Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 19
... gauge theories full Lorentz invariance is still maintained by adding to the r.h.s. of eq . ( 2.12 ) a term pro- portional to a constant timelike four ... THEORY 19 A classical description of spontaneous symmetry breaking Gauge theories.
... gauge theories full Lorentz invariance is still maintained by adding to the r.h.s. of eq . ( 2.12 ) a term pro- portional to a constant timelike four ... THEORY 19 A classical description of spontaneous symmetry breaking Gauge theories.
Page 132
... Gauge theories . We have seen that at low energies the weak interactions are well described by a four - fermion current current theory . However , this theory , being unrenormalizable , cannot be the complete field theory . What can we ...
... Gauge theories . We have seen that at low energies the weak interactions are well described by a four - fermion current current theory . However , this theory , being unrenormalizable , cannot be the complete field theory . What can we ...
Page 351
... gauge theories have turned out to be of crucial impor- tance for the understanding of all interactions . We have confidence that the electromagnetic and weak interactions are described by a system of non - Abelian gauge fields . The ...
... gauge theories have turned out to be of crucial impor- tance for the understanding of all interactions . We have confidence that the electromagnetic and weak interactions are described by a system of non - Abelian gauge fields . 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