Dark Particles at the LHC: LHC-Friendly Dark Matter Characterization via Non-Linear EFT

TL;DR

This paper introduces a flexible non-linear EFT framework for describing LHC phenomenology of extended scalar sectors and dark matter interactions, capturing diverse models and collider signatures without specifying UV origins.

Contribution

It develops a general non-linear EFT approach for scalar and fermion sectors, enabling comprehensive dark matter and collider phenomenology analysis independent of UV details.

Findings

Framework captures a wide range of DM models and signatures.

Allows analysis of collider signals like mono-h and mono-Z.

Provides correlations to diagnose new particle properties.

Abstract

In this work we illustrate a general framework to describe the LHC phenomenology of extended scalar (and fermion) sectors, with focus on dark matter (DM) physics, based on an effective field theory (EFT) with non-linearly realized electroweak symmetry. Generalizing Higgs EFT (HEFT), the setup allows to include a generic set of new scalar resonances, without the need to specify their UV origin, that could for example be at the interface of the Standard Model (SM) and the DM world. In particular, we study the case of fermionic DM interacting with the SM via two mediators, each of which can possess either CP property and originate from various electroweak representations in the UV theory. Besides trilinear interactions between the mediators and DM or SM pairs (including pairs of gauge field-strength tensors), the EFT contains all further gauge-invariant operators up to mass dimension $D=5$. While remaining theoretically consistent, this setup offers enough flexibility to capture the phenomenology of many benchmark models used to interpret the results of experimental DM and BSM searches, such as two-Higgs doublet extensions of the SM or singlet extensions. Furthermore, the presence of two mediators with potentially sizable couplings allows to account for a broad variety of interesting collider signatures, as for example detectable mono-$h$ and mono-$Z$ signals. Correlations can be employed to diagnose the nature of the new particles.