ffner展宽器高倍率展宽脉冲的理论与实验研究

在理论上分析了 ffner展宽器的色散特性 ,给出了展宽脉冲随 ffner展宽器系统参数变化的关系 .据此在实验上建立了一台 ffner飞秒展宽器系统 ,将 19fs的种子脉冲无色差展宽至 6 0 5ps ,测量结果与理论计算一致 .     

(O)ffner展宽器高倍率展宽脉冲的理论与实验研究

在理论上分析了(O)ffner展宽器的色散特性,给出了展宽脉冲随(O)ffner展宽器系统参数变化的关系.据此在实验上建立了一台(O)ffner飞秒展宽器系统,将19 fs的种子脉冲无色差展宽至605 ps,测量结果与理论计算一致.     

Öffner展宽器高倍率展宽脉冲的理论与实验研究

在理论上分析了(O)ffner展宽器的色散特性,给出了展宽脉冲随(O)ffner展宽器系统参数变化的关系.据此在实验上建立了一台(O)ffner飞秒展宽器系统,将19 fs的种子脉冲无色差展宽至605 ps,测量结果与理论计算一致.     

Oeffner展宽器高倍率展宽脉冲的理论与实验研究

在理论上分析了Oeffner展宽器的色散特性，给出了展宽脉冲随Oeffner展宽器系统参数变化的关系．据此在实验上建立了一台Oeffner飞秒展宽器系统，将19fs的种子脉冲无色差展宽至605ps，测量结果与理论计算一致．     

光栅展宽系统中脉冲展宽比受高阶色散影响的数值分析

分析了光栅展宽器中高阶色散对飞秒种子脉冲展宽量的影响,给出了精确计算展宽器展宽倍数的公式,并且针对反射式共焦望远镜系统引入的球差对展宽系统的色散量进行了修正.通过数值计算与实验结果比较验证了理论计算的精确性,从而为准确估算光栅展宽器中脉冲的色散致展宽量提供了有效的方法.     

啁啾脉冲放大激光系统中展宽器色散的解析算法

时域色散精密控制是超短激光产生及其应用中的关键技术之一,它通过控制各波长的光程产生相对延迟从而改变脉冲宽度.展宽器是啁啾脉冲放大激光系统中对激光脉冲展宽的装置,基于光线追迹法研究光线在展宽器中的传输路径,可计算飞秒脉冲中各波长的光程,进而计算脉冲展宽量并应用于系统设计.由于展宽器的光程表达式复杂,直接对其求导获得色散表达式较困难,目前只能采用数值导数获得近似解,这在计算过程中会引入误差,不利于激光系统精确设计和优化.本文介绍了一种易实现的求解展宽器色散的解析算法,通过归纳展宽器光程表达式特点,引入四个基元函数,将光程表达式分解和反复代换,可得到高阶色散的精确解析值.本文首先对Martinez型展宽器重新光线追迹,获得与Offner型展宽器一致的相位表达式,其次通过解析算法获得了两种展宽器的精确高阶色散值,最后将解析算法与数值算法的结果进行了比较.该解析算法对于啁啾脉冲放大系统的参数设计具有实用价值.     

基于耗散孤子种子的啁啾脉冲光纤放大系统输出特性

以不同滤波器带宽下获得的全正色散光纤激光器耗散孤子作为啁啾脉冲放大(CPA)系统的种子脉冲, 研究了光栅对和光纤展宽器CPA系统输出脉冲的可压缩性. 结果表明, 对于大能量耗散孤子种子脉冲, 当CPA系统采用正色散光纤展宽器时, 光纤群速色散与自相位调制之间的相互作用不仅可抑制耗散孤子脉冲光谱调制的影响, 还可使脉冲在光纤展宽器中自相似演化, 从而可提高CPA输出脉冲的可压缩性. 通过优化光纤展宽器长度, 对于耗散孤子种子源, 采用光纤展宽器的CPA系统输出脉冲可压缩性与主脉冲所占脉冲总能量之比均优于采用光栅对展宽器时的情况.     

飞秒激光啁啾脉冲放大中脉冲展宽技术研究

计算了啁啾脉冲放大技术中光栅展宽器对钛宝石飞秒脉冲的时域展宽量,并从实验中进行了观测.计算了放大器腔内元件的群色散量,进而提出了省略腔外展宽器的可能性.     

用于飞秒脉冲放大器的马丁内兹展宽器与欧浮纳展宽器性能比较

用解析法针对多通和再生两种放大器，分别研究啁啾脉冲放大技术中马丁内兹展宽器和欧浮纳展宽器的特性和适用范围.我们认为在多通放大器和再生放大器中，马丁内兹展宽器均可以很好地补偿色散；如果使用再生放大器时需要将脉冲宽度展得更宽，可采用紧凑型欧浮纳展宽器. 关键词： 啁啾脉冲放大技术 马丁内兹展宽器 欧浮纳展宽器     

超短脉冲展宽压缩系统的三维模型分析

在超短脉冲的展宽压缩系统的实验过程中,需要入射到展宽器中的光束倾斜一定角度.研究了在三维下光束倾斜入射到展宽压缩系统的情况,通过光束追迹法建立了展宽压缩系统的三维数学模型,给出了光束的水平倾斜角对展宽压缩系统的光程、群延时(GD)、群延时色散(GDD)等的影响,给出了展宽压缩系统的不同参数的相互补偿关系.通过计算,在引...     

Parameters optimization and phase analysis of decentered grating stretchers

A decentered grating stretcher for chirped pulse amplification systems is analyzed with oblique meridional ray tracing. Several formulae and conclusions are developed to design and optimize the stretcher. On basis of an analytical phase expression with an explicit significance, the expressions of the second-, third- and approximate fourth-order phases at the central wavelength are presented with only independent variables. These simplify the parameter design for this kind of stretcher and the phase compensation design of the whole amplifier system, which has been demonstrated with a practical example.     

新型无象差展宽器色散量的光线追迹计算法

对无象差展宽器的结构进行了改进,利用光线追迹法计算了其色散量,分析了展宽结果与展宽器各参量的关系,数值模拟了飞秒脉冲的展宽过程,为该展宽器的优化设计与精细调节提供了依据.     

新型无象差展宽器色散量的光线追迹计算法

对无象差展宽器的结构进行了改进，利用光线追迹法计算出其色散量，分析了展宽结果与展宽器各参量的关系，数值模拟了飞秒脉冲的展宽过程，为该展宽器的优化设计与精细调节提供了依据。     

Theoretical and experimental studies on a compact stretcher with large spectral bandwidth and high transmission efficiency

To ensure safe and effective amplification for the chirped pulse amplification laser facility, many factors such as pulse spectral width, pulse duration, grating parameters and incidence angle parameter are considered carefully in the design of the pulse stretcher. A compact four pass Offner stretcher design is given out. Experiment results show that the stretcher has broad spectral width, large stretching ratio and high transmission efficiency. By comparison, the calculated result of the dispersion effect on the pulse duration is completely consistent with the experiment result.     

Long-term carrier-envelope phase stability from a grating-based, chirped pulse amplifier

We demonstrate a carrier-envelope phase (CEP) stabilized, chirped pulse laser amplifier that exhibits greatly improved intrinsic long-term CEP stability compared with that of other amplifiers. This system employs a grating-based stretcher and compressor and a cryogenically cooled laser amplifier. Single-shot carrier envelope phase noise measurements are also presented that avoid underestimation of this parameter caused by fringe averaging and represent a rigorously accurate upper limit on CEP noise.     

Polarization control in a large-stroke optical fiber delay line

In the context of an optical fiber delay-line implementation by use of silica fiber stretching capability, we experimentally demonstrate that highly birefringent fibers preserve their ability to maintain the polarization coherence in spite of the high magnitude of the stresses applied to them during large stretching. Two experimental demonstrations are presented. In the first, polarization cross coupling versus stretching is characterized. This stretching induces a variation of group delay in the span 0-45 cm. The second is a test of the fiber stretcher in an interferometric application.     

Investigation of tunable stretcher for ultrashort pulses based on silica wires with subwavelength-diameters

A new type of tunable stretcher for ultra-short pulses is presented based on silica wires with subwavelength-diameters. Through proper design of the diameters of wires and the refractive indices of surrounding environment, we obtain large second-order dispersion and small higher-order dispersion, which are beneficial for pulses broadening around the operation wavelength. Analysis proves that 5-cm of such wires can broaden over 180 times for ultra-short pulses with 30-fs pulse-width. Tunable stretching ratio of stretcher is obtained by changing refractive indices of surrounding environment.     

A High Efficiency Yb3+-doped Fiber Ring Cavity Laser with Narrow Line-widthRound-trip Dispersion Calculation for Martinez Pulse Stretcher

A novel Yb3+-doped fiber ring cavity laser pumped by a 977 nm laser diode is presented with its output laser wavelength of 1060 nm. Based on a fiber Bragg grating (FBG), the laser exhibits 0.20 nm line-width, 7.5 mW laser output power, 40 dB signal-to-noise ratio (SNR) and 66% slope efficiency.This paper proposed a ray-tracing model for the Martinez stretcher, derived the calculation formulae for the stretcher of a grating-spherical mirror system and discussed the error for the total dispersion resulted from the spatial dispersion. The calculated results show that the error could be ignored for the beam returned to the stretcher for the second pass in the wavelength range of 750 nm and 850 nm.