Ranks of overpartitions: Asymptotics and inequalities
Alexandru Ciolan

TL;DR
This paper derives asymptotic formulas for overpartition rank generating functions, proves their equidistribution modulo c, and confirms certain inequalities between ranks for specific n values, advancing understanding of overpartition statistics.
Contribution
It provides the first asymptotic analysis of overpartition rank generating functions and proves conjectured inequalities, offering new insights into overpartition distribution and rank relations.
Findings
Overpartition ranks are asymptotically equidistributed modulo c.
Confirmed inequalities between overpartition ranks for n=6 and n=10.
Derived asymptotic formulas for overpartition rank generating functions.
Abstract
In this paper we compute asymptotics for the coefficients of an infinite class of overpartition rank generating functions. Using these results, we show that the number of overpartitions of with rank congruent to modulo is equidistributed with respect to for any as and, in addition, we prove some inequalities between ranks of overpartitions conjectured by Ji, Zhang and Zhao (2018), and Wei and Zhang (2018) for and
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Ranks of Overpartitions: Asymptotics and Inequalities
Alexandru Ciolan
Mathematical Institute, University of Cologne, Weyertal 86–90, 50931 Cologne, Germany
Abstract.
In this paper we compute asymptotics for the coefficients of an infinite class of overpartition rank generating functions. Using these results, we show that the number of overpartitions of with rank congruent to modulo is equidistributed with respect to for any as and, in addition, we prove some inequalities between ranks of overpartitions conjectured by Ji, Zhang and Zhao (2018), and Wei and Zhang (2018) for and
Key words and phrases:
Asymptotics, circle method, Dyson’s rank, inequalities, Kloosterman sums, overpartitions
2010 Mathematics Subject Classification:
11P72, 11P76, 11P82
1. Introduction and statement of results
1.1. Motivation
A partition of a positive integer is a non-increasing sequence of positive integers (called parts), usually written as a sum, which add up to The number of partitions of is denoted by For example, as the partitions of are Extending the definition, we set, by convention, and for
Among many other famous achievements, Ramanujan [24] proved that if then
[TABLE]
In order to give a combinatorial proof of these congruences, Dyson [12] introduced the rank of a partition, often known also as Dyson’s rank, which is defined to be the largest part of the partition minus the number of its parts. Dyson conjectured that the partitions of form 5 groups of equal size when sorted by their ranks modulo and that the same is true for the partitions of when working modulo 7, conjecture which was proved by Atkin and Swinnerton-Dyer [5].
An overpartition of is a partition in which the first occurrence of a part may be overlined. We denote by the number of overpartitions of For example, as the overpartitions of are Overpartitions are natural combinatorial structures associated with the -binomial theorem, Heine’s transformation or Lebesgue’s identity. For an overview and further motivation, the reader is referred to [9] and [22].
Both the partition and overpartition ranks have been extensively studied. By proving that some generating functions associated to the rank are holomorphic parts of harmonic Maass forms, Bringmann and Ono [8] showed that the rank partition function satisfies some other congruences of Ramanujan type. In the same spirit, Bringmann and Lovejoy [7] proved that the overpartition rank generating function is the holomorphic part of a harmonic Maass form of weight 1/2, while Dewar [11] made certain refinements.
It is customary to denote by the number of partitions of with rank and by the number of partitions of with rank congruent to modulo The corresponding quantities for overpartitions, and are denoted by an overline.
By means of generalized Lambert series, Lovejoy and Osburn [18] gave formulas for the rank differences for and while rank differences for were determined by Jennings-Shaffer [14]. Recently, by using -series manipulations and the and -dissection of the overpartition rank generation function, Ji, Zhang and Zhao [16] proved some identities and inequalities for the rank difference generating functions of overpartitions modulo 6 and 10, and conjectured a few others. Some further inequalities were conjectured by Wei and Zhang [26].
It is one goal of this paper to prove these conjectures. The other, more general, goal is to compute asymptotics for the ranks of overpartitions and this is what we will start with, the inequalities mentioned above, as well as the asymptotic equidistribution of following then as a consequence. In doing so, we rely on the Hardy-Ramanujan circle method and the modular transformations for overpartitions established by Bringmann and Lovejoy [7]. While the main ideas are essentially those used by Bringmann [6] in computing asymptotics for partition ranks, several complications arise and some modifications need to be carried out.
The paper is structured as follows. The rest of this section is dedicated to introducing some notation that is needed in the sequel and to formulating our main results. An outline of the proof of Theorem 1 is given in Section 2, and its proof in detail, along with that of the equidistribution of is given in Section 3. In the final section we show how to use Theorem 1 in order to prove the inequalities conjectured by Ji, Zhang and Zhao [16], and Wei and Zhang [26], which are stated in Theorems 2–4 together with some other inequalities.
1.2. Notation and preliminaries
The overpartition generating function (see, e.g., [9]) is given by
[TABLE]
where
[TABLE]
denotes, as usual, Dedekind’s eta function and with and If we use the standard -series notation
[TABLE]
for and then we know from [17] that
[TABLE]
If are coprime positive integers, and if by we denote the primitive -th root of unity, we set
[TABLE]
Let be a positive integer. Set if is even, and if is odd. Moreover, put and let the integer be defined by the congruence If let
[TABLE]
Throughout we will use, for reasons of space, the shorthand notation and In what follows, are coprime integers (in case we set and this is the only case when is allowed), and is defined by the congruence Further, let
[TABLE]
be the multiplier occurring in the transformation law of the partition function, where
[TABLE]
Remark 1*.*
The sums
[TABLE]
are known in the literature as Dedekind sums. For a nice discussion of their properties and how to compute them for small values of the reader is referred to [4, p. 62].
We next define several Kloosterman sums. Here and throughout we write to denote summation over the integers that are coprime to
If let
[TABLE]
and
[TABLE]
If and let
[TABLE]
and if and let
[TABLE]
To state our results, we need at last the following quantities. The motivation behind their expressions becomes clear if one writes down explicitly the computations done in Section 3. If let
[TABLE]
and
[TABLE]
1.3. Statement of results
We are now in shape to state our main results.
Theorem 1**.**
If are coprime positive integers with and is arbitrary, then
[TABLE]
Remark 2*.*
In computing the sums and from Theorem 1, the integer is assumed to be even, cf. Bringmann and Lovejoy [7, pp. 14–15].
While the sums involved in the asymptotic formula of might look a bit cumbersome at first, for small values of they can be computed without much effort. We exemplify below the particular instances when and we will come back to Example 2, in more detail, in Section 4.
Example 1*.*
If and the second sum in (1) does not contribute (as ), while the main asymptotic contribution from the first sum is given by the term corresponding to If we have and and if we have and Without difficulty, we see that if and if from where
[TABLE]
Example 2*.*
If and the first sum in (1) does not contribute, while the main asymptotic contribution from the second sum is given by the term corresponding to In this case, and the only positive value of is attained for As such, we have and hence
[TABLE]
On using Theorem 1 together with the identity
[TABLE]
which follows by the orthogonality of roots of unity, and the well-known fact (see, e.g., [13]) that
[TABLE]
as we obtain the following consequence.
Corollary 1**.**
If , then for any we have, as
[TABLE]
Remark 3*.*
A similar result for partition ranks was obtained recently by Males [19].
Remark 4*.*
A Rademacher-type convergent series expansion for was found by Zuckerman [27, p. 321, eq. (8.53)], and is given by
[TABLE]
The following inequalities were conjectured by Ji, Zhang and Zhao [16, Conjecture 1.6 and Conjecture 1.7], and Wei and Zhang [26, Conjecture 5.10].
Conjecture 1** (Ji–Zhang–Zhao, 2018).**
- (i)
For and we have
[TABLE] 2. (ii)
For we have
[TABLE]
Conjecture 2** (Wei–Zhang, 2018).**
For we have
[TABLE]
[TABLE]
[TABLE]
As an application of Theorem 1, we prove these conjectures and, in fact, a bit more.
Theorem 2**.**
For we have
[TABLE]
[TABLE]
[TABLE]
Theorem 3**.**
For we have
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
Theorem 4**.**
For we have
[TABLE]
[TABLE]
[TABLE]
Remark 5*.*
Similar identities and inequalities were studied, for instance, by Alwaise, Iannuzzi and Swisher [1], Bringmann [6], and Mao [20] for ranks of partitions, and by Jennings-Shaffer and Reihill [15], and Mao [21] for -ranks of partitions without repeated odd parts. By establishing identities for the overpartition rank generating functions evaluated at roots of unity analogous to those found in [15, pp. 35–38] for the -rank, the reader can come up with many other such inequalities.
Remark 6*.*
Ji, Zhang and Zhao [16] proved (1.13) for whereas the inequality (1.14) is new.
Remark 7*.*
The identities from (1.8) and (1.9) were proved by Ji, Zhang and Zhao [16], who further proved that for and for While (1.14) follows easily now for the inequality is not at all clear for , as the same authors also showed that for and for For a list of the identities and inequalities already proven, see [16, Theorem 1.4].
Remark 8*.*
The identity and inequalities from (1.8) were also proved by Wei and Zhang [26, p. 25].
2. Strategy of the proof
For the reader’s benefit, we outline the main steps in proving Theorem 1, along with several other estimates that will be used in what follows.
2.1. Circle method
The main idea of our approach is the Hardy-Ramanujan circle method. By Cauchy’s Theorem we have, for
[TABLE]
where may be taken to be the circle of radius parametrized by with in which case we obtain
[TABLE]
If are adjacent Farey fractions in the Farey sequence of order we put
[TABLE]
Splitting the path of integration along the Farey arcs where and with we have
[TABLE]
where
The reader familiar with some basics from Farey theory might immediately recognize the inequality
[TABLE]
for together with several other known facts (which are otherwise very easy to prove) such as
[TABLE]
For a nice introduction to Farey fractions, one can consult [3, Chapter 5.4].
2.2. Modular transformation laws
Our next step in the proof of Theorem 1 requires the modular transformations111In passing, we correct the definitions of and as some misprints occurred in their original expressions from [7, p. 8]. The necessary changes become clear on consulting the proof, see [7, pp. 11–17]. for established by Bringmann and Lovejoy [7], the proof of which can be found in [7, pp. 11–17]. For coprime with and and as in Section 1.2, let
[TABLE]
Furthermore, if
[TABLE]
we consider, for and as defined in Section 1.2, the Mordell-type integral
[TABLE]
If is even and or if is odd, and there might be a pole at In these cases we need to take the Cauchy principal value of the integral. We will make this precise at a later stage.
By using Poisson summation and proceeding similarly to Andrews [2], Bringmann and Lovejoy [7] proved the following transformation laws222Some further corrections are in order; namely, the “” sign in front of the expressions from (3)–(6) in their original formulation [7, Theorem 2.1] should be a “”, and the other way around for (1) and (2), the reason being that the “” sign from the expression of the residues (see [7, p. 13]) is meant to be a “”. All necessary modifications are made here..
Theorem 5** ([7, Theorem 2.1]).**
Assume the notation above and let and with and
- (1)
If and then
[TABLE] 2. (2)
If and then
[TABLE] 3. (3)
If and then
[TABLE] 4. (4)
If and then
[TABLE] 5. (5)
If and then
[TABLE] 6. (6)
If and then
[TABLE]
In addition to these modular transformations, we need some further estimates.
2.3. The Mordell integral
In the previous subsection we introduced
[TABLE]
Recalling the definition (2.2), it is easy to see that
[TABLE]
and so can only have poles in points of the form
[TABLE]
with
For and or there may be a pole at The same is true if and In both cases we must consider the Cauchy principal value of the integral that is, instead of we choose as path of integration the real line indented below 0.
The following333Note that there are a few typos in the formulation of the original result from which this lemma is inspired. More precisely, in the statement of [6, Lemma 3.1], should read should read and the factor from the definition of should be removed. These changes, however, do not affect the proof. is adapted after [6, Lemma 3.1].
Lemma 1**.**
Let and where and are adjacent Farey fractions in the Farey sequence of order If
[TABLE]
and is the fractional part of then
[TABLE]
Proof.
Let us first treat the case when is odd and we encounter no poles. We have and
[TABLE]
If we write with then since The substitution yields
[TABLE]
where is the line passing through 0 at an angle of argument One easily sees that, for
[TABLE]
As the integrand from (2.4) has no poles, we can shift the path of integration to the real line and obtain
[TABLE]
The inequality
[TABLE]
follows immediately for from the definition of and some easy manipulations, while the estimate
[TABLE]
is clear. Therefore we have
[TABLE]
and, noting that
[TABLE]
the claim follows on making the substitution
If is even and then we proceed similarly as above. If, however, the integrand in (2.3) has a pole at in both of the cases and instead of we must consider the path of integration to be the real line indented below 0.
For simplicity, let us present the case when as the case is completely analogous. After doing the same change of variables as before and (if needed) shifting the path of integration (which will now consist of a straight line passing through 0 at an angle with a small segment centered at 0 removed and replaced by a semicircle inclined also at an angle ), the new path of integration will be given by where is the positively oriented semicircle of radius around 0 below the real line and
[TABLE]
If we let be the enclosed path of integration and we set
[TABLE]
then by the Residue Theorem we obtain
[TABLE]
since inside and on the only pole of is at with residue
[TABLE]
On and we have and \Big{|}e^{-\frac{2kw^{2}}{\pi z}}\Big{|}=e^{-\frac{2k}{\pi}\operatorname{Re}\left(\frac{1}{z}\right)R^{2}}, thus the two corresponding integrals tend to 0 as whereas on we have, after a change of variables,
[TABLE]
Proceeding now along the same lines as before, we obtain
[TABLE]
and the proof is complete. ∎
2.4. Kloosterman sums
The following is a variation of [2, Lemma 4.1], cf. Bringmann [6, Lemma 3.2].
Lemma 2**.**
Let and with
- (i)
We have
[TABLE] 2. (ii)
If we have
[TABLE] 3. (iii)
If we have
[TABLE]
The implied constants are independent of and and can be taken arbitrarily.
Proof.
Part (i) follows simply on replacing by in the proof of Andrews [2, Lemma 4.1]. As the proof of (2.7) is completely analogous to that of (2.6), we deal only with part (ii). We set if is odd, and if is even. Since depends only on the residue class of modulo the left-hand side of (2.6) can be rewritten as
[TABLE]
where runs over a set of primitive residues modulo Furthermore, we have
[TABLE]
and the proof is concluded on invoking part (i) and noting that ∎
3. Asymptotics for and
We turn our focus now to the proof of Theorem 1 and proceed as described in the strategy outlined in Section 2, the whole section being dedicated to this purpose.
Proof of Theorem 1.
On using Cauchy’s Theorem and splitting the path of integration into Farey arcs as explained in Section 2.1, we obtain, from (2.1) and Theorem 5,
[TABLE]
For the reader’s convenience, we divide our proof into several steps. We start by estimating the sums and which, as we shall see, will give the main contribution. The sums and will go into an error term and will be dealt with at the end. Here the analysis will also split, as the latter two sums can be treated together.
3.1. Estimates for the sums and
To estimate notice that we can write
[TABLE]
where and the coefficients and are independent of and
On replacing by in (1.1), we have
[TABLE]
where we write It follows that
[TABLE]
with
[TABLE]
We treat the sum coming from the constant term and the two sums coming from the case separately. The former will contribute to the main term, while the latter two sums will contribute to the error term. We denote the associated sums by , and and we first estimate ( is dealt with in a similar manner).
We recall, from Section 2.1, the easy facts that
[TABLE]
We write
[TABLE]
and denote the associated sums by and This way of splitting the integral is motivated by the Farey dissection used by Rademacher [23, pp. 504–509]. It allows us to interchange summation with the integral and yields a so-called complete Kloosterman sum and two incomplete Kloosterman sums. Lemma 2 applies to both types of sums.
We first consider As we have already seen,
[TABLE]
thus as Clearly, the coefficients of regarded as a series in when evaluated at a root of unity satisfy
[TABLE]
thus, in light of the transformation behavior shown in Theorem 5, the coefficients and satisfy
[TABLE]
As the integral that appears inside the sum does not depend on in evaluating we can perform summation with respect to Using, in turn, the bound (3.3), Lemma 2, the estimates from (3.1), and the well-known bound for all we obtain
[TABLE]
For a proof of the fact that see, e.g., [3, p. 296]. Here we bound trivially
[TABLE]
and choose where denotes, as usual, the number of divisors of
Since and are treated in the exact same way, we only consider Writing
[TABLE]
we see that
[TABLE]
Again, from basic facts of Farey theory, it follows that
[TABLE]
conditions which imply the restriction of to one or two intervals in the range Therefore we can use Lemma 2 to estimate the above expression just as in the case of
As for the estimation of we can split the integration path into
[TABLE]
and denote the associated sums by and The sums and contribute to the error term and, since they are of the same shape, we only consider Further, decomposing
[TABLE]
gives
[TABLE]
Using the facts that
[TABLE]
this sum can be estimated as before against Thus,
[TABLE]
We stop here for the moment with the estimation of and turn our attention to This sum is treated in a similar manner, but some comments regarding necessary modifications are in order. On noting that
[TABLE]
we see that
[TABLE]
where By the same argument as for one sees immediately that the part which might contribute to the main term can come only from those terms with A straightforward, but rather tedious, computation shows that such terms can arise only for in the first sum, respectively for in the second sum obtained by expressing as shown in (3.7). In the former case, the contribution is given by
[TABLE]
and, in the latter, by
[TABLE]
To evaluate note that one can split the sum over into groups based on the value which is defined in terms of and In each such group, the value of (hence the condition ) is independent of and the number of terms satisfying is finite and bounded in terms of (hence of ). Moreover, the coefficients and are independent of in any such fixed group. Since the terms with from (3.8) can be estimated as in the case of we obtain
[TABLE]
with and as defined in (1.4) and (1.5). In a completely similar way, we compute
[TABLE]
where we define
[TABLE]
and
[TABLE]
An easy computation shows that if then for all and that if and only if and case which is impossible as it leads to and by assumption is odd, while the condition implies that is odd as well. Therefore will only contribute to the error term.
To finish the estimation of these sums, we are only left with computing integrals of the form
[TABLE]
which, upon substituting are equal to
[TABLE]
To compute these integrals, we proceed in the way described by Dragonette [10, p. 492] and made more precise by Bringmann [6, p. 3497]. In doing so, we enclose the path of integration by including the smaller arc of the circle through and tangent to the imaginary axis at 0, which we denote by If then is given by with Using the fact that and on the smaller arc, the integral along this arc is seen to be of order O\big{(}n^{-\frac{3}{4}}\big{)}. By Cauchy’s Theorem, the path of integration in (3.10) can be further changed into the larger arc of hence
[TABLE]
Making the substitution gives
[TABLE]
where and Using the Hankel integral formula, we compute (see, e.g, [25, §3.7 and §6.2])
[TABLE]
hence
[TABLE]
On applying (3.11) to (3.6) and (3.9) for and respectively, we have
[TABLE]
3.2. Estimates for the sums and
We show that these sums contribute only to the error term. Let us start our discussion with which equals
[TABLE]
Although not written down explicitly in [7], one can readily see, e.g., by inspecting the proof of Theorem 2.1 from [7, pp. 11–17], that
[TABLE]
where we set We can rewrite this as
[TABLE]
with and the coefficients being independent of and Now the sum coming from will go, as we have seen in the case of into an error term of the form hence
[TABLE]
As for the sum coming from the constant term, let us denote it simply by on splitting the path of integration exactly as in the case of and working out the estimates in a similar manner, we obtain
[TABLE]
By applying part (iii) of Lemma 2 and arguing as in the case of (except that now ), we get
[TABLE]
proving the claim.
We next deal with and The reader interested in writing down the computations explicitly will see that the two sums can be expressed as
[TABLE]
and
[TABLE]
where and the coefficients and are independent of and Since , it is obvious that both sums will be of order the argument being the same as for
3.3. Estimates for the sums and
The estimation of the remaining sums and is not difficult and is inspired by Bringmann [6, p. 3497]. Let us, however, elaborate a bit more here. Again, we split the path of integration as in (3.2). The resulting sums can each be bounded on the various intervals of integration by
[TABLE]
for any Here we have used, in turn, a trivial bound for the Kloosterman sums appearing in front of the integrals from and Lemma 1, and the easy estimate
[TABLE]
By this we conclude the rather lengthy proof of Theorem 1. ∎
Proof of Corollary 1.
Let us first assume On combining Theorem 1 and identity (1.7), we obtain
[TABLE]
where and is arbitrary. As we know that
[TABLE]
Since (as summation of the terms in (3.3) can only start from meaning that the asymptotic contribution of these sums is (at most) of order thus dominated by
We claim that the same is true for the contribution coming from the sums. For this, note that, directly from the definition (1.4), it follows that therefore
[TABLE]
If summation of the terms in (3.3) starts from (note that ), then there is nothing to prove; so assume It is an easy exercise to prove that equality above cannot be, in fact, obtained, and that, since we have with thereby proving the claim.
In case we leave it as an exercise, to the interested reader, to prove that the coefficients of are of order and are thus dominated by This can be done by using the transformation behavior described in [7, Corollary 4.2] and carrying out estimates similar to those from the proof of Theorem 1. ∎
4. A few inequalities
In this section we prove the inequalities stated in Theorems 2–4. We will elaborate more on Theorem 2, while only sketching the main steps in the proofs of Theorems 3 and 4, as the ideas are similar.
Before giving the proof of Theorem 2, we must establish some identities. The following is an easy generalization of [16, Lemma 3.1].
Lemma 3**.**
If is odd and , then
[TABLE]
Proof.
Plugging into (1.2) gives
[TABLE]
Using the fact that which can be easily deduced from (see, e.g., [17, Proposition 1.1]), and noting that and for odd, we can rewrite (4.1) as
[TABLE]
which concludes the proof. ∎
In a similar fashion, we have the following result. For a proof of the case see [16, Lemma 2.1].
Lemma 4**.**
If is odd and then
[TABLE]
Proof of Theorem 2.
Setting and in Lemma 3, we obtain
[TABLE]
and
[TABLE]
Subtracting (4) from (4) yields
[TABLE]
thus proving (1.11) is equivalent to showing that, for
[TABLE]
For we have and if and only if in which case hence
[TABLE]
whereas, for and we have if and only if in which case thus
[TABLE]
We further compute
[TABLE]
and so the term corresponding to in the sum from (4.4) is given by
[TABLE]
Using a trivial bound for the Kloosterman sum from (4.5) and taking into account the contributions coming from the various error terms involved, estimates which we make explicit at the end of this section, we see that this term is dominant for hence
[TABLE]
for In Mathematica we see that the inequality is true for as well.
To prove (1.12), we set and in Lemma 3 and obtain
[TABLE]
and
[TABLE]
Combining (4) and (4) and setting we obtain
[TABLE]
hence, as it is easy to see that proving the claim amounts to showing
[TABLE]
for all which follows from the estimates used for proving (1.11). The proof of (1.13) follows simply on adding the inequalities (1.11) and (1.12). ∎
We can also sketch now the proofs of Theorems 3 and 4.
Proof of Theorem 3 (Sketch).
Reasoning along the same lines, on setting in Lemma 4 and recalling (1.3), the claim is equivalent to proving
[TABLE]
for It is easy to see that, for and we have and if and only if in which case thus the dominant term of
[TABLE]
is given by
[TABLE]
By working out similar bounds as in the proof of (1.11) and checking numerically for the small values of the proof of (1.14) is concluded.
The inequalities (1.15)–(1.17) are equivalent to those from (1.18)–(1.20). The proof relies on the identity
[TABLE]
and details are left to the interested reader. The fact that follows easily from adding the identities and ∎
Proof of Theorem 4 (Sketch).
By using either [26, Lemma 5.1] (on identifying the notation ) or identity (1.7) (which, in combination with (1.2), amounts to the same result), we have
[TABLE]
In light of Remark 7, to prove the inequalities (1.21)–(1.23) it suffices to show that, for
[TABLE]
[TABLE]
[TABLE]
Therefore, on combining (4.9) and (4.10), the first inequality above is equivalent to
[TABLE]
whereas, for the second and third are equivalent, on combining (4.8) and (4.9), to
[TABLE]
Again, the attentive reader might wonder what happens with the term (coming from the case in (1.7)), to which Theorem 5 does not apply, as its statement is formulated under the assumption However, while working out the transformations found by Bringmann and Lovejoy in this case, see [7, Corollary 4.2], and doing the same estimates as in the proof of Theorem 1, one can easily infer that the sums involved are of order Therefore, as grows large, we only need to prove (4.12) and (4.13), which follow immediately from Theorem 1. Again, explicit bounds can be provided just as described in the next subsection, and a numerical check for the small values of concludes the proof. ∎
4.1. Some explicit computations
As we have mentioned earlier, we will now fill in the missing details from the proof of (1.11), by explaining how to bound the different sums and error terms appearing in (4.4) and (4.5). The same arguments apply for all the other inequalities. We have already seen that
[TABLE]
and that the term corresponding to in (4.4) equals
[TABLE]
By using a trivial bound for the Kloosterman sums involved, the remaining terms can be estimated against
[TABLE]
and the contribution coming from is seen to be less than
[TABLE]
Making the path of integration symmetric in (3.6) introduces an error that can be estimated against
[TABLE]
while integrating along the smaller arc of gives an error not bigger than
[TABLE]
The sums and do not contribute in the case whereas can be treated simultaneously. The contribution coming from can be estimated against
[TABLE]
and that coming from against
[TABLE]
Using the bound (3.3) for and we get and and similarly for and Finally, the estimates in Lemma 1 can be made explicit so as to give
[TABLE]
and
[TABLE]
For and we proceed just like in (4.15) to get
[TABLE]
as an overall bound for the main contribution in (4.5) and we use the same estimates from (4.16)–(4.22) on changing whatever necessary, e.g., the sums will now run over and Putting all estimates together, we see that the term in (4.14) is dominant for The inequality (1.11) can be checked numerically in Mathematica to hold true also for
Acknowledgments
The author is grateful to Kathrin Bringmann for suggesting this project and for many useful discussions, and to Chris Jennings-Shaffer for permanent advice, as well as for the patience of carefully reading an earlier version of the manuscript and double-checking some computations. The author would also like to kindly thank the anonymous referee for the very helpful suggestions made on improving the exposition of this paper. The work was supported by the European Research Council under the European Union’s Seventh Framework Programme (FP/2007–2013)/ERC Grant agreement n. 335220 — AQSER.
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