proposition 14.55 The fundamental, the antifundamental and the adjoint

open in the book · parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2207 · p. 566

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proposition 14.55: The fundamental, the antifundamental and the adjoint14.55corollary 14.18: A Casimir acts as a number on an irreducible representation14.18definition 14.51: Gell-Mann basis14.51proposition 14.53: Killing form of su(3)14.53corollary A.377: The adjoint representation is irreducibleA.377example A.358: Rank two: su(3)A.358theorem 14.57: \vect3\otimes\bar\vect3 = \vect1\oplus\vect814.57theorem 102.12: Which quark combinations can be colour singlets102.12proof : ch:12-lie-groups-fibre-bundles@proof-25proofdefinition 14.8: Casimir element14.8equation 14.6: eq:lie-expgen14.6remark 14.6: What U(g) is for14.6theorem 5.158: Schur's first lemma5.158theorem A.354: Harish-Chandra, quoted: the labels separateA.354proof : ch:12-lie-groups-fibre-bundles@proof-6proofdefinition 14.49: The special unitary group in three dimensions14.49lemma A.371: The generating traceA.371proposition 14.52: Structure constants and the symmetric tensor14.52equation 14.15: eq:lie-killing-components14.15theorem 14.13: Cartan's criterion14.13proposition 14.54: The two Casimir operators of su(3)14.54proof : ch:12-lie-groups-fibre-bundles@proof-23prooftheorem A.376: su(3) is simpleA.376proof : app:A-long-proofs@proof-232prooftheorem A.346: RacahA.346proposition 102.6: Mesons are q\barq, baryons are qqq102.6proof : ch:12-lie-groups-fibre-bundles@proof-26proofproof : ch:12-lie-groups-fibre-bundles@prooflink-6proofdefinition 102.10: Colour102.10corollary 102.13: The selection rule of the eightfold way102.13proof : ch:04-qcd@proof-5proof

Edges

typedirectionnode provenancewhere
depends_on A Casimir acts as a number on an irreducible representation declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2227
depends_on Gell-Mann basis declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2227
depends_on Killing form of $\mathfrak{su}(3)$ declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2227
depends_on The adjoint representation is irreducible declared appendices/A-long-proofs.tex:18438
depends_on Rank two: $\mathfrak{su}(3)$ declared appendices/A-long-proofs.tex:17278
depends_on $\vect{3}\otimes\bar{\vect{3}} = \vect{1}\oplus\vect{8}$ declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2289
depends_on Which quark combinations can be colour singlets declared parts/11-qft-standard-model/04-qcd.tex:508
proves ch:12-lie-groups-fibre-bundles@proof-25 declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2230