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AbstractAbstract
[en] A wide class of neutrino physics motivated models are characterized by the spontaneous violation of a global U(1) lepton number symmetry at or below the electroweak scale by an SU(2)xU(1) singlet vacuum expectation value <σ>< or ∼O(1) TeV. In all these models the main Higgs decay channel is likely to be 'invisible', e.g. h→JJ, where J denotes the associated weakly interacting pseudoscalar Goldstone boson - the majoron. This leads to events with large missing energy that could be observable at LEP and affect the Higgs mass bounds obtained, as well as lead to novel ways to search for Higgs bosons and high-energy supercolliders such as the LHC/SSC. (orig.)
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ANNIHILATION, BRANCHING RATIO, ELECTRON-POSITRON INTERACTIONS, FEYNMAN DIAGRAM, HIGGS BOSONS, HIGGS MODEL, LAGRANGIAN FIELD THEORY, LEPTON NUMBER, MAJORANA THEORY, NEUTRINOS, PAIR PRODUCTION, PARTICLE WIDTHS, POTENTIALS, QUANTUM FLAVORDYNAMICS, QUANTUM NUMBERS, REST MASS, SU-2 GROUPS, SYMMETRY BREAKING, U-1 GROUPS, WEAK HADRONIC DECAY, WEAK PARTICLE DECAY, WEINBERG LEPTON MODEL
DECAY, DIAGRAMS, ELEMENTARY PARTICLES, FERMIONS, FIELD THEORIES, INFORMATION, INTERACTIONS, LEPTON-LEPTON INTERACTIONS, LEPTONS, LIE GROUPS, MASS, MASSLESS PARTICLES, MATHEMATICAL MODELS, PARTICLE DECAY, PARTICLE INTERACTIONS, PARTICLE MODELS, PARTICLE PRODUCTION, PARTICLE PROPERTIES, POSTULATED PARTICLES, QUANTUM FIELD THEORY, SU GROUPS, SYMMETRY GROUPS, U GROUPS, UNIFIED GAUGE MODELS
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