基于预啁啾控制的极宽带光参量放大

在以飞秒钛宝石放大系统的倍频光为抽运光和超连续白光为信号光的光参量放大中，针对抽运光的宽带特点，分析了一种新的极宽带相位匹配方法.结果表明，10nm的抽运光带宽可得到近400nm的相位匹配带宽，若抽运光带宽达到20nm,相位匹配带宽就能达到近600nm.零色散波长为800nm的光子晶体光纤产生的超连续谱经光纤传输后为二次啁啾，宽带抽运光经棱镜对展宽具有线性啁啾，满足了极宽带相位匹配方法所需要的光谱分布.理论计算了对输入脉冲进行预啁啾控制应选择的光纤长度和棱镜对在光路中的插入量，为实现极宽带光参量放大提供了     

基于预啁啾控制的极宽带光参量放大

在以飞秒钛宝石放大系统的倍频光为抽运光和超连续白光为信号光的光参量放大中,针对抽运光的宽带特点,分析了一种新的极宽带相位匹配方法.结果表明,10nm的抽运光带宽可得到近400nm的相位匹配带宽,若抽运光带宽达到20nm,相位匹配带宽就能达到近600nm.零色散波长为800nm的光子晶体光纤产生的超连续谱经光纤传输后为二次啁啾,宽带抽运光经棱镜对展宽具有线性啁啾,满足了极宽带相位匹配方法所需要的光谱分布.理论计算了对输入脉冲进行预啁啾控制应选择的光纤长度和棱镜对在光路中的插入量,为实现极宽带光参量放大提供了 关键词： 啁啾 极宽带相位匹配 光参量放大 光子晶体光纤     

双泵浦光子晶体光纤参量放大研究

利用光子晶体光纤在不同零色散波长附近具有不同色散的特性，研究了在零色散波长为780 nm和1550 nm附近的双泵浦光子晶体光纤参量放大过程.在780 nm附近，讨论了零色散波长变化对双泵浦光子晶体光纤参量放大的影响.数值模拟结果表明:当零色散波长发生微小的变化时，信号增益谱带宽会发生很大的变化.当两泵浦光之间的波长差值减小时，零色散波长的变化对参量放大的影响在很大程度上可以得到抑制，但是增益带宽会有一定的减小.依据这一原理，在1550 nm附近设计光子晶体光纤中的色散平坦光纤参量放大，在5 m长的光子晶体光纤中，当峰值功率为10 W时，得到了增益为65 dB，带宽达到420 nm且极为平坦的增益谱.     

熔锥型宽带耦合器的研制

介绍了全光纤熔融拉锥型3dB宽带耦合器的理论设计，根据理论设计制作了样品。应用耦合模理论分析了全光纤非对称熔融拉锥型耦合器的宽带特性；提出了3dB宽带耦合器的制作方案，在此基础上制作了样品；对样品进行测试，样品带宽大约为300nm(在1300nm～1600nm波长之间)，附加损耗小于0.5dB，完全达到了实用化的要求。     

Wideband subwavelength gratings for coupling between silicon-on-insulator waveguides and optical fibers

We propose and experimentally demonstrate a novel subwavelength grating coupler on silicon-on-insulator, for coupling to optical fibers with a wide optical bandwidth. Theoretical analysis and design optimization of the coupler are described. About 73?nm 1?dB bandwidth was experimentally demonstrated with -5.6 dB coupling efficiency. Better than -3.4 dB efficiency with 86?nm 1?dB bandwidth is predicted for these structures with optimized buried oxide thickness.     

Optical filter with tunable wavelength and bandwidth based on cholesteric liquid crystals

An optical filter with tunable wavelength and bandwidth has been demonstrated using two cholesteric liquid crystals configured in a reflection mode, in which the incident light is first reflected by one cholesteric liquid crystal and then by the other one. The central wavelength can be tuned from 527 nm to 574 nm and the bandwidth can be changed from 10 nm to 80 nm. It has potential applications in many fields, especially in optical communications and multispectral and hyperspectral imaging systems.     

分布式光纤布拉格光栅解调系统

提出并实现了一种可满足工程实用要求的分布式光纤布拉格光栅解调系统。该系统通过可调谐光纤F-P滤波器的连续扫描实现波长信号的解调。该传感系统扫描带宽50nm,单点工作带宽5nm,对一股应用系统每根单纤可设20∽30个点,分辨力5pm。     

Novel split-band erbium-doped fiber amplifier

In this paper we design a 120 nm bandwidth erbium-doped fiber amplifier using a seed light injection method for the first time. It is shown that when the wavelength of the seed light varies from 1520 to 1570 nm, the gain at 1610 nm reaches maximum near 1553 nm and increases as the seed light power. Based on the method, a novel split-band EDFA configuration is designed. The split-band architecture employs a 1550/1610 nm waveband multiplexer/demultiplexer and two independent sub-bands which pass in parallel through separate branches of the optical amplifier. The signals at independent sub-bands are combined and flattened before output, resulting in a broadband gain-flattened optical amplifier with 120 nm bandwidth.     

非对称型光学交错梳状滤波器

提出了一种基于Gires-Tournois腔的非对称型光学交错梳状滤波器。理论上,通过调整两个波片的偏振延迟和Gires-Tournois腔的反射率,可以获得任意光谱带宽比的非对称型交错梳状滤波器件。分别对输出带宽比M=1∶3和M=1∶7的非对称型交错梳状滤波器的输出进行了数值模拟,确定两个波片的延迟和Gires-Tournois腔的反射率。分别设计和研制出了输出光谱带宽比M=1∶3和M=1∶7的器件,其中M=1∶3器件的两个输出通道的3 dB带宽分别为0.385 nm和1.161 nm,比值为M=1∶3.02,M=1∶7器件的两个输出通道的3 dB带宽分别为0.191 nm和1.331 nm比值M=1∶6.75。实验结果(光谱带宽比)与设计要求基本符合。     

Amplification of fluorescence using collinear picosecond optical parametric amplification at degeneracy

We demonstrate the output characteristic of broadband parametric amplification of incoherent light pulses in a 355-nm pumped degenerate picosecond optical parametric amplification with either saturated or unsaturated amplification.The optical parametric amplifier is seeded by the fluorescence generated in a solution of pyridine-1 dye in ethanol.With the saturated amplification,we can obtain high energy incoherent light pulses,whose full width at half maximum bandwidth varies from 16 nm to 53 nm for the different phase matching angles near degeneracy.Moreover,the unsaturated bandwidth of the amplified pulses fits well to the calculated result at degeneracy.Selecting s-polarized fluorescence with a Glan-Taylor prism,the maximum bandwidth of the amplified fluorescence is found to be 59 nm for a purely s-polarized seed.The maximum output energy is 0.67 mJ for the optical parametric amplifier.By using an optical filter and compressor,the generated high energy incoherent light has great potential as the incoherent pump,signal or idler wave of a parametric down-conversion process,so that a wave with a high degree of coherence can be generated from an incoherent pump light.