Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 36
... bosons is = g2 ( v , La Lov ) . 4 ) Goldstone bosons have disappeared . They have been « incorporated » in the new massive gauge fields , since , as can be seen in the case of weak fields , the new A is Aμ + SAμ : μ ( 5.16 ) μ SAμ ...
... bosons is = g2 ( v , La Lov ) . 4 ) Goldstone bosons have disappeared . They have been « incorporated » in the new massive gauge fields , since , as can be seen in the case of weak fields , the new A is Aμ + SAμ : μ ( 5.16 ) μ SAμ ...
Page 133
... bosons W ± and W ° with masses M. and M , coupled to the currents in the required gauge fashion with a coupling constant g ; ii ) couplings among these vector bosons themselves according to the gauge prescription , involving the same ...
... bosons W ± and W ° with masses M. and M , coupled to the currents in the required gauge fashion with a coupling constant g ; ii ) couplings among these vector bosons themselves according to the gauge prescription , involving the same ...
Page 141
... bosons . v ) If the Higgs bosons are very heavy also strong interactions arise . vi ) Breakdown of -e universality may be a probe for Higgs bosons inside hadrons . vii ) Lepton - neutrino pairs , left - handed , coupled just like e - v ...
... bosons . v ) If the Higgs bosons are very heavy also strong interactions arise . vi ) Breakdown of -e universality may be a probe for Higgs bosons inside hadrons . vii ) Lepton - neutrino pairs , left - handed , coupled just like e - v ...
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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