Question: How many homomorphisms are there from $D_5$ to $V_4$, where $D_5$ is the dihedral group of order $10$ and $V_4$ the Klein four-group? I've used the fact that since $V_4$ is abelian, the commutator subgroup of $D_5$ is contained in the kernel of any homomorphism. However, I am having trouble determining the order of the commutator subgroup.
Thanks in advance 🙂
Best Answer
The commutator of $D_5$ has five elements. But we can also proceed without having this information.
Let $r,s$ be the rotation and the spiegelung (reflection) generating $D_5$, seen as the symmetry group of the pentagram. There is a relation joining $r,s$. But $r^5=1$, so the image of $r$ is the one in $V_4$, the only element of order dividing $5$ in $V_4$. It remains to see that $s$ can be mapped into each element of $V_4$.
So there are four homomorphisms $D_5\to V_4$.
Computer aid, here sage:
Final later EDIT:
Above there is a computation of the commutator group for $D_5$ done by sage. Let us do this manually. First of all, let us write explicitly the relation of the two generators of $D_5$, $r$ (geometrically interpreted as) the rotation of the plane around origin with angle $2\pi/5$, and $s$ the symmetry, (spiegelung, i.e.) the reflection w.r.t. the $Ox$ axis. Imagine also the points $\zeta_k=\exp \frac{2\pi i}5$, $k=0,1,2,3,4$, in the same complex plane. Then $$ srs^{-1}=srs=r^{-1}\ , $$ and this relation can be visualized as follows. Consider the complex plane, pass via $s$ in the mirrored world, the mirrored rotation $r$ is then in the opposite direction, it is the way the mirror works. It follows $$ srs^{-1}r^{-1}=r^{-2}\ . $$ The subgroup generated by $r^{-2}$ is ths subgroup of rotations, $R=\{1,r,r^2,r^3, r^4\}$. To see that this is the commutator group, we use the non-trivial "determinant" morphism, which maps "a symmetry" in $D_5$ to $+1$, respectively $-1$, depending on the conservation of the orientation of plane. By geometric means it is well defined. Commutators are mapped to $+1$, since the image group is commutative. And exactly the rotation elements in $R$ are mapped to $+1$. No other elements can be in the commutator.