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2015
DOI: 10.1103/physrevd.91.055020
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Rare meson decay through off-shell doubly charged scalars

Abstract: The presence of charged scalars is almost inevitable in most of the beyond standard model scenarios. They are expected to be detected easily if they are there due to their electromagnetic charge. These charged scalars can be produced at the LHC and their decays may lead to interesting signals-multilepton final states, displaced vertices, etc. These charged particles also play crucial roles in low energy rare processes. Thus apart from the collider searches in low energy rare processes their presence can be sme… Show more

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Cited by 7 publications
(8 citation statements)
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References 27 publications
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“…We can estimate this as follows: from Eqs. (6) and (15) one can see that the ratio of the constants is ð2 6 π 3 Þ −1 ¼ 5.0 × 10 −4 , which provide most of the difference between Table I and II. The channels which have the largest upper limit are J=ψD Ãþ s l − l − , which are about 10 −28 .…”
Section: Theoretical Formalismmentioning
confidence: 93%
See 1 more Smart Citation
“…We can estimate this as follows: from Eqs. (6) and (15) one can see that the ratio of the constants is ð2 6 π 3 Þ −1 ¼ 5.0 × 10 −4 , which provide most of the difference between Table I and II. The channels which have the largest upper limit are J=ψD Ãþ s l − l − , which are about 10 −28 .…”
Section: Theoretical Formalismmentioning
confidence: 93%
“…Theoretically, the heavy bosons cannot on the mass shell, their contribution is reflected in effective interaction vertices [10]. Such low energy processes include the rare decays of top quark [11], τ lepton [11][12][13], or charged mesons [10,14,15]. Surely the branching ratios of these decay modes will be very small due to the large Higgs mass and small coupling constant.…”
Section: Introductionmentioning
confidence: 99%
“…So MLRSM-EFT scenario offers very convoluted contributions to 0ν2β process, and the usual constraints need to be revisited. The leptonic current for this process, and the meson decays (M + → M − l + l + ) are the same [247][248][249][250]. Thus the prediction for meson decays through Majorana neutrinos and doubly charged scalars will also be modified.…”
Section: Jhep09(2019)035mentioning
confidence: 96%
“…The first example follows from Ref. [3] where an outline of the algorithm was given for scalar propagators only. Consider the decay of a heavy lepton 0 to three leptons 1 , 2 , and 3 , mediated by scalars which we will call ∆.…”
Section: A 'Toy' Examplementioning
confidence: 99%