There are a few questions on SE about the well-known homeomorphism $SO(3)\cong \Bbb R P^3$, but I thought it would be fun to collect as many proofs as we can find in one spot.
Background:
- $SO(3)$ is the group of orientation-preserving orthogonal transformations of $\Bbb R^3$, or equivalently the group of $3\times 3$ real matrices $A$ with $AA^\top=I$ and $\det A=1$
- $\Bbb R P^3$ is the space of lines going through the origin in $\Bbb R^4$ topologized equivalently as
- $\left(\Bbb R^4\setminus\{0\}\right)/\sim$, where $x\sim cx$ for all $x\in\Bbb R^4\setminus\{0\}$ and $c\in\Bbb R\setminus\{0\}$ or
- $D^3/\sim$, where $p\sim -p$ for all $p\in S^2$
- Both spaces are oriented $3$-manifolds with smooth structures
- $SO(3)$ is diffeomorphic (and thus homeomorphic) to $\Bbb R P^3$
- As varieties, $SO(3)$ is affine while $\Bbb R P^3$ is projective. Thus, they are not isomorphic as varieties.
You can find some proofs of the homeomorphism $SO(3)\cong \Bbb R P^3$ here, here, and in Hatcher $\S3.D$ (currently at the bottom of page $293$).
I will start with Hatcher's proof along with a version I've written using quaternions.
One direction I'm curious about is to think of $SO(3)$ as the Stiefel manifold $V_2(\Bbb R^3)$, and to somehow turn a pair of orthonormal vectors in $\Bbb R^3$ into a line in $\Bbb R^4$.
Hatcher's proof:
We define a map $\varphi\colon D^3\to SO(3)$ which takes a vector $p\in D^3$ to the rotation about the line spanned by $p$ by $|p|\pi$ radians (see $\ast$ below). If $p\in S^2$, then $\varphi(p)=\varphi(-p)$, so we have an induced $\tilde\varphi\colon \Bbb RP^3\to SO(3)$. It's clear $\tilde\varphi$ is injective since we can recover the axis of rotation and the rotation angle. Further, since every matrix $A\in SO(3)$ has either one or three real eigenvectors, every transformation must be rotation about some axis. It follows that $\tilde\varphi$ is surjective. Since $SO(3)$ is compact, $\tilde\varphi$ is a homeomorphism.
$\ast$: We use the right-hand-rule orientation convention here, so if your thumb points along $p$, your fingers wrap around in the rotation direction. This is akin to the direction of a magnetic field around a cable with an electric current.
Quaternionic proof:
Identify $\Bbb R^4$ with $\Bbb H$ via $(a,b,c,d)\mapsto a+bi+cj+dk$.
Given a line $\ell\in\Bbb RP^3$, pick a unit quaternion $h$ which spans $\ell$ over $\Bbb R$. We define $\psi_\ell\colon \Bbb R^4\to\Bbb R^4$ by $x\mapsto hxh^*$ (where $h^*$ is the quaternionic conjugate of $h$). Since the only other choice of unit quaternion is $-h$, $\ell\mapsto \psi_\ell$ is well-defined.
Now $\psi_\ell(1)=h1h^*=|h|^2=1$, so in the basis $1,i,j,k$, the matrix of $\psi_\ell$ is $$\begin{pmatrix}1 & 0\\0 & A \end{pmatrix}.$$
On the other hand, the standard inclusion $Sp(1)\to GL(4;\Bbb R)$ lands in $SO(4)$, and this shows that the $3\times 3$ matrix $A$ is in $SO(3)$. We hence obtain $\tilde\psi\colon \Bbb RP^3\to SO(3)$. Some more work is required to show $\tilde\psi$ is a bijection, but this is at least a familiar fact to anyone familiar with computer graphics, for example.