TY - JOUR
T1 - Electron efficiency measurements with the ATLAS detector using 2012 LHC proton–proton collision data
AU - Barnes, Sarah
AU - Bielski, Rafal
AU - Cox, Brian
AU - Da Via, Cinzia
AU - Dann, Nick
AU - Forcolin, Giulio
AU - Forti, Alessandra
AU - Iturbe Ponce, Julia
AU - Li, Xingguo
AU - Loebinger, Frederick
AU - Marsden, Stephen
AU - Masik, Jiri
AU - Menary, Stephen
AU - Munoz Sanchez, Francisca
AU - Neep, Thomas
AU - Oh, Alexander
AU - Ospanov, Rustem
AU - Pater, Joleen
AU - Peters, Yvonne
AU - Pilkington, Andrew
AU - Pin, Arnaud
AU - Price, Darren
AU - Qin, Yang
AU - Raine, John
AU - Roberts, Rhys
AU - Shaw, Savanna
AU - Tomlinson, Lee
AU - Watts, Stephen
AU - Wilk, Fabian
AU - Woudstra, Martin
AU - Wyatt, Terence
AU - ATLAS Collaboration
PY - 2017
Y1 - 2017
N2 - This paper describes the algorithms for the reconstruction and identification of electrons in the central region of the ATLAS detector at the Large Hadron Collider (LHC). These algorithms were used for all ATLAS results with electrons in the final state that are based on the 2012 pp collision data produced by the LHC at s√s = 8 TeVTeV . The efficiency of these algorithms, together with the charge misidentification rate, is measured in data and evaluated in simulated samples using electrons from Z→ee, Z→eeγ and J/ψ→ee decays. For these efficiency measurements, the full recorded data set, corresponding to an integrated luminosity of 20.3 fb −1 , is used. Based on a new reconstruction algorithm used in 2012, the electron reconstruction efficiency is 97% for electrons with ET=15 GeV and 99% at ET=50GeV . Combining this with the efficiency of additional selection criteria to reject electrons from background processes or misidentified hadrons, the efficiency to reconstruct and identify electrons at the ATLAS experiment varies from 65 to 95%, depending on the transverse momentum of the electron and background rejection.
AB - This paper describes the algorithms for the reconstruction and identification of electrons in the central region of the ATLAS detector at the Large Hadron Collider (LHC). These algorithms were used for all ATLAS results with electrons in the final state that are based on the 2012 pp collision data produced by the LHC at s√s = 8 TeVTeV . The efficiency of these algorithms, together with the charge misidentification rate, is measured in data and evaluated in simulated samples using electrons from Z→ee, Z→eeγ and J/ψ→ee decays. For these efficiency measurements, the full recorded data set, corresponding to an integrated luminosity of 20.3 fb −1 , is used. Based on a new reconstruction algorithm used in 2012, the electron reconstruction efficiency is 97% for electrons with ET=15 GeV and 99% at ET=50GeV . Combining this with the efficiency of additional selection criteria to reject electrons from background processes or misidentified hadrons, the efficiency to reconstruct and identify electrons at the ATLAS experiment varies from 65 to 95%, depending on the transverse momentum of the electron and background rejection.
UR - https://www.scopus.com/pages/publications/85016328339
U2 - 10.1140/epjc/s10052-017-4756-2
DO - 10.1140/epjc/s10052-017-4756-2
M3 - Article
SN - 1434-6044
VL - 77
JO - European Physical Journal C. Particles and Fields
JF - European Physical Journal C. Particles and Fields
IS - 195
ER -