Abstract

The LHCb Outer Tracker is a gaseous detector covering an area of 5 × 6 m2 with 12 double layers of straw tubes. The performance of the detector is presented based on data of the LHC Run 2 running period from 2015 and 2016. Occupancies and operational experience for data collected in pp, pPb and PbPb collisions are described. An updated study of the ageing effects is presented showing no signs of gain deterioration or other radiation damage effects. In addition several improvements with respect to LHC Run 1 data taking are introduced. A novel real-time calibration of the time-alignment of the detector and the alignment of the single monolayers composing detector modules are presented, improving the drift-time and position resolution of the detector by 20%. Finally, a potential use of the improved resolution for the timing of charged tracks is described, showing the possibility to identify low-momentum hadrons with their time-of-flight.

Highlights

  • The LHCb experiment is dedicated to the study of CP violation and rare decays of hadrons with b and c quarks at the Large Hadron Collider

  • The tracking system of the detector is composed of a silicon-strip vertex detector, close to the proton-proton interaction region, and five tracking stations: two upstream and three downstream of a dipole magnet with bending power of around 4 Tm

  • The drift-time measurement capabilities of the Outer Tracker (OT) have been used to measure the time of flight of tracks, which can be exploited for particle identification and for primary interaction vertex assignment and distinction

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Summary

Introduction

Thanks to improvements on the LHC magnets during the Long Shutdown 1 (LS1) period in 2013 and 2014, the LHC provided collisions at a higher centre-of-mass energy of 13 TeV in Run 2 (versus 7 and 8 TeV in Run 1) and proton bunches with a time spacing of 25 ns instead of 50 ns While these conditions are closer to the design values, they are novel, challenging circumstances, motivating the documentation of the performance of the detector in this paper. The drift-time measurement capabilities of the OT have been used to measure the time of flight of tracks, which can be exploited for particle identification and for primary interaction vertex assignment and distinction This method was developed and used for the first time in Run 2, and is presented in section 8 together with its performance

Part I
Performance in Run 2 pp collisions
Occupancies and hits from previous bunch crossings
Hit asymmetries for both magnet polarities
Hit multiplicities in lead-lead and proton-lead collisions
Long term stability of C-frames positions
Effects of opening and closing C-frames
Monitoring of the bridge position
Part II
Performance and monitoring
Module and monolayer spatial alignment
FE-module t0 calibration
TR-relation
Resolution
Time-stamp for single tracks
Time-of-flight for pions and protons
Time-stamp of primary vertices
Findings
Conclusions
Full Text
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