TGC测器的γ灵敏度测量

叶邦角; S.Tsuno; T.Kobayashi

doi:10.11804/NuclPhysRev.18.02.096

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TGC测器的γ灵敏度测量

叶邦角, S.Tsuno, T.Kobayashi

文章导航 > 原子核物理评论 > 2001 > 18(2): 96-100

叶邦角, S.Tsuno, T.Kobayashi. TGC测器的γ灵敏度测量[J]. 原子核物理评论, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

引用本文:

叶邦角, S.Tsuno, T.Kobayashi. TGC测器的γ灵敏度测量[J]. 原子核物理评论, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

YE Bang-jiao, S.Tsuno, T.Kobayashi. Measurement of γ ray Sensitivity of Thin Gap Chamber[J]. Nuclear Physics Review, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

Citation:

YE Bang-jiao, S.Tsuno, T.Kobayashi. Measurement of γ ray Sensitivity of Thin Gap Chamber[J]. Nuclear Physics Review, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

TGC测器的γ灵敏度测量

doi: 10.11804/NuclPhysRev.18.02.096

1中国科学技术大学近代物理系; 2东京大学国际基本粒子物理研究中心

Measurement of γ ray Sensitivity of Thin Gap Chamber

(1 Department of Modern Physics; University of Science and Technology of China; Hefei 230026; China; 2 ICEPP; University of Tokyo; Tokyo 113; Japan);

摘要: 欧洲核子中心的大型强子对撞机探测器预计工作在 1 0 34 /(cm2·s)亮度 ,这将导致实验大厅的本底非常严重 .薄气隙室将作为 ATLAS实验中的前端 μ子触发器 .按照模拟计算 ,实验大厅薄气隙室周围的主要本底是中子和光子 .报告了薄气隙室探测器的 γ灵敏度的实验测量 .使用 γ能量从20ke V到1.8Me V的放射性 γ源 .目前测量的灵敏度小于 1 % ,与用 EGS4模拟计算结果相吻合. The Large Hadron Collider (LHC) at the European Laboratory for Particle Physics (CERN) is expected to operate at the luminosity of 10 34 /(cm 2 ·s), and the resulting background condition in the experimental hall would be quit severe. Thin Gap Chamber (TGC) will be used for forward muon triggering in the ATLAS experiment. According to a simulation, the main source of the background around TGC in the experimental hall is neutrons and photons. The sensitivity measurement for TGC...
- 薄气隙室 /
- ATLAS谱仪 /
- γ灵敏度
Abstract: The Large Hadron Collider (LHC) at the European Laboratory for Particle Physics (CERN) is expected to operate at the luminosity of 10 34 /(cm 2 ·s), and the resulting background condition in the experimental hall would be quit severe. Thin Gap Chamber (TGC) will be used for forward muon triggering in the ATLAS experiment. According to a simulation, the main source of the background around TGC in the experimental hall is neutrons and photons. The sensitivity measurement for TGC...
- thin gap chamber /
- ATLAS spectrograph /
- γ sensitivity

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TGC测器的γ灵敏度测量

doi: 10.11804/NuclPhysRev.18.02.096

1中国科学技术大学近代物理系; 2东京大学国际基本粒子物理研究中心

收稿日期: 1900-01-01
修回日期: 1900-01-01
刊出日期: 2001-06-20

关键词:

薄气隙室 /

ATLAS谱仪 /

γ灵敏度

摘要: 欧洲核子中心的大型强子对撞机探测器预计工作在 1 0 34 /(cm2·s)亮度 ,这将导致实验大厅的本底非常严重 .薄气隙室将作为 ATLAS实验中的前端 μ子触发器 .按照模拟计算 ,实验大厅薄气隙室周围的主要本底是中子和光子 .报告了薄气隙室探测器的 γ灵敏度的实验测量 .使用 γ能量从20ke V到1.8Me V的放射性 γ源 .目前测量的灵敏度小于 1 % ,与用 EGS4模拟计算结果相吻合. The Large Hadron Collider (LHC) at the European Laboratory for Particle Physics (CERN) is expected to operate at the luminosity of 10 34 /(cm 2 ·s), and the resulting background condition in the experimental hall would be quit severe. Thin Gap Chamber (TGC) will be used for forward muon triggering in the ATLAS experiment. According to a simulation, the main source of the background around TGC in the experimental hall is neutrons and photons. The sensitivity measurement for TGC...

English Abstract

叶邦角, S.Tsuno, T.Kobayashi. TGC测器的γ灵敏度测量[J]. 原子核物理评论, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

引用本文:

叶邦角, S.Tsuno, T.Kobayashi. TGC测器的γ灵敏度测量[J]. 原子核物理评论, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

YE Bang-jiao, S.Tsuno, T.Kobayashi. Measurement of γ ray Sensitivity of Thin Gap Chamber[J]. Nuclear Physics Review, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096

Citation:

YE Bang-jiao, S.Tsuno, T.Kobayashi. Measurement of γ ray Sensitivity of Thin Gap Chamber[J]. Nuclear Physics Review, 2001, 18(2): 96-100. doi: 10.11804/NuclPhysRev.18.02.096