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Neutrino mass constraints on electroweak parameters

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Figure 2.1: A conceptual drawing of the TWIST spectrometer. The superconducting solenoid is inside the steel yoke (the yoke itself is required to produce the highly uniform 2 Tesla field for the drift chamber)
Table 3.1: Constraints on µ-decay couplings g µ γ . The first eight rows give naturalness expectations in units of (v/Λ) 2 × (m ν /1 eV) on contributions from n = 6 muon decay operators (defined in Section 3.2 below) based on one-loop matching with the n =
Figure 3.1: Contributions from the operators (a) O V , AD (6) ˜ and (b) O W, AD (6) (denoted by the shaded box) to the amplitude for µ-decay
Figure 3.2: One-loop graphs for the matching contributions of the n = 6 operators (denoted by the shaded box) to the n = 4 mass operator O M, AD(4)
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Mixing among n = 6 operators Operator Renormalization: Matching and Mixing Conclusions Conclusions

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