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By C. Shores, et. al.,

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6 6 ) : f f zeD*, t s r . 50). 1) and applying ( 2 . 3 ) we o b t a i n . f K(C , t ) < p ( t ) d t (a+ f i c r v v M V + ~ ^ f t c = < „' - V r - 2 4 ! - ' t where E i s i d e n t i t y m a t r i x o f o r d e r n. 5, r where found, |K(t) = (^ ( t ) ,. , ^ ( 1 ) ) l defined on i s n-dimensional t h e contour T, 30 v e c t o r - f u n c t i o n t o be t h e elements o f which satisfy Holder's condition. 5) t h e v e c t o r - f u n c t i o n of Holder, o f any a n a l y t i c ( 2 . 5 ) i s due t o t h e f a c t p i s an a r b i t r a r y i .

69) . 1) . 59) equation j (£+ i ( t , £ ) ) ( H t ) - X ( t ) ) K p o 0 t o equation ( 2 . 2). 74) r to the Sokhotzky-Plemelj's 1 limit at z^t sr, o zeD* in (2,74) and applying f o r m u l a , we o b t a i n : , i 44 f K(t t) ( (t)-X(t))dt V ! , . 73) Similarly, + c 5ffi J_ — f=£; 2 as : *(t )-Jt(t )-tr(t ), t o (

17). 17) . 25) 1 gej? 26) by: the branch satisfying the conditions: / B -iaf 2 I m / B*-4af From e q u a t i o n s ( 3 . 29) >0 a t e <4a£. 17) 1 . 1 ) . 17) 2 with the order of regularity I t is satisfies o f Theorem solvable 52 that: ReA (0)=0. 2). 1) t h e i s proved. 3,2. 1. The f u n c t i o n f ( x ) belongs t o t h e c l a s s C^(R'), i f i t infinitely differentiable in R and i s equal t o zero outside o fa segment. 19) C™(R') . 8 when o f electromagnetic f i e l d a t t h e great values o f t .

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