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Moriond EW, 3 Mar 200 8 Tagir Aushev (EPFL, ITEP) 1 B K S 0 0 B K S K S B K S 0 B D *+ D *- B a 1 , a 1 K, b 1 , b 1 K... (4S) B CP B CP Measurements of φ 1 and φ 2 Tagir Aushev For the Belle Collaboration (EPFL, Lausanne ITEP, Moscow)

Measurements of φ 1 and φ 2

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Measurements of φ 1 and φ 2. B → K S p 0 p 0 B → K S K S B → K S p 0 B → D *+ D *- B → a 1 p , a 1 K, b 1 p , b 1 K... U (4S) → B CP B CP. Tagir Aushev For the Belle Collaboration (EPFL, Lausanne ITEP, Moscow). CKM matrix & unitary triangle. relative - PowerPoint PPT Presentation

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Page 1: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 1

B → KS 0 0

B → KS KS

B → KS 0

B → D*+ D*-

B → a1 , a1K, b1 , b1 K...(4S) → BCP BCP

Measurements of φ1 and φ2

Tagir AushevFor the Belle Collaboration

(EPFL, LausanneITEP, Moscow)

Page 2: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 2

† *1 0ud cd cbV V V V V *ubV tdV *

tbV

,

0,1

0,0

ud

cd cb

V

V V

*ubV tb

cd cb

V

V V

tdV

*

*

* *

* *arg , arg , argtd ubtb cd cb ud

ud tub td b cd cb

V V

V V

V V V V

V V V V

relative

magnitudes

CKM matrix & unitary triangle

Page 3: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 3

CP Violationin the Standard Model

• Triangle is well measured• φ1() mainly from B0→J/Ψ KS “golden mode”• Smaller and smaller room for the vertex position, but it is still in• New decay modes are examining to find a New Physics

Page 4: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 4

TCPV measurement on B-factory

B’s are produced in a boosted frame t is measured from vertex positions

B’s are entangled flavor of B1 at time t2 is determined by B2 decay

Page 5: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 5

8GeV (e-) 3.5GeV (e+)

Silicon Vertex Tracker

5-layer, double-sided strips

Drift Chamber40-layer, small

cell

DIRC (PID)quartz

Cherenkov detector

EM CalorimeterCsI crystals

Flux ReturnRPC and

LST instrument

ed iron

1.5 TSolenoi

d

Belle & BaBar B-factories

Page 6: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 6

BaBar collected 510 fb-1

Lpeak

=1.71×1034cm−2 s−1

∫Ldt=770 fb−1

Current luminosities

Page 7: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 7

BD(0,+)D0

After evidence for DCPV in BD-

D+ recently shown by Belle all BDD decays has a special interest

B.R. and charge asym for BD+D0 were updated by Belle:

B.R. = (3.85 ± 0.31 ± 0.38)·10-4

BaBar’06: (3.8 ± 0.6 ± 0.5)·10-

4

A = 0.00 ± 0.08 ± 0.02BaBar’06: -0.13 ± 0.14 ± 0.02

Also an upper limit for BD0D0 :B.R.<0.43·10-4@90%C.L.

hep-ex/0802.2988

Page 8: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 8

TCPV in B0D*+D*–

B0D*+D*– is b ccd transition and so sensitive to sin2 just like the “Golden” B0cc K0 making it an important check

Series of papers were published by Belle and BaBar

Recently the results are updated with latest statistics

Belle result is the first time presented

Belle Preliminary

N=545 +- 29

Phys.Rev.D76:111102,2007

Page 9: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 9

BaBar: R = 0.143 0.034 0.008

Belle: R = 0.116 0.042 0.004

Since it is a decay of S VV CP-eigenstate depends on angular momentum of the VV system:

• Separating the CP-odd fraction,

R, is done via a 1D angular

analysis

Helicity of B0D*+D*–

Belle Preliminary

Page 10: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 10

TCPV in B0D*+D*–

S=-sin21 A=-C

BaBar -0.66 ± 0.19 ± 0.04 +0.02 ± 0.11 ± 0.02

Belle -0.93 ± 0.24 ± 0.15 +0.16 ± 0.13 ± 0.02

tmtmtt

tttA dd

fBfB

fBfBCP

CPCP

CPCP

cossin)()(

)()()(

00

00

AS

Belle Preliminary

Page 11: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 11

Penguin dominated B decays are sensitive to NP

+

New Physics may introduces extra CP phase in the decay

Deviation of Time-dependent CP violation parameters from the SM expectation Hint of New Physics

Searches for a New Physics

SM

s,dq

qNP

s,dq

q

Page 12: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 12

TCPV in B0 → KS00 :bsqqNsig = 307±32

22Bbeambc pEM

Belle +0.43+/-0.49+/-0.09BaBar +0.72+/-0.71+/-0.08Average+0.52+/-0.41

Belle -0.17+/-0.24+/-0.06BaBar -0.23+/-0.52+/-0.13Average -0.18+/-0.22

LR>0.9, good tag

X

SM expectation

>2 from the SM

Phys.Rev.D76:071101,2007

Belle Preliminary

S=-sin21

A=-C

Page 13: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 13

TCPV in B0→KS π0

Nsig = 459 ± 29B.R.= (10.3±0.7±0.6)·10-6

Belle +0.33+/-0.35+/-0.08BaBar +0.40+/-0.23+/-0.03

Belle -0.05+/-0.14+/-0.05BaBar -0.24+/-0.15+/-0.03

S=sin21

A=-C

Phys.Rev.D77:012003,2008

Phys.Rev.D76:091103,2007

Page 14: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 14

~90o±10o

Measurements of φ2

was measured in and systems

The same matrix elements are also involved to the B decays to axial vectors a1, b1 …

Some of them can be used only with much larger statistics

Page 15: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 15

Measurement B a1

6

110

10)3.26.19.14(

).(.).(.

aRBaBRB

First time-dep CP asymmetry in B → a1+

0B

0B

PRL 98, 181803 (2007)

BaBar

?,779eff

608 ± 53 B0→a1 (461 ± 53 flav.-tagged)

Belle Preliminary

Page 16: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 16

B→00

Latest result from Belle:

Page 17: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 17

B decays to light mesons

B→b10π+: (6.7±1.7±1.0)·10-6

B→a10π+: (20.4±4.7±3.4)·10-6

B→b10K+: (9.1±1.7±1.0)·10-6

B→a1+K0: (34.9±5.0±4.4)·10-6

B→b1-π+: (10.9±1.2±0.9)·10-6

B→a1-π0: (13.2±2.7±2.1)·10-6

B→b1-K+: (7.4±1.0±1.0)·10-6

B→a1-K+: (16.3±2.9±2.3)·10-6

No charge asym’s foundPRL 99:261801, 2007PRL 100:051803, 2008PRL 99:241803, 2007

Page 18: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 18

CPCP Violating Decays of Violating Decays of thethe(4S)(4S)

CP violation !!

J/KS

11

J/KS

21

CP1 CP1

J/KL

11

J/KL

21

CP1

Y(4S)CP1

J/KS

11

CKS

C1KS

(2S)KS

21

CP1

B0

B0_

Page 19: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 19

Partial reconstruction

Partial reconstruction

Full reconstruction

+

-

KS

J/

+

-

+

-

J/c

KSSignal MC

J/(ll)KS

J/(any)KS

Y(4S)

_B0

B0

About 40 times higher eff. than full reconstruction method

1.1(0.6) inclusive-J/(c) events in 535 million Y(4S) decays

Page 20: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 20

Nsig=-1.5 -2.8 events+3.6

Br(Y(4S)B0B0J/KS+J/(c)KS) 4x107 (90%C.L.)

SM prediction : 1.4x10-7

Results with 535M Y(4S) decaysControl sample

B D(*)- and D*- B0 c KS and J/ KS

Nsig=35 ±16 events

B0 J/KS

B0 J/(c) KS

With 30 billion Y(4S) (30ab-1),

such decays will be observed

with 5 significance

Page 21: Measurements of  φ 1  and  φ 2

Moriond EW, 3 Mar 2008 Tagir Aushev (EPFL, ITEP) 21

Summary

• CP violations was measured in various B decays

– Both mixing-induced & direct CPV observed

• Excellent agreement with Standard Model

– Small room for New Physics remains in flavour sector

• Next order of the statistics is needed to give an answer for the New Physics existence