last updated on 20110901
Study of the Suppressed Decays B- → D*K-, D* → Dπ0/γ, D → K+π-

The decay B- → D(*)K- (D = D(*)0 or D(*)0) plays an important role for the determination of the CP-violating angle φ3. The information of φ3 is extracted from the interference, which occurs when D(*)0 and D(*)0 decay to the same final state. The D* meson can be reconstructed from D* → Dπ0 or D* → Dγ. So-called ADS method uses the following D decay to K+π-, for which the effect of CP violation can be enhanced by the comparable magnitudes of interfering amplitudes [PRL 78, 3257 (1997), PRD 63, 036005 (2001)]. In 2010, we obtained the first evidence for B- → DK-, D → K+π- by introducing improved discrimination of the continuum background from e+e- → qq (q = u, d, s, c) [PRL 106, 231803 (2011)]. In this report, we show a result for B- → D*K-, D* → Dπ0/γ, D → K+π- based on the full 772 million BB pairs collected at Υ(4S) resonance.

The signal yield is extracted by a two dimensional fit on ΔE and NB', where NB' is a varibale for discriminating qq background. We note that NB' is obtained from NB' = ln(NB+0.6)/(1.0-NB) with NB being the varibable used for B- → DK-, D → K+π-. In Figs. 1 and 2, we show the result of the fit. We measure the ratio RD*K,Dπ0 and the asymmetry AD*K,Dπ0 defined by
Fig0c        Fig0d
where rB* = |A(B-D*0K-)/A(B- → D*0K-)|, rD = |A(D0 → K+π-)/A(D0 → K-π+)|, δB* = δ(B-D*0K-) - δ(B- → D*0K-), and δD = δ(D0 → K-π+) - δ(D0 → K+π-). For rD and δD, we have experimental inputs [HFAG page for charm physics]. Obtained results (PRELIMINARY) are

RD*K,Dπ0 = [1.0 +0.8-0.7 (stat) +0.1-0.2 (syst)] × 10-2            AD*K,Dπ0 = 0.4 +1.1-0.7 (stat) +0.2-0.1 (syst)
   RD*K,Dγ = [3.6 +1.4-1.2 (stat) ±0.2 (syst)] × 10-2               AD*K,Dγ = - 0.51 +0.33-0.29 (stat) ±0.08 (syst)

where the first evidence for D*K signal is obtaied for the γ mode with a significance of 3.5σ (including systematic error). For rB* = 0.1 [CKMfitter page], our results indicate negative cos(δB*D)cosφ3 and positive sin(δB*D)cosφ3 (consistent with the result obtained by B- → D*K-, D* → Dπ0/γ, D → KSπ+π- [PRD 81, 112002 (2010), PRL 105, 121801 (2010)]). Extraction of φ3 will be given by including other observables later.

Relevant figures:

Fig1 Fig1
Fig. 1 (related to RD*K,Dπ0): Result of the fit for the π0 mode (left) and the γ mode (right). Charge-conjugate decays are included.
The ΔE distributions (upper) and the NB' distributions (lower) are obtained by projecting in NB' > 1.0 and |ΔE| < 0.03 GeV, respectively.
The fitted sample is shown with dots with error bars and the PDF is shown with the solid blue curve, for which the components are shown
with thicker long-dashed red (D*K), long-dashed magenta (D*π), long-dashed brown (DK and Dπ), dash-dotted green (BB background),
and dashed blue (qq background). Better figures (eps format) are obtained by clicking the figures.
Fig2
Fig2
Fig. 2 (related to AD*K,Dπ0): ΔE distributions (NB' > 1.0) for the π0 mode (upper) and the γ mode (lower).
We show the distributions for B- (left) and B+ (right) candidates. The curves show the same components as in Fig. 1.
Better figures (eps format) are obtained by clicking the figures.