In-beam charged particle detector using 0.2-mm thick plastic scintillator for the J-PARC KOTO experiment

The KOTO experiment at J-PARC is dedicated to searching for the rare decay $K_L\rightarrow \pi^0\nu \bar{\nu}$. This decay violates CP symmetry and is sensitive to new physics beyond the Standard Model (SM) because its branching ratio is predicted to be 3 × 10−11 with a small theoretical uncertainty in SM. One of main backgrounds is caused by a small contamination of charged kaons in the neutral beam. We installed a new charged particle detector in the beam to reject the background events by detecting charged kaons directly. This detector consists of a 0.2-mm-thick plastic scintillator film and 12-𝜇m-thick aluminized mylar. The scintillation photons escaping from the scintillator surface are reflected by the mylar and are detected with multiple photomultiplier tubes on the sides. In the data taken in 2024, we conclude light yield is 18.5 photoelectrons and inefficiency is $5×10^{−4}$ at the 0.4 MIP threshold. As a result, we can eliminate charged kaon background.

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Publication Details

Published
2024-12-17
DOI
https://doi.org/10.22323/1.476.0969
Primary Topic
Radiation Detection and Scintillator Technologies
Type
article
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article

In-beam charged particle detector using 0.2-mm thick plastic scintillator for the J-PARC KOTO experiment

Keita Ono
Radiation Detection and Scintillator Technologies
article

In-beam charged particle detector using 0.2-mm thick plastic scintillator for the J-PARC KOTO experiment

Keita Ono
article en

Abstract

The KOTO experiment at J-PARC is dedicated to searching for the rare decay $K_L\rightarrow \pi^0\nu \bar{\nu}$. This decay violates CP symmetry and is sensitive to new physics beyond the Standard Model (SM) because its branching ratio is predicted to be 3 × 10−11 with a small theoretical uncertainty in SM. One of main backgrounds is caused by a small contamination of charged kaons in the neutral beam. We installed a new charged particle detector in the beam to reject the background events by detecting charged kaons directly. This detector consists of a 0.2-mm-thick plastic scintillator film and 12-𝜇m-thick aluminized mylar. The scintillation photons escaping from the scintillator surface are reflected by the mylar and are detected with multiple photomultiplier tubes on the sides. In the data taken in 2024, we conclude light yield is 18.5 photoelectrons and inefficiency is $5×10^{−4}$ at the 0.4 MIP threshold. As a result, we can eliminate charged kaon background.

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