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1 Sketch of Lagrangian Formalism |
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1 | (76) |
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1 | (7) |
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1.2 Galilean Transformations: Principle of Galilean Relativity |
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8 | (5) |
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1.3 Poincare and Lorentz Transformations: The Principle of Special Relativity |
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13 | (10) |
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1.4 Principle of Least Action |
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23 | (1) |
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24 | (5) |
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1.6 Generalized Coordinates, Corrdinate Transformations and Symmetries of an Action |
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29 | (7) |
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1.7 Examples of Continuous (Field) Systems |
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36 | (8) |
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1.8 Action of a Constrained System: The Recipe |
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44 | (7) |
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1.9 Action of a Constrained System: Justification of the Recipe |
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51 | (1) |
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1.10 Description of Constrained System by Singular Action |
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52 | (2) |
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1.11 Kinetic Versus Potential Energy: Forceless Mechanics of Hertz |
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54 | (2) |
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1.12 Electromagnetic Field in Lagrangian Formalism |
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56 | (21) |
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56 | (3) |
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1.12.2 Nonsingular Lagrangian Action of Electrodynamics |
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59 | (4) |
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1.12.3 Manifestly Poincare-Invariant Formulation in Terms of a Singular Lagrangian Action |
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63 | (2) |
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1.12.4 Notion of Local (Gauge) Symmetry |
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65 | (3) |
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1.12.5 Lorentz Transformations of Three-Dimensional Potential: Role of Gauge Symmetry |
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68 | (1) |
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1.12.6 Relativistic Particle on Electromagnetic Background |
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69 | (3) |
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1.12.7 Poincare Transformations of Electric and Magnetic Fields |
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72 | (5) |
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77 | (42) |
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2.1 Derivation of Hamiltonian Equations |
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77 | (8) |
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77 | (2) |
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2.1.2 From Lagrangian to Hamiltonian Equations |
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79 | (4) |
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2.1.3 Short Prescription for Hamiltonization Procedure, Physical Interpretation of Hamiltonian |
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83 | (2) |
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2.1.4 Inverse Problem: From Hamiltonian to Lagrangian Formulation |
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85 | (1) |
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2.2 Poisson Bracket and Symplectic Matrix |
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85 | (2) |
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2.3 General Solution to Hamiltonian Equations |
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87 | (4) |
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2.4 Picture of Motion in Phase Space |
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91 | (2) |
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2.5 Conserved Quantities and the Poisson Bracket |
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93 | (3) |
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2.6 Phase Space Transformations and Hamiltonian Equations |
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96 | (4) |
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2.7 Definition of Canonical Transformation |
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100 | (2) |
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2.8 Generalized Hamiltonian Equations: Example of Non-canonical Poisson Bracket |
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102 | (4) |
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2.9 Hamiltonian Action Functional |
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106 | (1) |
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2.10 Schrodinger Equation as the Hamiltonian System |
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107 | (6) |
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2.10.1 Lagrangian Action Associated with the Schrodinger Equation |
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108 | (3) |
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2.10.2 Probability as a Conserved Charge Via the Noether Theorem |
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111 | (2) |
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2.11 Hamiltonization Procedure in Terms of First-Order Action Functional |
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113 | (1) |
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2.12 Hamiltonization of a Theory with Higher-Order Derivatives |
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114 | (5) |
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114 | (2) |
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2.12.2 Ostrogradsky Method |
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116 | (3) |
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3 Canonical Transformations of Two-Dimensional Phase Space |
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119 | (8) |
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3.1 Time-Independent Canonical Transformations |
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119 | (4) |
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3.1.1 Time-Independent Canonical Transformations and Symplectic Matrix |
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119 | (2) |
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3.1.2 Generating Function |
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121 | (2) |
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3.2 Time-Dependent Canonical Transformations |
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123 | (4) |
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3.2.1 Canonical Transformations and Symplectic Matrix |
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123 | (2) |
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3.2.2 Generating Function |
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125 | (2) |
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4 Properties of Canonical Transformations |
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127 | (28) |
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4.1 Invariance of the Poisson Bracket (Symplectic Matrix) |
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128 | (5) |
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4.2 Infinitesimal Canonical Transformations: Hamiltonian as a Generator of Evolution |
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133 | (3) |
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4.3 Generating Function of Canonical Transformation |
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136 | (4) |
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4.3.1 Free Canonical Transformation and Its Function F(q1, p1, τ) |
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136 | (1) |
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4.3.2 Generating Function S(q, q1, τ) |
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137 | (3) |
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4.4 Examples of Canonical Transformations |
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140 | (5) |
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4.4.1 Evolution as a Canonical Transformation: Invariance of Phase-Space Volume |
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140 | (3) |
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4.4.2 Canomical Transformations in Perturbation Theory |
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143 | (1) |
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4.4.3 Coordinates Adjusted to a Surface |
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144 | (1) |
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4.5 Transformation Properties of the Hamiltonian Action |
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145 | (1) |
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4.6 Summary: Equivalent Definitions for Canonical Transformation |
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146 | (1) |
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4.7 Hamilton-Jacobi Equation |
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147 | (4) |
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4.8 Action Functional as a Generating Function of Evolution |
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151 | (4) |
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155 | (12) |
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5.1 Poincare-Cartan Integral Invariant |
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155 | (7) |
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155 | (2) |
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5.1.2 Line Integral of a Vector Field, Hamiltonian Action, Poincare-Cartan and Poincare Integral Invariants |
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157 | (2) |
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5.1.3 Invariance of the Poincare-Cartan Integral |
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159 | (3) |
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5.2 Universal Integral Invariant of Poincare |
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162 | (5) |
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6 Potential Motion in a Geometric Setting |
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167 | (36) |
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6.1 Analysis of Trajectories and the Principle of Maupertuis |
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167 | (7) |
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6.1.1 Trajectory: Separation of Kinematics from Dynamics |
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168 | (2) |
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6.1.2 Equations for Trajectory in the Hamiltonian Formulation |
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170 | (1) |
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6.1.3 The Principle of Maupertuis for Trajectories |
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171 | (1) |
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6.1.4 Lagrangian Action for Trajectories |
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172 | (2) |
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6.2 Description of a Potential Motion in Terms of a Pair of Riemann Spaces |
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174 | (4) |
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6.3 Some Notions of Riemann Geometry |
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178 | (11) |
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178 | (5) |
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6.3.2 Covariant Derivative and Riemann Connection |
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183 | (2) |
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6.3.3 Parallel Transport: Notions of Covariance and Coordinate Independence |
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185 | (4) |
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6.4 Definition of Covariant Derivative Through Parallel Transport: Formal Solution to the Parallel Transport Equation |
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189 | (2) |
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6.5 The Geodesic Line and Its Reparametrization Covariant Equation |
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191 | (2) |
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6.6 Example: A Surface Embedded in Euclidean Space |
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193 | (3) |
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6.7 Shortest Line and Geodesic Line: One More Example of a Singular Action |
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196 | (4) |
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6.8 Formal Geometrization of Mechanics |
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200 | (3) |
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7 Transformations, Symmetries and Noether Theorem |
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203 | (34) |
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7.1 The Notion of Invariant Action Functional |
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203 | (3) |
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7.2 Coordinate Transformation, Induced Transformation of Functions and Symmetries of an Action |
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206 | (5) |
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7.3 Examples of Invariant Actions, Galileo Group |
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211 | (3) |
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7.4 Poincare Group, Relativistic Particle |
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214 | (1) |
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7.5 Symmetries of Equations of Motion |
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215 | (3) |
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218 | (2) |
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7.7 Infinitesimal Symmetries |
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220 | (3) |
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7.8 Discussion of the Noether Theorem |
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223 | (1) |
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7.9 Use of Noether Charges for Reduction of the Order of Equations of Motion |
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224 | (1) |
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225 | (3) |
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7.11 Symmetries of Hamiltonian Action |
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228 | (9) |
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7.11.1 Infinitesimal Symmetries Given by Canonical Transformations |
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228 | (2) |
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7.11.2 Structure of Infinitesimal Symmetry of a General Form |
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230 | (4) |
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7.11.3 Hamiltonian Versus Lagrangian Global Symmetry |
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234 | (3) |
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8 Hamiltonian Formalism for Singular Theories |
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237 | (66) |
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8.1 Hamiltonization of a Singular Theory: The Recipe |
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238 | (9) |
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238 | (4) |
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242 | (5) |
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8.2 Justification of the Hamiltonization Recipe |
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247 | (7) |
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8.2.1 Configuration-Velocity Space |
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247 | (2) |
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249 | (3) |
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8.2.3 Comparison with the Dirac Recipe |
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252 | (2) |
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8.3 Classification of Constraints |
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254 | (1) |
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8.4 Comment on the Physical Interpretation of a Singular Theory |
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255 | (4) |
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8.5 Theory with Second-Class Constraints: Dirac Bracket |
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259 | (3) |
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8.6 Examples of Theories with Second-Class Constraints |
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262 | (4) |
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8.6.1 Mechanics with Kinematic Constraints |
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262 | (2) |
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8.6.2 Singular Lagrangian Action Underlying the Schrodinger Equation |
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264 | (2) |
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8.7 Examples of Theories with First-Class Constraints |
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266 | (8) |
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266 | (2) |
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8.7.2 Semiclassical Model for Description of Non Relativistic Spin |
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268 | (6) |
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8.8 Local Symmetries and Constraints |
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274 | (7) |
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8.9 Local Symmetry Does Not Imply a Conserved Charge |
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281 | (1) |
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8.10 Formalism of Extended Lagrangian |
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281 | (5) |
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8.11 Local Symmetries of the Extended Lagrangian: Dirac Conjecture |
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286 | (4) |
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8.12 Local Symmetries of the Initial Lagrangian |
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290 | (3) |
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8.13 Conversion of Second-Class Constraints by Deformation of Lagrangian Local Symmetries |
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293 | (10) |
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8.13.1 Conversion in a Theory with Hidden SO(1, 4) Global Symmetry |
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296 | (2) |
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8.13.2 Classical Mechanics Subject to Kinematic Constraints as a Gauge Theory |
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298 | (3) |
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8.13.3 Conversion in Maxwell-Proca Lagrangian for Massive Vector Field |
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301 | (2) |
Bibliography |
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303 | (2) |
Index |
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305 | |