Knecht and Urech's result for n=2:

knechtsu2res =  1/12 * UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]]]] * UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[ν]], Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[ν]]]]] +  1/6 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], CovariantFieldDerivative[MM[x], x, LorentzIndex[ν]]]]^2 -  1/32 * (UTrace[NM[Adjoint[MM[x]], UMatrix[UChi[]][x]]] + UTrace[NM[Adjoint[UMatrix[UChi[]][x]], MM[x]]])^2 +  1/2 * (UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ1]]], CovariantFieldDerivative[UMatrix[UChi[]][x], x, LorentzIndex[μ1]]]] + UTrace[NM[Adjoint[CovariantFieldDerivative[UMatrix[UChi[]][x], x, LorentzIndex[μ1]]], CovariantFieldDerivative[MM[x], x, LorentzIndex[μ1]]]]) -  1/6 * UTrace[NM[GRight[LorentzIndex[μ], LorentzIndex[ν]][x], MM[x], GLeft[LorentzIndex[μ], LorentzIndex[ν]][x], Adjoint[MM[x]]]] -  I/6 * (UTrace[NM[GLeft[LorentzIndex[μ], LorentzIndex[ν]][x], Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], CovariantFieldDerivative[MM[x], x, LorentzIndex[ν]]] + NM[GRight[LorentzIndex[μ], LorentzIndex[ν]][x], CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[ν]]]]]) +  1/2 * UTrace[NM[Adjoint[UMatrix[UChi[]][x]], UMatrix[UChi[]][x]]] -  1/12 * (UTrace[NM[GLeft[LorentzIndex[μ], LorentzIndex[ν]][x], GLeft[LorentzIndex[μ], LorentzIndex[ν]][x]]] + UTrace[NM[GRight[LorentzIndex[μ], LorentzIndex[ν]][x], GRight[LorentzIndex[μ], LorentzIndex[ν]][x]]]) +  1/2 * ( Det[Adjoint[UMatrix[UChi[]][x]]] + Det[UMatrix[UChi[]][x]]) +  1/6 * FieldStrengthTensor[LorentzIndex[μ], QuantumField[Vector[1], LorentzIndex[ν]][x], x, Explicit -> False]^2 * UTrace[UMatrix[UChiralSpurion[]][x]]^2 -  3 * f^2/4 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]]] * (UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]]] + UTrace[NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]]) +  (3/4 - z) f^2 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]]] * UTrace[UMatrix[UChiralSpurion[]][x]]^2 +  2 * z * f^2 * UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]]]] * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] -  3 * f^2/4 * (UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], UMatrix[UChiralSpurionRight[]][x], MM[x]]] * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], UMatrix[UChiralSpurionRight[]][x], MM[x]]] + UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] * UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]]) +  2 * z * f^2 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], UMatrix[UChiralSpurionRight[]][x], MM[x]]] * UTrace[NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] -  f^2/8 * (UTrace[NM[Adjoint[UMatrix[UChi[]][x]], MM[x]]] + UTrace[NM[Adjoint[MM[x]], UMatrix[UChi[]][x]]]) * (UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]]] + UTrace[NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]]) -  z * f^2 * (UTrace[NM[Adjoint[UMatrix[UChi[]][x]], MM[x]]] + UTrace[NM[Adjoint[MM[x]], UMatrix[UChi[]][x]]]) * UTrace[NM[UMatrix[UChiralSpurion[]][x]]]^2 +  (1/4 + 2 * z) f^2 * (UTrace[NM[Adjoint[UMatrix[UChi[]][x]], MM[x]]] + UTrace[NM[Adjoint[MM[x]], UMatrix[UChi[]][x]]]) * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] +  (1/8 - z) * f^2 * UTrace[NM[NM[UMatrix[UChi[]][x], Adjoint[MM[x]]] - NM[MM[x], Adjoint[UMatrix[UChi[]][x]]], UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]] + NM[NM[Adjoint[UMatrix[UChi[]][x]], MM[x]] - NM[Adjoint[MM[x]], UMatrix[UChi[]][x]], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]], UMatrix[UChiralSpurionRight[]][x], MM[x]]] +  f^2/4 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], UCommutator[CQRight[LorentzIndex[μ]][x], UMatrix[UChiralSpurionRight[]][x]], MM[x]] + NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], UCommutator[CQLeft[LorentzIndex[μ]][x], UMatrix[UChiralSpurionLeft[]][x]], Adjoint[MM[x]]]] +  f^2/4 * UTrace[NM[Adjoint[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]]], UMatrix[UChiralSpurionRight[]][x], MM[x], CQLeft[LorentzIndex[μ]][x]] + NM[CovariantFieldDerivative[MM[x], x, LorentzIndex[μ]], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]], CQRight[LorentzIndex[μ]][x]]] +  (3/2 + 3 * z + 12 * z^2) * f^4 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]]^2 -  3 * f^4/2 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]] + NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]] -  (3 * z + 12 * z^2) * f^4 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], MM[x], UMatrix[UChiralSpurionLeft[]][x], Adjoint[MM[x]]]] * UTrace[UMatrix[UChiralSpurion[]][x]]^2 +  (3/8 - 3/4 * z + z^2) * f^4 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]] + NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]]^2 +  (3 * z/2 - 2 * z^2) * f^4 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]] + NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]] * UTrace[UMatrix[UChiralSpurion[]][x]]^2 -  z^2 * f^4 * UTrace[NM[UMatrix[UChiralSpurionRight[]][x], UMatrix[UChiralSpurionRight[]][x]] - NM[UMatrix[UChiralSpurionLeft[]][x], UMatrix[UChiralSpurionLeft[]][x]]]^2 +  4 * z^2 * f^4 * UTrace[UMatrix[UChiralSpurion[]][x]]^4

4 z^2 < Q >^4 f^4 - z^2 (< Q _ R '6 Q _ R > - < Q _ L '6 Q _ L >)^2 f^4 + (z^2 - (3 z)/4 + 3/8) (< Q _ L '6 Q _ L > + < Q _ R '6 Q _ R >)^2 f^4 + (12 z^2 + 3 z + 3/2) < Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† >^2 f^4 + ((3 z)/2 - 2 z^2) (< Q _ L '6 Q _ L > + < Q _ R '6 Q _ R >) < Q >^2 f^4 - (12 z^2 + 3 z) < Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† > < Q >^2 f^4 - 3/2 (< Q _ L '6 Q _ L > + < Q _ R '6 Q _ R >) < Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† > f^4 + (3/4 - z) < ÷s _ μ(÷„)^† '6 ÷s _ μ(÷„) > < Q >^2 f^2 - z (< ÷„^† '6 χ > + < χ^† '6 ÷„ >) < Q >^2 f^2 - 3/4 < ÷s _ μ(÷„)^† '6 ÷s _ μ(÷„) > (< Q _ L '6 Q _ L > + < Q _ R '6 Q _ R >) f^2 - 1/8 (< ÷„^† '6 χ > + < χ^† '6 ÷„ >) (< Q _ L '6 Q _ L > + < Q _ R '6 Q _ R >) f^2 + 1/4 (< ÷s _ μ(÷„)^† '6 (c _ μ^R Q _ R '6 Q _ R - Q _ R '6 c _ μ^R Q _ R) '6 ÷„ > + < ÷s _ μ(÷„) '6 (c _ μ^L Q _ L '6 Q _ L - Q _ L '6 c _ μ^L Q _ L) '6 ÷„^† >) f^2 + 2 z < ÷s _ μ(÷„)^† '6 Q _ R '6 ÷„ > < ÷s _ μ(÷„) '6 Q _ L '6 ÷„^† > f^2 - 3/4 (< ÷s _ μ(÷„)^† '6 Q _ R '6 ÷„ >^2 + < ÷s _ μ(÷„) '6 Q _ L '6 ÷„^† >^2) f^2 + 1/4 (< ÷s _ μ(÷„)^† '6 Q _ R '6 ÷„ '6 c _ μ^L Q _ L > + < ÷s _ μ(÷„) '6 Q _ L '6 ÷„^† '6 c _ μ^R Q _ R >) f^2 + (2 z + 1/4) (< ÷„^† '6 χ > + < χ^† '6 ÷„ >) < Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† > f^2 + 2 z < ÷s _ μ(÷„) '6 ÷s _ μ(÷„)^† > < Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† > f^2 + (1/8 - z) (< (χ^† '6 ÷„ - ÷„^† '6 χ) '6 Q _ L '6 ÷„^† '6 Q _ R '6 ÷„ > + < (χ '6 ÷„^† - ÷„ '6 χ^†) '6 Q _ R '6 ÷„ '6 Q _ L '6 ÷„^† >) f^2 + 1/6 < ÷s _ μ(÷„)^† '6 ÷s _ ν(÷„) >^2 - 1/32 (< ÷„^† '6 χ > + < χ^† '6 ÷„ >)^2 + 1/6 γ _ (μ ν)^2 < Q >^2 + 1/2 ({χ^†} + {χ}) + 1/2 (< ÷s _ μ _ 1(÷„)^† '6 ÷s _ μ _ 1(χ) > + < ÷s _ μ _ 1(χ)^† '6 ÷s _ μ _ 1(÷„) >) + 1/2 < χ^† '6 χ > + 1/12 < ÷s _ μ(÷„) '6 ÷s _ μ(÷„)^† > < ÷s _ ν(÷„) '6 ÷s _ ν(÷„)^† > + 1/12 (-< G _ (μ ν)^L '6 G _ (μ ν)^L > - < G _ (μ ν)^R '6 G _ (μ ν)^R >) - 1/6 i (< G _ (μ ν)^L '6 ÷s _ μ(÷„)^† '6 ÷s _ ν(÷„) > + < G _ (μ ν)^R '6 ÷s _ μ(÷„) '6 ÷s _ ν(÷„)^† >) - 1/6 < G _ (μ ν)^R '6 ÷„ '6 G _ (μ ν)^L '6 ÷„^† >


Converted by Mathematica  (July 10, 2003)