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 BR(KL→π0vv¯), which could yield information about potential new physics, by itself and in combination with the measurement of BR(K+→π+vv¯) of NA62. A full descripti...

Full description

Saved in:
Bibliographic Details
Published inJournal of physics. Conference series Vol. 1350; no. 1; pp. 12092 - 12097
Main Authors van Dijk, M W U, Banerjee, D, Bernhard, J, Brugger, M, Charitonidis, N, D'Alessandro, G L, Doble, N, Gatignon, L, Gerbershagen, A, Montbarbon, E, Moulson, M, Rae, B, Rosenthal, M, Veit, B M
Format Journal Article
LanguageEnglish
Published Bristol IOP Publishing 01.11.2019
Subjects
Online AccessGet full text
ISSN1742-6588
1742-6596
DOI10.1088/1742-6596/1350/1/012092

Cover

More Information
Summary:The KLEVER experiment is proposed to run in the CERN ECN3 underground cavern from 2026 onward. The goal of the experiment is to measure BR(KL→π0vv¯), which could yield information about potential new physics, by itself and in combination with the measurement of BR(K+→π+vv¯) 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 × 1013 protons on target every 16.8 s, with 5 × 1019 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 π0 decays in the target, and Λ → nπ0 decays, which mimic the signal decay.
Bibliography:ObjectType-Article-1
SourceType-Scholarly Journals-1
ObjectType-Feature-2
content type line 14
ISSN:1742-6588
1742-6596
DOI:10.1088/1742-6596/1350/1/012092