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The K12 beamline for the KLEVER experiment
The KLEVER experiment is proposed to run in the CERN ECN3 underground cavern from 2026 onward. The goal of the experiment is to measure ${\rm{BR}}(K_L \rightarrow \pi^0v\bar{v})$, which could yield information about potential new physics, by itself and in combination with the measurement of ${\rm{BR...
Autores principales: | , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.18429/JACoW-IPAC2019-THPGW061 https://dx.doi.org/10.1088/1742-6596/1350/1/012092 http://cds.cern.ch/record/2692792 |
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author | Van Dijk, Maarten Banerjee, Dipanwita Bernhard, Johannes Brugger, Markus Charitonidis, Nikolaos D'Alessandro, Gian Luigi Doble, Niels Gatignon, Laurent Gerbershagen, Alexander Montbarbon, Eva Moulson, Matthew Rae, Bastien Rosenthal, Marcel Veit, Benjamin |
author_facet | Van Dijk, Maarten Banerjee, Dipanwita Bernhard, Johannes Brugger, Markus Charitonidis, Nikolaos D'Alessandro, Gian Luigi Doble, Niels Gatignon, Laurent Gerbershagen, Alexander Montbarbon, Eva Moulson, Matthew Rae, Bastien Rosenthal, Marcel Veit, Benjamin |
author_sort | Van Dijk, Maarten |
collection | CERN |
description | The KLEVER experiment is proposed to run in the CERN ECN3 underground cavern from 2026 onward. The goal of the experiment is to measure ${\rm{BR}}(K_L \rightarrow \pi^0v\bar{v})$, which could yield information about potential new physics, by itself and in combination with the measurement of ${\rm{BR}}(K^+ \rightarrow \pi^+v\bar{v})$ of NA62. A full description will be given of the considerations in designing the new K12 beamline for KLEVER, as obtained from a purpose made simulation with FLUKA. The high intensities required by KLEVER, $2 \times 10^{13}$ protons on target every 16.8 s, with $5 \times 10^{19}$ protons accumulated over 5 years, place stringent demands on adequate muon sweeping to minimize backgrounds in the detector. The target and primary dump need to be able to survive these demanding conditions, while respecting strict radiation protection criteria. A series of design choices will be shown to lead to a neutral beamline sufficiently capable of suppressing relevant backgrounds, such as photons generated by $\pi^0$ decays in the target, and $\Lambda \rightarrow n\pi^0$ decays, which mimic the signal decay. |
id | oai-inspirehep.net-1745722 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | oai-inspirehep.net-17457222022-04-08T07:53:29Zdoi:10.18429/JACoW-IPAC2019-THPGW061doi:10.1088/1742-6596/1350/1/012092http://cds.cern.ch/record/2692792engVan Dijk, MaartenBanerjee, DipanwitaBernhard, JohannesBrugger, MarkusCharitonidis, NikolaosD'Alessandro, Gian LuigiDoble, NielsGatignon, LaurentGerbershagen, AlexanderMontbarbon, EvaMoulson, MatthewRae, BastienRosenthal, MarcelVeit, BenjaminThe K12 beamline for the KLEVER experimentAccelerators and Storage RingsThe KLEVER experiment is proposed to run in the CERN ECN3 underground cavern from 2026 onward. The goal of the experiment is to measure ${\rm{BR}}(K_L \rightarrow \pi^0v\bar{v})$, which could yield information about potential new physics, by itself and in combination with the measurement of ${\rm{BR}}(K^+ \rightarrow \pi^+v\bar{v})$ of NA62. A full description will be given of the considerations in designing the new K12 beamline for KLEVER, as obtained from a purpose made simulation with FLUKA. The high intensities required by KLEVER, $2 \times 10^{13}$ protons on target every 16.8 s, with $5 \times 10^{19}$ protons accumulated over 5 years, place stringent demands on adequate muon sweeping to minimize backgrounds in the detector. The target and primary dump need to be able to survive these demanding conditions, while respecting strict radiation protection criteria. A series of design choices will be shown to lead to a neutral beamline sufficiently capable of suppressing relevant backgrounds, such as photons generated by $\pi^0$ decays in the target, and $\Lambda \rightarrow n\pi^0$ decays, which mimic the signal decay.CERN-ACC-2019-243oai:inspirehep.net:17457222019 |
spellingShingle | Accelerators and Storage Rings Van Dijk, Maarten Banerjee, Dipanwita Bernhard, Johannes Brugger, Markus Charitonidis, Nikolaos D'Alessandro, Gian Luigi Doble, Niels Gatignon, Laurent Gerbershagen, Alexander Montbarbon, Eva Moulson, Matthew Rae, Bastien Rosenthal, Marcel Veit, Benjamin The K12 beamline for the KLEVER experiment |
title | The K12 beamline for the KLEVER experiment |
title_full | The K12 beamline for the KLEVER experiment |
title_fullStr | The K12 beamline for the KLEVER experiment |
title_full_unstemmed | The K12 beamline for the KLEVER experiment |
title_short | The K12 beamline for the KLEVER experiment |
title_sort | k12 beamline for the klever experiment |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.18429/JACoW-IPAC2019-THPGW061 https://dx.doi.org/10.1088/1742-6596/1350/1/012092 http://cds.cern.ch/record/2692792 |
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