2012/01/03 by Moffat, J. W.
#FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph)
paper · doi:10.48550/arxiv.1201.0736
An electroweak (EW) model has been investigated (Moffat) in which the energy E < μ=√λMW, where λ is a gauge parameter and MW is the W boson mass. For large enough λ the scalar boson mass μ=√λMW can be heavy enough to avoid detection in LHC experiments. The theory is perturbatively renormalizable for the decoupled scalar interactions. The Born approximation tree graph unitarity can be ensured by postulating that the effective coupling constant g\rm eff(s) vanishes as 1/√(s) or faster as s→∞, predicting that the EW interactions become weaker at high energies, and longitudinally polarized WL WL→ WL WL scattering does not violate Born approximation tree graph unitarity.