actions of $\mathbb{Z}_2$ on spheres Let $S^m$ be the $m$-sphere and $$F(S^m,2)/\mathbb{Z}_2=\{(a,b)\mid a,b\in S^m, a\neq b\}/(a,b)\sim (b,a)$$ be the $2$-nd unordered configuration space on $S^m$. Why $F(S^m,2)/\mathbb{Z}_2$ is homotopy equivalent to $\mathbb{R}P^m$?
Note that $F(S^m,2)/\mathbb{Z}_2$ is obtained by the action of $\mathbb{Z}_2$ on $F(S^m,2)$ by permuting coordinates $(a,b)\to (b,a)$. But   $\mathbb{R}P^m$ is obtained by the action of $\mathbb{Z}_2$ on $S^m$ by the antipodal map. Although $F(S^m,2)\cong TS^m \simeq S^m$, the actions of $\mathbb{Z}_2$ are different. 
Added Question: Is $F(S^m,2)/\mathbb{Z}_2$ homeomorphic to $\mathbb{R}P^m\times \mathbb{R}^m$?
 A: Observe that:


*

*$F(S^m,2)/\mathbb{Z}_2$ is the space of all unordered pairs of points on $S^m$.

*$\mathbb{R}P^m$ is the space of all unordered pairs of antipodal points on $S^m$.
The first space deformation retracts onto the second.  Specifically, given an unordered pair $\{a,b\}$ of points on $S^m$ that are not antipodal, let $C$ be the great circle containing them.  Then we can move $a$ and $b$ directly away from each other along $C$ until they are antipodal, which defines the required deformation retraction.
A: Define $i:S^m\to F(S^m,2)$ by $i(a)=(a,-a)$.  This map is equivariant with respect to the $\mathbb{Z}_2$-actions on both sides, and I claim it actually realizes $S^m$ as a $\mathbb{Z}_2$-equivariant deformation retract of $F(S^m,2)$.  Indeed, given a point $(a,b)\in F(S^m,2)$, we can continuously move $a$ and $b$ in opposite directions from each other along the great circle joining them until they are antipodal, and every stage of this homotopy is $\mathbb{Z}_2$-equivariant.
An alternative description of the induced deformation retraction on the quotients is the following.  Think of $\mathbb{R}P^m$ as the set of lines through $0$ in $\mathbb{R}^{m+1}$, and think of $F(S^m,2)/\mathbb{Z}_2$ as the set of lines in $\mathbb{R}^{m+1}$ that intersect $S^m$ at two points.  Given such a line, take the midpoint of its two intersections with $S^m$, and translate your line continuously so the midpoint moves in a straight line to the origin.
