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Single event effects in high-energy accelerators

The radiation environment encountered at high-energy hadron accelerators strongly differs from the environment relevant for space applications. The mixed-field expected at modern accelerators is composed of charged and neutral hadrons (protons, pions, kaons and neutrons), photons, electrons, positro...

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Autores principales: García Alía, Rubén, Brugger, Markus, Danzeca, Salvatore, Cerutti, Francesco, de Carvalho Saraiva, Joao Pedro, Denz, Reiner, Ferrari, Alfredo, Foro, Lionel L, Peronnard, Paul, Røed, Ketil, Secondo, Raffaello, Steckert, Jens, Thurel, Yves, Toccafondo, Iacocpo, Uznanski, Slawosz
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1361-6641/aa5695
http://cds.cern.ch/record/2320261
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author García Alía, Rubén
Brugger, Markus
Danzeca, Salvatore
Cerutti, Francesco
de Carvalho Saraiva, Joao Pedro
Denz, Reiner
Ferrari, Alfredo
Foro, Lionel L
Peronnard, Paul
Røed, Ketil
Secondo, Raffaello
Steckert, Jens
Thurel, Yves
Toccafondo, Iacocpo
Uznanski, Slawosz
author_facet García Alía, Rubén
Brugger, Markus
Danzeca, Salvatore
Cerutti, Francesco
de Carvalho Saraiva, Joao Pedro
Denz, Reiner
Ferrari, Alfredo
Foro, Lionel L
Peronnard, Paul
Røed, Ketil
Secondo, Raffaello
Steckert, Jens
Thurel, Yves
Toccafondo, Iacocpo
Uznanski, Slawosz
author_sort García Alía, Rubén
collection CERN
description The radiation environment encountered at high-energy hadron accelerators strongly differs from the environment relevant for space applications. The mixed-field expected at modern accelerators is composed of charged and neutral hadrons (protons, pions, kaons and neutrons), photons, electrons, positrons and muons, ranging from very low (thermal) energies up to the TeV range. This complex field, which is extensively simulated by Monte Carlo codes (e.g. FLUKA) is due to beam losses in the experimental areas, distributed along the machine (e.g. collimation points) and deriving from the interaction with the residual gas inside the beam pipe. The resulting intensity, energy distribution and proportion of the different particles largely depends on the distance and angle with respect to the interaction point as well as the amount of installed shielding material. Electronics operating in the vicinity of the accelerator will therefore be subject to both cumulative damage from radiation (total ionizing dose, displacement damage) as well as single event effects which can seriously compromise the operation of the machine. This, combined with the extensive use of commercial-off-the-shelf components due to budget, performance and availability reasons, results in the need to carefully characterize the response of the devices and systems to representative radiation conditions.
id oai-inspirehep.net-1674670
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2017
record_format invenio
spelling oai-inspirehep.net-16746702019-09-30T06:29:59Zdoi:10.1088/1361-6641/aa5695http://cds.cern.ch/record/2320261engGarcía Alía, RubénBrugger, MarkusDanzeca, SalvatoreCerutti, Francescode Carvalho Saraiva, Joao PedroDenz, ReinerFerrari, AlfredoForo, Lionel LPeronnard, PaulRøed, KetilSecondo, RaffaelloSteckert, JensThurel, YvesToccafondo, IacocpoUznanski, SlawoszSingle event effects in high-energy acceleratorsAccelerators and Storage RingsThe radiation environment encountered at high-energy hadron accelerators strongly differs from the environment relevant for space applications. The mixed-field expected at modern accelerators is composed of charged and neutral hadrons (protons, pions, kaons and neutrons), photons, electrons, positrons and muons, ranging from very low (thermal) energies up to the TeV range. This complex field, which is extensively simulated by Monte Carlo codes (e.g. FLUKA) is due to beam losses in the experimental areas, distributed along the machine (e.g. collimation points) and deriving from the interaction with the residual gas inside the beam pipe. The resulting intensity, energy distribution and proportion of the different particles largely depends on the distance and angle with respect to the interaction point as well as the amount of installed shielding material. Electronics operating in the vicinity of the accelerator will therefore be subject to both cumulative damage from radiation (total ionizing dose, displacement damage) as well as single event effects which can seriously compromise the operation of the machine. This, combined with the extensive use of commercial-off-the-shelf components due to budget, performance and availability reasons, results in the need to carefully characterize the response of the devices and systems to representative radiation conditions.oai:inspirehep.net:16746702017
spellingShingle Accelerators and Storage Rings
García Alía, Rubén
Brugger, Markus
Danzeca, Salvatore
Cerutti, Francesco
de Carvalho Saraiva, Joao Pedro
Denz, Reiner
Ferrari, Alfredo
Foro, Lionel L
Peronnard, Paul
Røed, Ketil
Secondo, Raffaello
Steckert, Jens
Thurel, Yves
Toccafondo, Iacocpo
Uznanski, Slawosz
Single event effects in high-energy accelerators
title Single event effects in high-energy accelerators
title_full Single event effects in high-energy accelerators
title_fullStr Single event effects in high-energy accelerators
title_full_unstemmed Single event effects in high-energy accelerators
title_short Single event effects in high-energy accelerators
title_sort single event effects in high-energy accelerators
topic Accelerators and Storage Rings
url https://dx.doi.org/10.1088/1361-6641/aa5695
http://cds.cern.ch/record/2320261
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