Well, well well, wellity well well...I have no idea what to write about for this last blog entry. =/
Let's talk about...Riemann spheres!
So, at some point in this complex analysis course, you'll have learned that we really ought to think of the complex plane C as lying on the Riemann sphere ˆC:=C∪{∞}. Doing so means that meromorphic functions f:C→C (i.e.: they have poles) may be thought of as holomorphic functions f:C→ˆC. Moreover, if the behaviour of f(z) is nice enough at z=∞ (i.e.: no essential singularities), then f can be extended to a holomorphic function f:ˆC→ˆC.
One class of these holomorphic functions between Riemann spheres that you've encountered in this course are Mobius transformations: z↦az+bcz+d, where ad−bc≠0. You've already seen some nice facts about them. You know that they are conformal (definition: angle-preserving) transformations, that they take circles/lines to circles/lines and you know that they're bijections. In fact, they are precisely the collection of all bijective holomorphic maps between Riemann spheres.
Let's prove this!
Consider a bijective holomorphic function f:ˆC→ˆC. Since this is bijective, let a,b∈C respectively denote the points which map to 0=f(a) and ∞=f(b). We may assume by precomposing f with a Mobius transformation that b≠∞. Now z=a must be an order 1 zero, or else there'd be a small neighbourhood around it where two points map to some ϵ close to 0. Likewise we can argue that z=b must be an order 1 pole of f by considering the function f(1z). Thus, the function g(z)=(z−b)f(z)z−a is a holomorphic function on ˆC with neither zeros nor poles. In particular, its absolute value function |f| is a continuous function on a compact domain (because spheres are totes closed and bounded) and hence must be bounded. Thus, by Liouville's theorem, the function g(z) is equal to some non-zero constant c∈C: f:z↦cz−acz−b. Finally, −bc+ac≠0 since c≠0 and a=b would contradict the bijectivity of f. Thus, this is totes a Mobius transformation.
Note that using the same arguments, we can show that any holomorphic map between Riemann spheres takes the form of a rational function: a0+a1z+a2z2+…+anznb0+b1z+b2z2+…+bmzm!
In fact, I was going to play around with a few polynomials and count branch points and what not, leading us to the Riemann-Hurwitz formula; but it's getting late, and we really ought to give this semester a rest. =)
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