Abstract

Motivated by the SU(2)CMB modification of the cosmological model ΛCDM, we consider isolated fuzzy-dark-matter lumps, made of ultralight axion particles whose masses arise due to distinct SU(2) Yang–Mills scales and the Planck mass MP. In contrast to SU(2)CMB, these Yang–Mills theories are in confining phases (zero temperature) throughout most of the Universe’s history and associate with the three lepton flavours of the Standard Model of particle physics. As the Universe expands, axionic fuzzy dark matter comprises a three-component fluid which undergoes certain depercolation transitions when dark energy (a global axion condensate) is converted into dark matter. We extract the lightest axion mass ma,e=0.675×10−23 eV from well motivated model fits to observed rotation curves in low-surface-brightness galaxies (SPARC catalogue). Since the virial mass of an isolated lump solely depends on MP and the associated Yang–Mills scale the properties of an e-lump predict those of μ- and τ-lumps. As a result, a typical e-lump virial mass ∼6.3×1010M⊙ suggests that massive compact objects in galactic centers such as Sagittarius A* in the Milky Way are (merged) μ- and τ-lumps. In addition, τ-lumps may constitute globular clusters. SU(2)CMB is always thermalised, and its axion condensate never has depercolated. If the axial anomaly indeed would link leptons with dark matter and the CMB with dark energy then this would demystify the dark Universe through a firmly established feature of particle physics.

Highlights

  • Dark matter was introduced as an explanation for the anomalous, kinematic behavior of luminous test matter in comparison with the gravity exerted by its luminous surroundings, e.g., virialised stars within a galaxy [1] or a virialised galaxy within a cluster of galaxies [2]

  • To determine all parameters of ΛCDM at a high accuracy, cosmological distance scales can be calibrated by high-redshift data, coming from precision observations of the Cosmic Microwave Background (CMB) or from largescale structure surveys probing Baryon Acoustic Oscillations (BAO)

  • Having fixed the scales of SU(2)CMB, SU(2)e and linked their lumps to dark energy and the dark-matter halos of low-surface-brightness galaxies, respectively, we associate the lumps of SU(2) ̄ and SU(2)ø with Ωpdm,0 of the dark-sector cosmological model in Equation (4)

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Summary

Introduction

Dark matter was introduced as an explanation for the anomalous, kinematic behavior of luminous test matter in comparison with the gravity exerted by its luminous surroundings, e.g., virialised stars within a galaxy [1] or a virialised galaxy within a cluster of galaxies [2]. Because these cores were separated in the course of nonthermal depercolation halos of axion particles, correlated due to gravitational virialisation on the scale of their de Broglie wavelength, were formed around the condensates Such a halo reaches out to a radius, say, of r200 where its mass density starts to fall below 200 times the critical cosmological energy density of the spatially flat FLRW Universe. Having fixed the scales of SU(2)CMB , SU(2)e and linked their lumps to dark energy and the dark-matter halos of low-surface-brightness galaxies, respectively, we associate the lumps of SU(2) ̄ and SU(2)ø with Ωpdm,0 of the dark-sector cosmological model in Equation (4).

Analysis of Rotation Curves
Fuzzy Dark Matter
Analysis of RCs in the SNFW Model
Analysis of RCs in the Burkert Model
Galactic Central Regions and the Dark Sector of the Universe
Speculations on Origins of Milky Way’s Structure
Summary and Outlook
Full Text
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