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1.
Via saturated absorption spectroscopy and the third-harmonic detection technique, the hyperfine spectra of 127I2 near 532 nm have been observed within the tuning range of a mini Nd︰YVO4-KTP laser. The laser is frequency stabilized against one hyperfine structure (hfs) component of 127I2. The analysis of error signal shows that it is possible to realize a frequency stability of 3.0×10-13 at 1 s average time.  相似文献   

2.
By using a diode-pumped Nd:YVO4 / KTP intracavity frequency-doubling mini-laser and frequency modulation optical heterodyne spectroscopy, we have obtained spectrum of127I2 hyperfine structure near 532 nm. The laser frequency is locked to hyperfine transitions of I2. The analysis of error servo signal demonstrates that the laser frequency stability can reach 10−12 at 1 second average time.  相似文献   

3.
提出了调频单模激光二极管的相干长度理论计算公式,并用由特种光纤构成的全光纤Mach-Zehnder干涉仪进行了实验验证。  相似文献   

4.
分析了自发辐射与注入种子信号在激光建立过程中的竞争对种子注入的影响. 利用单块非平面环形腔单频激光器作为种子振荡信号,注入到高重复频率Q开关构成的从动激光器,获得单脉冲能量大于5mJ、脉冲宽度40ns的单纵模振荡脉冲激光输出. 测试了种子激光器在不同频率、功率及在从动激光器不同抽运能量下种子注入现象发生的几率实验. 结果表明,频率匹配和从动激光器的抽运能量是影响种子注入发生几率的重要因素.  相似文献   

5.
532 nm单频Nd:YVO4/KTP激光器及碘吸收谱线观测的研究   总被引:2,自引:0,他引:2  
用Nd:YVO4/KTP内腔倍频激光器在515 mW抽运时,获得了40.4 mW的单频532 nm绿光.分析了获得单频运转的原因,并从理论上分析、实验中验证了用增加腔长的办法,可减小自由运转激光器的频率漂移.用其单频输出观测到1997年国际米定义咨询委员会(CCDM)推荐谱线以外的一些新的12吸收谱线.  相似文献   

6.
利用2mmKDP晶体对中心波长790nm、脉冲宽度75fs、晶体表面强度约1011W/cm2的超短超强激光脉冲进行了倍频实验研究。通过对基频脉冲能量及频率啁啾的优化,可以获得高于40%的能量转化效率。观测了基频脉冲频率啁啾对倍频光产生的影响,发现激光脉冲啁啾为零时对应的倍频转化效率最高;对于相同的光栅相对位置,正啁啾基频脉冲的倍频转化效率高于负啁啾。  相似文献   

7.
本文从讨论培频效率入手,分析了影响倍频效率的原因,给出BBO晶体氩离子腔内培频紫外激光器的设计方案,制作了激光器,并得到了紫外激光输出。  相似文献   

8.
提出一种利用激光跟踪仪标定机器人工具坐标系的方法。利用激光跟踪仪确定机器人的基坐标系,将机器人基坐标系与激光跟踪仪的测量坐标系统一。通过机器人运动学方程获得机器人末端连杆坐标系相对基坐标系的变换关系,利用激光跟踪仪测量拟合得到机器人工具坐标系,利用坐标变换初步确定机器人工具参数。通过机器人单轴旋转运动对工具坐标系原点进行修正,最终确定工具参数。最后通过机器人重定位运动对误差进行计算。实验结果表明,修正后x,y,z坐标的RMS(root mean square,均方根)误差分别为0.127 1,0.141 3和0.117 4mm,精度是修正前的2.5倍。  相似文献   

9.
Orthogonally linear polarized lasers(Ⅰ)--principle and devices   总被引:1,自引:0,他引:1  
Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect,stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c/4L instead of c/2L.  相似文献   

10.
Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect, stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c4L instead of c2L.  相似文献   

11.
本文在首先分析了高空钠层光谱特性和激光光谱的基础上,提出要获得最大激光导星回波信号,激光频率与钠原子频率应满足的匹配关系.采用智能化激光锁频的方式实现了钠层激光导星的制备,采用成像望远镜和单反相机,获得了钠层激光导星图像.同时,借助于激光雷达这一有利工具,获得了钠导星制备与成像中的激光能量、回波光子数等重要参考数据.  相似文献   

12.
采用铬原子束激光感生荧光激光稳频技术解决铬原子光刻实验中激光频率随时间漂移的问题.从理论和实验两个方面对铬原子束激光感生荧光强度随激光功率和坩埚温度的变化情况进行了研究.结果显示,在坩埚温度一定的情况下,由于铬原子的饱和效应,当激光功率增大到6 mW左右时,荧光斑点的中心强度会达到饱和然后随激光功率的增加变化不大.另外,随着激光功率的增加,荧光斑点轮廓曲线的半高宽在变大的同时,对比度减小.在激光功率一定的情况下,由于铬原子喷射的个数与坩埚温度成正比,荧光斑点的中心强度随坩埚温度的增加而增加,并且不出现饱和效应;随着坩埚温度的升高,荧光斑点轮廓曲线的半高宽基本不变,而对比度增大.这些变化趋势和理论结果符合地很好.  相似文献   

13.
利用声光调制器(AOM)的偏频特性,以甲烷(CH4)分子吸收线R9支一条强吸收线(λ=1.637 8μm)作为参考频率,实现了对外腔式半导体激光器的无调制频率锁定.实验中在100 s内典型的频率起伏小于5.6 MHz,较激光器自由运转时的频率起伏34 MHz有了显著的改善.该方法实现了对半导体激光器的无调制锁频,并且适用于分子光谱领域,满足光纤通信中对激光器输出波长的要求,在波分复用领域中将有很好的应用前景.  相似文献   

14.
LD泵浦Nd:YAG激光毛化轧辊粗糙度的模拟分析   总被引:1,自引:1,他引:0  
针对CO2激光器和灯泵浦的Nd:YAG激光器毛化技术的不足,利用半导体泵浦Nd:YAG激光器进行轧辊毛化。此装置具有峰值功率较高,光学质量好,使用寿命长,维护成本低等优点。本文利用半导体泵浦Nd:YAG激光器对轧辊毛化试验,分析了泵浦功率、脉冲频率、脉冲宽度、离焦量以及点阵密度等加工参数对毛化坑形貌和表面粗糙度的影响规律,并根据实验结果对表面粗糙度进行数值模拟,最后对模拟结果与实验值进行比较,得出了可以有效使用该模拟方法给出加工参数的调整规律结论。  相似文献   

15.
研制了一种基于正交偏振形式的双频分布式布拉格反射(Distributed Bragg Reflection, DBR)光纤激光器光纤压力传感器系统。当外部压力作用在光纤激光器谐振腔上时,光纤晶体双折射的变化会引起正交偏振方向上的激光频率发生变化,从而导致输出拍频频率改变。利用快速光电二极管将双频激光输出的拍频信号转换成射频电信号,通过一个射频混频电路将该信号与频率合成器产生的本地振荡信号混频并低通滤波放大整形,变为400 M以下的调频信号,再利用ECL定时计数电路系统记录拍频信息并通过USB接口送入计算机。实验表明,在0~1.5 N范围内线性拟合度高达99.97 %,压力灵敏度为400 MHz·N-1。  相似文献   

16.
This note reports a new type of incoherent pulse laser Doppler lidar velocimeter with iodine molecular filter as a frequency discriminator. Its transmitter subsystem applies a Nd:YAG pulse laser which is injected with a single longitudinal-mode diode pumped continuous seeder laser.The field experiment proved that this velocimeter measurement results are consistent with those measured by photoelectric velocimeter. Measurements of eight different velocities show that the standard deviation is 0.56 m/s, the range resolution is 3.75 m.  相似文献   

17.
根据Yb^3 的光谱特性,提出一种实现激光单频运转的方法,这种方法使用简单的F-P腔,利用饱和吸收体的饱和吸收效应,就可以获得稳定的、窄线宽、单频的激光。  相似文献   

18.
研究高重频激光对半主动激光制导导引头的干扰效果与导引头的信息处理能力和干扰信号样式的关系. 设计了一套激光半主动制导对抗半实物仿真系统,从信号级研究了导引头的工作原理并设计了多种抗干扰算法进行信号处理,提供了干扰效果评估方案. 分析了导引头在搜索阶段高重频激光对导引头编码识别过程的影响,以及导引头在跟踪阶段高重频激光的干扰频率、能量、位置和干扰时机对导引头不同抗干扰措施条件下的干扰效果. 实验结果表明,干扰脉冲的能量越大,干扰源与目标的夹角越大,干扰效果越明显;提高干扰激光脉冲的频率会提高干扰成功的概率,缩小导引头的时间波门的宽度会增强导引头的抗干扰能力.   相似文献   

19.
在分析脉冲激光铣削材料去除机理的基础上,系统研究了激光单脉冲能量、重复频率、激光束扫描速度和辅助吹气压力等工艺参数对硬质合金激光铣削量和质量的影响,观察不同工艺参数条件下激光铣削的表面微观形貌。通过激光铣削工艺分析,可利用较优的激光铣削工艺加工各种硬质合金试样。  相似文献   

20.
探讨了在相对论领域内,激光的频率、脉冲波形和强度对氢原子辐射波的效应.结果表明激光的频率对氢原子辐射波的影响比脉冲波形的影响效果显著.同时对激光的强度与氢原子辐射谐波在空间中的分布关系也进行了分析和讨论  相似文献   

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