By Hamlet K. Avetissian
This booklet is on various nonlinear schemes of unfastened Electron Lasers, Laser Accelerators, and Electron-Positron pair creation and covers the idea of interplay of sturdy and great powerful laser fields with charged debris and vacuum. those issues may be within the middle of primary study within the subsequent decade. the writer, who has over 30 years of expertise during this box, has built non-linear idea and new methods to unravel respective relativistic classical and quantum difficulties. The booklet may be specially worthy for researchers, scholars and practitioners within the fields of Particle and Laser Physics.
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Extra resources for Relativistic Nonlinear Electrodynamics: Interaction of Charged Particles with Strong and Super Strong Laser Fields
Example text
Such behavior of the particle in the intrinsic frame of the wave corresponds to the cases ξ > ξcr (large velocities close to the Cherenkov one at which ξcr is small and the condition ξ > ξcr is achievable) and ξ < ξcr in the laboratory frame of reference, respectively (see Eq. 7)). Note that because of the particle reflection from the standing barrier in the frame of reference of the slowed wave we term the revealed nonlinear phenomenon a “reflection” one. Hence, the threshold-coherent nature of spontaneous Cherenkov effect over the particle velocity (vth = c/n0 ) causes the threshold for the external wave intensity (ξth ≡ ξcr ), which in turn causes the phenomenon of particle “reflection” from the plane EM wave.
And Za = 1. In Fig. 8a the envelopes of partial differential cross sections as a function of the number of emitted or absorbed photons for circular polarization of EM wave are shown for the deflection angle ϑ ≡ ∠ΠΠ = 10 mrad. 1. The dotted and dashed lines correspond to initial electron momentum parallel and antiparallel to the laser propagation direction k, respectively, and the solid line gives the nonrelativistic result. The energy change of a particle is characterized by the absorption/emission (AE) cross section.
The dotted and dashed lines correspond to initial electron momentum parallel and antiparallel to the laser propagation direction k, respectively, and the solid line gives the nonrelativistic result. The energy change of a particle is characterized by the absorption/emission (AE) cross section. Partial AE differential cross section will be (s) dσae =s dO dσ (s) dσ (−s) − dO dO . 149) In Fig. 8b the envelopes of partial AE differential cross sections for circular polarization of EM wave are shown for the same parameters.