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NUMERICAL SIMULATIONS OF HARMONICS GENERATION BY THE REFLECTION OF AN INTENSE LINEARLY POLARIZED LASER BEAM NORMALLY INCIDENT ON AN OVERDENSE PLASMA

机译:一种谐波线性偏振激光束的反射通常入射在泛抗血浆中的数值模拟

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We use an Eulerian Vlasov code for the numerical solution of the one-dimensional relativistic Vlasov-Maxwell equations for both electrons and ions [1, 2], and a particle-in-cell (PIC) code[3] to study the generation of harmonics in the reflection of a high intensity linearly polarized laser wave normally incident on an overdense plasma. The oscillation of the laser wave at the plasma edge creates an oscillating space-charge, giving rise to an oscillating electric field. If the intensity of the wave is sufficiently high to make the oscillation of the electrons relativistic, then the plasma edge oscillates nonlinearly in the field of the laser beam, which results in an important distortion in the reflected wave, associated with the generation of harmonics. We consider the case when the laser beam wavelength λ is much greater than the scale length of the gradient in the plasma density at the edge L_(edge) (λL_(edge)), and n/n_c =100. The two codes show general qualitative agreement for the mechanisms of harmonics generation, although some quantitative details differ somewhat.
机译:我们使用Eulerian Vlasov代码进行电子和离子[1,2]的一维相对论Vlasov-MaxWell方程的数值解[1,2],以及用于研究生成的粒子 - 细胞(PIC)代码[3]高强度线性偏振激光波通常入射在过阵等离子体上的谐波。等离子体边缘的激光波的振荡产生振荡空间电荷,从而产生振荡电场。如果波的强度足够高,以使电子相对论的振荡,则等离子体边缘在激光束的场上非线性地振荡,这导致反射波的重要变形,与谐波的产生相关联。当激光束波长λ远高于边缘L_(边缘)(λ L_(边缘))和N / N_C = 100的等离子体密度中的梯度的刻度长度大得多。这两项代码显示了谐波生成机制的一般定性协议,尽管一些定量细节有些不同。

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