The evaluated leading order Lagrangian:
![]()
Redundant terms are discarded:
![lll = DiscardTerms[ll, Retain -> {Particle[PhiMeson , RenormalizationState[0]] -> 4, Particle[AxialVector[0] , RenormalizationState[0]] -> 1}, CommutatorReduce -> True, Method -> Coefficient] // Simplify ;](../HTMLFiles/index_144.gif)
Generator matrices are traced:
![]()
Indices are supplied:
![]()
![]()
Calculation of the Feynman rule:
![fields = {QuantumField[Particle[AxialVector[0], RenormalizationState[0]], LorentzIndex[μ1], SUNIndex[I1]][p1], QuantumField[Particle[PhiMeson, RenormalizationState[0]], SUNIndex[I2]][p2], QuantumField[Particle[PhiMeson, RenormalizationState[0]], SUNIndex[I3]][p3], QuantumField[Particle[PhiMeson, RenormalizationState[0]], SUNIndex[I4]][p4], QuantumField[Particle[PhiMeson, RenormalizationState[0]], SUNIndex[I5]][p5]}](../HTMLFiles/index_148.gif)
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![]()
![melsimplified = CheckF[I * (If[Head[lal] == Plus, Plus @@ ((WriteString["stdout", "."] ; IndicesCleanup[Contract[FunctionalD[PhiToFC[#], fields]] // SUNReduce // SUNReduce // SUNReduce // SUNReduce // SUNReduce // SUNReduce]) & /@ (List @@ lal))]), "A4MesonWeakMel"] ;](../HTMLFiles/index_160.gif)
.......................................................................................................................................................................................................................................................................................................................................................
![]()
![]()
Converted by Mathematica (July 10, 2003)