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US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 1
Level-1 CSC Trigger SimulationLevelLevel--1 CSC Trigger Simulation1 CSC Trigger Simulation
Darin Acosta
University of FloridaMay 2001
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 2
Simulation StrategySimulation StrategySimulation Strategy
Studies have been carried out using the object-oriented software framework of CMS
• Geant3 for hit generation• “ORCA” for detector and trigger simulation
Entire L1 CSC Trigger scheme coded in C++• Perfect agreement achieved between simulation and
hardware for millions of events (MPC, SR, SP)Trigger rate, efficiency, and PT resolution studied
for L = 1034 cm-2s-1
• Pile-up includes 17.3 minimum bias collisions per beam crossing and neutron hits from much earlier crossings
• Aim for single muon rate <10 kHz with >90% efficiency
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 3
ORCA Production SchemeORCA Production SchemeORCA Production SchemeSignal
Zebra fileswith HITS
ORCADigitization
(merge signal and MB)
ObjectivityDatabase
HEPEVTntuples
CMSIM
HLT AlgorithmsNew
ReconstructedObjects
MC Prod.
ORCA
Prod.
HLT Grp
Databases
ORCAooHit
FormatterObjectivityDatabase
MB
ObjectivityDatabase
Catalog import
Catalog import
ObjectivityDatabaseObjectivityDatabaseytivitcejbOytivitcejbOesabataDesabataD
Mirrored D
b’s(CERN
, US, Italy,…)
Geant3
Pyt
hia
6O
RC
A
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 4
Strip FE cards
Wire FE cards
Port Card
PC
Sector Receiver
Sector Processor
OPTICAL
SR SP
CSC Muon Sorter
Global µ Trigger
DTRPC
FE
FE
Global L1
2µ / chamber
3µ / port card
3µ / sector
4µ
4µ
4µ4µ
LCT
Strip LCT + Motherboard card
Wire LCT card
In counting
house
TMB
LCT
RPC Interface Module
RIM
CSC Muon Trigger SchemeCSC Muon Trigger SchemeCSC Muon Trigger SchemeOn-Chamber Trigger Primitives
3-D Track-Finding and Measurement
Combination of all 3 Muon Systems
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 5
Geometric CoverageGeometric CoverageGeometric Coverage
ME4 descoped
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 6
CSC PT ResolutionCSC PCSC PTT ResolutionResolution
• Track segment in ME1 required to have a reasonable measurement (resolution worse than 70% otherwise)
• Track segments in three CSC stations required for optimum PT resolution and rate reduction (implemented in Sector Processor prototype)
PT < 35 GeV
1.2 < |η| < 2.0
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 7
CSC Trigger Efficiency vs. PTCSC Trigger Efficiency vs. CSC Trigger Efficiency vs. PPTT
Trigger threshold defined at 90% efficiency
Sharper turn-on for better PT resolution
Require ME1 for good PTresolution
1.2 < |η| < 2.4
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 8
CSC Trigger Efficiency vs. ηCSC Trigger Efficiency vs. CSC Trigger Efficiency vs. ηη
Significant acceptance loss when 3 stations are required and no ME4
ME4/2 ME4/1
Loose: 2 or more stations including ME1 in endcap,but any two in DT/CSCoverlap region~90% efficiency
Tight: 3 or more stations including ME1 in endcap and MB1 in DT/CSCoverlap ~70% efficiency but better PT resolution
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 9
CSC Single Muon RateCSC Single CSC Single Muon Muon RateRateWeighted minimum bias sample used to estimate rate for L = 1034
Require “tight” track conditions ( ε ≈ 70%)to get acceptable rate from standalone CSC trigger
5 kHz rate for threshold set at 25 GeV
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 10
Previous study did not include effect of punch-through or neutron hits
Had used weighted events with muons
But no significant change in rate or efficiency (< 10%) is seen when effects are included
So real muons dominate the trigger rate
CSC Rate with NeutronsCSC Rate with NeutronsCSC Rate with Neutrons
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 11
CSC Rate without ME4CSC Rate without ME4CSC Rate without ME4
Trigger rate for “loose” condition increases by ~50% if ME4 is removed because of fewer 3-station tracks ⇒ worse PT resolution
Trigger rate for “tight”condition stays about the same because 3-station tracks already required
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 12
Global Muon Trigger EfficiencyGlobal Global MuonMuon Trigger EfficiencyTrigger Efficiency
Recover some inefficiency by combining DT and CSC (loose) with the RPC muon system in an optimized way (see next slide)
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 13
Global Muon Trigger RateGlobal Global Muon Muon Trigger RateTrigger Rate
The GMT optimized algorithm gives an efficiency close to the “OR” of RPC and CSC, but a rate close to the “AND” of the two.
Optimized ⇒ RPC coincidence required in certain regions, choose lowest PT reported by RPC and DT/CSC when matched
8.1 kHz0.18%96.1%optimized
7.2 kHz0.07%89.7%AND
23 kHz1.6%97.6%OR
Rate PT>25
GhostsEfficiencyAlgorithm
Uses “loose” criteria for CSC trigger
US CMS DOE/NSF Review: May 8-10, 2001. D. Acosta, UF 14
ConclusionsConclusionsConclusionsThe previous simulations are the most detailed done to
date of the CMS muon trigger• FE amplifier response/noise is in, neutrons are in, etc.• Trigger logic mostly validated against current hardware
designs (some updates needed)
But we need detailed validation against real data• Testbeam and cosmic ray data
This requires physicist support!• Postdocs, students
It’s important to design a highly efficient L1 CSC Trigger• L2 and L3 algorithms use L1 candidates as seeds.
If L1 misses the muon, physics may be lost…• Must have ME1, and re-scoping ME4 helps at high luminosity• RPC noise/trigger rate may be unacceptably large to help GMT