2005 CERN-CLAF School of High-Energy Physics: Malargüe, Argentina, 27 February-12 March 2005 : Proceedings, Issue 15Nick Ellis |
From inside the book
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Page 38
... symmetry at the quantum level . Since the charges are conserved they must commute with the Hamiltonian : [ Qo , H ] = 0 . - ( 230 ) There are several possibilities in the quantum mechanical realization of a symmetry . Wigner - Weyl ...
... symmetry at the quantum level . Since the charges are conserved they must commute with the Hamiltonian : [ Qo , H ] = 0 . - ( 230 ) There are several possibilities in the quantum mechanical realization of a symmetry . Wigner - Weyl ...
Page 41
... symmetry group , it seems that the fact that we are expanding around a particular vacuum expectation value of the scalar field has resulted in a loss of symmetry . This is , however , not the case . The full quantum theory is symmetric ...
... symmetry group , it seems that the fact that we are expanding around a particular vacuum expectation value of the scalar field has resulted in a loss of symmetry . This is , however , not the case . The full quantum theory is symmetric ...
Page 72
... symmetry , and in particular gauge symmetry . The Lagrangian of the Standard Model can be written just including all possible renormalizable terms ( i.e. , with canonical dimension smaller than or equal to 4 ) compatible with the gauge ...
... symmetry , and in particular gauge symmetry . The Lagrangian of the Standard Model can be written just including all possible renormalizable terms ( i.e. , with canonical dimension smaller than or equal to 4 ) compatible with the gauge ...
Contents
Introduction to QCD in hadronic collisions | 81 |
CP violation in meson decays | 131 |
Experimental aspects of cosmic rays | 177 |
Copyright | |
4 other sections not shown
Common terms and phrases
air showers amplitude angle anomaly Auger Observatory bosons calculation calorimeter charged particles Cherenkov collisions colour constraints contribution cosmic rays coupling constant CP violation cross-section dead-time decays defined density depends detector diagram Dirac effect electric field electromagnetic electrons emission energy equation event example experimental fermions flavour fluorescence gauge group gauge invariance gauge transformations given gluon hadronic Hamiltonian high-energy integral interaction ionization Lagrangian lepton Lett Lorentz LVL1 trigger magnetic field mass massless matrix measurements meson momentum muons neutrinos non-Abelian Nucl observables operators pair parameters parton perturbation phase photon Phys physics Pierre Auger Observatory potential processes quantization quantum field theory quark radiation readout renormalization representation result scalar field scale shown in Fig signal spinor Standard Model supersymmetric symmetry T/DAQ Tevatron vacuum vector Xmax