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This overview examines the local performance of the Cathode Strip Chamber (CSC) trigger within the Level-1 Trigger System during muon beam tests at the LHC. We provide an introduction to the LHC, focusing on the Compact Muon Solenoid (CMS) and its architecture. The role of muons as penetrating particles is discussed, along with the necessity of efficient trigger systems to filter data. Key findings include the effectiveness of the Andrey Pattern for achieving high efficiency with low ghost rates, utilizing both muon and pion data from the tests.
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Local Performance of the Local Cathode Strip Chamber Trigger in a Muon Beam Test
Overview: • Introduction to LHC • Overview of CMS • Overview of Trigger Architecture • Overview of Cathode Strip Chamber (CSC) • Level-1 Trigger System • Plots for efficiency • Conclusion
LHC • 14 TeV center of mass energy • 27 km circumference
CMS What is a muon? Muons are point particles identical to electrons except over 200 times more massive (105.2 MeV) The illustration shows the smaller orbit for muons in a hydrogynic atom due to their mass
CMS Why Muons? • Muons are penetrating. • Electrons are too light to make it through absorbers • Taus are too unstable to make it through absorbers • Hadrons interact strongly with matter
Trigger Architecture • Need Trigger System to filter out data
Cathode Strip Chambers (CSC) • Provide 3-D tracks of charged particles called Local Charge Tracks (LCT’s)
Level-1 Trigger System • ALCT and CLCT find 2-D tracks • TMB receives and correlates these tracks to make a 3-D Correlated LCT • MPC receives up to 18 LCT’s from the different TMB’s and selects the best 3 • SR/SP receives the 3 LCT’s from the TMB
2004 Test Beam • 100GeV muons for asynchronous run • 100GeV pions for synchronous run (along with muons)
Conclusions • Andrey Pattern does the best for higher nph patterns • Keeps Efficiency high and ghost rates low