Emission and its back-reaction accompanying electron motion in relativistically strong and QED-strong pulsed laser fields

被引：98

作者：

Sokolov, Igor V. ^{[1
]}

Nees, John A. ^{[2
,3
]}

Yanovsky, Victor P. ^{[2
,3
]}

Naumova, Natalia M. ^{[4
]}

Mourou, Gerard A. ^{[5
]}

机构：

[1] Univ Michigan, Space Phys Res Lab, Ann Arbor, MI 48109 USA

[2] Univ Michigan, Ctr Ultrafast Opt Sci, Ann Arbor, MI 48109 USA

[3] Univ Michigan, FOCUS Ctr, Ann Arbor, MI 48109 USA

[4] Ecole Polytech, CNRS, Lab Opt Appl, UMR ENSTA 7639, F-91761 Palaiseau, France

[5] Ecole Polytech, CNRS, Inst Lumiere Extreme, UMR ENSTA 3205, F-91761 Palaiseau, France

来源：

PHYSICAL REVIEW E | 2010年 / 81卷 / 03期

关键词：

NONRELATIVISTIC QUANTUM ELECTRODYNAMICS; PLANE ELECTROMAGNETIC WAVE; COMPTON-SCATTERING; RADIATION REACTION; PAIR PRODUCTION; CONSTANT FIELD; PHOTONS; PLASMA; ACCELERATOR; GENERATION;

D O I：

10.1103/PhysRevE.81.036412

中图分类号：

O35 [流体力学]; O53 [等离子体物理学];

学科分类号：

070204 ; 080103 ; 080704 ;

摘要：

The emission from an electron in the field of a relativistically strong laser pulse is analyzed. At pulse intensities of J >= 2 x 10(22) W/cm(2) the emission from counterpropagating electrons is modified by the effects of quantum electrodynamics (QED), as long as the electron energy is sufficiently high: epsilon >= 1 GeV. The radiation force experienced by an electron is for the first time derived from the QED principles and its applicability range is extended toward the QED-strong fields.

引用

页数：13

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