Cargando…

CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications

The super proton synchrotron (SPS) is the second largest accelerator at CERN where protons are accelerated between 16 and 450 GeV/c. Beam losses, leading to the mixed-field radiation of up to MGy magnitude, pose a threat to the reliability of the electronic equipment and polymer materials located in...

Descripción completa

Detalles Bibliográficos
Autores principales: Biłko, Kacper, García Alía, Rubén, Di Francesca, Diego, Aguiar, Ygor, Danzeca, Salvatore, Gilardoni, Simone, Girard, Sylvain, Esposito, Luigi Salvatore, Fraser, Matthew Alexander, Mazzola, Giuseppe, Ricci, Daniel, Sebban, Marc, Velotti, Francesco Maria
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:https://dx.doi.org/10.1109/TNS.2023.3261181
http://cds.cern.ch/record/2875172
_version_ 1780978881565556736
author Biłko, Kacper
García Alía, Rubén
Di Francesca, Diego
Aguiar, Ygor
Danzeca, Salvatore
Gilardoni, Simone
Girard, Sylvain
Esposito, Luigi Salvatore
Fraser, Matthew Alexander
Mazzola, Giuseppe
Ricci, Daniel
Sebban, Marc
Velotti, Francesco Maria
author_facet Biłko, Kacper
García Alía, Rubén
Di Francesca, Diego
Aguiar, Ygor
Danzeca, Salvatore
Gilardoni, Simone
Girard, Sylvain
Esposito, Luigi Salvatore
Fraser, Matthew Alexander
Mazzola, Giuseppe
Ricci, Daniel
Sebban, Marc
Velotti, Francesco Maria
author_sort Biłko, Kacper
collection CERN
description The super proton synchrotron (SPS) is the second largest accelerator at CERN where protons are accelerated between 16 and 450 GeV/c. Beam losses, leading to the mixed-field radiation of up to MGy magnitude, pose a threat to the reliability of the electronic equipment and polymer materials located in the tunnel and its vicinity. In particular, in the arc sectors, where both main magnets and radiation sensors are periodically arranged, the total ionizing dose (TID) is of concern for the front-end electronics of a logarithmic position system (ALPS). The SPS is equipped with multiple radiation detection systems, such as beam loss monitors (BLMs), RadMons, and as of 2021, the distributed optical fiber radiation sensor (DOFRS) that combined all together provides a very comprehensive picture of both the TID spatial distribution and its time evolution. Within this study, the overview of measured 2021 and 2022 TID levels is presented, together with the demonstration of capabilities offered by the different radiation monitors. The DOFRS, supported by the passive radiophotoluminescence (RPL) dosimeter measurements, is used to assess the TID values directly at the electronic racks, which turned out to be reaching several tens of Gy/year, potentially affecting the ALPS lifetime.
id cern-2875172
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2023
record_format invenio
spelling cern-28751722023-10-18T09:19:55Zdoi:10.1109/TNS.2023.3261181http://cds.cern.ch/record/2875172engBiłko, KacperGarcía Alía, RubénDi Francesca, DiegoAguiar, YgorDanzeca, SalvatoreGilardoni, SimoneGirard, SylvainEsposito, Luigi SalvatoreFraser, Matthew AlexanderMazzola, GiuseppeRicci, DanielSebban, MarcVelotti, Francesco MariaCERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance ImplicationsAccelerators and Storage RingsDetectors and Experimental TechniquesThe super proton synchrotron (SPS) is the second largest accelerator at CERN where protons are accelerated between 16 and 450 GeV/c. Beam losses, leading to the mixed-field radiation of up to MGy magnitude, pose a threat to the reliability of the electronic equipment and polymer materials located in the tunnel and its vicinity. In particular, in the arc sectors, where both main magnets and radiation sensors are periodically arranged, the total ionizing dose (TID) is of concern for the front-end electronics of a logarithmic position system (ALPS). The SPS is equipped with multiple radiation detection systems, such as beam loss monitors (BLMs), RadMons, and as of 2021, the distributed optical fiber radiation sensor (DOFRS) that combined all together provides a very comprehensive picture of both the TID spatial distribution and its time evolution. Within this study, the overview of measured 2021 and 2022 TID levels is presented, together with the demonstration of capabilities offered by the different radiation monitors. The DOFRS, supported by the passive radiophotoluminescence (RPL) dosimeter measurements, is used to assess the TID values directly at the electronic racks, which turned out to be reaching several tens of Gy/year, potentially affecting the ALPS lifetime.oai:cds.cern.ch:28751722023
spellingShingle Accelerators and Storage Rings
Detectors and Experimental Techniques
Biłko, Kacper
García Alía, Rubén
Di Francesca, Diego
Aguiar, Ygor
Danzeca, Salvatore
Gilardoni, Simone
Girard, Sylvain
Esposito, Luigi Salvatore
Fraser, Matthew Alexander
Mazzola, Giuseppe
Ricci, Daniel
Sebban, Marc
Velotti, Francesco Maria
CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title_full CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title_fullStr CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title_full_unstemmed CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title_short CERN Super Proton Synchrotron Radiation Environment and Related Radiation Hardness Assurance Implications
title_sort cern super proton synchrotron radiation environment and related radiation hardness assurance implications
topic Accelerators and Storage Rings
Detectors and Experimental Techniques
url https://dx.doi.org/10.1109/TNS.2023.3261181
http://cds.cern.ch/record/2875172
work_keys_str_mv AT biłkokacper cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT garciaaliaruben cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT difrancescadiego cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT aguiarygor cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT danzecasalvatore cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT gilardonisimone cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT girardsylvain cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT espositoluigisalvatore cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT frasermatthewalexander cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT mazzolagiuseppe cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT riccidaniel cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT sebbanmarc cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications
AT velottifrancescomaria cernsuperprotonsynchrotronradiationenvironmentandrelatedradiationhardnessassuranceimplications