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B Decays to Measure g

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CP violation with B0 - yKS (sin2b) is well established. Agrees with Standard Model ... Reconstruct low momentum p in D* - Dp, but not rest of D. More signal events, ... – PowerPoint PPT presentation

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Title: B Decays to Measure g


1
B Decays to Measure g
  • Stephen Bailey
  • Harvard University
  • for the BaBar Collaboration
  • PASCOS 2003
  • Mumbai, India

2
Background
  • CP violation with B0 -gt yKS (sin2b) is well
    established
  • Agrees with Standard Model
  • Now we need to overconstrain the unitarity
    triangle to check consistency
  • g arg(VudVub / Vcd Vcb)
  • g -arg(Vub)in standard phase convention
  • Results from BaBar at PEP-II ee- -gt U(4S) -gt
    BBbar
  • 88 million BBbar pairs

h
g
r
3
Many Methods none are easy
  • Amplitude relationships with B- -gt D0CP K- and
    friends
  • Squashed amplitude triangles BR(B- ? D0bar
    K-) ltlt BR(B- ? D0 K-)
  • Interference involving doubly Cabibbo suppressed
    D0 decays
  • sin(2bg) with B0 -gt D()- p, r, a1,
  • Cabibbo suppressed B0 -gt D() p-
  • Use B0 -gt Ds() p and SU(3) to estimate B0 -gt
    D() p-
  • Progress on both full and partial reconstruction
    techniques
  • B -gt pp, Kp, KK
  • Several options with various theoretical
    trade-offs

4
B? ? D0CP K? and friends
  • D0CP (D0 D0bar) / Ö2 CP even or odd
    decays, e.g. KK-
  • Measure sides of amplitude triangles to determine
    g
  • Ö2 A(B- -gt D0CPK-) A(B- -gt D0K-) A(B- -gt
    D0barK-)
  • Ö2 A(B- -gt D0CPK-) A(B- -gt D0K-) A(B- -gt
    D0barK-) e-igeid
  • Sensitivity to g depends on r A(B- -gt
    D0barK-) / A(B- -gt D0K-)

strong phase
weak phase
5
B- ? D0 K-
hep-ex/0207087
D0 -gt Kp only
  • Use D0 -gt K-p, K-pp-p, K-pp0

B -gt D0p
B -gt D0K
(81M BBbar pairs 75 fb-1)
PDG BF(B- -gt D0p-) (5.30.5)x10-3
D0 -gt Kp only
with kaon ID cut and 3s mES cut
6
B? ? D0CP K?
hep-ex/0207087
  • B? ? D0KK- K?
  • 36.8 8.4 4.0 signal events
  • B? ? D0pp- K?
  • Upcoming
  • backgrounds from B -gt ppK

7
B? ? D0CP K? and friends
hep-ex/0207087
  • Direct CP asymmetry from D0CP states
  • ACP 0.17 0.23 0.09/-0.07

(81M BBbar pairs 75 fb-1)
8
B- ? D0bar K-
  • Hard BR(B- ? D0bar K-) ltlt BR(B- ? D0 K-)
  • Interference from doubly Cabibbo suppressed D0
    decays
  • B- -gt D0barK- (small) --gt Kp- (big)
  • B- -gt D0 K- (big) --gt Kp- (small)
  • Plan
  • Measure B- -gt D0(bar) K-w/ D0bar -gt Kp-,
    Kp-pp-, Kp-p0
  • Measure Multiple D0CP modes
  • See Gronau, hep-ph/0211282

9
B? ? D0CP K? Summary
hep-ex/0207087
  • B- -gt D0 K- measured
  • R(B -gt D0K/D0p) (8.31 0.35 0.20)
  • D0CP -gt KK- initial results available
  • Direct Asymmetry ACP 0.17 0.23 0.09/-0.07
  • More modes (e.g. D0CP -gt pp) in progress
  • More data coming too
  • Cabibbo suppressed modesin progress

(81M BBbar pairs 75 fb-1)
10
sin(2b g) with B0 ? D()p
  • Both D()p- and D()-p from B0 and B0bar
  • Interference -gt CP violation
  • B0 B0bar mixing e-i2b
  • b -gt u Vub e-ig
  • Large difference in branching fractions
  • BFfavored(B0 -gt D()-p) 3x10-3
  • BFsuppressed(B0 -gt D()p-) 10-6
  • Small CP violating effect expected (2)
  • Measure one weak phase (2bg) anda strong phase
    (d) for each mode

11
sin(2b g) B0 ? Ds()p
hep-ex/0207053
too small to measure w/ current data
  • l() 0.02
  • Use B0 -gt Ds()p- to estimateA(B0 -gt D()p-)
    via SU(3) symmetry
  • Introduces theoretical uncertainty
  • B0 -gt Dsp-
  • Use Ds -gt fp, KsK, KbarK
  • 21.4 5.1 signal events
  • BF(B0 -gt Dsp-) (3.2 0.9 1.0) x 10-5
  • 84M BBbar pairs 78 fb-1
  • BF(B0 -gt Dsp-) lt 4.1 x 10-5 90 CL

12
sin(2b g) Fully reconstructed B0 ? D()p
  • Fully reconstruct both Dp and Dp
  • Time evolution for each state f
  • Four ls include one weak phase (2bg) and two
    strong phases (d())

arg(lDp-) -(2bgd) arg(lD-p) -(2bg-d)
arg(lDp-) -(2bgd) arg(lD-p) -(2bg-d)
13
sin(2b g) Fully reconstructed B0 ? D()p
  • We have thousands of fully reconstructed B0 -gt Dp
    andB0 -gt Dp
  • The sin(2bg) fitter is being studied
  • The results arent unblinded yet
  • mES from B0 -gt D-p with 5.2 fb-1
  • very clean signal
  • now we have almost 20x more data

5.2 fb-1 B0 ? D-p
14
sin(2b g) Partially reconstructed B0 ? Dp
  • Another method Partial D reconstruction
  • Reconstruct low momentum p in D -gt Dp, but not
    rest of D
  • More signal events,but also more background
  • N(tagged) gt 40 000 eventsin full dataset

20.3 fb-1 only a fraction of the current data,
but shows approximate S/B
15
sin(2b g) Partially reconstructed B0 ? Dp
  • Unreconstructed D daughters could affect tag
    sidevertex position measurement
  • Validate partial reco. method with a lifetime
    measurement
  • t(B0) (1.510 0.040 0.041) ps (with 20.7
    fb-1)
  • cf PDG t(B0) (1.548 0.032) ps
  • hep-ex/0212012 submitted to PRD
  • Proceeding with sin(2bg) fit, results not
    unblinded yet

16
B0 ? pp, Kp, KK
  • Amplitude relationships with B -gt pp, Kp, KKmay
    also measure or constrain g
  • Theoretical interpretation is complicated
  • Penguins
  • Rescattering contributions
  • SU(3) symmetry breaking
  • etc.
  • For a recent brief review, see Fleischer,
    hep-ph/0207324
  • For now well quote branching fractions (BF) and
    Asymmetries (A) and let you plug the numbers into
    your favorite theory

17
B0 ? pp, Kp, KK
hep-ex/0207055 hex-ex/0207065 hex-ex/0207063 hep-e
x/0206053
(81 fb-1 except K0p, KK0bar 54 fb-1)
18
Many More Modes
  • Exploring many other modes which could measure g
    or 2bg
  • B -gt D()K()
  • B -gt D()KS
  • B -gt D KS p
  • B -gt D() K() p
  • Dalitz analysis of B -gt ppp
  • etc.

19
Outlook
  • The Good News Were making progress
  • B- -gt D0CP K-
  • Several sides of amplitude triangles measured
  • ACP 0.17 0.23 0.09/-0.07
  • sin(2bg) with B0 -gt D()p
  • Decay modes reconstructed
  • Lifetime measurement checks method
  • sin(2bg) fit results in progress
  • B0 -gt pp, Kp, KK
  • Many branching fractions measured
  • Need theoretical input for interpretation
  • Final story will likely involve
  • B factory measurements of many decay modes
  • Hadronic accelerator results with Bs decays
  • Theoretical input
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