The evaluated leading order Lagrangian:
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Redundant terms are discarded:
![lll = DiscardTerms[ll, Retain -> {Particle[PhiMeson , RenormalizationState[0]] -> 5, Particle[Scalar[1], RenormalizationState[0]] -> 1}, CommutatorReduce -> True, Method -> Expand] // Simplify ;](../HTMLFiles/index_303.gif)
Generator matrices are traced:
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Indices are supplied:
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Calculation of the Feynman rule:
![fields = {QuantumField[Particle[PhiMeson, RenormalizationState[0]], 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], QuantumField[Particle[Scalar[1], RenormalizationState[0]]][p6]}](../HTMLFiles/index_307.gif)
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![melsimplified = CheckF[((WriteString["stdout", "."] ; Simplify[I * SUNReduce[SUNReduce[SUNReduce[FunctionalD[#, fields] // Contract]]]]) & /@ lal), "ChPTW3-5meson-melsimplified"] ;](../HTMLFiles/index_312.gif)
Another check that two different evaluations with specific components give the same result:
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Converted by Mathematica (July 10, 2003)