Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 72
... Higgs boson mass is partial - wave unitarity violated in the lowest - order diagrams for W and Z scattering . They found a limit to the Higgs mass ( 11.15 ) MH 8π ν 2 ) 3GF ( 2342 ) , in order to have no violation of tree graph ...
... Higgs boson mass is partial - wave unitarity violated in the lowest - order diagrams for W and Z scattering . They found a limit to the Higgs mass ( 11.15 ) MH 8π ν 2 ) 3GF ( 2342 ) , in order to have no violation of tree graph ...
Page 140
... Higgs mass . There are reasons to believe that in a W + W production process w ° W + W- radiative corrections may become big if both energy and Higgs mass are large with respect to the vector - boson mass . Details have not yet been ...
... Higgs mass . There are reasons to believe that in a W + W production process w ° W + W- radiative corrections may become big if both energy and Higgs mass are large with respect to the vector - boson mass . Details have not yet been ...
Page 141
... Higgs mass cannot be estimated from corrections to the ratio of charged and neutral vector - boson masses . But it happens that very heavy fermions split indeed M. and M。, in a way depending on the mass differences within the fermion ...
... Higgs mass cannot be estimated from corrections to the ratio of charged and neutral vector - boson masses . But it happens that very heavy fermions split indeed M. and M。, in a way depending on the mass differences within the fermion ...
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Common terms and phrases
algebra angle antineutrino Aµ(x background BJORKEN bosons branching ratio Cabibbo calculated CDHS CERN chamber charge charged-current charmed particles colour conservation coupling constant covariant covariant derivative cross-section decay modes define detector diagonal diagram dimuon events discussed distribution doublets electron energy equation experimental experiments FAISSNER fermions field flavour flux function Gargamelle gauge group gauge theories GeV/c gives GLASHOW gluons Goldstone hadron Higgs invariant isospin kaons Lagrangian lepton Lett mass matrix mass term massless MeV/c² momentum muon neutral currents neutral-current neutrino and antineutrino neutrino beam Nucl nucleon observed obtained orthogonal parameters parity violation parton Phys physical pion production proton Q₁ quark mass reactions Rendiconti S.I.F. representation scalar scattering sin² singlets spectrum strong interactions SU₂ symmetry target transformation U₁ vacuum expectation values vacuum vector weak WEINBERG y-distributions zero µ²