Abstract

We study electroweak scale Dark Matter (DM) whose interactions with baryonic matter are mediated by a heavy anomalous Z′. We emphasize that when the DM is a Majorana particle, its low-velocity annihilations are dominated by loop suppressed annihilations into the gauge bosons, rather than by p-wave or chirally suppressed annihilations into the SM fermions. Because the Z′ is anomalous, these kinds of DM models can be realized only as effective field theories (EFTs) with a well-defined cutoff, where heavy spectator fermions restore gauge invariance at high energies. We formulate these EFTs, estimate their cutoff and properly take into account the effect of the Chern-Simons terms one obtains after the spectator fermions are integrated out. We find that, while for light DM collider and direct detection experiments usually provide the strongest bounds, the bounds at higher masses are heavily dominated by indirect detection experiments, due to strong annihilation into W+W−, ZZ, Zγ and possibly into gg and γγ. We emphasize that these annihilation channels are generically significant because of the structure of the EFT, and therefore these models are prone to strong indirect detection constraints. Even though we focus on selected Z′ models for illustrative purposes, our setup is completely generic and can be used for analyzing the predictions of any anomalous Z′-mediated DM model with arbitrary charges.

Highlights

  • Models the mass bound on a thermal relic is expected to be significantly more modest

  • We study electroweak scale Dark Matter (DM) whose interactions with baryonic matter are mediated by a heavy anomalous Z

  • Even though we focus on selected Z models for illustrative purposes, our setup is completely generic and can be used for analyzing the predictions of any anomalous Z -mediated DM model with arbitrary charges

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Summary

Low-energy effective theory

We will review building of an EFT for a new gauge group which appears to be anomalous at low energies. If we choose the counterterm such that CN vanishes, and the effective action is invariant under the SU(N ) transformation (that we identify with the EW group transformation), we will not need any momentum shift between the two diagrams to restore gauge invariance. This is because the counterterm is imposing EW gauge invariance already. If we are not enforcing gauge invariance at the Lagrangian level with an appropriate Wess-Zumino counterterm, we are obliged to do it by choosing a non-trivial momentum shift, so that eventually all the three (and higher) point functions of the theory are well defined. Where ΓνNρG stands for the three-point function with the gauge boson Vμ replaced by its corresponding Goldstone boson

Dark matter models with heavy anomalous Z
Application to dark matter models
Annihilation cross sections into the SM gauge bosons
Relic abundance
Indirect detection
Gamma ray continuum searches
Gamma ray line searches
Neutrino telescopes
Colliders and direct detection
Summary of results
Comments on validity of our results
Conclusions
A Effective triple gauge boson couplings
Full Text
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