Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 23
... define ( 3.25 ) ( M2 ) ij - 2V дрідр = ( M2 ) ; ; introducing the shifted field ( 3.26 ) q ' = q ― v , we can ... definition ( 3.25 ) ( 3.27 ) M2Rav = 0 ( for each x ) . 0 it 6 ) Now we consider the linear space for the algebra , i.e. ...
... define ( 3.25 ) ( M2 ) ij - 2V дрідр = ( M2 ) ; ; introducing the shifted field ( 3.26 ) q ' = q ― v , we can ... definition ( 3.25 ) ( 3.27 ) M2Rav = 0 ( for each x ) . 0 it 6 ) Now we consider the linear space for the algebra , i.e. ...
Page 34
... defines the following functional ( 5.3 ) F ( 0 ( x ) ) = ( v , O ( x ) q ( x ) ) , 0 ( x ) OT ( x ) = 1 , which for fixed x is a function defined over the compact space of group para- meters . Let us require ( 5.4 ) SF ( 0 ( x ) ) = 0 ...
... defines the following functional ( 5.3 ) F ( 0 ( x ) ) = ( v , O ( x ) q ( x ) ) , 0 ( x ) OT ( x ) = 1 , which for fixed x is a function defined over the compact space of group para- meters . Let us require ( 5.4 ) SF ( 0 ( x ) ) = 0 ...
Page 508
... definition of ( Q ) will exclude from the summation , besides light neutrinos , contributions from the elastic process ... defined from the as- signements of Q ,, ( I'1 ) ,, ( I ' ) , and from sin 0 , where 0 is the Weinberg angle [ 2 ] ...
... definition of ( Q ) will exclude from the summation , besides light neutrinos , contributions from the elastic process ... defined from the as- signements of Q ,, ( I'1 ) ,, ( I ' ) , and from sin 0 , where 0 is the Weinberg angle [ 2 ] ...
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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