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• W2903882189 abstract "We demonstrate that in a recently proposed unified leptoquark model based on the gauge group $SU(4{)}_{C}ifmmodetimeselsetexttimesfi{}SU(2{)}_{L}ifmmodetimeselsetexttimesfi{}U(1{)}_{R}$ significant deviations from the Standard Model values of ${R}_{K}$ and ${R}_{{K}^{*}}$ can be accommodated without any need of extra heavy fermions. Low energy data, in particular lepton-flavor-violating $ensuremath{mu}$ decays and ${K}_{L}ensuremath{rightarrow}eensuremath{mu}$, severely constrain the available parameter space. We show that in the allowed part of the parameter space (i) some of the lepton-flavor-violating tau decay branching ratios are predicted to be close to their current experimental limits. (ii) The underlying scalar leptoquarks can be probed at the LHC via their dominant decay modes into tau leptons and electrons and the third generation quarks. (iii) The constraints from meson oscillations imply that the masses of scalar gluons, another pair of colored multiplets around, have to be bigger than around 15 TeV, and thus, they can be probed only at a future 100 TeV collider. In both neutral and charged variants, these scalars decay predominantly into third generation quarks, with up to $O(10%)$ branching ratios into family-mixed final states. Besides that, we comment on the phenomenology of the scalar gluons in the current scenarios in the case that the $B$-decay anomalies eventually disappear." @default.
• W2903882189 created "2018-12-22" @default.
• W2903882189 creator A5009879959 @default.
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• W2903882189 date "2020-05-19" @default.
• W2903882189 modified "2023-09-24" @default.
• W2903882189 title "Collider phenomenology of a unified leptoquark model" @default.
• W2903882189 cites W1492480441 @default.
• W2903882189 cites W1529292243 @default.
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• W2903882189 cites W1560070765 @default.
• W2903882189 cites W1903994748 @default.
• W2903882189 cites W1965311100 @default.
• W2903882189 cites W1966205939 @default.
• W2903882189 cites W1970296662 @default.
• W2903882189 cites W1976959645 @default.
• W2903882189 cites W1996218638 @default.
• W2903882189 cites W1999069976 @default.
• W2903882189 cites W2011734771 @default.
• W2903882189 cites W2023949567 @default.
• W2903882189 cites W2031106460 @default.
• W2903882189 cites W2031275832 @default.
• W2903882189 cites W203209958 @default.
• W2903882189 cites W2039716321 @default.
• W2903882189 cites W2079880545 @default.
• W2903882189 cites W2113808159 @default.
• W2903882189 cites W2115200652 @default.
• W2903882189 cites W2129535822 @default.
• W2903882189 cites W2130084207 @default.
• W2903882189 cites W2150718882 @default.
• W2903882189 cites W2163749882 @default.
• W2903882189 cites W2178828159 @default.
• W2903882189 cites W2236661759 @default.
• W2903882189 cites W2238713807 @default.
• W2903882189 cites W2255019588 @default.
• W2903882189 cites W2278241181 @default.
• W2903882189 cites W2279275894 @default.
• W2903882189 cites W2282905657 @default.
• W2903882189 cites W2302365184 @default.
• W2903882189 cites W2309892451 @default.
• W2903882189 cites W2337119164 @default.
• W2903882189 cites W2345317779 @default.
• W2903882189 cites W2406276746 @default.
• W2903882189 cites W2463480065 @default.
• W2903882189 cites W2559250318 @default.
• W2903882189 cites W2569205317 @default.
• W2903882189 cites W2608323199 @default.
• W2903882189 cites W2609436106 @default.
• W2903882189 cites W2616775231 @default.
• W2903882189 cites W2638422081 @default.
• W2903882189 cites W2661398033 @default.
• W2903882189 cites W2747178068 @default.
• W2903882189 cites W2749699019 @default.
• W2903882189 cites W2752640842 @default.
• W2903882189 cites W2753339657 @default.
• W2903882189 cites W2766383761 @default.
• W2903882189 cites W2766841679 @default.
• W2903882189 cites W2767174810 @default.
• W2903882189 cites W2771243136 @default.
• W2903882189 cites W2775630683 @default.
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• W2903882189 cites W2786453416 @default.
• W2903882189 cites W2788309516 @default.
• W2903882189 cites W2794765155 @default.
• W2903882189 cites W2808939453 @default.
• W2903882189 cites W2810428888 @default.
• W2903882189 cites W2885926324 @default.
• W2903882189 cites W2887667301 @default.
• W2903882189 cites W2888584155 @default.
• W2903882189 cites W2891135394 @default.
• W2903882189 cites W2899140785 @default.
• W2903882189 cites W2900236209 @default.
• W2903882189 cites W2903032355 @default.
• W2903882189 cites W2949247842 @default.
• W2903882189 cites W2950570720 @default.
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• W2903882189 doi "https://doi.org/10.1103/physrevd.101.095024" @default.
• W2903882189 hasPublicationYear "2020" @default.
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