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On the nonlocal properties of relativistic ponderomotive force
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10.1063/1.4817745
/content/aip/journal/pop/20/8/10.1063/1.4817745
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/8/10.1063/1.4817745
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Effects of the curvature and third derivative of the field amplitude on the particle orbit. The field has (a) zero gradient and positive or negative curvature, (b) finite gradient and positive or negative curvature, and (c) zero gradient and positive or negative third derivative at . The blue line denotes the field pattern and the black solid line represents the particle orbit in the - plane. In the lower part, the unperturbed orbits are shown for comparison.

Image of FIG. 2.
FIG. 2.

Transverse laser field profiles considered in Sec. IV A , i.e., Gaussian and super Gaussian , and B, i.e., and concave hollows.

Image of FIG. 3.
FIG. 3.

Comparison between the numerical trajectories for the oscillation center of an electron obtained from the Lie perturbation method up to (I) the first and (II) third orders, and (III) the averaging method up to the third order with respect to . An electron interacts with a laser beam having an envelope , where and . The black solid line shows the electron trajectory calculated by the full-order equation of motion.

Image of FIG. 4.
FIG. 4.

Numerical trajectories for the oscillation center of an electron interacting with a laser field having transverse envelopes (a) and (b) , where and . Blue and red lines show the oscillation center trajectories obtained by the ponderomotive formulae up to the first and third orders, respectively.

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/content/aip/journal/pop/20/8/10.1063/1.4817745
2013-08-12
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: On the nonlocal properties of relativistic ponderomotive force
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/8/10.1063/1.4817745
10.1063/1.4817745
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