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A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC

The ATLAS Collaboration has planned significant upgrades to the muon system, in order to cope with the instantaneous luminosity that will be delivered by the Large Hadron Collider (LHC) machine. The upgrades will allow the Muon Spectrometer to keep and improve its current performance for the High Lu...

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Detalles Bibliográficos
Autores principales: Albano, Andrea, Aloisio, Alberto, Izzo, Vincenzo, Vari, Riccardo, Corradi, Massimo
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1109/NSS/MIC44867.2021.9875882
http://cds.cern.ch/record/2798220
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author Albano, Andrea
Aloisio, Alberto
Izzo, Vincenzo
Vari, Riccardo
Corradi, Massimo
author_facet Albano, Andrea
Aloisio, Alberto
Izzo, Vincenzo
Vari, Riccardo
Corradi, Massimo
author_sort Albano, Andrea
collection CERN
description The ATLAS Collaboration has planned significant upgrades to the muon system, in order to cope with the instantaneous luminosity that will be delivered by the Large Hadron Collider (LHC) machine. The upgrades will allow the Muon Spectrometer to keep and improve its current performance for the High Luminosity LHC program (HL-LHC) expected to start in ∼2027. Together with the detector, most of the trigger and readout electronics of the Muon Spectrometer will be replaced, so that all hit data will be optically transferred from the frontend to the backend boards, where the first-level muon trigger (L0Muon) will be executed with latency of 10 $\mu$s and maximum trigger rate of 1 MHz. For the Barrel region, the L0 muon trigger algorithm is performed off-detector by 32 ATCA FPGA-based boards, called Sector Logic (SL), which receive detector data, perform the L0 algorithm, use the muon candidate track information from the MDT detectors and send the muon trigger candidate information to the Central Trigger Processor. In this work, we present a proof of concept of the trigger candidate identification algorithm for the L0Muon trigger in the barrel region. It is executed in the SL FPGA and it is based on a massive use of Digital Signal Processors (DSPs) Slices available in a Xilinx FPGA device. The algorithm is able to identify up to three muon candidates with a transverse momentum (pT) higher than a given threshold, and uses the DSP features of manipulating a large amount of bits and of providing results of its calculation in few clock cycles, with a low and deterministic latency. We discuss a first implementation of our architecture in a Xilinx Evaluation board based on a Kintex-7 FPGA, although the design can be easily targeted to newer or larger devices, such as the Ultrascale+ that will be used in the experiment. We describe the logic resources occupation of the design, its performances in terms of maximum operation frequency and latency.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2021
record_format invenio
spelling cern-27982202023-05-24T13:22:48Zdoi:10.1109/NSS/MIC44867.2021.9875882http://cds.cern.ch/record/2798220engAlbano, AndreaAloisio, AlbertoIzzo, VincenzoVari, RiccardoCorradi, MassimoA Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHCParticle Physics - ExperimentThe ATLAS Collaboration has planned significant upgrades to the muon system, in order to cope with the instantaneous luminosity that will be delivered by the Large Hadron Collider (LHC) machine. The upgrades will allow the Muon Spectrometer to keep and improve its current performance for the High Luminosity LHC program (HL-LHC) expected to start in ∼2027. Together with the detector, most of the trigger and readout electronics of the Muon Spectrometer will be replaced, so that all hit data will be optically transferred from the frontend to the backend boards, where the first-level muon trigger (L0Muon) will be executed with latency of 10 $\mu$s and maximum trigger rate of 1 MHz. For the Barrel region, the L0 muon trigger algorithm is performed off-detector by 32 ATCA FPGA-based boards, called Sector Logic (SL), which receive detector data, perform the L0 algorithm, use the muon candidate track information from the MDT detectors and send the muon trigger candidate information to the Central Trigger Processor. In this work, we present a proof of concept of the trigger candidate identification algorithm for the L0Muon trigger in the barrel region. It is executed in the SL FPGA and it is based on a massive use of Digital Signal Processors (DSPs) Slices available in a Xilinx FPGA device. The algorithm is able to identify up to three muon candidates with a transverse momentum (pT) higher than a given threshold, and uses the DSP features of manipulating a large amount of bits and of providing results of its calculation in few clock cycles, with a low and deterministic latency. We discuss a first implementation of our architecture in a Xilinx Evaluation board based on a Kintex-7 FPGA, although the design can be easily targeted to newer or larger devices, such as the Ultrascale+ that will be used in the experiment. We describe the logic resources occupation of the design, its performances in terms of maximum operation frequency and latency.ATL-DAQ-PROC-2021-020oai:cds.cern.ch:27982202021-12-15
spellingShingle Particle Physics - Experiment
Albano, Andrea
Aloisio, Alberto
Izzo, Vincenzo
Vari, Riccardo
Corradi, Massimo
A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title_full A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title_fullStr A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title_full_unstemmed A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title_short A Trigger Demonstrator for the L0 Muon Barrel Trigger of the ATLAS Experiment for HL-LHC
title_sort trigger demonstrator for the l0 muon barrel trigger of the atlas experiment for hl-lhc
topic Particle Physics - Experiment
url https://dx.doi.org/10.1109/NSS/MIC44867.2021.9875882
http://cds.cern.ch/record/2798220
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