Abstract

Recently, the KOTO experiment reported their new preliminary result of searching for the decay $K_L\to\pi^0\nu\bar{\nu}$. Three candidate events were observed in the signal region, which exceed significantly the expectation based on the standard model. On the other hand, the new NA62 and previous BNL-E949 experiments yielded a consistent result and confirmed the standard model prediction in the charged meson decay $K^+\to\pi^+\nu\bar{\nu}$. Furthermore, the two decays are bound by a well-motivated relation from an analysis of isospin symmetry that is hard to break by the new physics of heavy particles. In this work, we study the issue by a systematic effective field theory approach with three of the simplest scenarios, in which the $K_L$ may decay into a new light neutral particle $X$, i.e., $K_L\to\pi^0X$, $K_L\to \gamma\gamma X$, or $K_L\to\pi^0XX$. We assess the feasibility of the scenarios by simulations and by incorporating constraints coming from NA62 and other relevant experiments. Our main conclusion is that the scenario $K\to\pi XX$ for a long lived scalar $X$ seems more credible than the other two when combining distributions and other experimental constraints while the region below the KOTO's blind box provides a good detection environment to search for all three scenarios for a relatively heavy $X$.

Highlights

  • The flavor changing neutral current decays of the neutral and charged kaons K → πννprovide a clean venue to examine precisely the standard model (SM) and to search for new physics beyond it

  • Three candidate events were observed in the signal region, which exceed significantly the expectation based on the standard model

  • The two decays are bound by a well-motivated relation from an analysis of isospin symmetry that is hard to break by the new physics of heavy particles

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Summary

Introduction

The flavor changing neutral current decays of the neutral and charged kaons K → πννprovide a clean venue to examine precisely the standard model (SM) and to search for new physics beyond it. When X is so heavy (roughly mX > 190 MeV) that none of the candidate events can be accommodated or even all of its signals drop below the blind box (mX > 270 MeV), we use the above background estimates to set a 90% C.L. upper bound on the decay branching ratio.

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