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AbstractAbstract
[en] We investigate the fermions of the standard model without a Higgs scalar. Instead, we consider a nonlocal four-quark interaction in the tensor channel which is characterized by a single dimensionless coupling f. Quantization leads to a consistent perturbative expansion for small f. The running of f is asymptotically free and therefore induces a nonperturbative scale Λch, in analogy to the strong interactions. We argue that spontaneous electroweak symmetry breaking is triggered at a scale where f grows large and find the top quark mass of the order of Λch. We also present a first estimate of the effective Yukawa coupling of a composite Higgs scalar to the top quark, as well as the associated mass ratio between the top quark and the W boson.
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(c) 2010 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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BASIC INTERACTIONS, BOSONS, ELEMENTARY PARTICLES, FERMIONS, FIELD THEORIES, GRAND UNIFIED THEORY, INTERACTIONS, INTERMEDIATE BOSONS, INTERMEDIATE VECTOR BOSONS, MATHEMATICAL MODELS, NUCLEAR POTENTIAL, PARTICLE MODELS, POSTULATED PARTICLES, POTENTIALS, QUANTUM FIELD THEORY, QUARKS, TOP PARTICLES, UNIFIED GAUGE MODELS, WEAK INTERACTIONS
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