theorem 26.17 Counting the physical degrees of freedom

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theorem 26.17: Counting the physical degrees of freedom26.17proposition 26.19: Second-class constraints come in pairs26.19remark 26.18: The Frobenius theorem is owed by Part II26.18theorem 26.14: First-class constraints generate gauge transformations26.14corollary A.642: The constraints are first classA.642definition 26.23: Gauge conditions26.23proposition 26.32: Constraint structure of the free Maxwell field26.32proposition 26.34: Proca constraints are second class26.34proposition 26.29: Reparametrization invariance and the mass-shell constraint26.29theorem 26.42: The Hamiltonian structure of general relativity26.42proof : ch:09-constrained-hamiltonian-dynamics@proof-6proofdefinition 26.12: First and second class26.12proposition 5.119: Normal form of a non-degenerate antisymmetric form5.119definition 26.20: Dirac bracket26.20proposition 26.24: The Faddeev–Popov determinant26.24proposition 26.25: The Liouville measure of a second-class surface26.25theorem 26.21: Properties of the Dirac bracket26.21proof : ch:09-constrained-hamiltonian-dynamics@proof-7proofdefinition 26.8: Total Hamiltonian26.8proposition 26.10: The four outcomes26.10definition 26.16: Extended Hamiltonian26.16postulate 26.47: Dirac quantization26.47proof : ch:09-constrained-hamiltonian-dynamics@proof-5proofproposition A.639: The first two bracketsA.639theorem A.641: The normal–normal bracketA.641proof : app:A-long-proofs@proof-388proofproposition 26.5: Primary constraints26.5proposition 26.37: Constraint structure of Yang–Mills theory26.37proof : ch:09-constrained-hamiltonian-dynamics@proof-13proofproposition 113.3: Degrees of freedom before and after113.3proof : ch:09-constrained-hamiltonian-dynamics@proof-14prooftheorem 40.5: Energy–momentum relation40.5proof : ch:09-constrained-hamiltonian-dynamics@proof-12proofproposition 26.41: The ADM form of the Einstein–Hilbert Lagrangian26.41notation A.636: Densities and smearingA.636proposition 26.43: The hypersurface-deformation algebra26.43proof : ch:09-constrained-hamiltonian-dynamics@proof-16proof

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typedirectionnode provenancewhere
depends_on Second-class constraints come in pairs declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:490
depends_on The Frobenius theorem is owed by Part II declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:490
depends_on First-class constraints generate gauge transformations declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:490
depends_on The constraints are first class declared appendices/A-long-proofs.tex:31367
depends_on Gauge conditions declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:792
depends_on Constraint structure of the free Maxwell field declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:1174
depends_on Proca constraints are second class declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:1299
depends_on Reparametrization invariance and the mass-shell constraint declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:1071
depends_on The Hamiltonian structure of general relativity declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:1649
proves ch:09-constrained-hamiltonian-dynamics@proof-6 declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:493