Electroweak model and constraints on new physics

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Universal extra dimensions and the Higgs boson mass (2002, methodology): “ (mH,1/R) parameters as a change of variables from (S,T) because the number of ﬁtting parameters is two in both cases. Thus, we can simply use the ∆χ2 contours in the (S,T) plane, for example, in Ref.[22]. The resulting 90% C.L. allowed region is shown in Fig.3. The region of smaller 1/R and larger ”
The Weak Neutral Current (2013, methodology): “that the neutral current is dominated by the exchange of a single Z boson. (Figure reprinted as permitted according to journal guidelines from Phys. Rev. D 86 (2012) 010001, J. Erler and P. Langacker [15].) Lq NC = 2 v2 1 u 5 2 u gu LV g LA 5 u+ d gd gd 5 d = 2 v2 L L gu LL u L u u L+ g LR ”
Constraints on flavor-diagonal non-standard neutrino interactions from Borexino Phase-II (2019, unknown): “which is consistent with theoretical expectations [31] and comparable in precision with the value found by the reactor νee scattering experiment TEXONO [80]:”
Basis-independent methods for the two-Higgs-doublet model III: The CP-conserving limit, custodial symmetry, and the oblique parameters S, T, U (2010, methodology): “The oblique parameters can be expressed in terms of the transverse part of the gauge boson two-point functions [19, 24]:(25) αT ≡ Π new WW (0) m(2)W − Π new ZZ (0) m(2)Z , (5.”