03 - Lie groups and homomorphisms

We expand on our discussion of groups to include the maps between groups. We also present the idea behind Lie groups. Finally we give a formal definition of a group representation.

Lie Groups

A Lie group is a group with one or more continuous parameters that may also have a geometric interpretation. The abelian group $\mathsf{U}(1)$ has a single, continuous parameter that served as a coordinate on the circle, $S^{1}$.

The translations associated to the vector space $\mathbb{R}^{n}$ also form an abelian Lie group. Actually, this idea holds for any vector space. Essentially, translations model the group of vector addition.

The general linear group of invertible matrices is - unsurprisingly - also a group. It is a group whose operation is matrix multiplication. Given that each matrix element is a continuous parameter, $\mathsf{GL}(V)$ is also a Lie group.

Note that the full vector space of endomorphisms $\mathsf{End}(V)$ is not a group under matrix multiplication, as some matrices are not invertible.

Homomorphisms

Let $G$ and $H$ be groups. A map $f$ between these groups is called a group homomorphism if it respects the group multiplication,

$$f(gh) = f(g)f(h),\quad g,h \in G.$$

In this language, a linear map might be thought of as a vector space homomorphism.

We are now in a position to give our first precise definition of a representation. A group representation of a group $G$ on a vector space $V$ is a homomorphism $\pi$ from $G$ to a subgroup of $\mathsf{GL}(V)$:

$$\pi : G \rightarrow \mathsf{GL}(V).$$

In this context $V$ is called a module for $G$ or a $G$-module.

A Confounding Point

One confusing thing about groups like $\mathsf{GL}(V)$, $\mathsf{U}(n)$, and $\mathsf{O}(n)$ is that they are also defined in terms of matrices that are supposed to represent them.

The homomorphism $\pi$ is a trivial in these so-called defining modules. As we shall see in detail, groups like $\mathsf{O}(n)$ have their own identity, independent of their definition in terms of space like $\mathsf{End}(\mathbb{R}^{n}$). In particular, there is an infinite tower of modules for $\mathsf{O}(n)$, each with a different dimension.


Sean Downes

Theoretical physicist, coffee and outdoor recreation enthusiast.

https://www.pasayten.org
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04 - The Exponential Map

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02 - Groups