Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 312
M. Baldo Ceolin, Società italiana di fisica. - Unlike the charged current which seems to have pure V A coupling , the right- handed contribution to the neutral currents g may be composed of i ) V— A ... charged-current cross- section ratio.
M. Baldo Ceolin, Società italiana di fisica. - Unlike the charged current which seems to have pure V A coupling , the right- handed contribution to the neutral currents g may be composed of i ) V— A ... charged-current cross- section ratio.
Page 315
... current events . The hadron energy distri- butions of neutral- and charged - current events in different radial ( energy ) intervals are shown in fig . 33a ) and b ) for neutrino and antineutrino , respec- tively . To avoid a direct ...
... current events . The hadron energy distri- butions of neutral- and charged - current events in different radial ( energy ) intervals are shown in fig . 33a ) and b ) for neutrino and antineutrino , respec- tively . To avoid a direct ...
Page 375
... current is consistent with the form c ( - d sin 0 ̧ + s cos 0 ̧ ) , which is obtained if one introduces a second SU2 ... charged current entering in the effective weak Hamiltonian cannot be less than of its conventional strength given by ...
... current is consistent with the form c ( - d sin 0 ̧ + s cos 0 ̧ ) , which is obtained if one introduces a second SU2 ... charged current entering in the effective weak Hamiltonian cannot be less than of its conventional strength given by ...
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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