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1 | (5) |
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2 Singualar Lagrangians and Local Symmetries |
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6 | (18) |
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6 | (1) |
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7 | (2) |
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2.3 Algorithm for detecting local symmetries on Lagrangian level |
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9 | (5) |
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14 | (6) |
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2.5 Generator of gauge transformations and Noether identities |
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20 | (4) |
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3 Hamiltonian Approach. The Dirac Formalism |
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24 | (27) |
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24 | (1) |
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24 | (3) |
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3.3 The Hamilton equations of motion |
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27 | (16) |
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3.3.1 Streamlining the Hamilton equations of motion |
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29 | (4) |
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3.3.2 Alternative derivation of the Hamilton equations |
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33 | (4) |
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37 | (6) |
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3.4 Iterative procedure for generating the constratints |
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43 | (3) |
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3.4.1 Particular algorithm for generating the constraints |
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44 | (2) |
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3.5 First and second class constraints. Dirac brackets |
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46 | (5) |
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4 Symplectic Approach to Constrained Systems |
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51 | (16) |
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51 | (3) |
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4.2 The case fab singular |
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54 | (6) |
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4.2.1 Example: particle on a hypersphere |
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58 | (2) |
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4.3 Interpretation of W(L) and F |
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60 | (2) |
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4.4 The Faddeev-Jackiw reduction |
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62 | (5) |
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5 Local Symmetries within the Dirac Formalism |
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67 | (23) |
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67 | (1) |
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5.2 Local symmetries and canonical transformations |
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68 | (2) |
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5.3 Local symmetries of the Hamilton equations of motion |
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70 | (2) |
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5.4 Local symmetries of the total and extended action |
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72 | (3) |
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5.5 Local symmetries of the Lagrangian action |
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75 | (3) |
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5.6 Solution of the recursive relations |
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78 | (5) |
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5.7 Reparametrization invariant approach |
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83 | (7) |
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90 | (18) |
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90 | (1) |
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6.2 Gauge identites and Dirac's conjecture |
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90 | (8) |
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6.3 General system with two primaries and one secondary constraint |
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98 | (3) |
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6.4 Counterexamples to Dirac's conjecture? |
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101 | (7) |
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7 BFT Embedding of Second Class Systems |
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108 | (24) |
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108 | (1) |
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7.2 Summary of the BFT-procedure |
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109 | (4) |
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113 | (3) |
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7.4 Examples of BFT embedding |
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116 | (16) |
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7.4.1 The multidimensional rotator |
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116 | (2) |
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7.4.2 The Abelian self-dual model |
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118 | (3) |
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7.4.3 Abelian self-dual model and Maxwell-Chern-Simons theory |
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121 | (5) |
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7.4.4 The non-abelian SD model |
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126 | (6) |
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8 Hamilton-Jacobi Theory of Constrained Systems |
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132 | (22) |
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132 | (5) |
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8.1.1 Caratheodory's integrability conditions |
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133 | (2) |
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8.1.2 Characteristic curves of the HJ-equations |
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135 | (2) |
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8.2 HJ equations for first class systems |
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137 | (2) |
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8.3 HJ equations for second class systems |
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139 | (15) |
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8.3.1 HPF for reduced second class systems |
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139 | (2) |
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141 | (4) |
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8.3.3 HJ equations for second class systems via BFT embedding |
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145 | (3) |
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148 | (6) |
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9 Operator Quantization of Second Class Systems |
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154 | (10) |
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154 | (1) |
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9.2 Systems with only second class constraints |
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155 | (1) |
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9.3 Systems with first and second class constraints |
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156 | (8) |
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9.3.1 Example: the free Maxwell field in the Coulomb gauge |
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160 | (2) |
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162 | (2) |
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10 Functional Quantization of Second Class Systems |
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164 | (10) |
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164 | (1) |
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10.2 Partition function for second class systems |
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165 | (9) |
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11 Dynamical Gauges. BFV Functional Quantization |
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174 | (49) |
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174 | (1) |
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175 | (6) |
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11.3 BFV quantization of a quantum mechanical model |
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181 | (14) |
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11.3.1 The gauge-fixed effective Lagrangian |
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182 | (4) |
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11.3.2 The conserved BRST charge in configuration space |
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186 | (1) |
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11.3.3 The gauge fixed effective Hamiltonian |
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187 | (3) |
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11.3.4 The BRST charge in phase space |
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190 | (5) |
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11.4 Quantization of Yang-Mills thery in the Lorentz gauge |
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195 | (9) |
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11.5 Axiomatic BRST apprach |
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204 | (11) |
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11.5.1 The BRST charge and Hamiltonian for rank one theories |
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205 | (4) |
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11.5.2 FV Principal Theorem |
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209 | (2) |
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11.5.3 A large class of gauges |
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211 | (1) |
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11.5.4 Connecting Zψ with the quantum partition function in a physical gauge. The SU (N) Yang-Mills theory |
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212 | (3) |
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11.6 Equivalence of the SD and MCS models |
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215 | (6) |
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11.7 The physical Hilbert space. Some remarks |
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221 | (2) |
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12 Field-Antifield Quantization |
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223 | (48) |
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223 | (1) |
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12.2 Axiomatic field-antifield formalism |
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224 | (7) |
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12.3 Constructive proof of the field-antifield formalism for a restricted class of theories |
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231 | (16) |
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12.3.1 From the FV-phase-space action to the Hamiltonian master equation |
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232 | (6) |
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12.3.2 Transition to configuration space |
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238 | (9) |
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12.4 The Lagrangian master equation |
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247 | (6) |
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12.5 The quantum master equation |
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253 | (8) |
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12.5.1 An alternative derivation of the quantum master equation |
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256 | (3) |
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12.5.2 Gauge invariant correlation functions |
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259 | (2) |
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12.6 Anomalous gauge theories. The chiral Schwinger model |
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261 | (10) |
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12.6.1 Quantum Master equation and the anomaly |
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265 | (6) |
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A Local Symmetries and Singular Lagrangians |
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271 | (7) |
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A.1 Local symmetry transformations |
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271 | (3) |
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A.2 Bianchi identities and singular Lagrangians |
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274 | (4) |
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B The BRST Charge of Rank One |
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278 | (3) |
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C BRST Hamiltonian of Rank One |
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281 | (2) |
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D The FV Principal Theorem |
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283 | (4) |
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E BRST Quantization of SU (3) Yang-Mills Theory in α-gauges |
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287 | (4) |
Bibliography |
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291 | (10) |
Index |
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301 | |