This is the lemma from my Geometry textbook (Notes on Geometry by E.Rees), and I would like to get some help on interpreting the proof of this lemma.
Before we go on, I would like to specify what $G$, $\overline{G}$, $G_t$ stands for.
- $G$ is a crystal group, and by the definition of my textbook, this is a subgroup of isometry group of $\mathbb{R}^n$, which contains $n$ independent translations, but no arbitrarily small translations. My textbook really doesn't say anything more, but I think this is a symmetry group of the lattice of $\mathbb{R}^n$.
- Am I understanding the concept of the crystal group correctly?
$G_t = G \cap \mathbb{R}^n$ is called a point group, and according to my textbook, this is a normal subgroup (of $G$) of translations.
$\overline{G}=G/G_t$. And, my textbook says (without a proof) it is a subgroup of $O(n)$, the orthogonal group of $\mathbb{R}^n$. And I think this just means that $\overline{G}$ is a set of orthogonal matrices that preserves the lattice.
- I am kinda lost here already because if we let $f \in G$ be a translation, then I think the left coset $fG_t$ is a set of translations, but why $fG_t$ could become a set of orthogonal matrices? This question might sound silly due to my lacking of knowledge in Group Theory (especially, quotient group). But, please help.
Proof of the lemma:
Given $A \in \overline{G}$, there is an $x \in \mathbb{R}^n$ such that $(A,x) \in G$. If $v \in G_t$, then $(I,v) \in G$. We show that $Av \in G_t$, that is $(I,Av) \in G$: $$(A,x)(I,v)(A,x)^{-1}=(I,Av).$$
As this is independent of $x$, the action is well defined. (End of Proof)
First of all, I don't know why my book used notations such as $(A,x),(I,v)$. What do these notations really mean? If I could know what this means, then I would be able to find out what $(A,x)^{-1}$ means.
Assuming I know what $\overline{G}$ is, $A$ must be some rotation about the origin. And, we just want to show that $Av \in G_t$. But, why do we have to show $Av \in G_t$ like the given proof? If $A$ preserves the lattice, then $Av$ is in the lattice, so considering it as a translation, we just get what we desire.