4.1 Article

Chaotic electron dynamics in a FEL with realizable quadrupole wiggler and Gaussian electron beam

期刊

CANADIAN JOURNAL OF PHYSICS
卷 101, 期 1, 页码 17-29

出版社

CANADIAN SCIENCE PUBLISHING
DOI: 10.1139/cjp-2021-005317

关键词

chaotic motion; free-electron laser; realizable quadrupole wiggler; Gaussian electron beam; ion-channel guiding

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This paper investigates the chaotic dynamics of electrons moving with relativistic velocity in a realizable quadrupole wiggler. The nonlinearity of the wiggler magnetic field is found to be the main cause of the chaotic electron motion at large radial distances. Using an electron beam with Gaussian density and an ion channel can control and suppress the chaotic motion of electrons.
Chaotic motion of electrons causes a considerable decrease in gain and efficiency of free-electron lasers (FELs). In this paper, we study chaotic dynamics of electrons moving with relativistic velocity in a realizable (three-dimensional) quadrupole wiggler when the radial dependency of wiggler magnetic field is fully taken into account using time series, Poincare ' surface-of-section maps, and Liapunov exponents. The electron beam is also considered to be realizable with Gaussian density profile and an ion channel is considered as a guiding device for the electron beam. We show that the chaotic behavior of electron motion is due to the nonlinearity of quadrupole wiggler magnetic field and the chaotic electron motion occurs at almost large radial distances in which the wiggler magnetic field is large. Also, we find that one can control the electron chaotic motion by using electron beam with Gaussian density rather than the electron beam with uniform density. Furthermore, we investigate the effect of ion channel and find that when the electrostatic force of ion channel overcomes the nonlinearity effect of quadrupole wiggler magnetic field and self-repulsive force arises from electron beam, the electron motion becomes non-chaotic. We also investigate the electron motion under Budker condition and show that the Budker condition cannot guarantee the electron motion becoming completely non-chaotic.

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