Abstract
Using 2.93 fb^{-1} of e^{+}e^{-} collision data collected at a center-of-mass energy of 3.773GeV with the BESIII detector, the first observation of the doubly Cabibbo-suppressed decay D^{+}→K^{+}π^{+}π^{-}π^{0} is reported. After removing decays that contain narrow intermediate resonances, including D^{+}→K^{+}η, D^{+}→K^{+}ω, and D^{+}→K^{+}ϕ, the branching fraction of the decay D^{+}→K^{+}π^{+}π^{-}π^{0} is measured to be (1.13±0.08_{stat}±0.03_{syst})×10^{-3}. The ratio of branching fractions of D^{+}→K^{+}π^{+}π^{-}π^{0} over D^{+}→K^{-}π^{+}π^{+}π^{0} is found to be (1.81±0.15)%, which corresponds to (6.28±0.52)tan^{4}θ_{C}, where θ_{C} is the Cabibbo mixing angle. This ratio is significantly larger than the corresponding ratios for other doubly Cabibbo-suppressed decays. The asymmetry of the branching fractions of charge-conjugated decays D^{±}→K^{±}π^{±}π^{∓}π^{0} is also determined, and no evidence for CP violation is found. In addition, the first evidence for the D^{+}→K^{+}ω decay, with a statistical significance of 3.3σ, is presented and the branching fraction is measured to be B(D^{+}→K^{+}ω)=(5.7_{-2.1}^{+2.5}_{stat}±0.2_{syst})×10^{-5}.
Highlights
2.93 fb−1 of eþe− collision data collected at a center-of-mass energy
which corresponds to ð6.28 Æ
This ratio is significantly larger than the corresponding ratios
Summary
CP violation in charmed-hadron decays is expected to be small, up to a few 10−3 for singly Cabibbo-suppressed processes, and much smaller for CF and DCS processes [12,15]. The invariant mass of the πþπ− pair must satisfy the condition jMπþπ− − MK0Sj > 20 MeV=c2 to reject the dominant peaking background from the singly Cabibbo-suppressed decay Dþ → K0SKþπ[0]. This requirement corresponds to about Æ5σ of the experimental resolution. To suppress non-ω backgrounds, the ω helicity angle is required to satisfy j cos θωj > 0.57, where θω is the opening angle between the normal to the ω → πþπ−π0 decay plane and the direction of the Dþ meson in the ω rest frame. The normalized slope parameter λ=λmax, introduced in Ref. [38], is required to be MtBagC (GeV/c2)
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