Yukawa hierarchies are generated from powers of fully anarchic spurions in higher SU(2) and SU(3) flavor representations via progressive rank lifting through composite outer products, with explicit models and predictions for FCNCs and stochastic gravitational waves.
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Nelson-Barr models with vector-like quark doublets suppress hadronic CP violation to three loops via an accidental symmetry in the renormalizable theory, yielding phenomenologically viable solutions distinct from singlet-based models.
MAFS describes 15 flavor observables in SU(5) and SO(10) GUTs using 5 or 3 fitted small parameters at factor-of-two accuracy, implying large neutrino mixings and approximate leptogenesis without extra parameters in SU(5).
A subconstituent compositeness reading of the B-lattice organizes fermion masses and mixings on a ninths ladder with Z9 charges, yielding CKM/PMNS forms, m3 ≃ 51 meV, ma ∼ 7–12 μeV, and tanβ ≃ 10–16 from Λ and ε = 14/75.
citing papers explorer
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Hierarchies from Higher Flavor Spin
Yukawa hierarchies are generated from powers of fully anarchic spurions in higher SU(2) and SU(3) flavor representations via progressive rank lifting through composite outer products, with explicit models and predictions for FCNCs and stochastic gravitational waves.
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Nelson-Barr Models with Vector-Like Quark Doublets
Nelson-Barr models with vector-like quark doublets suppress hadronic CP violation to three loops via an accidental symmetry in the renormalizable theory, yielding phenomenologically viable solutions distinct from singlet-based models.
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Maximal Abelian Flavor Symmetries
MAFS describes 15 flavor observables in SU(5) and SO(10) GUTs using 5 or 3 fitted small parameters at factor-of-two accuracy, implying large neutrino mixings and approximate leptogenesis without extra parameters in SU(5).
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Generation as Compositeness: A Subconstituent Interpretation of the $B$-Lattice Flavor Hierarchy
A subconstituent compositeness reading of the B-lattice organizes fermion masses and mixings on a ninths ladder with Z9 charges, yielding CKM/PMNS forms, m3 ≃ 51 meV, ma ∼ 7–12 μeV, and tanβ ≃ 10–16 from Λ and ε = 14/75.