(g − 2) μ versus K → π + E miss induced by the (B − L)23 boson

Abstract To address the long-standing (g − 2) μ anomaly via a light boson, in ref. [1] we proposed to extend the standard model (SM) by the local (B − L)23, under which only the second and third generations of fermions are charged. It predicts an invisible Z′ with mass O 100 $$ \mathcal{O}(100) $$ M...

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Main Authors: Zhaofeng Kang, Yoshihiro Shigekami
Format: Article
Language:English
Published: SpringerOpen 2021-04-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP04(2021)238
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spelling doaj-e0e83af838a34021885ed063898cd9d82021-05-02T11:07:57ZengSpringerOpenJournal of High Energy Physics1029-84792021-04-012021412310.1007/JHEP04(2021)238(g − 2) μ versus K → π + E miss induced by the (B − L)23 bosonZhaofeng Kang0Yoshihiro Shigekami1School of Physics, Huazhong University of Science and TechnologySchool of Physics, Huazhong University of Science and TechnologyAbstract To address the long-standing (g − 2) μ anomaly via a light boson, in ref. [1] we proposed to extend the standard model (SM) by the local (B − L)23, under which only the second and third generations of fermions are charged. It predicts an invisible Z′ with mass O 100 $$ \mathcal{O}(100) $$ MeV, and moreover it has flavor-changing neutral current (FCNC) couplings to the up-type quarks at tree level. Such a Z′, via K L → π 0 + Z′(→ v v ¯ $$ v\overline{v} $$ ) 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 Z′ can readily do this job if it is no longer responsible for the (g − 2) μ anomaly. We further find that both anomalies can be explained with moderate tuning of the CP violation, but may contradict the B meson decays.https://doi.org/10.1007/JHEP04(2021)238Beyond Standard ModelCP violationGauge SymmetryKaon Physics
collection DOAJ
language English
format Article
sources DOAJ
author Zhaofeng Kang
Yoshihiro Shigekami
spellingShingle Zhaofeng Kang
Yoshihiro Shigekami
(g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
Journal of High Energy Physics
Beyond Standard Model
CP violation
Gauge Symmetry
Kaon Physics
author_facet Zhaofeng Kang
Yoshihiro Shigekami
author_sort Zhaofeng Kang
title (g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
title_short (g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
title_full (g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
title_fullStr (g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
title_full_unstemmed (g − 2) μ versus K → π + E miss induced by the (B − L)23 boson
title_sort (g − 2) μ versus k → π + e miss induced by the (b − l)23 boson
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-04-01
description Abstract To address the long-standing (g − 2) μ anomaly via a light boson, in ref. [1] we proposed to extend the standard model (SM) by the local (B − L)23, under which only the second and third generations of fermions are charged. It predicts an invisible Z′ with mass O 100 $$ \mathcal{O}(100) $$ MeV, and moreover it has flavor-changing neutral current (FCNC) couplings to the up-type quarks at tree level. Such a Z′, via K L → π 0 + Z′(→ v v ¯ $$ v\overline{v} $$ ) 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 Z′ can readily do this job if it is no longer responsible for the (g − 2) μ anomaly. We further find that both anomalies can be explained with moderate tuning of the CP violation, but may contradict the B meson decays.
topic Beyond Standard Model
CP violation
Gauge Symmetry
Kaon Physics
url https://doi.org/10.1007/JHEP04(2021)238
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