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Relic density of Dark Matter in the Inert Doublet Model beyond Leading Order. I) The Heavy Mass Case

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arxiv 1906.11269 v3 pith:7YXNSPTW submitted 2019-06-26 hep-ph hep-ex

classification hep-phhep-ex
keywords densityone-looprelicdarkcaseco-annihilationcorrectionsdoublet
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

A full renormalisation of the Inert Doublet Model (IDM) is presented and exploited for a precise calculation of the relic density of Dark Matter (DM) at one-loop. In this first paper, we study the case of a DM candidate with $m_{\rm DM} \sim 500$ GeV. In this regime, the co-annihilation channels are important. We therefore compute, for a wide range of relative velocities, the full next-to-leading order electroweak corrections to 7 annihilation/co-annihilation processes that contribute $\sim$ 70\% to the relic density of DM. These corrected cross-sections are interfaced with {\tt micrOMEGAs} to obtain the one-loop correction to the freeze-out relic density. Due to the accurate measurement of this observable, the one-loop corrections are relevant. We discuss the one-loop renormalisation scheme dependence and point out the influence, at one-loop, of a parameter that solely describes the scattering in the dark sector. A tree-level computation of the relic density is not sensitive to this parameter.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Full Next-To Leading-Order Electroweak and QCD Corrections to the Relic Density in the CxSM

    hep-ph 2026-07 conditional novelty 6.0 of 10

    NLO QCD and electroweak corrections to the CxSM dark-matter relic density are computed and released in the public code RelExt@NLO; the corrections shift the allowed parameter region in both directions.

  2. The effects of a scalar singlet Leptoquark at the $Z$ factory

    hep-ph 2026-03 conditional novelty 5.0 of 10

    A scalar singlet leptoquark that explains B-meson anomalies produces a ~0.7% decrease in Z→τ+τ−, which future Z-factory measurements could detect, while Z→μ+μ− is essentially unchanged.

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