anomalous right-handed top quark couplings kang young lee (konkuk univ.) tevatron b physics kisti...
DESCRIPTION
Contents Introduction B→X s γ decays B q -B q mixing Results Top quark decays Summary -TRANSCRIPT
Anomalous Right-handed Top Quark Couplings
Kang Young Lee(Konkuk Univ.)
Tevatron B physics workshop @ KISTI 2009. 8. 24.
Based on
J. P. Lee and KYL, arXiv:0809.0751. J. P. Lee and KYL, Phys. Rev. D 78, 056004 (2008).KYL and W. Y. Song, Phys. Rev. D 66, 057901 (2002).
Contents
• Introduction
• B→Xsγ decays
• Bq-Bq mixing
• Results• Top quark decays• Summary
-
Introduction• LHC : the top quark factory in a sense
• More than 108-109 top quarks will be produced at LHC in a year (if LHC works at full power).
• Top quark couplings will be directly tested.
• Nondiagonal couplings may be observed.
• Anomalous top quark couplings are worth examining at present.
The CKM matrix
Not directly measured >0.74without unitarity D0 arXiv: 0803.0739CDF Note 8968
Effective Lagrangian
Vtqeff : measures SM-like left-handed couplings
ξq : measures right-handed couplings
Underlying new physics• Effective electroweak chiral Lagrangian• General Left-Right model (VL
CKM≠VRCKM)
• Etc.
New particles, neutral current interactions are ignored.
ΔB=1 effective Hamiltonian
Oi : SM operatorsOi‘ : chiral conjugate operators
SM Wilson coefficients
B→Xsγ decays
Turn on the right-handed couplings
with the new loop functions
Branching ratio
SM prediction at NNLOfor
M. Misiak and M. Steinhauser, NPB 764, 62 (2007)M. Misiak et al., PRL 98, 022002 (2007).
World average value of measurement HFAG
-
Mass and width differences
Schreodinger equation
Note that
Bq-Bq mixing
Transition amplitude
with
SM predictions A. Lenz and U. Nierste, JHEP 06, 072 (2007)
Measurements
HFAG
CDF, PRL 97, 242003 (2006)D0, D0 note 5618-CONF
We obtain
ξb =0
Results
We obtain
ξs =0
No CP violation is predicted in Bs-Bs mixing in the SM. (No phase in Vts and Vtb)
Combined analysis of current data of Bs-Bs mixing tells us that there exists some CP violation.
Our prediction of the phase of M12s is dominated
by the phase of Vtqeff.
The phase of Bd-Bd mixing is directly measured.
-
-
-
ξb =0
A. Lenz and U. Nierste, JHEP 06, 072 (2007)
ξs =0
sin 2β
Top quark decays
Nondiagonal top quark decays
which is insensitive to ξs and directly measure Vtseff .
Large deviation from the SM prediction is possible.
Note that in the SM
Can we measure it?
• Model independent study on the anomalous right-handed top quark couplings have been performed.
• Combined analysis of B→Xsγ decays and Bq-Bq mixing provides valuable information.
• Constraints on new physics parameters and predictions of departure from the SM are obtained.
• Nondiagonal top quark decays might examine the tsW coupling independently.
Summary
-
Backup Slides