窄脉冲外差体制CO2激光主动成像研究

根据大目标外差探测时发射功率P_T与距离R₂成正比规律的脉冲激光雷达方程和天线定理,利用国内最新研制的小型高重频电光调Q波导CO₂激光器,采用非线性扫描和激光器不等时发射技术,设计研制了一套窄脉冲外差体制CO₂激光主动成像系统,对室内20m处大目标实现了像元素64×32、成像速率10帧/s实时成像显示,图像质量较好,激光器峰值功率约为60W、脉冲重复频40KHz、前沿50ns、脉宽300ns.     

Frequency stabilization of pulsed CO2 laser using setup-time method

A new method for laser-frequency stabilization by controlling the pulse setup time is presented. The frequency-stabilization system monitors the pulse setup time continuously, and controls it by adjusting the cavity length. Laser frequency is stabilized to the center of the gain curve when the setup time is the shortest. The system is used to stabilize a radio-frequency-excited waveguide CO 2 laser tuned by grating, and the shift of laser frequency is estimated to be less than ±25 MHz for an extended period. The system has the advantages of compact structure, small volume, and low cost. It can be applied for frequency stabilization of other kinds of pulsed lasers with adjustable cavity.     

相干多普勒测风激光雷达低信噪比区域回波信号的估计方法

相干多普勒测风激光雷达通常会采用周期图最大值法（PM）提取不同距离门信号的多普勒频移（对应风速）信息。由于噪声和相干效率的影响,个别距离门信号会出现信噪比（SNR）突然降低的情况,从而导致系统的探测概率降低,影响系统整体的探测性能。为了解决个别距离门信号多普勒频移的错误估计问题,提出了一种新的非线性自适应多普勒频移估计方法。该方法利用风速的连续性,标定错误距离门,并自适应地利用强信噪比区域的多普勒频移统计数据来弥补信噪比变差而出现的估计错误。分别利用了仿真模型和一套1.54μm全光纤相干激光雷达系统获得了风场测量数据,对比了使用该技术前后反演得到的风速趋势,证明该方法能够有效地解决上述问题。     

Development of an all-fiber heterodyne lidar for range and velocity measurements

A 1550-nm all-fiber monostatic lidar system based on linear chirp amplitude modulation and heterodyne detection for the measurements of range and velocity is presented. The signal processing method is given, after which the relationship between the peak frequency values in the final signal spectrum, the target＇s range, and the line-of-sight velocity is obtained in the presence of the fiber end-face-reflected signal plaguing many monostatic lidar systems. The range of an electric fan as well as the line-of-sight fan speed of different levels is tested. This proposed system has a potential application for the space-borne landing system.     

Laser-diode-pumped zigzag oscillator power slab Nd：YAG master amplifier

A Q-switched distributed Bragg reflector fiber laser using a graphene passive saturable absorber is proposed in a cavity consisting of a fiber Bragg grating and Faraday rotator mirror as end mirrors, together with a highly doped erbium-doped fiber as a gain source. The laser has a Q-switched threshold of about 28 mW and a tunable repetition rate of 10.4-18.0 kHz with varying pump power. The shortest pulse width obtained from the system is 3.7 μs, with a maximum pulse energy and peak power of 22.2 nJ and 3.4 mW, respectively.     

A Kilowatt Diode-Pumped Solid-State Heat-Capacity Double-Slab Laser

A kilowatt diode-pumped solid state heat capacity laser is fabricated with a double-slab Nd：YAG. Using the theoretical model of heat capacity laser output laser characteristics, the relationships between the output power, temperature and time are obtained. The slab is 59 × 40×4.5mm^3 in size. The average pump power is 11.2kW, the repetition rate is i kHz, and the duty cycle is 20%. During the running time of i s, the output energy of the laser has a fluctuation with the maximal output energy at 2.06 J, and the maximal output average power is 2.06kW. At the end of the second, the output energy declines to about 50% compared to the beginning. The therma/effects can be improved with one slab cooled by water. The experimental results are consistent with the calculation data.     

Comparison of different side-pumping configurations for high power laser diode pumped solid-state laser

Ray-tracing method is used to simulate the distribution of absorption in crystal rod for different side-pumping configuration. The distribution of pumping power and absorption efficiency is compared, and the numerical results are presented. The results show that the more uniform pumping and the higher absorption coefficient are obtained with a diffuse cavity. And the method of the slow axis of laser diode stack perpendicular to the axis of lasing gives the higher central pumping density.     

饱和激发下叶绿素荧光非线性变化及影响分析

叶绿素浓度是海洋初级生产力的重要指标之一,激光诱导荧光技术可以实现海水叶绿素浓度的快速测量。测量叶绿素浓度的传统激光诱导荧光原理,是利用叶绿素荧光与水体Raman散射的强度比值（I_F/R）进行反演,即叶绿素浓度n_chl＝CI_F/R,其中C为系统常量。这是依据叶绿素荧光685 nm、水体Raman散射强度都与激发光强呈线性关系。然而,该理论并没有考虑诱导荧光饱和现象的存在。当诱导激光强度达到一定程度后,685 nm荧光强度随激发光强非线性变化。另外,值得注意的是,水体Raman散射并不存在信号饱和现象。为了探讨饱和激发造成荧光非线性变化的影响,在激光诱导荧光技术测量叶绿素浓度的实验中,设计两种测量方案,即：不同激光功率诱导单一浓度样本的荧光测量,和固定激光功率时不同浓度样本的荧光测量。实验中利用Nd∶YAG三倍频激光355 nm激发获得叶绿素溶液的404 nm处 Raman散射和685 nm荧光。实验结果分为2部分进行讨论：（1）为了分析饱和激发造成荧光变化的非线性特性,通过调节激发光功率测量溶液的受激发射光谱,发现水体Raman散射强度与激发光强呈线性关系,而685 nm荧光强度出现饱和激发下的非线性变化。而且,随叶绿素浓度的增加,685 nm荧光的非线性趋势更为明显,Raman散射强度与激发光强的线性关系中斜率变小。数据分析表明,685 nm荧光数据拟合的4阶多项式和Raman散射效率值,可以定性地表征685 nm荧光的饱和程度。（2）考虑实际海洋激光雷达探测叶绿素浓度应用中存在饱和激发荧光非线性现象,为了分析荧光非线性对传统叶绿素浓度反演理论适用性的影响,在固定激发光强情况下对不同浓度叶绿素溶液的发射光谱进行测量。将激发光功率调节至52.00,80.70,132.10和197.30 mW·cm-2,获取相应激发光强下685 nm荧光与水体Raman散射的强度比值和叶绿素浓度之间的关系。实验表明,激发光强不变的情况下,685 nm荧光与水体Raman散射的强度比值,与叶绿素浓度仍满足线性关系。但是,在较高光强激发时,饱和激发造成的叶绿素荧光非线性变化,导致利用传统激光诱导荧光理论反演的叶绿素浓度值偏小。因此,需要对饱和激发下荧光非线性的影响进行修正,其关系为I_F/R=n_chl/C+C_F,修正值C_F不可忽略。另外,值得一提的是,修正关系中系统常量C随激发光强增加而增大。研究表明,饱和激发造成的荧光非线性,会对激光诱导荧光技术测量叶绿素浓度产生影响,但由于造成荧光非线性因素的复杂性,仅通过荧光数据拟合获得的多项式,无法定量说明其影响权重。然而,当激发光强不变时,可以实验测量获得基于激光诱导荧光原理的修正关系,从而准确反演叶绿素浓度。