Preface |
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xiii | |
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I Introductory Survey, Electromagnetism as a Gauge Theory, and Relativistic Quantum Mechanics |
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1 | (112) |
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1 The Particles and Forces of the Standard Model |
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3 | (38) |
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1.1 Introduction: the Standard Model |
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3 | (1) |
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1.2 The fermions of the Standard Model |
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4 | (8) |
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4 | (4) |
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8 | (4) |
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1.3 Particle interactions in the Standard Model |
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12 | (18) |
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1.3.1 Classical and quantum fields |
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12 | (3) |
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1.3.2 The Yukawa theory of force as virtual quantum exchange |
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15 | (4) |
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1.3.3 The one-quantum exchange amplitude |
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19 | (2) |
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1.3.4 Electromagnetic interactions |
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21 | (1) |
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22 | (4) |
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1.3.6 Strong interactions |
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26 | (3) |
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1.3.7 The gauge bosons of the Standard Model |
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29 | (1) |
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1.4 Renormalization and the Higgs sector of the Standard Model |
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30 | (4) |
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30 | (3) |
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1.4.2 The Higgs boson of the Standard Model |
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33 | (1) |
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34 | (7) |
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35 | (6) |
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2 Electromagnetism as a Gauge Theory |
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41 | (22) |
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41 | (2) |
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2.2 The Maxwell equations: current conservation |
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43 | (2) |
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2.3 The Maxwell equations: Lorentz covariance and gauge invariance |
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45 | (4) |
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2.4 Gauge invariance (and covariance) in quantum mechanics |
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49 | (3) |
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2.5 The argument reversed: the gauge principle |
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52 | (4) |
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2.6 Comments on the gauge principle in electromagnetism |
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56 | (7) |
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62 | (1) |
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3 Relativistic Quantum Mechanics |
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63 | (24) |
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3.1 The Klein-Gordon equation |
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63 | (3) |
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3.1.1 Solutions in coordinate space |
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64 | (1) |
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3.1.2 Probability current for the KG equation |
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65 | (1) |
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66 | (6) |
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3.2.1 Free-particle solutions |
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69 | (1) |
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3.2.2 Probability current for the Dirac equation |
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70 | (2) |
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72 | (2) |
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3.4 The negative-energy solutions |
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74 | (6) |
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3.4.1 Positive-energy spinors |
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74 | (1) |
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3.4.2 Negative-energy spinors |
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75 | (1) |
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3.4.3 Dirac's interpretation of the negative-energy solutions of the Dirac equation |
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76 | (1) |
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3.4.4 Feynman's interpretation of the negative-energy solutions of the KG and Dirac equations |
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77 | (3) |
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3.5 Inclusion of electromagnetic interactions via the gauge principle: the Dirac prediction of g = 2 for the electron |
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80 | (7) |
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83 | (4) |
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4 Lorentz Transformations and Discrete Symmetries |
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87 | (26) |
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4.1 Lorentz transformations |
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87 | (8) |
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87 | (2) |
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89 | (6) |
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4.2 Discrete transformations: P, C and T |
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95 | (18) |
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95 | (4) |
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99 | (4) |
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103 | (1) |
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104 | (4) |
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108 | (1) |
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109 | (4) |
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II Introduction to Quantum Field Theory |
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113 | (106) |
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5 Quantum Field Theory I: The Free Scalar Field |
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115 | (34) |
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5.1 The quantum field: (i) descriptive |
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115 | (10) |
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5.2 The quantum field: (ii) Lagrange-Hamilton formulation |
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125 | (19) |
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5.2.1 The action principle: Lagrangian particle mechanics |
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125 | (4) |
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5.2.2 Quantum particle mechanics a la Heisenberg-Lagrange-Hamilton |
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129 | (2) |
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5.2.3 Interlude: the quantum oscillator |
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131 | (2) |
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5.2.4 Lagrange-Hamilton classical field mechanics |
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133 | (4) |
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5.2.5 Heisenberg-Lagrange-Hamilton quantum field mechanics |
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137 | (7) |
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5.3 Generalizations: four dimensions, relativity and mass |
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144 | (5) |
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146 | (3) |
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6 Quantum Field Theory II: Interacting Scalar Fields |
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149 | (34) |
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6.1 Interactions in quantum field theory: qualitative introduction |
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149 | (3) |
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6.2 Perturbation theory for interacting fields: the Dyson expansion of the S-matrix |
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152 | (6) |
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6.2.1 The interaction picture |
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153 | (3) |
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6.2.2 The S-matrix and the Dyson expansion |
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156 | (2) |
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6.3 Applications to the 'ABC theory |
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158 | (25) |
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6.3.1 The decay C → A + B |
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159 | (4) |
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6.3.2 A + B → A + B scattering: the amplitudes |
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163 | (9) |
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6.3.3 A + B → A + B scattering: the Yukawa exchange mechanism, s and u channel processes |
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172 | (2) |
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6.3.4 A + B → A + B scattering: the differential cross section |
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174 | (3) |
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6.3.5 A + B → A + B scattering: loose ends |
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177 | (2) |
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179 | (4) |
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7 Quantum Field Theory III: Complex Scalar Fields, Dirac and Maxwell Fields; Introduction of Electromagnetic Interactions |
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183 | (36) |
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7.1 The complex scalar field: global U(1) phase invariance, particles and antiparticles |
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184 | (7) |
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7.2 The Dirac field and the spin-statistics connection |
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191 | (5) |
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7.3 The Maxwell field Aμ(x) |
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196 | (10) |
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7.3.1 The classical field case |
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196 | (3) |
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199 | (7) |
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7.4 Introduction of electromagnetic interactions |
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206 | (4) |
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7.5 P, C and T in quantum field theory |
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210 | (9) |
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210 | (1) |
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211 | (2) |
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213 | (2) |
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215 | (4) |
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III Tree-Level Applications in QED |
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219 | (78) |
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8 Elementary Processes in Scalar and Spinor Electrodynamics |
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221 | (48) |
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8.1 Coulomb scattering of charged spin-0 particles |
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221 | (6) |
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8.1.1 Coulomb scattering of s+ (wavefunction approach) |
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221 | (3) |
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8.1.2 Coulomb scattering of s+ (field-theoretic approach) |
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224 | (1) |
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8.1.3 Coulomb scattering of s- |
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225 | (2) |
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8.2 Coulomb scattering of charged spin-1/2 particles |
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227 | (7) |
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8.2.1 Coulomb scattering of e- (wavefunction approach) |
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227 | (3) |
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8.2.2 Coulomb scattering of e- (field-theoretic approach) |
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230 | (1) |
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8.2.3 Trace techniques for spin summations |
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230 | (3) |
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8.2.4 Coulomb scattering of e+ |
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233 | (1) |
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234 | (8) |
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8.3.1 The amplitude for e-s+ → e-s+ |
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234 | (5) |
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8.3.2 The cross section for e-s+ → e-s+ |
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239 | (3) |
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8.4 Scattering from a non-point-like object: the pion form factor in e-π+ → e-π+ |
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242 | (5) |
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8.4.1 e- scattering from a charge distribution |
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243 | (1) |
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244 | (1) |
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8.4.3 Current conservation |
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245 | (2) |
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8.5 The form factor in the time-like region: e+e- → π+π- and crossing symmetry |
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247 | (3) |
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8.6 Electron Compton scattering |
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250 | (4) |
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8.6.1 The lowest-order amplitudes |
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250 | (1) |
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251 | (1) |
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8.6.3 The Compton cross section |
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252 | (2) |
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8.7 Electron muon elastic scattering |
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254 | (3) |
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8.8 Electron-proton elastic scattering and nucleon form factors |
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257 | (12) |
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258 | (1) |
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8.8.2 Current conservation |
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259 | (4) |
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263 | (6) |
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9 Deep Inelastic Electron-Nucleon Scattering and the Parton Model |
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269 | (28) |
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9.1 Inelastic electron-proton scattering: kinematics and structure functions |
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269 | (3) |
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9.2 Bjorken scaling and the parton model |
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272 | (9) |
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9.3 Partons as quarks and gluons |
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281 | (3) |
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9.4 The Drell-Yan process |
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284 | (4) |
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9.5 e+e- annihilation into hadrons |
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288 | (9) |
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292 | (5) |
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IV Loops and Renormalization |
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297 | (64) |
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10 Loops and Renormalization I: The ABC Theory |
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299 | (28) |
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10.1 The propagator correction in ABC theory |
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300 | (11) |
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10.1.1 The O(g2) self-energy Π[ 2](q2) |
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300 | (7) |
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307 | (1) |
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10.1.3 Field strength renormalization |
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308 | (3) |
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10.2 The vertex correction |
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311 | (3) |
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10.3 Dealing with the bad news: a simple example |
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314 | (4) |
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10.3.1 Evaluating Π[ 2](q2) |
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314 | (2) |
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10.3.2 Regularization and renormalization |
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316 | (2) |
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10.4 Bare and renormalized perturbation theory |
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318 | (6) |
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10.4.1 Reorganizing perturbation theory |
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318 | (3) |
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10.4.2 The O(g2ph) renormalized self-energy revisited: how counter terms are determined by renormalization conditions |
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321 | (3) |
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324 | (3) |
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326 | (1) |
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11 Loops and Renormalization II: QED |
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327 | (34) |
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327 | (2) |
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11.2 The O(e2) fermion self-energy |
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329 | (2) |
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11.3 The O(e2) photon self-energy |
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331 | (2) |
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11.4 The O(e2) renormalized photon self-energy |
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333 | (3) |
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11.5 The physics of Π[ 2]y(q2) |
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336 | (9) |
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11.5.1 Modified Coulomb's law |
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336 | (2) |
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11.5.2 Radiatively induced charge form factor |
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338 | (1) |
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11.5.3 The running coupling constant |
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339 | (5) |
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11.5.4 Πy[ 2] in the s-channel |
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344 | (1) |
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11.6 The O(e2) vertex correction, and Z1 = Z2 |
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345 | (3) |
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11.7 The anomalous magnetic moment and tests of QED |
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348 | (5) |
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11.8 Which theories are renormalizable - and does it matter? |
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353 | (8) |
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360 | (1) |
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A Non-relativistic Quantum Mechanics |
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361 | (4) |
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365 | (4) |
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C Maxwell's Equations: Choice of Units |
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369 | (2) |
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D Special Relativity: Invariance and Covariance |
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371 | (6) |
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377 | (10) |
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387 | (6) |
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393 | (6) |
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H Elements of Non-relativistic Scattering Theory |
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399 | (6) |
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H.1 Time-independent formulation and differential cross section |
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399 | (2) |
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H.2 Expression for the scattering amplitude: Born approximation |
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401 | (1) |
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H.3 Time-dependent approach |
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402 | (3) |
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I The Schrodinger and Heisenberg Pictures |
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405 | (2) |
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J Dirac Algebra and Trace Identities |
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407 | (4) |
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407 | (2) |
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407 | (1) |
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407 | (1) |
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J.1.3 Hermitian conjugate of spinor matrix elements |
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408 | (1) |
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J.1.4 Spin sums and projection operators |
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408 | (1) |
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409 | (2) |
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K Example of a Cross Section Calculation |
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411 | (6) |
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K.1 The spin-averaged squared matrix element |
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413 | (1) |
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K.2 Evaluation of two-body Lorentz-invariant phase space in `laboratory' variables |
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413 | (4) |
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L Feynman Rules for Tree Graphs in QED |
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417 | (4) |
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417 | (1) |
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418 | (1) |
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418 | (3) |
References |
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421 | (6) |
Index |
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427 | |