calculation, residue theorem
Let f(z)=−πzcot(πz) as a meromorphic function on the whole of C.
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Locate all poles of f and determine their residues.
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Show that for each n≥1 the coefficient of z2n in the Taylor expansion of f(z) about z=0 coincides with
an=k=1∑∞k2n2.
Solution.
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The poles of f are precisely the poles of sinπzz since cosπz is entire. Since sinπz has a simple pole at 0, it follows that sinπzz is analytic near the origin, so the poles of f are at Z∖{0}. Given k∈Z∖{0}, sinπz has a simple zero at k, so we may take the following limit from the real direction and apply L'Hôpital's:
Res(f;k)=z→klim(z−k)f(z)=−πx→klimsinπxx(x−k)=−πx→klimπcosπxx+x−k=−cosπkk=(−1)k+1k.
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We have the representation
πcotπz=z1+k=1∑∞z2−k22z⟹f(z)=−1−k=1∑∞z2−k22z2.
Set g(z)=∑k=1∞z2−k22 so that f(z)=−1−z2g(z). Then
f(2n)(0)=−j=0∑2n(j2n)(dzjdjz2)(0)g(2n−j)(0)=−22!(2n−2)!(2n)!g(2n−2)(0)=−(2n)(2n−1)g(2n−2)(0)
Since g is a Laurent series, it converges uniformly on compact sets, so we may differentiate term-by-term. Notice that
z2−k22z2=2+z2−k22k2=2+k(z−k1−z+k1)
and so
g(2n−2)(z)g(2n−2)(0)=k=1∑∞k((−1)2n−2(z−k)2n−1(2n−2)!−(−1)2n−2(z+k)2n−1(2n−2)!)=k=1∑∞k((z−k)2n−1(2n−2)!−(z+k)2n−1(2n−2)!)=k=1∑∞k((−k)2n−1(2n−2)!−k2n−1(2n−2)!)=−2k=1∑∞k2n(2n−2)!.
Hence,
f(2n)(0)=2k=1∑∞k2nn!⟹(2n)!f(2n)(0)=k=1∑∞k2n2.