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Improving topological cluster reconstruction using calorimeter cell timing in ATLAS

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Improving topological cluster reconstruction using calorimeter cell timing in ATLAS. / The ATLAS collaboration.
In: European Physical Journal C: Particles and Fields, Vol. 84, No. 5, 455, 03.05.2024.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

The ATLAS collaboration 2024, 'Improving topological cluster reconstruction using calorimeter cell timing in ATLAS', European Physical Journal C: Particles and Fields, vol. 84, no. 5, 455. https://doi.org/10.1140/epjc/s10052-024-12657-1

APA

The ATLAS collaboration (2024). Improving topological cluster reconstruction using calorimeter cell timing in ATLAS. European Physical Journal C: Particles and Fields, 84(5), Article 455. https://doi.org/10.1140/epjc/s10052-024-12657-1

Vancouver

The ATLAS collaboration. Improving topological cluster reconstruction using calorimeter cell timing in ATLAS. European Physical Journal C: Particles and Fields. 2024 May 3;84(5):455. doi: 10.1140/epjc/s10052-024-12657-1

Author

The ATLAS collaboration. / Improving topological cluster reconstruction using calorimeter cell timing in ATLAS. In: European Physical Journal C: Particles and Fields. 2024 ; Vol. 84, No. 5.

Bibtex

@article{3ba56181935543f7b5085c42a84ce043,
title = "Improving topological cluster reconstruction using calorimeter cell timing in ATLAS",
abstract = "Clusters of topologically connected calorimeter cells around cells with large absolute signal-to-noise ratio (topo-clusters) are the basis for calorimeter signal reconstruction in the ATLAS experiment. Topological cell clustering has proven performant in LHC Runs 1 and 2. It is, however, susceptible to out-of-time pile-up of signals from soft collisions outside the 25 ns proton-bunch-crossing window associated with the event{\textquoteright}s hard collision. To reduce this effect, a calorimeter-cell timing criterion was added to the signal-to-noise ratio requirement in the clustering algorithm. Multiple versions of this criterion were tested by reconstructing hadronic signals in simulated events and Run 2 ATLAS data. The preferred version is found to reduce the out-of-time pile-up jet multiplicity by $${\sim }50\%$$ ∼ 50 % for jet $$p_{\textrm{T}}\sim 20$$ p T ∼ 20 GeV and by $${\sim }80\%$$ ∼ 80 % for jet $$p_{\textrm{T}} \gtrsim 50$$ p T ≳ 50 GeV, while not disrupting the reconstruction of hadronic signals of interest, and improving the jet energy resolution by up to 5% for $$20< p_{\textrm{T}} < 30$$ 20 < p T < 30 GeV. Pile-up is also suppressed for other physics objects based on topo-clusters (electrons, photons, $$\tau $$ τ -leptons), reducing the overall event size on disk by about $$6\%$$ 6 % in early Run 3 pile-up conditions. Offline reconstruction for Run 3 includes the timing requirement.",
author = "{The ATLAS collaboration} and A.E. Barton and I.A. Bertram and G. Borissov and E.V. Bouhova-Thacker and Ruby Ferguson and James Ferrando and H. Fox and Alina Hagan and R.C.W. Henderson and R.W.L. Jones and V. Kartvelishvili and P.A. Love and E.J. Marshall and L. Meng and D. Muenstermann and N. Ribaric and K. Rybacki and M. Smizanska and S. Spinali and A.M. Wharton",
year = "2024",
month = may,
day = "3",
doi = "10.1140/epjc/s10052-024-12657-1",
language = "English",
volume = "84",
journal = "European Physical Journal C: Particles and Fields",
issn = "1434-6044",
publisher = "SPRINGER",
number = "5",

}

RIS

TY - JOUR

T1 - Improving topological cluster reconstruction using calorimeter cell timing in ATLAS

AU - The ATLAS collaboration

AU - Barton, A.E.

AU - Bertram, I.A.

AU - Borissov, G.

AU - Bouhova-Thacker, E.V.

AU - Ferguson, Ruby

AU - Ferrando, James

AU - Fox, H.

AU - Hagan, Alina

AU - Henderson, R.C.W.

AU - Jones, R.W.L.

AU - Kartvelishvili, V.

AU - Love, P.A.

AU - Marshall, E.J.

AU - Meng, L.

AU - Muenstermann, D.

AU - Ribaric, N.

AU - Rybacki, K.

AU - Smizanska, M.

AU - Spinali, S.

AU - Wharton, A.M.

PY - 2024/5/3

Y1 - 2024/5/3

N2 - Clusters of topologically connected calorimeter cells around cells with large absolute signal-to-noise ratio (topo-clusters) are the basis for calorimeter signal reconstruction in the ATLAS experiment. Topological cell clustering has proven performant in LHC Runs 1 and 2. It is, however, susceptible to out-of-time pile-up of signals from soft collisions outside the 25 ns proton-bunch-crossing window associated with the event’s hard collision. To reduce this effect, a calorimeter-cell timing criterion was added to the signal-to-noise ratio requirement in the clustering algorithm. Multiple versions of this criterion were tested by reconstructing hadronic signals in simulated events and Run 2 ATLAS data. The preferred version is found to reduce the out-of-time pile-up jet multiplicity by $${\sim }50\%$$ ∼ 50 % for jet $$p_{\textrm{T}}\sim 20$$ p T ∼ 20 GeV and by $${\sim }80\%$$ ∼ 80 % for jet $$p_{\textrm{T}} \gtrsim 50$$ p T ≳ 50 GeV, while not disrupting the reconstruction of hadronic signals of interest, and improving the jet energy resolution by up to 5% for $$20< p_{\textrm{T}} < 30$$ 20 < p T < 30 GeV. Pile-up is also suppressed for other physics objects based on topo-clusters (electrons, photons, $$\tau $$ τ -leptons), reducing the overall event size on disk by about $$6\%$$ 6 % in early Run 3 pile-up conditions. Offline reconstruction for Run 3 includes the timing requirement.

AB - Clusters of topologically connected calorimeter cells around cells with large absolute signal-to-noise ratio (topo-clusters) are the basis for calorimeter signal reconstruction in the ATLAS experiment. Topological cell clustering has proven performant in LHC Runs 1 and 2. It is, however, susceptible to out-of-time pile-up of signals from soft collisions outside the 25 ns proton-bunch-crossing window associated with the event’s hard collision. To reduce this effect, a calorimeter-cell timing criterion was added to the signal-to-noise ratio requirement in the clustering algorithm. Multiple versions of this criterion were tested by reconstructing hadronic signals in simulated events and Run 2 ATLAS data. The preferred version is found to reduce the out-of-time pile-up jet multiplicity by $${\sim }50\%$$ ∼ 50 % for jet $$p_{\textrm{T}}\sim 20$$ p T ∼ 20 GeV and by $${\sim }80\%$$ ∼ 80 % for jet $$p_{\textrm{T}} \gtrsim 50$$ p T ≳ 50 GeV, while not disrupting the reconstruction of hadronic signals of interest, and improving the jet energy resolution by up to 5% for $$20< p_{\textrm{T}} < 30$$ 20 < p T < 30 GeV. Pile-up is also suppressed for other physics objects based on topo-clusters (electrons, photons, $$\tau $$ τ -leptons), reducing the overall event size on disk by about $$6\%$$ 6 % in early Run 3 pile-up conditions. Offline reconstruction for Run 3 includes the timing requirement.

U2 - 10.1140/epjc/s10052-024-12657-1

DO - 10.1140/epjc/s10052-024-12657-1

M3 - Journal article

VL - 84

JO - European Physical Journal C: Particles and Fields

JF - European Physical Journal C: Particles and Fields

SN - 1434-6044

IS - 5

M1 - 455

ER -