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自由空间中激光诱导的线性场粒子加速。

Laser-Induced Linear-Field Particle Acceleration in Free Space.

机构信息

Department of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, 02139, Massachusetts, USA.

Singapore Institute of Manufacturing Technology, 2 Fusionopolis Way, Innovis, 138634, Singapore.

出版信息

Sci Rep. 2017 Sep 11;7(1):11159. doi: 10.1038/s41598-017-11547-9.

Abstract

Linear-field particle acceleration in free space (which is distinct from geometries like the linac that requires components in the vicinity of the particle) has been studied for over 20 years, and its ability to eventually produce high-quality, high energy multi-particle bunches has remained a subject of great interest. Arguments can certainly be made that linear-field particle acceleration in free space is very doubtful given that first-order electron-photon interactions are forbidden in free space. Nevertheless, we chose to develop an accurate and truly predictive theoretical formalism to explore this remote possibility when intense, few-cycle electromagnetic pulses are used in a computational experiment. The formalism includes exact treatment of Maxwell's equations and exact treatment of the interaction among the multiple individual particles at near and far field. Several surprising results emerge. We find that electrons interacting with intense laser pulses in free space are capable of gaining substantial amounts of energy that scale linearly with the field amplitude. For example, 30 keV electrons (2.5% energy spread) are accelerated to 61 MeV (0.5% spread) and to 205 MeV (0.25% spread) using 250 mJ and 2.5 J lasers respectively. These findings carry important implications for our understanding of ultrafast electron-photon interactions in strong fields.

摘要

自由空间中的线性场粒子加速(与需要粒子附近组件的直线加速器等几何形状不同)已经研究了 20 多年,其最终能够产生高质量、高能多粒子束的能力仍然是一个非常感兴趣的话题。当然,可以认为,由于自由空间中禁止一阶电子-光子相互作用,自由空间中的线性场粒子加速是非常值得怀疑的。然而,当在计算实验中使用强、少周期电磁脉冲时,我们选择开发一种准确且真正可预测的理论形式来探索这种遥远的可能性。该形式包括对麦克斯韦方程组的精确处理以及对近场和远场中多个单个粒子之间相互作用的精确处理。出现了一些令人惊讶的结果。我们发现,与自由空间中的强激光脉冲相互作用的电子能够获得大量与场幅度成线性比例的能量。例如,使用 250mJ 和 2.5J 激光,30keV 的电子(2.5%的能散)分别被加速到 61MeV(0.5%的能散)和 205MeV(0.25%的能散)。这些发现对我们理解强场中的超快电子-光子相互作用具有重要意义。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a4f4/5593863/d875ef9039b4/41598_2017_11547_Fig1_HTML.jpg

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