Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 96
... strong and weak interactions is that of CP conservation by strong interactions . The discussion assumes also a gauge group for strong interactions , precisely colour SU ,, giving rise to QCD ( quantumchromodynamics ) . Such non ...
... strong and weak interactions is that of CP conservation by strong interactions . The discussion assumes also a gauge group for strong interactions , precisely colour SU ,, giving rise to QCD ( quantumchromodynamics ) . Such non ...
Page 141
... strong inter- action with the Higgs boson . iv ) A strong interaction for such heavy fermions can be avoided if left and right - handed multiplets are in the same representation . This implies pure vector coupling to the vector bosons ...
... strong inter- action with the Higgs boson . iv ) A strong interaction for such heavy fermions can be avoided if left and right - handed multiplets are in the same representation . This implies pure vector coupling to the vector bosons ...
Page 368
... strong interactions . - It is well known that the strong interactions are approximately invariant under the symmetry groups SU ,, SUA , ... , SU 2L - SU2R , SU3L SUзR ) ...... .. In the limit 0 the QCD Lagrangian is invariant under the ...
... strong interactions . - It is well known that the strong interactions are approximately invariant under the symmetry groups SU ,, SUA , ... , SU 2L - SU2R , SU3L SUзR ) ...... .. In the limit 0 the QCD Lagrangian is invariant under the ...
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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