目录 Preface Acknowledgements Notational conventions Note added in proof: the discovery of the top quark (?) Note added in proof: the demise of the SSC 1 Field theory and pre-gauge theory of weak interactions 1.1 A brief introduction to field theory 1.2 Pre-gange theory of weak interactions 1.3 The spin and isospin structure 1.4 Tests of the V-A structure and 'lepton universality' 2 The need for a gauge theory 2.1 The intermediate vector boson 2.2 Towards a renormalizable theory 2.3 Gauge symmetry 2.4 Freedom to choose the gauge 2.5 Summary 3 Spontaneous symmetry breaking: the Goldstone theorem and the Higgs phenomenon 3.1 Spontaneously broken symmetries in field theory: Goldstone's theorem 3.2 The Higgs mechanism 3.3 Unitarity and renormalizability 3.4 Suwmmary 4 Construction of the standard model 4.1 Model building (towards the standard model) 4.2 The standard model 4.3 Discovery of W and Z0 5 Lowest order tests of the SM in the leptonic sector 5.1 Phenomenology of purely leptonic reactions 5.2 A check of the minimal Higgs mechanism 5.3 Support for the SM from hadronic collider data 5.4 Concluding remarks 6 The Higgs boson 6.1 Introductory remarks 6.2 Higgs decay 6.3 Higgs production at the Z0 mass 6.4 Limits on the Higgs mass 6.5 Concluding comments 7 The standard model beyond lowest order 7.1 Radiative corrections 7.2 Renormalization and physical parameters 7.3 The effective fine structure constant 7.4 The muon lifetime revisited 7.5 Estimates of one loop corrections 7.6 Higher order corrections 7.7 Practical problems in testing radiative corrections 7.8 Strategies to overcome the imprecision in Mw 7.9 Testing the minimal Higgs mechanism 7.10 Beyond the standard model 8 e+e- physics and the standard model 8.1 Electron-positron storage rings 8.2 The new e+e- colliders: TRISTAN and LEP 8.3 e+e- physics at energies [[ Mz 8.4 e+e- and the standard model 8.5 LEP data near the Z0 peak 8.6 Determination of the SM parameters of the Z0 8.7 Neutrino counting 8.8 Asymmetries and polarization measurements at the Z0 peak 8.9 Conclusions 9 Extension to the hadrons; quark-lepton universality 9.1 Charm, bottom and top 9.2 Quark mixing 9.3 Electroweak interaction of the quarks 9.4 The GIM mechanism 9.5 Colour 9.6 Summary of the quark sector of the standard model 9.7 Quark masses and the KM matrix 10 Phenomenology of semi-leptonic reactions 10.1 Model independent tests 10.2 Parity violation in electron-nucleus scattering 10.3 Optical rotation 10.4 Summary 11 The discovery of the narrow vector resonances 11.1 Introduction 11.2 The 'new' particles 11.3 Some qualitative features of QCD 11.4 Quark-lepton parallelism 11.5 Flavour classification of hadrons 11.6 The J/ψ and the OZI rule 11.7 Experimental status of the J/ψ spectroscopy 11.8 Properties of the J/ψ(3097) and ψ'(3685) 11.9 Baryouic decay of J/ψ 11.10 The T family and its experimental status 12 Hidden flavour bound states 12.1 Quarkonium 12.2 J/ψ decays. Calculation of the widths 12.3 Determination of as 12.4 Leptonic widths 12.5 Exotics: glueballs, hybrids, etc. 12.6 ψ'→π: a puzzle 12.7 Conclusions 13 Open heavy flavours 13.1 Discovery and basic properties of charm and bottom particles 13.2 Charm decay 13.3 B physics 13.4 Production of heavy fiavours 13.5 Heavy fiavours at LEP 13.6 Final comments 14 The heavy lepton τ 14.1 Introduction 14.2 Discovery of the τ lepton 14.3 Properties of the τ lepton 14.4 τ decay 14.5 The τ neutrino 14.6 Rare τ decays 14.7 Miscellaneous and conclusions 15 Towards the parton model deep inelastic scattering 15.1 Electron-muon scattering 15.2 Elastic electron-proton scattering 15.3 Inelastic electron-nucleon scattering 15.4 Inelastic neutrino-nucleon scattering 15.5 Deep inelastic scattering and scaling behaviour 15.6 Polarization effects in deep inelastic scattering 16 The quark-parton model 16.1 The introduction of partons 16.2 Antipartons 16.3 Partons as quarks 16.4 The detailed quark-parton model 16.5 Charged lepton induced reactions for Q2 of order M2z 16.6 Behaviour of the quark number densities as x → 0 16.7 The missing constituents--gluons 16.8 The parton model in polarized deep inelastic scattering 16.9 Appendix to Chapter 16: The patton model as an impulse approximation 17 Experimental tests of the quark-parton model 17.1 Deep inelastic scaling functions for Q2 [[ M2Z 17.2 Neutrino cross-sections in the quark-parton model for Q2 [[M2Z 17.3 Cross-sections in the quark-parton model for Q2 comparable with M2Z 17.4 Application of the parton model to related processes Appendix 1: Elements of field theory A1.1 Fields and creation operators A1.2 Parity, charge conjugation and G-parity A1.3 The S-matrix Appendix 2: Feynman rules for QED, QCD and the SM A2.1 Relation between S-matrix and Feynman amplitude A2.2 QCD and QED A2.3 The SM A2.4 Some examples of Feynman amplitudes A2.5 Colour sums A2.6 The Gell-Mann SU(3) matrices A2.7 The Fierz reshuffle theorem A2.8 Dimension of matrix elements Appendix 3: Conserved vector currents and their charges References Analytic subject index for vols. 1 and 2
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