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Excitation of individual Raman Stokes lines of up-to 9th order using rectangular shaped optical pulses at 530 nm

机译:在530nm处使用矩形光脉冲的矩形光脉冲的各个拉曼斯托克斯线的激励

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We demonstrate the selective excitation of Raman Stokes lines of up-to 9th order with relatively high extinction ratio pumped by rectangular shaped optical pulses at 530 nm of 100 ns duration. The rectangular shaped optical pulses at 530 nm were generated by frequency doubling of an adaptively pulse shaped fiber MOPA operating at 1060 nm. This kind of pulse shape is optimal for frequency conversion since all parts of the pulse experiences the same Raman gain. Therefore, it is possible for a pulse to transfer all of its energy through sequential frequency Raman shifts to successive order Stokes components. Consequently, by adjusting the pump power it is possible to achieve selective excitation of the Raman shift with little residual pump powers. Here, we have achieved extinction ratio as much as 15 dB from successive Stokes lines by coupling 530 nm light in a 1 km long Pirelli Freelight fiber. In addition, we were able to obtain up-to 9th order Stokes shift by launching 5 W of average pump power to the Raman gain medium. Maximum Stokes shifted power of 54 mW was recorded for a launched pump power of 5W. We attribute this to the large background loss of silica fibre in the visible region.
机译:我们展示了在100ns持续时间的530nm处被矩形光脉冲泵浦的相对高的第9阶的拉曼斯托克斯线的选择性激发。 530nm处的矩形光脉冲由在1060nm下操作的自适应脉冲形纤维MOPA的频率加倍产生。这种脉冲形状对于频率转换是最佳的,因为脉冲的所有部分都经历了相同的拉曼增益。因此,脉冲可以通过顺序频率拉曼转移到连续顺序的斯托克地区组件来传送所有能量。因此,通过调节泵功率,可以实现具有很少的残留泵功率的拉曼转变的选择性激发。在这里,我们通过在1 km长的Pirelli Freelight纤维中耦合530nm光,从连续的斯托克斯线上实现了远的斯托克斯线。此外,我们能够通过向拉曼增益介质发射5W平均泵电源来获得最新的第9阶Stokes。最大斯托克斯换档功率为54兆瓦的推出泵功率为5W。我们将这一点归因于可见区域中的二氧化硅纤维的大背景丧失。

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