1. Belle II の物理 (high-ish scale) SUSY
Yukihiro Mimura (National Taiwan University)
Talk at Flavor Physics Workshop 2017 (10.31)

2. Today’s Menu Introduction LHC results Implications to Flavor Physics
Belle II physics Heavier Higgs, New FCNC source, GUT
Exotics Baryon/lepton number violation?
Conclusion

3. LHC results

6. Gluino mass bound Unified gaugino mass at GUT scale
If gaugino masses are unified,

7. Good News & Bad News for “highish scale” SUSY
Everything is consistent.
(125 GeV Higgs mass, FCNC suppression, Cosmology)
Bad News:
May not be observed at LHC (run-II) Little hierarchy Problem (Cancellation in the minimization condition)

8. Good News & Bad News from 125 GeV Higgs mass
Stop mass and/or mixing (A-term) are large They are sensitive to radiative EWSB.
Good News:
Consistent with no sign in direct SUSY search Implication to flavor physics

9. RGE-induced off-diagonal elements in sfermion mass matrices

10. 125GeV Higgs mass in MSSM Sfermions are heavy (10 TeV ?).
Sfermions are 2-3 TeV, but A0 is large (A0 ~ 5 TeV)
It can still affect to “accurate” flavor physics via the RGE-induced FCNCs.
(So long ! ) or

11. Belle II Physics

12. , 2.
, CP violation
, Lepton flavor violation 6. .

13. Quark-lepton unification?, 2.
, CPV
, LFV .
New FCNC/CP source
Left- or right-handed?
Quark-lepton unification?
Lepto-quark?

14. CMSSM NUHM1 NUHM2 Very roughly, for For large , is possible.
(at M_GUT)
NUHM2

15. LUX, XENON1T, PandaX Heavy?? b u Neutralino LSP-Nucleon scattering s s
Non-holomorphic corrections (see later)
Neutralino LSP-Nucleon scattering
Dutta-YM-Santoso, PRD80(2009)095005 s
LUX, XENON1T,
PandaX
Heavy?? s

16. PandaX-II 2017, Aug.

17. Brief review of Higgs Penguin FCNC in SUSY
It comes from finite correction due to SUSY br. b s
(Choudhury-Gaur, Babu-Kolda, …)

18. Double Higgs-Penguin for B meson mixings
(Hamzaoui-Pospelov-Toharia, Buras et.al., Bobeth et.al., …) s b
h,H,A s b
Right-handed squark FCNC source is important.

20. Under SO(10) GUT boundary condition
Dutta-YM, PRD78(2008)071702
Before the measurement of Bs phase

21. CKMfitter
Unitarity Triangle

22. Box contribution is dominant if there is only left-handed FCNC source.

23. SM All the other data are satisfied at the green points.
Dutta-YM, PRD91(2015)095011
All the other data are satisfied at the green points.

24. CMS/LHCb combined results (Nature 522 (2015) 68)
SM predictions :

25. Popular FCNC source (folklore)

26. from neutrino FCNC source
Dutta-YM, PRD75(2007)

27. ?
b-d FCNC > b-s FCNC
It is possible if they are induced by anti-symmetric coupling.
Dutta-YM, PRD91(2015)095011

28. In SU(5) GUT Anti-symmetric FCNC source Br depends on slepton masses.
arXiv:

29. Note on in SM due to CKM unitarity Clean test Belle II Goal :
Belle, PRL 114(2015)151601
Belle II Goal :
Model independent analysis
by Hurth-Lunghi-Porod

30. Quark-lepton unification?1. 2.
, CPV
, LFV
New FCNC/CP source
Left- or right-handed?
Quark-lepton unification?

31. Exotics
Baryon/lepton number violation

32. Lepton number violating B meson decays

33. Baryon number violating processes (Kuzmin, Glashow)
(Forbidden?)
Wait for HyperKamiokande
Proton decay
Neutron-anti-neutron oscillations Baryon-antibaryon oscillations
Double-proton decay
Hydrogen-antihydrogen oscillations

34. How about Heavy flavor baryons?
TeV scale diquark mediation (with a flavor suppression) gives an achievable order of magnitude. (Chacko-Mohapatra)
SM singlet
(Ajaib-Gogoladze-YM-Shafi)
(Dutta-YM-Mohapatra)
How about Heavy flavor baryons?

35. LHCb, arXiv:

36. Summary
LHC results : All heavy? But, it can still affect to “accurate” flavor measurements.
Precise measurements are the key to new FCNC sources, and heavier Higgs masses.
The b-d transition can be larger than the b-s transition. Then, is larger than in unified models.
Accurate (CPV) measurement is helpful to check the scenarios of new FCNC sources.
Exotics : Lepton/baryon number violating processes

37. Thank you very much!

38. Five candidates of the anti-symmetric bi-fermion couplings
Neutron and electron EDMs can be as large as the current bounds. 38 38

39. K meson mixing data are satisfied at the green points.
Phys. Rev. D91 (2015) SM
K meson mixing data are satisfied at the green points.

40. Feature 1 :
For a naive hierarchy , we obtain

41. If is small, one of is small.
Feature 2 :
If is small, one of is small.

42. Implication the couplings
induce FCNC in the right-handed sleptons (in addition to the left-handed ones from Dirac neutrino couplings)
The electron electric dipole moment is generated even if Higgsino mass and scalar trilinear coupling are real.
Experimental bound:

43. Flavor Changing Neutral Current (FCNC) in SUSY GUTs
Too much FCNCs in general SUSY breaking masses.
Flavor universality of SUSY breaking is assumed.
Even if so, off-diagonal elements are induced by RGEs via heavy particle loops (right-handed neutrino, colored Higgs).
(Borzumati-Majiero, Moroi, Chang-Majiero-Murayama, …)
Investigating FCNCs in quarks and leptons is important
to find a footprint of GUT scale physics.

44. Neutron-antineutron oscillations
(Current bound)
Cold neutron beam from reactor (Grenoble, France (1994))
(J. Phys. G36, , Mohapatra)

45. Global fits by GAMBIT collaboration (Global And Modular Beyond-the-Standard-mode Inference Tool)
CMSSM

46. NUHM1
NUHM2

48. MSSM7:

49. Best fits by
GAMBIT collaboration,