Difference between revisions of "O(3) Electrodynamics: A Second Reply to Hunter"
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− | 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.[[Category:Scientific Paper]] | + | 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. |
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+ | [[Category:Scientific Paper|o electrodynamics second reply hunter]] | ||
[[Category:Electrodynamics]] | [[Category:Electrodynamics]] |
Revision as of 10:47, 1 January 2017
Scientific Paper | |
---|---|
Title | O(3) Electrodynamics: A Second Reply to Hunter |
Read in full | Link to paper |
Author(s) | Myron W Evans |
Keywords | B(3), Stokes Theorem |
Published | 2000 |
Journal | Apeiron |
Volume | 7 |
Number | 1-2 |
No. of pages | 4 |
Pages | 29-32 |
Read the full paper here
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.