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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2023
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nima.2023.168770 http://cds.cern.ch/record/2846753 |
_version_ | 1780976650188488704 |
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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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