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2016
DOI: 10.1007/978-3-319-22617-0_4
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Cited by 35 publications
(49 citation statements)
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References 53 publications
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“…L counts the loop level at which the operator is generated, E φ,V,ψ count the insertions of pions, elementary SM gauge bosons and fermions, d counts the derivatives and χ the mass insertions. Finally, µ ≥ 0 takes into account if some operator is further suppressed due to symmetry arguments [92] while E 4f ≥ 0 counts insertions of G-breaking effective four-fermion operators such as those responsible for the SM Yukawas.…”
Section: Condensate and Pngbsmentioning
confidence: 99%
“…L counts the loop level at which the operator is generated, E φ,V,ψ count the insertions of pions, elementary SM gauge bosons and fermions, d counts the derivatives and χ the mass insertions. Finally, µ ≥ 0 takes into account if some operator is further suppressed due to symmetry arguments [92] while E 4f ≥ 0 counts insertions of G-breaking effective four-fermion operators such as those responsible for the SM Yukawas.…”
Section: Condensate and Pngbsmentioning
confidence: 99%
“…To generate a visible NP effect in the b → sµ + µ − transition, there must be sufficiently large flavour violating interactions involving left-handed quarks. But apart 2 Contrary to [24], we will include resonances associated with U (1) X and SU (3)c in the following. 3 In models where the Higgs boson is implemented as a pseudo Nambu-Goldstone boson these mixing terms correspond to an expansion in the Higgs non-linearities.…”
Section: A Quark Flavour Physicsmentioning
confidence: 99%
“…In this work we will cover, in a two-site model approximation [22][23][24], all the possible couplings emerging from the interplay among the top partners sector and the composite operators sourced by the strong regime. The SO(5) invariance will fix the interactions of the following Lagrangian…”
Section: Assumptions and Set-upmentioning
confidence: 99%
“…The aim of this work is to explore the low energy implications from the interplay among three matter sectors: elementary states, composite fermionic partners and spin-1 resonances in a SO(5) CHM, within the two-site model approximation [22][23][24]. We will consider the interactions of the vector resonances ρ, here assumed to be triplets of SU (2) L × SU (2) R , with a set of SO(5)-invariant fermionic currents.…”
Section: Introductionmentioning
confidence: 99%