The free-space Green function of the Laplacian for the Poisson equation gives the electric potential
For , its electric multipole expansion begins with
Define the total electric charge and electric dipole moment by
Then
The analogous solution for the magnetic vector potential is
Its apparent coefficient is . For each component, the supplied identity and the divergence-free vector field condition give
The divergence theorem turns this into a surface integral outside the compact support of the current density, where . Hence , so the term vanishes.

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