Abstract

Asymmetric dark matter (ADM) is motivated by the similar cosmological mass densities measured for ordinary and dark matter. We present a comprehensive theory for ADM that addresses the mass density similarity, going beyond the usual ADM explanations of similar number densities. It features an explicit matter-antimatter asymmetry generation mechanism, has one fully worked out thermal history and suggestions for other possibilities, and meets all phenomenological, cosmological and astrophysical constraints. Importantly, it incorporates a deep reason for why the dark matter mass scale is related to the proton mass, a key consideration in ADM models. Our starting point is the idea of mirror matter, which offers an explanation for dark matter by duplicating the standard model with a dark sector related by a $Z_2$ parity symmetry. However, the dark sector need not manifest as a symmetric copy of the standard model in the present day. By utilising the mechanism of "asymmetric symmetry breaking" with two Higgs doublets in each sector, we develop a model of ADM where the mirror symmetry is spontaneously broken, leading to an electroweak scale in the dark sector that is significantly larger than that of the visible sector. The weak sensitivity of the ordinary and dark QCD confinement scales to their respective electroweak scales leads to the necessary connection between the dark matter and proton masses. The dark matter is composed of either dark neutrons or a mixture of dark neutrons and metastable dark hydrogen atoms. Lepton asymmetries are generated by the $CP$-violating decays of heavy Majorana neutrinos in both sectors. These are then converted by sphaleron processes to produce the observed ratio of visible to dark matter in the universe. The dynamics responsible for the kinetic decoupling of the two sectors emerges as an important issue that we only partially solve.

Highlights

  • Cosmological observations have uncovered that the matter content of the standard model is responsible for just 5% of the energy or mass density of the present-day universe

  • The remaining energy density consists of the unknown dark matter (DM) and dark energy components, which according to the latest Planck results make up 27% and 68% respectively [1]

  • Since the evidence for DM comes from cosmological and astrophysical data, and the only confirmed mode of interaction is through gravity, it is common to imagine dark matter as being one or more new particles that constitute a hidden or dark sector which

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Summary

INTRODUCTION

Cosmological observations have uncovered that the matter content of the standard model is responsible for just 5% of the energy or mass density of the present-day universe. Of interest to this work is the idea that the physics of the dark sector can be differentiated from the visible sector yet connected by a mirror symmetry which is spontaneously broken at a higher energy scale.2 This is related to works that posit dark matter as a bound state of a dark sector containing at least a confining SUðNÞ gauge group. We have that the Yukawa couplings that generate masses for fermions in the two sectors are independent of each other while, above the scale of EWSB, the mirror symmetry imposes that any CP violation from the Yukawa Lagrangian will be the same This results in equal lepton asymmetries being created in the visible and dark sectors with rapid sphaleron reprocessing producing almost equal baryon asymmetries in the two sectors.

THE MODEL
Yukawa couplings
ASYMMETRIC SYMMETRY BREAKING
Higgs potentials
Dark confinement
NEUTRINO MASSES
Small cross-sector coupling case
Significant cross-sector coupling case
SYMMETRIC LEPTOGENESIS
Boltzmann equations
Small ρ versus large ρ
Resonant enhancement of CP violation
COSMOLOGICAL HISTORY
Sphaleron reprocessing in the visible and dark sectors
Thermal history
Small ρ case
Thermal decoupling mechanism
Dark big bang nucleosynthesis
Dark matter self-interaction constraints
Findings
CONCLUSION
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