Week 9 Worksheet - Solutions

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Laurent Series

    1. 1z3=1z113z=1zn=0(3z)n=1z+3z2+9z3+ whenever |3z|<1 i.e. |z|>3.
    2. 1z(1z)=1zn=0zn=1z+1+z+z2+ whenever |z|<1.
    3. z3exp(1/z)=z3n=01n!zn=z3+z2+z2!+13!+14!z+ on C{0}. \item cos(1/z)=n=0(1)n(2n)!z2n=112!z2+14!z416!z6+ on C{0}.
  1. First note that 1z+1={11(z)=n=0(z)n|z|<11z11(1z)=1zn=0(1z)n|z|>1 and that 1z3={1311z3=13n=0(z3)n|z|<31z113z=1zn=0(3z)n|z|>3 using geometric series.

    n=0(z)n13n=0(z3)n

    1zn=0(1z)n13n=0(z3)n

    1zn=0(1z)n+1zn=0(3z)n

    1. 1z2(z1)=1z211z=1z2n=0zn=1z2+1z+1+z+z2+z3+ on Ann(0,0,1)
    2. First note that 1z=11(1z)=n=0(1z)n whenever |z1|<1. Differentiating gives 1z2=n=0n(1z)n1=n=0(n+1)(1z)n whenever 0<|z1|<1. Then calculate that 1z2(1z)=1z1(1z2)=1z1n=0(n+1)(z1)n=1z1+2+3(z1)+4(z1)2+ for 0<|z1|<1.
    1. Just 1(z1)2
    2. 1z1=n=0zn for |z|<1 and so 1(z1)2=(1z1)=n=0nzn1=n=0(n+1)zn on Ann(0,0,1). (Note that f is holomorphic on B(0,1).)
    3. From part b) we have n=0n+1zn=1(1z1)2=z21(1z)2 whenever |z|>1. Thus 1(1z)2=1z2n=0n+1zn on Ann(0,1,).

Isolated Singularities

    1. z2+1=(z+i)(zi) has simple zeroes at i and i so f has simple poles at i and i.
    2. z4+16=(z2eiπ/4)(z2e3iπ/4)(z2e5iπ/4)(z2e7πi/4) has simple zeroes at 2eiπ/4,2e3iπ/4,2e5iπ/4,2e7iπ/4 so f has simple zeroes at each of those points.
    3. z4+2z2+1=(z2+1)2=(z+i)2(zi)2 has zeroes of order two at i and i so f has poles of order two at i and i.
    4. z2+z1=(z152)(z1+52) has simple zeroes so f has simple poles at 152 and 1+52.
    1. Since sin(1/z)=n=0(1)n(2n+1)!1zn has infinitely many non-zero coefficients the singularity is essential.
    2. The function g(z)=(sin(z))2 is holomorphic on all of C so is represented by a power series (sin(z))2=n=0anzn with infinite radius of convergence. However (sinz)2 has a zero of order two at the origin: the coefficients a0 and a1 are both zero whereas a2 is non-zero. Indeed, calculating derivatives ((sinz)2)=2(sinz)(cosz)((sinz)2)=2(cosz)22(sinz)2 we see that the first derivative is zero at the origin while the second is non-zero at the origin. Thus 1z3(sinz)2=1z3(a2z2+a3z3+)=a2z+a3+a4z+a5z2+ with a2 non-zero so we have a simple pole at the origin.
    3. From our power series for cosine 1cos(z)z2=1z2(1(1z22!+z44!z66!+))=1z2(z22!z44!+z66!)=12!z24!+z46! so the singularity at the origin is removable.
  1. Fix M>0 such that |f(z)|M for all zD. Fix R>0 such that B(b,R)D. Since f is holomorphic on Ann(b,0,R) it has a Laurent series thereon. From Laurent's theorem an=12πiγf(z)(zb)n+1dz where γ(t)=b+reit for every 0<r<R and every nN. Thus |an|=12π|γf(z)(zb)n+1dz|12π2πrBrn+1=Brn from our estimation lemma. Since r>0 was arbitrary we conclude that an=0 for all nN. Thus the singularity is removable.