Abstract
Gauge fields can be composed as finite-part products of subcanonical fermion fields which involve a mass scale Λ2. At energies of the order Λ the usual particle interpretation breaks down. The consequences of such «gauge fermions» are considered for a Λ of the order of the Planck mass. Gauge invariance determines uniquely the coupling parameters in a theory of self-interacting gauge fermions. Transversal gauge fields arise as bound states of gauge fermions which have mass zero for the symmetric case and which exhibit the Higgs phenomenon for a spontaneously broken symmetry. The breakdown arises by fermion condensation. The mass scale Λ leads to a large renormalization of the basic strong coupling.
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