Abstract

The “Cabibbo Angle Anomaly” (CAA) originates from the disagreement between the CKM elements Vud and Vus extracted from superallowed beta and kaon decays, respectively, once compared via CKM unitarity. It points towards new physics with a significance of up to 4 σ, depending on the theoretical input used, and can be explained through modified W couplings to leptons. In this context, vector-like leptons (VLLs) are prime candidates for a corresponding UV completion since they can affect Wℓν couplings at tree-level, such that this modification can have the dominant phenomenological impact. In order to consistently assess agreement data, a global fit is necessary which we perform for gauge-invariant dimension-6 operators and all patterns obtained for the six possible representations (under the SM gauge group) of VLLs. We find that even in the lepton flavour universal case, including the measurements of the CKM elements Vus and Vud into the electroweak fit has a relevant impact, shifting the best fit point significantly. Concerning the VLLs we discuss the bounds from charged lepton flavour violating processes and observe that a single representation cannot describe experimental data significantly better than the SM hypothesis. However, allowing for several representations of VLLs at the same time, we find that the simple scenario in which N couples to electrons via the Higgs and Σ1 couples to muons not only explains the CAA but also improves the rest of the electroweak fit in such a way that its best fit point is preferred by more than 4 σ with respect to the begin.

Highlights

  • Since vector-like leptons (VLLs) can couple to SM leptons and the Higgs, they mix with the former after EW symmetry breaking [24]

  • In order to consistently assess agreement data, a global fit is necessary which we perform for gauge-invariant dimension-6 operators and all patterns obtained for the six possible representations of VLLs

  • Allowing for several representations of VLLs at the same time, we find that the simple scenario in which N couples to electrons via the Higgs and Σ1 couples to muons explains the CAA and improves the rest of the electroweak fit in such a way that its best fit point is preferred by more than 4 σ with respect to the begin

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Summary

Vector-like leptons

Moving beyond the model independent approach of the last subsection, we consider models with VLLs. The possible representations under the SM gauge group are given in table 1 Since these fermions are vectorial, they can have bare mass terms (already before EW symmetry breaking) and interact with SM gauge bosons via the covariant derivative which was defined in eq (2.3).. Note that if the VLLs N and Σ0 are Majorana fermions, N corresponds to the right-handed neutrino in the type I seesaw [14, 93], while Σ0 corresponds to the mediator in the III mechanism [16, 94, 95] In this case N and Σ0 generate the neutrino mass matrices. In the phenomenological analysis we will assume that such a mechanism is at work [99, 100], or that the VLLs N and Σ0 are Dirac fermions, meaning that the effects in modified W and Z couplings can be sizeable

Observables
Radiative lepton decays Using the branching ratio written as
LFU test
EW precision observables
Cabibbo angle anomaly
Analysis
Model independent analysis
Vector like leptons
Conclusions
A Miscellaneous formulas
Full Text
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