Problems of Atomic Science and Technology 2022
DOI: 10.46813/2022-142-036
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Simulation of Plasma Wakefield Focusing and Self-Focusing of a Short Sequence of Electron Bunches Depending on the Bunch Length, Shape and Distance Between Bunches

Abstract: By using two-dimensional numerical simulation, the ratio between the effects of wakefield focusing and selffocusing during the propagation of a short sequence of electron bunches in plasma has been simulated. Cases of dominant wakefield focusing have been demonstrated. In addition, the collection data is presented on the parameters of the bunch length, shape and distance between bunches correspond to certain ratios of wakefield focusing and selffocusing that can be used in further studies.

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“…Electromagnetic radiation fluxes and beams of charged particles due to the development of self-modulation instability can be broken into a chain of particle bunches (see [9 -11]) or a chain of electromagnetic pulses (see [12]), which excite a wakefield in the plasma, which effectively accelerate charged particles (see [13 -16]). Also, due to the development of self-modulation instability, electromagnetic radiation can be broken down into a chain of electromagnetic pulses that excite a wakefield in the plasma, which effectively accelerates charged particles, and they can continue to excite the wakefield and accelerate charged particles to even higher energies (see [17,18]). Also, in a nonequilibrium current plasma or a plasma with particle flows, a strong electric double layer can form (see [8]), which accelerates charged particles to high energies.…”
Section: Introductionmentioning
confidence: 99%
“…Electromagnetic radiation fluxes and beams of charged particles due to the development of self-modulation instability can be broken into a chain of particle bunches (see [9 -11]) or a chain of electromagnetic pulses (see [12]), which excite a wakefield in the plasma, which effectively accelerate charged particles (see [13 -16]). Also, due to the development of self-modulation instability, electromagnetic radiation can be broken down into a chain of electromagnetic pulses that excite a wakefield in the plasma, which effectively accelerates charged particles, and they can continue to excite the wakefield and accelerate charged particles to even higher energies (see [17,18]). Also, in a nonequilibrium current plasma or a plasma with particle flows, a strong electric double layer can form (see [8]), which accelerates charged particles to high energies.…”
Section: Introductionmentioning
confidence: 99%