radar transmitting device based on electro-optical modulation and laser radar

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Application publication date: 20190806