In
mathematics, the pentagonal number theorem, originally due to
Euler
Leonhard Euler ( , ; 15 April 170718 September 1783) was a Swiss mathematician, physicist, astronomer, geographer, logician and engineer who founded the studies of graph theory and topology and made pioneering and influential discoveries in ma ...
, relates the product and series representations of the
Euler function. It states that
:
In other words,
:
The exponents 1, 2, 5, 7, 12, ... on the right hand side are given by the formula for ''k'' = 1, −1, 2, −2, 3, ... and are called (generalized)
pentagonal numbers
A pentagonal number is a figurate number that extends the concept of triangular and square numbers to the pentagon, but, unlike the first two, the patterns involved in the construction of pentagonal numbers are not rotationally symmetrical. Th ...
. (The constant term 1 corresponds to
.)
This holds as an identity of convergent
power series
In mathematics, a power series (in one variable) is an infinite series of the form
\sum_^\infty a_n \left(x - c\right)^n = a_0 + a_1 (x - c) + a_2 (x - c)^2 + \dots
where ''an'' represents the coefficient of the ''n''th term and ''c'' is a con ...
for
, and also as an identity of
formal power series.
A striking feature of this formula is the amount of cancellation in the expansion of the product.
Relation with partitions
The identity implies a
recurrence
Recurrence and recurrent may refer to:
*''Disease recurrence'', also called relapse
*''Eternal recurrence'', or eternal return, the concept that the universe has been recurring, and will continue to recur, in a self-similar form an infinite number ...
for calculating
, the number of
partitions of ''n'':
:
or more formally,
:
where the summation is over all nonzero integers ''k'' (positive and negative) and
is the ''k''
th generalized pentagonal number. Since
for all
, the apparently infinite series on the right has only finitely many non-zero terms, enabling an efficient calculation of ''p''(''n'').
Franklin's bijective proof
The theorem can be interpreted
combinatorially in terms of
partitions. In particular, the left hand side is a
generating function
In mathematics, a generating function is a way of encoding an infinite sequence of numbers () by treating them as the coefficients of a formal power series. This series is called the generating function of the sequence. Unlike an ordinary ser ...
for the number of partitions of ''n'' into an even number of distinct parts minus the number of partitions of ''n'' into an odd number of distinct parts. Each partition of ''n'' into an even number of distinct parts contributes +1 to the coefficient of ''x''
''n''; each partition into an odd number of distinct parts contributes −1. (The article on
unrestricted partition functions discusses this type of generating function.)
For example, the coefficient of ''x''
5 is +1 because there are two ways to split 5 into an even number of distinct parts (4+1 and 3+2), but only one way to do so for an odd number of distinct parts (the one-part partition 5). However, the coefficient of ''x''
12 is −1 because there are seven ways to partition 12 into an even number of distinct parts, but there are eight ways to partition 12 into an odd number of distinct parts, and 7 − 8 = −1.
This interpretation leads to a proof of the identity by canceling pairs of matched terms (
involution method).
Consider the
Ferrers diagram of any partition of ''n'' into distinct parts. For example, the diagram below shows ''n'' = 20 and the partition 20 = 7 + 6 + 4 + 3.
:
Let ''m'' be the number of elements in the smallest row of the diagram (''m'' = 3 in the above example). Let ''s'' be the number of elements in the rightmost 45 degree line of the diagram (''s'' = 2 dots in red above, since 7−1 = 6, but 6−1 > 4). If ''m'' > ''s'', take the rightmost 45-degree line and move it to form a new row, as in the matching diagram below.
:
If m ≤ s (as in our newly formed diagram where ''m'' = 2, ''s'' = 5) we may reverse the process by moving the bottom row to form a new 45 degree line (adding 1 element to each of the first ''m'' rows), taking us back to the first diagram.
A bit of thought shows that this process always changes the parity of the number of rows, and applying the process twice brings us back to the original diagram. This enables us to pair off Ferrers diagrams contributing 1 and −1 to the ''x
n'' term of the series, resulting in a net coefficient of 0 for ''x
n''. This holds for every term ''except'' when the process cannot be performed on every Ferrers diagram with n dots. There are two such cases:
1) ''m'' = ''s'' and the rightmost diagonal and bottom row meet. For example,
:
Attempting to perform the operation would lead us to:
:
which fails to change the parity of the number of rows, and is not reversible in the sense that performing the operation again does ''not'' take us back to the original diagram. If there are ''m'' elements in the last row of the original diagram, then
:
where the new index ''k'' is taken to equal ''m''. Note that the sign associated with this partition is (−1)
''s'', which by construction equals (−1)
''m'' and (−1)
''k''.
2) ''m'' = ''s''+1 and the rightmost diagonal and bottom row meet. For example,
:
Our operation requires us to move the right diagonal to the bottom row, but that would lead to two rows of three elements, forbidden since we're counting partitions into distinct parts. This is the previous case but with one fewer row, so
:
where we take ''k'' = 1−''m'' (a negative integer). Here the associated sign is (−1)
''s'' with ''s'' = ''m''−1 = −''k'', therefore the sign is again (−1)
''k''.
In summary, it has been shown that partitions into an even number of distinct parts and an odd number of distinct parts exactly cancel each other, producing null terms 0''x
n'', except if ''n'' is a generalized pentagonal number
, in which case there is exactly one Ferrers diagram left over, producing a term (−1)
''k''''x
n''. But this is precisely what the right side of the identity says should happen, so we are finished.
Partition recurrence
We can rephrase the above proof, using
partitions, which we denote as:
,
where
.
The number of partitions of ''n'' is the partition function ''p''(''n'') having generating function:
:
Note that is the reciprocal of the product on the left hand side of our identity:
:
Let us denote the expansion of our product by
,
so that
:
.
Multiplying out the left hand side and equating coefficients on the two sides, we obtain
''a
0'' ''p''(0) = 1 and
for all
. This gives a recurrence relation defining ''p''(''n'') in terms of ''a
n'', and vice versa a recurrence for ''a
n'' in terms of ''p''(''n''). Thus, our desired result:
:
for
is equivalent to the identity
where
and ''i'' ranges over all integers such that
(this range includes both positive and negative i, so as to use both kinds of generalized pentagonal numbers). This in turn means:
:
.
In terms of sets of partitions, this is equivalent to saying that the following sets are of equal cardinality:
:
and
,
where
denotes the set of all partitions of
.
All that remains is to give a bijection from one set to the other, which is accomplished by the function ''φ'' from ''X'' to ''Y'' which maps the partition
to the partition
defined by:
:
This is an involution (a self-inverse mapping), and thus in particular a bijection, which proves our claim and the identity.
See also
The pentagonal number theorem occurs as a special case of the
Jacobi triple product.
Q-series generalize Euler's function, which is closely related to the
Dedekind eta function
In mathematics, the Dedekind eta function, named after Richard Dedekind, is a modular form of weight 1/2 and is a function defined on the upper half-plane of complex numbers, where the imaginary part is positive. It also occurs in bosonic string ...
, and occurs in the study of
modular forms. The
modulus of the
Euler function (see there for picture) shows the
fractal
In mathematics, a fractal is a geometric shape containing detailed structure at arbitrarily small scales, usually having a fractal dimension strictly exceeding the topological dimension. Many fractals appear similar at various scales, as il ...
modular group symmetry and occurs in the study of the interior of the
Mandelbrot set
The Mandelbrot set () is the set of complex numbers c for which the function f_c(z)=z^2+c does not diverge to infinity when iterated from z=0, i.e., for which the sequence f_c(0), f_c(f_c(0)), etc., remains bounded in absolute value.
This ...
.
References
*
*
External links
*
On Euler's Pentagonal Theoremat MathPages
*
De mirabilis proprietatibus numerorum pentagonaliumat Scholarly Commons.
{{DEFAULTSORT:Pentagonal Number Theorem
Theorems in number theory
Articles containing proofs
Integer partitions