Show that the Cartesian components of the transverse current density j(r, t) used to define the Coulomb
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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
where the transverse delta function is
Transcribed Image Text:
j_.x(x, t) = [ d³r¹ $ž (r— r')je(r', t), jL,k(r, -
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