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Fiber amplifier CPA system using divided-pulse amplification for multi-mJ extraction

机译:使用分脉冲放大的光纤放大器CPA系统用于多mJ提取

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Ytterbium-doped fiber chirped-pulse amplification (FCPA) systems have seen an unprecedented power development in recent years. Thus, nowadays they are capable of producing multi-GW peak powers at pulse energies beyond one millijoule [1]. In order to avoid both nonlinear pulse distortions and optically induced damage in these systems, the intensity inside of the signal core of the amplifying fiber has to be reduced by many orders of magnitude. This is achieved by employing fibers with extremely large mode-field diameters (MFDs) and by using largely stretched pulses. However, the scaling of the MFD is typically restricted by production tolerances of the particular fiber design. On the other hand, the geometrical dimension of the laser system typically restrict the attainable stretched pulse durations. The performance of femtosecond FCPA systems could be further improved by using spatially [2] or temporally separated amplification, the latter approach also known as divided-pulse amplification (DPA) [3]. Up to now in DPA the separation of the pulses was usually limited to a few picoseconds.
机译:近年来,掺光纤chi脉冲放大(FCPA)系统得到了空前的发展。因此,如今,它们能够以超过1毫焦耳的脉冲能量产生多GW峰值功率[1]。为了避免这些系统中的非线性脉冲畸变和光学上的损坏,放大光纤信号芯内部的强度必须降低许多数量级。这可以通过使用具有极大模场直径(MFD)的光纤以及使用较大的拉伸脉冲来实现。但是,MFD的缩放通常受特定光纤设计的生产公差限制。另一方面,激光系统的几何尺寸通常会限制可达到的扩展脉冲持续时间。飞秒FCPA系统的性能可以通过使用空间[2]或时间上分开的放大来进一步提高,后者的方法也称为分脉冲放大(DPA)[3]。迄今为止,在DPA中,脉冲间隔通常限制在几皮秒内。

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