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doi: 10.1088/1748-0221/18/11/p11006 , 10.48550/arxiv.2306.09738 , 10.3204/pubdb-2023-07553 , 10.3204/pubdb-2023-04995
handle: 10261/351080 , https://repository.ubn.ru.nl/handle/2066/298585 , 11588/953094 , 11368/3100924 , 11245.1/6ed9ffce-c337-40f4-b73f-c5c2db8b7d33 , 20.500.11851/11010 , 10852/108246 , 2066/298585 , 2434/1032456 , 20.500.11770/361266 , 11572/412632 , 11390/1270526 , 2108/345452 , 11590/462751 , 11568/1238888 , 11587/507466 , 11585/955680 , 11582/344554 , 1959.3/477057
doi: 10.1088/1748-0221/18/11/p11006 , 10.48550/arxiv.2306.09738 , 10.3204/pubdb-2023-07553 , 10.3204/pubdb-2023-04995
handle: 10261/351080 , https://repository.ubn.ru.nl/handle/2066/298585 , 11588/953094 , 11368/3100924 , 11245.1/6ed9ffce-c337-40f4-b73f-c5c2db8b7d33 , 20.500.11851/11010 , 10852/108246 , 2066/298585 , 2434/1032456 , 20.500.11770/361266 , 11572/412632 , 11390/1270526 , 2108/345452 , 11590/462751 , 11568/1238888 , 11587/507466 , 11585/955680 , 11582/344554 , 1959.3/477057
Abstract The ATLAS experiment relies on real-time hadronic jet reconstruction and b-tagging to record fully hadronic events containing b-jets. These algorithms require track reconstruction, which is computationally expensive and could overwhelm the high-level-trigger farm, even at the reduced event rate that passes the ATLAS first stage hardware-based trigger. In LHC Run 3, ATLAS has mitigated these computational demands by introducing a fast neural-network-based b-tagger, which acts as a low-precision filter using input from hadronic jets and tracks. It runs after a hardware trigger and before the remaining high-level-trigger reconstruction. This design relies on the negligible cost of neural-network inference as compared to track reconstruction, and the cost reduction from limiting tracking to specific regions of the detector. In the case of Standard Model HH → bb̅bb̅, a key signature relying on b-jet triggers, the filter lowers the input rate to the remaining high-level trigger by a factor of five at the small cost of reducing the overall signal efficiency by roughly 2%.
Bottom: particle identification, Final state: ((n)jet), final state: ((n)jet), Jet: bottom, Track data analysis: jet, costs, bottom: particle identification, Efficiency, Signature, trigger algorithms, High Energy Physics - Experiment, Subatomär fysik, High Energy Physics - Experiment (hep-ex), Engineering, Tracks, Subatomic Physics, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Trigger: hardware, Trigger concepts and systems, info:eu-repo/classification/ddc/610, Settore FIS/01, Trigger algorithm, Trigger Algorithms, Data analysis method, trigger concepts and systems (hardware and software), Jet: trigger, Trigger algorithms, ATLAS, : Trigger algorithms, Nuclear and Plasma Physics, Nuclear & Particles Physics, 004, Physical sciences, P p: scattering, CERN LHC Coll, Trigger concepts and systems (hardware and software), Statistical analysis, track data analysis: jet, Physical Sciences, High energy physics; ATLAS experiment; B-tagging; Hadronic jets; Hardware and software; High-level triggers; System hardware; System softwares; Track reconstruction; Trigger algorithms; Trigger concept and system (hardware and software); Cost reduction, Higgs particle: pair production, jet: bottom, jet: trigger, signature, p p: scattering, data analysis method, [PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex], neural network, 610, FOS: Physical sciences, Bioengineering, bottom: pair production, 530, Trigger algorithms | Trigger concepts and systems (hardware and software), Trigger Concepts And Systems (Hardware And Software), Trigger algorithms; Trigger concepts and systems (hardware and software), statistical analysis, 539, High Energy Physics, Trigger algorithms, Trigger concepts and systems (hardware and software), P p: colliding beams, 500, Jet: hadronic, jet: hadronic, tracks, Neural network, Costs, efficiency, Higgs particle: hadronic decay, Experimental High Energy Physics, trigger: hardware, Hadron-hadron collisions, Bottom: pair production, p p: colliding beams, 500.2
Bottom: particle identification, Final state: ((n)jet), final state: ((n)jet), Jet: bottom, Track data analysis: jet, costs, bottom: particle identification, Efficiency, Signature, trigger algorithms, High Energy Physics - Experiment, Subatomär fysik, High Energy Physics - Experiment (hep-ex), Engineering, Tracks, Subatomic Physics, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], Trigger: hardware, Trigger concepts and systems, info:eu-repo/classification/ddc/610, Settore FIS/01, Trigger algorithm, Trigger Algorithms, Data analysis method, trigger concepts and systems (hardware and software), Jet: trigger, Trigger algorithms, ATLAS, : Trigger algorithms, Nuclear and Plasma Physics, Nuclear & Particles Physics, 004, Physical sciences, P p: scattering, CERN LHC Coll, Trigger concepts and systems (hardware and software), Statistical analysis, track data analysis: jet, Physical Sciences, High energy physics; ATLAS experiment; B-tagging; Hadronic jets; Hardware and software; High-level triggers; System hardware; System softwares; Track reconstruction; Trigger algorithms; Trigger concept and system (hardware and software); Cost reduction, Higgs particle: pair production, jet: bottom, jet: trigger, signature, p p: scattering, data analysis method, [PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex], neural network, 610, FOS: Physical sciences, Bioengineering, bottom: pair production, 530, Trigger algorithms | Trigger concepts and systems (hardware and software), Trigger Concepts And Systems (Hardware And Software), Trigger algorithms; Trigger concepts and systems (hardware and software), statistical analysis, 539, High Energy Physics, Trigger algorithms, Trigger concepts and systems (hardware and software), P p: colliding beams, 500, Jet: hadronic, jet: hadronic, tracks, Neural network, Costs, efficiency, Higgs particle: hadronic decay, Experimental High Energy Physics, trigger: hardware, Hadron-hadron collisions, Bottom: pair production, p p: colliding beams, 500.2
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