The light sgoldstino phenomenology: explanations for the muon (g − 2) deviation and KOTO anomaly

A bstract In this work, we study the long-standing experimental anomaly in muon ( g − 2) and also recent anomalous excess in K L → π 0 + v v ¯ at the J-PARC KOTO experiment with sgoldstino. After supersymmetry breaking, the interactions between quarks and sgoldstino ( s ) make the decays K → π + s s...

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Veröffentlicht in:The journal of high energy physics 2020-10, Vol.2020 (10), p.1-18, Article 197
Hauptverfasser: Liu, Xuewen, Li, Ying, Li, Tianjun, Zhu, Bin
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Sprache:eng
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Zusammenfassung:A bstract In this work, we study the long-standing experimental anomaly in muon ( g − 2) and also recent anomalous excess in K L → π 0 + v v ¯ at the J-PARC KOTO experiment with sgoldstino. After supersymmetry breaking, the interactions between quarks and sgoldstino ( s ) make the decays K → π + s sizable through loop diagrams, which affects the measurements of decays K → π + invisible. Furthermore, the couplings between photons and sgoldstino contribute to ∆ a μ as well as the bino-slepton contribution. With satisfying all known experimental constraints such as from NA62, E949, E137, Orsay, KTEV and CHARM experiments, these two anomalies can be explained simultaneously. The mass of CP-even sgoldstino is close to the neutral pion mass which does not violate the Grossman-Nir bound. The parameter space can be further tested in future NA62, DUNE experiments, as well as experiments in the LHC.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP10(2020)197