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“New Prospects for Higgs Compositeness in h → Z γ,” “Leading SU(3)-breaking corrections to the baryon magnetic moments in Chiral Perturbation Theory,”Ī. Azatov, R. Contino, A. Di Iura and J. Galloway, L. S. Geng, J. Martin Camalich, L. Alvarez-Ruso and M. J. Vicente Vacas, “Dipole operator constraints on composite Higgs models,” “Charming CP Violation and Dipole Operators from RS Flavor Anarchy,” “Non Minimal Terms in Composite Higgs Models and in QCD,”Ī. Simone, O. Matsedonskyi, R. Rattazzi and A. Wulzer,Ĭ. Delaunay, J. F. Kamenik, G. Perez and L. Randall, “Light top partners and precision physics,” Zumino, Structure of phenomenological Lagrangians. “The Other Natural Two Higgs Doublet Model,” J. Mrazek, A. Pomarol, R. Rattazzi, M. Redi, J. Serra and A. Wulzer, “Testing the Muon g-2 Anomaly at the LHC,” “Explanation of the Muon g-2 Anomaly with Vectorlike Leptons and its Implications for Higgs Decays,”Ī. Freitas, J. Lykken, S. Kell and S. Westhoff,
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“Anthropic solution to the magnetic muon anomaly: the charged see-saw,” K. Kannike, M. Raidal, D. M. Straub and A. Strumia, “The Higgs as a Composite Nambu-Goldstone Boson,” ( g − 2 ) of the electron is related to the one of the muon as, One interesting prediction is that the contribution to the This can be realized if left-handed or right-handed fermions That are only broken by mixings proportional to the SM Yukawa couplings. In fact, partial compositenessĪllows to elegantly realize this hypothesis: this requires that the composite sector possesses flavor symmetries Tension with flavor constraints can be eliminated if the theory realizes MFV. For example B r 50 TeV much larger than the value expected for these models if they are relevant to Nevertheless, severe bounds exist especially in the lepton sector. The hypothesis of partial compositeness can suppress flavor transitions beyond the SM. It is interesting to cast our results into the broader flavor picture of partially composite Higgs models, see įor a detailed discussion. Without GB structure the Higgs can have additional non-derivative interactions with the heavy fermions that dominate Note that in theories with vector-like leptons To the SM where it is suppressed by m 2 μ / m 2 h compared to the gauge one. The contribution from Higgs exchange is not sub-leading contrary In the CCWZ parametrization this is particularly simple since the only off-diagonal terms in the mass matrixĪre the elementary-composite mixings. Within an explicit model the couplings in the equation above are obtained by rotating the matrices of couplings to the mass basis.įor this purpose, given the smallness of the muon mass, it is sufficient to use the rotation matrices to first order in the mixings. These contributions can be, in general, complex and generate both electric and magnetic dipole moments. ( v = 246 GeV) valid to first order in the mixings and in the limit m χ ≫ m Z, W, h. M μ m χ 8 π 2 v 2 ( ^ g W + L ) ( ^ g W + R ) ∗ M μ m χ 4 π 2 v 2 ( ^ g Z L ) ( ^ g Z R ) ∗