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ALICE Central Trigger System for LHC Run 3

A major upgrade of the ALICE experiment is in progress and will result in high-rate data taking during LHC Run 3 (2022-2024). The LHC interaction rate at Point 2 where the ALICE experiment is located will be increased to 50 kHz in Pb–Pb collisions and 1 MHz in pp collisions. The ALICE experiment wil...

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Autores principales: Kvapil, Jakub, Bhasin, Anju, Bombara, Marek, Evans, David, Jusko, Anton, Kluge, Alexander, Krivda, Marian, Kralik, Ivan, Lietava, Roman, Nayak, Sanket Kumar, Ragoni, Simone, Villalobos Baillie, Orlando
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1051/epjconf/202125104022
http://cds.cern.ch/record/2773261
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author Kvapil, Jakub
Bhasin, Anju
Bombara, Marek
Evans, David
Jusko, Anton
Kluge, Alexander
Krivda, Marian
Kralik, Ivan
Lietava, Roman
Nayak, Sanket Kumar
Ragoni, Simone
Villalobos Baillie, Orlando
author_facet Kvapil, Jakub
Bhasin, Anju
Bombara, Marek
Evans, David
Jusko, Anton
Kluge, Alexander
Krivda, Marian
Kralik, Ivan
Lietava, Roman
Nayak, Sanket Kumar
Ragoni, Simone
Villalobos Baillie, Orlando
author_sort Kvapil, Jakub
collection CERN
description A major upgrade of the ALICE experiment is in progress and will result in high-rate data taking during LHC Run 3 (2022-2024). The LHC interaction rate at Point 2 where the ALICE experiment is located will be increased to 50 kHz in Pb–Pb collisions and 1 MHz in pp collisions. The ALICE experiment will be able to read out data at these interaction rates leading to an increase of the collected luminosity by a factor of up to about 100 with respect to LHC Runs 1 and 2. To satisfy these requirements, a new readout system has been developed for most of the ALICE detectors, allowing the full readout of the data at the required interaction rates without the need for a hardware trigger selection. A novel trigger and timing distribution system will be implemented, based on Passive Optical Network (PON) and GigaBit Transceiver (GBT) technology. To assure backward compatibility a triggered mode based on RD12 Trigger- Timing-Control (TTC) technology, as used in the previous LHC runs, will be maintained and re-implemented under the new Central Trigger System (CTS). A new universal ALICE Trigger Board (ATB) based on the Xilinx Kintex Ultrascale FPGA has been designed to function as a Central Trigger Processor (CTP), Local Trigger Unit (LTU), and monitoring interfaces.In this paper, this new hybrid multilevel system with continuous readout will be described, together with the triggering mechanism and algorithms. An overview of the CTS, the design of the ATB and the different communication protocols will be presented.
id cern-2773261
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2021
record_format invenio
spelling cern-27732612023-01-31T09:43:16Zdoi:10.1051/epjconf/202125104022http://cds.cern.ch/record/2773261engKvapil, JakubBhasin, AnjuBombara, MarekEvans, DavidJusko, AntonKluge, AlexanderKrivda, MarianKralik, IvanLietava, RomanNayak, Sanket KumarRagoni, SimoneVillalobos Baillie, OrlandoALICE Central Trigger System for LHC Run 3nucl-exNuclear Physics - Experimenthep-exParticle Physics - Experimentphysics.ins-detDetectors and Experimental TechniquesA major upgrade of the ALICE experiment is in progress and will result in high-rate data taking during LHC Run 3 (2022-2024). The LHC interaction rate at Point 2 where the ALICE experiment is located will be increased to 50 kHz in Pb–Pb collisions and 1 MHz in pp collisions. The ALICE experiment will be able to read out data at these interaction rates leading to an increase of the collected luminosity by a factor of up to about 100 with respect to LHC Runs 1 and 2. To satisfy these requirements, a new readout system has been developed for most of the ALICE detectors, allowing the full readout of the data at the required interaction rates without the need for a hardware trigger selection. A novel trigger and timing distribution system will be implemented, based on Passive Optical Network (PON) and GigaBit Transceiver (GBT) technology. To assure backward compatibility a triggered mode based on RD12 Trigger- Timing-Control (TTC) technology, as used in the previous LHC runs, will be maintained and re-implemented under the new Central Trigger System (CTS). A new universal ALICE Trigger Board (ATB) based on the Xilinx Kintex Ultrascale FPGA has been designed to function as a Central Trigger Processor (CTP), Local Trigger Unit (LTU), and monitoring interfaces.In this paper, this new hybrid multilevel system with continuous readout will be described, together with the triggering mechanism and algorithms. An overview of the CTS, the design of the ATB and the different communication protocols will be presented.A major upgrade of the ALICE experiment is in progress and will result in high-rate data taking during LHC Run 3 (2022-2024). The LHC interaction rate at Point 2 where the ALICE experiment is located will be increased to $50\ \mathrm{kHz}$ in Pb--Pb collisions and $1\ \mathrm{MHz}$ in pp collisions. The ALICE experiment will be able to read out data at these interaction rates leading to an increase of the collected luminosity by a factor of up to about 100 with respect to LHC Runs 1 and 2. To satisfy these requirements, a new readout system has been developed for most of the ALICE detectors, allowing the full readout of the data at the required interaction rates without the need for a hardware trigger selection. A novel trigger and timing distribution system will be implemented, based on Passive Optical Network (PON) and GigaBit Transceiver (GBT) technology. To assure backward compatibility a triggered mode based on RD12 Trigger-Timing-Control (TTC) technology, as used in the previous LHC runs, will be maintained and re-implemented under the new Central Trigger System (CTS). A new universal ALICE Trigger Board (ATB) based on the Xilinx Kintex Ultrascale FPGA has been designed to function as a Central Trigger Processor (CTP), Local Trigger Unit (LTU), and monitoring interfaces. In this paper, this new hybrid multilevel system with continuous readout will be described, together with the triggering mechanism and algorithms. An overview of the CTS, the design of the ATB and the different communication protocols will be presented.arXiv:2106.08353oai:cds.cern.ch:27732612021
spellingShingle nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
physics.ins-det
Detectors and Experimental Techniques
Kvapil, Jakub
Bhasin, Anju
Bombara, Marek
Evans, David
Jusko, Anton
Kluge, Alexander
Krivda, Marian
Kralik, Ivan
Lietava, Roman
Nayak, Sanket Kumar
Ragoni, Simone
Villalobos Baillie, Orlando
ALICE Central Trigger System for LHC Run 3
title ALICE Central Trigger System for LHC Run 3
title_full ALICE Central Trigger System for LHC Run 3
title_fullStr ALICE Central Trigger System for LHC Run 3
title_full_unstemmed ALICE Central Trigger System for LHC Run 3
title_short ALICE Central Trigger System for LHC Run 3
title_sort alice central trigger system for lhc run 3
topic nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
physics.ins-det
Detectors and Experimental Techniques
url https://dx.doi.org/10.1051/epjconf/202125104022
http://cds.cern.ch/record/2773261
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