|
gptkbp:instanceOf
|
gptkb:Lie_group
|
|
gptkbp:adjoint_representation_dimension
|
8
|
|
gptkbp:associatedWith
|
gptkb:special_unitary_group_SU(3)
|
|
gptkbp:basisFor
|
gptkb:Gell-Mann_matrices
|
|
gptkbp:Cartan_subalgebra_dimension
|
2
|
|
gptkbp:centralTo
|
trivial
|
|
gptkbp:compact
|
true
|
|
gptkbp:complexification
|
gptkb:sl(3,C)
|
|
gptkbp:dimensions
|
8
|
|
gptkbp:dual_Coxeter_number
|
3
|
|
gptkbp:Dynkin_diagram
|
two nodes connected by a single edge
|
|
gptkbp:field
|
complex numbers
|
|
gptkbp:fundamental_representation_dimension
|
3
|
|
gptkbp:highest_weight_representations
|
labeled by two non-negative integers
|
|
https://www.w3.org/2000/01/rdf-schema#label
|
Lie algebra su(3)
|
|
gptkbp:isSimple
|
true
|
|
gptkbp:Killing_form
|
non-degenerate
|
|
gptkbp:rank
|
2
|
|
gptkbp:realForm
|
gptkb:su(3)
|
|
gptkbp:relatedTo
|
quark model
eightfold way
|
|
gptkbp:structure_constants
|
f^{abc}
|
|
gptkbp:type
|
gptkb:A2
|
|
gptkbp:usedIn
|
gptkb:quantum_chromodynamics
particle physics
representation theory
theory of strong interactions
|
|
gptkbp:Weyl_group
|
gptkb:symmetric_group_S_3
|
|
gptkbp:bfsParent
|
gptkb:Gell-Mann_matrices
|
|
gptkbp:bfsLayer
|
5
|