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Management of interactions between Raman induced solitons and dispersive waves in photonic crystal fibers at the advanced stage of supercontinuum generation

机译:超连续谱产生后期的拉曼诱发孤子与光子晶体光纤中色散波之间相互作用的管理

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We have studied experimentally [1] and numerically the dynamics of negatively prechirped pulses with different input peak powers in PCF with resultant spectral broadening and supercontinuum generation. After the initial compression stage of a few cm, the input pulse, as it corresponds to a high order soliton, undergoes fission into multiple fundamental solitons [2] accompanied by emission of non-soliton radiation [3]. Spectra of these solitons are shifted toward longer wavelengths by Raman induced frequency shift [4] (RIF) producing spectral broadening at the red edge of the spectrum. We show that the radiation emitted by stonger solitons can be absorbed by trailing solitons, altering their path. This can lead to additional soliton quasi-elastic or quasi-plastic collisions and to an enhancement of the power in certain spectral regions of the generated supercontinuum or, even more interestingly, in the generation of new frequency components. The process of interaction of solitons with dispersive waves is extremely sensitive to manageable input pulse parameters. For example small variations in initial chirp parameter can result in variations of the collision mode between solitons from a quasi-elastic to a quasi-plastic [5]. Fig.1 demonstrates an example of a plastic collision at C = −1.16 when the colliding solitons combine into one giant solitary wave which keeps propagating at large group velocity. In the process a strong spectral band is generated, which extends the SC spectrum beyond 1500 nm.
机译:我们已经进行了实验研究[1],并在数值上对PCF中具有不同输入峰值功率的负线性调频脉冲的动力学进行了研究,从而产生了谱展宽和超连续谱。在几厘米的初始压缩阶段之后,与高阶孤子相对应的输入脉冲会裂变为多个基本孤子[2],并伴有非孤子辐射的发射[3]。这些孤子的光谱通过拉曼引起的频移[4](RIF)移向更长的波长,从而在光谱的红色边缘产生光谱加宽。我们表明,石ger孤子发出的辐射可以被尾随的孤子吸收,改变它们的路径。这可能导致额外的孤子准弹性或准塑性碰撞,并导致所生成的超连续谱的某些频谱区域中功率的增强,或者甚至更有趣地是,在生成新的频率分量时。孤子与色散波的相互作用过程对可控输入脉冲参数极为敏感。例如,初始线性调频参数的微小变化会导致孤子之间的碰撞模式从准弹性到准塑性变化[5]。图1展示了一个例子,当碰撞的孤子组合成一个巨大的孤波时,在C = −1.16时发生塑性碰撞,该孤波以较大的群速度继续传播。在此过程中会产生一个很强的光谱带,它将SC光谱扩展到1500 nm以上。

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