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Soliton induced supercontinuum generation in photonic crystal fiber

机译:孤子诱导光子晶体光纤中的超连续谱产生

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Soliton induced supercontinuum (SC) generation using an index-guiding triangular photonic crystal fiber (PCF) is experimentally studied by pumping with 140-fs pulses at several wavelengths in the positive slope anomalous dispersion region. The focused beam incident upon the PCF core is first confirmed by in situ observation based on the reflection method to make sure accurate input coupling conditions. The influence of pumping wavelength on the spectral profile of SC is examined as a function of input peak power P0. Processes initiating SC generation are governed by the fission of higher-order solitons, which lead to the soliton self-frequency shift (SSFS) by intrapulse Raman scattering associated with blue-shifted Cherenkov type phase matched radiation. The fission of higher-order solitons is clearly observed in the input P0 dependent spectrum and a plot of the square root of frequency shift versus input P0. Further increase of input P0 leads to a new SSFS accompanied by an additional blue-shifted peak located at shorter wavelength than that of the previous one. These processes continue to develop successive blue-shifted and SSFS peaks as increasing the input P0, which determine the spectral width of SC. Spectral profile of SC is also dominated by these initial and growth processes. SC spectra obtained in the vicinity of zero dispersion wavelength shows smooth but relatively narrow, while SC generation at deep anomalous dispersion site exhibits broad bandwidth at relatively low P0. The input P0 required for approaching a saturated SC which is almost the same feature within the tuning pump wavelengths is decreased as increasing the degree of anomalous dispersion.
机译:通过在正斜率异常色散区域中以多个波长的140 fs脉冲泵浦,实验研究了使用折射率引导三角光子晶体光纤(PCF)产生的孤子诱导的超连续谱(SC)。首先通过基于反射法的原位观察来确认入射到PCF磁芯上的聚焦光束,以确保准确的输入耦合条件。根据输入峰值功率P0来检查泵浦波长对SC光谱曲线的影响。引发SC生成的过程受高阶孤子的裂变支配,其通过与蓝移Cherenkov型相位匹配辐射相关的脉冲内拉曼散射而导致孤子自频移(SSFS)。在依赖于输入P0的频谱中,可以清楚地观察到高阶孤子的裂变,以及频移平方根与输入P0的关系图。输入P0的进一步增加会导致出现一个新的SSFS,并伴有另一个蓝移峰,该峰的波长比前一个波长短。随着输入P0的增加,这些过程继续形成连续的蓝移和SSFS峰值,这决定了SC的光谱宽度。这些初始过程和生长过程也控制着SC的光谱轮廓。在零色散波长附近获得的SC光谱显示出平滑但相对较窄,而在深的异常色散位置处的SC生成在相对较低的P0处显示出宽带宽。随着异常色散程度的增加,接近饱和SC所需的输入P0减小,该饱和SC在调谐泵浦波长内几乎相同。

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