Distinctive signals of frustrated dark matter

Abstract

Abstract We study a renormalizable model of Dirac fermion dark matter (DM) that communicates with the Standard Model (SM) through a pair of mediators — one scalar, one fermion — in the representation (6, 1, 4 3 $$ \frac{4}{3} $$ ) of the SM gauge group SU(3)c × SU(2)L × U(1) Y . While such assignments preclude direct coupling of the dark matter to the Standard Model at tree level, we examine the many effective operators generated at one-loop order when the mediators are heavy, and find that they are often phenomenologically relevant. We reinterpret dijet and pair-produced resonance and jets + E T miss $$ {E}_{\mathrm{T}}^{\mathrm{miss}} $$ searches at the Large Hadron Collider (LHC) in order to constrain the mediator sector, and we examine an array of DM constraints ranging from the observed relic density Ω χ h Planck 2 $$ {h}_{\mathrm{Planck}}^2 $$ to indirect and direct searches for dark matter. Tree-level annihilation, available for DM masses starting at the TeV scale, is required in order to produce Ω χ h Planck 2 $$ {h}_{\mathrm{Planck}}^2 $$ through freeze-out, but loops — led by the dimension-five DM magnetic dipole moment — are nonetheless able to produce signals large enough to be constrained, particularly by the XENON1T experiment. In some benchmarks, we find a fair amount of parameter space left open by experiment and compatible with freeze-out. In other scenarios, however, the open space is quite small, suggesting a need for further model-building and/or non-standard cosmologies.

Keywords

• Dark Matter at Colliders
• Models for Dark Matter
• Particle Nature of Dark Matter
• Specific BSM Phenomenology