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light cone gauge : ウィキペディア英語版
light cone gauge

In theoretical physics, light cone gauge is an approach to remove the ambiguities arising from a gauge symmetry. While the term refers to several situations, a null component of a field ''A'' is set to zero (or a simple function of other variables) in all cases.〔(''The light cone gauge'' Samir D. Mathur )〕〔''QCD calculations in the light-cone gauge'' Nuclear Physics B - Volume 165, Issue 2, 24 March 1980, Pages 237–268 by D.J. Pritchard, W.J. Stirling ()〕
==Gauge theory==

In gauge theory, light-cone gauge refers to the condition A^+=0 where
:A^+ (x^0,x^1,x^2,x^3) = A^0 (x^0,x^1,x^2,x^3) +A^3 (x^0,x^1,x^2,x^3)
It is a method to get rid of the redundancies implied by Yang–Mills symmetry.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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