大功率、高效率、高消光比铒光纤多波长超荧光光源

采用改进的反射式Mach-Zehnder干涉滤波器，对双程后向结构掺铒光纤超荧光光源(DPB SFS) 分别进行光谱分割和光谱预分割，构建了两种结构的多波长超荧光光纤光源（MW SFS），波长间隔为～0.8 nm时，在1550 nm附近（1542～1559 nm）20个波长的功率波动小于0.5 dB其中前者消光比高达27 dB；后者消光比～18 dB，在泵浦光功率为72.8 mW时，最大输出功率25.3 mW，光光转换效率高达34.8%改变Mach-Zehnder干涉仪的臂长差，采用光谱预分割技术，得到1550 nm附近波长间隔～0.4 nm、消光比～16 dB的50个波长输出     

High Power Photonic Crystal Fibre Raman Laser

A cw Raman laser based on a 100-m photonic crystal fibre is demonstrated with up to 3.8 W output power at the incident pump power of 12 W, corresponding to an optical-to-optical efficiency of about 31.6%.. The second order Stokes light, which is firstly reported in a cw photonic crystal fibre Raman laser, is obtained at 1183nm with an output power of 1.6 W and a slope efficiency of about 45.7%.     

A Low-Pump-Threshold Photonic Crystal Fibre Raman Laser

We investigate a photonic crystal fibre Raman laser using fibre Bragg grating pairs as cavity mirrors. The threshold pump power is up to 0.65 W by decreasing the cavity loss and using a photonic crystal fibre with high Raman gain coefficient. A maximum continuous-wave output power of 2. 7 W is obtained at the maximum incident pump power of 5.6 W. The corresponding optical conversion efficiency and the slope efficiency are about 48% and 56%, respectively.     

High power wavelength-defined all-fiber Yb3+-doped double clad fiber laser

An all-fiber Yb3+-doped double-clad fiber laser using FBGs as cavity mirrors is investigated in this paper. Continuous-wave (CW) output power of 1.18 W with defined wavelength at 1.06 um and narrow line-width of less than 0.1 nm is obtained. The slope efficiency and the maximum optical-to-optical efficiency of laser output are 68% and 51%, respectively, with respect to absorbed pump power.     

高非线性光子晶体光纤中飞秒脉冲的传输特性和超连续谱产生机制的实验研究及模拟分析

用实验和数值模拟两种方法研究了高非线性光子晶体光纤中飞秒激光脉冲的传输特性和超连续谱的产生机理，给出了抽运脉冲在三种不同中心波长情况下输出光谱展宽并形成超连续谱的实际测量及理论模拟结果.研究表明：在零色散波长抽运时，光谱展宽以自相位调制为主，同时三阶色散的影响明显，传输脉冲在时域内出现振荡次峰.而在反常色散区抽运时，光谱展宽的初期以自相位调制为主，随后根据抽运功率的不同孤子自频移、高阶光孤子的裂变和四波混频效应会逐渐增强，进而成为光谱展宽的主要原因.与此相应，在时域中能明显看到孤子的形成和红移，飞秒传输脉 关键词： 光子晶体光纤 高非线性光子晶体光纤 飞秒脉冲激光 超连续谱     

飞秒脉冲作用下光子晶体光纤超连续谱的产生

采用钛宝石超快fs激光器泵浦2m长光子晶体光纤产生超连续谱,重点研究了不同输入功率下350～959nm波长范围内光谱的演变过程,实验中产生的超连续光谱宽度超过550nm分析表明,内脉冲喇曼散射和孤子自频移在开始阶段对光谱长波方向上的展宽起主要作用,这些新的频率成分与随后光谱向短波方向的拓展有密切关系.     

纳秒激光通过光子晶体光纤的光谱特性

超连续谱(sc)的产生是一种十分复杂的非线性现象,其特征是强光脉冲通过非线性介质后,脉冲谱宽被大大展宽,从几十nm到几百nm,故也称为白光光谱.光子晶体光纤(PCF)问世不久,人们就发现小模面积的光子晶体光纤是产生超连续谱的一种优良材料.     

LD泵浦掺铥(Tm3+)光纤激光器的数值分析

首先从掺铥光纤激光器的速率方程和光传输方程出发，建立数学模型，通过Matlab软件进行数值计算，分析了泵浦光和激光沿光纤的分布以及各能级离子数的变化。在不同掺杂浓度下，研究了小信号增益与入纤泵浦功率的关系以及泵浦光和激光功率与增益介质长度的关系。在不同泵浦功率下，研究了输出功率与输出耦合镜反射率的关系。进一步对不同泵浦吸收系数，研究了斜率效率和泵浦阈值与光纤长度的关系。分析结果表明：存在最佳光纤长度和最佳耦合输出透过率，使得激光输出功率达到最佳值。     

48-波长线形腔多波长掺铒光纤激光器

采用两个光纤环镜作为腔镜构成线形腔可调谐多波长掺铒光纤激光器.将铒光纤浸入77 K的液氮中,选择可调谐光纤环镜作为输出腔镜,利用Mach-Zehnder干涉仪的滤波特性和输出端光纤环镜反射率的宽带可调特性,获得了波长间隔～0.4 nm、最大波长数目48个的多波长激光的稳定输出,同时实现了在1525～1555 nm范围内,多波长激光运转区域的灵活调节.     

High-power all-fiber 1.0/1.5 μm dual-band pulsed MOPA source

The simultaneous dual-band pulsed amplification is demonstrated from an Er/Yb co-doped fiber(EYDF), and consequently a high-power all-fiber single-mode 1.0/1.5 μm dual-band pulsed master oscillator power amplifier(MOPA) laser source is realized for the first time, to the best of our knowledge, based on one singlegain fiber. The simultaneous outputs at 1061 and 1548 nm of the laser source have the maximum powers of 10.7 and 25.8 W with the pulse widths of 9.5 ps and 2 ns and the pulse repetition rates of 178 and 25 MHz, respectively. This EYDF MOPA laser source is seeded by two separate preamplifier chains operating at 1.0 and 1.5 μm wavebands. The dependence of the laser output powers on the length of the large-mode area EYDF, the ratio of the powers of the two signals launched into the booster amplifier, and the wavelength of the 1 μm seed signal are also investigated experimentally.