Author Affiliations
1School of Science, Changchun University of Science and Technology, Changchun 130022, China2Shandong Provincial Engineering and Technical Center of Light Manipulations, Shandong Provincial Key Laboratory of Optics and Photonic Device, School of Physics and Electronics, Shandong Normal University, Jinan 250358, China3School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 101407, Chinashow less
Fig. 1. Schematic diagram of experimental setup. M, 800 nm HR mirror; G, grating; CL, cylindrical lens; LC-SLM, liquid crystal spatial light modulator; MLA, microlens array; L, plano-convex lens; FS, fused silica; DM, dichroic mirror; IS, integrating sphere.实验装置示意图(M, 800 nm高反镜; G, 光栅; CL, 柱面镜; LC-SLM, 液晶空间光调制器; MLA, 微透镜阵列; L, 平凸透镜; FS, 熔融石英; DM, 二向色镜; IS, 积分球)
Fig. 2. (a) Evolution trend of supercontinuum generation by the spatiotemporal modulation femtosecond pulse filamentation with the increasing of iterative generation; (b) supercontinuum spectra of several typical iterative generations.(a)时空调制飞秒脉冲成丝的超连续辐射随迭代代数的演化; (b)典型迭代代数对应的超连续辐射光谱
Fig. 3. Spectral intensity integration (400−700 nm) of the supercontinuum as a function of the iterative generation.超连续辐射光谱积分(400−700 nm波段)随迭代代数的变化
Fig. 4. Initial envelopes of shaped laser pulse with typical iteration generations of (a) 1, (b) 3, (c) 8 and (d) 17, respectively.典型迭代代数对应整形激光脉冲初始包络, 图中迭代代数依次为(a) 1, (b) 3, (c) 8和(d) 17