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1 Origins I: From the arrow of time to the first quantum field |
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1 | (29) |
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1.1 Quantum prehistory: crises in classical physics |
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1 | (2) |
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1.2 Early work on cavity radiation |
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3 | (5) |
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1.3 Planck's route to the quantization of energy |
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8 | (6) |
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1.4 First inklings of field quantization: Einstein and energy fluctuations |
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14 | (4) |
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1.5 The first true quantum field: Jordan and energy fluctuations |
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18 | (12) |
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2 Origins II: Gestation and birth of interacting field theory: from Dirac to Shelter Island |
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30 | (27) |
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2.1 Introducing interactions: Dirac and the beginnings of quantum electrodynamics |
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31 | (9) |
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2.2 Completing the formalism for free fields: Jordan, Klein, Wigner, Pauli, and Heisenberg |
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40 | (6) |
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2.3 Problems with interacting fields: infinite seas, divergent integrals, and renormalization |
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46 | (11) |
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3 Dynamics I: The physical ingredients of quantum field theory: dynamics, symmetries, scales |
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57 | (12) |
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4 Dynamics II: Quantum mechanical preliminaries |
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69 | (39) |
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4.1 The canonical (operator) framework |
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70 | (16) |
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4.2 The functional (path-integral) framework |
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86 | (10) |
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96 | (10) |
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106 | (2) |
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5 Dynamics III: Relativistic quantum mechanics |
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108 | (24) |
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5.1 The Lorentz and Poincare groups |
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108 | (3) |
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5.2 Relativistic multi-particle states (without spin) |
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111 | (3) |
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5.3 Relativistic multi-particle states (general spin) |
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114 | (7) |
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5.4 How not to construct a relativistic quantum theory |
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121 | (4) |
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5.5 A simple condition for Lorentz-invariant scattering |
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125 | (5) |
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130 | (2) |
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6 Dynamics IV: Aspects of locality: clustering, microcausality, and analyticity |
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132 | (39) |
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6.1 Clustering and the smoothness of scattering amplitudes |
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133 | (5) |
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6.2 Hamiltonians leading to clustering theories |
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138 | (6) |
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6.3 Constructing clustering Hamiltonians: second quantization |
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144 | (5) |
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6.4 Constructing a relativistic, clustering theory |
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149 | (10) |
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6.5 Local fields, non-localizable particles! |
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159 | (5) |
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6.6 From microcausality to analyticity |
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164 | (5) |
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169 | (2) |
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7 Dynamics V: Construction of local covariant fields |
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171 | (48) |
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7.1 Constructing local, Lorentz-invariant Hamiltonians |
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171 | (2) |
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7.2 Finite-dimensional representations of the homogeneous Lorentz group |
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173 | (4) |
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7.3 Local covariant fields for massive particles of any spin: the Spin-Statistics theorem |
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177 | (7) |
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7.4 Local covariant fields for spin-1/2 (spinor fields) |
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184 | (14) |
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7.5 Local covariant fields for spin-1 (vector fields) |
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198 | (4) |
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7.6 Some simple theories and processes |
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202 | (13) |
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215 | (4) |
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8 Dynamics VI: The classical limit of quantum fields |
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219 | (21) |
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8.1 Complementarity issues for quantum fields |
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219 | (4) |
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8.2 When is a quantum field "classical"? |
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223 | (5) |
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8.3 Coherent states of a quantum field |
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228 | (6) |
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8.4 Signs, stability, symmetry-breaking |
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234 | (4) |
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238 | (2) |
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9 Dynamics VII: Interacting fields: general aspects |
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240 | (67) |
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9.1 Field theory in Heisenberg representation: heuristics |
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241 | (12) |
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9.2 Field theory in Heisenberg representation: axiomaties |
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253 | (15) |
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9.3 Asymptotic formalism I: the Haag--Ruelle scattering theory |
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268 | (13) |
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9.4 Asymptotic formalism II: the Lehmanu--Symanzik--Zimmermann (LSZ) theory |
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281 | (8) |
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9.5 Spectral properties of field theory |
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289 | (8) |
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9.6 General aspects of the particle--field connection |
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297 | (7) |
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304 | (3) |
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10 Dynamics VIII: Interacting fields: perturbative aspects |
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307 | (67) |
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10.1 Perturbation theory in interaction picture and Wick's theorem |
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309 | (5) |
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10.2 Feynman graphs and Feynman rules |
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314 | (11) |
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10.3 Path-integral formulation of field theory |
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325 | (16) |
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10.4 Graphical concepts: N-particle irreducibility |
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341 | (18) |
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10.5 How to stop worrying about Haag's theorem |
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359 | (12) |
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371 | (3) |
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11 Dynamics IX: Interacting fields: non-perturbative aspects |
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374 | (40) |
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11.1 On the (non-)convergence of perturbation theory |
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376 | (10) |
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11.2 "Perturbatively non-perturbative" processes: threshhold bound states |
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386 | (14) |
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11.3 "Essentially non-perturbative" processes: non-Borel-summability in field theory |
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400 | (11) |
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411 | (3) |
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12 Symmetries I: Continuous spacetime symmetry: why we need Lagrangians in field theory |
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414 | (55) |
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12.1 The problem with derivatively coupled theories: seagulls, Schwinger terms, and T* products |
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414 | (2) |
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12.2 Canonical formalism in quantum field theory |
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416 | (5) |
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12.3 General condition for Lorentz-invariant field theory |
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421 | (5) |
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12.4 Noether's theorem, the stress-energy tensor, and all that stuff |
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426 | (5) |
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12.5 Applications of Noether's theorem |
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431 | (12) |
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12.6 Beyond Poincare: supersymmetry and superfields |
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443 | (21) |
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464 | (5) |
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13 Symmetries II: Discrete spacetime symmetries |
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469 | (18) |
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13.1 Parity properties of a general local covariant field |
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470 | (4) |
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13.2 Charge-conjugation properties of a general local covariant field |
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474 | (3) |
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13.3 Time-reversal properties of a general local covariant field |
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477 | (1) |
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13.4 The TCP and Spin-Statistics theorems |
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478 | (7) |
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485 | (2) |
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14 Symmetries III: Global symmetries in field theory |
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487 | (22) |
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14.1 Exact global symmetries are rare! |
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489 | (3) |
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14.2 Spontaneous breaking of global symmetries: the Goldstone theorem |
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492 | (3) |
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14.3 Spontaneous breaking of global symmetries: dynamical aspects |
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495 | (12) |
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507 | (2) |
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15 Symmetries IV: Local symmetries in field theory |
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509 | (60) |
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15.1 Gauge symmetry: an example in particle mechanics |
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509 | (3) |
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15.2 Constrained Hamiltonian systems |
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512 | (7) |
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15.3 Abelian gauge theory as a constrained Hamiltonian system |
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519 | (10) |
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15.4 Non-abelian gauge theory: construction and functional integral formulation |
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529 | (15) |
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15.5 Explicit quantum-breaking of global symmetries: anomalies |
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544 | (8) |
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15.6 Spontaneous symmetry-breaking in theories with a local gauge symmetry |
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552 | (13) |
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565 | (4) |
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16 Scales I: Scale sensitivity of field theory amplitudes and effective field theories |
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569 | (41) |
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16.1 Scale separation as a precondition for theoretical science |
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570 | (1) |
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16.2 General structure of local effective Lagrangians |
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571 | (3) |
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16.3 Scaling properties of effective Lagrangians: relevant, marginal, and irrelevant operators |
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574 | (7) |
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16.4 The renormalization group |
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581 | (7) |
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16.5 Regularization methods in field theory |
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588 | (7) |
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16.6 Effective field theories: a compendium |
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595 | (13) |
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608 | (2) |
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17 Scales II: Perturbatively renormalizable field theories |
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610 | (52) |
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17.1 Weinberg's power-counting theorem and the divergence structure of Feynman integrals |
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613 | (16) |
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17.2 Counterterms, subtractions, and perturbative renormalizability |
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629 | (16) |
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17.3 Renormalization and symmetry |
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645 | (7) |
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17.4 Renormalization group approach to renormalizability |
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652 | (8) |
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660 | (2) |
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18 Scales III: Short-distance structure of quantum field theory |
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662 | (50) |
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18.1 Local composite operators in field theory |
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664 | (15) |
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18.2 Factorizable structure of field theory amplitudes: the operator product expansion |
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679 | (19) |
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18.3 Renormalization group equations for renormalized amplitudes |
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698 | (10) |
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708 | (4) |
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19 Scales IV: Long-distance structure of quantum field theory |
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712 | (42) |
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19.1 The infrared catastrophe in unbroken abelian gauge theory |
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713 | (11) |
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19.2 The Bloch Nordsieck resolution |
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724 | (4) |
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19.3 Unbroken non-abelian gauge theory: confinement |
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728 | (16) |
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19.4 How confinement works: three-dimensional gauge theory |
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744 | (8) |
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752 | (2) |
| Appendix A The functional calculus |
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754 | (2) |
| Appendix B Rates and cross-sections |
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756 | (5) |
| Appendix C Majorana spinor algebra |
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761 | (4) |
| References |
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765 | (12) |
| Index |
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777 | |