An alternative view on the electroweak interactions
arXiv:1008.3780 · doi:10.1142/S0217751X11053699
Abstract
We discuss an alternative to the Higgs mechanism which leads to gauge invariant masses for the electroweak bosons. The key idea is to reformulate the gauge invariance principle which, instead of being applied as usual at the level of the action, is applied at the level of the quantum fields. In other words, we define gauge invariant quantum fields which are used to build the action. In that framework, the Higgs field is not necessarily a physical degree of freedom but can merely be a dressing field that does not propagate. If the Higgs boson is not propagating, the weak interactions must become strongly coupled below 1 TeV and have a non-trivial fixed point and would thus be renormalizable at the non-perturbative level. On the other hand, if a gauge invariant Higgs boson is introduced in the model, its couplings to the fermions and the electroweak bosons can be quite different from those expected in the standard model.
10 pages
References in corpus (17)
- A Stueckelberg Extension of the Standard Model
- Constituent Quarks from QCD
- Invariant Mass Distribution of Jet Pairs Produced in Association with a W boson in ppbar Collisions at sqrt(s) = 1.96 TeV
- Charges from Dressed Matter: Construction
- Scales of Fermion Mass Generation and Electroweak Symmetry Breaking
- One loop beta functions and fixed points in Higher Derivative Sigma Models
- Scale of fermion mass generation
- Upper bound on the scale of Majorana-neutrino mass generation
- Symmetry breaking, conformal geometry and gauge invariance
- Scales of Mass Generation for Quarks, Leptons and Majorana Neutrinos
- The Electroweak Interactions as a Confinement Phenomenon
- The electroweak chiral Lagrangian reanalyzed
- Effective Theory for Dark Matter and a New Force in the Dark Matter Sector
- The Higgs Boson Might Not Couple To B Quarks
- Invisible Higgs boson, continuous mass fields and unHiggs mechanism
- Calculation of the Higgs Boson Mass Using the Complementarity Principle
- Hidden Supersymmetry