Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 381
... particles are stable . They can only decay if violations of the Cabibbo structure exist . Since these must be small , the weak decays of t- and b - flavoured particles into particles composed of u , d , s and c quarks will not proceed ...
... particles are stable . They can only decay if violations of the Cabibbo structure exist . Since these must be small , the weak decays of t- and b - flavoured particles into particles composed of u , d , s and c quarks will not proceed ...
Page 477
... particles . DASP has studied the semi - leptonic decays of charmed particles by an- alysing inclusive electron events . Events of this type can come from the decay of charmed particles , but also from a variety of other sources ...
... particles . DASP has studied the semi - leptonic decays of charmed particles by an- alysing inclusive electron events . Events of this type can come from the decay of charmed particles , but also from a variety of other sources ...
Page 487
... particles had been produced together with e and u . Since the detector covered only two thirds of 47 , additionally produced particles had a fair chance to escape detection . Besides the experimental uncertainties there was the question ...
... particles had been produced together with e and u . Since the detector covered only two thirds of 47 , additionally produced particles had a fair chance to escape detection . Besides the experimental uncertainties there was the question ...
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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