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The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter
CMS is one of the four experiments being constructed for the LHC. The electromagnetic calorimeter (ECAL) is made of lead tungstate (PbWO4) crystals. Scintillation light from the crystals in the barrel is detected by avalanche photo diodes (APD). The number of scintillation photons emitted by the cry...
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Lenguaje: | eng |
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2007
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Acceso en línea: | https://dx.doi.org/10.1109/TNS.2007.906169 http://cds.cern.ch/record/1063357 |
_version_ | 1780913222858047488 |
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author | Teller, O |
author_facet | Teller, O |
author_sort | Teller, O |
collection | CERN |
description | CMS is one of the four experiments being constructed for the LHC. The electromagnetic calorimeter (ECAL) is made of lead tungstate (PbWO4) crystals. Scintillation light from the crystals in the barrel is detected by avalanche photo diodes (APD). The number of scintillation photons emitted by the crystals and the amplification of the APD are both temperature dependent. Keeping the constant term of the energy resolution (the contribution to the fractional energy resolution which is independent of energy) below a few tenths of percent requires the temperature of crystals and APDs to be stabilized to within 0.057 K. In this contribution, we describe the innovative solutions which have been developed and implemented to achieve this performance. |
id | cern-1063357 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2007 |
record_format | invenio |
spelling | cern-10633572019-09-30T06:29:59Zdoi:10.1109/TNS.2007.906169http://cds.cern.ch/record/1063357engTeller, OThe design of the cooling system for the CMS Barrel Electromagnetic CalorimeterDetectors and Experimental TechniquesEngineeringCMS is one of the four experiments being constructed for the LHC. The electromagnetic calorimeter (ECAL) is made of lead tungstate (PbWO4) crystals. Scintillation light from the crystals in the barrel is detected by avalanche photo diodes (APD). The number of scintillation photons emitted by the crystals and the amplification of the APD are both temperature dependent. Keeping the constant term of the energy resolution (the contribution to the fractional energy resolution which is independent of energy) below a few tenths of percent requires the temperature of crystals and APDs to be stabilized to within 0.057 K. In this contribution, we describe the innovative solutions which have been developed and implemented to achieve this performance.oai:cds.cern.ch:10633572007 |
spellingShingle | Detectors and Experimental Techniques Engineering Teller, O The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title | The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title_full | The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title_fullStr | The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title_full_unstemmed | The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title_short | The design of the cooling system for the CMS Barrel Electromagnetic Calorimeter |
title_sort | design of the cooling system for the cms barrel electromagnetic calorimeter |
topic | Detectors and Experimental Techniques Engineering |
url | https://dx.doi.org/10.1109/TNS.2007.906169 http://cds.cern.ch/record/1063357 |
work_keys_str_mv | AT tellero thedesignofthecoolingsystemforthecmsbarrelelectromagneticcalorimeter AT tellero designofthecoolingsystemforthecmsbarrelelectromagneticcalorimeter |