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Morimitsu Tanimoto Niigata University, JAPAN March 20 2013 @ MPIK Heidelberg Collaborated with Yusuke Shimizu and Kei Yamamoto

Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

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Page 1: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Morimitsu Tanimoto

       Niigata University, JAPAN   

March 20 2013 @ MPIK Heidelberg  

Collaborated with Yusuke Shimizu and Kei Yamamoto   

Page 2: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Plan of My talk

1Brief Review of CP Violation

2Experimental Status

3 Sbottom-Quark Mixing

Page 3: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

SM explains successfully CP violation of K and Bd    mesons. Triumph of Kobayashi-Maskawa model

1 Probing New Physics in B mesons

Page 4: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

CP violation for beginner

Page 5: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

,

Page 6: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 7: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Direct CP Violation

Tree Diagram in SM

CP asymmetry

Penguin Diagram in SM

Decay Amplitudes

- Ratio of Penguin and Tree

-strong phase shift -weak CP phase,

- Tree -Penguin,

Page 8: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

CP Violation in Mixing

Page 9: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Bd and Bs non-leptonic decays

Page 10: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Golden Mode in CP violation of B meson

New Physics ?

Standard Model

Page 11: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Experiment

CP Violation !

Time-dependent Asymmetry

Page 12: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

However,

there is still possibility to find New Physics in the CP violation phenomena (especially in Bs system) !  

TeV Scale Physics in LHC Era!

Precise measurement of CP violation in B mesons !

Page 13: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

The dispersive part of the mixing

The absorptive part of the mixing

Parameterization of New Physics(NP)

( We neglect NP at tree level decay in our work)

: Magnitude of NP normalized to SM

: NP relative phase

dispersive part absorptive part

Hamiltonian inducing mixing

New Physics?

Page 14: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Bd

Page 15: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

2 Expeimental Staus of B mesons

×

Page 16: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

CKM fit

No significant deviation !but,

New Physics Contributions to most loop processes still possible !

Page 17: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 18: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 19: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 20: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

T. Hurth, Mahmound, FarXiv:1211.6453v2

Page 21: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

LHCb first result in autumn 2013 ?

K. Hara KEK-ph 2013 March 6

Page 22: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 23: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 24: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 25: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

D0 Anomaly

Page 26: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 27: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

CP Violation in Bs

Page 28: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

New PhysicsSM

Observation

Page 29: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 30: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 31: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 32: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

SM prediction is same as in

Page 33: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Let’s discussion about CP asymmetries of meson .

Non-leptonic CP asymmetry in Bd and Bs

SM prediction

If there is only the KM phase,

Time dependent CP asymmetries

But there may be deviation between SM prediction and experimental results !

SM

Page 34: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 35: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 36: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Direct CP Violation in Charm Decays Direct CP Violation in Charm DecaysIn the case of Final state being a CP eigenstate

,Naive Estimation in SM

Page 37: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 38: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Still large error , New Physics ?

Another Direct CP Violation CP Violation of b→sγ ?

×

Page 39: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

How large contributions of Squark flavor mixing

in CP asymmetries of B mesons ?

3 Can we find SUSY in B decays ?

LHCb, Bell, Babar, etc. new results

SUSY parameter

Squark flavor mixing parameters

CP asymmetries in Bd and Bs

We constrain squark flavor mixing parametersby LHCb etc. results   + CEDM of strange quark + BR(b→s γ)

We predict CP asymmetries.

Our strategy:

Page 40: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Search for SUSY particles

So indirect search is also significant.For example, CP asymmetries of B mesons.

Page 41: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 42: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Squark flavor mixing

qL

qR

dSb

Page 43: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Assume

Page 44: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 45: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 46: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Experimental Constraints

Moriond2013:

Page 47: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 48: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

photon

Page 49: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 50: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Experimental Constraints

Page 51: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

arXiv:1211.5228 Hisano et al.Improved

Experimental Constraints

from Neutron EDM

Page 52: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 53: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 54: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 55: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 56: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 57: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 58: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

90% C.L.

Page 59: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 60: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

  4 Summary

Flavor Physics progress in LHC Era !

Page 61: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 62: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

ΔB=1 Effective Hamiltonian

Page 63: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

New CP Violating phases in

Page 64: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

D0 Anomaly (Tevatron)

Page 65: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

D0 Anomaly

Page 66: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Direct CP violation of decay

Experimental results :

Constraints from

SM prediction :

Dominant termin SM

Page 67: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

10-100 TeV, but depends on models

Page 68: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

Direct CP asymmetry

PenguinTree

+

Bs → K π- +

: weak phase

: strong phase

: relative magnitude of Penguin

: Tree level amplitude

Bs → K π-+

Page 69: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s
Page 70: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s

A few %

Page 71: Morimitsu Tanimoto - Startseite · 2017. 11. 21. · K. Hara KEK-ph 2013 March 6. D0 Anomaly. CP Violation in Bs. SM New Physics Observation. SM prediction is same as in. Let’s