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Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations

The Large Hadron Collider (LHC) at the European Organization for Nuclear Research (CERN) is the largest accelerator in the world, spanning a circumference of 26.7 km. During its operation, small fractions of the beams are being continuously lost. This leads to mixed-field radiation that might affect...

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Autores principales: Biłko, Kacper, Bahamonde Castro, Cristina, Brugger, Markus, García Alía, Rubén, Kadi, Yacine, Lechner, Anton, Lerner, Giuseppe, Stein, Oliver
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TNS.2020.2970168
http://cds.cern.ch/record/2725326
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author Biłko, Kacper
Bahamonde Castro, Cristina
Brugger, Markus
García Alía, Rubén
Kadi, Yacine
Lechner, Anton
Lerner, Giuseppe
Stein, Oliver
author_facet Biłko, Kacper
Bahamonde Castro, Cristina
Brugger, Markus
García Alía, Rubén
Kadi, Yacine
Lechner, Anton
Lerner, Giuseppe
Stein, Oliver
author_sort Biłko, Kacper
collection CERN
description The Large Hadron Collider (LHC) at the European Organization for Nuclear Research (CERN) is the largest accelerator in the world, spanning a circumference of 26.7 km. During its operation, small fractions of the beams are being continuously lost. This leads to mixed-field radiation that might affect electronic equipment through both cumulative and single-event effects. This article considers the radiation environment during Run 2 (years 2015–2018) in the LHC arc sectors that constitute approximately 70% of the accelerator, housing a huge amount of electronics. There, the main magnets’ configuration is periodic, and the main contributor to losses is the interaction of the beams with residual gas molecules, resulting in relatively low-radiation levels, as opposed to different parts of the LHC. However, as presented, there are locations where losses are no longer dominated by residual gas. In these locations, radiation levels are higher by up to more than two orders of magnitude and could, therefore, be problematic in terms of cumulative radiation effects on electronics. In this article, the dose measurements from beam loss monitors have been combined with the FLUKA simulation for the arc sectors in order to indirectly retrieve the residual gas densities and radiation profile under the magnet cryostats, at the equipment level, for the losses caused by residual gas. Estimations for the radiation levels in the arc sectors during the high-luminosity LHC era and potential implications for the electronics are discussed as well.
id oai-inspirehep.net-1808323
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
record_format invenio
spelling oai-inspirehep.net-18083232020-09-28T17:07:37Zdoi:10.1109/TNS.2020.2970168http://cds.cern.ch/record/2725326engBiłko, KacperBahamonde Castro, CristinaBrugger, MarkusGarcía Alía, RubénKadi, YacineLechner, AntonLerner, GiuseppeStein, OliverRadiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC OperationsDetectors and Experimental TechniquesAccelerators and Storage RingsThe Large Hadron Collider (LHC) at the European Organization for Nuclear Research (CERN) is the largest accelerator in the world, spanning a circumference of 26.7 km. During its operation, small fractions of the beams are being continuously lost. This leads to mixed-field radiation that might affect electronic equipment through both cumulative and single-event effects. This article considers the radiation environment during Run 2 (years 2015–2018) in the LHC arc sectors that constitute approximately 70% of the accelerator, housing a huge amount of electronics. There, the main magnets’ configuration is periodic, and the main contributor to losses is the interaction of the beams with residual gas molecules, resulting in relatively low-radiation levels, as opposed to different parts of the LHC. However, as presented, there are locations where losses are no longer dominated by residual gas. In these locations, radiation levels are higher by up to more than two orders of magnitude and could, therefore, be problematic in terms of cumulative radiation effects on electronics. In this article, the dose measurements from beam loss monitors have been combined with the FLUKA simulation for the arc sectors in order to indirectly retrieve the residual gas densities and radiation profile under the magnet cryostats, at the equipment level, for the losses caused by residual gas. Estimations for the radiation levels in the arc sectors during the high-luminosity LHC era and potential implications for the electronics are discussed as well.oai:inspirehep.net:18083232020
spellingShingle Detectors and Experimental Techniques
Accelerators and Storage Rings
Biłko, Kacper
Bahamonde Castro, Cristina
Brugger, Markus
García Alía, Rubén
Kadi, Yacine
Lechner, Anton
Lerner, Giuseppe
Stein, Oliver
Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title_full Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title_fullStr Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title_full_unstemmed Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title_short Radiation Environment in the LHC Arc Sections During Run 2 and Future HL-LHC Operations
title_sort radiation environment in the lhc arc sections during run 2 and future hl-lhc operations
topic Detectors and Experimental Techniques
Accelerators and Storage Rings
url https://dx.doi.org/10.1109/TNS.2020.2970168
http://cds.cern.ch/record/2725326
work_keys_str_mv AT biłkokacper radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT bahamondecastrocristina radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT bruggermarkus radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT garciaaliaruben radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT kadiyacine radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT lechneranton radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT lernergiuseppe radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations
AT steinoliver radiationenvironmentinthelhcarcsectionsduringrun2andfuturehllhcoperations