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Formation and amplification of flat top picosecond pump pulses for OPCPA systems

机译:用于OPCPA系统的平顶皮秒泵浦脉冲的形成和放大

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OPCPA systems based on non-collinear parametric amplification provides amplification bandwidths sufficient for formation of sub-10 fs pulses with peak powers of terawatt level [1], however both total gain and gain spectral bandwidth sensitively depend on spatial shape of the pump pulses [1]. Contrary to the Gaussian pulses, the pump pulses with a rectangular temporal profile would provide a uniform gain for all chirped seed spectral components, thereby avoiding spectral distortion and would allow to achieve higher pump-to-signal conversion efficiency and improve amplified pulse contrast ration with reference to parametric super fluorescence background [2]. For the pump pulses of 30–100 ps duration the application of spectral and electro optical pulse shaping methods is rather limited due to narrow pulse spectrum (fractions of nanometer) and insufficient temporal resolution of optoelectronic schemes, while pulse shape obtained by using pulse stacking methods is extremely sensitive to mechanical and thermal perturbations in the interferometric scale.
机译:基于非共线参数放大的OPCPA系统提供的放大带宽足以形成峰值功率为TB的亚10 fs脉冲[1],但是总增益和增益频谱带宽均敏感地取决于泵浦脉冲的空间形状[1] ]。与高斯脉冲相反,具有矩形时间分布的泵浦脉冲将为所有chi种子频谱分量提供均匀的增益,从而避免频谱失真,并可以实现更高的泵浦至信号转换效率,并提高放大后的脉冲对比度。参考参量超荧光背景[2]。对于持续时间为30–100 ps的泵浦脉冲,由于窄的脉冲光谱(纳米级数)和光电方案的时间分辨率不足,光谱和电光脉冲整形方法的应用受到了很大限制,而使用脉冲堆叠方法获得的脉冲形状对干涉尺度的机械和热扰动极为敏感。

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