Abstract
So far all evidences of dark matter (DM) come from astrophysical and cosmological observations, due to the gravitational interactions of DM. It is possible that the true DM particle in the universe joins gravitational interactions only, but nothing else. Such a Gravitational DM (GDM) may act as a weakly interacting massive particle (WIMP), which is conceptually simple and attractive. In this work, we explore this direction by constructing the simplest scalar GDM particle χs. It is a ℤ2 odd singlet under the standard model (SM) gauge group, and naturally joins the unique dimension-4 interaction with Ricci curvature, ξsχs2ℛ, where ξs is the dimensionless nonminimal coupling. We demonstrate that this gravitational interaction ξsχs2ℛ, together with Higgs-curvature nonminimal coupling term ξhH†Hℛ, induces effective couplings between χs2 and SM fields, and can account for the observed DM thermal relic abundance. We analyze the annihilation cross sections of GDM particles and derive the viable parameter space for realizing the DM thermal relic density. We further study the direct/indirect detections and the collider signatures of such a scalar GDM. These turn out to be highly predictive and testable.
Highlights
Where ξs is the corresponding dimensionless nonminimal coupling
Since the same cubic vertex φχsχs determines both the Higgs invisible decays and the Gravitational DM (GDM) thermal relic abundance, we find that the LHC bound on
We presented a minimal construction of such a gravitational dark matter (GDM), where a scalar GDM particle χs couples to the standard model (SM) through the unique dimension-4 operator (1.1) which contains the fields χ2s and Ricci curvature R
Summary
We present the formulation of the scalar GDM χs and derive its induced interactions with the SM particles. We first consider the GDM in Jordan frame, where the nonminimal coupling (1.1) is manifest. We make the Weyl transformation on the metric and convert the action into Einstein frame, in which the nonminimal term (1.1) is fully transformed away and result in a new set of effective operators. We will systematically derive the relevant Feynman vertices for χs in Einstein frame
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