We apply the on-shell amplitude techniques in the domain of dark matter. Without evoking fields and Lagrangians, an effective theory for a massive spin-$S$ particle is defined in terms of on-shell amplitudes, which are written down using the massive spinor formalism. This procedure greatly simplifies the study of theories with a higher-spin dark matter particle. In particular, it provides an efficient way to calculate the rates of processes controlling dark matter production, and offers better physical insight into how different processes depend on the relevant scales in the theory. We demonstrate the applicability of these methods by exploring two scenarios where higher-spin DM is produced via the freeze-in mechanism. One scenario is minimal, involving only universal gravitational interactions, and is compatible with dark matter masses in a very broad range from sub-TeV to the GUT scale. The other scenario involves direct coupling of higher-spin DM to the Standard Model via the Higgs intermediary, and leads to a rich phenomenology, including dark matter decay signatures.
Cited by 4
Criado et al., A complete effective field theory for dark matter
J. High Energ. Phys. 2021, 81 (2021) [Crossref]
Arcadi et al., The Higgs-portal for dark matter: effective field theories versus concrete realizations
Eur. Phys. J. C 81, 653 (2021) [Crossref]
Criado et al., Higher-spin particles at high-energy colliders
J. High Energ. Phys. 2021, 254 (2021) [Crossref]
Cvitan et al., Gauging the Higher-Spin-Like Symmetries by the Moyal Product. II
Symmetry 13, 1581 (2021) [Crossref]
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- 1 Université Paris-Saclay / University of Paris-Saclay
- 2 Deutsches Elektronen-Synchrotron / Deutsche Elektronen-Synchrotron DESY [DESY]