Abstract
We study the effect of interference on the lepton number violating~(LNV) and lepton number conserving~(LNC) three-body meson decays $M_1^{+}\to l_i^{+} l_j^{\pm}\pi^{\mp}$, that arise in a TeV scale Left Right Symmetric model~(LRSM) with degenerate or nearly degenerate right handed~(RH) neutrinos. LRSM contains three RH neutrinos and a RH gauge boson. The RH neutrinos with masses in the range of $M_N \sim$ (MeV - few GeV) can give resonant enhancement in the semi-leptonic LNV and LNC meson decays. In the case, where only one RH neutrino contributes to these decays, the predicted new physics branching ratio of semi-leptonic LNV and LNC meson decays $M_1^{+}\to l_i^{+} l_j^{+}\pi^{-}$ and $M_1^{+}\to l_i^{+} l_j^{-}\pi^{+}$ are equal. We find that with at least two RH neutrinos contributing to the process, the LNV and LNC decay rates can differ. Depending on the neutrino mixing angles and $CP$ violating phases, the branching ratios of LNV and LNC decay channels mediated by the heavy neutrinos can be either enhanced or suppressed, and the ratio of these two rates can differ from unity.
Highlights
The observation of light neutrino masses and mixings clearly indicates the existence of beyond-the-StandardModel (BSM) physics
We study the effect of interference on the lepton number violating (LNV) and lepton number conserving (LNC) three-body meson decays Mþ1 → lþi lÆj π∓ that arise in a TeV-scale left-right symmetric model (LRSM) with degenerate or nearly degenerate right-handed (RH) neutrinos
We study the three-body LNV and LNC meson decays—Mþ1 → lþi lþj M−2 and Mþ1 → lþi l−j Mþ2 for the LRSM, in particular focusing on the implications of possible interference effects that may occur due to degenerate or nearly degenerate RH neutrino states
Summary
The observation of light neutrino masses and mixings clearly indicates the existence of beyond-the-StandardModel (BSM) physics. While LHC searches are mostly sensitive to MN ∼ Oð100Þ GeV–few TeV, and MWR up to a few TeV, the rare LNV and LNC semileptonic meson decays on the other hand are sensitive to a much smaller RH neutrino mass range MN∼ (MeV–few GeV), and to a much higher value of the WR gauge boson mass. This scenario changes dramatically if more than one heavy neutrino state contributes in these processes with a nontrivial RH neutrino mixing matrix In this case, the predictions for the LNV and LNC meson decay rates can differ widely due to the interference among the contributions of different RH neutrinos. We summarize our most important findings in the conclusion
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