Quantum Haplodynamics, Dark Matter and Dark Energy
arXiv:1402.4106 · doi:10.1155/2014/361587
Abstract
In quantum haplodynamics (QHD) the weak bosons, quarks and leptons are bound states of fundamental constituents, denoted as haplons. The confinement scale of the associated gauge group SU(2)_h is of the order of TeV. One scalar state has zero haplon number and is the resonance observed at the LHC. In addition, there exist new bound states of haplons with no counterpart in the SM, having a mass of the order of 0.5 TeV up to a few TeV. In particular, a neutral scalar state with haplon number 4 is stable and can provide the dark matter in the universe. The QHD, QCD and QED couplings can unify at the Planck scale. If this scale changes slowly with cosmic time, all of the fundamental couplings, the masses of the nucleons and of the DM particles, including the cosmological term (or vacuum energy density), will evolve with time. This could explain the dark energy of the universe.
Version accepted for publication in Advances in High Energy Physics. Extended discussion and references added
References in corpus (5)
- Dynamics of dark energy
- First results from the LUX dark matter experiment at the Sanford Underground Research Facility
- Dark energy: a quantum fossil from the inflationary Universe?
- Hubble expansion and structure formation in the "running FLRW model" of the cosmic evolution
- Constraining the Variation in Fine-Structure Constant Using SDSS DR8 QSO Spectra
Cited by in corpus (9)
- Dynamical vacuum energy in the expanding Universe confronted with observations: a dedicated study
- The cosmology: from inflation to dark energy through running
- Cosmological constant vis-a-vis dynamical vacuum: bold challenging the CDM
- Nonsingular Decaying Vacuum Cosmology and Entropy Production
- Fundamental constants and cosmic vacuum: the micro and macro connection
- Higgs potential from extended Brans-Dicke theory and the time-evolution of the fundamental constants
- Baryogenesis from leptomesons
- Dark Energy and the Time Dependence of Fundamental Particle Constants
- Excited lepton baryogenesis