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Let be a finite group that acts on a finite set,
. Given elements
and
, we introduce the cycle notation,
to denote that
, but
for all
. We say that
is a
-cycle in
. Conceptually, this is a natural construction: the action of
on
induces a map,
, of
into the symmetric group of
. This allows us to decompose the image of any element
into disjoint cycles.
Let the expression denote the number of
-cycles of
. Let
be the set of all
-cycles contained in elements of
. In particular, for
,
because
-cycles are fixed points of elements of
, and
fixes every element of
. Note that if
is nonempty, then
acts on
by conjugation: if
, then
is a cycle in
, so
. Parker’s lemma is the following:
Lemma 1 (Parker’s Lemma) The number of orbits of
on
is
At first glance, this lemma appears to be a straightforward application of Burnside’s orbit counting lemma:
In fact, the case is Burnside’s lemma: the number,
, is the number of
-cycles of
, i.e.
. However, for
, if
is nonempty, then
. Thus, we cannot simply equate terms:
, in general. The difficulties described above suggest that Parker’s lemma is a stronger statement than Burnside’s lemma. In fact, I am unaware of any proof in the literature that deduces Parker’s lemma as a consequence of Burnside’s Lemma. The aim of this post is to establish Parker’s lemma as a simple consequence of Burnside’s lemma.
Proof: We assume that is nonempty, otherwise the result is trivial. We note that by Burnside’s lemma
Define subsets by
For each , choose
such that
. Let
be the pointwise stabilizer of
. Then
is the set of elements of
that contain
, and
is the stabilizer of
. Note that
for
, with
. Indeed, if
, where
, then
is disjoint from
, i.e.
, which is a contradiction. Thus, because
, we see that
is a partition of
. Therefore,
, and hence
because . Now, we count the order of
and
by counting points along the fiber of the canonical projection
Indeed,
Thus,
as desired.