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Wakefield damping in a distributed coupling linear accelerator

The number of cells in a <math altimg="si3.svg" display="inline" id="d1e680"><mi>π</mi></math>-mode standing wave (SW) accelerating structure for the Compact Linear Collider (CLIC) project is limited by mode overlap with nearby modes. The distrib...

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Detalles Bibliográficos
Autores principales: Ericson, Evan, Grudiev, Alexej, Bertwistle, Drew, Boland, Mark J.
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2023.168770
http://cds.cern.ch/record/2846753
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author Ericson, Evan
Grudiev, Alexej
Bertwistle, Drew
Boland, Mark J.
author_facet Ericson, Evan
Grudiev, Alexej
Bertwistle, Drew
Boland, Mark J.
author_sort Ericson, Evan
collection CERN
description The number of cells in a <math altimg="si3.svg" display="inline" id="d1e680"><mi>π</mi></math>-mode standing wave (SW) accelerating structure for the Compact Linear Collider (CLIC) project is limited by mode overlap with nearby modes. The distributed coupling scheme avoids mode overlap by treating each cell as independent. Designs of cells suitable for distributed coupling with strong wakefield suppression by waveguide damping have not previously been studied. In this paper we develop a SW cell to be used in a distributed coupling structure that can satisfy the CLIC transverse wake potential limit. From the middle cell of the CLIC-G* traveling wave (TW) structure, a SW cell is designed and then adapted to perform as a cell in a distributed coupling structure. Its wake potentials in an ideal case of open boundaries are reduced to satisfy the wake potential threshold. An electric boundary is added to the model to simulate total reflection at the distribution network. A horizontal coupler cell that connects to the distribution network such that the reflected wakefields remain similar to the open boundary case is simulated. A triplet module which takes advantage of cell-to-cell coupling to reduce reflected wake potential is presented.
id cern-2846753
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2023
record_format invenio
spelling cern-28467532023-10-26T04:47:27Zdoi:10.1016/j.nima.2023.168770http://cds.cern.ch/record/2846753engEricson, EvanGrudiev, AlexejBertwistle, DrewBoland, Mark J.Wakefield damping in a distributed coupling linear acceleratorphysics.acc-phAccelerators and Storage RingsThe number of cells in a <math altimg="si3.svg" display="inline" id="d1e680"><mi>π</mi></math>-mode standing wave (SW) accelerating structure for the Compact Linear Collider (CLIC) project is limited by mode overlap with nearby modes. The distributed coupling scheme avoids mode overlap by treating each cell as independent. Designs of cells suitable for distributed coupling with strong wakefield suppression by waveguide damping have not previously been studied. In this paper we develop a SW cell to be used in a distributed coupling structure that can satisfy the CLIC transverse wake potential limit. From the middle cell of the CLIC-G* traveling wave (TW) structure, a SW cell is designed and then adapted to perform as a cell in a distributed coupling structure. Its wake potentials in an ideal case of open boundaries are reduced to satisfy the wake potential threshold. An electric boundary is added to the model to simulate total reflection at the distribution network. A horizontal coupler cell that connects to the distribution network such that the reflected wakefields remain similar to the open boundary case is simulated. A triplet module which takes advantage of cell-to-cell coupling to reduce reflected wake potential is presented.The number of cells in a $\pi$-mode standing wave (SW) accelerating structure for the Compact linear Collider (CLIC) project is limited by mode overlap with nearby modes. The distributed coupling scheme avoids mode overlap by treating each cell as independent. Designs of cells suitable for distributed coupling with strong wakefield damping have not previously been studied. In this paper we develop a SW cell to be used in a distributed coupling structure that can satisfy the CLIC transverse wakepotential limit. From the middle cell of the CLIC-G* travelling wave (TW) structure, a SW cell is designed. The cell is adapted to be suitable for distributed coupling. Its wakepotentials in an ideal case of open boundaries are reduced to satisfy the wakepotential threshold. An electric boundary is added to the model to simulate total reflection at the distribution network. A horizontal coupler cell that connects to the distribution network such that the reflected wakefields remain similar to the open boundary case is simulated. A triplet module which takes advantage of cell-to-cell coupling to reduce reflected wakepotential is presented.arXiv:2301.02340oai:cds.cern.ch:28467532023-01-05
spellingShingle physics.acc-ph
Accelerators and Storage Rings
Ericson, Evan
Grudiev, Alexej
Bertwistle, Drew
Boland, Mark J.
Wakefield damping in a distributed coupling linear accelerator
title Wakefield damping in a distributed coupling linear accelerator
title_full Wakefield damping in a distributed coupling linear accelerator
title_fullStr Wakefield damping in a distributed coupling linear accelerator
title_full_unstemmed Wakefield damping in a distributed coupling linear accelerator
title_short Wakefield damping in a distributed coupling linear accelerator
title_sort wakefield damping in a distributed coupling linear accelerator
topic physics.acc-ph
Accelerators and Storage Rings
url https://dx.doi.org/10.1016/j.nima.2023.168770
http://cds.cern.ch/record/2846753
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AT grudievalexej wakefielddampinginadistributedcouplinglinearaccelerator
AT bertwistledrew wakefielddampinginadistributedcouplinglinearaccelerator
AT bolandmarkj wakefielddampinginadistributedcouplinglinearaccelerator