Abstract

The WIMPs are considered one of the favorable dark matter (DM) candidates, but as the upper bounds on the interactions between DM and standard model (SM) particles obtained by the upgraded facilities of DM direct detections get lower and lower. Researchers turn their attentions to search for less massive DM candidates, i.e. light dark matter of MeV scale. The recently measured anomalous transition in $^8$Be suggests that there exists a vectorial boson which may mediate the interaction between DM and SM particles. Based on this scenario, we combine the relevant cosmological data to constrain the mass range of DM, and have found that there exists a model parameter space where the requirements are satisfied, a range of $10.4 \lesssim m_{\phi} \lesssim $ 16.7 MeV for scalar DM, and $13.6 \lesssim m_{V} \lesssim $ 16.7 MeV for vectorial DM is demanded. Then a possibility of directly detecting such light DM particles via the DM-electron scattering is briefly studied in this framework.

Highlights

  • The issue concerning dark matter (DM) refers to two aspects, one is the identities of DM, i.e. what is DM, and another aspect is how DM particles interact among themselves and with standard model (SM) particles

  • It is generally believed that the interactions related to the DM sector must be of a new type beyond the standard model (BSM)

  • The MeV scalar and vectorial DM has been studied in this work, with the new boson X indicated by the 8Be anomalous transition being the mediator

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Summary

Introduction

The issue concerning DM refers to two aspects, one is the identities of DM, i.e. what is (are) DM, and another aspect is how DM particles interact among themselves and with SM particles. The vector boson X discussed in Ref. For the scattering between possible scalar, vectorial, and fermionic DM and target nucleus, the spin-independent interaction induced by exchanging the vector boson X is dominant For MeV DM with vector form interaction induced by X , the annihilation of the fermionic DM pair is s-wave dominant, so it is inconsistent with the CMB observation. In this work the search for DM via its scattering with electron will be discussed for our concerned model. After this introduction, we present the concrete forms of interactions between SM and DM with new boson X exchanged, and estimate the DM p-wave annihilation rate. The last section is devoted to a brief conclusion and discussion

Interactions between SM and DM
The couplings
DM annihilations
Scalar DM
Vectorial DM
Analysis on X–DM coupling
DM mass with constraints of Neff
DM–electron scattering
Conclusion and discussion
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