Primary Authors: Michael Feindt, Dominik Horn, Michal Kreps, Thomas Kuhr
In case of a finite decay width difference between the mass eigenstates of the Bs system, ΔΓs = Γ(Bs,L) - Γ(Bs,H), the experimental sensitivity to CP violation is improved and can even be measured in analyses without flavor tagging. The dominant contribution to ΔΓs is believed to come from the Bs → Ds(*)+ Ds(*)- decay, which is predominantly CP-even and saturates ΔΓs under certain theoretical assumptions, resulting in the relation 2 BR(Bs → Ds(*)+ Ds(*)-) ≈ ΔΓs / (Γs + ΔΓs/2).
In a data sample corresponding to an integrated luminosity of 6.8 fb-1 collected by the displaced track trigger we reconstruct about 750 Bs → Ds(*)+ Ds(*)- decays and measure the Bs production rate times Bs → Ds(*)+ Ds(*)- branching ratios relative to the normalization mode B0 → Ds+ D-:
fDs(*)Ds(*) = fs/fd BR(Bs → Ds(*)+ Ds(*)-) / BR(Ds+ D-)The relative branching fractions are determined in a simultaneous mass fit to two signal and two normalization samples. The measured fDs(*)Ds(*) values depend on the yields observed on the four samples and the relative efficiency of signal and normalization modes. An accurate determination of the relative efficiencies is achieved by taking into account, for the first time, the Dalitz structure of the Ds+ decay.
The analysis is described in detail in Public Note 10721.
fDsDs = 0.183 ± 0.021 ± 0.017
fDs*Ds = 0.424 ± 0.046 ± 0.035
fDs*Ds* = 0.654 ± 0.072 ± 0.065
fDs(*)Ds(*) = 1.261 ± 0.095 ± 0.112,
BR(Bs → Ds+ Ds-) = (0.49 ± 0.06 ± 0.05 ± 0.08) %,
BR(Bs → Ds*± Ds∓) = (1.13 ± 0.12 ± 0.09 ± 0.19) %,
BR(Bs → Ds*+ Ds*-) = (1.75 ± 0.19 ± 0.17 ± 0.29) %,
BR(Bs → Ds(*)+ Ds(*)-) = (3.38 ± 0.25 ± 0.30 ± 0.56) %,
ΔΓs / Γs = (6.99 ± 0.54 ± 0.64 ± 1.20)%.