Abstract

For the 2016 physics data runs, the L1 trigger system of the compact muon solenoid (CMS) experiment underwent a major upgrade to cope with the increasing instantaneous luminosity of the CERN LHC whilst maintaining a high event selection efficiency for the CMS physics program. Most subsystem specific trigger processor boards were replaced with powerful general purpose processor boards, conforming to the MicroTCA standard, whose tasks are performed by firmware on an field-programmable gate array of the Xilinx Virtex 7 family. Furthermore, the muon trigger system moved from a subsystem centered approach, where each of the three muon detector systems provides muon candidates to the global muon trigger (GMT), to a region-based system, where muon track finders (TFs) combine information from the subsystems to generate muon candidates in three detector regions that are then sent to the upgraded GMT. The upgraded GMT receives up to 108 muons from the processors of the muon TFs in the barrel, overlap, and endcap detector regions. The muons are sorted in two steps and duplicates are identified for removal. The first step treats muons from different processors of a TF in one detector region. Muons from TFs in different detector regions are compared in the second step. An isolation variable is calculated, using energy sums from the calorimeter trigger and added to each of the best eight muons before they are sent to the upgraded global trigger (GT) where the final trigger decision is made. The upgraded GMT algorithm is implemented on a general purpose processor board that uses optical links at 10 Gb/s to receive the input data from the muon TFs and the calorimeter energy sums, and to send the selected muon candidates to the upgraded GT.

Highlights

  • A FTER having been upgraded during its first long shutdown in 2013 and 2014 the CERN LHC started its second running period (Run-II) in 2015

  • In the global muon trigger (GMT), the muons are sorted in two sorting stages, duplicate muons are removed and up to eight muons are sent to the global trigger (GT), doubling the number of muons the legacy GT received

  • In case of a tie in quality, the muons coming from the barrel muon TF (BMTF) and the endcap muon TF (EMTF) win over muons from the overlap muon TF (OMTF) and muons from the wedge or sector on the lower φ side win over muons from their neighboring wedge or sector, except for the boundary at the φ wrap-around where muons from wedge 12 or sector 6 win over muons from wedge 1 or sector 1, respectively

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Summary

INTRODUCTION

A FTER having been upgraded during its first long shutdown in 2013 and 2014 the CERN LHC started its second running period (Run-II) in 2015. With such LHC performance parameters the trigger rate of the first level (L1) of the compact muon solenoid (CMS) trigger system would have increased by around a factor of six, with respect to the time before the long shutdown, were the trigger thresholds kept the same [1]. If the muon is produced within a jet of other particles via an in-flight decay, those other particles leave a significant energy deposit in the calorimeters, allowing the separation of the two different cases To achieve these improvements, more sophisticated algorithms were developed that require more powerful hardware, which has become available in the time since the design of the legacy trigger system. The performance of the upgraded trigger measured from early 2016 collision data is studied

CMS Detector
UPGRADED MUON TRIGGER
Common Hardware
GLOBAL MUON TRIGGER
Hardware and Firmware
Muon Sorting
Duplicate Muon Removal
Isolation
Commissioning of the Upgrade Trigger
Results of Studies on Data Taken During the LHC Startup 2016
Findings
CONCLUSION
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