Question: Show that the Cartesian components of the transverse current density j(r, t) used to define the Coulomb gauge vector potential can be written in terms

Show that the Cartesian components of the transverse current density j⊥(r, t) used to define the Coulomb gauge vector potential can be written in terms of the total current density j(r, t) as

j_.x(x, t) = [ dr $ (r r')je(r', t), jL,k(r, -

where the transverse delta function is

j_.x(x, t) = [ dr $ (r r')je(r', t), jL,k(r, -

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