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The evaluated leading order Lagrangian:
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Redundant terms are discarded:
![lll = DiscardTerms[ll, Retain -> {Particle[PhiMeson , RenormalizationState[0]] -> 1, Particle[PseudoScalar[0] , RenormalizationState[0]] -> 1, Particle[Scalar[1], RenormalizationState[0]] -> 1}, CommutatorReduce -> True, Method -> Expand] // Simplify](../HTMLFiles/index_12.gif)
![(2 c _ 5^( ) !, _ 0^( ) s^( ) (< σ^6 '6 Overscript[p^( ), ->] · Overscript[σ, ->] '6 Overscript[ϕ^( ), ->] · Overscript[σ, ->] > + < σ^6 '6 Overscript[ϕ^( ), ->] · Overscript[σ, ->] '6 Overscript[p^( ), ->] · Overscript[σ, ->] > + 2 < σ^6 '6 Overscript[ϕ^( ), ->] · Overscript[σ, ->] > p^( )^0))/f _ ϕ^(ó )](../HTMLFiles/index_13.gif)
Generator matrices are traced:
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Indices are supplied:
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Calculation of the Feynman rule:
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Another check that two different evaluations with specific components give the same result:
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Converted by Mathematica (July 10, 2003)