2022
DOI: 10.48550/arxiv.2207.00023
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A Consistent Theory of Kinetic Mixing and the Higgs Low-Energy Theorem

Martin Bauer,
Patrick Foldenauer
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“…2 and m 2 τ,µ /m 2 Z . Following the analysis of [73], because Z D interacts at leading order with SM fields (the τ or µ, depending on whether we consider Scenario A or Scenario B, and its corresponding neutrino), we have included the effects of both the kinetic mixing of the Z D with the U (1) Y and SU (2) L gauge fields. Given that the coefficient es w /(12π 2 c w ) ≈ 1.4 × 10 −3 , it is trivial to see that both kinetic mixing coefficients trivially satisfy precision electroweak constraints from, e.g., [19], as long as M Z D − m Z > ∼ 10 GeV.…”
Section: Precision Constraintsmentioning
confidence: 99%
“…2 and m 2 τ,µ /m 2 Z . Following the analysis of [73], because Z D interacts at leading order with SM fields (the τ or µ, depending on whether we consider Scenario A or Scenario B, and its corresponding neutrino), we have included the effects of both the kinetic mixing of the Z D with the U (1) Y and SU (2) L gauge fields. Given that the coefficient es w /(12π 2 c w ) ≈ 1.4 × 10 −3 , it is trivial to see that both kinetic mixing coefficients trivially satisfy precision electroweak constraints from, e.g., [19], as long as M Z D − m Z > ∼ 10 GeV.…”
Section: Precision Constraintsmentioning
confidence: 99%