Abstract

For the first time, the strong phase difference between D0 and {overline{D}}^0to {pi}^{+}{pi}^{-}{pi}^{+}{pi}^{-} amplitudes is determined in bins of the decay phase space. The measurement uses 818 pb−1 of e+e− collision data that is taken at the ψ(3770) resonance and collected by the CLEO-c experiment. The measurement is important for the determination of the CP -violating phase γ in B± → DK± (and similar) decays, where the D meson (which represents a superposition of D0 and {overline{D}}^0 ) subsequently decays to π+π−π+π−. To obtain optimal sensitivity to γ, the phase space of the D → π+π−π+π− decay is divided into bins based on a recent amplitude model of the decay. Although an amplitude model is used to define the bins, the measurements obtained are model-independent. The CP -even fraction of the D → π+π−π+π− decay is determined to be F+4π = 0.769 ± 0.021 ± 0.010, where the uncertainties are statistical and systematic, respectively. Using simulated B± → DK±, D → π+π−π+π− decays, it is estimated that by the end of the current LHC run, the LHCb experiment could determine γ from this decay mode with an uncertainty of (±10 ± 7)°, where the first uncertainty is statistical based on estimated LHCb event yields, and the second is due to the uncertainties on the parameters determined in this paper.

Highlights

  • Between b → u W − and b → c W − quark transitions

  • Using 818 pb−1 of e+e− collision data collected by the CLEO-c detector, the hadronic parameters of the D → 4π± decay are measured in bins of phase space for the first time

  • This allows the UT angle γ to be determined using only B± → DK± decays where D decays to the 4π± final state; previously only phase space integrated measurements have been possible [19, 20], which need to be combined with other final states to obtain constraints on γ [20, 46]

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Summary

Formalism

The mass eigenstates of the D meson, |D1,2 , can be written in terms of the flavour eigenstates,. The D0 and D0 decay amplitudes for a final state f are defined Afp = fp|H|D0 and. For two-, three- and four-body pseudo-scalar final states the phase space dimensionality is 0, 2 and 5, respectively. The branching fraction for D0 → fi and D0 → fi decays are defined, Kif = |Afp|2φ(p)dp i. Where φ(p) gives the density of states at p From these follow the quantities Tif = Kif/ i Kif and Tif = Kif / i Kif , which give the fraction of D0 → f and D0 → f decays that populate phase space bin i, respectively.. To describe the interference of D0 → f and D0 → f amplitudes integrated over the region i, the bin-averaged sine and cosine are defined, cfi = sfi =

Kif Kif
Binning
KS0 veto bin
Model predictions of the hadronic parameters
Alternate binning
Optimal binning
Event selection
Systematics
Results and consistency checks
Sensitivity studies
10 Summary
A Helicity variables
B Statistical and systematic correlations
List of files
Hyper-binning

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