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1 From Particles to Fields |
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1 | (44) |
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1.1 Motivating the Quantum Field Theory |
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1 | (2) |
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1.2 Quantum Propagation Amplitude for the Non-relativistic Particle |
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3 | (14) |
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1.2.1 Path Integral for the Non-relativistic Particle |
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4 | (2) |
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1.2.2 Hamiltonian Evolution: Non-relativistic Particle |
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6 | (3) |
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1.2.3 A Digression into Imaginary Time |
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9 | (4) |
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1.2.4 Path Integral for the Jacobi Action |
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13 | (4) |
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1.3 Quantum Propagation Amplitude for the Relativistic Particle |
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17 | (3) |
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1.3.1 Path Integral for the Relativistic Particle |
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17 | (3) |
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1.4 Mathematical Structure of G(x2; x1) |
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20 | (9) |
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1.4.1 Lack of Transitivity |
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20 | (1) |
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1.4.2 Propagation Outside the Light Cone |
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20 | (1) |
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1.4.3 Three Dimensional Fourier Transform of G(x2; x1) |
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21 | (3) |
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1.4.4 Four Dimensional Fourier Transform of G(x2; x1) |
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24 | (2) |
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1.4.5 The First Non-triviality: Closed Loops and G(x; x) |
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26 | (1) |
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1.4.6 Hamiltonian Evolution: Relativistic Particle |
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27 | (2) |
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1.5 Interpreting G(x2; x1) in Terms of a Field |
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29 | (10) |
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1.5.1 Propagation Amplitude and Antiparticles |
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32 | (3) |
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1.5.2 Why do we Really Need Antiparticles? |
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35 | (2) |
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1.5.3 Aside: Occupation Number Basis in Quantum Mechanics |
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37 | (2) |
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1.6 Mathematical Supplement |
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39 | (6) |
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1.6.1 Path Integral From Time Slicing |
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39 | (2) |
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1.6.2 Evaluation of the Relativistic Path Integral |
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41 | (4) |
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45 | (22) |
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2.1 Sources that Disturb the Vacuum |
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45 | (7) |
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2.1.1 Vacuum Persistence Amplitude and G(x2; X1) |
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45 | (5) |
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2.1.2 Vacuum Instability and the Interaction Energy of the Sources |
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50 | (2) |
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2.2 From the Source to the Field |
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52 | (12) |
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2.2.1 Source to Field: Via Functional Fourier Transform |
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53 | (4) |
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2.2.2 Functional Integral Determinant: A First Look at Infinity |
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57 | (6) |
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2.2.3 Source to the Field: via Harmonic Oscillators |
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63 | (1) |
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2.3 Mathematical Supplement |
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64 | (3) |
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2.3.1 Aspects of Functional Calculus |
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64 | (3) |
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3 From Fields to Particles |
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67 | (64) |
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3.1 Classical Field Theory |
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68 | (19) |
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3.1.1 Action Principle in Classical Mechanics |
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68 | (2) |
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3.1.2 From Classical Mechanics to Classical Field Theory |
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70 | (4) |
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74 | (3) |
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3.1.4 Complex Scalar Field |
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77 | (1) |
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3.1.5 Vector Potential as a Gauge Field |
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78 | (3) |
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3.1.6 Electromagnetic Field |
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81 | (6) |
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3.2 Aside: Spontaneous Symmetry Breaking |
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87 | (3) |
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3.3 Quantizing the Real Scalar Field |
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90 | (6) |
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3.4 Davies-Unruh Effect: What is a Particle? |
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96 | (5) |
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3.5 Quantizing the Complex Scalar Field |
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101 | (3) |
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3.6 Quantizing the Electromagnetic Field |
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104 | (21) |
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3.6.1 Quantization in the Radiation Gauge |
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105 | (4) |
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3.6.2 Gauge Fixing and Covariant Quantization |
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109 | (6) |
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115 | (6) |
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3.6.4 Interaction of Matter and Radiation |
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121 | (4) |
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3.7 Aside: Analytical Structure of the Propagator |
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125 | (3) |
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3.8 Mathematical Supplement |
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128 | (3) |
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3.8.1 Summation of Series |
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128 | (1) |
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3.8.2 Analytic Continuation of the Zeta Function |
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129 | (2) |
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4 Real Life I: Interactions |
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131 | (58) |
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131 | (8) |
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4.1.1 The Paradigm of the Effective Field Theory |
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132 | (4) |
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4.1.2 A First Look at the Effective Action |
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136 | (3) |
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4.2 Effective Action for Electrodynamics |
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139 | (7) |
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4.2.1 Schwinger Effect for the Charged Scalar Field |
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142 | (1) |
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4.2.2 The Running of the Electromagnetic Coupling |
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143 | (3) |
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4.3 Effective Action for the λφ4 Theory |
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146 | (6) |
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152 | (10) |
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4.4.1 Setting up the Perturbation Series |
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153 | (3) |
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4.4.2 Feynman Rules for the λφ4 Theory |
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156 | (4) |
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4.4.3 Feynman Rules in the Momentum Space |
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160 | (2) |
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4.5 Effective Action and the Perturbation Expansion |
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162 | (2) |
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4.6 Aside: LSZ Reduction Formulas |
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164 | (3) |
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4.7 Handling the Divergences in the Perturbation Theory |
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167 | (9) |
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4.7.1 One Loop Divergences in the λφ4 Theory |
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168 | (3) |
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4.7.2 Running Coupling Constant in the Perturbative Approach |
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171 | (5) |
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4.8 Renormalized Perturbation Theory for the λφ4 Model |
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176 | (4) |
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4.9 Mathematical Supplement |
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180 | (9) |
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4.9.1 Lea from the Vacuum Energy Density |
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180 | (4) |
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4.9.2 Analytical Structure of the Scattering Amplitude |
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184 | (5) |
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5 Real Life II: Fermions and QED |
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189 | (72) |
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5.1 Understanding the Electron |
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189 | (2) |
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5.2 Non-relativistic Square Roots |
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191 | (4) |
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5.2.1 Square Root of pαpaα and the Pauli Matrices |
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191 | (1) |
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5.2.2 Spin Magnetic Moment from the Pauli Equation |
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192 | (1) |
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5.2.3 How does φ Transform? |
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193 | (2) |
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5.3 Relativistic Square Roots |
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195 | (6) |
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5.3.1 Square Root of pαpα and the Dirac Matrices |
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195 | (2) |
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5.3.2 How does φ Transform? |
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197 | (3) |
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5.3.3 Spin Magnetic Moment from the Dirac Equation |
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200 | (1) |
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5.4 Lorentz Group and Fields |
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201 | (11) |
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5.4.1 Matrix Representation of a Transformation Group |
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201 | (1) |
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5.4.2 Generators and their Algebra |
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202 | (1) |
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5.4.3 Generators of the Lorentz Group |
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203 | (2) |
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5.4.4 Representations of the Lorentz Group |
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205 | (1) |
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5.4.5 Why do we use the Dirac Spinor? |
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206 | (2) |
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208 | (1) |
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209 | (3) |
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5.5 Dirac Equation and the Dirac Spinor |
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212 | (4) |
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5.5.1 The Adjoint Spinor and the Dirac Lagrangian |
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212 | (1) |
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213 | (1) |
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5.5.3 Plane Wave solutions to the Dirac Equation |
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214 | (2) |
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5.6 Quantizing the Dirac Field |
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216 | (16) |
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5.6.1 Quantization with Anticommutation Rules |
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216 | (3) |
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5.6.2 Electron Propagator |
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219 | (3) |
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5.6.3 Propagator from a Fermionic Path Integral |
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222 | (2) |
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224 | (2) |
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5.6.5 Schwinger Effect for the Fermions |
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226 | (5) |
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5.6.6 Feynman Rules for QED |
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231 | (1) |
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5.7 One Loop Structure of QED |
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232 | (18) |
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5.7.1 Photon Propagator at One Loop |
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234 | (11) |
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5.7.2 Electron Propagator at One Loop |
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245 | (3) |
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5.7.3 Vertex Correction at One Loop |
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248 | (2) |
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5.8 QED Renormalization at One Loop |
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250 | (5) |
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5.9 Mathematical Supplement |
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255 | (6) |
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5.9.1 Calculation of the One Loop Electron Propagator |
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255 | (2) |
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5.9.2 Calculation of the One Loop Vertex Function |
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257 | (4) |
A Potpourri of Problems |
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261 | (18) |
Annotated Reading List |
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279 | (2) |
Index |
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281 | |