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New clic-g structure design
The baseline design of the Compact Linear Collider main linac accelerating structure is called ‘CLIC-G’. It is described in the CLIC Conceptual Design Report (CDR) [1]. As shown in Fig. 1, a regular cell of the structure has four waveguides to damp unwanted high-order-modes (HOMs). These waveguides...
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Lenguaje: | eng |
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2016
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Acceso en línea: | http://cds.cern.ch/record/2157079 |
_version_ | 1780950705283006464 |
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author | Zha, Hao Grudiev, Alexej |
author_facet | Zha, Hao Grudiev, Alexej |
author_sort | Zha, Hao |
collection | CERN |
description | The baseline design of the Compact Linear Collider main linac accelerating structure is called ‘CLIC-G’. It is described in the CLIC Conceptual Design Report (CDR) [1]. As shown in Fig. 1, a regular cell of the structure has four waveguides to damp unwanted high-order-modes (HOMs). These waveguides are dimensioned to cut off the fundamental working frequency in order to prevent the degradation of the fundamental mode Q-factor. The cell geometry and HOM damping loads had been extensively optimized in order to maximize the RF-to-beam efficiency, to minimize the cost, and to meet the beam dynamics and the high gradient RF constraints [2] |
id | cern-2157079 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21570792023-07-20T15:04:50Zhttp://cds.cern.ch/record/2157079engZha, HaoGrudiev, AlexejNew clic-g structure designAccelerators and Storage RingsThe baseline design of the Compact Linear Collider main linac accelerating structure is called ‘CLIC-G’. It is described in the CLIC Conceptual Design Report (CDR) [1]. As shown in Fig. 1, a regular cell of the structure has four waveguides to damp unwanted high-order-modes (HOMs). These waveguides are dimensioned to cut off the fundamental working frequency in order to prevent the degradation of the fundamental mode Q-factor. The cell geometry and HOM damping loads had been extensively optimized in order to maximize the RF-to-beam efficiency, to minimize the cost, and to meet the beam dynamics and the high gradient RF constraints [2]CERN-ACC-2016-0066CLIC-Note-1066oai:cds.cern.ch:21570792016-05-11 |
spellingShingle | Accelerators and Storage Rings Zha, Hao Grudiev, Alexej New clic-g structure design |
title | New clic-g structure design |
title_full | New clic-g structure design |
title_fullStr | New clic-g structure design |
title_full_unstemmed | New clic-g structure design |
title_short | New clic-g structure design |
title_sort | new clic-g structure design |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/2157079 |
work_keys_str_mv | AT zhahao newclicgstructuredesign AT grudievalexej newclicgstructuredesign |