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Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation
The LHC will be upgraded in several phases with the goal of obtaining an instantaneous lumi- nosity of 5-7 x 10^34 cm-2s-s at the center of mass energy of 14 TeV and integrated luminosity of 3000 fb-1. In order to profit from the high luminosity and high energy runs of the LHC, the ATLAS collaborati...
Autores principales: | , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2014
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.22323/1.180.0093 http://cds.cern.ch/record/2003090 |
_version_ | 1780946171660861440 |
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author | Chapman, J Dai, T Diehl, E Feng, H Guan, L Mikenberg, G Smakhtin, V Yu, J M Zhou, B Zhu, J Zhao, Z |
author_facet | Chapman, J Dai, T Diehl, E Feng, H Guan, L Mikenberg, G Smakhtin, V Yu, J M Zhou, B Zhu, J Zhao, Z |
author_sort | Chapman, J |
collection | CERN |
description | The LHC will be upgraded in several phases with the goal of obtaining an instantaneous lumi- nosity of 5-7 x 10^34 cm-2s-s at the center of mass energy of 14 TeV and integrated luminosity of 3000 fb-1. In order to profit from the high luminosity and high energy runs of the LHC, the ATLAS collaboration plans to upgrade the present endcap small wheel muon spectrometer to im- prove the muon triggering as well as precision tracking. The proposed New Small Wheel (nSW) will be composed of two four-layer Micromegas detectors (MM) detector sandwiched between two four-layer small-strip Thin Gap Chambers (sTGC) quadruplets, where MM for precision tracking and sTGC for Level-1 triggering. In this paper, we focus on the Garfield [ 1 ] simulation of the sTGC detector to understand its timing performance and charge production. We also stud- ied the sTGC timing under different magnetic fields and high voltages. These studies provide important guide lines for the sTGC detector and electronics development. |
id | oai-inspirehep.net-1290921 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | oai-inspirehep.net-12909212019-09-30T06:29:59Zdoi:10.22323/1.180.0093http://cds.cern.ch/record/2003090engChapman, JDai, TDiehl, EFeng, HGuan, LMikenberg, GSmakhtin, VYu, J MZhou, BZhu, JZhao, ZUnderstand ATLAS NSW Thin Gap Chamber from Garfield SimulationDetectors and Experimental TechniquesThe LHC will be upgraded in several phases with the goal of obtaining an instantaneous lumi- nosity of 5-7 x 10^34 cm-2s-s at the center of mass energy of 14 TeV and integrated luminosity of 3000 fb-1. In order to profit from the high luminosity and high energy runs of the LHC, the ATLAS collaboration plans to upgrade the present endcap small wheel muon spectrometer to im- prove the muon triggering as well as precision tracking. The proposed New Small Wheel (nSW) will be composed of two four-layer Micromegas detectors (MM) detector sandwiched between two four-layer small-strip Thin Gap Chambers (sTGC) quadruplets, where MM for precision tracking and sTGC for Level-1 triggering. In this paper, we focus on the Garfield [ 1 ] simulation of the sTGC detector to understand its timing performance and charge production. We also stud- ied the sTGC timing under different magnetic fields and high voltages. These studies provide important guide lines for the sTGC detector and electronics development.oai:inspirehep.net:12909212014 |
spellingShingle | Detectors and Experimental Techniques Chapman, J Dai, T Diehl, E Feng, H Guan, L Mikenberg, G Smakhtin, V Yu, J M Zhou, B Zhu, J Zhao, Z Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title | Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title_full | Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title_fullStr | Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title_full_unstemmed | Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title_short | Understand ATLAS NSW Thin Gap Chamber from Garfield Simulation |
title_sort | understand atlas nsw thin gap chamber from garfield simulation |
topic | Detectors and Experimental Techniques |
url | https://dx.doi.org/10.22323/1.180.0093 http://cds.cern.ch/record/2003090 |
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