Gordienko S, Pukhov A, Shorokhov O, Baeva T
Institut für Theoretische Physik I, Heinrich-Heine-Universität Düsseldorf, Düsseldorf D-40225, Germany.
Phys Rev Lett. 2005 Mar 18;94(10):103903. doi: 10.1103/PhysRevLett.94.103903.
We demonstrate analytically and numerically that focusing of high harmonics produced by the reflection of a few-femtosecond laser pulse from a concave plasma surface opens a new way to unprecedentally high intensities. The key features allowing the boosting of the focal intensity are the harmonics coherency and the small exponent of the power-law decay of the harmonics spectrum. Using similarity theory and direct particle-in-cell simulations, we find that the intensity at the focus scales as I(CHF) alpha a(3)(0)I(0), where a(0) and I(0) alpha a(2)(0) are the dimensionless relativistic amplitude and the intensity of the incident laser pulse. The scaling suggests that due to the coherent harmonic focusing (CHF), the Schwinger intensity limit can be reached using lasers with I(0) approximately 10(22) W/cm(2). The pulse duration at the focus scales as tau(CHF) alpha 1/a(2)(0) and reaches the subattosecond range.
我们通过解析和数值方法证明,由飞秒激光脉冲从凹面等离子体表面反射产生的高次谐波聚焦,为实现前所未有的高强度开辟了一条新途径。实现聚焦强度增强的关键特性是谐波的相干性和谐波谱幂律衰减的小指数。利用相似性理论和直接的粒子模拟,我们发现焦点处的强度按(I(CHF) \alpha a(3)(0)I(0))缩放,其中(a(0))和(I(0) \alpha a(2)(0))分别是无量纲相对论振幅和入射激光脉冲的强度。这种缩放表明,由于相干谐波聚焦(CHF),使用强度约为(10(22) W/cm(2))的激光可以达到施温格强度极限。焦点处的脉冲持续时间按(\tau(CHF) \alpha 1/a(2)(0))缩放,并达到亚阿秒范围。