The Muon Magnetic Moment and Supersymmetry
By D. Stockinger. 2006
147 citations recorded by the source corpus.
The present review is devoted to the muon magnetic moment and its role in supersymmetry phenomenology. Analytical results for the leading supersymmetric oneand two-loop contributions are provided, numerical examples are given and the dominant tanβ sign(μ)/M SUSY behaviour is qualitatively explained. The consequences of the Brookhaven measurement are discussed. The 2σ deviation from the Standard Model prediction implies preferred ranges for supersymmetry parameters, in particular upper and lower mass bounds. Correlations with other observables from collider physics and cosmology are reviewed. We give, wherever possible, an intuitive understanding of each result before providing a detailed discussion. PACS numbers: 12.60.Jv,13.40.Em,14.60.Ef The Muon Magnetic Moment and Supersymmetry 1
Subfields: Artificial Intelligence, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/960241029af2a31c5a5464ef2ff10baa7e004df3
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Citations in the corpus
- A Call for New Physics : The Muon Anomalous Magnetic Moment and Lepton Flavor Violation (2016, background): “gative or positive contribution to g 2, along with the value for tan. Anyway, it is easy to see that there is plenty of room to accommodate the g 2 for several values of tan;A , and m ~. See Refs. [250, 279] for details. 10.1.2. Connecting g 2 and !e The correlation between g 2 and !e has been inves”
- The Next-to-Minimal Supersymmetric extension of the Standard Model reviewed (2009, background): “For a recent review we refer the reader to Stöckinger [120].”
- The electroweak contributions to $(g-2)_\mu$ after the Higgs boson mass measurement (2013, background): “s neglected in Ref. [21] are important. Inserting the measured value of the Higgs boson mass, and taking into account all contributions including top, bottom, charm and τ loops and diagrams 2 In Ref. [26], Eq.(70), a similar function f S ( x) is defined, where S ) = xfH )−4 . Additionally, Eqs. (14),”
- SuperIso v2.3: A program for calculating flavor physics observables in supersymmetry (2008, unknown): “op 1 − 4α π ln MSUSY mµ , (229) where MSUSY is a typical superpartner mass scale. The dominant two loop contributions from the photonic Barr-Zee diagrams with physical Higgs bosons are as follows [58] a(χγH) µ = α2m2 µ 8π 2M2 W sin θW X k=1,2 ( ai Re[λai µ λ ai χ + k ] fPS(m2 χ /M2 ai) + X hi Re[λ”