Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 206
... distributions ( 1.4 ) is isotropic . The laboratory an- gular distribution clearly is not . As discussed in subsect . 1'3 we can reconstruct the proper Lorentz transformation if we know the neutrino energy and the target mass . The ...
... distributions ( 1.4 ) is isotropic . The laboratory an- gular distribution clearly is not . As discussed in subsect . 1'3 we can reconstruct the proper Lorentz transformation if we know the neutrino energy and the target mass . The ...
Page 432
... distribution . Here the indices correspond to the reactions quoted above . The errors are estimates of the precision ... distribution , while for y decay we get a distribution with dN / dp2 distribution with dN / dp2 = const or dN / dp ...
... distribution . Here the indices correspond to the reactions quoted above . The errors are estimates of the precision ... distribution , while for y decay we get a distribution with dN / dp2 distribution with dN / dp2 = const or dN / dp ...
Page 552
... distributions in different hadrons , the nonvalence distributions are fully determined also . Further , the nonvalence quarks in the pion then have a wider distribution in fractional momentum than those in the nucleon . This picture is ...
... distributions in different hadrons , the nonvalence distributions are fully determined also . Further , the nonvalence quarks in the pion then have a wider distribution in fractional momentum than those in the nucleon . This picture is ...
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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