Role of high ponderomotive energy in laser-induced nonsequential double ionization

被引:17
|
作者
Shaaran, T. [1 ]
Camus, N. [1 ]
Dura, J. [2 ]
Fechner, L. [1 ]
Thai, A. [2 ]
Britz, A. [2 ]
Baudisch, M. [2 ]
Steinle, T. [2 ]
Senftleben, A. [3 ]
Schroeter, C. D. [1 ]
Ullrich, J. [1 ,4 ]
Pfeifer, T. [1 ]
Keitel, C. H. [1 ]
Biegert, J. [2 ,5 ]
Hatsagortsyan, K. Z. [1 ]
Moshammer, R. [1 ]
机构
[1] Max Planck Inst Kernphys, Saupfercheckweg 1, D-69117 Heidelberg, Germany
[2] ICFO Inst Ciencies Foton, Mediterranean Technol Pk, Castelldefels 08860, Barcelona, Spain
[3] Univ Kassel, Ctr Interdisciplinary Nanostruct Sci & Technol CI, Inst Phys, Heinrich Plett Str 40, D-34132 Kassel, Germany
[4] Phys Tech Bundesanstalt, Bundesallee 100, D-38116 Braunschweig, Germany
[5] ICREA, Barcelona 08010, Spain
基金
欧盟地平线“2020”;
关键词
MULTIPHOTON ABSORPTION; ATOMS;
D O I
10.1103/PhysRevA.99.023421
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The laser-induced nonsequential double ionization (NSDI) of rare gas atoms in the near and mid-IR laser fields is studied experimentally and theoretically. We investigate electron-electron correlation at high recollision energies, experimentally achieving ponderomotive energies (U-p) above 80 eV. The contribution of the two dominant channels of NSDI in the photoelectron momentum distribution, impact, and excitation ionization, are both shown to scale with ponderomotive energy and are well reproduced by theory. Surprisingly, for a large U-p in mid-IR fields, a noticeable electron-electron anticorrelation signal emerges at low photoelectron momenta, which cannot be explained by these mechanisms within state-of-the-art theoretical approaches.
引用
收藏
页数:5
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