Abstract

In this work we study the possibility that dark matter fields transform in the $(1,0)\oplus(0,1)$ representation of the Homogeneous Lorentz Group. In an effective theory approach, we study the lowest dimension interacting terms of dark matter with standard model fields, assuming that dark matter fields transform as singlets under the standard model gauge group. There are three dimension-four operators, two of them yielding a Higgs portal to dark matter. The third operator couple the photon and $Z^0$ fields to the higher multipoles of dark matter, yielding a \textit{spin portal} to dark matter. For dark matter ($D$) mass below a half of the $Z^0$ mass, the decays $Z^0\to \bar{D} D$ and $H\to \bar{D}D$ are kinematically allowed and contribute to the invisible widths of the $Z^0$ and $H$. We calculate these decays and use experimental results on these invisible widths to constrain the values of the low energy constants finding in general that effects of the spin portal can be more important that those of the Higgs portal. We calculate the dark matter relic density in our formalism, use the constraints on the low energy constants from the $Z^0$ and $H$ invisible widths and compare our results with the measured relic density, finding that dark matter with a $(1,0)\oplus(0,1)$ space-time structure must have a mass $M>43 ~ GeV$.

Highlights

  • The elucidation of the nature of dark matter is one of the most important problems in high energy physics [1]

  • Indirectly detect dark matter particles, based mainly in the WIMP paradigm [4]. The latter is based on the fact that the proper description of the measured dark matter relic density, ΩeDxMp h2 1⁄4 0.1186 Æ 0.0020 [3,5], requires dark matter to have annihilation cross sections into standard model particles of the order of those produced by the weak interactions

  • For spin-one matter fields with a dark gauge group Uð1ÞD, the lowest-dimension operators transforming as standard model and dark gauge group singlets are of the form ψ Oψ where O is one of the 36 matrix operators in the covariant basis f1; χ; Sμν; χSμν; Mμν; Cμναβg

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Summary

INTRODUCTION

The elucidation of the nature of dark matter is one of the most important problems in high energy physics [1]. Indirectly detect dark matter particles, based mainly in the WIMP paradigm [4] The latter is based on the fact that the proper description of the measured dark matter relic density, ΩeDxMp h2 1⁄4 0.1186 Æ 0.0020 [3,5], requires dark matter to have annihilation cross sections into standard model particles of the order of those produced by the weak interactions. In order to solve the constraints, we need to know the algebraic structure of a covariant basis for the operators acting in the ð1; 0Þ ⊕ ð0; 1Þ representation space, which was previously worked out in [38] This basis naturally contains a chirality operator, χ, and spin-one matter fields can be decomposed into chiral components transforming in the (1,0) (right) and (0,1) (left) representations. VIII and close with an Appendix with the required trace calculations for operators in the ð1; 0Þ ⊕ ð0; 1Þ representation space

QUANTUM FIELD THEORY FOR SPIN-ONE MATTER FIELDS
DARK MATTER AS SPIN-ONE MATTER FIELDS
LIGHT DARK MATTER
D DÞ g2t S2W 24πM4
Boltzman equation
Annihilation of dark matter into a fermion-antifermion pair
Dark matter annihilation into two photons
Dark matter relic density
Y ðxf Þ þ sffiffiffiffiffiffiffiffiffiffiffiffiffi 90
DARK MATTER WITH A HIGHER MASS
DIRECT DETECTION OF DARK MATTER
VIII. CONCLUSIONS

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