CP violation in lepton number violating semihadronic decays of K,D,Ds,B,BcK, D, D_s, B, B_c

preprint2014arXivOpen access

Abstract

We study the CP violation in lepton number violating meson decays M±→ℓ1±ℓ2±M′∓M^{\pm} \to \ell_1^{\pm} \ell_2^{\pm} M^{' \mp}, where MM and M′M^{'} are pseudoscalar mesons, M=K,D,Ds,B,BcM=K, D, D_s, B, B_c and M′=π,K,D,DsM^{'}=π, K, D, D_s, and the charged leptons are ℓ1,ℓ2=e,μ\ell_1, \ell_2 = e, μ. It turns out that the CP-violating difference S−(M)≡[Γ(M−→ℓ1−ℓ2−M′+)−Γ(M+→ℓ1+ℓ2+M′−)]S_{-}(M) \equiv [Γ(M^- \to \ell_1^- \ell_2^- M^{' +})-Γ(M^+ \to \ell_1^+ \ell_2^+ M^{' -})] can become appreciable when two intermediate on-shell Majorana neutrinos NjN_j (j=1,2j=1,2) participate in these decays. Our calculations show that the asymmetry becomes largest when the masses of N1N_1 and N2N_2 are almost degenerate, i.e., when the mass difference ΔMNΔM_N becomes comparable with the (small) decay widths ΓNΓ_N of these neutrinos: ΔMN≫̸ΓNΔM_N \not\gg Γ_N. We show that in such a case, the CP ratio ACP(M)≡[Γ(M−→ℓ1−ℓ2−M′+)−Γ(M+→ℓ1+ℓ2+M′−)]/[Γ(M−→ℓ1−ℓ2−M′+)+Γ(M+→ℓ1+ℓ2+M′−)]{\cal A}_{CP}(M) \equiv [Γ(M^- \to \ell_1^- \ell_2^- M^{' +})-Γ(M^+ \to \ell_1^+ \ell_2^+ M^{' -})]/[Γ(M^- \to \ell_1^- \ell_2^- M^{' +})+Γ(M^+ \to \ell_1^+ \ell_2^+ M^{' -})] becomes a quantity ∼1\sim 1. The observation of CP violation in these decays would be consistent with the existence of the well-motivated ννMSM model with two almost degenerate heavy neutrinos in the mass range between MN∼0.1M_N \sim 0.1-10110^1 GeV.

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