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In most undergraduate courses, groups are first introduced as a primarily algebraic concept – a set equipped with a number of algebraic operations (group multiplication, multiplicative inverse, and multiplicative identity) and obeying a number of rules of algebra (most notably the associative law). It is only somewhat later that one learns that groups are not solely an algebraic object, but can also be equipped with the structure of a manifold (giving rise to Lie groups) or a topological space (giving rise to topological groups). (See also this post for a number of other ways to think about groups.)

Another important way to enrich the structure of a group {G} is to give it some geometry. A fundamental way to provide such a geometric structure is to specify a list of generators {S} of the group {G}. Let us call such a pair {(G,S)} a generated group; in many important cases the set of generators {S} is finite, leading to a finitely generated group. A generated group {(G,S)} gives rise to the word metric {d: G \times G \rightarrow {\bf N}} on {G}, defined to be the maximal metric for which {d(x,sx) \leq 1} for all {x \in G} and {s \in S} (or more explicitly, {d(x,y)} is the least {m} for which {y = s_1^{\epsilon_1} \ldots s_m^{\epsilon_m} x} for some {s_1,\ldots,s_m \in S} and {\epsilon_1,\ldots,\epsilon_m \in \{-1,+1\}}). This metric then generates the balls {B_S(R) := \{ x \in G: d(x,\hbox{id}) \leq R \}}. In the finitely generated case, the {B_S(R)} are finite sets, and the rate at which the cardinality of these sets grow in {R} is an important topic in the field of geometric group theory. The idea of studying a finitely generated group via the geometry of its metric goes back at least to the work of Dehn.

One way to visualise the geometry of a generated group is to look at the (labeled) Cayley colour graph of the generated group {(G,S)}. This is a directed coloured graph, with edges coloured by the elements of {S}, and vertices labeled by elements of {G}, with a directed edge of colour {s} from {x} to {sx} for each {x \in G} and {s \in S}. The word metric then corresponds to the graph metric of the Cayley graph.

For instance, the Cayley graph of the cyclic group {{\bf Z}/6{\bf Z}} with a single generator {S = \{1\}} (which we draw in green) is given as

while the Cayley graph of the same group but with the generators {S = \{2,3\}} (which we draw in blue and red respectively) is given as

We can thus see that the same group can have somewhat different geometry if one changes the set of generators. For instance, in a large cyclic group {{\bf Z}/N{\bf Z}}, with a single generator {S = \{1\}} the Cayley graph “looks one-dimensional”, and balls {B_S(R)} grow linearly in {R} until they saturate the entire group, whereas with two generators {S = \{s_1,s_2\}} chosen at random, the Cayley graph “looks two-dimensional”, and the balls {B_S(R)} typically grow quadratically until they saturate the entire group.

Cayley graphs have three distinguishing properties:

  • (Regularity) For each colour {s \in S}, every vertex {x} has a single {s}-edge leading out of {x}, and a single {s}-edge leading into {x}.
  • (Connectedness) The graph is connected.
  • (Homogeneity) For every pair of vertices {x, y}, there is a unique coloured graph isomorphism that maps {x} to {y}.

It is easy to verify that a directed coloured graph is a Cayley graph (up to relabeling) if and only if it obeys the above three properties. Indeed, given a graph {(V,E)} with the above properties, one sets {G} to equal the (coloured) automorphism group of the graph {(V,E)}; arbitrarily designating one of the vertices of {V} to be the identity element {\hbox{id}}, we can then identify all the other vertices in {V} with a group element. One then identifies each colour {s \in S} with the vertex that one reaches from {\hbox{id}} by an {s}-coloured edge. Conversely, every Cayley graph of a generated group {(G,S)} is clearly regular, is connected because {S} generates {G}, and has isomorphisms given by right multiplication {x \mapsto xg} for all {g\in G}. (The regularity and connectedness properties already ensure the uniqueness component of the homogeneity property.)

From the above equivalence, we see that we do not really need the vertex labels on the Cayley graph in order to describe a generated group, and so we will now drop these labels and work solely with unlabeled Cayley graphs, in which the vertex set is not already identified with the group. As we saw above, one just needs to designate a marked vertex of the graph as the “identity” or “origin” in order to turn an unlabeled Cayley graph into a labeled Cayley graph; but from homogeneity we see that all vertices of an unlabeled Cayley graph “look the same” and there is no canonical preference for choosing one vertex as the identity over another. I prefer here to keep the graphs unlabeled to emphasise the homogeneous nature of the graph.

It is instructive to revisit the basic concepts of group theory using the language of (unlabeled) Cayley graphs, and to see how geometric many of these concepts are. In order to facilitate the drawing of pictures, I work here only with small finite groups (or Cayley graphs), but the discussion certainly is applicable to large or infinite groups (or Cayley graphs) also.

For instance, in this setting, the concept of abelianness is analogous to that of a flat (zero-curvature) geometry: given any two colours {s_1, s_2}, a directed path with colours {s_1, s_2, s_1^{-1}, s_2^{-1}} (adopting the obvious convention that the reversal of an {s}-coloured directed edge is considered an {s^{-1}}-coloured directed edge) returns to where it started. (Note that a generated group {(G,S)} is abelian if and only if the generators in {S} pairwise commute with each other.) Thus, for instance, the two depictions of {{\bf Z}/6{\bf Z}} above are abelian, whereas the group {S_3}, which is also the dihedral group of the triangle and thus admits the Cayley graph

is not abelian.

A subgroup {(G',S')} of a generated group {(G,S)} can be easily described in Cayley graph language if the generators {S'} of {G'} happen to be a subset of the generators {S} of {G}. In that case, if one begins with the Cayley graph of {(G,S)} and erases all colours except for those colours in {S'}, then the graph foliates into connected components, each of which is isomorphic to the Cayley graph of {(G',S')}. For instance, in the above Cayley graph depiction of {S_3}, erasing the blue colour leads to three copies of the red Cayley graph (which has {{\bf Z}/2{\bf Z}} as its structure group), while erasing the red colour leads to two copies of the blue Cayley graph (which as {A_3 \equiv {\bf Z}/3{\bf Z}} as its structure group). If {S'} is not contained in {S}, then one has to first “change basis” and add or remove some coloured edges to the original Cayley graph before one can obtain this formulation (thus for instance {S_3} contains two more subgroups of order two that are not immediately apparent with this choice of generators). Nevertheless the geometric intuition that subgroups are analogous to foliations is still quite a good one.

We saw that a subgroup {(G',S')} of a generated group {(G,S)} with {S' \subset S} foliates the larger Cayley graph into {S'}-connected components, each of which is a copy of the smaller Cayley graph. The remaining colours in {S} then join those {S'}-components to each other. In some cases, each colour {s \in S\backslash S'} will connect a {S'}-component to exactly one other {S'}-component; this is the case for instance when one splits {S_3} into two blue components. In other cases, a colour {s} can connect a {S'}-component to multiple {S'}-components; this is the case for instance when one splits {S_3} into three red components. The former case occurs precisely when the subgroup {G'} is normal. (Note that a subgroup {G'} of a generated group {(G,S)} is normal if and only if left-multiplication by a generator of {S} maps right-cosets of {G'} to right-cosets of {G'}.) We can then quotient out the {(G',S')} Cayley graph from {(G,S)}, leading to a quotient Cayley graph {(G/G', S \backslash S')} whose vertices are the {S'}-connected components of {(G,S)}, and the edges are projected from {(G,S)} in the obvious manner. We can then view the original graph {(G,S)} as a bundle of {(G',S')}-graphs over a base {(G/G',S\backslash S')}-graph (or equivalently, an extension of the base graph {(G/G',S\backslash S')} by the fibre graph {(G',S')}); for instance {S_3} can be viewed as a bundle of the blue graph {A_3} over the red graph {{\bf Z}/2{\bf Z}}, but not conversely. We thus see that the geometric analogue of the concept of a normal subgroup is that of a bundle. The generators in {S \backslash S'} can be viewed as describing a connection on that bundle.

Note, though, that the structure group of this connection is not simply {G'}, unless {G'} is a central subgroup; instead, it is the larger group {G' \rtimes \hbox{Aut}(G')}, the semi-direct product of {G'} with its automorphism group. This is because a non-central subgroup {G'} can be “twisted around” by operations such as conjugation {g' \mapsto sg's^{-1}} by a generator {s \in S}. So central subgroups are analogous to the geometric notion of a principal bundle. For instance, here is the Heisenberg group

\displaystyle  \begin{pmatrix} 1 & {\bf F}_2 & {\bf F}_2 \\ 0 & 1 & {\bf F}_2 \\ 0 & 0 & 1 \end{pmatrix}

over the field {{\bf F}_2} of two elements, which one can view as a central extension of {{\bf F}_2^2} (the blue and green edges, after quotienting) by {{\bf F}_2} (the red edges):

Note how close this group is to being abelian; more generally, one can think of nilpotent groups as being a slight perturbation of abelian groups.

In the case of {S_3} (viewed as a bundle of the blue graph {A_3} over the red graph {{\bf Z}/2{\bf Z}}), the base graph {{\bf Z}/2{\bf Z}} is in fact embedded (three times) into the large graph {S_3}. More generally, the base graph {(G/G', S \backslash S')} can be lifted back into the extension {(G,S)} if and only if the short exact sequence {0 \rightarrow G' \rightarrow G \rightarrow G/G' \rightarrow 0} splits, in which case {G} becomes a semidirect product {G \equiv G' \rtimes H} of {G'} and a lifted copy {H} of {G/G'}. Not all bundles can be split in this fashion. For instance, consider the group {{\bf Z}/9{\bf Z}}, with the blue generator {1} and the red generator {3}:

This is a {{\bf Z}/3{\bf Z}}-bundle over {{\bf Z}/3{\bf Z}} that does not split; the blue Cayley graph of {{\bf Z}/3{\bf Z}} is not visible in the {{\bf Z}/9{\bf Z}} graph directly, but only after one quotients out the red fibre subgraph. The notion of a splitting in group theory is analogous to the geometric notion of a global gauge. The existence of such a splitting or gauge, and the relationship between two such splittings or gauges, are controlled by the group cohomology of the sequence {0 \rightarrow G' \rightarrow G \rightarrow G/G' \rightarrow 0}.

Even when one has a splitting, the bundle need not be completely trivial, because the bundle is not principal, and the connection can still twist the fibres around. For instance, {S_3} when viewed as a bundle over {{\bf Z}/2{\bf Z}} with fibres {A_3} splits, but observe that if one uses the red generator of this splitting to move from one copy of the blue {A_3} graph to the other, that the orientation of the graph changes. The bundle is trivialisable if and only if {G'} is a direct summand of {G}, i.e. {G} splits as a direct product {G = G' \times H} of a lifted copy {H} of {G/G'}. Thus we see that the geometric analogue of a direct summand is that of a trivialisable bundle (and that trivial bundles are then the analogue of direct products). Note that there can be more than one way to trivialise a bundle. For instance, with the Klein four-group {{\bf Z}/2{\bf Z} \times {\bf Z}/2{\bf Z}},

the red fibre {{\bf Z}/2{\bf Z}} is a direct summand, but one can use either the blue lift of {{\bf Z}/2{\bf Z}} or the green lift of {{\bf Z}/2{\bf Z}} as the complementary factor.

Gauge theory” is a term which has connotations of being a fearsomely complicated part of mathematics – for instance, playing an important role in quantum field theory, general relativity, geometric PDE, and so forth.  But the underlying concept is really quite simple: a gauge is nothing more than a “coordinate system” that varies depending on one’s “location” with respect to some “base space” or “parameter space”, a gauge transform is a change of coordinates applied to each such location, and a gauge theory is a model for some physical or mathematical system to which gauge transforms can be applied (and is typically gauge invariant, in that all physically meaningful quantities are left unchanged (or transform naturally) under gauge transformations).  By fixing a gauge (thus breaking or spending the gauge symmetry), the model becomes something easier to analyse mathematically, such as a system of partial differential equations (in classical gauge theories) or a perturbative quantum field theory (in quantum gauge theories), though the tractability of the resulting problem can be heavily dependent on the choice of gauge that one fixed.  Deciding exactly how to fix a gauge (or whether one should spend the gauge symmetry at all) is a key question in the analysis of gauge theories, and one that often requires the input of geometric ideas and intuition into that analysis.

I was asked recently to explain what a gauge theory was, and so I will try to do so in this post.  For simplicity, I will focus exclusively on classical gauge theories; quantum gauge theories are the quantization of classical gauge theories and have their own set of conceptual difficulties (coming from quantum field theory) that I will not discuss here. While gauge theories originated from physics, I will not discuss the physical significance of these theories much here, instead focusing just on their mathematical aspects.  My discussion will be informal, as I want to try to convey the geometric intuition rather than the rigorous formalism (which can, of course, be found in any graduate text on differential geometry).

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