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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...
Autores principales: | , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2017
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1361-6641/aa5695 http://cds.cern.ch/record/2320261 |
_version_ | 1780958561094860800 |
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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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