Abstract

Effective theories are well established theoretical frameworks to describe the effect of energetically widely separated UV models on observables at lower energy scales. Due to the complexity of the effective theory when taking all the Standard Model symmetries and degrees of freedoms into account, tensioning the entire system in a completely agnostic way against experimental measurements results in constraints on the Wilson Coefficients of the effective operators that either bears little information or challenge intrinsic assumptions imposed on the effective field theory framework. In general, a specific high-scale extension of the Standard Model only induces a subset of all possible operators. Thus, by investigating which operators are induced by different classes of the Standard Model extensions and comparing to which precision observables they contribute, we show that it is possible to obtain an improved understanding of which UV model is realised in nature. We consider 15 UV models which are single scalar field extensions of the Standard Model and compute their dimension-6 operators after integrating out the heavy scalars up to 1-loop level. Only very few of these scenarios remain indistinguishable, while most of the models can be phenomenologically separated from one another. Most of these scenarios possess their own characteristic operator signature. Following the approach outlined here, a comparative analysis of a wide range of models will allow to assess at what level the effective field theory series can be truncated and which experimental measurements to prioritise.

Highlights

  • To explain the shortcomings of the Standard Model of particle physics, a plethora of extensions have been proposed that introduce new particles and interactions at high energies

  • It has become increasingly popular to tension experimental measurements with theory predictions using the language of effective field theories (EFTs)

  • The complexity of the operator space, already at dimension-6 within Standard Model Effective Field Theory (SMEFT), and the limited precision with which operators can be constrained experimentally jeopardize the applicability of this framework if no assumptions on the Standard Model extensions are imposed

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Summary

INTRODUCTION

To explain the shortcomings of the Standard Model of particle physics, a plethora of extensions have been proposed that introduce new particles and interactions at high energies. To showcase how a comprehensive consideration of phenomenological and theoretical constraints can result in an improved characterization of possible UV theories from EFT operators alone, we apply this approach to 15 different single-particle extensions of the SM, covering a wider range of models from colored to uncolored scalars.1 After integrating out these heavy non-SM particles from each BSM Lagrangian, we compute the dimension-6 effective operators up to 1-loop level, including the mixing between light and heavy degrees of freedom [24,31,45,46,47,48,49].

INTEGRATING OUT HEAVY FIELDS
INTERPLAY BETWEEN OBSERVABLES AND OPERATORS
OBSERVABLES AND BSM CLASSIFICATION
EWPO-LO and BSM classification
EWPO-NLO-I and BSM classification
Higgs signal strengths and BSM classification
EWPO-NLO-II and BSM classification
BSM CLASSIFICATION
CONCLUSIONS
Tree-level contribution
Full Text
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