Savart

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The Stewart–Walker lemma provides necessary and sufficient conditions for the linear perturbation of a tensor field to be gauge-invariant. ΔδT=0 if and only if one of the following holds

1. T0=0

2. T0 is a constant scalar field

3. T0 is a linear combination of products of delta functions δab

Derivation

A 1-parameter family of manifolds denoted by ϵ with 0=4 has metric gik=ηik+ϵhik. These manifolds can be put together to form a 5-manifold 𝒩. A smooth curve γ can be constructed through 𝒩 with tangent 5-vector X, transverse to ϵ. If X is defined so that if ht is the family of 1-parameter maps which map 𝒩𝒩 and p00 then a point pϵϵ can be written as hϵ(p0). This also defines a pull back hϵ* that maps a tensor field Tϵϵ back onto 0. Given sufficient smoothness a Taylor expansion can be defined

hϵ*(Tϵ)=T0+ϵhϵ*(XTϵ)+O(ϵ2)

δT=ϵhϵ*(XTϵ)ϵ(XTϵ)0 is the linear perturbation of T. However, since the choice of X is dependent on the choice of gauge another gauge can be taken. Therefore the differences in gauge become ΔδT=ϵ(XTϵ)0ϵ(YTϵ)0=ϵ(XYTϵ)0. Picking a chart where Xa=(ξμ,1) and Ya=(0,1) then XaYa=(ξμ,0) which is a well defined vector in any ϵ and gives the result

ΔδT=ϵξT0.

The only three possible ways this can be satisfied are those of the lemma.

Sources

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