TY - GEN
T1 - The ATLAS High-Level Calorimeter Trigger in Run-2
AU - Wiglesworth, Graig
AU - Aaboud, M.
AU - Aad, G.
AU - Abbott, B.
AU - Abbott, DC
AU - Abdinov, O.
AU - Abud, AA
AU - Abhayasinghe, DK
AU - Abidi, S.H.
AU - AbouZeid, Ossama Sherif Alexander
AU - Abraham, NL
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B.S.
AU - Adachi, Sosuke
AU - Abramowicz, H.
AU - Adam, Luise
AU - Bourdarios, C.
AU - Besjes, Geert-Jan
AU - Camplani, Alessandra
AU - Alonso Diaz, Alejandro
AU - Galster, Gorm Aske Gram Krohn
AU - Hansen, Jørn Dines
AU - Dam, Mogens
AU - Hansen, Jørgen Beck
AU - de Almeida Dias, Flavia
AU - Hansen, Peter Henrik
AU - Monk, James William
AU - hqz214, hqz214
AU - Bajic, Milena
AU - Stark, Simon Holm
AU - Ignazzi, Rosanna
AU - Xella, Stefania
AU - Petersen, Troels Christian
AU - ATLAS Collaboration
PY - 2019/4/30
Y1 - 2019/4/30
N2 - The ATLAS Experiment uses a two-level triggering system to identify and record proton-proton collision events containing a wide variety of physics signatures. It reduces the event rate from the bunch crossing rate of 40 MHz to an average recording rate of 1 kHz, whilst maintaining high efficiency for interesting collision events. It is composed of an initial hardware-based level-1 trigger followed by a software-based high-level trigger. A central component of the high-level trigger is the calorimeter trigger. This is responsible for processing data from the electromagnetic and hadronic calorimeters in order to identify electrons, photons, taus, jets and missing transverse energy. This paper presents the performance of the high-level calorimeter trigger in Run-2, noting the improvements that have been made in response to the challenges of operating at high luminosity.
AB - The ATLAS Experiment uses a two-level triggering system to identify and record proton-proton collision events containing a wide variety of physics signatures. It reduces the event rate from the bunch crossing rate of 40 MHz to an average recording rate of 1 kHz, whilst maintaining high efficiency for interesting collision events. It is composed of an initial hardware-based level-1 trigger followed by a software-based high-level trigger. A central component of the high-level trigger is the calorimeter trigger. This is responsible for processing data from the electromagnetic and hadronic calorimeters in order to identify electrons, photons, taus, jets and missing transverse energy. This paper presents the performance of the high-level calorimeter trigger in Run-2, noting the improvements that have been made in response to the challenges of operating at high luminosity.
U2 - 10.1088/1742-6596/1162/1/012038
DO - 10.1088/1742-6596/1162/1/012038
M3 - Conference article
SN - 1742-6596
VL - 1162
JO - Journal of Physics - Conference Series
JF - Journal of Physics - Conference Series
M1 - UNSP 012038
ER -