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LHC signatures of τ-flavoured vector leptoquarks

A bstract We consider the phenomenological signatures of Simplified Models of Flavourful Leptoquarks, whose Beyond-the-Standard Model (SM) couplings to fermion generations occur via textures that are well motivated from a broad class of ultraviolet flavour models (which we briefly review). We place...

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Published in:The journal of high energy physics 2022-08, Vol.2022 (8), p.127-31, Article 127
Main Authors: Bernigaud, Jordan, Blanke, Monika, de Medeiros Varzielas, Ivo, Talbert, Jim, Zurita, José
Format: Article
Language:English
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Summary:A bstract We consider the phenomenological signatures of Simplified Models of Flavourful Leptoquarks, whose Beyond-the-Standard Model (SM) couplings to fermion generations occur via textures that are well motivated from a broad class of ultraviolet flavour models (which we briefly review). We place particular emphasis on the study of the vector leptoquark ∆ μ with assignments ( 3 , 1 , 2 / 3) under the SM’s gauge symmetry, SU(3) C × SU(2) L × U(1) Y , which has the tantalising possibility of explaining both R K ∗ and R D ∗ anomalies. Upon performing global likelihood scans of the leptoquark’s coupling parameter space, focusing in particular on models with tree-level couplings to a single charged lepton species, we then provide confidence intervals and benchmark points preferred by low (er)-energy flavour data. Finally, we use these constraints to further evaluate the (promising) Large Hadron Collider (LHC) detection prospects of pairs of τ -flavoured ∆ μ , through their distinct (a)symmetric decay channels. Namely, we consider direct third-generation leptoquark and jets plus missing-energy searches at the LHC, which we find to be complementary. Depending on the simplified model under consideration, the direct searches constrain the ∆ μ mass up to 1500-1770 GeV when the branching fraction of ∆ μ is entirely to third-generation quarks (but are significantly reduced with decreased branching ratios to the third generation), whereas the missing-energy searches constrain the mass up to 1150-1700 GeV while being largely insensitive to the third-generation branching fraction.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP08(2022)127