@Studentmath That's easy to show that way. I don't think in the exam they will accept that. Will they? Don't I need to show that somehow in another way? Although in the solution they didn't even bother explaining what you just wrote.
I'm not sure what the question is, but if you just want to show that these 3 vectors are part of K, it's sufficient and necessery to show they uphold $x^2+y^2-z^2=1$
So if I want to show that those 3 vectors $\in K$ it's enough to explain as you wrote? I don't need to expand somehow the equation $x^2+y^2-z^2=1$ in some way to get those 3 vectors algebrically
No need for that, but not sure what the question is, if you do not bring up a reason as to why you thought of these three vectors one might think you are cheating.
@TedShifrin Let $K$ be the closed disc, with two smaller open discs deleted. [So that it looks like (o o)] Show that if $f: K \rightarrow K$ is a homeomorphism without a fixed point, then $f$ reverses orientation and cyclically permuted the boundary circles.
(I'm stuck near the end of it, but it's a fun problem.)
Anyway, if I can show that at least one of the boundary circles moves to another one, I can show that they cyclically permute: assume they don't; then one of them is sent to itself (in a manner without fixed points) and the other two are swapped. Collapse the other two boundary circles to two points; this induces a map from the disc to itself without fixed points, which is nonsense.
So they cyclically permute. In that case, collapse all the boundary circles, each to a distinct point; so the map $f$ induces a self-map of the 2-sphere without fixed points, which thus must have degree -1 and be orientation-reversing.
(To see that an automorphism without a fixed point exists, imagine the three deleted open discs as placed on a sphere, each of whose center is placed equidistant from the others on some great circle, all of which have the same radius; rotate the sphere $2\pi/3$ in such a manner that the great circle is mapped to itself (I'm not sure what the word for this axis of rotation is), then reflect it across the plane that contains the great circle.)
@TedShifrin Yeah, I've thought of that; you get an endo with exactly three fixed points. I'm not sure how to use that. (I'm aware that there's a formulation of Lefschetz that counts fixed points, or something? But I don't know it.)
@TedShifrin Well, by Whitney any map is homotopic to a smooth map, but I'm not assuming my homeomorphism is smooth, and I certainly don't want to homotope since I lose all my fixed point info
The issue comes with non-transverse intersection. Then we don't know what intersection number means topologically, unless you make things PL or something.
Right, @Hippa, but the sum definitely is NOT zero.
If you have a reasonable definition of index, sure. I'm wiggling the function if I have nontransverse intersection with the diagonal, and adding up the contributions of the wiggles. This all makes sense PL.
@TedShifrin I want to use a parity argument: $\sum \iota(f,x) \neq 0 \pmod 2$ because the $\iota$ have to be $\pm 1$ or something. But I don't have the background to assert that the $\iota$ have to be $\pm 1$.
My counterexample didn't work. I was going to suggest $z \mapsto z^2$ since the extension would have 3 fixed points. But it's also not even close to an automorphism.
Consider the mapping $re^{i\theta}\mapsto \frac{r}{1+r}e^{i\theta}$ which maps the complex plane onto the open unit disc, preserving the argument of each point. This is a homeomorphism. Now we can take the closure of the disk in $\Bbb R^2$ and obtain a compactification of the complex plane which effectively adds one point at infinity for each value of $\theta\in [0, 2\pi)$. Does this object have a name?
It is sort-of analogous to the two-point compactification of $\Bbb R$.