proposition 26.19 Second-class constraints come in pairs

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proposition 26.19: Second-class constraints come in pairs26.19definition 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 26.17: Counting the physical degrees of freedom26.17theorem 26.21: Properties of the Dirac bracket26.21proof : ch:09-constrained-hamiltonian-dynamics@proof-7proofdefinition 26.11: The final constraint set26.11definition 22.29: Poisson bracket22.29proposition 26.13: The first-class functions close26.13proposition 26.34: Proca constraints are second class26.34definition 5.110: Bilinear map5.110definition 5.113: Non-degenerate form5.113definition 5.111: Symmetric and antisymmetric forms5.111equation 5.139: eq:lin-bilinear-congruence5.139definition 5.135: The symplectic group5.135definition 24.2: Symplectic vector space24.2proposition 24.3: Even dimension and the canonical basis24.3theorem A.68: DarbouxA.68theorem 5.138: A symplectic transformation has determinant +15.138proof : ch:03-linear-algebra-representations@proof-54proofdefinition 26.23: Gauge conditions26.23example 26.22: Holonomic constraints26.22theorem A.617: Jacobi identity for the Dirac bracketA.617remark 26.26: What the factor is doing26.26proof : ch:09-constrained-hamiltonian-dynamics@proof-10proofdefinition 24.20: Liouville volume24.20proposition A.619: The Dirac bracket is a projected Hamiltonian flowA.619proof : ch:09-constrained-hamiltonian-dynamics@proof-11proofremark 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.642proposition 26.32: Constraint structure of the free Maxwell field26.32proposition 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 26.8: Total Hamiltonian26.8postulate 26.47: Dirac quantization26.47neighborhood truncated

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typedirectionnode provenancewhere
depends_on First and second class declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:563
depends_on Normal form of a non-degenerate antisymmetric form declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:563
depends_on Dirac bracket declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:608
depends_on The Faddeev–Popov determinant declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:820
depends_on The Liouville measure of a second-class surface declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:876
depends_on Counting the physical degrees of freedom declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:490
depends_on Properties of the Dirac bracket declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:628
proves ch:09-constrained-hamiltonian-dynamics@proof-7 declared parts/03-classical-mechanics/09-constrained-hamiltonian-dynamics.tex:566