Liu C S, Tripathi V K
Institute for Plasma Research, University of Maryland, College Park 20742, USA.
J Opt Soc Am A Opt Image Sci Vis. 2001 Jul;18(7):1714-8. doi: 10.1364/josaa.18.001714.
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 (r4) 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 1018 W/cm2, where I is the axial laser intensity and lambda(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/cm2 when nonlinear plasma permittivity approaches saturation, the radial profile in the axial region becomes broader than the Gaussian.
一个强超短激光脉冲在等离子体中传播时,由于相对论性质量非线性效应会发生自聚焦和自相位调制。在径向坐标(r)中对光程函数展开式包含四次项((r^4)),这使得径向强度分布的形状得以改变。在随时间变化的自聚焦和频率下移的共同作用下,脉冲前沿会获得严重畸变的时间形状。对于(I(\lambda)^2(\mu) < 2.8×10^{18} W/cm^2)(其中(I)是轴向激光强度,(\lambda(\mu))是以微米为单位的激光波长),由于边缘光线比傍轴光线收敛得更快,其径向分布从高斯分布转变为超高斯分布。在相反的情况(I(\lambda)^2(\mu) > 2.8×10^{18} W/cm^2),即非线性等离子体介电常数接近饱和时,轴向区域的径向分布会比高斯分布更宽。