射频板条CO2激光器输出光束的光学变换

射频激励板条CO2激光器输出激光近场光斑近似为一条线,远场光斑为O形图样。在垂直于光束传输方向的平面内,光束在一个方向发散很大,无法用于激光加工。根据激光器不同的激光功率级别及光束尺寸,分别采用了圆柱面镜、滤波光阑、扩束望远镜等不同组合的方法,将200 W激光器输出光束变换成远场光束为Φ6、近似TEM00模的圆形光束,500 W激光器远场光束为Φ10的低阶模的圆形光束。成功用于激光切割。     

半导体激光泵浦亚稳态氩气激光器实现激光振荡

采用基于体布拉格光栅的窄线宽半导体激光器作为泵浦源,以电容耦合式射频激励Ar, He混合气体放电等离子体为增益介质,在双程纵向泵浦的结构下实现了连续波模式的912 nm的激光输出。     

A miniature electron beam pumped laser

The 1.73 μm XeI laser has been operated in a fully continuous mode using a table-top electron beam pumped laser setup. A 12 keV electron beam sent through a 300 nm thick silicon nitride membrane into a laser gas mixture of typically 600 mbar gas pressure was used for pumping. A low loss cavity was installed, resulting in a very low pumping power of 37 mW to reach laser threshold. The geometrical conditions for the laser setup such as the shape of the beam pumped volume and its overlap with the optical mode volume are discussed. The laser scheme has been clearly identified as a recombination laser scheme by operating the laser in pulsed mode and observing the time structure of the laser pulse.     

A novel picosecond distributed feedback dye laser arrangement for excimer laser pumping

A distributed feedback dye laser arrangement is described which can generate pulses at the subharmonic wavelengths of the main excimer laser lines (308 nm, 248 nm, 193 nm, etc.). The laser can be pumped with broadband lasers, such as the XeCl^* laserpumped dye laser with competing cavities. The laser is designed to be used as a part of a femtosecond, terawatt excimer laser system.     

激光箔条云对激光导引头的干扰效果研究

激光箔条云对激光有很高的散射率,光电对抗中越来越多地采用激光箔条云作为激光无源假目标实施无源干扰,或作为激光漫反射体与激光有源干扰设备配合使用,实施激光角度欺骗干扰。基于箔条云对激光的散射原理,分析了两种干扰方式的原理,设计了激光箔条云对激光导引头的有源角度欺骗干扰实验方法,给出了所需测试设备及布站要求。结果表明,干扰效果理想。该干扰方法具有灵活、机动、快速等特点,可作为一种激光有源角度欺骗干扰的新手段。     

大芯径空气包层微结构光纤实现kW级激光传输

kW级高功率激光柔性传输是激光清洗、激光焊接、激光刻蚀等高功率激光加工领域中必备的环节,而实现高功率激光低损耗传输的光纤是其关键器件。目前高功率激光传输光纤采用大芯径传能光纤,仍然存在着弯曲损耗大、柔性差等问题,并且使用过程中要经常维护。华南师范大学特种光纤研究中心提出一种大芯径空气包层微结构光纤,利用包层的空气孔可以极大降低激光泄露的风险,降低光纤制备过程中对耐高温涂敷层的严苛要求,实验结果证实该光纤在室温无制冷条件下可实现kW级激光传输,从而为10 kW级高功率激光柔性传输奠定基础。     

High efficiency hydrocarbon-free resonance transition potassium laser

We experimentally demonstrate a high efficiency potassium laser using a 0.15 nm bandwidth alexandrite laser as the pump source. The laser uses naturally occurring helium as the buffer gas. We achieve a 64% slope efficiency and a 57% optical to optical conversion. A pulsed laser model shows good agreement with the data.     

Generation of 2-nJ pulses from a femtosecond ytterbium fiber laser

We report a mode-locked ytterbium fiber laser that generates femtosecond pulses with energies as large as 2.2 nJ. This represents a 20-fold improvement in pulse energy compared with that of previously reported femtosecond Yb fiber lasers. The laser produces pulses as short as 52 fs, which are to our knowledge the shortest pulses to date from a Yb fiber laser. The laser is diode pumped by a wavelength-division multiplexing coupler, which leads to excellent stability.     

半导体激光器在医学上的应用

半导体激光器于１９６２年问世以来，在很多领域有了迅速的发展。近年来，国际上各种波长的激光二极管的报道令人目不暇接，从而半导体激光器在医学上的应用也随着波长的扩展、高功率激光阵列的出现以及可兼容的光纤导光和激光能量参数微机控制的出现而迅速发展起来。半导体激光器具有体积小、重量轻、成本低、波长可选择等优点，在眼科、矫形、皮肤、肿瘤、牙科、妇科、泌尿科和普外科等都有应用。尤其是半导体激光器作为激光针灸与原来的中医针灸理论中的腧穴、经络理论相结合，成为一种新兴的激光针灸仪。本文主要叙述了激光与生物组织的相互作用以及半导体激光在基础医学中的一些具体应用。     

F-P半导体激光放大器弱信号机制下的增益特性研究

利用直接耦合的激光器放大器对,观察了弱信号机制下Fabry-Perot的半导体激光放大器的光放大.测量了放大器增益随放大器注入电流的变化关系,并将实验结果同理论模型相比较,发现理论和实验是一致的.把F-P放大器看作是一个光电探测器,通过测量放大器的短路光电流,得到了激光器同放大器之间的耦合效率.     

激光器与轨道的相对位置对动态加热的影响

 通过分析光束入射的角度因子将激光器在地平面上的安放位置进行分类,采用了几何分析和数值模拟的方法,探讨了聚焦激光束在加热运动圆柱体过程中,为了达到一定的加热功率水平和能量水平以取得最好的加热效果而应采取的措施,即应当以激光垂直入射的轨道点为中心,以激光的有效工作时间为取值范围,并参考大气对激光能量的衰减,相对于轨道选取适当的距离进行加热。该研究从理论上说明了激光器与圆柱体运动轨道的相对位置对激光动态加热的影响可以看作一个优化问题,存在最优解,进而对于合理使用激光器进行动态加热具有参考价值。     

激光测距仪信噪比与激光发散角最佳值的选取

研讨激光测距仪的信噪比和激光发散角如何选取最佳值的问题。如果信噪比为SNR，激光发散角为θt，则取SNR θt^2最小时的信噪比和激光发散角为最佳值。     

Single-longitudinal-mode fiber laser with a passive multiple-ring cavity and its application for video transmission

A single-longitudinal-mode erbium-doped fiber laser with a passive multiple-ring cavity (MRC) is proposed for the first time to the authors' knowledge. The laser is fundamentally structured by insertion of three different short ring cavities, which serve as mode filters, into the main cavity. When it is combined with a mode-restricting intracavity fiber Bragg grating, the MRC resonator ensures single-longitundinal-mode laser oscillation. The laser can successfully suppress side-mode frequencies of as much as 1 GHz and provide an output power of 23 mW with a side-mode suppression ratio of 51 dB at 1533 nm. The short-term linewidth of the laser output measured is ~2 kHz . The ability of this fiber laser to act as an AM transmitter source is also demonstrated.     

低强度激光辐照HeLa细胞诱导增殖效应的可见光谱特性

比较研究了可见波段405,514,633和785nm低强度激光辐照HeLa细胞的促增殖效应。实验采用100和1 000J.m-2两种有效能量密度的可见光波辐照细胞,照射后24,48,72h采用MTT法检测细胞活性。结果表明,405,633,785nm激光均能促进HeLa细胞增殖,且呈波长和时间依赖性;633nm激光辐照对细胞促增殖效应最显著;514nm激光辐照对HeLa细胞促增殖效应较不明显。不同光剂量对细胞增殖效应不同,405,633,785nm激光辐照时能量密度为1 000J.m-2的辐照组细胞增殖均较100J.m-2辐照组明显,而514nm激光辐照时1 000J.m-2辐照组与100J.m-2辐照组细胞增殖的差异不明显。     

Wavelength-independent all-optical synchronization of a Q-switched 100-ps microchip laser to a femtosecond laser reference source

We present a Q-switched microchip laser emitting 1064-nm pulses as short as 100 ps synchronized to a cavity dumped femtosecond laser emitting 800-nm pulses as short as 80 fs. The synchronization is achieved by presaturating the saturable absorber of the microchip laser with femtosecond pulses even though both lasers emit at widely separated wavelengths. The mean timing jitter is 40 ps and thus considerably shorter than the pulse duration of the microchip laser.     

倍频纳秒激光驱动类氖锗X射线激光的研究

利用JB19等程序分别对基频和倍频激光驱动条件下类氖锗X射线激光进行了模拟计算,结果表明利用倍频激光驱动同样也能够获得高强度的类氖锗X射线激光输出,只是对驱动激光的输出要求要高3.3倍.尽管如此,这也为将来在大型激光装置上开展类氖系列X射线激光研究指明了方向.初步的实验研究也证实了利用倍频纳秒激光驱动能够获得类氖锗X射线激光输出的结果. 关键词： X射线激光 类氖锗 数值模拟     

激光参数对红外成像系统干扰效果影响的实验研究

 针对激光对红外成像系统的干扰效果是光电对抗领域的一个研究热点,采用波长10.6 μm的CO2调谐脉冲激光器,通过漫反射板反射激光能量到像元数为320×240的多晶硅非制冷焦平面红外热像仪上进行激光干扰红外成像系统的实验。在实验中研究了干扰激光能量、重复频率、波长、光斑大小等激光参数对干扰效果的影响,并从图像质量的角度分析了激光参数对干扰效果的影响。结果表明,随着干扰激光能量密度、重复频率、波长和光斑的增大,干扰效果提高。此外,漫反射干扰的效果证明这种干扰方式是可行的,该方式可避免干扰源成为未来将出现的反辐射光电制导武器的诱饵,为CO2激光干扰装备提供一种新的战术配置方法。     

Cr~(2+):ZnSe全固态中红外激光器

建立了一种高质量、高效率全固态中红外激光系统,并对激光输出的效率、光束质量等指标进行了测试。首先,以二极管激光器为泵浦源,Tm~(3+):YAP晶体为增益介质,搭建了输出波长为1.97μm的近红外激光器。然后,以Tm~(3+):YAP激光器为泵浦源,自行开发研制的Cr~(2+):ZnSe单晶为增益介质,搭建了全固态中红外激光器。最后,测试了全固态中红外激光器的光束质量及激光器出光效率,并对谐振腔光效率的理论输出值与实际的激光器出光参数进行了对比。实验结果表明:此全固态中红外激光器的光光转换效率为17.2%,斜率效率为20%,在最高输出能量为3 W时的光束质量(M~2)在x和y方向分别为1.7和1.73,光束基本为圆形的高斯光斑。     

A comparative study on diode-pumped single-frequency Tm:YAG and Tm:GdVO<Subscript>4</Subscript> lasers

In this paper, we present experimental results concerning on the laser characteristics of Tm:YAG laser and Tm: GdVO₄ laser. At room temperature, the maximum output power of Tm:YAG laser and Tm:GdVO₄ laser is 210 and 145 mW, respectively. High efficiency can be achieved for both lasers at room temperature. Nevertheless, compared with Tm:GdVO₄ laser, Tm:YAG laser can operate on single frequency with high power easily. As much as 60 mW of 2013.9 nm single-longitudinal-mode (SLM) laser was achieved for Tm:YAG laser. For Tm:GdVO₄ laser 51 mW of 1919.7 nm SLM laser was achieved. The SLM Tm:YAG laser is better for using as a seed laser for coherent wind measurements and differential absorption LIDAR systems.     

Multiwavelength investigation of laser-damage performance in potassium dihydrogen phosphate after laser annealing

The laser-induced damage performance of potassium dihydrogen phosphate and deuterated potassium dihydrogen phosphate nonlinear optical crystals after pre-exposure to lower-energy laser pulses (laser annealing, also known as laser conditioning) is investigated as a function of wavelength for both the damaging and conditioning pulses. We obtain a quantitative evaluation of the bulk damage performance of these materials by measuring the density of damage events as a function of laser parameters. This new method allows for a detailed assessment of the improvement of material performance from laser conditioning and reveals the key parameters for optimizing performance depending on the operational wavelength.