Abstract

Dark mesons are bosonic composites of a new, strongly-coupled sector beyond the Standard Model. We consider several dark sectors with fermions that transform under the electroweak group, as arise from a variety of models including strongly-coupled theories of dark matter (e.g., stealth dark matter), bosonic technicolor (strongly-coupled indcued electroweak symmetry breaking), vector-like confinement, etc. We consider theories with two and four flavors under an SU(N) strong group that acquire variously chiral, vector-like, and mixed contributions to their masses. We construct the non-linear sigma model describing the dark pions and match the ultraviolet theory onto a low energy effective theory that provides the leading interactions of the lightest dark pions with the Standard Model. We uncover two distinct classes of effective theories that are distinguishable by how the lightest dark pions decay: “Gaugephilic”: where π0 → Zh, π± → W h dominate once kinematically open, and “Gaugephobic”: where {pi}^0to overline{f}f , {pi}^{pm}to overline{f}^{prime }f dominate. Custodial SU(2) plays a critical role in determining the “philic” or “phobic” nature of a model. In dark sectors that preserve custodial SU(2), there is no axial anomaly, and so the decay π0 → γγ is highly suppressed. In a companion paper, we study dark pion production and decay at colliders, obtaining the constraints and sensitsivity at the LHC.

Highlights

  • Which at least an entire Higgs doublet emerges in the low energy effective theory

  • The two examples used above become tr(ΣH†) + h.c. and Tr(ΣH†H + h.c.) respectively, where Σ is the non-linear sigma model (NLSM) field. At this point it is useful to distinguish between the dark sectors that we consider in this paper and early proposals for dynamical electroweak symmetry breaking

  • In this paper we have studied dark sectors that arise from a new, strongly-coupled confining gauge group SU(ND) with dark fermions transforming under the electroweak part of the SM

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Summary

Defining the dark sector

Throughout this paper, we will refer to the new strong sector as the “dark” sector. It consists of a strongly-coupled “dark gauge group” SU(ND) with its own “dark confinement scale”, and “dark fermions” or “dark flavors” that transform under the dark group as well as the electroweak part of the Standard Model. The two examples used above become tr(ΣH†) + h.c. and Tr(ΣH†H + h.c.) respectively, where Σ is the NLSM field At this point it is useful to distinguish between the dark sectors that we consider in this paper and early proposals for dynamical electroweak symmetry breaking (technicolor). In addition to grouping dark fermions into multiplets of (gauged) SU(2)W ≡ SU(2)L, we assign them to multiplets of SU(2)R classify interactions in SU(2)L × SU(2)R language Put another way, interactions among the SM Higgs multiplet and dark fermions break the combination of the SU(2)R Higgs potential symmetry and the SU(Nfund) (or SU(Nanti)) flavor symmetries of the dark fermions down to a common SU(2), which we relabel as SU(2)R. Symmetry contain no terms with explicit t3R, while a generic custodial violating dark sector can have one or more such terms.

Effective interactions of dark pions
Dark pion triplet interactions in custodial preserving strong sectors
Two-Higgs doublet models
Neutral dark pion decay to diphotons
Two-flavor theories
Two-flavor chiral theory
Two-flavor vector-like theories
Four-flavor theories
Mixing with the Higgs and goldstones
Dark pion couplings to the SM
Dark sector custodial violation
Discussion
A Gaugephobic 2HDMs
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