| Preface |
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vii | |
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1 | (76) |
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1 Quantum Field Theory -- Why and How |
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3 | (12) |
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1.1 Schwinger's Action Principle |
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5 | (5) |
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1.2 Free-Field Kinematics |
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10 | (5) |
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2 Functional Preliminaries |
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15 | (18) |
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2.1 Functional Differentiation |
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16 | (1) |
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17 | (1) |
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2.3 Quadratic (Gaussian) Translation |
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18 | (5) |
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2.4 Functional Integration |
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23 | (4) |
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2.5 Cluster Decomposition |
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27 | (3) |
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30 | (3) |
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3 Functional Field Theory |
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33 | (18) |
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3.1 The Generating Functional |
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33 | (5) |
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3.2 A Gauge Digression: SU(N)-QCD |
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38 | (3) |
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3.3 Coupled Fermion and Boson Fields |
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41 | (3) |
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3.4 Fields at the Same Point |
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44 | (7) |
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4 The Generating Functional and the S-Matrix |
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51 | (10) |
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4.1 The Generating Functional Operator |
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51 | (3) |
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4.2 Asymptotic Conditions |
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54 | (1) |
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55 | (4) |
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4.4 A Bremsstrahlung Example |
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59 | (2) |
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5 Schwinger/Fradkin Representations |
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61 | (16) |
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61 | (5) |
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66 | (3) |
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5.3 The Bloch--Nordsieck - IR - Eikonal Approximation |
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69 | (4) |
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5.4 A Convenient Reformulation |
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73 | (4) |
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77 | (54) |
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79 | (4) |
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6 Radiative Corrections of the Photon Propagator |
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83 | (24) |
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6.1 Functional Approach to the Photon Propagator |
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83 | (4) |
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6.2 Higher-order Radiative Correction |
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87 | (3) |
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6.3 The DP Model for a Single Closed Fermion Loop |
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90 | (6) |
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6.4 The Extended DP Model, and the Finiteness of Z3 |
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96 | (7) |
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103 | (4) |
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7 Radiative Corrections to the Electron Propagator |
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107 | (10) |
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107 | (1) |
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108 | (3) |
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111 | (4) |
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115 | (2) |
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8 A QED Symmetry-Breaking Model of Vacuum Energy |
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117 | (14) |
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117 | (3) |
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120 | (3) |
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123 | (1) |
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124 | (3) |
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8.5 Application to Dark Energy |
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127 | (2) |
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129 | (2) |
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131 | (62) |
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133 | (4) |
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9 Explicit, Non-Perturbative Gauge Invariance |
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137 | (14) |
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137 | (5) |
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9.2 Gluon Summations and Explicit Gauge Invariance |
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142 | (5) |
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147 | (4) |
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10 QCD Transverse Fluctuations |
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151 | (10) |
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151 | (4) |
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10.2 A Phenomenological Expression of Transverse Imprecision |
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155 | (2) |
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157 | (4) |
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11 Quark Binding Potential |
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161 | (10) |
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11.1 Use of the Eikonal Approximation |
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161 | (6) |
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11.2 Estimation of the "Model Pion" Mass |
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167 | (4) |
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12 Nucleon Scattering and Binding |
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171 | (22) |
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171 | (1) |
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172 | (12) |
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12.3 A Qualitative Binding Potential |
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184 | (5) |
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189 | (1) |
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12.5 Summary and Speculation |
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190 | (3) |
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Astrophysical Speculations |
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193 | (40) |
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Astrophysical Speculations |
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195 | (2) |
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13 Inflation as the Precursor of Dark Energy |
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197 | (8) |
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197 | (3) |
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200 | (2) |
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13.3 A Cosmological Speculation |
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202 | (1) |
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203 | (2) |
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14 Quantum Tachyon Dynamics |
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205 | (28) |
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206 | (4) |
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210 | (5) |
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215 | (3) |
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14.4 Photon Emission and Reabsorption |
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218 | (2) |
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14.5 Kinematic of Tachyon-Particle Reactions |
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220 | (1) |
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14.5.1 Blocking the reaction → T + T |
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221 | (1) |
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14.5.2 Scattering: T + p = T' + p' |
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222 | (1) |
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14.6 From Ehrenfest's Theorem to Loop Annihilation |
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223 | (4) |
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14.7 NASA's Fermi Bubbles |
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227 | (2) |
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229 | (4) |
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233 | (26) |
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Appendix A Equivalence Example of the DP Model |
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235 | (2) |
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Appendix B Intuitive Justification of the DP Model |
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237 | (2) |
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Appendix C Connected Cluster-Expansion Functional |
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239 | (2) |
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Appendix D Fradkin's Representations for non-Abelian GC[ A] and L[ A] |
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241 | (4) |
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Appendix E Effective Locality and Transverse Imprecision |
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245 | (4) |
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Appendix F Tachyonic Photon Emission |
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249 | (2) |
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Appendix G Relativistic Tachyon Notation |
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251 | (8) |
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G.1 Free Tachyon Equation |
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251 | (1) |
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252 | (1) |
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G.2.1 Positive energy solutions |
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252 | (1) |
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G.2.2 Negative energy solutions |
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253 | (1) |
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G.3 Some Useful Formulae, Valid for |p| ≥ M |
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254 | (1) |
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G.4 "Spin" of the Tachyon |
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254 | (1) |
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255 | (2) |
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257 | (2) |
| First Epilogue |
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259 | (2) |
| Second Epilogue |
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261 | (2) |
| Bibliography |
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263 | |