We use an alternative notation for the lowest order lagrangian (in minkowski
space the minus of euclidean space goes),
![lag = 1/4 DecayConstant[PhiMeson]^2 (UTrace[NM[USmall[LorentzIndex[μ1]][x], USmall[LorentzIndex[μ1]][x]] + UChiPlus[x]])](../HTMLFiles/index_15.gif)
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Which is easily seen to agree with the usual one,
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Perturbation around the solution of the equation of motion, keeping only the
squared terms.
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![1/4 (2 < ∂ _ μ _ 1(Overscript[ξ^( ), ->]) · Overscript[σ, ->] '6 ∂ _ μ _ 1(Overscript[ξ^( ), ->]) · Overscript[σ, ->] > + 4 < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 ∂ _ μ _ 1(Overscript[ξ^( ), ->]) · Overscript[σ, ->] '6 Γ _ μ _ 1 > - 4 < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Γ _ μ _ 1 '6 ∂ _ μ _ 1(Overscript[ξ^( ), ->]) · Overscript[σ, ->] > - < χ _ + '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] > - 4 < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Γ _ μ _ 1 '6 Γ _ μ _ 1 > - < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 u _ μ _ 1 '6 u _ μ _ 1 > + 4 < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Γ _ μ _ 1 '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 Γ _ μ _ 1 > + < Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 u _ μ _ 1 '6 Overscript[ξ^( ), ->] · Overscript[σ, ->] '6 u _ μ _ 1 >)](../HTMLFiles/index_22.gif)
Writing out with indices.
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Converted by Mathematica (July 10, 2003)