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• W2091251102 endingPage "1543" @default.
• W2091251102 startingPage "1530" @default.
• W2091251102 abstract "If the electroweak symmetry-breaking sector becomes strong at energies above 1 TeV as a result of the absence of a low-mass Higgs boson, and if only the minimal complement of Higgs particles is present, one expects an isovector spin-1 meson of mass 2 TeV/${c}^{2}$, and width 400 GeV, decaying mostly to ${W}^{ifmmodepmelsetextpmfi{}}$Z or ${W}^{+}$${W}^{mathrm{ensuremath{-}}}$, on very general grounds. Thus, if longitudinal W's and Z's and Higgs bosons are actually fermion-antifermion composites, one must study systems other than this heavy vector meson to learn the nature of the constituents. The role in such studies played by the corresponding spin-1 isoscalar meson, also expected to have a mass of ensuremath{approxeq}2 TeV/${c}^{2}$, is examined, and compared with the corresponding role played by the ensuremath{omega} in hadron physics." @default.
• W2091251102 created "2016-06-24" @default.
• W2091251102 creator A5024488855 @default.
• W2091251102 creator A5031574184 @default.
• W2091251102 date "1988-09-01" @default.
• W2091251102 modified "2023-09-24" @default.
• W2091251102 title "Substructure of the strongly interacting Higgs sector" @default.
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