Zhang Y X, Rykovanov S, Shi Mingyuan, Zhong C L, He X T, Qiao B, Zepf M
Center for Applied Physics and Technology, HEDPS, SKLNPT, and School of Physics, Peking University, Beijing 100871, China.
Helmholtz Institute Jena, 07743 Jena, Germany.
Phys Rev Lett. 2020 Mar 20;124(11):114802. doi: 10.1103/PhysRevLett.124.114802.
A new regime in the interaction of a two-color (ω,2ω) laser with a nanometer-scale foil is identified, resulting in the emission of extremely intense, isolated attosecond pulses-even in the case of multicycle lasers. For foils irradiated by lasers exceeding the blow-out field strength (i.e., capable of fully separating electrons from the ion background), the addition of a second harmonic field results in the stabilization of the foil up to the blow-out intensity. This is then followed by a sharp transition to transparency that essentially occurs in a single optical cycle. During the transition cycle, a dense, nanometer-scale electron bunch is accelerated to relativistic velocities and emits a single, strong attosecond pulse with a peak intensity approaching that of the laser field.
一种双色(ω,2ω)激光与纳米级箔相互作用的新机制被发现,这导致了极强烈、孤立的阿秒脉冲的发射——即使在多周期激光的情况下也是如此。对于被超过吹出场强(即能够使电子与离子背景完全分离)的激光照射的箔,加入二次谐波场会使箔在达到吹出强度之前保持稳定。随后会迅速过渡到透明状态,这一过程基本上在单个光学周期内发生。在过渡周期中,一个密集的纳米级电子束被加速到相对论速度,并发射出一个单一的、强烈的阿秒脉冲,其峰值强度接近激光场的峰值强度。