sin2β

The mixing induced CP asymmetry, aJ/Ψ K0, in the Bd → J/Ψ K0 decays allows to determine the sine of the angle 2β almost without any hadronic uncertainties. In this case the CP asymmetry appears in the interference between amplitudes describing decays with and without mixing. The simples case is when the final state is a specific CP state. The following time dependent asymmetry is studied :

sin2β formula

The decay is dominated by a single (tree level) amplitude ( the same process can be described by a Penguin diagram which brings corrections at order ~ λ4 ). It implies that Cf ~ 0 and the expression simplify to :

sin2β-bis formula

The constraint on sin2β is obtained combining the experimental measurement on B0 → J/Ψ K0 decays to the data-driven determination of the theoretical error, obtained from the time-dependent asymmetry of B0 → J/Ψ π0 and the determination of decay rate and the C parameter of the time-dependent asymmetry in B0 → J/Ψ K0, following the prescription of hep-ph/0507290. The constraint on sin2β from B0 decays to K0 and higher charmonium states is not included, since the experimental information to determine the theoretical error on that is missing. The world averages for the experimental observables (taken from HFAG when not specified) are summarized in the table below


Observable B0 → J/Ψ π0 B± → J/Ψ π± B0 → J/Ψ K0
Branching Ratio [10-5] 2.02 ± 0.25 4.8 ± 0.4 86.3 ± 3.5
C / -ACP -0.11 ± 0.20 -0.09 ± 0.08 0.002 ± 0.021
S -0.68 ± 0.25 - 0.668 ± 0.026

Using these values, we obtain the following shapes for the theoretical error (top-left) and the value (top-right) of sin2β, shown also on the



theoretical error on sin2β
(EPS) [JPG]

theoretical error on sin2β
ΔS = 0.000 ± 0.012

theoretical error on sin2β
(EPS) [JPG]

Distribution of sin2β from B0 → J/Ψ K0
sin2β = 0.668 ± 0.028

present bound from sin2β
(EPS) [JPG]

sin2β bound from B0 → J/Ψ K0 shown on the (ρ, η) plane


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