首页> 外文会议>Nonlinear Frequency Generation and Conversion: Materials and Devices XVII >Nearly fully compressed 1053 nm pulses directly obtained from 800 nm laser-seeded Photonic Crystal Fiber below zero dispersion point
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Nearly fully compressed 1053 nm pulses directly obtained from 800 nm laser-seeded Photonic Crystal Fiber below zero dispersion point

机译:从零色散点以下的800 nm激光种子光子晶体光纤直接获得几乎完全压缩的1053 nm脉冲

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We report a simple robust and broadly spectral-adjustable source generating near fully compressed 1053 nm 62 fs pulses directly out of a highly-nonlinear photonic crystal fiber. A dispersion-nonlinearity balance of 800 nm Ti:Sa 20 fs pulses was obtained initially by negative pre-chirping and then launching the pulses into the fibers' normal dispersion regime. Following a self-phase modulation spectral broadening, some energy that leaked below the zero dispersion point formed a soliton whose central wavelength could be tuned by Self-Frequency-Raman-Shift effect. Contrary to a common approach of power, or, fiber-length control over the shift, here we continuously varied the state of polarization, exploiting the Raman and Kerr nonlinearities responsivity for state of polarization. We obtained soliton pulses with central wavelength tuned over 150 nm, spanning from well below 1000 to over 1150 nm, of which we could select stable pulses around the 1μm vicinity. With linewidth of > 20 nm FWHM Gaussian-like temporal-shape pulses with ~ 62 fs duration and near flat phase structure we confirmed high quality pulse source. We believe such scheme can be used for high energy or high power glass lasers systems, such as Nd or Yb ion-doped amplifiers and systems.
机译:我们报告了一个简单的健壮且可宽频谱可调的光源,直接从高度非线性的光子晶体光纤中产生了接近完全压缩的1053 nm 62 fs脉冲。首先通过负预-,然后将脉冲发射到光纤的正常色散状态,获得800 nm Ti:Sa 20 fs脉冲的色散非线性平衡。自相位调制频谱展宽后,泄漏到零色散点以下的一些能量形成了一个孤子,其中心波长可以通过自频拉曼位移效应进行调谐。与通常的功率控制方法或对位移的光纤长度控制方法相反,在这里,我们不断利用偏振态的拉曼和Kerr非线性响应性来不断改变偏振态。我们获得了中心波长调谐在150 nm以上,从远低于1000到超过1150 nm的孤子脉冲,其中我们可以选择1μm附近的稳定脉冲。线宽> 20 nm FWHM高斯样时间形状脉冲,持续时间约62 fs,相位结构接近平坦,我们确认了高质量的脉冲源。我们相信这种方案可用于高能量或高功率玻璃激光器系统,例如Nd或Yb离子掺杂放大器和系统。

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