|
gptkbp:instanceOf
|
gptkb:gauge_theory
|
|
gptkbp:basedOn
|
gptkb:SU(2)_group
|
|
gptkbp:describes
|
gptkb:weak_interaction
|
|
gptkbp:dimensions
|
three generators
|
|
gptkbp:form
|
gptkb:Lie_group
|
|
gptkbp:hasApplication
|
gptkb:lattice_gauge_theory
condensed matter physics
particle physics
|
|
gptkbp:hasChiralFermions
|
true
|
|
gptkbp:hasCouplingConstant
|
g
|
|
gptkbp:hasCovariantDerivative
|
D_μ
|
|
gptkbp:hasFieldStrengthTensor
|
F^a_{μν}
|
|
gptkbp:hasGaugeBoson
|
gptkb:W_boson
gptkb:Z_boson
photon (after symmetry breaking)
|
|
gptkbp:hasGaugeField
|
A^a_μ
|
|
gptkbp:hasLagrangian
|
Yang-Mills Lagrangian
|
|
gptkbp:hasLocalSymmetry
|
gptkb:SU(2)
|
|
gptkbp:hasPhysicalImplication
|
asymptotic freedom
confinement (in pure gauge theory)
|
|
gptkbp:hasSpontaneousSymmetryBreaking
|
SU(2) × U(1) → U(1)
|
|
https://www.w3.org/2000/01/rdf-schema#label
|
SU(2) gauge theory
|
|
gptkbp:isNonAbelian
|
true
|
|
gptkbp:isSimple
|
true
|
|
gptkbp:partOf
|
electroweak theory
|
|
gptkbp:relatedTo
|
gptkb:Yang-Mills_theory
|
|
gptkbp:represents
|
adjoint representation
fundamental representation
|
|
gptkbp:studiedIn
|
gptkb:quantum_field_theory
|
|
gptkbp:symmetry
|
non-abelian
|
|
gptkbp:usedIn
|
gptkb:Standard_Model
|
|
gptkbp:bfsParent
|
gptkb:'t_Hooft–Polyakov_monopole
gptkb:Seiberg–Witten_solution
|
|
gptkbp:bfsLayer
|
7
|