Physics Asked by hyportnex on February 4, 2021
In https://arxiv.org/abs/hep-ph/0010057 the following vector calculus equality is claimed without proof although in note [4] the cryptic comment is made that "The relation is essentially the momentum space identity $(mathbf{k}timesmathbf{A})^2=mathbf{k}^2mathbf{A}^2-(mathbf{k}mathbf{A})^2$ in position space":
Indeed there is the vector relation:
begin{align}
int mathbf{A}^2(x)d^3 x
& = frac{1}{4pi} int d^3 x d^3 x’ frac{[nabla times mathbf{A}(x)] cdot [nabla timesmathbf{A}(x’)]}{vert mathbf{x}-mathbf{x’} vert}
& qquad + frac{1}{4pi} int d^3 x d^3 x’ frac{[nabla cdot mathbf{A}(x)] [nabla cdot mathbf{A}(x’)]}{vert mathbf{x}-mathbf{x’} vert} tag{6}label{6}
& qquad + rm{surface terms}
end{align}
Each of the two terms is positive; hence (up to the surface term question) we can minimize the integral of $mathbf{A}^2$ by choosing $nabla cdot mathbf{A} = 0.$ With this choice the integral of $mathbf{A}^2$ is minimal in accord with our above remarks and is expressed only in terms of the magnetic field $nabla times mathbf{A}$
This $eqref{6}$ is indeed a very interesting identity and Gubarev, et al, go on to show it also in relativistically invariant form.
When $mathbf{A}$ is the vector potential, $mathbf{B}=nablatimesmathbf{A}$, then in the Coulomb gauge $nablacdotmathbf{A}=0$ and
$$int mathbf{A}^2(x)d^3 x = frac{1}{4pi} int d^3 x d^3 x’ frac{mathbf{B}(x) cdot mathbf{B}(x’)}{vert mathbf{x}-mathbf{x’} vert} + rm{surface terms}$$
Ignoring the "surface terms" in the infinity and assuming that the integrals of $eqref{6}$ are positive indeed then we have the gauge independent minimum on the right side dependent only on the $mathbf{B}$ field:
$$int mathbf{A}^2(x)d^3 x ge frac{1}{4pi} int d^3 x d^3 x’ frac{mathbf{B}(x) cdot mathbf{B}(x’)}{vert mathbf{x}-mathbf{x’} vert}.$$
I have two questions:
As @flevinBombastus has suggested here is a sketch of the proof of the equality in Equation $(6)$ based on [1]. Start with $$nabla^2frac{1}{|mathbf x - mathbf x'|}=-delta(mathbf x - mathbf x')$$ and $$nabla times (nabla times mathbf v)=nabla (nablacdot mathbf v) - nabla^2 mathbf v$$ Then $$mathbf{A}(mathbf x) = int d^3x' mathbf{A}(mathbf x')delta(mathbf x - mathbf x') =-int d^3x' mathbf{A}(mathbf x')nabla'^2frac{1}{|mathbf x - mathbf x'|},$$ therefore $$int d^3x mathbf{A}(mathbf x)cdotmathbf{A}(mathbf x)=-intint d^3x d^3x' mathbf{A}(mathbf x)cdot mathbf{A}(mathbf x')nabla'^2frac{1}{|mathbf x - mathbf x'|}$$
Now integrate RHS by parts over $mathbf x'$. If $mathbf A$ vanishes at infinity then the surface term will vanish, and after some more rearrangements and partial integration we get the required identity Eq. (6). Interestingly, the same procedure also works for the scalar product of two vector fields. This takes care of the 1st question.
[1] Durand: "On an identity for the volume integral of the square of a vector field,” Am.J.Phys. 75 (6), June 2007
Answered by hyportnex on February 4, 2021
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