半导体可饱和吸收镜实现高频脉冲激光研究进展

介绍了作为固体激光器、半导体激光器和光纤激光器被动锁模吸收体的半导体可饱和吸收镜(SESAM)的基本原理和制作方法。详细阐述了利用半导体可饱和吸收镜对同体激光器和光泵垂直外腔面发射半导体激光器进行被动锁模，获得重复率为几吉赫到几百吉赫的超短脉冲激光的方法。     

半导体可饱和吸收镜自启动的Kerr锁模Cr4+∶YAG激光器

采用传统的X型像散腔 ,利用一块精心设计的半导体可饱和吸收镜 (SESAM)做启动元件 ,实现了自启动的Kerr锁模Cr4+ ∶YAG激光器。输出脉冲的最窄脉宽小于 80fs,脉冲重复频率为 12 0MHz,脉冲峰值功率可以达到 10 0W以上     

连续可调谐Cr~(4+):YAG激光器

介绍了一种在1500um附近连续可调谐的Cr~(4+):YAG激光器,最大可调谐范围达160um。室温下,当吸收功率为5W时,得到了370mW的连续输出,激光器的抽运阈值为1.94W。     

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.     

Mode locked Er-doped fiber laser with single-wall carbon nanotube saturable absorber

A mode locked Er-doped fiber laser based on a single-wall carbon nanotube saturable absorber is demonstrated. A high quality single-wall carbon nanotubes （SWCNTs） absorber film is fabricated by a polymer composite. The pulse duration is 488 fs with 9.6-nm spectral width at the center of 1564 nm. The repetition rate is 30.4 MHz. The maximum output power is 3 mW. And the single pulse energy is 0.1 nJ.     

双波长外腔面发射激光器

双波长激光光源在干涉测量、非线性频率变换产生中红外及太赫兹波段相干辐射等方面有重要的应用.外腔面发射激光器具有输出功率高、光束质量好、发射波长可设计等突出优势,非常适合用于双波长的产生.用有源区为In0.185Ga0.815As/GaAs应变多量子阱、设计波长为960 nm,以及有源区为In0.26Ga0.74As/GaAsP0.02应变多量子阱、设计波长为1080 nm的两块半导体增益芯片,在一个共线Y型谐振腔中,获得了激光波长分别为953 nm和1100 nm的双波长输出,对应光谱线宽为1.1 nm和2.7 nm,波长间隔147 nm.室温下,每块增益芯片的抽运吸收功率均为5.8 W时,双波长激光器总的输出功率达到293 mW.     

波导耦合纳米光栅结构的光学滤波和角分辨调谐特性

利用干涉光刻技术制备了波导耦合纳米光栅结构,系统研究了其波导共振模式的角分辨调谐特性及其对光栅参数、入射光偏振特性的依赖关系,并作了相应的理论模拟.特别研究了光栅周期和厚度对波导共振模式角分辨调谐速率的影响.实验结果对于器件进一步应用于滤波、生物传感技术具有重要的指导意义. 关键词： 波导耦合光栅 干涉光刻 角分辨 调谐速率     

Wavelength tunable ultra-short pulses based on a flat broadband spectrum generated in a nonlinear ytterbium-doped fiber amplifier

We present a nonlinear ytterbium-doped fiber amplifier based on enhanced nonlinear effects that can produce a flat broadband spectrum ranging from 1050–1225 nm with a maximum average output power of 7.8 W at 14 W pump power.Its repetition rate is 89 MHz. Using a pair of gratings and two knife edges as a filter, wavelength tunable picosecond pulses of tens to hundreds of milliwatts can be obtained in the broadband spectrum range. The output power, pulse width, and spectrum(center wavelength and linewidth) are adjusted by tuning the distance of the grating pair and/or the knife edges.Fixing the distance between the two gratings at 15 mm and keeping the output spectrum linewidth at approximately 20 nm,the shortest pulse width obtained is less than 1 ps centered at 1080 nm. The longest wavelength of the short pulses is around1200 nm, and its output power and pulse width are 40 m W and 5.79 ps, respectively. The generation of a flat broadband spectrum is also discussed in this paper.     

常用激光峰值功率公式误差分析

为分析脉冲激光中常用峰值功率公式的误差,对高斯脉冲、双曲正割脉冲、洛仑兹脉冲、非对称双曲正割脉冲的常用峰值功率公式的误差进行了解析计算。结果表明：高斯脉冲、双曲正割脉冲、洛仑兹脉冲、非对称双曲正割脉冲中,常规峰值功率公式的结果与实际峰值功率的误差分别为6.3%,13.6%,22.1%,20.9%。在具体实验基础上采用数值方法分析了非常规脉冲的情形,给出了精确计算峰值功率的方法。     

掺镨钒酸钆晶体的研究

生长了新型激光晶体Pr:GdVO4,经XRD分析可知生长的晶体与纯GdVO4晶体结构一致,晶体质量良好.室温下测试了晶体400～3000 nm范围内的吸收光谱.通过对吸收光谱研究,发现σ谱图中各吸收峰吸收强度更大,宜选择入射光传播方向和电矢量均垂直于光轴的方向进行激光实验.采用404 nm的激发源抽运Pr:GdVO4晶体,测试其荧光光谱,发现其在可见波段有宽且强荧光发射(604 nm、616 nm),对应于1D2→3H4.比较不同浓度晶体的荧光谱,荧光强度呈现如下趋势:0.5;>0.7;>0.32;.