Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 245
... assuming o3 / σ = / σn 2. Errors shown are statistical ( see also table I ) . v : o Gargamelle , ⚫ BEBC ( this experiment ) ; v : △ Gargamelle , △ BEBC ( this experiment ) ; □ BEBC from muon spectrum . = average cross - section , in ...
... assuming o3 / σ = / σn 2. Errors shown are statistical ( see also table I ) . v : o Gargamelle , ⚫ BEBC ( this experiment ) ; v : △ Gargamelle , △ BEBC ( this experiment ) ; □ BEBC from muon spectrum . = average cross - section , in ...
Page 281
... assuming Bjorken scaling and neglecting the intermediate- boson propagator , we have the double differential cross - section for scattering of v ( ) on protons or neutrons : ( 6 ) dov , dx dy = G2 ME π y2 [ F ( x ) ( 1 − y ) + 22 2 x ...
... assuming Bjorken scaling and neglecting the intermediate- boson propagator , we have the double differential cross - section for scattering of v ( ) on protons or neutrons : ( 6 ) dov , dx dy = G2 ME π y2 [ F ( x ) ( 1 − y ) + 22 2 x ...
Page 483
... assuming the semi - leptonic decays Dev , DevK and DevK * ( 892 ) , with a V - A coupling for the weak current . Theoretical electron spectra [ 34 , 35 ] for the decay of D's at rest were taken from a paper of Ali and Yang [ 34 ] . Note ...
... assuming the semi - leptonic decays Dev , DevK and DevK * ( 892 ) , with a V - A coupling for the weak current . Theoretical electron spectra [ 34 , 35 ] for the decay of D's at rest were taken from a paper of Ali and Yang [ 34 ] . Note ...
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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