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Lepton Flavour Violating tau and mu decays induced by scalar leptoquark

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arxiv 1009.3886 v1 pith:HGQQVWC2 submitted 2010-09-20 hep-ph

classification hep-ph
keywords scalarbranchingflavourleptonleptoquarklimitsratioscouplings
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

We show that the scalar leptoquark Yukawa couplings generate a significant lepton flavour violation. We compute the light scalar leptoquark contributions to the branching ratios (Br) of the lepton flavour violating (LFV) decays $\ell \to \ell_i \ell_j \bar{\ell}_j$ and $\ell \rightarrow \ell^{\prime} \gamma$ with (i,j = e,$\mu$). We discuss the role of the relevant input parameters to these decay rates which are the Yukawa couplings ($h_{a\ell}$) with ($a=u,c,t$), the light scalar mass $M_{S_{1}}$ and the mixing angle $\sin2\theta_{LQ}$. We investigate the experimental limits from $(g-2)_\mu$, $\mu-e$ conversion and $\pi \to e \nu_e, \mu \nu_\mu$ to get constraint on the input parameter space. We predict that the upper limits on the branching ratios of $\tau \to \ell_i \ell_j \bar{\ell}_j $ can reach the experimental current limits. We also show that it is possible to accommodate both $\tau \to \ell_i \ell_j \bar{\ell}_j$ and $\tau \to \ell\gamma$ branching ratios for certain choices of LQ parameters.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Constraints on scalar leptoquarks from lepton and kaon physics

    hep-ph 2019-08 accept novelty 6.0 of 10

    Scalar leptoquark couplings are constrained by a comprehensive set of upper bounds from tau, muon, electron, and kaon decay data, including standard model interference in rare K to pi l+ l- modes.

  2. Scalar leptoquark effects on $B \to \mu \bar\nu$ decay

    hep-ph 2019-09 conditional novelty 5.0 of 10

    A scalar leptoquark S1 near 1 TeV can raise B to mu nu to the Belle central value, but required Yukawa couplings are large and several LHC and EDM constraints already cut into that parameter space.

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