English

$(g-2)_{\mu}$ Versus $K \to \pi+E_{miss}$ Induced by the $(B-L)_{23}$ Boson

High Energy Physics - Phenomenology 2021-04-30 v3 High Energy Physics - Experiment

Abstract

To address the long-standing (g2)μ(g-2)_{\mu} anomaly via a light boson, in Ref. [1] we proposed to extend the standard model (SM) by the local (BL)23(B-L)_{23}, under which only the second and third generations of fermions are charged. It predicts an invisible ZZ' with mass O(100){\cal O}(100) MeV, and moreover it has flavor-changing neutral current (FCNC) couplings to the up-type quarks at tree level. Such a ZZ', via KLπ0+Z(ννˉ)K_L \to \pi^0 + Z'(\to \nu \bar{\nu}) at loop level, may be a natural candidate to account for the recent KOTO anomaly. In this article, we investigate this possibility, to find that ZZ' can readily do this job if it is no longer responsible for the (g2)μ(g-2)_{\mu} anomaly. We further find that both anomalies can be explained with moderate tuning of the CP violation, but may contradict the BB meson decays.

Keywords

Cite

@article{arxiv.2008.09793,
  title  = {$(g-2)_{\mu}$ Versus $K \to \pi+E_{miss}$ Induced by the $(B-L)_{23}$ Boson},
  author = {Zhaofeng Kang and Yoshihiro Shigekami},
  journal= {arXiv preprint arXiv:2008.09793},
  year   = {2021}
}

Comments

21 pages, 6 figures, v3: text and Figs. 2, 4 are improved