Convolution estimates and the number of disjoint partitions
Paata Ivanisvili

TL;DR
This paper provides an upper bound estimate for the number of disjoint partitions within a finite set collection, extending previous results to arbitrary numbers of partitions using convolution estimates.
Contribution
It generalizes the Kane-Tao result for three partitions to any finite number of disjoint partitions with a new bounding function.
Findings
Derived an explicit upper bound for the count of disjoint partitions.
Extended previous specific case to general finite cases.
Provided a mathematical estimate involving the function c(n).
Abstract
Let be a finite collection of sets. We count the number of ways a disjoint union of subsets in is a set in , and estimate this number from above by where This extends the recent result of Kane-Tao, corresponding to the case where , to an arbitrary finite number of disjoint partitions.
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Convolution estimates and the number of disjoint partitions
Paata Ivanisvili
Department of Mathematics, Kent State University
1300 Lefton Esplanade, Kent OH 44242
[email protected] This paper is based upon work supported by the National Science Foundation under Grant No. DMS-1440140 while the author was in residence at the Mathematical Sciences Research Institute in Berkeley, California, during the Spring 2017 semester.
(Submitted: May 27, 2017; Accepted: May 27, 2017; Published: XX
Mathematics Subject Classifications: 11B30)
Abstract
Let be a finite collection of sets. We count the number of ways a disjoint union of subsets in is a set in , and estimate this number from above by where
[TABLE]
This extends the recent result of Kane–Tao, corresponding to the case where , to an arbitrary finite number of disjoint partitions.
1 Introduction
Let be the Hamming cube of dimension . Set to be the corner of . Take a finite number of functions , and define the convolution at the corner as
[TABLE]
Given define its norm () in a standard way
[TABLE]
For we set
[TABLE]
Our main result is the following theorem
Theorem 1**.**
For any , and any we have
[TABLE]
Moreover, for each fixed exponent is the best possible in the sense that it cannot be replaced by any larger number.
As an immediate application we obtain the following corollary (see Section 2.3 below).
Corollary 2**.**
Let be a finite collection of sets. Then
[TABLE]
where denotes the disjoint union, and denotes cardinality of the set.
The corollary extends a recent result of Kane–Tao [1], corresponding to the case where , to an arbitrary finite number disjoint partitions.
2 The proof of the theorem
Following [1] the proof goes by induction on the dimension of the cube . The case , which is the most difficult, is the main contribution of the current paper.
2.1 Basis:
In this case, set and for . Then the inequality (1) takes the form
[TABLE]
We do encourage the reader first to try to prove (3) in the case , or visit [1], to see what is the obstacle. For example, when equality in (3) is attained at several points. Besides, direct differentiation of (3) reveals many “bad” critical points at which finding the values of (3) would require numerical computations [1]. The number of critical points together with equality cases increases as becomes larger, therefore one is forced to come up with a different idea. We will overcome this obstacle by looking at (3) in dual coordinates.
Without loss of generality we can assume that and are nonnegative for . Moreover, we can assume that for all otherwise the inequality (3) is trivial.
Let us divide (3) by . Denoting we see that it is enough to prove the following lemma.
Lemma 3**.**
For any and all we have
[TABLE]
where
Proof.
For the lemma is trivial. By induction on , monotonicity of the map
[TABLE]
and the fact that is decreasing, we can assume that all are strictly positive. For convenience we set . Introducing new variables we rewrite (4) as follows
[TABLE]
Concavity of the function provides us with a simple representation of the logarithmic function
[TABLE]
Therefore we are left to show that for all and all we have
[TABLE]
where and . Notice that given a vector , the infimum of in cannot be reached at infinity because of the slow growth of the logarithmic function. Therefore, we look at critical points of in
[TABLE]
Notice that . Therefore
[TABLE]
Setting , and introducing new variables again we are left to show that
[TABLE]
for all . It is straightforward to check that on the diagonal, i.e., when .
In general, we notice that critical points of satisfy the equation
[TABLE]
Equation (5) gives the identity , and so at critical points (5) we are only left to show
[TABLE]
Since the mapping
[TABLE]
is increasing on and decreasing on the remaining part of the ray, we can assume without loss of generality that numbers of equal to , and the remaining numbers of equal to . Moreover, we can assume that otherwise the statement is already proved. From (5), we have
[TABLE]
From the equality of the first and the third expressions in (7) it follows that
[TABLE]
In order to be positive we assume that the numerator of (8) is non negative. If we plug the expression for from (8) into the first equality of (7) then after some simplifications we obtain the following equation in the variable
[TABLE]
It follows from (7) that , and so using (9) we obtain
[TABLE]
Therefore at critical points (6) simplifies as follows
[TABLE]
Now it is pretty straightforward to show that (10) is non negative even under the assumption for . Indeed, notice that , and the map
[TABLE]
is increasing on . Therefore it is enough to check nonnegativity of (10) when , in which case the inequality follows again using , and the fact that the map
[TABLE]
is increasing for . ∎
Remark 4*.*
Choice gives equality in (4), and this confirms the fact that is the best possible in Theorem 1.
2.2 Inductive step
Inductive step is the same as in [1] without any modifications. This is a standard argument for obtaining estimates on the Hamming cube (see for example [2]). In order to make the paper self contained we decided to repeat the argument.
Suppose (1) is true on the Hamming cube of dimension . Without loss of generality assume , and set for all . Define
[TABLE]
For , let where is the vector consisting of the first coordinates of , and number denotes the last coordinate of . Set
[TABLE]
We have
[TABLE]
2.3 The proof of Corollary 2
Without loss of generality we may assume that all the sets in are subsets of with some natural (see [1]). For define functions
[TABLE]
as follows:
[TABLE]
if the set lies in , and otherwise. Finally we define
[TABLE]
if the set lies in , and otherwise. Notice that in this case inequality (1) becomes (2).
Acknowledgements
I would like to thank an anonymous referee, and Benjamin Jaye for helpful comments.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] D. Kane, T. Tao, A bound on Partitioning Clusters. The Electronic Journal of Combinatorics , Volume 24, Issue 2 (2017), Paper #P 2.31, Pages 13.
- 2[2] P. Ivanisvili, A. Volberg. Poincaré inequality 3/2 on the Hamming cube. ar Xiv:1608.04021 (2016).
