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Efficient spectral conversion and temporal compression of femtosecond pulses in SF6

机译:在SF 6 中有效的光谱转换和逐秒脉冲的时间压缩

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A Ti:sapphire based laser system provided 30-fs pulses centered at 800 nm with up to 3 mJ energy was used in the experiment. The input beam was focused by a concave mirror with radius of 3 m into a 1.5 m long glass cell. No iris-diaphragm or other beam reshaping tools were used for filament adjustment. The gas cell was filled with SF6 or for comparison with Ar at variable pressure of 0.1–0.7 bar. After the filament start point the laser radiation was spatially confined and propagated through the entire gas cell. Diameter of central, bright part of the beam was in a range of 2 mm directly after the output window. The output spectra recorded directly after the cell filled gases are shown in Fig. 1. The filament in SF6 demonstrate qualitatively different spectral shape, as compared to Ar, with dramatic enhancement in frequency conversion out of fundamental spectral range especially towards the higher-frequency domain. FWHM of the detected spectrum reached almost octave bandwidth of 440–875 nm.
机译:Ti:基于蓝宝石的激光系统提供了30-FS脉冲以800nm为中心,在实验中使用了高达3 MJ的能量。输入光束通过凹面镜聚焦,半径为3μm到1.5米长的玻璃单元中。没有使用虹膜隔膜或其他光束重塑工具用于灯丝调节。将气体电池填充有SF 6 或以0.1-0.7巴的可变压力与AR进行比较。在灯丝开始点之后,激光辐射在空间上限制并通过整个气体细胞传播。中央的直径,梁的明亮部分在输出窗口后直接在2毫米的范围内。在细胞填充气体之后直接记录的输出光谱在图1中示出。与AR相比,SF 6 中的灯丝展示了定性不同的光谱形状,其频率转换出的基本光谱的剧烈增强距离较高频域的范围。检测到的频谱的FWHM几乎达到了440-875 nm的八度带宽。

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