It is well established that a regular tetrahedron has 12 orientation preserving symmetries, the group $A_4$.
To better understand these symmetries, I set out to identify them geometrically: Prove that the rigid (orientation preserving) motions which send a regular tetrahedron to itself are precisely
- The identity
- Rotations of $\pm 120^\circ$ around a line through the tetrahedron's center and a vertex
- Rotations of $180^\circ$ around a line through the tetrahedron's center and the midpoint of an edge.
My proof is below, to which I request verification and feedback, in particular the portion between the "[*]" symbols, which I'd like verification of or suggestions to make it (or its exposition) simpler or more clear.
Note: This question does not ask for lists of these symmetries, visualizations, or linear algebra or coordinate based derivations, but rather a synthetic, geometric proof of exactly which motions send the tetrahedron to itself.
Proof: Let us call a such a motion an admissible motion. Since a regular tetrahedron has a unique center $C$, any admissible motion must keep $C$ as a fixed point. In $\mathbb R^3$, the motions with a fixed point are precisely the rotations around a line $\ell$ including this point; hence, an admissible motion must be a rotation around a line $\ell$ passing through $C$. Furthermore, since $\ell$ penetrates the tetrahedron, it must pass through exactly two fixed points $S$ and $S'$on the surface of the tetrahedron. Such a rotation will be admissible if and only if it sends faces to faces.
Recall that a rotation around $\ell$ sends a plane [added: not containing $\ell$] to itself if and only if the plane is normal to $\ell$. Similarly, if the rotation sends a line [added: other than $\ell$] to itself, this line must be normal to $\ell$.
Suppose $S$ is a vertex. Then exactly one face $F$ is normal to $\ell$. Since $F$ will remain in its plane, an admissible rotation must send $F$ to itself. This happens if and only if the angle of rotation $\theta$ is $\pm 120^\circ$. Such a rotation sends the remaining faces to each other cyclically and is therefore admissible.
Now, suppose instead that fixed point $S$ is on an edge $E$ but is not a vertex. Then $S$ is on only one edge, so an admissible rotation must send this edge to itself. This happens precisely when $\theta = 180^\circ$, $\ell$ is normal to $E$, and $S$ is the midpoint of $E$. By symmetry, $S'$ will be the midpoint of the unique edge $E'$ non-adjacent to $E$.
We now show that any such rotation is admissible. [*] Given any two non-adjacent edges, the four faces of the tetrahedron are precisely the triangles with a side as one edge and their remaining (opposite) vertex on an endpoint of the other edge. Since rotation about $\ell$ sends $E$ and $E'$ to themselves, it swaps pairs of these faces [*], which shows that it sends faces to faces and is admissible.
Finally, fixed point $S$ might be on a face $F$ but not an edge. Since $S$ is on only one face, an admissible rotation must send $F$ to itself, requiring $\ell$ to be normal to $F$, which can only happen if $\ell$ goes through a vertex, which reduces to the first case above. This completes the proof.