目錄
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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