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Chiral Fermion Delocalization in Deconstructed Higgsless Theories
High Energy Physics - Phenomenology · Submitted 1 Aug 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim {I construct a renormalizable $SU(2)^{89}\times U(1)$ gauge theory with standard-model-like phenomenology for the gauge bosons masses and the weak interactions of the light fermions (including the $b$) but in which all vacuum expectation values are about 2 TeV.
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The abstract, sentence by sentence
{I construct a renormalizable $SU(2)^{89}\times U(1)$ gauge theory with standard-model-like phenomenology for the gauge bosons masses and the weak interactions of the light fermions (including the $b$) but in which all vacuum expectation values are about 2 TeV. This is a deconstructed version of a Higgsless model with a flat extra dimension. The fermions are delocalized on the theory space in an unusual way, with LH and RD fermions on alternate nodes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | {I construct a renormalizable $SU(2)^{89}\times U(1)$ gauge theory with standard-model-like phenomenology for the gauge bosons masses and the weak interactions of the light fermions (including the $b$) but in which all vacuum expectation values are about 2 TeV. | contribution 0.99 | 0.95 | 0.20 | asserted 1.00 |
| s1 | This is a deconstructed version of a Higgsless model with a flat extra dimension. | method 0.39 | 0.52 | 0.09 | asserted 1.00 |
| s2 | The fermions are delocalized on the theory space in an unusual way, with LH and RD fermions on alternate nodes. | contribution 0.49 | 0.84 | 0.21 | asserted 1.00 |
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Original abstract
{I construct a renormalizable $SU(2)^{89}\times U(1)$ gauge theory with standard-model-like phenomenology for the gauge bosons masses and the weak interactions of the light fermions (including the $b$) but in which all vacuum expectation values are about 2 TeV. This is a deconstructed version of a Higgsless model with a flat extra dimension. The fermions are delocalized on the theory space in an unusual way, with LH and RD fermions on alternate nodes.
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