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Latest results on CP violation in B-meson mixing G.Borissov, Lancaster University, UK Flavour workshop, IPPP, Durham, 4-7 September 2013

Latest results on CP violation in B -meson mixing

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Latest results on CP violation in B -meson mixing. G.Borissov, Lancaster University, UK Flavour workshop, IPPP, Durham, 4-7 September 2013. Introduction. CP violation in mixing of neutral B mesons is a very active research direction Several new results are published recently - PowerPoint PPT Presentation

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Page 1: Latest results on CP violation in  B -meson mixing

Latest results on CP violationin B-meson mixing

G.Borissov, Lancaster University, UK

Flavour workshop,IPPP, Durham, 4-7 September 2013

Page 2: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 2

Introduction

• CP violation in mixing of neutral B mesons is a very active research direction

• Several new results are published recently

• Even more are expected

• SM predicts a very small value of CP violation compared to the current experimental sensitivity

• Uncertainties of the SM prediction are even less

• This opens an excellent possibility of searching for the new physics contribution by detecting a significant deviation of CP violation from zero – one of the "null tests" of the SM

Page 3: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 3

CP violation in mixing

– Can occur in any flavour-specific decay of neutral B mesons

– Semileptonic decays provide the simplest way to measure it

• Experimental observable of CP violation in mixing – semileptonic charge asymmetry of Bd and Bs mesons, or the asymmetry of the ``wrong-charge" decay of B mesons:

0B 0B

X

mix

0B 0B

X

mix

sdqXBXB

XBXBa

qq

qqqsl ,;

)()(

)()(00

00

Page 4: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 4

Mass mixing matrix

• Semileptonic charge asymmetry is related to the parameters of mass matrix (M-iΓ/2) describing the propagation of system:

• Δmq and ΔΓq are the mass and width difference of two physical states Bs

H (heavy) and Bs

L (light)

• mq12 and Γq

12 are non-diagonal elements of the (M-iΓ/2) matrix

12

1212

1212,,

12,,

arg

cos2

2

q

qq

qqHqLqq

qLqHqq

m

mmmm

),( 00 BB

12tan qq

qqsl m

a

Page 5: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 5

CP violation in mixing in the standard model

• SM prediction of CP violation in mixing:

– using prediction of adsl and as

sl from A. Lenz, U. Nierste, hep-ph/1102.4274

– Very small values and even smaller uncertainties

5

4

10)3.09.1(

10)6.01.4(

ssl

dsl

a

a

Page 6: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 6

Measurement of adsl (DØ)

• charge asymmetry of reconstructed semileptonic B0 decays: – B0→μ+D*−ν : ~545K events

– B0→μ+D−ν : ~740K events

– No initial flavour tagging: measure integrated asymmetry

and translate it into adsl

• resulting adsl is reduced by factor χd≈0.186

– Reversal of magnet polarities significantlyreduces systematics

• Result:(D0) )%14.045.068.0( d

sla

),(),(

),(),((*)00(*)00

(*)00(*)00

DBBNDBBN

DBBNDBBNA

B0→μ+D−ν

B0→μ+D*−ν

Page 7: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 7

Measurement of adsl (BaBar)

• Original method to measure adsl

• Semi-inclusive selection of semileptonic B0→l+D*−ν decays

• Tag initial state of B0 by the chargeof additional kaon from the second B0 meson:

• ~5.4 M partially reconstructed decays B0→l+D*−ν selected

• The most precise value of adsl

obtained:

)()(

)()(

KlNKlN

KlNKlNAll

F. Simonetto, EPS-2013

(BaBar) )%16.006.0( 36.032.0

d

sla

Page 8: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 8

Measurements of adsl

• Combination of all available results

• Mean value of these measurements (my average):

• Consistent with the SM prediction

new)(BaBar )%16.006.0(

(D0) )%14.045.068.0(

Belle) (BaBar, )%56.005.0(

36.032.0

dsl

dsl

dsl

a

a

a

)%26.023.0( dsla

Page 9: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 9

Measurement of assl (DØ)

• Charge asymmetry of reconstructed semileptonic B0

s decays:

– B0s→μ+D(*)−

sν : ~204K events

– Ds→φπ decay used

– No initial flavour tagging: measure integrated asymmetry

and translate it into assl

• Reduction factor is χs ≈ 0.5

– Reversal of magnet polarities significantly reduces systematics

• Result:(D0) )%17.074.012.1( s

sla

),(),(

),(),((*)00(*)00

(*)00(*)00

ssssss

ssssss

DBBNDBBN

DBBNDBBNA

Page 10: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 10

Measurement of assl (LHCb)

• Charge asymmetry of reconstructed semileptonic B0

s decays:

– B0s→μ+D(*)−

sν : ~185K events

– Clean signal selection with low background

– No initial flavour tagging• Reduction factor is χs ≈ 0.5

– Production asymmetry is suppresseddue to high oscillation frequency of Bs

– Reversal of magnet polarities significantly reduces systematics

• Result:

– arXiv: 1308.1048

(LHCb) )%36.050.006.0( ssla

Magnet up

Magnet down

Page 11: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 11

Measurements of assl

• Combination of all available results

• Mean value of these measurements (my average):

• Consistent with the SM prediction

(LHCb) )%36.050.006.0(

(D0) )%17.074.012.1(

ssl

ssl

a

a

)%48.048.0( ssla

Page 12: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 12

Dimuon charge asymmetry (DØ)

– N++, N−− − number of events with two muons of the same charge

– Measured in collisions so far

• After subtracting all possible background sources (not related to CP violation) the residual asymmetry reflects the contribution of CP-violating processes:

• ~3.9σ deviation from the SM expectation

NN

NNA

bkgCP AAA

pp

Page 13: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 13

Contributions to dimuon charge asymmetry

• Mixing of B mesons is a natural source of dimuon pairs at collider → CP violation in mixing contributes to the like-sign dimuon charge asymmetry

• Considered so far as the only contribution to the like-sign dimuon charge asymmetry:

– Linear contribution from both adsl and as

sl

– Kd and Ks – determined by the production and decay properties of Bd and Bs

pp

BX

X

0B0B

ssls

dsld

mixCP

mixCPCP

aKaKA

AA

Page 14: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 14

Comparison with dimuon asymmetry

• Using only direct measurements of ad

sl and assl we get:

– to be compared with the dimuon result:

• There is some tension between these results, at about 2σ

DØ dimuons

Combination12

), (from )%094.0024.0( ssl

dslCP aaA

) (from )%092.0272.0( CPA

This comparison is obsolete because a new source of the like-sign dimuon asymmetry is identified recently

Page 15: Latest results on CP violation in  B -meson mixing

15

Contributions to dimuon charge asymmetry

• Recently one more contribution to the like-sign dimuon charge asymmetry is identified– G. Borissov, B. Hoeneisen, PRD 87, 074020(2013)

• It comes from CP violation in interference of decays with and without mixing

– This contribution is proportional to ΔΓd/Γd

– KΓ – determined by the production and decay properties of Bd

– It is much larger in magnitude than the contribution from CP violation in mixing considered so far

d

dintCP

ssls

dsld

mixCP

intCP

mixCPCP

KA

aKaKA

AAA

Page 16: Latest results on CP violation in  B -meson mixing

CP violation in interference• CP violation in the interference of B0 decay with and

without mixing to the same CP-eigenstate final state fCP which decays to muon

• This type of CP violation also contributes to the dimuon asymmetry:

0B

0B

0B

mix

CPf

0B0B

0B

mix

CPf

0B0B

0B

mix

CPf

BX

)()( 00CPCP fBfB

Page 17: Latest results on CP violation in  B -meson mixing

Example: B0→D+D−

• Consider the process producing the positive like-sign dimuon pair:

– The state D+D− is CP-even and is accessible from both

– Both D+ and D− can decay to muon, but only D+→μ+X contributes to the like-sign dimuon pair sample

• Numerically, the asymmetry is huge in magnitude and negative in sign:

XDDDB

Xb

XBbpp

;0

0

00 and BB

328.01

)2sin()()(

)()(200

00

d

d

x

x

DDBDDB

DDBDDB

d

dd

mx

Page 18: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 18

Bs meson contribution

• Contribution to the dimuon charge asymmetry:

• Corresponding contribution from Bs meson is strongly suppressed:

– sin(2βs) = 0.036

– ΔΓs/Γs = 0.15 ± 0.02

– xs /(1+xs2) = 0.037

d

sd

d

d

d

dintCP

mx

x

xBA

;

1)2sin()( 2

0

s

ss

s

s

s

sss

intCP

mx

x

xBA

;

1)2sin()( 2

Page 19: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 19

Numerical values

• SM contribution to the like-sign dimuon asymmetry due to CP violation in interference of B0 decay with and without mixing is

• To be compared with the SM contribution due to CP violation in mixing, considered so far:

• and with the experimental value of the like-sign dimuon asymmetry:

)%008.0035.0()( SMAintCP

)%001.0008.0()( SMAmixCP

D0) experiment( )%092.0272.0( CPA

Page 20: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 20

Width difference of B0

• Contribution AintCP is proportional to ΔΓd

• Prediction of the width difference of B0 in the SM:

– see A. Lenz, U. Nierste, arXiv: 1102.4274 [hep-ph]

• Experimental value is less precise:

• Need a better experimental measurement of ΔΓd

– "Forgotten null test"

– See T. Gershon, arXiv:1007.5135 [hep-ph]

0008.00042.0)( SMd

d

018.0015.0)( SMd

d

Page 21: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 21

Comparison of all measurements

• Dimuon charge asymmetry:

• Using independent measurements:

– adsl = (0.23 ± 0.26)% (my average)

– assl = (−0.48 ± 0.48)% (my average)

– ΔΓd / Γd = (1.5 ± 1.8)% (World average, PDG-2013)

– Results are consistent within 1σ

– Precision is determined by the width difference of ΔΓd / Γd

– Need to improve the precision of ΔΓd / Γd

d

dssls

dsldCP KaKaKA

D0)( )%092.0272.0( CPA

ts)measurement Independen( )%175.0147.0( CPA

Page 22: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 22

Final result on dimuon asymmetry (DØ)

• D0 collaboration prepares the final result on the dimuon asymmetry– Full statistics

– Complete analysis of the dependence of asymmetry on muon impact parameter

– Model-independent result on ACP

– Provides an independent measurement of adsl , ad

sl , ΔΓd / Γd

– Will be available soon (hopefully)

Page 23: Latest results on CP violation in  B -meson mixing

6 September 2013 G.Borissov, Latest results on CP violation 23

Conclusions

• Study of CP violation in mixing – a very active research area

• Several new results (D0, LHCb, BaBar) became available recently

• ~3.8σ deviation from the SM expectation in the dimuon charge asymmetry

• Independent measurements of adsl , ad

sl , ΔΓd / Γd are consistent with the dimuon asymmetry within 1σ

• This comparison depends on the value of ΔΓd / Γd which is known with poor precision

• New measurements of this "forgotten" parameter are required