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Investigation of short-wave edge in high power supercontinuum with different peak power

机译:不同峰值功率的大功率超连续谱中短波边缘的研究

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The peak power of pump pulse is a key factor in the generation of supercontinuum source. Observably, as the peakpower of the pump pulse increases, the spectral range of the supercontinuum becomes wider. In order to study the blueshift limit of PCF fiber at different peak powers, in our experiment, the change in peak power is achieved by introducinga different length of chirped fiber after the oscillator to vary the pulse width. The pump source is a self-made laser withpulse duration, operating wavelength and repetition rate of 12 ps, 1064 nm and 68 MHz, respectively, which are injectedinto the photonic crystal fiber after three stages of amplification. Finally, a supercontinuum with an average power of358 W in the spectral range of 466 nm to 2400 nm was achieved. Experiments have shown that the introduction of largepositive chirp has a significant effect on the supercontinuum of the 10 W class, but for a supercontinuum with asufficiently high average power (over 100 W level supercontinuum spectrum). after the peak power threshold isexceeded, further blue shift of the spectrum cannot be achieved by increasing the peak power, but the high peak powerhelps to improve the spectral flatness of the supercontinuum. The four-wave mixing, dispersive wave generation,radiation trapping with the soliton play much important role in the blue-shift of SC spectrum, but the short-wave edge islimited by the group velocity matching condition, which is determined by the dispersion characteristics of the PCF, notonly peak power of the pump pulse. In order to further extend the short-wave spectrum, other methods are required, forexample, changing the structural characteristic of the PCF, etc.
机译:泵浦脉冲的峰值功率是产生超连续谱源的关键因素。可以看出,作为高峰 泵浦脉冲的功率增加,超连续谱的光谱范围变宽。为了学习蓝 PCF光纤在不同峰值功率下的位移极限,在我们的实验中,峰值功率的变化是通过引入 在振荡器之后改变光纤的不同长度以改变脉冲宽度。泵浦光源是一种自制的激光器,具有 分别注入了12 ps,1064 nm和68 MHz的脉冲持续时间,工作波长和重复频率 经过三个阶段的放大后进入光子晶体光纤。最后,平均功率为 在466 nm至2400 nm的光谱范围内获得358W。实验表明,引入大 正chi对10 W级的超连续谱有显着影响,但对于具有10 W级的超连续谱, 足够高的平均功率(超过100 W级别的超连续谱)。在峰值功率阈值是 如果超出此范围,则无法通过增加峰值功率来实现频谱的进一步蓝移,但是会出现高峰值功率 有助于改善超连续谱的光谱平坦度。四波混频,色散波的产生, 孤子的辐射俘获在SC光谱的蓝移中起着重要作用,但短波边缘是 受组速度匹配条件的限制,该条件由PCF的色散特性确定,而不是 仅泵浦脉冲的峰值功率。为了进一步扩展短波频谱,需要使用其他方法 例如,改变PCF的结构特性等。

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