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Dark matter coupling to electroweak gauge and Higgs bosons: an effective field theory approach

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arxiv 1305.0021 v1 pith:4AZIQYFO submitted 2013-04-30 hep-ph

Dark matter coupling to electroweak gauge and Higgs bosons: an effective field theory approach

classification hep-ph
keywords couplinggammadark-mattereffectivefieldmattertheorywimp
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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If dark matter is a new species of particle produced in the early universe as a cold thermal relic (a weakly-interacting massive particle-WIMP), its present abundance, its scattering with matter in direct-detection experiments, its present-day annihilation signature in indirect-detection experiments, and its production and detection at colliders, depend crucially on the WIMP coupling to standard-model (SM) particles. It is usually assumed that the WIMP couples to the SM sector through its interactions with quarks and leptons. In this paper we explore the possibility that the WIMP coupling to the SM sector is via electroweak gauge and Higgs bosons. In the absence of an ultraviolet-complete particle-physics model, we employ effective field theory to describe the WIMP--SM coupling. We consider both scalars and Dirac fermions as possible dark-matter candidates. Starting with an exhaustive list of operators up to dimension 8, we present detailed calculation of dark-matter annihilations to all possible final states, including gamma gamma, gamma Z, gamma h, ZZ, Zh, W+ W-, hh, and f fbar, and demonstrate the correlations among them. We compute the mass scale of the effective field theory necessary to obtain the correct dark-matter mass density, and well as the resulting photon line signals.

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Cited by 1 Pith paper

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  1. Constraining Effective Field Theories for dark matter candidates annihilating into gamma-ray lines with CTAO

    hep-ph 2025-09 conditional novelty 4.0

    Using CTAO projected line sensitivity, the paper forecasts lower bounds on effective dark matter interaction scales above 10 TeV for TeV mass dark matter, with direct detection dominating the fermionic dipole operator.