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Effect of transverse magnetic fields on high-harmonic generation in intense laser-solid interaction

机译:横向磁场对强激光-固体相互作用中高次谐波产生的影响

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摘要

The effect of transverse magnetic fields on surface high-harmonic generation in intense laser-solid interactions is investigated. It is shown that the longitudinal motion of electrons can be coupled with the transverse motion via the magnetic fields, which lead to even-order harmonics under normal laser incidence. The dependence of the coupling efficiency and hence even harmonic generation with preplasma scale length and magnetic field strength are presented based upon particle-in-cell simulations. When the magnetic field is parallel to the laser electric field, the spectral intensity of the second harmonic is proportional to the magnetic field strength in a wide range up to 160 MG, while the situation with the magnetic field perpendicular to the laser electric field is more complicated. The second harmonic generation due to the magnetic field also tends to increase with the plasma density scale lengths, which is different from the high-harmonic generation by the oscillating mirror mechanism. With the increase of the laser spot size from a laser wavelength lambda(L), both the magnetic field-induced harmonics and oscillating mirror high harmonics tend to increase first and then become saturated after 3 lambda(L). The magnetic field-induced second harmonic may be used to evaluate large self-generated magnetic fields developed near the critical density region and the preplasma conditions.
机译:研究了横向磁场对强激光-固体相互作用中表面高次谐波产生的影响。结果表明,电子的纵向运动可以通过磁场与横向运动耦合,从而在正常的激光入射下导致偶次谐波。基于细胞内颗粒模拟,给出了耦合效率的依赖性,因此甚至产生了具有等离子体前标尺长度和磁场强度的谐波。当磁场平行于激光电场时,二次谐波的光谱强度在高达160 MG的宽范围内与磁场强度成正比,而磁场垂直于激光电场的情况则更多复杂。由于磁场引起的二次谐波的产生也趋于随着等离子体密度标度长度的增加而增加,这与通过振荡镜机构产生的高谐波产生不同。随着激光光斑尺寸从激光波长λ(L)开始增加,磁场感应的谐波和振荡镜高谐波都倾向于先增大,然后在3λ(L)之后达到饱和。磁场感应的二次谐波可用于评估在临界密度区域和等离子条件附近产生的大型自生磁场。

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