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Measurements related to the CKM angle bf1 from BABAR

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Comparison with LASS data. Is this behaviour expected for a Kp S-P phase ? ... Global phase p added to LASS data points; Remarkable agreement! ... – PowerPoint PPT presentation

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Title: Measurements related to the CKM angle bf1 from BABAR


1
Measurements related to the CKM angle b/f1 from
BABAR
  • Marc Verderi
  • LLR Ecole polytechnique
  • For the BABAR collaboration
  • XXXIXèmes Rencontres de Moriond
  • Interactions ÉlectroFaibles et Théories Unifiées,
    2004

2
Introduction
  • sin2b measured with very high precision
  • but with 4-fold ambiguity on b
  • Reduce to a two-fold ambiguity if measuring cos2b
    sign
  • Present new method and first measurement of cos2b
    sign with B0?J/y K0 events
  • Present CP measurements of penguin dominated
    channels
  • B0?fKS
  • B0 ?KK-KS B ?KKSKS
  • New measurement !
  • B0?p0KS
  • B0?f0(980)KS
  • First measurement !

3
Measurement of cos2b signwith B0?J/y K0
4
cos2b with B0?J/yK0 ?
  • The CP content of the Scalar?Vector Vector
    B0?J/yK0(892) decay is both even and odd.
  • cos2b appears through CP-even CP-odd
    interferences in the observables
  • d0,d,d? strong phases of the decay amplitudes
  • Strong phases determined on neutral and charged
    B?J/yK decays, up to the two-fold ambiguity
  • Sign flip of cos(d-d?) and cos(d?-d0) between
    the two strong phases solutions !

? sign of cos2b is ambiguous ! with K(892)
alone.
5
Measurement of amplitudes
  • Amplitudes measured by angular analysis of
  • B0?J/y(Kp-)0 (c.c.)
  • B?J/y(KSp) (c.c.)
  • B?J/y(Kp0) (c.c.)

BABAR
L82fb-1
B0?J/y(Kp-)
B0?J/y(KSp0)
13114 evts
237651 evts
value stat. syst. A02
0.566 0.012 0.005 A2 0.204 0.015
0.005 A?2 0.230 0.015 0.004 d-d0
2.729 0.101 0.052 d?-d0 0.184 0.070 0.046
B?J/y(Kp0)
B?J/y(KSp)
67027 evts
79133 evts
mES (GeV/c2)
mES (GeV/c2)
  • Note BTW the 7.6s significance non-trivial strong
    phase
  • d-d?0.5970.0770.017
  • With ambiguous solution ( solution II )
  • d-d03.554 d?-d02.958

6
Accounting for a Kp S-wave
  • The ambiguity becomes
  • But the ambiguity on g can be broken !
  • Kp mass spectrum shows more than the K(892)
  • A broad Kp S-wave is known to lie in the K(892)
    region too Nucl. Phys. B 296, 493, (1988)
  • Introduction of a new amplitude to describe
    B?J/y(Kp)S-wave
  • relative strengths of the P and S contributions
  • And a new relative phase
  • gdS-d0

BABAR
Kp- L 82fb-1
7
Breaking the strong phases ambiguity
BABAR
  • Phase of a resonance rotates counterclockwise
    with mass
  • Wigner causality principle !
  • In the K(892) region
  • P-wave phase moves fast
  • S-wave phase moves slow
  • ? gdS-d0 must rotate clockwise
  • Fit for P and S wave intensities and g by Kp mass
    bin, fixing d-d0 and d?-d0 to
  • Solution I (2.729, 0.184)
  • Solution II (3.554, 2.958)
  • Physical behaviour observed for solution II !

P-wave intensity
Kp- L 82fb-1
S-wave intensity
sol. I
gdS-d0
sol. II
8
Comparison with LASS data
  • Is this behaviour expected for a Kp S-P phase ?
  • Compare with LASS data
  • Kp?Kp(n)
  • I1/2 contribution
  • Global phase p added to LASS data points
  • Remarkable agreement!
  • A bit surprising because very different processes
    !
  • Keep Solution II as the physical solution !
  • Note solution I is the one reported up to now !

BABAR
LASS data
sol. I
sol. II
Kp- L 82fb-1
9
Measurement of cos2b sign
  • cos2b measured by a time and angular analysis of
    the B0?J/y(KSp0)0 sample
  • 104 tagged events (low statistics !)
  • Fit with sin2b free in the fit
  • Fit with sin2b 0.731

BABAR
cos2b0.68
cos2b3.32
Dt (ps)
  • Assuming sin2b and cos2b comes from the same
    angle 2b, from Monte Carlo
  • Exclude cos2b
  • -(1-sin22b)1/2-0.68
  • _at_ 89 CL

PRELIMINARY !!!
10
CP measurements with penguin dominated modes
11
Windows to new physics
  • Decay time distribution
  • In naive picture
  • C0
  • S-hf.sin2b
  • In the following, report C and S values.
  • Penguin dominated modes, e.g. B0?fK0,
  • are sensitive to new physics through the loop.
  • Modes measure a sin2beff value which may differ
    from sin2b in SM by at most 0.2 to 0.4, depending
    on the mode

12
B0?fKS B0?fKL
BABAR
  • In SM, measures
  • sin2b, for B0?fKS
  • -sin2b, for B0?fKL

B0?fKS
BABAR
B0?fKL
L108fb-1 B0?fKS 709 events
BABAR
B0?fKL
5216 events
13
B0?KK-KSB?KKSKS
L111fb-1
  • 3 body decay B0?KK-KS
  • (excluding B0?fK0 events)
  • Together measurement of branching ratios to
    determine CP-even fraction, through isospin
    symmetry Belle Collaboration, Phys. Rev D69,
    012001 (2004)

BABAR
B0?KK-KS 20116 events
B?KKSKS 12214 events
14
CP with B?KKKS
  • even determination
  • Br(B0?KK-K0)
  • (23.82.01.6)10-6
  • Br(B?KKSKS)
  • (10.71.21.0)10-6
  • even0.980.150.04
  • Consistency check with angular distribution
  • decay measures sin2b

BABAR
  • Also, first measurement of CP-violating charge
    asymmetry with B?KKSKS
  • ACP(B?KKSKS) -0.042 0.114(stat) 0.02(syst)

15
B0?p0KS
  • Measures sin2b in SM
  • KS direction used to determine B0 vertex
  • Constrain in x-y to beam-spot
  • Cross checks with B0?J/yKS and B?pKS, ignoring
    J/y or p
  • B0 lifetime.

BABAR
L113 fb-1 12216 events
BABAR
16
B0?f0(980)KS ?pp-
?
  • Structure of scalar meson 0(980) obscure
  • But recent studies hep-ph/0011191 (2000) favor
    usual qq state
  • Decay can be dominated by b?sss penguin since
  • ss sizeable
  • b?uus tree doubly Cabbibo suppressed compared to
    leading penguin.
  • In this case, decay measures
  • Quasi 2-body analysis
  • Cut on the Dalitz plot to reduce contributions
    from r0 and f0(1370)
  • First observation of B0?f0(980)KS !

BABAR
L111fb-1 9414(stat)6(syst) evts
Total Continuum All bgk.
17
CP fit of B0?f0(980)KS
  • Consistency check fitting pp- mass spectrum with
    relativistic Breit-Wigner
  • CP fit result

BABAR
L111fb-1
BABAR
Total Continuum All bgk.
Total Continuum All bgk.
18
Summary of sin2b measurements from BABAR
  • Shows all sin2b measurements from BABAR
  • Including those not presented today

19
Summary
  • Many new results !
  • New method to break the B?J/y K strong phases
    and related cos2b sign ambiguities
  • Preliminary measurement of cos2b sign.
  • CP measurements with
  • New measurement of KK-KS and first measurement
    of KKSKS
  • First measurement with f0KS
  • Results being published
  • KSp0 submitted to PRL
  • Final result for fK0

20
and conclusion
  • At the present level of statistics, from cos2b
    sign measurement and CP measurements in penguin
    modes, BABARs picture of sin2b is Standard
    Model like.

21
Backup
22
C
23
cos2b contour plots
24
BELLE
25
Introduction
  • b?ccs
  • B0?J/y,Y(2S),cc1 KS
  • High precision measurement of sin2b
  • B0?J/y K0
  • Measurement of cos2b sign
  • b?ccd
  • Possible penguin pollution
  • B0?D()D(), J/y p0
  • Measure sin2b
  • b?sss
  • Penguin dominated modes
  • Sensitive to new physics
  • Measure sin2b in the SM
  • B0?fKS
  • B0 ?KK-KS B ?KKSKS
  • B0?hKS
  • B0?p0KS
  • B0?f0(980)KS
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