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Status of the AFP project in the ATLAS experiment
Status of the AFP project in the ATLAS experiment is summarized. The AFP system is composed of a tracker to detect intact, diffractively scattered protons, and of a time-of-flight detector serving to suppress background from pile-up interactions. The whole system, located around 210~m from the main...
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Lenguaje: | eng |
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2014
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Acceso en línea: | https://dx.doi.org/10.1063/1.4916008 http://cds.cern.ch/record/1974510 |
_version_ | 1780945034261037056 |
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author | Tasevsky, Marek |
author_facet | Tasevsky, Marek |
author_sort | Tasevsky, Marek |
collection | CERN |
description | Status of the AFP project in the ATLAS experiment is summarized. The AFP system is composed of a tracker to detect intact, diffractively scattered protons, and of a time-of-flight detector serving to suppress background from pile-up interactions. The whole system, located around 210~m from the main ATLAS detector, is placed in Roman Pots which move detectors from and to the incident proton beams. A typical distance of the closest approach of the tracker to these beams is 2--3~mm. The main physics motivation lies in measuring diffractive processes in runs with not a very high amount of pile-up. |
id | cern-1974510 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-19745102019-09-30T06:29:59Zdoi:10.1063/1.4916008http://cds.cern.ch/record/1974510engTasevsky, MarekStatus of the AFP project in the ATLAS experimentParticle Physics - ExperimentStatus of the AFP project in the ATLAS experiment is summarized. The AFP system is composed of a tracker to detect intact, diffractively scattered protons, and of a time-of-flight detector serving to suppress background from pile-up interactions. The whole system, located around 210~m from the main ATLAS detector, is placed in Roman Pots which move detectors from and to the incident proton beams. A typical distance of the closest approach of the tracker to these beams is 2--3~mm. The main physics motivation lies in measuring diffractive processes in runs with not a very high amount of pile-up.ATL-FWD-PROC-2014-002oai:cds.cern.ch:19745102014-12-08 |
spellingShingle | Particle Physics - Experiment Tasevsky, Marek Status of the AFP project in the ATLAS experiment |
title | Status of the AFP project in the ATLAS experiment |
title_full | Status of the AFP project in the ATLAS experiment |
title_fullStr | Status of the AFP project in the ATLAS experiment |
title_full_unstemmed | Status of the AFP project in the ATLAS experiment |
title_short | Status of the AFP project in the ATLAS experiment |
title_sort | status of the afp project in the atlas experiment |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.1063/1.4916008 http://cds.cern.ch/record/1974510 |
work_keys_str_mv | AT tasevskymarek statusoftheafpprojectintheatlasexperiment |