b. dutta
DESCRIPTION
Grand Unified Models, Proton Decay and Phase of. B. Dutta. Texas A&M University. Phys.Rev.Lett.100:181801,2008; arXiv:0805.2988 ; To appear. Collaborator: Yukihiro Mimura. ICHEP 08. Introduction. Flavor Violation in Grand Unified Models. Large FCNCs exist for general SUSY breaking masses. - PowerPoint PPT PresentationTRANSCRIPT
B. Dutta
Texas A&M University
Phys.Rev.Lett.100:181801,2008; arXiv:0805.2988; To appear
Grand Unified Models, Proton Decay and Phase of
Collaborator: Yukihiro Mimura
ICHEP 08
Large FCNCs exist for general SUSY breaking masses.
Flavor universality of SUSY breaking is assumed to solve the flavor problem.
FCNCs can still be induced by RGEs.
In MSSM, the quark FCNCs are small due to small CKM mixings.
If there is a heavy particle, e.g., heavy right handed neutrino, the loop corrections can induce sizable FCNCs due to large neutrino mixing. (Borzumati-Masiero)
Flavor Violation in Grand Unified Models
The flavor violation effects teach us GUT scale physics
Introduction
and are correlated.
In this talk :
In GUT models,
(Belle)
The phase of . Is also restricted
We will study large CP phase in SU(5) and SO(10) GUT models.
The nature of FCNC and CP violation is very important to test the existence of new physics
FCNC and New Physics
Dutta, Mimura, Phys.Rev.Lett.97:241802,2006.
Large Phase of
CP violation in
Measurements :
SM prediction : small!
2.2 sigma deviation from the SM
(arXiv: 0712.2397)
(arXiv: 0802.2255)
Combined data analysis by UTfit: More than 3 sigma deviation from the SM
arXiv:0803.0659
However, experimental result of does not constrain size of SUSY contribution much.
Accurate measurement of mass difference is consistent with SM.
There is room for a sizable SUSY contribution.
One may think that large SUSY contribution is not allowed.
New Physics Contribution in the Mixing
Due to free phases in the Yukawa coupling
[Tevatron]
What is this large SUSY contribution?
SU(5) GUT
Down quarks and lepton doublet are unified in
Right-handed neutrino :
Both RH down-squarks and LH sleptons can have FCNC effects.
(Moroi, Akama-Kiyo-Komine-Moroi, Baek-Goto-Okada-Okumura, …)
U is the MNS neutrino mixing matrix.
SU(5) GUT…
The flavor violating elements in m25 induces Bs mixing
Both left- and right-squarks have FCNC effects in SO(10).
Flavor violating effects are larger in the box diagram in SO(10).
SO(10) GUT
In the SO(10) model, can be large due to left-right box enhancement.
can be suppressed by a choice of vacua.
If (8,2,1/2) (in 126 Higgs) is light, it generates FCNC in the quark sector
For example,
Light (8,2,1/2) is needed to suppress proton decay.
(Dutta-Mimura-Mohapatra, Phys.Rev.Lett.100:181801,2008. )
SO(10) GUT…
(8,2,1/2) introduces flavor violation only in the squark sector
If is suppressed by a choice of the vacua, constraint is important.
However, can be adjusted to be the experimental rangeunless is enhanced too much by gluino contribution.
(this requires small left-right mixing for sbottom)
Direct CP violation of can be largefor large
Large Tan
h0, H0, A0
bR sL
bRsL
Double penguin diagram can have largeContribution
This diagram’s contribution (~tan4/MA4)
Similar single penguin diagrams contribute to Bs process (~2tan6/MA
4)
Large Bs phase induces larger Bs process even for tan~20 for universal boundary condition
Both SU(5) and SO(10) get contribution from this diagram
Chargino and gluino mediated penguins contribute
Conclusion We study the bound of from the LFV in SUSY GUT models.
SUSY spectrum is restricted in SU(5) modelwhere Dirac neutrino is the origin of the large phase.
SO(10) models can generate larger phases.
We expect further accurate experimentsto learn more about the GUT scale physics from the