Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 43
... corresponding to the eigen- value g2 + g'2 , while A corresponds to the eigenvalue zero : eigenvalue 0 eigenvector 1 √g2 + g'a ( gB + g ' A3 ) = A , 1 g2 + g'a - ( g ' B — gA3 ) = 2 . √g2 + g'2 2 The field A has clearly to be ...
... corresponding to the eigen- value g2 + g'2 , while A corresponds to the eigenvalue zero : eigenvalue 0 eigenvector 1 √g2 + g'a ( gB + g ' A3 ) = A , 1 g2 + g'a - ( g ' B — gA3 ) = 2 . √g2 + g'2 2 The field A has clearly to be ...
Page 84
... correspond to the remaining neutral generators of G. We then have the following proposition 1 . Proposition 1. The matrix μmn = undefined above has an inverse . μmn Proof . Let us suppose that has one eigenvector q corresponding to the ...
... correspond to the remaining neutral generators of G. We then have the following proposition 1 . Proposition 1. The matrix μmn = undefined above has an inverse . μmn Proof . Let us suppose that has one eigenvector q corresponding to the ...
Page 88
M. Baldo Ceolin, Società italiana di fisica. into a corresponding vector ( 14.45 ) [ W ] where the fields of V are such that the submatrix { c } , limited to the values of corresponding to the indices of V ( we call them 1 , l ...
M. Baldo Ceolin, Società italiana di fisica. into a corresponding vector ( 14.45 ) [ W ] where the fields of V are such that the submatrix { c } , limited to the values of corresponding to the indices of V ( we call them 1 , l ...
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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