Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
From inside the book
Results 1-3 of 49
Page 136
... consider the interaction term { gMZB2 = { gMZ { ( B1 ) 2 + ( B2 ) 2 + ( 1 / c2 ) ( W ° ) 2 } . For example , this implies the vertex M Z mmmm g C = cos 0 . A self - energy diagram arising from this is WH w H This diagram involves a ...
... consider the interaction term { gMZB2 = { gMZ { ( B1 ) 2 + ( B2 ) 2 + ( 1 / c2 ) ( W ° ) 2 } . For example , this implies the vertex M Z mmmm g C = cos 0 . A self - energy diagram arising from this is WH w H This diagram involves a ...
Page 137
... consider the vertex Z2 B2 Wo X < 113 It gives rise to the self - energy diagram 0 n- M2 / c2 is produced . W + 1 which is quadratic in the Z mass m . But again , the W ° correction has a factor 1 / c2 and no deviation is produced . = W ...
... consider the vertex Z2 B2 Wo X < 113 It gives rise to the self - energy diagram 0 n- M2 / c2 is produced . W + 1 which is quadratic in the Z mass m . But again , the W ° correction has a factor 1 / c2 and no deviation is produced . = W ...
Page 416
... consider the absence of any such signal a clear indication that the D ° does not get produced below a threshold energy E. Thus E > 3.1 GeV , if we consider production th th via an intermediate photon . If we also consider direct 416 G ...
... consider the absence of any such signal a clear indication that the D ° does not get produced below a threshold energy E. Thus E > 3.1 GeV , if we consider production th th via an intermediate photon . If we also consider direct 416 G ...
Other editions - View all
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