One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams
This paper makes use of a one-dimensional kinetic model to investigate the nonlinear longitudinal dynamics of a long coasting beam propagating through a perfectly conducting circular pipe with radius r_{w}. The average axial electric field is expressed as ⟨E_{z}⟩=-(∂/∂z)⟨ϕ⟩=-e_{b}g_{0}∂λ_{b}/∂z-e_{b...
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American Physical Society
2015-09-01
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Series: | Physical Review Special Topics. Accelerators and Beams |
Online Access: | http://doi.org/10.1103/PhysRevSTAB.18.094201 |
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doaj-251c25b0656846dd823ed2fdc59ae1792020-11-24T21:26:29ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022015-09-0118909420110.1103/PhysRevSTAB.18.094201One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beamsRonald C. DavidsonHong QinThis paper makes use of a one-dimensional kinetic model to investigate the nonlinear longitudinal dynamics of a long coasting beam propagating through a perfectly conducting circular pipe with radius r_{w}. The average axial electric field is expressed as ⟨E_{z}⟩=-(∂/∂z)⟨ϕ⟩=-e_{b}g_{0}∂λ_{b}/∂z-e_{b}g_{2}r_{w}^{2}∂^{3}λ_{b}/∂z^{3}, where g_{0} and g_{2} are constant geometric factors, λ_{b}(z,t)=∫dp_{z}F_{b}(z,p_{z},t) is the line density of beam particles, and F_{b}(z,p_{z},t) satisfies the 1D Vlasov equation. Detailed nonlinear properties of traveling-wave and traveling-pulse (soliton) solutions with time-stationary waveform are examined for a wide range of system parameters extending from moderate-amplitudes to large-amplitude modulations of the beam charge density. Two classes of solutions for the beam distribution function are considered, corresponding to: (i) the nonlinear waterbag distribution, where F_{b}=const in a bounded region of p_{z}-space; and (ii) nonlinear Bernstein-Green-Kruskal (BGK)-like solutions, allowing for both trapped and untrapped particle distributions to interact with the self-generated electric field ⟨E_{z}⟩.http://doi.org/10.1103/PhysRevSTAB.18.094201 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Ronald C. Davidson Hong Qin |
spellingShingle |
Ronald C. Davidson Hong Qin One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams Physical Review Special Topics. Accelerators and Beams |
author_facet |
Ronald C. Davidson Hong Qin |
author_sort |
Ronald C. Davidson |
title |
One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
title_short |
One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
title_full |
One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
title_fullStr |
One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
title_full_unstemmed |
One-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
title_sort |
one-dimensional kinetic description of nonlinear traveling-pulse and traveling-wave disturbances in long coasting charged particle beams |
publisher |
American Physical Society |
series |
Physical Review Special Topics. Accelerators and Beams |
issn |
1098-4402 |
publishDate |
2015-09-01 |
description |
This paper makes use of a one-dimensional kinetic model to investigate the nonlinear longitudinal dynamics of a long coasting beam propagating through a perfectly conducting circular pipe with radius r_{w}. The average axial electric field is expressed as ⟨E_{z}⟩=-(∂/∂z)⟨ϕ⟩=-e_{b}g_{0}∂λ_{b}/∂z-e_{b}g_{2}r_{w}^{2}∂^{3}λ_{b}/∂z^{3}, where g_{0} and g_{2} are constant geometric factors, λ_{b}(z,t)=∫dp_{z}F_{b}(z,p_{z},t) is the line density of beam particles, and F_{b}(z,p_{z},t) satisfies the 1D Vlasov equation. Detailed nonlinear properties of traveling-wave and traveling-pulse (soliton) solutions with time-stationary waveform are examined for a wide range of system parameters extending from moderate-amplitudes to large-amplitude modulations of the beam charge density. Two classes of solutions for the beam distribution function are considered, corresponding to: (i) the nonlinear waterbag distribution, where F_{b}=const in a bounded region of p_{z}-space; and (ii) nonlinear Bernstein-Green-Kruskal (BGK)-like solutions, allowing for both trapped and untrapped particle distributions to interact with the self-generated electric field ⟨E_{z}⟩. |
url |
http://doi.org/10.1103/PhysRevSTAB.18.094201 |
work_keys_str_mv |
AT ronaldcdavidson onedimensionalkineticdescriptionofnonlineartravelingpulseandtravelingwavedisturbancesinlongcoastingchargedparticlebeams AT hongqin onedimensionalkineticdescriptionofnonlineartravelingpulseandtravelingwavedisturbancesinlongcoastingchargedparticlebeams |
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