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Self-focusing and frequency broadening of an intense short-pulse laser in plasmas

机译:等离子体中强短脉冲激光的自聚焦和扩频

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An intense ultrafast laser pulse propagating through a plasma undergoes self focusing and self-phase-modulation as a result of relativistic mass nonlinearity. The inclusion of a quartic (r(4)) term in the expansion of the eikonal in the radial coordinate r allows the modification of the shape of the radial intensity profile. The front of the pulse, under the combined effects of time-dependent self-focusing and frequency downshifting, acquires a severely distorted temporal shape. The radial profile for I lambda (2)(mu) < 2.8 x 10(18) W/cm(2), where I is the axial laser intensity and (mu) is the laser wavelength in micrometers, is transformed from a Gaussian to a super-Gaussian because of the faster convergence of the marginal rays than the paraxial rays. In the opposite case of I lambda (2)(mu) > 2.8 x 10(18) W/cm(2) when nonlinear plasma permittivity approaches saturation, the radial profile in the axial region becomes broader than the Gaussian. (C) 2001 Optical Society of America. [References: 17]
机译:由于相对论质量非线性,在等离子体中传播的强超快激光脉冲会经历自聚焦和自相位调制。在径向坐标r的eikonal展开中包含四次(r(4))项可以修改径向强度轮廓的形状。在依赖于时间的自聚焦和降频的综合作用下,脉冲的前部获得了严重失真的时间形状。 Iλ(2)(μ)<2.8 x 10(18)W / cm(2)的径向轮廓由以下公式转换,其中I是轴向激光强度,而λμ是以微米为单位的激光波长。高斯到超高斯,因为边缘光线的收敛速度比近轴光线快。在I lambda(2)μ> 2.8 x 10(18)W / cm(2)的相反情况下,当非线性等离子体介电常数接近饱和时,轴向区域的径向轮廓将比高斯宽。 (C)2001年美国眼镜学会。 [参考:17]

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