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特定領域「フレーバー物理の新展開」研究会2009 @ 蒲郡. B physics and supersymmetry with general flavor mixing. Ken-ichi Okumura (Tohoku University) In collaboration with John Foster and Leszek Roszkowski. Based on. hep-ph/0604121, hep-ph/0510422, hep-ph/0506146, hep-ph/0410323. Plan of talk. Introduction
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特定領域「フレーバー物理の新展開」研究会2009 @ 蒲郡 B physics and supersymmetry with general flavor mixing Ken-ichi Okumura (Tohoku University) In collaboration with John Foster and Leszek Roszkowski Based on hep-ph/0604121, hep-ph/0510422, hep-ph/0506146, hep-ph/0410323
Plan of talk • Introduction • Supersymmetry with general flavor mixing • b-s transitions • Conclusion
Why Supersymmetry ? SM S.P.Martin (1997) MSSM
Supersymmetry doubles flavor Soft mass Tri-linear term Gaugino mass
Minimal flavor violation (MFV) Super CKM basis
Origin of flavor mixing Ex) Seesaw mechanism Large flavor mixing (MSN matrix) “Probe of GUT scale int.” SUSY GUT Radiative correction S.Baek, T.Goto Y.Okada KO (2000)
Collider vs flavor physics LHC SUSY Lagragian Mass spectrum Flavor Physics ! mixing Complementary each other
M.Misiak&M.Steinhauser (2006) NP effects interfere with the SM GFM Add MFV
Not diagonal ! SUSY KO and L.Roszkowski (2001)
Higgs mediated FCNC Non-holomorphic Integrate out SUSY particles NG :Flavor diagonal
P.Ball and R.Fleischer (2006) Lattice CKM angle & side
CP violation in CKMfitter UTfit
Conclusion • We reported current limits on flavor mixing in b-s transitions in minimal supersymmetry (beyond leading order+Higgs mediated). • Constraint from Bs mixing is quite severe for RR and RL mixing at moderate-large tanβ(~30)despite relatively large theoretical uncertainty. • Precision measurement of Φ3 + Bs mixing can improve the bound (or find NP) as well as BR(Bs→μμ). • Low tanβregion can be covered by tCPV in radiative decay. • Combined with the spectrum measurement, such a measurement provides a clue to high energy scale.