Preface |
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xiii | |
I THE PATH INTEGRAL IN QUANTUM MECHANICS |
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1 | (70) |
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Action in Classical Mechanics |
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3 | (14) |
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The Variational Principle and Equations of Motion |
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3 | (3) |
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A Mathematical Note: The Notion of the Functional |
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6 | (3) |
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The Action as a Function of the Boundary Conditions |
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9 | (4) |
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Symmetries of the Action and Conservation Laws |
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13 | (4) |
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The Path Integral in Quantum Mechanics |
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17 | (22) |
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The Green Function of the Schrodinger Equation |
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17 | (4) |
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21 | (4) |
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The Path Integral for Free Motion |
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25 | (6) |
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Free Motion: Straightforward Calculation of the Path Integral |
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26 | (1) |
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Free Motion: Path Integral Calculation by the Stationary Phase Method |
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27 | (4) |
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The Path Integral for the Harmonic Oscillator |
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31 | (2) |
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Imaginary Time and the Ground State Energy |
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33 | (6) |
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The Euclidean Path Integral |
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39 | (32) |
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The Symmetric Double Well |
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39 | (22) |
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Quantum Mechanical Instantons |
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42 | (7) |
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The Contribution from the Vicinity of the Instanton Trajectory |
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49 | (4) |
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Calculation of the Functional Determinant |
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53 | (8) |
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A Particle in a Periodic Potential. Band Structure |
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61 | (4) |
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65 | (2) |
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67 | (4) |
II INTRODUCTION TO QUANTUM FIELD THEORY |
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71 | (154) |
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Classical and Quantum Fields |
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73 | (26) |
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From Large Number of Degrees of Freedom to Particles |
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73 | (4) |
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77 | (2) |
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79 | (4) |
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79 | (2) |
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Quantization via Path Integrals |
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81 | (2) |
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The Equivalence of QFT & Statistical Physics |
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83 | (3) |
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Free Field Quantization: From Fields to Particles |
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86 | (13) |
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86 | (2) |
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88 | (1) |
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89 | (2) |
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Elementary Excitations of the Field |
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91 | (8) |
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Vacuum Energy in &phis;4 Theory |
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99 | (32) |
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100 | (7) |
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Simple Calculation of Casimir Energy |
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100 | (3) |
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Casimir Energy: Calculation Via Path Integral |
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103 | (4) |
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Effective Potential of &phis;4 Theory |
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107 | (24) |
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Calculation of Ueff(&phis;) |
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109 | (2) |
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The Explicit Form of Ueff |
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111 | (2) |
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Renormalization of Mass and Coupling Constant |
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113 | (4) |
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Running Coupling Constant, Dimensional Transmutation and Anomalous Dimensions |
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117 | (7) |
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Effective Potential of the Massive Theory |
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124 | (7) |
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The Effective Action in &phis;4 Theory |
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131 | (28) |
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Correlation Functions and the Generating Functional |
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132 | (3) |
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Z[J], W[J] and Correlation Functions of the Free Field |
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135 | (6) |
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The Classical Green Function |
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136 | (2) |
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138 | (3) |
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Generating Functionals in &phis;4 Theory |
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141 | (7) |
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141 | (1) |
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Generating Functionals: Expansion in λ |
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141 | (5) |
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Generating Functionals: the Loop Expansion |
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146 | (2) |
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148 | (11) |
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Expansion of the Functional Determinant |
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151 | (8) |
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Renormalization of the Effective Action |
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159 | (30) |
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159 | (6) |
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Explicit Form of the Diagrams |
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162 | (3) |
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The Structure of Ultraviolet Divergencies |
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165 | (3) |
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Pauli-Villars Regularization |
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168 | (6) |
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171 | (2) |
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About Dimensional Regularization |
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173 | (1) |
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The Regularized Inverse Propagator |
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174 | (5) |
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Analytic Continuation to Minkowski Space |
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176 | (3) |
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179 | (6) |
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179 | (2) |
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Renormalization of the Coupling Constant |
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181 | (1) |
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Renormalization of the Wave Function |
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182 | (3) |
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185 | (4) |
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189 | (18) |
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189 | (8) |
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Renormalization Group Equation |
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189 | (3) |
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General Solution of RG Equation |
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192 | (3) |
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195 | (2) |
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197 | (3) |
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Scale Transformations at the Tree Level |
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197 | (2) |
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199 | (1) |
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200 | (7) |
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207 | (18) |
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Correlators in Terms of Γ[&phis;] |
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207 | (3) |
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On the Properties of Perturbation Series |
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210 | (9) |
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On the Loop Expansion Parameter |
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210 | (4) |
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On the Asymptotic Nature of Perturbation Series |
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214 | (5) |
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On &phis;4 Theory with Large Coupling Constant |
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219 | (2) |
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The Cases d = 2 and d = 3: Second-Order Phase transitions |
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219 | (1) |
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The Cases d = 4: Possible Triviality of &phis;4 Theory |
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220 | (1) |
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221 | (4) |
III MORE COMPLEX FIELDS AND OBJECTS |
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225 | (180) |
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Second Quantisation: From Particles to Fields |
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227 | (20) |
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Identical Particles and Symmetry of Wave Functions |
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227 | (3) |
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230 | (10) |
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231 | (2) |
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Creation and Annihilation Operators |
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233 | (2) |
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235 | (1) |
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236 | (2) |
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Result: Recipe for Quantisation |
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238 | (2) |
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240 | (7) |
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240 | (1) |
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Creation and Annihilation Operators |
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241 | (1) |
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Many-Particle Hamiltonian |
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242 | (1) |
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242 | (5) |
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Path Integral for Fermions |
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247 | (42) |
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On the Formal Classical Limit for Fermions |
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247 | (2) |
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Grassmann Algebras: A Short Introduction |
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249 | (9) |
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Path Integral For Non-Relativistic Fermions |
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258 | (9) |
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Classical Pseudomechanics |
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259 | (4) |
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Path Integral Quantisation |
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263 | (4) |
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Generating Functional For Fermionic Fields |
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267 | (5) |
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Coupling of the Dirac Spinor and the &phis;4 Scalar Fields |
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272 | (9) |
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Loop Expansion and Diagram Techniques |
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273 | (5) |
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278 | (3) |
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Fermion Contribution to the Effective Potential |
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281 | (8) |
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289 | (54) |
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289 | (9) |
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289 | (1) |
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Example of a Globally Invariant Lagrangian |
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290 | (2) |
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Example of a Locally Invariant Lagrangian |
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292 | (1) |
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Lagrangian of Gauge Fields |
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293 | (5) |
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Dynamics of Gauge Invariant Fields |
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298 | (6) |
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298 | (1) |
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299 | (1) |
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300 | (1) |
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Gauge Freedom and Gauge Conditions |
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301 | (3) |
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Spontaneously Broken Symmetry |
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304 | (6) |
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304 | (1) |
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Goldstone Modes and Higgs Mechanism |
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305 | (2) |
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Elimination of Goldstone Modes. Goldstone Theorem |
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307 | (1) |
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308 | (2) |
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Quantization of Systems With Constraints |
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310 | (12) |
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310 | (2) |
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On Constrained Mechanical Systems |
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312 | (1) |
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312 | (1) |
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The Matrix of Poisson Brackets |
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313 | (1) |
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First and Second Order Constraints |
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314 | (3) |
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317 | (2) |
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319 | (3) |
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Hamiltonian Quantization of Yang - Mills Fields |
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322 | (8) |
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Quantization of Gauge Fields: Faddeev-Popov Method |
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330 | (3) |
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333 | (10) |
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Topological Objects in Field Theory |
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343 | (62) |
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344 | (3) |
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A Few Words about Solitons |
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347 | (3) |
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350 | (14) |
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Ginzburg-Landau Model of Superconductivity |
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351 | (1) |
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352 | (4) |
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356 | (1) |
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A Few Words about Topology and an Exotic String |
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357 | (6) |
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Vortex Solution in Other Contexts |
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363 | (1) |
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The 't Hooft-Polyakov Monopole |
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364 | (11) |
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Magnetic Properties of the Solution |
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366 | (2) |
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Lower Boundary on the Monopole Mass |
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368 | (2) |
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370 | (1) |
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A Few Words About the Topology |
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371 | (2) |
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373 | (2) |
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375 | (8) |
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375 | (4) |
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On the Vacuum Structure of Yang-Mills Theory |
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379 | (4) |
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383 | (22) |
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Quantum Correction to the Mass of the Kink |
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385 | (4) |
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Physical Contents of Fluctuations around the Kink |
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389 | (2) |
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391 | (4) |
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395 | (10) |
A Some Integrals and Products |
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405 | (8) |
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405 | (1) |
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Calculation of Πn (1 - x2/n2-&pi2) |
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406 | (2) |
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Calculation of 1ƒ1 dx/x In (1 - x) |
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408 | (1) |
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Calculation of ∞ƒ∞ dx/x2 In (1 + x2) |
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409 | (2) |
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411 | (2) |
B Splitting of Energy Levels in Double-Well Potential |
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413 | (4) |
C Lie Algebras |
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417 | (15) |
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417 | (2) |
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419 | (1) |
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The Idea of Classification. Levi-Maltsev Decomposition |
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420 | (4) |
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The Adjoint Representation |
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420 | (1) |
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Solvable and Nilpotent Algebras |
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421 | (1) |
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Reductive and Semisimple Algebras |
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422 | (2) |
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Classification of Complex Semisimple Lie Algebras |
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424 | (8) |
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The Cartan Subalgebra. Roots |
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424 | (1) |
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Properties of Roots. Cartan-Weyl Basis |
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425 | (2) |
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Cartan Matrix. Dynkin Schemes |
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427 | (2) |
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429 | (3) |
Index |
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432 | |