Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 72
... limit ( 11.15 ) and also from the marginally allowed limit G < 10-5G . Thus , for instance , di- rectly from ( 11.19 ) , for a Higgs mass ~ 102 GeV and m 。. ~ 1 GeV one would get G / G ~ 10-4 , which gives too much K - K mass ...
... limit ( 11.15 ) and also from the marginally allowed limit G < 10-5G . Thus , for instance , di- rectly from ( 11.19 ) , for a Higgs mass ~ 102 GeV and m 。. ~ 1 GeV one would get G / G ~ 10-4 , which gives too much K - K mass ...
Page 119
... limit on A ( meaning a limit below 1000 GeV ) , due to the fact that the currents satisfy an algebra , more particularly also the existence of charm . Nevertheless , a limit can be obtained , and we will discuss this in detail . This ...
... limit on A ( meaning a limit below 1000 GeV ) , due to the fact that the currents satisfy an algebra , more particularly also the existence of charm . Nevertheless , a limit can be obtained , and we will discuss this in detail . This ...
Page 368
... limit 0 the QCD Lagrangian is invariant under the symmetry group M SUSU of chiral transformations . In order to understand the approx- imate SUSUR invariance of the observed strong interactions , we have to suppose that the real world ...
... limit 0 the QCD Lagrangian is invariant under the symmetry group M SUSU of chiral transformations . In order to understand the approx- imate SUSUR invariance of the observed strong interactions , we have to suppose that the real world ...
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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