# Understanding “infinite” relations in groups

Consider the matrices $A = \frac{1}{5}\begin{pmatrix}5&0&0\\\ 2&2&1\\\ 2&1&2\end{pmatrix}$, $B = \frac{1}{5}\begin{pmatrix}2&2&1\\\ 0&5&0\\\ 1&2&2\end{pmatrix}$, and $C = \frac{1}{5}\begin{pmatrix}2&1&2\\\ 1&2&2\\\ 0&0&5\end{pmatrix}$.

The group $G\subset GL_3(\mathbb{C})$ they generate is free of rank 3. However, one also has:

$A^\infty := \lim_{k\rightarrow\infty}A^k = \begin{pmatrix}1&0&0\\\ 1&0&0\\\ 1&0&0\\\ \end{pmatrix}$, and similarly $B^\infty = \begin{pmatrix}0&1&0\\\ 0&1&0\\\ 0&1&0\\\ \end{pmatrix}$ and $C^\infty = \begin{pmatrix}0&0&1\\\ 0&0&1\\\ 0&0&1\\\ \end{pmatrix}$.

This leads to three "infinite" relations among $A$,$B$, and $C:$

$A^\infty B = B^\infty A$

$B^\infty C = C^\infty B$

$C^\infty A = A^\infty C$

Of course these are not true group relations since they involve infinite products and furthermore these infinite products are singular, hence do not actually lie in the group generated by $A$, $B$, and $C$, but rather are relations among elements of the "boundary" of this group (in an appropriate sense of the word boundary).

Question 1: I am wondering if anyone has studied such infinite/boundary relations on groups, and in particular if they have any usefulness in understanding any properties of the original group.

Question 2: Suppose $H$ is another free group of rank 3 in $GL_3(\mathbb{C})$. $H$ is of course isomorphic to $G$, but may not have any boundary relations. Is there a way to use the infinite relations to define a "stronger" notion of isomorphism which says that $G$ and $H$ are not isomorphic since they do not have the same infinite relations? Edit: Upon further thought, this latter question is more of a question about the particular representation of $G$ chosen, so perhaps it is not so interesting? Or maybe something aside from the usual stuff about isomorphism of representations might be relevant?

Motivation: Awhile back I was studying harmonic functions on the Sierpinski Gasket; these three matrices arise naturally in the evaluation of such functions. In this context the infinite relations above are equivalent to the statement that such functions are well-defined at each point of the Gasket. The relations above were occasionally useful for proving various facts, but at the time I never bothered to consider them in the context of group relations.

More generally they can arise in studying subgroups of $GL_n(R)$ for $R$ a commutative unital ring. In this case the "boundary" of the subgroup may be a subset of the singular elements of $Mat_n(R)$ and one can ask questions about relations between elements of this "boundary".

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One way to make sense of what you wrote is the following: your group $G$ has a boundary, and $G$ acts on it. Your $X^\infty$ correspond to points on that boundary, and the relations you wrote are statements about how those points move under the action of $G$. – Mariano Suárez-Alvarez Mar 15 '11 at 17:56
I meant to write Gromov boundary. That gives you a keyword to search for, by the way. – Mariano Suárez-Alvarez Mar 15 '11 at 17:59
@Mariano: Thanks for those ideas. – ARupinski Mar 15 '11 at 18:10
Such relations have been studied. In the case of profinite groups, profinite relations have this form. Say, every profinite group satisfies the law $\lim x^{n!} =1$. It should be in the book by Ribes and Zaleski "Profinite groups". – Mark Sapir Mar 15 '11 at 18:32
An afterword to Mariano's comment. Although I believe both notions were defined by Gromov, the term 'Gromov boundary' is normally used for word-hyperbolic groups, which these are not. In your case the group acts on a CAT(0) space, namely a symmetric space, and it is probably the boundary of this which you need to look at. (I have a feeling that this is spherical building, though I could be talking out of my hat.) Anyway, one place to look for the theory of CAT(0) spaces is Bridson & Haefliger's book Metric spaces of non-positive curvature. – HJRW Mar 16 '11 at 3:35

At the other end, I think that a word-hyperbolic group $G$ has a uniformity defined by Gromov whose completion points are called the Gromov boundary. However, multiplication is not uniformly continuous in this construction; rather you only have that the uniformity is left-invariant. Thus, the completion is not a topological group, but it does have a left action of $G$. You can only define right-infinite products, and you can only multiply them by group elements on the left. Still, you can do that much, which still lets you consider many interesting infinite relations.
Your example of groups of matrices is modeled by a uniformity of intermediate quality. The uniformity of the additive Lie group structure on $M_3(\mathbb{C})$ is not the same as the uniformity of the multiplicative Lie group structure on $GL_3(\mathbb{C})$, even though the topologies are the same. Multiplication extends to the completion, but inversion does not. (Toy model: The function $1/x$ on $\mathbb{R}^\times$ is not uniformly continuous in the standard metric on $\mathbb{R}$ and obviously does not extend to $0$.) The completion of $GL_3(\mathbb{C})$ is obviously $M_3(\mathbb{C})$, and any subgroup has an inherited uniformity and a completion which is then a semigroup. So an answer to your second question is that a discrete group can have many different semigroup-completed uniformities, some of which come from matrix representations.