首页> 外文会议>2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference >Sub-20 fs energetic near-IR pulses generated with cascaded soliton compression in short lithium niobate crystals
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Sub-20 fs energetic near-IR pulses generated with cascaded soliton compression in short lithium niobate crystals

机译:在短铌酸锂晶体中通过级联孤子压缩产生的低于20 fs的高能近红外脉冲

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Access to energetic µJ-multi-mJ ultra-short fs laser pulses is crucial for many research topics today and in the future. Typically, laser amplifier pulses are an order of magnitude longer that the single-cycle limit making pulse compression desirable. We use soliton compression using cascaded quadratic nonlinearities to compress energetic pulses towards few-cycle duration. Specifically, we obtain sub-20 fs solitons by launching 0.25 mJ 55 fs pulses at 1300 nm in a lithium niobate (LN) crystal as short as 1 mm. The solitons are formed by phase-mismatched (cascaded) second-harmonic generation (SHG): upon propagation little second harmonic (SH) is generated, but the fundamental wave (FW) will instead experience a strong Kerr-like nonlinear phase shift. The total FW refractive index is n1+nIcubicI1 where nIcubic = nISHG +nIKerr. It includes contributions from the material Kerr nonlinearity nIKerr > 0 and the cascaded quadratic nonlinearities nISHG ≃ − 4πd2eff/cε0λ1n21n2Δk. The goal is to achieve a self-defocusing nonlinearity nIcubic < 0 through a large phase mismatch Δk ≫ 0. In this case, solitons can be formed with normal dispersion, which means anywhere in the visible and near-IR. Moreover it is possible to compress multi-mJ pulse-energies because there are no self-focusing problems [1].
机译:获得高能量的µJ-multi-mJ超短fs激光脉冲对于当今和未来的许多研究课题都是至关重要的。通常,激光放大器脉冲比单周期限制长一个数量级,因此需要进行脉冲压缩。我们使用级联二次非线性的孤子压缩将高能脉冲压缩到几个周期的持续时间。具体来说,我们通过在短至1 mm的铌酸锂(LN)晶体中在1300 nm处发射0.25 mJ 55 fs脉冲来获得20 fs以下的孤子。孤子是由相位不匹配(级联)二次谐波生成(SHG)形成的:传播时几乎不会产生二次谐波(SH),但基波(FW)会经历强烈的Kerr样非线性非线性相移。总FW折射率为n 1 + n I 三次 I 1 ,其中n I 三次 = n I SHG + n I Kerr 。它包括来自材料Kerr非线性n I Kerr > 0和级联二次非线性n I SHG contributions的贡献−4πd 2 eff /cε 0 λ 1 n 2 1 n 2 Δk。目的是通过大的相位失配Δk≫ 0来实现自散焦非线性n I 三次 <0。在这种情况下,可以形成具有正常色散的孤子,这意味着可见光和近红外光的任何地方。此外,由于不存在自聚焦问题,因此有可能压缩多mJ的脉冲能量。

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