The trigger chambers of the ATLAS muon spectrometer: production and tests

被引:12
作者
Aloisio, A
Alviggi, M
Biglietti, M
Canale, V
Caprio, M
Carlino, G
Conventi, F
de Asmundis, R
Della Pietra, M
Della Volpe, D
Iengo, P
Patricelli, S
Sekhniaidze, G
Bocci, V
Di Mattia, A
Luminari, L
Nisati, A
Pastore, F
Falciano, S
Petrolo, E
Vari, R
Veneziano, S
Aielli, G
Camarri, P
Cardarelli, R
Di Simone, A
Di Ciaccio, A
Liberti, B
Salamon, A
Santonico, R
Bianco, H
Brambilla, E
Cataldi, G
Chiodini, G
Gorini, E
Grancagnolo, F
Perrino, R
Primavera, M
Spagnolo, S
Tassielli, G
Ventura, A
Ikeno, M
Iwasaki, H
Nagano, K
Sasaki, O
Tanaka, S
Hasegawa, Y
Ohshita, H
Takeshita, T
Ichimiya, R
机构
[1] INFN Sez Napoli, I-80126 Naples, Italy
[2] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[3] Univ Roma La Sapienza, Dipartimento Fis, I-00185 Rome, Italy
[4] Univ Roma Tor Vergata, I-00133 Rome, Italy
[5] Univ Lecce, I-73100 Lecce, Italy
[6] KEK, Tsukuba, Ibaraki, Japan
[7] Shinshu Univ, Matsumoto, Nagano 390, Japan
[8] Kobe Univ, Kobe, Hyogo, Japan
[9] Univ Tokyo, ICEPP, Tokyo, Japan
[10] Tokyo Metropolitan Univ, Tokyo 158, Japan
[11] Weizmann Inst Sci, IL-76100 Rehovot, Israel
[12] Technion Israel Inst Technol, IL-32000 Haifa, Israel
[13] Tel Aviv Univ, IL-69978 Tel Aviv, Israel
关键词
RPC; TGC; test stands;
D O I
10.1016/j.nima.2004.07.130
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
The ATLAS Muon Spectrometer (ATLAS Collaboration, ATLAS Muon Spectrometer Technical Design Report CERN/LHCC/97-22, ATLAS TDR 10, 1997.) will use dedicated detectors to trigger on muons and to identify the bunch-crossing at the appropriate rate. The Spectrometer has been designed to perform stand-alone triggering and measurement of union transverse momentum up to 1 TeV with good resolution (from 3% up to 10% at 1 TeV). The magnetic system is composed of three large superconducting air-core toroids instrumented with trigger and high-precision tracking chambers, a central part (barrel) composed of eight coils and two end-cap magnets. The high-precision tracking system is based on Monitored Drift Tube (MDT) and Cathode Strip Chambers (CSC) in the small angle-regions. The Level-1 trigger is provided by Resistive Plate Chambers (RPC) in the barrel and Thin Gap Chambers (TGC) in the end-cap. These detectors will also measure the track coordinates in the magnetic field direction (second coordinate), to complement the precision tracking provided by the MDT which only measure the track 2 coordinates in the bending direction of the magnetic field. The trigger system covers an area of 3650 M in the barrel and 2900 m(2) in the end-cap. In the barrel region three double-gap RPC stations are used, two in the middle and one in the outer MDT chamber layer. In the end-cap region one triple-gap TGC station is used, in front of the middle MDT station, and two double-gap TGC stations behind it. The mass production of both systems is under way. The systems were involved in extensive beam tests in 2002-2003, testing their compliance with LHC timing requirements using 25 ns beam bunching to emulate the LHC beam structure, aging under critical environment conditions and so on. (C) 2004 Elsevier B.V. All rights reserved.
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页码:265 / 271
页数:7
相关论文
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Caprio, M ;
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Della Pietra, M ;
della Volpe, D ;
Iengo, P ;
Patricelli, S ;
Sekhniaidze, G .
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