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Chirped-pulse-amplification system using a polarization-maintaining fiber stretcher matched to a Volume Bragg Grating

机译:使用偏振保持纤维担架的啁啾脉冲放大系统与卷布拉格光栅匹配

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Summary form only given. Chirped Pulse Amplification (CPA) systems using Ytterbium-doped fibers for amplification, Chirped Fiber Bragg Gratings (CFBG) for stretching, and diffraction gratings for compression are a reliable source of high-energy ultrashort pulses at wavelengths around 1μm [1]. Much more compact systems can be realized by replacing the grating compressor unit with Volume Bragg Gratings (VBG) and stretching in either VBGs [2] or CFBGs [3]. A disadvantage of these systems is the lack of dispersion variation and the difficulty of sufficiently exact dispersion matching in the production process of the VBG and the CFBG and the phase and amplitude ripples in these elements.Here we present a compact fiber CPA system similar to [4], consisting of a composite PM fiber stretcher and VBG compressor with dispersion matching up to the third order. Pulses with 10 nm bandwidth at 1030 nm central wavelength were generated. The VBG exhibits 13 nm spectral bandwidth and a stretching factor of 27 ps/nm, thus the pulses are stretched to 270 ps duration. Adjusting the length of positive and negative TOD PM fiber to 550 m and 20 m, respectively, we could achieve a compressed pulse duration of 270 fs FWHM (retrieved from the measured autocorrelation FWHM of 360 fs, see Fig. 1b). This value is close to the transform limit of 237 fs for the measured spectrum (Fig. 1b, inset). The achieved pulse peak power compared to the transform-limited case (temporal Strehl ratio) is calculated to 85%.
机译:摘要表格仅给出。啁啾使用掺镱光纤用于扩增脉冲放大(CPA)系统中,啁啾光纤光栅(CFBG)用于拉伸和压缩衍射光栅是高能量的超短脉冲的可靠来源的波长1μm左右[1]。更紧凑的系统可通过用卷布拉格光栅(VBG)代替光栅压缩机单元和拉伸在任一的VBG [2]或CFBGs [3]来实现。这些系统的缺点是缺乏分散变化和足够精确的分散匹配的在VBG和CFBG和在这些elements.Here相位和振幅波动的生产过程中的困难,我们提出类似于紧凑型光纤CPA系统[ 4],一复合PM光纤展宽器和VBG压缩机与分散匹配到第三级。产生与10纳米的带宽的脉冲在1030纳米的中心波长。的VBG表现出13纳米的光谱带宽和27个的PS / nm的拉伸系数,从而脉冲被拉伸至270皮秒的持续时间。调整正极和负极TOD PM光纤的长度550和20μm,分别,我们可以达到270个FS FWHM压缩脉冲持续时间(从所测量的自相关的360个FS FWHM检索,参见图1b)。此值是接近237个FS为测量光谱(图1b,插图)的变换极限。相比于变换极限情况下(时间Strehl比)所实现的脉冲峰值功率被计算为85 %。

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