Unimodal Sequence Generating Functions Arising from Partition Ranks
Kathrin Bringmann, Chris Jennings-Shaffer

TL;DR
This paper explores generating functions related to the rank of strongly unimodal sequences, providing combinatorial interpretations, identities involving mock modular forms, asymptotic analysis, and parity results, highlighting their connection to integer partition ranks.
Contribution
It introduces new generating functions that model the rank of strongly unimodal sequences and establishes their combinatorial and modular properties, extending understanding of partition-related functions.
Findings
Derived identities involving mock modular forms
Established asymptotic behavior of the generating functions
Proved a parity result for the functions
Abstract
In this paper we study generating functions resembling the rank of strongly unimodal sequences. We give combinatorial interpretations, identities in terms of mock modular forms, asymptotics, and a parity result. Our functions imitate a relation between the rank of strongly unimodal sequences and the rank of integer partitions.
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Unimodal sequence generating functions arising from partition ranks
Kathrin Bringmann
and
Chris Jennings-Shaffer
University of Cologne, Faculty of Mathematical and Natural Sciences, Mathematical Institute, Weyertal 86-90, 50931 Cologne, Germany
Abstract.
In this paper we study generating functions resembling the rank of strongly unimodal sequences. We give combinatorial interpretations, identities in terms of mock modular forms, asymptotics, and a parity result. Our functions imitate a relation between the rank of strongly unimodal sequences and the rank of integer partitions.
Key words and phrases:
unimodal sequences, strongly unimodal sequences, partitions, overpartitions, unimodal ranks, partition ranks, Dyson rank, -rank, asymptotics, modular forms, mock modular forms
2010 Mathematics Subject Classification:
05A16, 11F03, 11P81, 11P82
The research of the first author is supported by the Alfried Krupp Prize for Young University Teachers of the Krupp foundation and the research leading to these results receives funding from the European Research Council under the European Union’s Seventh Framework Programme (FP/2007-2013) / ERC Grant agreement n. 335220 - AQSER
1. Introduction and statement of results
A sequence of positive integers is a unimodal sequence of size if it is of the form
[TABLE]
The maximum value, , is called the peak. If the inequalities are strict, the sequence is called strongly unimodal. Such sequences are related to integer partitions. Recall that a finite sequence of positive integers is a partition of size if it is of the form
[TABLE]
Unimodal sequences, partitions, and similar objects appear throughout modern and classical literature on a variety of subjects including algebra, combinatorics, number theory, physics, and special functions [1, 3, 33, 34]. To motivate our results, we discuss a few highlights in number theory. We focus on strongly unimodal sequences, rather than unimodal sequences. The enumeration function for strongly unimodal sequences seems to have first appeared as in [1], along with a wealth of related functions; unimodal sequence type counting functions can also be found in older works such as [2, 9, 35].
We let denote the number of partitions of size and let denote the number of strongly unimodal sequences of size . We note that the conventions for zero are somewhat inconsistent between strongly unimodal sequences and partitions, as we set but . By standard counting techniques, the generating functions for partitions and strongly unimodal sequences are
[TABLE]
where we use the -Pochhammer symbol, for . This extends to arbitrary by setting . Furthermore, we let . Throughout the article, is a complex variable with .
Perhaps the three most famous results for the partition function are the following. There is the asymptotic formula of Hardy and Ramanujan [22, equation (1.41)]
[TABLE]
Moreover the function
[TABLE]
is Dedekind’s eta function, which is a modular form of weight (with multiplier). Lastly, there are Ramanujan’s congruences [31]
[TABLE]
By [32, Corollary 1.2], has a similar asymptotic behavior to (1.1)
[TABLE]
However, is essentially a mixed mock modular form instead of a modular form. A mock modular form is the holomorphic part of a harmonic Maass form with nontrivial non-holomorphic part. A harmonic Maass form is a function that transforms like a modular form, satisfies similar growth conditions, but needs to only be smooth and annihilated by the weighted hyperbolic Laplacian. A mixed mock modular form is basically an element of the tensor space of modular forms and mock modular forms. These terms and their encompassing theory can be found in [15]. While does not satisfy congruences as elegant as those of , it turns out that
[TABLE]
for any prime satisfying and [18, Theorem 1.4].
Both partitions and strongly unimodal sequences have a statistic defined on them called the rank. The rank of a partition is the largest part minus the number of parts. The rank of a strongly unimodal sequence is the number of terms after the peak minus the number of terms before the peak. We note that the peak is unique for a strongly unimodal sequence, and so there is no ambiguity in this definition as we might have with ordinary unimodal sequences. We let denote the number of partitions of size with rank and let denote the number of strongly unimodal sequences of size with rank . Again by standard counting techniques we have that the relevant generating functions are given by
[TABLE]
The rank for strongly unimodal sequences is somewhat new and first appeared in [18]. However, the rank of partitions has a longer history. It was introduced by Dyson [19] in an attempt to provide a combinatorial refinement for the Ramanujan congruences modulo and , which came to full fruition in [8]. Both and are of considerable interest because of their modular properties. All of Ramanujan’s third order mock theta functions are specializations of with taken to be a root of unity multiplied by a fractional power of ; that specializations of this type are always mock modular forms was established in [17]. Also, is one of the most well known examples of a quantum modular form, which are explained at the end of Section 4.
A key link between the rank of partitions and the rank of strongly unimodal sequences is the relation between the summands in their generating functions. In particular,
[TABLE]
It is through this connection that one can easily explain the mock modular properties of . Specifically, using a certain identity (see equation (3.2.2) and entry 3.4.7 in [5]), we have
[TABLE]
Due to work of Zwegers [37, 38], the mock modular properties of the functions on the right hand-side of (1.3) are well understood.
To introduce new restricted unimodal sequences, we take the relation in (1.2) as the guiding principle. We recall three additional well-known rank functions are defined by
[TABLE]
Respectively, these are the generating functions of the Dyson rank of overpartitions [26], the -rank of overpartitions [27], and the -rank of partitions without repeated odd parts [13, 28]. For completeness, an overpartition of size is a partition of size where the last appearance of each part may (or may not) be overlined. We replace with in the summands of the generating functions above and are led to the following three definitions:
[TABLE]
The need for the factor in the definitions of and becomes apparent below when we give the combinatorial interpretations, which are given at the beginning of Sections 3, 4, and 5. We also consider the cases of these functions and set
[TABLE]
Unimodal sequence type ranks of a similar shape were introduced by Kim, Lim, and Lovejoy [23]. Their functions are given by
[TABLE]
To recall one of the combinatorial interpretations, let
[TABLE]
Then is the number of odd-balanced unimodal sequences of with rank . A unimodal sequence being odd-balanced means that the peak is even, the subsequence of even parts is strongly unimodal, and each odd part appears to the left of the peak exactly as many times as it appears to the right of the peak. We note that since the odd parts appear identically on the left and right of the peak, the rank of an odd-balanced unimodal sequence is equal to the rank of the subsequence of even parts. Kim, Lim, and Lovejoy investigated these functions in terms of their mock modular and quantum modular behavior, as well as giving some parity results. The functions and were further studied by Barnett, Folsom, Ukogu, Wesley, and Xu [11] for their mock and quantum modular properties. Our first result gives the mock modular properties of , , and .
Theorem 1.1**.**
The functions , , and , if is specialized to a root of unity times a fractional power of , are essentially mixed mock modular forms.
Specifically, Theorem 1.1 follows from Corollaries 3.2, 4.2, and 5.2.
The next theorem gives the asymptotic behavior of and as .
Theorem 1.2**.**
We have, as ,
[TABLE]
Additionally, we fully determine the parity of .
Theorem 1.3**.**
We have that is odd if and only if , where is a prime congruent to or modulo , , , , and .
We note that the generating function was simultaneously and independently introduced by Barnett, Folsom, and Wesley [12]. There the relevant function is , which the authors study for its mock and quantum Jacobi properties. Furthermore, Theorem 1.3 given above was independently discovered and given as Conjecture 1.4 in [12], and Jeremy Lovejoy has given another proof in private communications.
The article is organized as follows. In Section 2, we give the various definitions, identities, and general results required in our proofs. In Section 3, we discuss the function , beginning with its combinatorial interpretation. As it turns out, this function is the one for which we can say the least, which is surprising as it comes from the simplest of the three ranks. The relevant statement of Theorem 1.1 is contained in Corollary 3.2. Section 4 is devoted to the investigation of the function . This includes the combinatorial interpretation, identities in terms mock modular objects for Theorem 1.1 in Corollary 4.2, and the asymptotic behavior given in Theorem 1.2 is proved toward the end of the section. We also give a brief note on the formal dual and its quantum modularity. We study in Section 5; again this includes the combinatorial interpretation, mock modular properties in Corollary 5.2 for Theorem 1.1, and the asymptotics of Theorem 1.2 are proved after Corollary 5.2. In this section we end with a proof of the parity classification in Theorem 1.3 for , which is related to the arithmetic of . We conclude the article with a few remarks in Section 6.
Acknowledgments
We thank Amanda Folsom and Jeremy Lovejoy for bringing [12] to our attention. We also thank the anonymous referees for their helpful comments and pointing out various typos in an earlier version of this manuscript.
2. Preliminaries
2.1. Combinatorial results
We require several known identities and transformation for -series. We state these results in a series of lemmas. In the statements of these identities we give restrictions for convergence, however we make no mention of this in our proofs as the convergence conditions are clear and the resulting identities hold in greater generality due to analytic continuation.
The first lemma is Heine’s transformation.
Lemma 2.1**.**
[21, equation (III.1)]** Suppose that . Then we have
[TABLE]
The following is known as Watson’s transformation.
Lemma 2.2**.**
[21, equation (III.18)]** Suppose that . Then we have
[TABLE]
The next lemma is often used with partial theta functions.
Lemma 2.3**.**
[5, Theorem 6.2.1]** Suppose that and . Then we have
[TABLE]
Furthermore we use another identity related to Lemma 2.3.
Lemma 2.4**.**
[5, entry 6.3.12]** The following identity holds,
[TABLE]
We also make use of the Bailey pair machinery [3, Chapter 3]. Recall that a pair of sequences is called a Bailey pair relative to if
[TABLE]
Bailey’s Lemma is as follows.
Lemma 2.5**.**
[3, Theorem 3.4]** If is a Bailey pair relative to , then, assuming convergence conditions,
[TABLE]
The following theorem of Lovejoy gives a convenient formula for constructing Bailey pairs.
Lemma 2.6**.**
[24, Theorem 8]** The following is a Bailey pair relative to :
[TABLE]
2.2. Analytic results
To recognize the functions of interest for this paper as mixed mock modular forms, we recall a few well-known functions. For , define the Jacobi theta function
[TABLE]
Moreover we require Zwegers -function for ,
[TABLE]
and for let the higher level Appel function be given by
[TABLE]
The function is a holomorphic Jacobi form and the mock modular properties of and are described in [37, 38].
To prove Theorem 1.2, we also require the following asymptotic behavior which follows directly from the modular transformation of the Dedekind -function
[TABLE]
where the limit is taken in any region , for fixed . Moreover we need the following Tauberian Theorem.
Theorem 2.7**.**
[15, Theorem 14.4]** Let be a power series with non-negative that are monotonically increasing and have radius of convergence equal to . Suppose that
[TABLE]
for , . Then we have
[TABLE]
Remark*.*
Theorem 2.7 is commonly stated without the additional boundedness condition. However, this seems to be in error and is discussed in detail in an upcoming article [16]. In the current article, we determine the asymptotic behavior of functions via modular transformations, which actually imply as in each region (and as such, the required bound holds), so that this detail is not of major concern.
3. The function
Since the series expansions of the summands of (1.4) have both positive and negative coefficients, we interpret and both as the difference of two non-negative counts. A left-heavy overlined unimodal sequence of size is a unimodal sequence of size such that the parts up to and including all occurences of the peak form an overpartition with largest part overlined, and the parts after the peak form an overpartition with all parts overlined. Then is the number of left-heavy overlined unimodal sequences of size with an even number of non-overlined parts minus those with an odd number of non-overlined parts. Furthermore, is the same difference of counts as , but with the added restraint that the rank of the strongly unimodal sequence consisting of the overlined parts is .
Example*.*
The left-heavy overlined unimodal sequences of are , , , , and . By accounting for the parity of the non-overlined parts, we find . The ranks of the strongly unimodal subsequences consisting of the overlined parts are, respectively, [math], [math], , , and [math].
The following lemma writes in terms of and .
Lemma 3.1**.**
We have
[TABLE]
Proof.
Lemma 2.4 gives, shifting in the definition of ,
[TABLE]
shifting in the definitions of and . This gives the claim. ∎
It is not hard to conclude the following representation using (mock) modular objects, which are defined in Section 2.2.
Corollary 3.2**.**
We have
[TABLE]
4. The function
Before we state the combinatorial interpretation of and , note that the summands of have non-negative coefficients since
[TABLE]
A unimodal sequence is an -left-heavy overlined unimodal sequence if the peak is even and appears overlined exactly once (suppose it is ), the parts before and after form an overpartition, all overlined odd parts appear to the left of , and all non-overlined parts are at least and appear identically on the left and right of . Then is the number of -left-heavy overlined unimodal sequences of size and is the number of -left-heavy overlined unimodal sequences of size such that the strongly unimodal sequence consisting of the overlined even parts has rank .
Example*.*
We have since the relevant sequences are: , , , , and . The residual ranks of these sequences are [math], [math], , , and [math], respectively.
The following proposition rewrites in terms of generalized Lambert series.
Proposition 4.1**.**
We have
[TABLE]
Proof.
Applying Lemma 2.3 with , and , we find that
[TABLE]
We handle the two sums in (4) separately. For the first, we apply Lemma 2.1 with , , , , and , which gives that
[TABLE]
Next we take , , , , , and in Lemma 2.2 to find that
[TABLE]
Combining (4.2) and (4.3) gives the first summand in the proposition.
For the the second series in (4) we apply Lemma 2.2 with , , , , , and . This gives that
[TABLE]
Letting in the last sum and combining terms gives the claim. ∎
We next rewrite in terms of (mock) modular objects.
Corollary 4.2**.**
We have
[TABLE]
The asymptotic formula for in Theorem 1.2 follows from Theorem 2.7, once we establish that is monotonic.
Lemma 4.3**.**
For , we have .
Proof.
To prove the claim, we show that has non-negative coefficients. For this, we note that
[TABLE]
We first verify that has non-negative coefficients for . Given two power series and , write to indicate that has non-negative coefficients. We see that
[TABLE]
and (, resp.) is the number of partitions of with largest part , where the only other allowed parts are and , and appears an odd (even, resp.) number of times. Taking an occurrence of and replacing it by and gives an injection from the partitions counted by to those of . Thus , which implies for . However, and do have negative coefficients. By a careful grouping of as rational functions, we find . Thus for all . We carefully group and as follows,
[TABLE]
where we make use of the fact that . We then find , and thus for all . ∎
The following calculation gives the asymptotics of .
Proof of the asymptotics for in Theorem 1.2.
We begin with the representation in (4),
[TABLE]
If and in a region where , we have and the sums become and respectively. Thus
[TABLE]
Using (2.1) gives that as . We now use Theorem 2.7 with , , and to obtain the claim.
For the reader concerned about taking the limit inside the sums, one can instead apply (mock) modular transformations to the representation in Corollary 4.2 to obtain the same results. However, these calculations are considerably longer. ∎
While does not appear to posses any quantum modular properties, the formal dual does. Recall that a function , () is a quantum modular form, of weight with respect to , if the obstruction to modularity,
[TABLE]
can be extended to an analytic function on an open subset of . Quantum modular forms were introduced by Zagier in [36].
Noting that , we obtain
[TABLE]
where the second equality is Theorem 15 of [7] with . In particular,
[TABLE]
Using the now standard techniques for false theta functions [14], one can show that (4.4) is a quantum modular form, where the values of the function on the rationals are given by taking radial limits. However, since neither the series for nor truncates if is a root of unity, the behavior of one function as approaches a root of unity says nothing about the other.
5. The function
A unimodal sequence is -left heavy if the largest part is even, all odd parts appear to the left of the peak, and the subsequence consisting of the even parts is strongly unimodal. Then is the number of -left heavy unimodal sequences of size and is the number of such sequences where the strongly unimodal sequence consisting of the even parts has rank .
Example*.*
We have since the relevant sequences are: , , , , and . The residual ranks of these sequences are [math], , , [math], and [math], respectively.
The following proposition rewrites in terms of generalized Lambert series. We note that a similar expression for can be found in [30, equation (4.29)].
Proposition 5.1**.**
We have
[TABLE]
Proof.
We use Lemma 2.4 with , , , and , which gives that
[TABLE]
By entry 12.3.2 of [4], we obtain that
[TABLE]
Using equation (12.2.5) of [4] and Lemma 7.9 of [20] yields
[TABLE]
giving the claim. ∎
In the following corollary, we rewrite in terms of known (mock) modular objects.
Corollary 5.2**.**
We have
[TABLE]
Next we prove the asymptotic formula for . We note that follows trivially by taking a sequence counted by and adding a single to the left of the peak. Furthermore, this also shows that for fixed .
Proof of the asymptotics for in Theorem 1.2.
By using Proposition 5.1, we have
[TABLE]
With , , and , we find that
[TABLE]
Moreover,
[TABLE]
Thus
[TABLE]
We now use Theorem 2.7 with , , and to obtain the claim.
Again for the reader concerned with taking limits inside sums, one may instead use modular transformations with the representation in Corollary 5.2. While one can save some effort by noting , where is a third order mock theta function, these calculations are still somewhat lengthy. ∎
A first step to prove Theorem 1.3 is to rewrite modulo 2.
Proposition 5.3**.**
We have that
[TABLE]
Proof.
By taking , , , , and then letting in Lemma 2.6 we have the following Bailey pair relative to ,
[TABLE]
We then apply Lemma 2.5, with , to this Bailey pair to obtain
[TABLE]
Thus, changing in the definition of , and then using (5.1), we obtain the claim. ∎
To relate the parity of to norms of ideals in , we rewrite the sum in Proposition 5.3.
Proposition 5.4**.**
We have that
[TABLE]
Proof.
Letting , and then swapping and , we rewrite the left-hand side as
[TABLE]
For the last step, we let in the first double sum and in the second we let .
To finish the claim, we have to prove that
[TABLE]
Substituting and , we find that the right-hand side equals
[TABLE]
letting in the second sum of the left-hand side. From this it is not hard to prove (5.2). ∎
We are now ready to prove Theorem 1.3.
Proof of Theorem 1.3.
The proof requires a small amount of standard algebraic number theory. For the reader not familiar with the definitions, we offer [10, Chapter 11] and [29] as two references. By Propositions 5.3 and 5.4,
[TABLE]
We note that and if and only if .
The case of [6, Lemma 3] states that each equivalence class of solutions to , with positive, contains a unique such that and . Recall that two solutions and are equivalent if with . As such, two solutions and are equivalent exactly if and generate the same ideal in , where . Since is a principal ideal domain, we see that
[TABLE]
Let denote the number of ideals of of norm . A formula for can be determined by standard methods and for our choice of it is given in the proof of Theorem 1.3 of [25]. In particular, suppose that is positive and , where the , , and are distinct primes with , , and . Then
[TABLE]
It is not hard to see that the parity of is as claimed, since . ∎
6. Concluding Remarks
This paper introduces and proves various properties of the functions , , and . It is not difficult to see additional results remain and so we briefly mention a few of these. The interpretation of and is as the difference of non-negative counts, but it appears that is always non-negative. We leave it as an open problem to prove that is non-negative and to give a combinatorial interpretation that clearly demonstrates this. Theorem 1.2 gives the asymptotics of and . One could also ask for the asymptotics of , , and , as well as how these ranks are asymptotically distributed as . Also one could introduce and study the moments of these rank functions.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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