Abstract

In leptophilic scenarios, dark matter interactions with nuclei, relevant for direct detection experiments and for the capture by celestial objects, could only occur via loop-induced processes. If the mediator is a scalar or pseudo-scalar particle, which only couples to leptons, the dominant contribution to dark matter-nucleus scattering would take place via two-photon exchange with a lepton triangle loop. The corresponding diagrams have been estimated in the literature under different approximations. Here, we present new analytical calculations for one-body two-loop and two-body one-loop interactions. The two-loop form factors are presented in closed analytical form in terms of generalized polylogarithms up to weight four. In both cases, we consider the exact dependence on all the involved scales, and study the dependence on the momentum transfer. We show that some previous approximations fail to correctly predict the scattering cross section by several orders of magnitude. Moreover, we quantitatively show that form factors in the range of momentum transfer relevant for local galactic dark matter, can be significantly smaller than their value at zero momentum transfer, which is the approach usually considered.

Highlights

  • QCD [28], which describes the dynamics of heavy quark-antiquark pairs at energy scales well below their masses, provides accurate predictions for, e.g., the decay rates and binding energies of heavy quarkonia and for top-pair production near threshold in electron-positron annihilation [29, 30]

  • We show the results for target protons, which at these momenta are the relevant degrees of freedom in the scattering of local galactic dark matter (DM) off standard matter, and we depict the partial contributions from the diagrams with the three charged leptons in the triangle loop: e, μ and τ; and the sum of the three contributions

  • We have considered the scattering of dark matter (DM) off standard matter nuclei, within leptophilic scenarios, by considering loop-induced interactions via a scalar and a pseudo-scalar mediator

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Summary

Amplitudes and form factors

We consider the case of a DM particle (χ) that couples to a SM singlet scalar (φS) or pseudo-scalar (φP ), which in turn, couples to SM leptons ( ) at tree level, but not to quarks, through interaction terms of the form. The leading interactions with nucleons are induced by the exchange of two virtual photons. The two virtual photons can scatter off a single nucleon [51, 95] or two nucleons [96, 99], and these two types of processes govern the elastic scattering of a DM particle off a nucleus A, with the total amplitude given by the sum of their individual amplitudes, Mβ = A(p )| L |A(p) = M(β1) + M(β2) ,. With β = {S, P } for scalar or pseudo-scalar interactions. The computation of these contributions is the main goal of this paper and we discuss them

One-body interactions
Two-body interactions
Comparison with previous results and discussion
Conclusions
A Differential equations for one-body interactions
Master integrals for the general kinematic case
Master integrals for the equal-mass case
Soft limit
Equal-mass limit
Soft asymptotic limit
Findings
Full Text
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