1. B physics and supersymmetry with general flavor mixing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/ , hep-ph/ , hep-ph/ , hep-ph/

2. Plan of talk Introduction Supersymmetry with general flavor mixing
b-s transitions
Conclusion

3. The SM: CKM paradigm

4. Why Supersymmetry ? SM
S.P.Martin (1997)
MSSM

5. Supersymmetry doubles flavor
Soft mass
Tri-linear term
Gaugino mass

6. Minimal flavor violation (MFV)
Super CKM basis

7. General Flavor Mixing

8. 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)

9. Collider vs flavor physics
LHC
SUSY Lagragian
Mass spectrum
Flavor Physics !
mixing
Complementary each other

10. b →s transitions

11. NP effects interfere with the SM
M.Misiak&M.Steinhauser (2006)
NP effects interfere with the SM
GFM
Add
MFV

12. MFV

14. Not diagonal !
SUSY
KO and L.Roszkowski (2001)

15. Higgs mediated FCNC Integrate out SUSY particles Non-holomorphic NG
:Flavor diagonal

17. J.Foster, KO, L.Roszkowski (2005)

19. P.Ball and R.Fleischer (2006)
Lattice
CKM angle & side

21. MFV

24. All combined : single insertion

26. CP violation in
CKMfitter
UTfit

28. 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 tanβ　region can be covered by tCPV in radiative decay.
Combined with the spectrum measurement, such a measurement provides a clue to high energy scale.