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The kaon identification system in the NA62 experiment at the CERN SPS

The fixed target experiment NA62 at CERN aims at measuring the ultra-rare decay K+→π+νν¯ , whose branching ratio is of the order of 10 −11 . The main challenges faced by the experiment to achieve a 10% precision measurement are the required beam intensity and background rejection factor. The differe...

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Autor principal: Lurkin, Nicolas
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2016.05.128
http://cds.cern.ch/record/2291116
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author Lurkin, Nicolas
author_facet Lurkin, Nicolas
author_sort Lurkin, Nicolas
collection CERN
description The fixed target experiment NA62 at CERN aims at measuring the ultra-rare decay K+→π+νν¯ , whose branching ratio is of the order of 10 −11 . The main challenges faced by the experiment to achieve a 10% precision measurement are the required beam intensity and background rejection factor. The differential Cherenkov detector KTAG must be able to tag charged kaons in an unseparated hadron beam with an average particle rate of 750 MHz, of which 45 MHz are kaons, with a time precision of at least 100 ps and an efficiency higher than 95%. The additional pion contamination must be kept lower than 10 −4 .
id oai-inspirehep.net-1513591
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2017
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spelling oai-inspirehep.net-15135912019-09-30T06:29:59Zdoi:10.1016/j.nima.2016.05.128http://cds.cern.ch/record/2291116engLurkin, NicolasThe kaon identification system in the NA62 experiment at the CERN SPSDetectors and Experimental TechniquesParticle Physics - ExperimentThe fixed target experiment NA62 at CERN aims at measuring the ultra-rare decay K+→π+νν¯ , whose branching ratio is of the order of 10 −11 . The main challenges faced by the experiment to achieve a 10% precision measurement are the required beam intensity and background rejection factor. The differential Cherenkov detector KTAG must be able to tag charged kaons in an unseparated hadron beam with an average particle rate of 750 MHz, of which 45 MHz are kaons, with a time precision of at least 100 ps and an efficiency higher than 95%. The additional pion contamination must be kept lower than 10 −4 .oai:inspirehep.net:15135912017
spellingShingle Detectors and Experimental Techniques
Particle Physics - Experiment
Lurkin, Nicolas
The kaon identification system in the NA62 experiment at the CERN SPS
title The kaon identification system in the NA62 experiment at the CERN SPS
title_full The kaon identification system in the NA62 experiment at the CERN SPS
title_fullStr The kaon identification system in the NA62 experiment at the CERN SPS
title_full_unstemmed The kaon identification system in the NA62 experiment at the CERN SPS
title_short The kaon identification system in the NA62 experiment at the CERN SPS
title_sort kaon identification system in the na62 experiment at the cern sps
topic Detectors and Experimental Techniques
Particle Physics - Experiment
url https://dx.doi.org/10.1016/j.nima.2016.05.128
http://cds.cern.ch/record/2291116
work_keys_str_mv AT lurkinnicolas thekaonidentificationsysteminthena62experimentatthecernsps
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