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Matter parity as the origin of scalar Dark Matter

Mario Kadastik, Kristjan Kannike, Martti Raidal

Abstract

We extend the concept of matter parity $P_M=(-1)^{3(B-L)}$ to non-supersymmetric theories and argue that $P_M$ is the natural explanation to the existence of Dark Matter of the Universe. We show that the non-supersymmetric Dark Matter must be contained in scalar 16 representation(s) of $SO(10),$ thus the unique low energy Dark Matter candidates are $P_M$-odd complex scalar singlet(s) $S$ and inert scalar doublet(s) $H_2.$ We have calculated the thermal relic Dark Matter abundance of the model and shown that its minimal form may be testable at LHC via the SM Higgs boson decays $H_1\to DM DM.$ The PAMELA anomaly can be explained with the decays $DM\to νl W$ induced via seesaw-like operator which is additionally suppressed by Planck scale. Because the SM fermions are odd under matter parity too, the DM sector is just our scalar relative.

Matter parity as the origin of scalar Dark Matter

Abstract

We extend the concept of matter parity to non-supersymmetric theories and argue that is the natural explanation to the existence of Dark Matter of the Universe. We show that the non-supersymmetric Dark Matter must be contained in scalar 16 representation(s) of thus the unique low energy Dark Matter candidates are -odd complex scalar singlet(s) and inert scalar doublet(s) We have calculated the thermal relic Dark Matter abundance of the model and shown that its minimal form may be testable at LHC via the SM Higgs boson decays The PAMELA anomaly can be explained with the decays induced via seesaw-like operator which is additionally suppressed by Planck scale. Because the SM fermions are odd under matter parity too, the DM sector is just our scalar relative.

Paper Structure

This paper contains 5 equations, 3 figures.

Figures (3)

  • Figure 1: Allowed $3\sigma$ regions for predominantly singlet DM in $(m_S, \;\lambda_{SH_1})$ plane for $b_S=5$GeV, $m_{H_0}=450$ GeV.
  • Figure 2: Allowed $(m_{H_0},\;\mu_2)$ parameter space for $\mu_{SH}=0$ and different values of $m_S$ represented by the color code.
  • Figure 3: Allowed $3\sigma$ regions in the singlet DM and SM Higgs boson mass plane for $\mu_S=0$ and $b_S=5$ GeV.