last updated on 20110730
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Measurement of the branching fraction and time dependent CP-violation in B0 → D*+ D*- decays with the Belle Experiment
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We report the measurement of the branching fraction, the polarization and
the parameters of the time dependent CP-violation for B0 → D
*+ D*- decays using the full data sample of 772
million BB-pairs, collected
at the Υ(4S) resonance with the Belle detector at the KEKB
asymmetric-energy e+e- collider.
B0 mesons are reconstructed in the following decay chains
B0 → D*+ ( → D+ π0 ) D*- ( → D0 π- )
B0 → D*+ ( → D0 π+ ) D*- ( → D- π0 )
B0 → D*+ ( → D0 π+ ) D*- ( → D0 π- )
where 4 D+ and 5 D0 decay modes are reconstructed.
Since this is a decay of a scalar meson to two vector mesons, the final state
is a mixture of multiple CP-eigenstates and therefore an angular analysis
has to be performed to determine the fraction of CP-even decays. This is
done using two of three possible angles of the transversity base which are
denoted as cos θtr and cos θ1. The relation
between the amplitudes Ai and the CP-eigenvalue is given in the
table below and the angular distribution is given by:
1/Γ (d2Γ(B0→ D*+D*-))/(dcos θtr dcos θ1) = 9/16 (2|A0|2 cos2 θ1 sin2 θtr
+2|A⊥|2 sin2 θ1 cos2 θtr +|A\\|2 sin2 θ1 sin2 θtr)
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L
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transversity basis
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CP even / odd
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0
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1/3 ( √2 A\\ - A0 )
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even
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1
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A⊥
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odd
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2
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1/3 ( A\\ + √2 A0 )
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even
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Table 1 : Relation between relative angular momentum and the amplitudes
in the transversity basis
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Illustration of transversity basis.
The decay modes B0 → Ds+ D*- and B0 → Ds*+ D*- are
used as control sample in the measurement of the CP-violation to check
for a potential bias.
Branching Fraction Measurement
The number of signal events is extracted with a two dimensional extended unbinned maximum likelihood fit on Mbc and ΔE. The shapes of the signal distribution are determined using simulated signal events and in the fit on the reconstructed data sample the position, the width and the fraction of the signal distribution as well as the parameters of the background description are free.
The fitted number of signal events is 1225 ± 59.
The reconstructed efficiencies are determined for each combination of D-decay channels separately using simulated signal events and corrected according to known differences between measured data and simulated events.
The resulting branching fraction is Bf(B0 → D*+ D*-) = (7.82 ± 0.38 ± 0.60) × 10-4
Fitted Mbc and ΔE distribution projected in the signal range of the other variable
Measurement of polarization and CP-violation
These two measurements are performed simultaneously with a five dimensional fit on Mbc, ΔE, two of the three angles of the transversity base and Δt. The signal shapes for the angles cos θtr and cos θ1 are determined for each of the three polarizations independently using simulated signal events.
The signal PDF for the Δt distribution is
PB0 ( Δt ) = 1/4 τB0 e-|Δt|/τB0 (1 - q Δw + q(1 - 2 w) ( (1 - 2 Podd(cos θtr, cos θ1 ))S sin (Δm Δt) + A cos (Δm Δt)) ),
where Podd is the probability of an event to be CP-odd.
The preliminary results are:
- R0 = 0.62 ± 0.03 ± 0.01
- R⊥ = 0.14 ± 0.02 ± 0.01
- S = -0.79 ± 0.13 ± 0.03
- A = 0.15 ± 0.08 ± 0.02
Both the measurement of the branching fraction and the polarization are well consistent with previous measurements at Belle and BaBar and the values for S and A are consistent with the standard model.
Projections of the angular distributions in the signal range of ΔE and Mbc. The black (green, red) line shows the total (signal, background) pdf, while orange, blue and cyan show the signal contribution for each polarization: 0, ⊥, \\
Δt distribution and raw asymmetry for good tags (r > 0.5) in the signal region of ΔE and Mbc, red corresponds to positive tags, black to negative ones and the dashed curve to the fitted background.