anomalous right-handed top quark couplings kang young lee (konkuk univ.) tevatron b physics kisti...

23
Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics workshop @ KISTI 2009. 8. 24.

Upload: christian-copeland

Post on 18-Jan-2018

220 views

Category:

Documents


0 download

DESCRIPTION

Contents Introduction B→X s γ decays B q -B q mixing Results Top quark decays Summary -

TRANSCRIPT

Page 1: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Anomalous Right-handed Top Quark Couplings

Kang Young Lee(Konkuk Univ.)

Tevatron B physics workshop @ KISTI 2009. 8. 24.

Page 2: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics 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).

Page 3: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Contents

• Introduction

• B→Xsγ decays

• Bq-Bq mixing

• Results• Top quark decays• Summary

-

Page 4: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

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.

Page 5: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

The CKM matrix

Not directly measured >0.74without unitarity D0 arXiv: 0803.0739CDF Note 8968

Page 6: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

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.

Page 7: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

ΔB=1 effective Hamiltonian

Oi : SM operatorsOi‘ : chiral conjugate operators

SM Wilson coefficients

B→Xsγ decays

Page 8: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Turn on the right-handed couplings

with the new loop functions

Page 9: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

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

Page 10: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

-

Mass and width differences

Schreodinger equation

Note that

Bq-Bq mixing

Page 11: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Transition amplitude

with

Page 12: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

SM predictions A. Lenz and U. Nierste, JHEP 06, 072 (2007)

Measurements

HFAG

CDF, PRL 97, 242003 (2006)D0, D0 note 5618-CONF

Page 13: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

We obtain

ξb =0

Results

Page 14: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

We obtain

ξs =0

Page 15: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

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.

-

-

-

Page 16: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

ξb =0

A. Lenz and U. Nierste, JHEP 06, 072 (2007)

Page 17: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

ξs =0

sin 2β

Page 18: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Top quark decays

Nondiagonal top quark decays

which is insensitive to ξs and directly measure Vtseff .

Large deviation from the SM prediction is possible.

Page 19: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Note that in the SM

Can we measure it?

Page 20: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

• 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

-

Page 21: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24
Page 22: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24

Backup Slides

Page 23: Anomalous Right-handed Top Quark Couplings Kang Young Lee (Konkuk Univ.) Tevatron B physics KISTI 2009. 8. 24