用于宽带啁啾脉冲光参量放大系统精确同步的新方法

基于非共线光参量放大,以波长800 nm飞秒激光的倍频光为抽运光,以激光二极管640 nm连续波激光为信号光,产生了与800 nm飞秒激光精确同步的无直流本底的1064 nm脉冲光。实验结果显示该1064 nm的光脉冲在脉冲能量和空间光束质量上均可作为1064 nm波长脉冲放大器的种子光。仅通过一级简单紧凑的非共线参量放大就可实现光周期量级的光参量啁啾脉冲放大系统的抽运激光和种子光的精确同步。     

Efficient Laser-Diode End-Pumped Passively Q-Switched Mode-Locked Yb：LYSO Laser Based on SESAM

We report an efficient Q-switched laser action based on a semiconductor saturable absorber mirrors （SESAMs） as passively Q-switched laser starter and a Yb：LYSO alloyed crystal as gain material pumped directly by 974nm InGaAs laser diodes. The output pulse duration is measured to be about 7μs, while the average power and the repetition rate of the pulse chain are about 0.92 W and 6.2 kHz, respectively, under 12.5 W absorbed pumping power. The Q-switched mode-locked pulse train is also observed in this setup. The laser performance shows that Yb：LYSO is a promising laser gain medium for laser-diode pumped compact solid-state lasers.     

钛宝石再生放大器1056nm波长稳定输出

讨论钛宝石再生放大器工作在１０５６ｎｍ波长时，获得稳定输出的条件，并在实验上成功地演示了稳定的放大脉冲输出，输出能量均方根起伏小于５％。     

超高亮度激光系统中光栅对脉冲整形器失调对输出脉冲时间特性的影响

在较全面地给出光栅对脉冲整形器失调产生附加相位项表达式的同时，详细地讨论了展宽器失调的附加相位放大系统传输过程中的变化，并与压缩器失调特性作了比较，分析了这些失调对超高亮度激光系统输出脉冲及其聚焦场时间特性的影响，得到了确定光栅对脉冲整形器失调容限的基本原则。     

与794nm飞秒激光精确同步的无直流背底的1064nm脉冲光的产生

基于非共线光参量放大(NOPA)，以宽带794nm飞秒激光的倍频光为抽运光，以连续的He-Ne激光为信号光，产生了与宽带794nm飞秒激光精确同步的无直流背底的1064nm的脉冲光.实验结果显示该1064nm的光脉冲可作为光参量啁啾脉冲放大系统的抽运激光链的种子光，从而实现用全光学方法实现OPCPA系统抽运光和信号光的精确同步.还将非共线光参量放大器置于经特殊设计的He-Ne激光腔内，也同样成功得到了无直流背底的1064nm的光脉冲.经一次光参量放大后所得到的1064nm光的光谱和空间啁啾特性与非共线光参量放大器置于He-Ne激光腔外时得到的1064nm的光脉冲相同，而其单脉冲能量约为腔外NOPA的10倍. 关键词： 非线性光参量放大 光参量啁啾脉冲放大 时间同步     

BBO晶体中级联非线性效应的实验研究

采用800 nm和400 nm两束飞秒激光脉冲在BBO晶体中同时满足相位匹配条件,产生差频、和频及其级联效应.实验运用了中心波长800 nm、重复频率10 Hz、脉宽60 fs及光斑直径7 mm的钛蓝宝石再生放大飞秒激光,输出约为10 mJ的能量以7:3分束.其中7 mJ光脉冲用一块非线性晶体BBO倍频至400 nm获得1.45 mJ能量,然后与另一束800 nm的3 mJ基频激光以非共线方式注入到另一块BBO中,在兼顾和频与差频的相位匹配条件下,即晶体对于和频与差频相位匹配状态同时存在少量失谐时,会同时产生267 nm与800 nm的和频与差频效应,新产生光波与原入射激光脉冲又经过进一步非线性混频作用,最终得到多达10余束可见、紫外的一维列阵.分析了此级联非线性效应的产生机理并讨论了入射光强度,啁啾,延迟等因素对级联效果的影响.     

A Compact All-Solid-State 630-ps 9.43-kHz High Power Nd：YAG/Nd：YVO4 Hybrid Laser System

We present a simple and compact design for an all-solid-state laser amplifier system which can output 9.43-kHz 630-ps, 3.5-W pulse trains under 20 W absorbed pumping power. The excellent matching between the repetition of its seed source and the fluorescence lifetime of the amplifying medium makes it quiet efficient for the four-pass amplifier to be pumped in cw mode without need of any synchronization device between the oscillator and the amplifier. The entire setup just covers an area of 55 × 25 cm^2. The output average power fluctuation is less than ±1.5% within 10min and 3% within 6h.     

内含光栏的光栅以展宽器式脉冲整形器的输出光束特性

在忽略空间衍射效应的情况下，研究了内含狭缝光栏的光栅对展宽器式脉冲整形器的输出光束的时间特性。通过与光束的空间传输特性类比解析了光栏宽度变化引起的脉宽变化以及脉冲轮廓出现时间衍射调制现象；讨论了空间衍射效应可忽略的条件；提出用光栏软边可消除这种调制。     

A Sensitive Scheme to Observe Weak Photo-Refraction Effects in Some Nonlinear Optical Crystals Pumped by Ultrashort Optical Pulses

We present a sensitive scheme, for the first time to our knowledge, to observe photo-retraction （PR） ettects in some nonlinear optical crystals, e,g. β-BBO, LBO and BIBO, pumped by an intense ultrashort laser pulse chain. These quite weak effects are ＂amplified＂ by sensitive cw intraeavity loss modulation. Our results show that they are repeatable and are dependent on pumping power and wavelength, and their response time ranges from tens of seconds to several minutes. The recorded dynamical transitions between the self-focusing to the self-defocusing （or vice versa） induced by the PR effect may be critically important for us to give more insight into the stability of some cascade nonlinear frequency conversions, e.g. multi-stage optical parametric amplifiers.     

磷酸盐钕玻璃的荧光寿命和损耗对激光增益特性的影响小能量0.35 μm激光-X射线转换研究

实验研究了目前使用的N2122和N3122掺钕磷酸盐玻璃中不同的OH基浓度对玻璃荧光寿命的影响,同时从实验和理论上研究了荧光寿命和损耗对激光增益特性的影响,结果表明:增加玻璃的荧光寿命是提高增益性能的一个重要方法,当玻璃的荧光寿命增加10%时小信号增益系数提高5%左右。提高钕玻璃的荧光寿命,可适当降低对损耗的要求,也能够保持它的增益性能不变。以小能量0.35 μm激光(<100J)辐照盘靶(5600 μm×4 μm),用软X射线平响应探测器测量X射线角分布(dE/dΩ)和X射线转换效率(ηx)。dE/dΩ=a+bcosθ,与φ角无关。ηx随激光入射角增加而下降。按金盘、多层膜(0.11 μm)金盘和CH膜(0.4 μm)金盘顺序,ηx依次下降。