Exercises:Mond - Topology - 1/Question 9

Section B

Question 9

The real projective plane, [ilmath]\mathbb{RP}^2[/ilmath] is defined as the quotient of the sphere, [ilmath]\mathbb{S}^2[/ilmath], by the equivalence relation that defines (for [ilmath]x\in\mathbb{S}^2\subset\mathbb{R}^3[/ilmath]) [ilmath]x\sim -x[/ilmath], that is it identifies antipodal points.

Show that [ilmath]\mathbb{RP}^2[/ilmath] is Hausdorff

Definitions

• We denote by [ilmath]\pi:\mathbb{S}^2\rightarrow\frac{\mathbb{S}^2}{\sim} [/ilmath] the canonical projection of the equivalence relation, [ilmath]\sim[/ilmath]. Note that this is a quotient map when we consider [ilmath]\frac{\mathbb{S}^2}{\sim} [/ilmath] with the quotient topology.

Solution outline

Suppose we take the points [ilmath]\alpha[/ilmath] and [ilmath]\beta[/ilmath] on the sphere. We could have balls (in [ilmath]\mathbb{R}^3[/ilmath]) that are centred at [ilmath]\alpha[/ilmath] and [ilmath]\beta[/ilmath] and they'd get quite large before touching (we want them to be disjoint!) However we must consider 4 open balls, one at each point [ilmath]\alpha[/ilmath], [ilmath]\beta[/ilmath], [ilmath]\gamma[/ilmath] and [ilmath]\delta[/ilmath], we see here even though [ilmath]\alpha[/ilmath] and [ilmath]\beta[/ilmath] are far apart that [ilmath]\beta[/ilmath] and [ilmath]\gamma[/ilmath] (which is antipodal to [ilmath]\alpha[/ilmath]) are actually rather close!

So rather than [ilmath]\epsilon\le\frac{1}{2}d(\alpha,\beta)[/ilmath] (for [ilmath]d[/ilmath] being the Euclidean metric of [ilmath]\mathbb{R}^3[/ilmath]) we must make sure that the ball at the antipodal point doesn't touch any others too!

It is clear that if [ilmath]\epsilon\le\frac{1}{2} d(\alpha,\gamma)=1[/ilmath] that the balls centred at [ilmath]\alpha[/ilmath] and [ilmath]\gamma[/ilmath] (or [ilmath]\beta[/ilmath] and [ilmath]\delta[/ilmath]) wont touch, we must make sure that [ilmath]\alpha[/ilmath] and [ilmath]\beta[/ilmath] don't touch, so use [ilmath]\epsilon\le d(\alpha,\beta)[/ilmath].

But as the diagram shows, [ilmath]\alpha[/ilmath] and [ilmath]\delta[/ilmath] could be rather close! (or equivalently, [ilmath]\gamma[/ilmath] and [ilmath]\beta[/ilmath]), so we need [ilmath]\epsilon<\frac{1}{2} d(\alpha,\delta)[/ilmath] too!

We can boil all these down into [ilmath]\epsilon\le\frac{1}{2}\text{min}(\{d(\alpha,\beta),d(\alpha,\delta)\})[/ilmath]

We will deal with the open sets, [ilmath]U[/ilmath], in terms of [ilmath]\pi^{-1}(U)[/ilmath] (as by definition, [ilmath]U\in\mathcal{P}(\frac{\mathbb{S}^2}{\sim})[/ilmath] is open in [ilmath]\frac{\mathbb{S}^2}{\sim}[/ilmath] if and only if [ilmath]\pi^{-1}(U)[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath], which we consider with the subspace topology inherited from [ilmath]\mathbb{R}^3[/ilmath] as usual) then we just have to find small enough open balls!

With this in mind, let [ilmath]a,b\in\mathbb{RP}^2[/ilmath] be given. We need to find two open sets (well... neighbourhoods will do... but open sets are neighbourhoods!), let's say [ilmath]U_a[/ilmath] and [ilmath]U_b[/ilmath] such that:

• [ilmath]a\in U_a[/ilmath], [ilmath]b\in U_b[/ilmath] and [ilmath]U_a\cap U_b=\emptyset[/ilmath]

Well:

• [ilmath]U_a[/ilmath] is open in [ilmath]\mathbb{RP}^2[/ilmath]

if and only if

• [ilmath]\pi^{-1}(U_a)[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath]

if and only if

• there exists an open set, [ilmath]V_a[/ilmath] in [ilmath]\mathbb{R}^3[/ilmath] such that [ilmath]V_a\cap\mathbb{S}^2=\pi^{-1}(U_a)[/ilmath]

Of course, the open balls of [ilmath]\mathbb{R}^3[/ilmath] are a basis, so we can think of [ilmath]V_a[/ilmath] as a union of open balls, or possibly just an open ball (as basis sets themselves are open, and also as an open ball can be expressed as a union of open balls).

This changes the question into, in terms of [ilmath]a[/ilmath] and [ilmath]b[/ilmath], what size balls can we consider in [ilmath]\mathbb{R}^3[/ilmath] such that they're disjoint. There's a caveat here. This is what is shown in the diagram.

If [ilmath]a[/ilmath] and [ilmath]b[/ilmath] are "far apart" on [ilmath]\mathbb{RP}^2[/ilmath], it is entirely possible (in the pre-image under [ilmath]\pi[/ilmath]) that the antipodal point of one is near the other!

So we must be careful to make sure our balls do not overlap at all!

Consider now [ilmath]\{x,-x\}=\pi^{-1}(a)[/ilmath] and [ilmath]\{y,-y\}=\pi^{-1}(b)[/ilmath]:

We notice also there is extra "structure" on [ilmath]\mathbb{R}^3[/ilmath], namely that it is a normed space, [ilmath](\mathbb{R}^3,\Vert\cdot\Vert)[/ilmath], and we consider the metric induced by the norm as the metric, [ilmath]d[/ilmath], for a metric space, [ilmath](\mathbb{R}^3,d)[/ilmath], then we see:

1. [ilmath]d(x,y)=d(y,x)[/ilmath] (by the symmetric property of a metric) and
2. [ilmath]d(-x,y)=\Vert -x-y\Vert = \Vert(-1)x+y\Vert=\Vert x+y\Vert=d(x,-y)[/ilmath]
3. We don't need to consider [ilmath]d(x,-x)[/ilmath] and [ilmath]d(y,-y)[/ilmath], also [ilmath]d(x,x)=d(y,y)=0[/ilmath] is not very helpful

So take:

• [ilmath]\epsilon\le\frac{1}{2}\text{min}(\{d(x,y),d(x,-y)\})[/ilmath] (Note: Smaller would work too, eg [ilmath]\frac{1}{4} [/ilmath] rather than [ilmath]\frac{1}{2} [/ilmath] - I hope I don't need to prove [ilmath]\frac{1}{2} [/ilmath] is sufficient?)
  • This should explain why [ilmath]d(x,-x)[/ilmath] and [ilmath]d(y,-y)[/ilmath] are of no use!

Then just place one of these open balls of radius [ilmath]\epsilon[/ilmath] at each of the 4 points. Job done!

Solution

We wish to show that [ilmath]\mathbb{RP}^2[/ilmath] is Hausdorff.

• Let [ilmath]a,b\in\mathbb{RP}^2[/ilmath] be given such that [ilmath]a\ne b[/ilmath], then
  • there exist [ilmath]x,y\in\mathbb{S}^2[/ilmath] such that [ilmath]\pi^{-1}(a)=\{x,-x\}[/ilmath] and [ilmath]\pi^{-1}(b)=\{y,-y\}[/ilmath]
    • Let [ilmath]\epsilon:=\frac{1}{2}\text{min}(\{d(x,y),d(x,-y)\})[/ilmath] Note that [ilmath]d(x,-y)=d(-x,y)[/ilmath] - see above in the outline section
      • Let [ilmath]V_a:=B_\epsilon(x)\cup B_\epsilon(-x)\subset\mathbb{R}^3[/ilmath] and [ilmath]V_b:=B_\epsilon(y)\cup B_\epsilon(-y)\subset\mathbb{R}^3[/ilmath]. These are open (in [ilmath]\mathbb{R}^3[/ilmath]) as open balls are open sets, and the union of open sets is open.
        • Now define [ilmath]U_a:=V_a\cap\mathbb{S}^2[/ilmath] and [ilmath]U_b:=V_b\cap\mathbb{S}^2[/ilmath], these are open in [ilmath]\mathbb{S}^2[/ilmath] (considered with the subspace topology it inherits from [ilmath]\mathbb{R}^3[/ilmath] - as mentioned in the outline)
          • Recall [ilmath]U\in\mathcal{P}(\mathbb{RP}^2)[/ilmath] is open if and only if [ilmath]\pi^{-1}(U)[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath]
          • Thus:
            1. [ilmath]\pi(U_a)[/ilmath] is open if and only if [ilmath]\pi^{-1}(\pi(U_a))[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath] and
            2. [ilmath]\pi(U_b)[/ilmath] is open if and only if [ilmath]\pi^{-1}(\pi(U_b))[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath]
          • It should be clear that [ilmath]\pi^{-1}(\pi(U_a))=U_a[/ilmath] and [ilmath]\pi^{-1}(\pi(U_b))=U_b[/ilmath] (by their very construction)
          • Thus:
            1. [ilmath]\pi(U_a)[/ilmath] is open if and only if [ilmath]\pi^{-1}(\pi(U_a))=U_a[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath] and
            2. [ilmath]\pi(U_b)[/ilmath] is open if and only if [ilmath]\pi^{-1}(\pi(U_b))=U_b[/ilmath] is open in [ilmath]\mathbb{S}^2[/ilmath]
          • As both right-hand-sides are true, we see [ilmath]\pi(U_a)[/ilmath] and [ilmath]\pi(U_b)[/ilmath] are both open in [ilmath]\mathbb{RP}^2[/ilmath]
          • We must now show [ilmath]U_a[/ilmath] and [ilmath]U_b[/ilmath] are disjoint.
            • Suppose there exists a [ilmath]p\in \pi(U_a)\cap\pi(U_b)[/ilmath] (that is that they're not disjoint and [ilmath]x[/ilmath] is in both of them), then:
              • clearly [ilmath]\exists q\in \pi^{-1}(\pi(U_a))\cap\pi^{-1}(\pi(U_b))[/ilmath] such that [ilmath]\pi(q)=p[/ilmath]
                • However [ilmath]\pi^{-1}(\pi(U_a))\cap\pi^{-1}(\pi(U_b))=U_a\cap U_b[/ilmath] and [ilmath]U_a\cap U_b=\emptyset[/ilmath] (by construction), so there does not exist such a [ilmath]q[/ilmath]!
                • If there is nothing in the pre-image of [ilmath]\pi(U_a)\cap\pi(U_b)[/ilmath] that maps to [ilmath]p[/ilmath] then we cannot have [ilmath]p\in \pi(U_a)\cap\pi(U_b)[/ilmath] - a contradiction
            • So there does not exist such a [ilmath]p[/ilmath], which means [ilmath]\pi(U_a)\cap\pi(U_b)=\emptyset[/ilmath], they're disjoint.

This completes the proof.