Abstract

We point out kaon decays to multiple charged leptons as a novel probe of light dark particles $X$. Previously neglected channels, such as ${K}^{+}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}(XX\ensuremath{\rightarrow}2({e}^{+}{e}^{\ensuremath{-}}))$, ${K}_{L}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}(XX\ensuremath{\rightarrow}2({e}^{+}{e}^{\ensuremath{-}}))$, and ${K}_{S}\ensuremath{\rightarrow}(XX\ensuremath{\rightarrow}2({e}^{+}{e}^{\ensuremath{-}}))$ may have very large rates, exceeding not only the Standard Model expectations but also possible backgrounds, such as Dalitz decays of neutral pions. We apply this idea to dark sector models where the production of dark Higgses or heavy neutral leptons leads to final states with several visible dark photons. We also investigate a recently proposed model of an MeV-scale QCD axion, where the rates for kaon decays to multiple axion states are large due to the nonlinear interactions of the axion with the light mesons. In addition, we point out new probes of this axion in pion decays, such as the single production of $a$ in ${\ensuremath{\pi}}^{+}\ensuremath{\rightarrow}\ensuremath{\nu}(({e}^{+}{)}^{*}\ensuremath{\rightarrow}{e}^{+}a\ensuremath{\rightarrow}{e}^{+}{e}^{+}{e}^{\ensuremath{-}})$, double production in pion capture ${\ensuremath{\pi}}^{\ensuremath{-}}+(p\text{ }\text{or}\text{ }\mathrm{D})\ensuremath{\rightarrow}aa+(n\text{ }\mathrm{or}\text{ }nn)\ensuremath{\rightarrow}\phantom{\rule{0ex}{0ex}}2({e}^{+}{e}^{\ensuremath{-}})+(n\text{ }\mathrm{or}\text{ }nn)$, as well as ${\ensuremath{\pi}}^{0}\ensuremath{\rightarrow}aaa\ensuremath{\rightarrow}3({e}^{+}{e}^{\ensuremath{-}})$. The latter decay is fixed at $\mathcal{B}({\ensuremath{\pi}}^{0}\ensuremath{\rightarrow}aaa)=1.0\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}3}$ for a 17 MeV axion.

Highlights

  • Low-energy extensions of the Standard Model (SM) typically operate with new states that are neutral under the SM group and have small couplings to SM particles

  • Neglected channels, such as Kþ → πþðXX → 2ðeþe−ÞÞ, KL → π0ðXX → 2ðeþe−ÞÞ, and KS → ðXX → 2ðeþe−ÞÞ may have very large rates, exceeding the Standard Model expectations and possible backgrounds, such as Dalitz decays of neutral pions. We apply this idea to dark sector models where the production of dark Higgses or heavy neutral leptons leads to final states with several visible dark photons

  • Rare kaon decays have been instrumental in learning about the properties and nature of weak interactions, P and CP violation, and one of the main drivers in establishing the Standard Model

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Summary

INTRODUCTION

Low-energy extensions of the Standard Model (SM) typically operate with new states that are neutral under the SM group and have small couplings to SM particles. The single production of particles X is most efficient when X is not coupled to a conserved current, and, the electroweak (EW) loop generating flavor-changing neutral currents (FCNC) can be enhanced by the masses of heavy particles, t, W, inside the loop This way, strong constraints on DS particles X can be obtained by studying K → πX and B → KðÃÞX transitions, when X is a Higgs-mixed scalar [4,5,6,7,8,9] or an axion or axionlike particle [10,11,12], or dark vector with the mass mixing with Z-boson [13,14].

NOVEL MULTILEPTON KAON DECAYS
Backgrounds
DARK CASCADES IN A Uð1Þd DARK SECTOR
Minimal model
Singlet-scalar extension
Missing energy from a dark neutrino sector
MULTIPLE PRODUCTION OF MEV-SCALE AXIONS
Double axion production in kaon decays
Triple axion production
Radiative pion decays
CONCLUSIONS
Findings
Uð1Þd plus scalar singlet
Full Text
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