In this post we’ll make sense of a holomorphic square root and logarithm.
Wrote this up because I was surprised how hard it was to find a decent complete explanation.
Let f:U→C be a holomorphic function.
A holomorphic n-th root of f is a function g:U→C
such that f(z)=g(z)n for all z∈U.
A logarithm of f is a function g:U→C such that
f(z)=eg(z) for all z∈U.
The main question …
Epistemic status: highly dubious.
I found almost no literature doing anything quite like what follows,
which unsettles me because it makes it likely that I’m overcomplicating things significantly.
1. Synopsis
Recently I was working on an elegant problem which was the original problem 6
for the 2015 International Math Olympiad, which reads as follows:
Problem [IMO Shortlist 2015 Problem C6]
Let S be a nonempty set of positive integers.
We say that a positive integer n is clean if it has a unique representation
as a sum of an odd number of distinct elements from S.
Prove that there exist infinitely many positive integers that are not clean.
Proceeding by contradiction, one can prove (try it!) that in fact all
sufficiently large integers have exactly one representation as a sum of an even subset of S.
Then, the problem reduces to …
For some reason several classes at MIT this year involve Fourier analysis.
I was always confused about this as a high schooler,
because no one ever gave me the “orthonormal basis” explanation, so here goes.
As a bonus, I also prove a form of Arrow’s Impossibility Theorem using binary Fourier analysis,
and then talk about the fancier generalizations using Pontryagin duality and the Peter-Weyl theorem.
In what follows, we let T=R/Z denote the “circle group”,
thought of as the additive group of “real numbers modulo 1”.
There is a canonical map e:T→C sending
T to the complex unit circle, given by e(θ)=exp(2πiθ …
Let V be a normed finite-dimensional real vector space and let U⊆V be an open set.
A vector field on U is a function ξ:U→V.
(In the words of Gaitsgory: “you should imagine a vector field as a domain,
and at every point there is a little vector growing out of it.”)
The idea of a differential equation is as follows.
Imagine your vector field specifies a velocity at each point.
So you initially place a particle somewhere in U, and then let it move freely,
guided by the arrows in the vector field.
(There are plenty of good pictures
online.) Intuitively,
for nice ξ it should be the case that the trajectory resulting is unique. This is the main take-away;
the proof itself is just for …