Triple product asymmetries in K, D_(s) and B_(s) decays

preprint2011arXivOpen access

Abstract

One distinguishes between "true" CP violating triple product (TP) asymmetries which require no strong phases and "fake" asymmetries which are due to strong phases but require no CP violation. So far a single true TP asymmetry has been measured in KL→π+π−e+e−K_L\to π^+π^- e^+e^-. A general discussion is presented for T-odd TP asymmetries in four-body decays. It is shown that TP asymmetries vanish for two identical and kinematically indistinguishable particles in the final state. Two examples are D0→K−π+π−π+D^0\to K^-π^+π^-π^+ and D+→K−π+π+π0D^+\to K^-π^+π^+π^0. A non-zero TP asymmetry can be expected when non-trivial kinematic correlations exist, as in the decay KL→e+e−e+e−K_L \to e^+ e^- e^+ e^-. Triple product asymmetries measured in charmed particle decays indicate an interesting pattern of final-state interactions. We reiterate a discussion of TP asymmetries in BB meson decays to two vector mesons each decaying to a pseudoscalar pair, extending results to decays where one vector meson decays into a lepton pair. We derive expressions for time-dependent TP asymmetries for neutral B decays to flavorless states in terms of the neutral BB mass difference ΔmΔm and the width-difference ΔΓΔΓ. Time-integrated true CP violating asymmetries, measurable for untagged BsB_s decays, are shown to be suppressed by neither Γs/ΔmsΓ_s/Δm_s nor ΔΓs/ΓsΔΓ_s/Γ_s if transversity amplitudes for CP-even and CP-odd states involve different weak phases. In contrast, fake asymmetries require flavor tagging and are suppressed by the former ratio when time-integrated. We apply our results to B→K∗ϕB\to K^*ϕ and Bs→ϕϕB_s\toϕϕ data and suggest an application for Bs→J/ψϕB_s\to J/ψϕ.

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