theorem 14.57 $\vect{3}\otimes\bar{\vect{3}} = \vect{1}\oplus\vect{8}$

open in the book · parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2283 · p. 567

Rests on

Supports

Neighborhood

Every logical edge within two steps of this node.

theorem 14.57: \vect3\otimes\bar\vect3 = \vect1\oplus\vect814.57proposition 14.55: The fundamental, the antifundamental and the adjoint14.55proposition 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-6proofcorollary 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 102.12: Which quark combinations can be colour singlets102.12proof : ch:12-lie-groups-fibre-bundles@proof-25proofdefinition 102.5: Quarks102.5equation 14.81: eq:lie-su3-3x3bar14.81experiment : Deep Inelastic Scatteringexperime…phenomenon 116.38: The quark spins do not account for the proton spin116.38phenomenon 102.9: The \Delta^++ violates the spin-statistics theorem102.9phenomenon 102.7: The nucleon magnetic moments come out right102.7proposition 116.29: The Gross–Llewellyn Smith sum rule in the parton model116.29proof : ch:04-qcd@proof-3proof

Edges

typedirectionnode provenancewhere
depends_on The fundamental, the antifundamental and the adjoint declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2289
depends_on Mesons are $q\bar{q}$, baryons are $qqq$ declared parts/11-qft-standard-model/04-qcd.tex:320
proves ch:12-lie-groups-fibre-bundles@proof-26 declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2292
proves ch:12-lie-groups-fibre-bundles@prooflink-6 declared parts/02-mathematical-methods/12-lie-groups-fibre-bundles.tex:2170