Abstract

In O(3) symmetry electrodynamics the field tensor is governed by a non-Abelian Stokes Theorem, as in any non-Abelian gauge theory. The comments on the B(3) component of this field tensor by Hunter in this Issue address B(3) as if it were a U(1) symmetry field, governed by the ordinary Stokes Theorem, and are therefore sequentially erroneous, because there is a basic misunderstanding of the nature of O(3) electrodynamics inherent in the article.