Difference between revisions of "O(3) Electrodynamics: A Second Reply to Hunter"

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==Abstract==
 
==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.[[Category:Scientific Paper]]
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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:Electrodynamics]]
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[[Category:Scientific Paper|o electrodynamics second reply hunter]]
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[[Category:Electrodynamics|o electrodynamics second reply hunter]]

Latest revision as of 19:45, 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.