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Finite Elements Magnetic Analysis of the CLIC MDI Region
Considering the current CLIC SiD detector design and the machine parameter L*, the final focus quadrupole QD0 will be placed inside the experiment itself. This configuration is very challenging from an integration point of view. Among several other aspects, the iron-dominated QD0 will need an active...
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Lenguaje: | eng |
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2012
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Acceso en línea: | http://cds.cern.ch/record/1428016 |
_version_ | 1780924281647005696 |
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author | Bartalesi, Antonio |
author_facet | Bartalesi, Antonio |
author_sort | Bartalesi, Antonio |
collection | CERN |
description | Considering the current CLIC SiD detector design and the machine parameter L*, the final focus quadrupole QD0 will be placed inside the experiment itself. This configuration is very challenging from an integration point of view. Among several other aspects, the iron-dominated QD0 will need an active magnetic shielding to avoid undesired interactions with the magnetic field generated by the main solenoid of the detector. This shielding will be provided by a superconducting anti-solenoid, and this paper aims to describe the method used to design such device, the results obtained and the issues still to be solved. |
id | cern-1428016 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2012 |
record_format | invenio |
spelling | cern-14280162019-09-30T06:29:59Zhttp://cds.cern.ch/record/1428016engBartalesi, AntonioFinite Elements Magnetic Analysis of the CLIC MDI RegionAccelerators and Storage RingsConsidering the current CLIC SiD detector design and the machine parameter L*, the final focus quadrupole QD0 will be placed inside the experiment itself. This configuration is very challenging from an integration point of view. Among several other aspects, the iron-dominated QD0 will need an active magnetic shielding to avoid undesired interactions with the magnetic field generated by the main solenoid of the detector. This shielding will be provided by a superconducting anti-solenoid, and this paper aims to describe the method used to design such device, the results obtained and the issues still to be solved.Considering the current CLIC SiD detector design and the machine parameter L*, the final focus quadrupole QD0 will be placed inside the experiment itself. This configuration is very challenging from an integration point of view. Among several other aspects, the iron-dominated QD0 will need an active magnetic shielding to avoid undesired interactions with the magnetic field generated by the main solenoid of the detector. This shielding will be provided by a superconducting anti-solenoid, and this paper aims to describe the method used to design such device, the results obtained and the issues still to be solved.arXiv:1202.6334oai:cds.cern.ch:14280162012-02-29 |
spellingShingle | Accelerators and Storage Rings Bartalesi, Antonio Finite Elements Magnetic Analysis of the CLIC MDI Region |
title | Finite Elements Magnetic Analysis of the CLIC MDI Region |
title_full | Finite Elements Magnetic Analysis of the CLIC MDI Region |
title_fullStr | Finite Elements Magnetic Analysis of the CLIC MDI Region |
title_full_unstemmed | Finite Elements Magnetic Analysis of the CLIC MDI Region |
title_short | Finite Elements Magnetic Analysis of the CLIC MDI Region |
title_sort | finite elements magnetic analysis of the clic mdi region |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/1428016 |
work_keys_str_mv | AT bartalesiantonio finiteelementsmagneticanalysisoftheclicmdiregion |