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The Koto II experiment

Abstract

KL → π0νν̅ is a golden mode for flavour physics: it is highly suppressed in the Standard Model, with a predicted branching ratio of 3 × 10−11 and a theoretical uncertainty of just 2\%, and is therefore extremely sensitive to new physics. The KOTO experiment at J-PARC is searching for this decay. Using the data taken in 2021, it has set the most stringent upper limit to date of 2.2 × 10−9 on the branching ratio at 90\% C.L. We present KOTO II, a next-generation experiment at J-PARC proposed in 2024, which aims to measure the KL → π0νν̅ branching ratio with a sensitivity below 10−12 in the 2030s.

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BibTeX
@misc{martellotti2026koto,
  title = {{The Koto II experiment}},
  author = {Silvia Martellotti},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.08514},
  eprint = {2611.08514},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.08514},
}
RIS
TY  - UNPB
TI  - The Koto II experiment
AU  - Silvia Martellotti
PY  - 2026
DA  - 2026/11/01
PB  - arXiv
DO  - 10.48550/arxiv.2611.08514
UR  - https://arxiv.org/abs/2611.08514
AB  - K_L → π^0νν̅ is a golden mode for flavour physics: it is highly suppressed in the Standard Model, with a predicted branching ratio of 3 × 10^−11 and a theoretical uncertainty of just 2\%, and is therefore extremely sensitive to new physics. The KOTO experiment at J-PARC is searching for this decay. Using the data taken in 2021, it has set the most stringent upper limit to date of 2.2 × 10^−9 on the branching ratio at 90\% C.L. We present KOTO II, a next-generation experiment at J-PARC proposed in 2024, which aims to measure the K_L → π^0νν̅ branching ratio with a sensitivity below 10^−12 in the 2030s.
ER  -