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In the previous set of notes, we saw that one could derive expansion of Cayley graphs from three ingredients: non-concentration, product theorems, and quasirandomness. Quasirandomness was discussed in Notes 3. In the current set of notes, we discuss product theorems. Roughly speaking, these theorems assert that in certain circumstances, a finite subset of a group
either exhibits expansion (in the sense that
, say, is significantly larger than
), or is somehow “close to” or “trapped” by a genuine group.
Theorem 1 (Product theorem in
) Let
, let
be a finite field, and let
be a finite subset of
. Let
be sufficiently small depending on
. Then at least one of the following statements holds:
- (Expansion) One has
.
- (Close to
) One has
.
- (Trapping)
is contained in a proper subgroup of
.
We will prove this theorem (which was proven first in the cases for fields
of prime order by Helfgott, and then for
and general
by Dinai, and finally to general
and
independently by Pyber-Szabo and by Breuillard-Green-Tao) later in this notes. A more qualitative version of this proposition was also previously obtained by Hrushovski. There are also generalisations of the product theorem of importance to number theory, in which the field
is replaced by a cyclic ring
(with
not necessarily prime); this was achieved first for
and
square-free by Bourgain, Gamburd, and Sarnak, by Varju for general
and
square-free, and finally by this paper of Bourgain and Varju for arbitrary
and
.
Exercise 1 (Girth bound) Assuming Theorem 1, show that whenever
is a symmetric set of generators of
for some finite field
and some
, then any element of
can be expressed as the product of
elements from
. (Equivalently, if we add the identity element to
, then
for some
.) This is a special case of a conjecture of Babai and Seress, who conjectured that the bound should hold uniformly for all finite simple groups (in particular, the implied constants here should not actually depend on
. The methods used to handle the
case can handle other finite groups of Lie type of bounded rank, but at present we do not have bounds that are independent of the rank. On the other hand, a recent paper of Helfgott and Seress has almost resolved the conjecture for the permutation groups
.
A key tool to establish product theorems is an argument which is sometimes referred to as the pivot argument. To illustrate this argument, let us first discuss a much simpler (and older) theorem, essentially due to Freiman, which has a much weaker conclusion but is valid in any group :
Theorem 2 (Baby product theorem) Let
be a group, and let
be a finite non-empty subset of
. Then one of the following statements hold:
- (Expansion) One has
.
- (Close to a subgroup)
is contained in a left-coset of a group
with
.
To prove this theorem, we suppose that the first conclusion does not hold, thus . Our task is then to place
inside the left-coset of a fairly small group
.
To do this, we take a group element , and consider the intersection
. A priori, the size of this set could range from anywhere from
to
. However, we can use the hypothesis
to obtain an important dichotomy, reminiscent of the classical fact that two cosets
of a subgroup
of
are either identical or disjoint:
Proposition 3 (Dichotomy) If
, then exactly one of the following occurs:
- (Non-involved case)
is empty.
- (Involved case)
.
Proof: Suppose we are not in the pivot case, so that is non-empty. Let
be an element of
, then
and
both lie in
. The sets
and
then both lie in
. As these sets have cardinality
and lie in
, which has cardinality less than
, we conclude from the inclusion-exclusion formula that
But the left-hand side is equal to , and the claim follows.
The above proposition provides a clear separation between two types of elements : the “non-involved” elements, which have nothing to do with
(in the sense that
, and the “involved” elements, which have a lot to do with
(in the sense that
. The key point is that there is a significant “gap” between the non-involved and involved elements; there are no elements that are only “slightly involved”, in that
and
intersect a little but not a lot. It is this gap that will allow us to upgrade approximate structure to exact structure. Namely,
Proposition 4 The set
of involved elements is a finite group, and is equal to
.
Proof: It is clear that the identity element is involved, and that if
is involved then so is
(since
. Now suppose that
are both involved. Then
and
have cardinality greater than
and are both subsets of
, and so have non-empty intersection. In particular,
is non-empty, and so
is non-empty. By Proposition 3, this makes
involved. It is then clear that
is a group.
If , then
is non-empty, and so from Proposition 3
is involved. Conversely, if
is involved, then
. Thus we have
as claimed. In particular,
is finite.
Now we can quickly wrap up the proof of Theorem 2. By construction, for all
,which by double counting shows that
. As
, we see that
is contained in a right coset
of
; setting
, we conclude that
is contained in a left coset
of
.
is a conjugate of
, and so
. If
, then
and
both lie in
and have cardinality
, so must overlap; and so
. Thus
, and so
, and Theorem 2 follows.
Exercise 2 Show that the constant
in Theorem 2 cannot be replaced by any larger constant.
Exercise 3 Let
be a finite non-empty set such that
. Show that
. (Hint: If
, show that
for some
.)
Exercise 4 Let
be a finite non-empty set such that
. Show that there is a finite group
with
and a group element
such that
and
.
Below the fold, we give further examples of the pivot argument in other group-like situations, including Theorem 2 and also the “sum-product theorem” of Bourgain-Katz-Tao and Bourgain-Glibichuk-Konyagin.
In the previous set of notes we introduced the notion of expansion in arbitrary -regular graphs. For the rest of the course, we will now focus attention primarily to a special type of
-regular graph, namely a Cayley graph.
Definition 1 (Cayley graph) Let
be a group, and let
be a finite subset of
. We assume that
is symmetric (thus
whenever
) and does not contain the identity
(this is to avoid loops). Then the (right-invariant) Cayley graph
is defined to be the graph with vertex set
and edge set
, thus each vertex
is connected to the
elements
for
, and so
is a
-regular graph.
Example 1 The graph in Exercise 3 of Notes 1 is the Cayley graph on
with generators
.
Remark 1 We call the above Cayley graphs right-invariant because every right translation
on
is a graph automorphism of
. This group of automorphisms acts transitively on the vertex set of the Cayley graph. One can thus view a Cayley graph as a homogeneous space of
, as it “looks the same” from every vertex. One could of course also consider left-invariant Cayley graphs, in which
is connected to
rather than
. However, the two such graphs are isomorphic using the inverse map
, so we may without loss of generality restrict our attention throughout to left Cayley graphs.
Remark 2 For minor technical reasons, it will be convenient later on to allow
to contain the identity and to come with multiplicity (i.e. it will be a multiset rather than a set). If one does so, of course, the resulting Cayley graph will now contain some loops and multiple edges.
For the purposes of building expander families, we would of course want the underlying group
to be finite. However, it will be convenient at various times to “lift” a finite Cayley graph up to an infinite one, and so we permit
to be infinite in our definition of a Cayley graph.
We will also sometimes consider a generalisation of a Cayley graph, known as a Schreier graph:
Definition 2 (Schreier graph) Let
be a finite group that acts (on the left) on a space
, thus there is a map
from
to
such that
and
for all
and
. Let
be a symmetric subset of
which acts freely on
in the sense that
for all
and
, and
for all distinct
and
. Then the Schreier graph
is defined to be the graph with vertex set
and edge set
.
Example 2 Every Cayley graph
is also a Schreier graph
, using the obvious left-action of
on itself. The
-regular graphs formed from
permutations
that were studied in the previous set of notes is also a Schreier graph provided that
for all distinct
, with the underlying group being the permutation group
(which acts on the vertex set
in the obvious manner), and
.
Exercise 1 If
is an even integer, show that every
-regular graph is a Schreier graph involving a set
of generators of cardinality
. (Hint: first show that every
-regular graph can be decomposed into
unions of cycles, each of which partition the vertex set, then use the previous example.
We return now to Cayley graphs. It is easy to characterise qualitative expansion properties of Cayley graphs:
Exercise 2 (Qualitative expansion) Let
be a finite Cayley graph.
- (i) Show that
is a one-sided
-expander for
for some
if and only if
generates
.
- (ii) Show that
is a two-sided
-expander for
for some
if and only if
generates
, and furthermore
intersects each index
subgroup of
.
We will however be interested in more quantitative expansion properties, in which the expansion constant is independent of the size of the Cayley graph, so that one can construct non-trivial expander families
of Cayley graphs.
One can analyse the expansion of Cayley graphs in a number of ways. For instance, by taking the edge expansion viewpoint, one can study Cayley graphs combinatorially, using the product set operation
of subsets of .
Exercise 3 (Combinatorial description of expansion) Let
be a family of finite
-regular Cayley graphs. Show that
is a one-sided expander family if and only if there is a constant
independent of
such that
for all sufficiently large
and all subsets
of
with
.
One can also give a combinatorial description of two-sided expansion, but it is more complicated and we will not use it here.
Exercise 4 (Abelian groups do not expand) Let
be a family of finite
-regular Cayley graphs, with the
all abelian, and the
generating
. Show that
are a one-sided expander family if and only if the Cayley graphs have bounded cardinality (i.e.
). (Hint: assume for contradiction that
is a one-sided expander family with
, and show by two different arguments that
grows at least exponentially in
and also at most polynomially in
, giving the desired contradiction.)
The left-invariant nature of Cayley graphs also suggests that such graphs can be profitably analysed using some sort of Fourier analysis; as the underlying symmetry group is not necessarily abelian, one should use the Fourier analysis of non-abelian groups, which is better known as (unitary) representation theory. The Fourier-analytic nature of Cayley graphs can be highlighted by recalling the operation of convolution of two functions , defined by the formula
This convolution operation is bilinear and associative (at least when one imposes a suitable decay condition on the functions, such as compact support), but is not commutative unless is abelian. (If one is more algebraically minded, one can also identify
(when
is finite, at least) with the group algebra
, in which case convolution is simply the multiplication operation in this algebra.) The adjacency operator
on a Cayley graph
can then be viewed as a convolution
where is the probability density
is the Kronecker delta function on
. Using the spectral definition of expansion, we thus see that
is a one-sided expander if and only if
is orthogonal to the constant function
, and is a two-sided expander if
is orthogonal to the constant function
.
We remark that the above spectral definition of expansion can be easily extended to symmetric sets which contain the identity or have multiplicity (i.e. are multisets). (We retain symmetry, though, in order to keep the operation of convolution by
self-adjoint.) In particular, one can say (with some slight abuse of notation) that a set of elements
of
(possibly with repetition, and possibly with some elements equalling the identity) generates a one-sided or two-sided
-expander if the associated symmetric probability density
We saw in the last set of notes that expansion can be characterised in terms of random walks. One can of course specialise this characterisation to the Cayley graph case:
Exercise 5 (Random walk description of expansion) Let
be a family of finite
-regular Cayley graphs, and let
be the associated probability density functions. Let
be a constant.
- Show that the
are a two-sided expander family if and only if there exists a
such that for all sufficiently large
, one has
for some
, where
denotes the convolution of
copies of
.
- Show that the
are a one-sided expander family if and only if there exists a
such that for all sufficiently large
, one has
for some
.
In this set of notes, we will connect expansion of Cayley graphs to an important property of certain infinite groups, known as Kazhdan’s property (T) (or property (T) for short). In 1973, Margulis exploited this property to create the first known explicit and deterministic examples of expanding Cayley graphs. As it turns out, property (T) is somewhat overpowered for this purpose; in particular, we now know that there are many families of Cayley graphs for which the associated infinite group does not obey property (T) (or weaker variants of this property, such as property ). In later notes we will therefore turn to other methods of creating Cayley graphs that do not rely on property (T). Nevertheless, property (T) is of substantial intrinsic interest, and also has many connections to other parts of mathematics than the theory of expander graphs, so it is worth spending some time to discuss it here.
The material here is based in part on this recent text on property (T) by Bekka, de la Harpe, and Valette (available online here).

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