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Higgsless electroweak symmetry breaking from theory space

Roshan Foadi1, Shrihari Gopalakrishna1 and Carl Schmidt1

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We investigate unitarity of W+W scattering in the context of theory space models of the form U(1) × [SU(2)]N × SU(2)N+1, which are broken down to U(1)EM by non-linear Σ fields, without the presence of a physical Higgs Boson. By allowing the couplings of the U(1) and the final SU(2)N+1 to vary, we can fit the W and Z masses, and we find that the coefficient of the term in the amplitude that grows as E2/mW2 at high energies is suppressed by a factor of (N+1)−2. In the N+1→ limit the model becomes a 5-dimensional SU(2) gauge theory defined on an interval, where boundary terms at the two ends of the interval break the SU(2) down to U(1)EM. These boundary terms also modify the Kaluza-Klein (KK) mass spectrum, so that the lightest KK states can be identified as the W and Z bosons. The T parameter, which measures custodial symmetry breaking, is naturally small in these models. Depending on how matter fields are included, the strongest experimental constraints come from precision electroweak limits on the S parameter.


Keywords

Spontaneous Symmetry Breaking

Beyond Standard Model

 

E-print Number: hep-ph/0312324

Cited: by |

Refers: to

PACS

11.30.Qc Spontaneous and radiative symmetry breaking

14.80.Bn Standard-model Higgs bosons

11.30.Ly Other internal and higher symmetries

14.70.Fm W bosons

12.60.Fr Extensions of electroweak Higgs sector

11.15.Ex Spontaneous breaking of gauge symmetries

Subjects

Particle physics and field theory

Dates

Issue 03 (March 2004)

Received 7 January 2004, accepted for publication 17 March 2004

Published 27 March 2004



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