We demonstrate how one can describe explicitly the present arbitrariness in solutions of relativistic wave equations in external electromagnetic fields of special form. This arbitrariness is connected to the existence of a transformation, which reduces eff
InthecaseoftheKlein-Gordonequation,theoperatorLz,
Lz=ih¯x 1 x 2,[Lz,P0]=[Lz,P3]=[K,Lz]=0, 21
canbeincluded(togetherwithP0andP3)inthecompletesetofintegralsofmotion,whereasfortheDiracequationcase,theoperatorJz,
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