钕玻璃链中50tw亚皮秒脉冲的产生及聚焦性研究

C. Rouyer, E. Mazataud, I. Allais, A. Pierre, S. Seznec
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摘要

为了研究物质与这种强脉冲的相互作用,近年来在开发超亮光源方面进行了大量的工作。一个非常有趣的目标是获得1019 W/cm2以上的强度,因为在这个范围内预计会出现新的效应,如相对论性电子、相干x射线短脉冲、密集和热等离子体中的巨大冲击压力……固体宽带放大介质耦合啁啾脉冲放大技术[1]是获得强脉冲和超短脉冲的最直接途径。钛蓝宝石、Cr3+:LiCAF、亚历山大变石是较好的介质。Nd-Glass有可能放大脉冲的时间只超过250秒,但由于现有放大器的尺寸,可以放大能量高达千焦耳的脉冲。在第一个实验中,我们从耦合到光纤的cw锁模nd - yag振荡器开始,注入到Nd-Glass再生放大器和Nd-Glass电源链中。然后采用双通道压缩方案对60 J啁啾脉冲进行压缩。然后输出20个TW-24J和1.2 ps脉冲[2]。然而,该系统的强度对比很差。我们已经开发了一种基于双光纤方案[3]和Ti:S放大器的新源,允许获得干净的450 fs脉冲。啁啾脉冲在再生放大器中发送,能够将脉冲能量从几个nJ增加到1 mJ,而增益不会缩小,光谱带宽为8 nm[图1,图2]。这些脉冲随后被送入Nd-Glass电源链并进一步压缩。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Generation of 50 TW subpicosecond pulses in a Nd-Glass Chain and focusability study
There has been recently a great deal of works on the development of ultrabright sources in order to study the interaction of matter with such intense pulses. A very interesting goal is to obtain intensities above 1019 W/cm2 because new effects are expected in this regime such as relativistic electrons, coherent X-Ray short pulses, huge shock pressures in dense and hot plasmas,... Solid state broadband amplifying media coupled to the Chirped Pulse Amplification technique [1] is the most direct way to get intense and ultrashort pulses. Ti-Sapphire, Cr3+:LiCAF, Alexandrite are such good media. Nd-Glass has the potential to amplify pulses only longer than 250 fs but because of the available amplifiers size allows very energetic pulses up to kilojoules. In a first experiment we started from a CW-Mode-Locked-Nd-YAG oscillator coupled to a fiber, injected into a Nd-Glass regenerative amplifier and in a Nd-Glass power chain. The 60 J chirped pulses were then compressed using double pass compressing scheme. 20 TW-24J and 1.2 ps pulses are then delivered [2]. However the intensity contrast in this system is very poor. We have developed a new source based on a double fiber scheme [3] and a Ti:S amplifier allowing to get clean 450 fs pulses. The chirped pulse is sent in a regenerative amplifier able to increase the pulse energy from a few nJ to 1 mJ without gain narrowing for a 8 nm spectral bandwidth [Fig. 1, Fig. 2.]. These pulse is then sent into the Nd-Glass power chain and further compressed.
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