1549312215-Complex_Analysis_for_Mathematics_and_Engineering_5th_edition__Mathews

(jair2018) #1
ANSWERS 605

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15b. f (z) = l + l L 2-n (zn + z - n).
n = l
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17. Since f (z) = L anzn is valid for lzl = 1 (explain), letting z = ei^8

n=-oo
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gives f ( ei^8 ) = I: anein^8 immediately. By Laurent's theorem, an =
n=-oo

z~i fct fJ~~ dz for all integers n (explain). Parametrizing Ci (O) with

z ( 8) = ei<P for 0 5 </> 5 211" gives the desired result. Show the det ails.

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  1. Since L C- n (z - a:)- n converges for lz - a l > r, the ratio test guarantees
    n=l
    that the series converges absolutely for { z : lz - al :2: s}, where s > r (show
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    t he details). Thus, if lz - a:I = s, the series L lc- nl s-n converges. Since
    n = l


lc-n (z - oT"I 5 lc-nl s - n for all lzl :2: s, the Weierstrass M -test gives us

our conclus ion. Explain.

Section 7.4. Singularities, Zeros, and Poles : page 283


la. Zeros of order 4 at ± i.

l e. Simple zeros at -1 ± i.


le. Simple zeros at ± i and ±3i.

lg. Simple zeros at '1±•, -q±;, and ±i.


li. Zeros of order 2 at 1±;"3 and -1.

Simple zeros at^1 ji and -~i, and a zero of order 4 at the origin.


2a. Poles of order 3 at ±i, and a pole of order 4 at 1.

2c. Simple poles at q±;, -q±•, and ± i.

2e. Simple poles at ±./3i and ~-

2g. Simple poles at z = n7r for n = ±1, ±2,...

2i. Simple poles at z = n7r for n = ±1, ±2, ... , and a pole of order 3 at the

origin.

2k. Simple poles at z = 2n11" for n = 0, ±1, ±2,...

3a. Removable singularity at the origin.

3c. Essential singularity at the origin.
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