Control of beam halo formation through nonlinear damping and collimation

This paper demonstrates that transverse beam halos can be controlled by combining nonlinear focusing and collimation. The study relies on one-dimensional, constant focusing particle-in-cell (PIC) simulations and a particle-core model. Beams with linear and nonlinear focusing are studied. Calculation...

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Main Authors: Kiran G. Sonnad, John R. Cary
Format: Article
Language:English
Published: American Physical Society 2005-06-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.8.064202
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spelling doaj-fa506539fe9645fe8c4c6f0f709eb1c52020-11-25T00:53:40ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022005-06-018606420210.1103/PhysRevSTAB.8.064202Control of beam halo formation through nonlinear damping and collimationKiran G. SonnadJohn R. CaryThis paper demonstrates that transverse beam halos can be controlled by combining nonlinear focusing and collimation. The study relies on one-dimensional, constant focusing particle-in-cell (PIC) simulations and a particle-core model. Beams with linear and nonlinear focusing are studied. Calculations with linear focusing confirm previous findings that the extent and density of the halo depend strongly upon the initial mismatch of the beam. Calculations with nonlinear focusing are used to study damping in the beam oscillations caused by the mismatch. Although the nonlinear force damps the beam oscillations, it is accompanied by emittance growth. This process is very rapid and happens within the first 2–3 envelope oscillations. After this, when the halo is collimated using a system of four collimators, further evolution of the beam shows that the halo is not regenerated. The elimination of the beam halo could allow either a smaller physical aperture for the transport system or it could allow a beam of higher current in a system with the same physical aperture. This advantage compensates for the loss of particles due to collimation.http://doi.org/10.1103/PhysRevSTAB.8.064202
collection DOAJ
language English
format Article
sources DOAJ
author Kiran G. Sonnad
John R. Cary
spellingShingle Kiran G. Sonnad
John R. Cary
Control of beam halo formation through nonlinear damping and collimation
Physical Review Special Topics. Accelerators and Beams
author_facet Kiran G. Sonnad
John R. Cary
author_sort Kiran G. Sonnad
title Control of beam halo formation through nonlinear damping and collimation
title_short Control of beam halo formation through nonlinear damping and collimation
title_full Control of beam halo formation through nonlinear damping and collimation
title_fullStr Control of beam halo formation through nonlinear damping and collimation
title_full_unstemmed Control of beam halo formation through nonlinear damping and collimation
title_sort control of beam halo formation through nonlinear damping and collimation
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2005-06-01
description This paper demonstrates that transverse beam halos can be controlled by combining nonlinear focusing and collimation. The study relies on one-dimensional, constant focusing particle-in-cell (PIC) simulations and a particle-core model. Beams with linear and nonlinear focusing are studied. Calculations with linear focusing confirm previous findings that the extent and density of the halo depend strongly upon the initial mismatch of the beam. Calculations with nonlinear focusing are used to study damping in the beam oscillations caused by the mismatch. Although the nonlinear force damps the beam oscillations, it is accompanied by emittance growth. This process is very rapid and happens within the first 2–3 envelope oscillations. After this, when the halo is collimated using a system of four collimators, further evolution of the beam shows that the halo is not regenerated. The elimination of the beam halo could allow either a smaller physical aperture for the transport system or it could allow a beam of higher current in a system with the same physical aperture. This advantage compensates for the loss of particles due to collimation.
url http://doi.org/10.1103/PhysRevSTAB.8.064202
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