Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 238
... energy is ob- viously very fundamental because it must tell something about the nature of the weak interaction and the structure of the nucleon . The first work to be done on this subject was started at CERN in 1963 using heavy - liquid ...
... energy is ob- viously very fundamental because it must tell something about the nature of the weak interaction and the structure of the nucleon . The first work to be done on this subject was started at CERN in 1963 using heavy - liquid ...
Page 243
... energy vs. radius from the beam axis . R ( cm ) 200 150 100 50 a ) b ) 0 50 100 150 200 0 50 100 150 200 E ( GeV ) - Fig . 3. Scatter plots of visible energy of events ... energy corrected THE STUDY OF HIGH - ENERGY NEUTRINO PHYSICS ETC. 243.
... energy vs. radius from the beam axis . R ( cm ) 200 150 100 50 a ) b ) 0 50 100 150 200 0 50 100 150 200 E ( GeV ) - Fig . 3. Scatter plots of visible energy of events ... energy corrected THE STUDY OF HIGH - ENERGY NEUTRINO PHYSICS ETC. 243.
Page 301
... energy of the right - sign muon ( or of the leading muon for like - sign events ) , energy of the « other » muon , ( PvP ) x = 2M ( E + Eu , ) H 2Eu , Eobs Sin2 ( 0μ ‚ / 2 ) M ( Ex + Eu2 ) με ( Eobs H με Еμ + Eμ , + Eμ ‚ ‹ E , ) , h En ...
... energy of the right - sign muon ( or of the leading muon for like - sign events ) , energy of the « other » muon , ( PvP ) x = 2M ( E + Eu , ) H 2Eu , Eobs Sin2 ( 0μ ‚ / 2 ) M ( Ex + Eu2 ) με ( Eobs H με Еμ + Eμ , + Eμ ‚ ‹ E , ) , h En ...
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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