2017
DOI: 10.1063/1.5018425
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Control of the diocotron instability of a hollow electron beam with periodic dipole magnets

Abstract: A method to control the diocotron instability of a hollow electron beam with periodic dipole magnetic fields has been investigated by a two-dimensional particle-in-cell simulation. At first, relations between the diocotron instability and several physical parameters such as the electron number density, the current and shape of the electron beam, and the solenoidal field strength are theoretically analyzed without periodic dipole magnetic fields. Then, we study the effects of the periodic dipole magnetic fields… Show more

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Cited by 15 publications
(11 citation statements)
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“…During these experiments, the same electron-lens current was seen by the antiprotons at each turn (the so-called "dc mode" of operation). More studies have followed, such as the calculation of the transverse kicks from the hollow electron-lens bends [20], the beam diocotron instability control [21], and the hollow electron gun characterization [22], as well as experimental and numerical studies for a hollow electron-lens system [23][24][25][26][27][28]. The above studies, as well as the existing electron-lens experience from Tevatron and RHIC [29][30][31][32][33][34], provide information for the design of a hollow electron-lens system that meets the halo removal requirements for the HL-LHC, as well as the future applications of beam collimation in the FCC-hh [35] at CERN or Super Proton-Proton Collider (SPPC) [36] in China.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…During these experiments, the same electron-lens current was seen by the antiprotons at each turn (the so-called "dc mode" of operation). More studies have followed, such as the calculation of the transverse kicks from the hollow electron-lens bends [20], the beam diocotron instability control [21], and the hollow electron gun characterization [22], as well as experimental and numerical studies for a hollow electron-lens system [23][24][25][26][27][28]. The above studies, as well as the existing electron-lens experience from Tevatron and RHIC [29][30][31][32][33][34], provide information for the design of a hollow electron-lens system that meets the halo removal requirements for the HL-LHC, as well as the future applications of beam collimation in the FCC-hh [35] at CERN or Super Proton-Proton Collider (SPPC) [36] in China.…”
Section: Introductionmentioning
confidence: 99%
“…For the pulsed mode, there are concerns about potential emittance growth due to electron beam profile distortions, field asymmetries between the entrance and the exit bending region of the hollow electron-lens system, and beam alignment errors. There currently is an effort ongoing to improve the beam transverse profile via simulation by reducing the hollow electron beam diocotron instability [21].…”
Section: Introductionmentioning
confidence: 99%
“…A two-dimensional radial-azimuthal explicit and electrostatic particle-in-cell code [39] was utilized to investigate the instability development and spoke dynamics. The code was extensively benchmarked and validated [40,41,42] and the convergence was also verified with different time steps, cell sizes and particles per cell in our study. An equidistant computational grids 64 × 512 in the radial and azimuthal dimensions was used.…”
Section: Pic/mcc Model Descriptionmentioning
confidence: 91%
“…This instability deforms the initially axisymmetric electron density distribution, leading, in the nonlinear phase, to the formation of a discrete number of vortices, and eventually breakup [46,48]. This test case has importance both from a fundamental physics point of view [11,48,43] as well as in practical applications such as beam collimation [49].…”
Section: D Diocotron Instabilitymentioning
confidence: 98%