(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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Online Access: | https://doi.org/10.1007/JHEP04(2021)238 |
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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 |
work_keys_str_mv |
AT zhaofengkang g2mversuskpemissinducedbythebl23boson AT yoshihiroshigekami g2mversuskpemissinducedbythebl23boson |
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1721492679945093120 |