Inverse problems of the Erdős-Ko-Rado type theorems for families of vector spaces and permutations
Abstract
Ever since the famous Erdős-Ko-Rado theorem initiated the study of intersecting families of subsets, extremal problems regarding intersecting properties of families of various combinatorial objects have been extensively investigated. Among them, studies about families of subsets, vector spaces and permutations are of particular concerns.
Recently, the authors proposed a new quantitative intersection problem for families of subsets: For , define its total intersection number as . Then, what is the structure of when it has the maximal total intersection number among all families in with the same family size? In [23], the authors studied this problem and characterized extremal structures of families maximizing the total intersection number of given sizes.
In this paper, we consider the analogues of this problem for families of vector spaces and permutations. For certain ranges of family size, we provide structural characterizations for both families of subspaces and families of permutations having maximal total intersection numbers. To some extent, these results determine the unique structure of the optimal family for some certain values of and characterize the relation between having maximal total intersection number and being intersecting. Besides, we also show several upper bounds on the total intersection numbers for both families of subspaces and families of permutations of given sizes.
Keywords: total intersection number, vector spaces, permutations.
AMS subject classifications: 05D05.
1 Introduction
For a positive integer , let and denote the collection of all -element subsets of . A family is called intersecting if any two of its members share at least one common element. The classic Erdős-Ko-Rado theorem states that if , an intersecting family has size at most ; if the equality holds, the family must be consisted of all -subsets of containing a fixed element. Inspired by this cornerstone result in extremal set theory, there have been a great deal of extensions and variations. As two major extensions, intersection problems for families of permutations and families of subspaces over a given finite field have drawn lots of attentions in these years.
Let be the finite field with elements and be an -dimensional vector space over . Denote as the collection of all -dimensional subspaces of and for , is called -intersecting if holds for all . In 1986, using spectra method, Frankl and Wilson [18] proved the following analogue result of Erdős-Ko-Rado theorem for -intersecting family of subspaces of . Since then, many other kinds of intersection problems for families of subspaces have been studied, for examples, see [7, 30, 5].
Theorem 1.1.
([18]) Let and be integers and let be a -intersecting family, then . Moreover, when , the equality holds if and only if is the family of -dim subspaces containing a fixed -dim subspace.
Let be the symmetric group of all permutations of and for , a subset is called -intersecting if there exist distinct integers such that for and . Let , if are distinct and are distinct, then is a coset of the stabilizer of points, which is referred as a -coset. In [16], Deza and Frankl proved the following theorem for -intersecting family of permutations.
Theorem 1.2.
([16]) For any positive integer , if is -intersecting, then .
Clearly, a -coset is a -intersecting family of size . Deza and Frankl [16] conjectured that the -cosets are the only -intersecting families of permutations with size . This conjecture was first confirmed by Cameron and Ku [6] and independently by Larose and Malvenuto [26]. As for -intersecting families of permutations when , in the same paper, Deza and Frankl also conjectured that the -cosets are the only largest -intersecting families in provided is large enough. Using eigenvalue techniques together with the representation theory of , Ellis, Friedgut and Pilpel [14] proved this conjecture.
Following the path led by Erdős, Ko and Rado, the above studies of intersections problems about subspaces and permutations share a same type of flavour: Given a family of subspaces or permutations with some certain kind of intersecting property, people try to figure out how large this family can be. Once the maximal size of the family with given intersecting property is determined, people turn to an immediate inverse problem — characterizing the structure of the extremal family. This gives rise to further studies of the stability and supersaturation for extremal families. In recent years, there have been a lot of works concerning this kind of inverse problems, for examples, see [2, 8, 1, 22, 11, 17, 29, 19, 9].
In this paper, with the same spirit, we consider an inverse problem for intersecting families of subspaces and permutations from another point of view. Instead of being intersecting, we assume that the family possesses a certain property that “maximizes” the intersections quantitatively. The study of this kind of inverse problem was first initiated by the first and the last authors in [23], where families of subsets were investigated.
To state the problem formally, first, we introduce the notion total intersection number of a family. Let be the underlying set with finite members, can be , or for an -dimensional space over , or . Consider a family , the total intersection number of is defined by
(1) |
where has different meanings for different s. When , ; when , ; when , . Moreover, we denote
(2) |
as the maximal total intersection number among all families in with the same size of and we denote it as for short if is clear. Similarly, for two families and in , the total intersection number between and is defined as
(3) |
Clearly, we have .
Certainly, the value of reveals the level of intersections among the members of : the larger is, the more intersections there will be in . For an integer , note that being -intersecting also indicates that possesses a large amount of intersections, therefore, it is natural to ask the relationship between being -intersecting and having large :
Question 1.3.
For and large enough, denote as the maximal size of the -intersecting family in . Let with size , if , is a -intersecting family? Or, if is a maximal -intersecting family in , do we have ?
In [23], by taking , we show that when and , the full -star (the family consisting of all -sets in containing fixed elements) is indeed the only structure of , which answers the Question 1.3 for the case . In this paper, when and is large enough, we obtain similar results for general ; when , we answer the Question 1.3 for the case . Noticed that the property of having maximal total intersection number can be considered for families of any size. Actually, we can ask the following more general question:
Question 1.4.
For a family , if , what can we say about its structure?
Aiming to solve these questions, we provide structural characterizations for optimal families satisfying for both of the cases when and . Moreover, we also obtain some upper bounds on for several ranges of for both cases. The detailed descriptions of our results will be shown in the following subsection.
1.1 Our results
When , through combinatorial arguments, we have the following theorem which shows the main structure of the optimal family with not much larger than .
Theorem 1.5.
Given positive integers and , let be a family of -dim subspaces of with size for some satisfying . Then, when , is contained in a full -star and when , contains a full -star.
When , for an integer , consider the subfamilies of consisting of pairwise disjoint -cosets and permutations from another -coset disjoint with all the former -cosets. We denote as the family of this form with size with maximal total intersection number. Using eigenvalue techniques together with the representation theory of , we prove that families of permutations of size having large total intersection numbers are close to the union of -cosets.
Theorem 1.6.
For a sufficiently large integer , there exist positive constants and such that the following holds. For integer , let and such that . If is a subfamily of with size and , then there exists some consisting of -cosets such that
Moreover, when , for some consisting of pairwise disjoint -cosets.
Moreover, using linear programming method over association schemes, we also have the following upper bounds on .
Theorem 1.7.
Given positive integers , , with and , for with , we have
(4) |
especially, when and , we have
(5) |
Theorem 1.8.
Given positive integers and , for with , we have
1.2 Notations and Outline
Throughout this paper, we shall use the following standard mathematical notations .
-
•
Denote as the set of all nonnegative integers. For any , let . For any such that , let .
-
•
Given finite set and any positive integer , denote as the family of all -subsets of and as the family of all subsets of .
-
•
For a given prime power and a positive integer , we denote as a finite field with elements and as the -dimensional vector space over . Moreover, for a vector with length , we denote as the position of for .
-
•
For two subspaces , we denote as the sum of these two subspaces and as the quotient subspace of by . If , we denote as the direct sum of . Moreover, we have and .
-
•
For a given prime power and positive integers , with , the Gaussian binomial coefficient is defined by
Usually, the is omitted when it is clear.
-
•
For a given family in and a -dim subspace , we denote as the subfamily in containing and is called the degree of in .
The remainder of the paper is organized as follows. In Section 2, we will introduce some basic notions and known results on general association schemes, representation theory of and spectra of Cayley graphs on . Moreover, we also include some preliminary lemmas for the proof of our main results. In Section 3, we consider families of vector spaces and prove Theorem 1.5. In Section 4, we consider families of permutations and prove Theorem 1.6. And we prove Theorem 1.7 and Theorem 1.8 in Section 5. Finally, we will conclude the paper and discuss some remaining problems in Section 6.
2 Preliminaries
In this section, we will introduce some necessary notions and related results to support proofs of our theorems. First, we will introduce some notions about general association schemes, which are crucial for the proof of the upper bounds on for and . Then, we shall give a brief introduction on the representation theory of . Finally, we will review some known results about spectra of Cayley graphs on . Readers familiar with these parts are invited to skip corresponding subsections. Based on these results, we will provide some new estimations about eigenvalues of Cayley graphs on for the proof of Theorem 1.6.
2.1 Association schemes
Association scheme is one of the most important topics in algebraic combinatorics, coding theory, etc. Many questions concerning distance-regular graphs are best solved in this framework, see [3],[4]. In 1973, by performing linear programming methods on specific association schemes, Delsarte [10] proved many of the sharpest bounds on the size of a code, which demonstrated the power of association schemes in coding theory. Since then, association schemes have been widely studied and related notions have also been extended to other objects, such as equiangular lines and special codes, etc. In this subsection, we only include some basic notions about association schemes. For more details about association schemes, we recommend [10] and [20] as standard references.
Let be a finite set with elements, and for any integer , let be a family of relations on . The pair is called an association scheme with classes if the following three conditions are satisfied:
-
1.
The set is a partition of and is the diagonal relation, i.e., .
-
2.
For , the inverse of the relation also belongs to .
-
3.
For any triple of integers , there exists a number such that, for all :
And s are called the of .
For relation , the adjacency matrix of is defined as follows:
The space consisting of all complex linear combinations of the matrices in an association scheme is called a - . Moreover, denote as the matrix with all entries 1, there is a set of pairwise orthogonal idempotent matrices , which forms another basis of this Bose-Mesner algebra. The relations between and are shown as follows:
(6) |
where are the eigenvalues of , which are called the of the association scheme; and are known as of the association scheme. Usually, denotes the number of 1’s in each row of and . According to [20], for , s and s have the following relation:
(7) |
Let be a set of relations on of an association scheme. Given a subset with , the of with respect to is an -tuple of nonnegative rational numbers given by
(8) |
Clearly, we have and .
Moveover, let be the indicator vector of with respect to , i.e., , if and , if . Then, can be rewritten as
(9) |
Besides, for , define
(10) |
and as the of . By combining and together, we have the following lemma which provides a linear relationship between s and s.
Lemma 2.1.
Given an association scheme with classes and . Let with size , then for and defined in and respectively, we have
As a consequence of Lemma 2.1, we have the following properties of .
Lemma 2.2.
([27], Theorem 12 in Section 6, Chapter 21) Given an association scheme with classes and . Let with size and be defined as , then for all .
Lemma 2.3.
With the same conditions as those in Lemma 2.2, for , we have
(11) |
2.2 Background on the representation theory of
A partition of is a nonincreasing sequence of positive integers summing to , i.e., a sequence with and , and we write . The Young diagram of is an array of cells, having left-justified rows, where row contains cells. For example, the Young diagram of the partition is:
{ytableau}&
If the array contains the numbers in some order in place of dots, we call it -tableau, for example,
{ytableau}5 & 1 3
2 4
6 7
is a -tableau. Two -tableaux are said to be row-equivalent if they have the same numbers in each row; if a -tableau has rows and columns , then we let be the row-stabilizer of and be the column-stabilizer of .
A -tabloid is a -tableau with unordered row entries. Given a tableau , denote as the tabloid it produces. For example, the -tableau above produces the following -tabloid:
For given group and set , denote as the identity in . The left action of on is a function (denoted by ) such that for all and
Now, consider the left action of on , the set of all -tabloids; let be the corresponding permutation module, i.e., the complex vector space with basis and the action of on linearly extended from the action of on . Given a -tableau , the corresponding -polytabloid is defined as
We define the Specht module to be the submodule of spanned by the -polytabloids:
As shown in [14], any irreducible representation of is isomorphic to some . This leads to a one to one correspondence between irreducible representations and partitions of . In the following of this paper, for convenience, we shall write for the equivalence class of the irreducible representation , for the character (The formal definition of the character of a representation will be presented in Section 2.3.1).
Let be a partition of . If its Young diagram has columns of lengths , then the partition is called the transpose (or conjugate) of . Consider each cell in the Young diagram of , the hook of is . The hook length of is . As an important parameter, the dimension of the Specht module is given by the following theorem:
Theorem 2.4.
([15]) If is a partition of with hook lengths , then
(12) |
As an immediate consequence of Theorem 2.4, we have .
2.3 Spectra of Cayley graphs on
2.3.1 Basics and known results
Given a group and an inverse-closed subset , the Cayley graph on generated by , denoted by , is the graph with vertex-set and edge-set . Cayley graphs have been studied for many years and are a class of the most important structures in algebraic graph theory. Here, we only consider a very special kind of Cayley graphs where and is a union of conjugacy classes.
For fixed , consider the Cayley graph on with generating set
When , the corresponding Cayley graph is also called the derangement graph on .
For , denote as the coset consisting of permutations with . In [14], by taking as a union of conjugacy classes, the authors used the representation theory of and obtained the following results about the eigenvalues of :
(13) |
where the character of is the map defined by
and denotes the trace of the linear map of . If there is no confusion, for a partition of , we also use the notation to denote the corresponding irreducible representation of (For this correspondence, see Theorem 14 in [14].).
Let be the number of derangements in , using the inclusion-exclusion formula, we have
From [14], we know that for , the eigenvalues of satisfy:
(14) | ||||
where is an absolute constant. And the eigenvalues of satisfy:
(15) | ||||
where depends on alone. As shown in [13], for s with different s and the same , their corresponding eigenspaces are the same with dimension . For each , define
It was proved in [14] that is the linear span of the characteristic functions of the -cosets of , i.e.,
where for and , is a -coset of . Moreover, write . Clearly, s are pairwise orthogonal and
(16) |
During their study of intersecting families for permutations in [14], Ellis, Friedgut and Pilpel developed several tools to estimate the spectra of s, we include the following three lemmas which are useful for our estimations of the eigenvalues of s.
Lemma 2.5.
([14], Lemma 6) Let be a finite group, let be inverse-closed and conjugation-invariant, and let be the Cayley graph on with generating set . Let be an irreducible representation of with dimension , and let be the corresponding eigenvalue of . Then
(17) |
Lemma 2.6.
([14], Claim 1 in Section 3.2.1) Let be an irreducible representation whose first row or column is of length . Then
(18) |
Theorem 2.7.
([28]) If , then there exists such that for all , any irreducible representation of which has all rows and columns of length at most has
(19) |
The above three lemmas provide a way to control based on the dimension of . When the structure of the partition is relatively simple, ’s dimension can be well bounded and therefore leads to a good control of . When the dimension of is relatively large, this method no longer works. Thus, we need the following results from [24] and [25].
Theorem 2.8.
([24], Theorem 3.7) Let and . Let be the Young diagram obtained from by removing the right most box from any row of the diagram so that the resulting diagram is still a partition of . Then
(20) |
Theorem 2.9.
([25], Theorem 3.5) Let be integers with , and . Then
(21) |
For positive integers and , we write if for some constant that depends only on .
Theorem 2.10.
([25], Theorem 3.9) Let be integers with , and , with , and . Then
(22) |
Let be integers with and . We define , and we also need the following lemma.
Lemma 2.11.
([25], Lemma 3.16) Let and . Then
(23) |
2.3.2 Some new results about s
In this part, first, we shall prove two identities of the linear combinations of s. Then, using aforementioned results, we will provide some new estimations about for and .
Based on the formula of , we have the following simple identity.
Proposition 2.12.
For any positive integer , we have
(24) |
Proof.
First, by interchanging the summation order of the LHS of (24), we have
Now, let and be the generating function of sequence . Then, we have and
Let and be the generating function of sequence . From the above equality and the property of products of generating functions, we immediately have
Therefore, and
This completes the proof of (24). ∎
As an application of Proposition 2.12, we can prove the following lemma.
Lemma 2.13.
For any integer ,
(25) | |||
(26) |
Proof.
Denote . According to (2.3.1), for fixed and , we have . However, this bound is not good enough. When the index varies from to , the constant might become relatively large. Thus, if we try to get similar identities as (25) and (26) for with , we need some more delicate evaluations about s for .
According to the structure of their corresponding partitions, we can divide into the following four parts:
Clearly, are formed by these four parts and all of them are pairwise disjoint. Based on the known results, we can prove the following bounds about s for .
Lemma 2.14.
Let be positive integers with sufficiently large. Then,
-
•
When , we have for all .
-
•
When , we have for , where is an absolute constant; and for or .
-
•
When , we have for ; and for .
Proof.
Consider the eigenvalues corresponding to irreducible representations in . For each , assume that the length of the first row or column of is . When , since is increasing in the range and is decreasing in the range , thus, we have . By Lemma 2.6, . When , has all rows and columns of length at most . Since is sufficiently large, by Theorem 2.7, . Therefore, for all , we have . Note that . By Lemma 2.5, we have
for all and . According to Theorem 2.9, . Thus, we also have .
Consider the eigenvalues corresponding to irreducible representations in . Based on structures of Young diagrams of and , one can easily get their hook lengths. Thus, by Theorem 2.4, and . Take in Theorem 2.10, for , we have
For and sufficiently large, this leads to and . For , we have and . This indicates that
for all , where are absolute constants. For , since we already have and , by Lemma 2.5 and , we have
Consider the eigenvalues corresponding to irreducible representations in . For , by Lemma 2.11, we have and . Therefore, we have
for all . For , based on the structure of , we have
by Theorem 2.8. Since and , we further have
From the first part of this proof, . Meanwhile, since , by Lemma 2.5, we have . Therefore, by the choice of , we have
Similarly, note that and , by Lemma 2.5, we also have
This completes the proof. ∎
3 Proof of Theorem 1.5
Let be a positive integer and be an -dimensional vector space over . In the following, if there is no confusion, we shall omit the field size in the Gaussian binomial coefficient and use “dim” in short for “dimensional”.
Lemma 3.1.
[20] Let be a -dim subspace of . Then, for integers satisfying , the number of -dim subspaces of whose intersection with has dimension is
Proposition 3.2.
For integer , denote as a -dim subspace of . Let be the family of all -dim subspaces of containing . Then, we have and
(27) |
Proof.
The first statement is an immediate consequence of Lemma 3.1.
Now, we present the proof of Theorem 1.5.
Proof of Theorem 1.5.
First, we shall show that the number of popular -dim subspaces is not large.
Claim 3.1.
Let , then .
Proof.
Otherwise, assume that there is an such that . We have
Since and , based on the choice of and , we have
(28) |
This leads to , a contradiction. ∎
Claim 3.1 enables us to proceed further estimation on . Next, we shall prove that the most popular -dim subspace is contained in the majority members of .
Claim 3.2.
There exists a -dim subspace such that .
Proof.
Denote as the most popular -dim subspace appearing in the members of .
-
•
When .
Consider the new family of size and for all . According to (1), we have . Therefore, by the optimality of , .
Given a positive integer , for variable , define the function . One can easily verify that is a convex increasing function when . Thus by Jensen Inequality, we have
(29) |
Note that , (29) leads to . Moreover, we also have
Note that for and , we can further obtain
(30) |
According to the calculation of (3), the choice of leads to . Note that , this indicates that . Therefore, by (3), we have .
-
•
When .
Write , where is a -dim subspace of and is the -dim subspace spanned by some . Let be another -dim subspace of , where . Consider the new family with size , where consists of all -dim subspaces containing and consists of -dim subspaces containing . Based on the structure of , according to (1), we have
Again, by the optimality of , we have . Therefore, (29) leads to . Now, consider the function for satisfying . Clearly, is a decreasing function and when is fixed, the term is decreasing as increases. Therefore, we have
Since , we have . Denote . Then, we have . Note that for , and . Thus, we have
This leads to
Combined with the upper bound given by (3), by the choice of and , we also have . ∎
Finally, we show that when , is contained in all members of ; when , all -dim subspaces of that contains are in .
-
•
When .
Assume that there exists an such that . Since for each ,
(31) |
Take in the above equality and consider the first term in the RHS. Assume that and . When , knowing that , we have . Therefore, we can write for some -dim subspace in . Note that there are at most different choices of such . And for each fixed , there are at most different choices of satisfying . Therefore, the number of such s is at most . When , since , the number of such s is upper bounded by . Therefore, we have
As for the second term, we have that . Therefore, combined with Claim 3.2, this leads to
(32) |
From the assumption, we know that is not contained in any full -star. Therefore, we can replace with some containing . Denote the resulting new family as , we have
where the second equality follows from . By (31) and Claim 3.2, we have . Therefore, based on (3) and the calculations in (3), we have
This contradicts the fact that . Thus, all must contain .
-
•
When .
Assume that there exists a with . Since and , clearly, there exists some such that . Take in (31), since the estimation in (3) is irrelevant to the choice of . Thus, with similar procedures, we can also obtain . On the other hand, by (31), we also have . Again, we can replace with and denote the resulting new family as . With similar arguments as those for the case , this procedure increases the value of strictly, a contradiction. Therefore, all -dim subspaces of containing are in .
This completes the proof of Theorem 1.5. ∎
4 Proof of Theorem 1.6
For any integer , there exist unique and such that . Denote as the subfamily of consisting of pairwise disjoint -cosets and pairwise disjoint -cosets from another -coset disjoint from the former -cosets.
Assume that
(33) |
where and . Note that for every ,
where . Hence, when , we have
(34) |
When , similarly, we have
(35) |
For both cases, if we denote , then we have
(36) |
To proceed the proof of Theorem 1.6, we need some additional notations and a stability result by Ellis, Filmus and Friedgut [12] (see Theorem 1 in [12]). Assume each permutation in is distributed uniformly. Then, for a function , the expected value of is defined by . The inner product of two functions is defined as , this induces the norm . Given , denote as the nearest integer to .
Theorem 4.1.
[12] There exist positive constants and such that the following holds. Let be a subfamily of with for some . Let be the characteristic function of and let be the orthogonal projection of onto . If for some , then
where is the characteristic function of a union of cosets of .
Proof of Theorem 1.6.
For the convenience of our proof, for , we denote . Set and , where and are the positive constants from Theorem 4.1. Let be the characteristic vector of . Write , where is the projection of onto the eigenspace and is the projection of onto the eigenspace . By the orthogonality of the eigenspaces, we have
(37) |
Moreover, since is Boolean and , we also have
(38) |
By the definition of , we have
(39) |
where is a matrix with entry under a certain ordering of all permutations in . According to the definition of , we can write , where is the matrix with entries
From a simple observation, we know that , where is the matrix with all entries and is the adjacency matrix of , i.e., the adjacency matrix of the Cayley graph on with generating set . Therefore, by (39), we have
(40) |
Since and are eigenspaces for all , , therefore,
According to Lemma 2.13, and . Therefore, we have
(41) |
On the other hand, write for some . By (4) and (4), we have
where . Note that , which indicates that
(42) |
To obtain an upper bound on , we need the following claim.
Claim 1. for some absolute constant .
Proof.
Denote . First, note that lies in and the eigenvalues corresponding to are . Thus, we have
(43) |
where is the orthogonal projection of (or ) onto .
Based on estimations about s for from Lemma 2.14, we have
(44) |
where is an absolute constant. This leads to
∎
Now, with the help of Claim 1 and (42), we have
From the definition, and . Thus, we have
Since , we have
By Theorem 4.1, there exists , a union of -cosets of such that
This leads to .
When , we have and . Since for this case, we need another estimation of . Similar to (4), we have
(45) |
Therefore, combined with (4), (4) leads to
(46) |
By Claim 1, we have . Thus, . As shown by Ellis et. al [14] (see Theorem 7 and Theorem 8 in [14]), this indicates that is the union of -cosets of . Since , these -cosets must be pairwise disjoint.
This completes the proof. ∎
Remark 4.2.
As an immediate consequence of Theorem 1.6, when , the optimal family with maximal total intersection number is “almost” the union of disjoint -cosets. However, due to the restrictions of parameters in Theorem 4.1, the structural characterization given by Theorem 1.6 becomes weaker as each value of and grows.
5 Upper bounds on maximal total intersection numbers for families from different schemes
In this section, we will show several upper bounds on maximal total intersection numbers for families of vector spaces and permutations using linear programming method for corresponding association schemes.
5.1 Grassmann scheme
In this subsection, we take as the Grassmann scheme, which can be regarded as a -analogue of the Johnson scheme (for explicit definition of Johnson scheme, see [20]).
For , denote as the set of all subspaces in with constant dimension and as the corresponding distance relation set, where . is called .
Theorem 5.1.
[10] Given , the eigenvalues and the dual eigenvalues of the Grassmann scheme are given by
(47) | |||
(48) |
where the and the are defined as follows:
(49) | ||||
(50) |
Now, consider a family with size . According to the definition of in (8), we have
This leads to
(51) |
Then, recall the definition of from (1), we have
(52) |
Based on the relationship between inner distribution s and dual distribution s, we have the following theorem.
Theorem 5.2.
Given a prime power and positive integers with , . Let with and be the dual distribution of . Then, we have
(53) | ||||
(54) |
Proof.
Proof of Theorem 1.7.
From Lemma 2.2, we know that for . This leads to . Thus, combined with , we have
This proves inequality .
Next, we shall use a linear programming method to give a lower bound of . From Lemma 2.1, we know that for ,
(55) |
Meanwhile, by Lemma 2.3, we also have and . Thus, this leads to
(56) |
Combining with , we further have
for . To obtain a lower bound on under the restrictions of the above inequality together with () from Lemma 2.2, we now consider the following LP problem:
(I) Choose real variables so as to
subject to
Note that when , by and , we have
Moveover, since , this also leads to , for . Therefore, by taking , we can obtain the optimal solution .
When , by (54), for with , we have:
(57) |
Consider the dual problem of (I), which is given as follows (see [27, Section 4 of Chapter 17]).
(II) Choose real variables so as to
subject to
We claim that , is a feasible solution to the above problem (II). To show this, we only need to prove that
(58) |
for . From and , we know that . Thereofore, and follows from the fact that is decreasing on when . With this feasible solution, we have
Therefore, it follows from that
This completes the proof of . ∎
As an immediate consequence of Theorem 1.7 and Proposition 3.2, we have the following corollaries showing that bounds in Theorem 1.7 are tight for some special cases.
Corollary 5.3.
Given a prime power , a positive integer with , for with , we have
(59) |
Proof.
Corollary 5.4.
Given a prime power , a positive integer with , for with , we have
(60) |
Proof.
Similarly, by , we have
Now, take as the family of all -dim subspaces containing some fixed -dim subspace. Clearly, . By Proposition 3.2, we have
Hence, follows from . ∎
5.2 The conjugacy scheme of symmetric group
Given a positive integer , we take as the symmetric group . Denote as the conjugacy classes of and the relations are defined as follows:
is called of .
For each element of , one can write
as a product of disjoint cycles with . This -tuple is called the cycle-shape of . Then, the conjugacy classes of are precisely
Clearly, each conjugacy class corresponds to a cycle-shape of respectively. In particular, corresponds to the cycle-shape . According to [20, Chapter 11.12], eigenvalues and dual eigenvalues of the conjugacy scheme of are given by
(61) |
where for , is the identity element in and denote irreducible characters of . Especially, denotes the trivial character, which maps all the elements of into .
Given with size , consider the inner distribution of with respect to . According to the definition of , can be rewritten as
Thus, one can easily obtain
(62) |
Given a cycle-shape , define . From the new expression of above, we have
(63) |
Now, according to the relationship between inner distribution s and dual distribution s, we have the following theorem.
Theorem 5.5.
Given positive integers and with . Let with and be the dual distribution of . Then, we have
(64) | ||||
(65) |
Proof.
Remark 5.6.
Actually, similar to the proof of Theorem 1.7, we can also use the linear programming approach to bound . For interested readers, the corresponding LP problem is formulated as follows:
(I) Choose real variables so as to
subject to
Note that when , the optimal solution is given by taking . When , we turn to the following the dual problem of (I).
(II) Choose real variables so as to
subject to
As an immediate consequence of Theorem 1.8, we have the following corollary.
Corollary 5.7.
Given a positive integer , let with , we have
(66) |
6 Concluding remarks
In this paper, we consider a new type of intersection problems which can be viewed as inverse problems of Erdős-Ko-Rado type theorems for vector spaces and permutations. This type of problems concerns extremal structures of the families of subspaces or permutations with maximal total intersection numbers. Through different methods, we obtain structural characterizations of the optimal family of subspaces and the optimal family of permutations satisfying . To some extent, these results determine the unique structure of the optimal families for certain values of and characterize the relation between maximizing and being intersecting, which partially answers Question 1.3. Moreover, using linear programming methods, we have also shown several upper bounds on . These bounds may provide a reference for the study of structures of optimal families.
However, our results have the following limits:
-
•
Take , Theorem 1.5 shows that for large enough and not too close to , the optimal family with maximal total intersection number is either contained in a full -star or containing a full -star. When , the quantitative shifting arguments in the proof of Theorem 1.5 no longer work. So, can we obtain similar structural results for families with size larger than ? Note that the intersection problem of vector spaces often requires tools from linear algebra or exterior algebra, maybe ideas from these areas can help us to tackle this problem.
-
•
For families of permutations, we consider the case for . Nevertheless, for (), nothing is known yet. It is worth noting that, in [13], the authors provide a stability result for families of permutations with size similar to Theorem 4.1. Thus, it is natural to wonder if we can extend the result of Theorem 1.6 to families with size using this stability result. Sadly, this requires more information about spectra of , which is beyond our capability.
Moreover, when becomes relatively large, the result of Theorem 1.6 seems to be trivial. Thus, for this case, more specific structural characterizations for families of permutations are also worth studying.
-
•
Due to the choice of feasible solutions of corresponding LP problems, our upper bounds on are no longer tight for families of subspaces with size or families of permutations with size , for . Therefore, one can try to find other more proper feasible solutions to improve these upper bounds.
Acknowledgements
The authors express their gratitude to the two anonymous reviewers for their detailed and constructive comments which are very helpful to the improvement of the presentation of this paper, especially for providing a simpler proof of Proposition 2.12 using the method of generating functions. And the authors also express their gratitude to the associate editor for his excellent editorial job.
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