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Edge effect in beam monitors

Quite often, particle-beam monitors have not the same cross-section as the beam pipe or vacuum chamber in which they are mounted. In that case, the electromagnetic field of the beam is distorted in the vicinity of the edges of the monitor. This field, at the junction of two rectangular beam pipes of...

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Detalles Bibliográficos
Autor principal: Cuperus, J H
Lenguaje:eng
Publicado: 1977
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0029-554X(77)90415-3
http://cds.cern.ch/record/878523
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author Cuperus, J H
author_facet Cuperus, J H
author_sort Cuperus, J H
collection CERN
description Quite often, particle-beam monitors have not the same cross-section as the beam pipe or vacuum chamber in which they are mounted. In that case, the electromagnetic field of the beam is distorted in the vicinity of the edges of the monitor. This field, at the junction of two rectangular beam pipes of different dimensions, is computed for a beam with constant charge along its length. Solutions which are less accurate but easier to apply are obtained with a first order approximation. The results are extended to intensity-modulated beams and circular or elliptical cross-sections. The errors, due to the edge effect, for the electrostatic pickup and the wall-current monitor are computed. The final formulas are simple and easy to apply to practical cases. (6 refs).
id cern-878523
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1977
record_format invenio
spelling cern-8785232019-09-30T06:29:59Zdoi:10.1016/0029-554X(77)90415-3http://cds.cern.ch/record/878523engCuperus, J HEdge effect in beam monitorsNuclear PhysicsQuite often, particle-beam monitors have not the same cross-section as the beam pipe or vacuum chamber in which they are mounted. In that case, the electromagnetic field of the beam is distorted in the vicinity of the edges of the monitor. This field, at the junction of two rectangular beam pipes of different dimensions, is computed for a beam with constant charge along its length. Solutions which are less accurate but easier to apply are obtained with a first order approximation. The results are extended to intensity-modulated beams and circular or elliptical cross-sections. The errors, due to the edge effect, for the electrostatic pickup and the wall-current monitor are computed. The final formulas are simple and easy to apply to practical cases. (6 refs).oai:cds.cern.ch:8785231977
spellingShingle Nuclear Physics
Cuperus, J H
Edge effect in beam monitors
title Edge effect in beam monitors
title_full Edge effect in beam monitors
title_fullStr Edge effect in beam monitors
title_full_unstemmed Edge effect in beam monitors
title_short Edge effect in beam monitors
title_sort edge effect in beam monitors
topic Nuclear Physics
url https://dx.doi.org/10.1016/0029-554X(77)90415-3
http://cds.cern.ch/record/878523
work_keys_str_mv AT cuperusjh edgeeffectinbeammonitors