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 |
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Hauptverfasser: | , , , |
Format: | Artikel |
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. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP10(2020)197 |