回流式水冷超薄多层镜的研究

 从理论和实验上讨论了水冷铜镜变形的规律, 从而设计出多种多层镜, 其中回流式多层镜在0.13MPa通水压力下净吸收86.9W激光功率时, 总变形仅 0.10μm,约为同等条件下普通水冷铜镜变形量的1/40。     

多层镜软X光能谱仪的结构设计与有限元分析

 8通道多层镜软X光能谱仪结构采用整体式,结合中心准直机构,保证了多层镜的角度,实现系统整体瞄准,大大简化了瞄准程序。建立了谱仪的3维模型,利用ANSYS软件完成了有限元分析。静力学分析结果表明,在重力作用下准直件的变形较大,y方向上的变形量为0.016 mm,通过增加准直筒厚度可消除影响。模态分析得到了影响谱仪使用性能必须避免的噪声。分析结果为保证谱仪测量精度提供了理论依据。     

一种提高波前空间校正能力的组合变形镜自适应光学系统

提出了一种利用光学共轭关系,实现多变形镜空间匹配从而提高波前空间校正能力的自适应光学系统方案.通过理论分析给出了组合变形镜的面形描述方法,在此基础上建立了一套基于由两块相同方形排列变形镜构成的组合波前校正器的完整自适应光学实验系统.通过数值仿真研究了该系统对前35阶Zernike像差的校正效果,并且通过实验对比了组合变形镜和单一变形镜对实际静态像差的闭环校正效果.结果表明组合变彤镜可以等效为一多单元变形镜,在直接斜率控制算法下正常稳定闭环工作,校正效果明显优于单一变形镜.组合变形镜技术通过空间匹配实现了增加波前校正器驱动单元数和等效交连值,有效地提高了对波前的空间校正能力,因此可以代替高成本的单一多驱动器变形镜用于自适应光学系统中高阶像差的校正.     

运用功能梯度结构降低大功率激光系统中镜面热变形的数值分析

 提出一种运用功能梯度结构以有效降低大功率激光系统中镜子温度和镜面热变形以及减缓热应力的新方法。讨论了环形分布和高斯分布2种类型的激光源。有限元分析结果表明，通过这种方法可使硅镜和铜镜的表面热变形成倍降低，并且还能同时显著降低镜体温度。讨论了代表热学和力学性质的函数表达式的斜率对镜面热变形的影响，研究表明：功能梯度结构的热物理对镜面形变产生重大影响，而力学性质对镜面形变的影响非常小。该结论可为具有该功能梯度结构的镜子优化设计和制造提供参考。     

相变制冷复合镜研究

提出一种新的复合式腔镜结构,利用硅镜(钼镜)和铜镜的优点,避免它们的缺点,可以有效地减小热畸变.对钼、铜复合镜作了与硅镜的对比实验.实验结果表明钼、铜复合镜的热畸变比硅镜的约小一半.     

相变制冷复合镜研究

提出一种新的复合式腔镜结构,利用硅镜(钼镜)和铜镜的优点,避免它们的缺点,可以有效地减小热畸变.对钼、铜复合镜作了与硅镜的对比实验.实验结果表明钼、铜复合镜的热畸变比硅镜的约小一半.     

相变制冷复合镜研究

 提出一种新的复合式腔镜结构,利用硅镜（钼镜）和铜镜的优点,避免它们的缺点,可以有效地减小热畸变。对钼、铜复合镜作了与硅镜的对比实验。实验结果表明钼、铜复合镜的热畸变比硅镜的约小一半。     

COIL用变形反射镜介质反射膜

 报道COIL激光用变形反射镜的介质反射多层膜实验。在真空镀膜机内制备了膜系Sub/Ag(SiO₂/HfO₂)⁴/air和Sub/Ag(YbF₃/ZnS)³/air, 反射率分别为99.90%和99.87%。在经历109次循环后变形镜物理特性无变化。研究了COIL激光辐射下热畸变和损伤特性。分别在功率密度为1.52kW/cm²和1.18kW/cm²的COIL激光辐照下,这两种膜系的变形镜波前变化为0.37l 和0.54l 。因此对于变形镜1kW/cm²激光功率密度是安全可靠的。     

双压电片变形反射镜样镜的设计与研制

双压电片变形反射镜作为波前校正器具有结构简单、变形量大、成本低及制造周期短的优点,能代替传统分立式变形镜从而降低自适应光学系统的成本.为验证工艺的可行性和了解双压电片变形反射镜的性能,制造了一块20单元的试验样镜.样镜采用了双层压电陶瓷的结构,其中一层作整体离焦电极以校正大幅值的离焦像差.利用Veeco干涉仪测最了样镜单元电极影响函数,分析了其埘前36项Zernike像差的校正能力.结果表明,样镜对离焦像差能获得高达8μm以上的校正量,对其它高阶像差也能适量校正,但校正能力随空间频率升高而降低,显示出其适合校正低阶像差的特性.此外,讨论了不同有效孔径下样镜对Zernike像差的拟合能力.     

变形镜受热变形引起的波前畸变仿真及补偿

针对变形镜自身受强激光辐照后热变形问题,利用ANSYS的多物理模型建立了变形镜的热机械模型并进行了计算。针对受强激光辐照后变形镜吸收了部分热量并产生了0.9μm的变形量,根据该变形镜热畸变分布特征,提出了一种利用补偿镜对热畸变进行补偿的方法,即在一个薄型镜面背后用一些约束头固定构成补偿镜,放置在变形镜的后续光路中。约束头在补偿镜上的位置与极头在变形镜上的位置对应错开分布。对三种不同形状约束头的补偿镜进行了计算,补偿后综合变形量降低到0.35,0.32和0.40μm。利用光束传输因子(BPF)对理想光束通过补偿镜后的效果进行评价,结果表明通过三种补偿镜后BPF值从0.906提高到了0.966,0.971和0.957。进一步的计算表明,补偿效果受约束头尺寸的影响较小。     

10 ps High Power Laser System at 248 nm

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10 Watts Double-Cladding Fiber Laser

Considering the wavelength characteristics of the pump high-power laser diode, a modified Fabry-Perot fiber laser resonator is designed. And a fiber laser with more than 10Watts output, near diffraction-limited and operating in the 1110nm region is developed.     

10瓦级双包层光纤激光器

考虑到所用大功率激光二极管的光谱特性，对光纤激光器的基本法布里-珀罗腔型稍加改变，研制出激光二极管抽运的10w级双包层光纤激光器，获得最高功率为11．8w、波长1100mm的单模激光输出。     

10 ps High Power Laser System at 248 nm

A simple 10 ps KrF laser system consisting of quenched dye laser oscillator pumped by a XeCl laser, a distributed feedback dye laser (DFDL), a three-stage dye amplifier and a two-stage KrF amplifier are described. The output of the laser system is 140 mJ with 10 ps pulse width by using polarization-multiplexing amplification. A focused output laser intensity of about 4×1015 W/cm2 is obtained. The saturation fluence for KrF laser is obtained with this laser.     

Diode-pumped 10 W continuous wave cesium laser

An efficient cesium vapor laser pumped with a continuous wave laser diode array has been demonstrated. The linewidth of the pump source was narrowed using the external cavity to match it to the cesium absorption line. The output power of the continuous wave cesium laser was 10 W, which exceeds previous results by more than a factor of 10, and the slope efficiency was 68%. The overall optical efficiency was 62%, which is a factor of 6 higher than previous pulsed laser results for alkali lasers with diode laser array pumping.     

Simultaneous emission on 10P and 10R branch lines from a hybrid CO2 laser

The use of cavity length control to obtain multiline emission from a hybrid CO₂ laser has been investigated. We have obtained simultaneous laser oscillation on up to four lines in the P and R branches of the 10 m band by operating the c.w. section above the lasing threshold. For sub-threshold operation of the c.w. section the hybrid laser emission is restricted to the stronger 10P lines.     

Period-Doubling in 10 GHz Gain-Switched DFB Laser Diode

The distinct period doubling behaviour in a 10 GHz gain-switched （GS） DFB laser is experimentally investigated in frequency domain and in time domain. The period doubling occurs as the frequency of the rf driving signal is close to or higher than the-3 dB cutoff frequency of the DFB laser diode, and the amplitude of the rf driving signal required to achieve period doubling increases linearly with the increasing bias current of the laser diode.     

Multifunctional high-performance 10-J level laser system

In this letter,we report a multifunctional high-performance Nd:glass laser system.Laser pulses from an all-fiber front end are first amplified by a regenerative amplifier to 10 mJ level,and then further amplified in a four-pass amplifier.The laser system can provide 10.3-J,3-ns laser pulses at 1053-nm wavelength.The shot-to-shot energy stability is better than 1.5%(RMS).The output laser beam is near diffraction limit.Binary amplitude masks are used to maintain a flat top near-field profile with a 71%fill factor.After the frequency conversion process,7 and 5.5 J pulses at 526.5 and 351 nm are obtained,respectively.     

La2CaB10O19晶体高效紫外激光输出研究

La2CaB10O19(LCB)为可通过Nd∶YAG激光三倍频产生355 nm紫外激光的非线性光学晶体,其光学性能可与商用化的LiB 3O 5(LBO)晶体媲美,但抗潮解特性优势明显。本文对用LCB晶体实现355 nm紫外激光输出的三倍频产生过程进行了优化设计,利用走离补偿方法来提高激光输出转换效率。通过在光路中加入沿θ=45°方向切割、厚度为1.2 mm的方解石晶体走离补偿片,在脉冲宽度为60 ns、重复频率10 kHz的激光参数下实现355 nm输出功率由12 W提升至20 W;在脉冲宽度为25 ps、重复频率为10 Hz的激光参数下355 nm转换效率由28.3%提升至35.2%。     

A Stabilized, Rationally Mode-Locked 10GHz Erbium Fiber Laser

A rationally mode-locked 10 GHz erbium fiber laser stabilized by a simple technique for extended time operation is described. The laser generates stable ~ 5 ps pulses that can be used in communications experiments. Back-to-back bit error rate (BER) measurements confirmed error-free operation for 6-8 hours, giving an error floor below 10 -14 . A receiver sensitivity of -19.7 dBm was achieved for BER of 10 -9 .