1.01 Winding numbers and the fundamental theorem of algebra
Below the video you will find accompanying notes and some pre-class questions.
- Next video: 1.02 Paths, loops and homotopies.
- Index of all lectures.
Notes
(0.00) I want to start this module by giving a rough sketch of how to prove the fundamental theorem of algebra using the idea of winding numbers. You may have seen something similar in a first course on complex analysis, where the winding number was defined using a contour integral. The aim of the current proof is to remove the need for complex analysis in this definition: the winding number is something purely topological.
The fundamental theorem of algebra
(2.24) Consider the circle of radius R in the complex plane. The points in this circle are precisely those of the form Reiθ. Let γR be the image of this circle under the map p:C→C. We can think of γR as a loop in C: γR(θ)=p(Reiθ).

(3.54) When R=0, γ0(θ)=p(0) is independent of θ. In other words, γ0 is the constant loop at the point p(0)∈C∖{0}.
(4.42) When R is very large, the term zn dominates in p, so γR(θ)≈δ(θ), where δ(θ)=Rneinθ.
Claim: (6.54) There is a homotopy invariant notion of winding number around the origin for paths in C∖{0} which gives zero for the constant loop and n for the loop δ(θ)=Rneinθ.
Homotopy invariant means, roughly, invariant under continuous deformations; in our situation, that means that the winding number of γR around the origin should be independent of R. Since γ0 has winding number zero and γR has winding number n for large R, this implies n=0.
Outlook
(9.24) The rest of this module will be about defining this notion of winding number, the notion of homotopy and homotopy invariance, and generalising it to other spaces. In a more general setting, the spaces we're interested in (in this example C∖{0}) will have an associated group (in this example the integers Z) called the fundamental group and loops will have winding ``numbers'' which are elements of this group.
This will have many applications, including:
- the Brouwer fixed point theorem (any continuous map from the 2-dimensional disc to itself has a fixed point).
- the fact that a trefoil knot cannot be unknotted.
- the fact that the three Borromean rings cannot be unlinked from one
another (despite the fact that they can be unlinked in pairs
ignoring the third).
Pre-class questions
- Go through the rough sketch proof and highlight all the steps which
seem to you not to be fully justified. We will discuss this in
class, and I will call upon you for suggestions. Later in the
module, we will revisit this proof and fill in all the gaps
(hopefully to your satisfaction).
Navigation
- Next video: 1.02 Paths, loops and homotopies.
- Index of all lectures.