1550251515-Classical_Complex_Analysis__Gonzalez_

(jair2018) #1
726

z - b = r2ei62,

A= IAleilT


Then

!( )
z -_ vi Ah r2 e (1/2)i(^111 +o^2 -2w+1!"+2k1r) ,
r

from which we select


fo(z) = vJAhr2 e(l/2)i(o 1 +o 2 -2w+1l")

r

= i vJAhr2 e(1/2)i(o 1 +o 2 -2w)

r

Chapter9

k = 0,1

resulting in a distribution of values of fo(z) along the x =axis as follows:
For 0 < z = x < a we find that

JO^1 ( ) _ X - -z. ./JAhr2

r

For z x > b,

For a < z = x < b, and x on the upper boundary of the cut,

fo(x) = i vlAlr1r2 ei1r/2 = _ vlAhr2


r r
For a < z = x < b, and x on the lower boundary,

fo(x) = i vlAhr2 ei1r/2 = vlAJr1r2
r r

Next, consider a circler+: z = Rei^6 , 0:::; (J:::; 271", with R > b, a small

circle 1i: z = rei^6 , 0 :::; (J :::; 271", with 0 < r < a, and a contour >. consisting


of the lower boundary of the cut from a+E to b-E [O < E < min(a-r, R-b)]

followed by the circle 1t= z - b = Eei^6 , -71" :::; (J :::; 7r, then the upper
boundary from b-E to a+E, and then the circle 1i: z-a = Eei^6 , 0:::; (J :::; 271",
as shown in Fig. 9.28. Note that E is to be taken small enough so that

a+ E < b - E.


Again, the strong form of the Cauchy-Goursat theorem gives

J fo(z) dz= J fo(z) dz+ 1:~· fo(x) dx + J fo(z) dz


r+ ~t ~t
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