Equivalent electron correlations in nonsequential double ionization of noble atoms
Electron correlation is encoded directly in the distribution of the energetic electrons produced in a recollision-impact double ionization process, and varies with the laser field and the target atoms. In order to get equivalent electron correlation effects, one should enlarge the laser intensity cu...
Saved in:
Published in | Chinese physics B Vol. 26; no. 2; pp. 166 - 170 |
---|---|
Main Author | |
Format | Journal Article |
Language | English |
Published |
01.02.2017
|
Subjects | |
Online Access | Get full text |
ISSN | 1674-1056 2058-3834 |
DOI | 10.1088/1674-1056/26/2/023202 |
Cover
Summary: | Electron correlation is encoded directly in the distribution of the energetic electrons produced in a recollision-impact double ionization process, and varies with the laser field and the target atoms. In order to get equivalent electron correlation effects, one should enlarge the laser intensity cubically and the laser frequency linearly in proportion to the second ionization potentials of the target atoms. The physical mechanism behind the transform is to keep the ponderomotive parameter unchanged when the laser frequency is enlarged. |
---|---|
Bibliography: | Shansi Dong1, Qiujing Han2, Jingtao Zhag1 (1. Department of Physics, Shanghai Normal University, Shanghai 200234, China; 2. Qingdao Binhan University, Qingdao 266555, China) Electron correlation is encoded directly in the distribution of the energetic electrons produced in a recollision-impact double ionization process, and varies with the laser field and the target atoms. In order to get equivalent electron correlation effects, one should enlarge the laser intensity cubically and the laser frequency linearly in proportion to the second ionization potentials of the target atoms. The physical mechanism behind the transform is to keep the ponderomotive parameter unchanged when the laser frequency is enlarged. 11-5639/O4 scaling law electron correlation double ionization |
ISSN: | 1674-1056 2058-3834 |
DOI: | 10.1088/1674-1056/26/2/023202 |