theorem 14.65 The two Casimir operators of the Poincaré algebra in $3+1$ dimensions

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theorem 14.65: The two Casimir operators of the Poincaré algebra in 3+1 dimensions14.65definition 14.63: Pauli–Lubanski vector14.63lemma 14.64: Properties of W14.64proposition 14.60: The quadratic invariant14.60example A.394: D = 4A.394proof : ch:12-lie-groups-fibre-bundles@proof-31proofequation 14.86: eq:lie-sopq-gen14.86equation 14.82: eq:lie-transl-gen14.82equation 14.90: eq:lie-algebrasopq14.90equation 14.97: eq:lie-jp-comm14.97equation 14.84: eq:lie-transl-comm14.84lemma 14.62: The Levi-Civita symbol is invariant14.62proof : ch:12-lie-groups-fibre-bundles@proof-30proofdefinition 14.8: Casimir element14.8proof : ch:12-lie-groups-fibre-bundles@proof-28prooftheorem A.385: Labels of a massive representationA.385theorem 14.43: The irreducible representations of su(2)14.43

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typedirectionnode provenancewhere
depends_on Pauli–Lubanski vector declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2903
depends_on Properties of $W$ declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2903
depends_on The quadratic invariant declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2903
depends_on $D = 4$ declared appendices/A-long-proofs.tex:19324
proves ch:12-lie-groups-fibre-bundles@proof-31 declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2906