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On the EKR-module Property

Cai Heng Li SUSTech International Center for Mathematics
Department of Mathematics
Southern University of Science and Technology
Shenzhen, Guangdong 518055
P. R. China
[email protected]
 and  Venkata Raghu Tej Pantangi Department of Mathematics
University of Lethbridge
Lethbridge, Alberta T1K3M4
Canada
[email protected]
Abstract.

In the recent years, the generalization of the Erdős-Ko-Rado (EKR) theorem to permutation groups has been of much interest. A transitive group is said to satisfy the EKR-module property if the characteristic vector of every maximum intersecting set is a linear combination of the characteristic vectors of cosets of stabilizers of points. This generalization of the well-know permutation group version of the Erdős-Ko-Rado (EKR) theorem, was introduced by K. Meagher in [23]. In this article, we present several infinite families of permutation groups satisfying the EKR-module property, which shows that permutation groups satisfying this property are quite diverse.

This work was partially supported by NSFC grant 11931005 to the first author. The second author is a PIMS CRG Post Doctoral Fellow.

1. Introduction

The Erdős-Ko-Rado (EKR) theorem [12] is a classical result in extremal set theory. This celebrated result considers collections of pairwise intersecting kk-subsets of an nn-set. The result states that if n2kn\geq 2k, for any collection 𝔖\mathfrak{S} of pairwise intersecting kk-subsets, the cardinality |𝔖|(n1k1)|\mathfrak{S}|\leq{n-1\choose k-1}. Moreover in the case n>2kn>2k, if |𝔖|=(n1k1)|\mathfrak{S}|={n-1\choose k-1}, then 𝔖\mathfrak{S} is a collection of kk-subsets containing a common point. (When n=2kn=2k, the collection of kk-subsets that avoid a fixed point, is also a collection of (n1k1){n-1\choose k-1} pairwise intersecting subsets.) From a graph-theoretic point of view, this is the characterization of maximum independent sets in Kneser graphs.

There are many interesting generalizations of this result to other classes of objects with respect to certain form of intersection. One such generalization given by Frankl and Wilson [14] considers collections of pairwise non-trivially intersecting kk-subspaces of a finite nn-dimensional vector space, which corresponds to independent sets in qq-Kneser graphs. The book [17] is an excellent survey, including many generalizations of the EKR theorem.

In this article, we are concerned with EKR-type results for permutation groups. The first result of this kind was obtained by Deza and Frankl [13], who investigated families of pairwise intersecting permutations. Two permutations σ,τSn\sigma,\tau\in S_{n} are said to intersect if the permutation στ1\sigma\tau^{-1} fixes a point. A set of permutations is called an intersecting set if στ1\sigma\tau^{-1} fixes a point for any two members σ\sigma and τ\tau of the set. Clearly the stabilizer in SnS_{n} of a point or its coset is a canonically occurring family of pairwise intersecting permutations, of size (n1)!(n-1)!. In [13], it was shown that if 𝒮\mathcal{S} is a family of pairwise intersecting permutations, then |𝒮|(n1)!|\mathcal{S}|\leq(n-1)!. In the same paper, it was conjectured that if the equality |𝒮|=(n1)!|\mathcal{S}|=(n-1)! is met, then 𝒮\mathcal{S} has to be a coset of a point stabilizer. This conjecture was proved by Cameron and Ku (see [8]). An independent proof was given by Larose and Malvenuto (see [20]). Later, Godsil and Meagher (see [15]) gave a different proof. A natural next step is to ask similar questions about general transitive permutation groups.

Let GG be a finite group acting transitively on a set Ω\Omega. An intersecting subset of GG with respect to this action is a subset 𝒮G\mathcal{S}\subset G in which any two elements intersect. Obviously, a point stabilizer GαG_{\alpha}, its left cosets gGαgG_{\alpha}, and right cosets GαgG_{\alpha}g are intersecting sets, which we call canonical intersecting sets. An intersecting set of maximum possible size is called a maximum intersecting set. Noting that the size of a canonical intersecting set is |Gα|=|G|/|Ω||G_{\alpha}|=|G|/|\Omega|, we see that the size of a maximum intersecting set is at least |G|/|Ω||G|/|\Omega|. It is now natural to ask the following:

(A) Is the size of every intersecting set in GG bounded above by the size of a point stabilizer?

(B) Is every maximum intersecting set canonical?

As mentioned above, the results of Deza-Frankl, Cameron-Ku, and Larose-Malvenuto show that the answer to both these questions in positive for the natural action of a symmetric group. However, not all permutation groups satisfy similar properties, although there are many interesting examples that do. We now formally define the conditions mentioned in the above questions.

Definition 1.1.

A transitive group GG on Ω\Omega is said to satisfy the EKR property if every intersecting set has size at most |G|/|Ω||G|/|\Omega|, and further said to satisfy the strict-EKR property if every maximum intersecting set is canonical.

When the action is apparent, these properties will be attributed to the group. We have already seen that the natural action of SnS_{n} satisfies both the EKR and the strict-EKR property. EKR properties of many specific permutation groups have been investigated (see [1, 3, 22, 25, 26, 27]). In particular, it was shown that all 22-transitive group actions satisfy the EKR property, see [25, Theorem 1.1], but not every 2-transitive group satisfies the strict-EKR property; for instance, with respect to the 22-transitive action of PGL(n,q)\mathrm{PGL}(n,q) (with n3n\geq 3) on the 1-spaces, the stabilizer of a hyperplane is also a maximum intersecting set. However, it is shown in [25] that 22-transitive groups satisfy another interesting property called the EKR-module property, defined below.

For a transitive group GG on Ω\Omega and a subset SGS\subset G, let

𝐯S=sSsG,\mathbf{v}_{S}=\sum\limits_{s\in S}s\in\mathbb{C}G,

the characteristic vector of SS in the group algebra G\mathbb{C}G. For α,βΩ\alpha,\beta\in\Omega and gGg\in G with gα=βg\cdot\alpha=\beta, we write

𝐯α,β=tGtα=βt=xGαgx=gxGαx=𝐯gGα,\mathbf{v}_{\alpha,\beta}=\sum_{\begin{subarray}{c}t\in G\\ t\cdot\alpha=\beta\end{subarray}}t=\sum\limits_{x\in G_{\alpha}}{gx}=g\sum\limits_{x\in G_{\alpha}}x=\mathbf{v}_{gG_{\alpha}},

the characteristic vector of the canonical intersecting set gGαgG_{\alpha}, which we call a canonical vector for convenience. The next definition was first introduced in [23].

Definition 1.2.

A finite transitive group GG on a set Ω\Omega is said to satisfy the EKR-module property if the characteristic vector of each maximum intersecting set of GG on Ω\Omega is a linear combination of canonical vectors, that is, the vectors in {𝐯α,βα,βΩ}\{\mathbf{v}_{\alpha,\beta}\mid\alpha,\beta\in\Omega\}.

The name is from the so called “module method” described in [2]. We remark that

  1. (a)

    a group action satisfying the strict-EKR property also satisfies the EKR-module property, but the converse statement is not true;

  2. (b)

    and there exist group actions that satisfy the EKR-module property but not the EKR property, see [24, Theorem 5.2], and the following Example 1.3;

Example 1.3.

Consider the action of A4A_{4} on the set Ω\Omega of cosets of a subgroup H2H\cong\mathbb{Z}_{2}. We observe that the Sylow 2-subgroup NN of A4A_{4} is an intersecting set. As 4=|N|>|A4/|Ω|=24=|N|>|A_{4}/|\Omega|=2, this action does not satisfy the EKR property. Consider an intersecting set 𝒮\mathcal{S}. Then given t𝒮t\in\mathcal{S}, the set 𝒮t1\mathcal{S}t^{-1} is an intersecting set containing the identity. By the definition of an intersecting set, we have 𝒮t1gA4gHg1=N\mathcal{S}t^{-1}\subset\bigcup\limits_{g\in A_{4}}gHg^{-1}=N. This shows that any maximum intersecting set must be coset of NN. Any coset of NN is a union of two disjoint cosets of HH, and thus this action satisfies the EKR-module property.

We will now construct an example of a group action that satisfies the EKR property, but not the EKR-module property. Prior to doing so, we mention a well-known result. Consider a transitive action of a group GG on a set Ω\Omega. A subset RGR\subset G is said to be a regular subset, if for any (α,β)Ω2(\alpha,\ \beta)\in\Omega^{2}, there is a unique rRr\in R such that rα=βr\cdot\alpha=\beta. Corollary 2.2 of [3] states that permutation groups which contain a regular subset, satisfy the EKR property.

For a group GG and a subgroup HGH\leqslant G, let

[G:H]={xHxG},[G:H]=\{xH\mid x\in G\},

the set of left cosets of HH in GG. Then GG acts transitively on [G:H][G:H] by left multiplication. Moreover, each transitive action of a group is equivalent to such a coset action.

Example 1.4.

Consider G=S5G=S_{5} (isomorphic to PGL(2,5)\mathrm{PGL}(2,5)) and a subgroup HGH\leq G isomorphic to the dihedral group of size 12. We consider the action of GG on Ω=[G:H]\Omega=[G:H]. We first show that this action satisfies the EKR property, by demonstrating the existence of a regular subset. We consider the cyclic subgroup C:=(1,2,3,4,5)C:=\left\langle(1,2,3,4,5)\right\rangle and the 44-cycle t:=(2,3,5,4)t:=(2,3,5,4). We claim that R:=CtCR:=C\cup tC is a regular set. As |R|=|Ω||R|=|\Omega|, this claim will follow by showing that for r,sRr,s\in R with rsr\neq s, we have rgHsgHrgH\neq sgH, for all gGg\in G. This is equivalent to showing that g1r1sgHg^{-1}r^{-1}sg\notin H, for all gGg\in G. It is easy to verify that for any two distinct r,sRr,s\in R , r1sr^{-1}s is either a 44-cycle or a 55-cycle, and thus g1r1sgHg^{-1}r^{-1}sg\notin H. We can now conclude that RR is a regular subset. Therefore, by [3, Corollary 2.2], GG satisfies the EKR property. Thus the size of any intersecting set is bounded above by |H|=12|H|=12.

Now we consider subgroup KA4K\cong A_{4} of GG. It is easy to check that KK1=KgHg1KK^{-1}=K\subset\cup gHg^{-1} and thus KK is a maximum intersecting set. In this case, canonical intersecting sets are cosets of a conjugate of HH. Every canonical intersecting set contains exactly 33 even permutations. Also every permutation in KK is even. Now consider the sign character λ\lambda. For every canonical intersecting set 𝒮\mathcal{S}, we have λ(𝐯S)=0\lambda(\mathbf{v}_{S})=0. On the other hand, we have λ(𝐯K)0\lambda(\mathbf{v}_{K})\neq 0. From this, we see that 𝐯K\mathbf{v}_{K} cannot be a linear combination of the characteristic vectors of the canonical intersecting sets. Therefore this action does not satisfy the EKR-module property.

We will now describe the main results of our paper.

1.1. Main Results

Our first result is a characterization of the EKR-module property of a group action, in terms of the characters of the group in question. Given a group GG, a complex character χ\chi of GG, and a subset AGA\subseteq G, by χ(𝐯A)\chi(\mathbf{v}_{A}), we denote the sum aAχ(a)\sum\limits_{a\in A}\chi(a). We now describe our first result, a characterization of the EKR-module property in terms of character sums.

Theorem 1.5.

Let GG be a finite group, H<GH<G, and Ω=[G:H]\Omega=[G:H]. Let C={χIrr(G):χ(𝐯H)=0}C=\{\chi\in{\rm Irr}(G):\ \chi(\mathbf{v}_{H})=0\}, and 𝔖\mathfrak{S} be the collection of maximum intersecting sets in GG. Then GG on Ω\Omega satisfies the EKR-module property if and only if χ(𝐯𝒮)=0\chi(\mathbf{v}_{\mathcal{S}})=0 for any 𝒮𝔖\mathcal{S}\in\mathfrak{S} and any χC\chi\in C.

We note that Example 1.4 can be viewed as an application of the above result. In Example 1.4, the sign character λ\lambda is a character such that λ(𝐯H)=0\lambda(\mathbf{v}_{H})=0. However, for the maximum intersecting set KK, we have λ(𝐯K)0\lambda(\mathbf{v}_{K})\neq 0. Thus by Theorem 1.5, the action in Example 1.4 does not satisfy the EKR-module property.

Given an action of GG on Ω\Omega, the derangement graph ΓG,Ω\Gamma_{G,\ \Omega} is the graph whose vertex set is GG, and vertices g,hGg,h\in G are adjacent if and only if gh1gh^{-1} does not fix any point in Ω\Omega. Then a set SGS\subseteq G is an intersecting set if and only if it is an independent set in ΓG,Ω\Gamma_{G,\ \Omega}. Therefore, the study of intersecting sets could benefit from the various results from spectral graph theory about independent sets. Many authors (for instance, see [26], [27]) have studied the EKR and strict-EKR properties of various group actions from this point of view. Theorem 3.4 is a characterization of the EKR-module property of a group action in terms of spectra of weighted adjacency matrices of the corresponding derangement graph.

It is well known (see [3, Corollary 2.2]) that permutation groups with regular subsets satisfy the EKR property. However, as observed in example 1.4, such groups do not necessarily satisfy the EKR-module property. The following theorem shows that every permutation group with a regular normal subgroup satisfies the EKR-module property.

Theorem 1.6.

Transitive groups actions with a regular normal subgroup satisfy the EKR-module property.

A few classes of permutation groups with a regular normal subgroup are Frobenius groups, affine groups, primitive groups of type HS, HC, and TW (for a description of these, we refer the reader to [28]).

After showing that all 22-transitive groups satisfy the EKR-module property, the authors of [25] mention that the next natural step is to consider rank 33 permutation groups. As a first step, we consider this problem for the class of primitive rank 33 permutation groups. The next theorem reduces the problem to almost simple groups. (Recall that a finite group is called almost simple if it has a unique minimal normal subgroup, which is non-abelian and simple.)

Theorem 1.7.

Let GG be a primitive permutation group on Ω\Omega of rank 33. Then either GG has the EKR-module property, or GG is an almost simple group.

We would like to mention that when nn is sufficiently large, the rank 33 action of SnS_{n} on 22-subsets of [n][n], satisfies the strict-EKR property, and thereby the EKR-module property. This was proved in [11]. Example 1.4 shows that this fails when n=5n=5.

In [6], a finite group GG is defined to satisfy the weak EKR property, if every transitive action of GG satisfies the EKR property. A finite group GG is defined to satisfy the strong EKR property, if every transitive action of GG satisfies the strict-EKR property. Theorem 11 of [6] shows that nilpotent group satisfies the weak EKR property. This result was extended to supersolvable groups in [21]. It is easy to check that every abelian group satisfies the strong EKR property. Theorem 33 of [6] states that a finite non-abelian nilpotent group satisfies the strong EKR property if and only if it is a direct product of a 22-group and an abelian group of odd order. We now make the following analogous definition.

Definition 1.8.

A finite group GG is said to satisfy the EKR-module property if every transitive action of GG satisfies the EKR-module property.

As mentioned before, groups with the strict-EKR property have the EKR-module property. It is then natural to ask whether the converse statement is true or not. It is shown in [6, Theorem 3] that there are infinitely many nilpotent groups of nilpotency class 22 that do not satisfy the strict-EKR property. The next result then answers the question in negative.

Theorem 1.9.

Nilpotent groups of nilpotency class 22 satisfy the EKR-module property.

It is shown in [6, Theorem 2] that a group GG satisfying the EKR property for every transitive action is necessarily solvable. However, it is shown in Lemma 6.2 that there do exist non-solvable groups which have the EKR-module property.

An analogue of the EKR-module property has been observed in other generalizations of the EKR theorem. Consider a graph XX and a prescribed set of “canonically” occurring cliques. We say that the graph satisfies the EKR-module property, if the characteristic vector of any maximum clique is a linear combination of the characteristic vectors of the canonical cliques. In the context of permutation groups satisfying the EKR-module property, the complement of the corresponding derangement graph satisfies the EKR-module property. In Chapter 5 of [17], there are a few examples of strongly regular graphs satisfying the EKR-module property. In [4], the authors show that Peisert-type graphs satisfy the EKR-module property. Let qq be an odd prime power. Let FF and EE be finite fields of order q2q^{2} and qq respectively. A Peisert-type graph of type (m,q)(m,q) is a Cayley graph of the form Cay(F,S)Cay(F,S), where the “connection” set SS is a union of mm distinct cosets of the multiplicative group E×E^{\times} in F×F^{\times}. It is clear that any set of the form sE+bsE+b, with sSs\in S and bFb\in F, is a clique. We deem these to be the canonical cliques. In [4], the authors show that characteristic vector of any maximum clique in a Peisert-type graph, is a linear combination of the characteristic vectors of canonical cliques. In § 7, we give a shorter independent proof of the same.

2. EKR-module property and character theory.

In this section, we gather some tools which are used to prove our main results, and then prove Theorem 1.5.

Let K=G(Ω)K=G_{(\Omega)} be the kernel of GG on Ω\Omega. Here Ω=[G:H]\Omega=[G:H] for some HGH\leq G. The following simple lemma shows that we may assume without loss of generality that KK is trivial.

Lemma 2.1.

Let π:GG/K\pi:G\to G/K be the natural quotient map. Then a subset 𝒮G\mathcal{S}\subset G is a maximum intersecting set of GG if and only if π(𝒮)\pi(\mathcal{S}) is a maximum intersecting set of G/KG/K.

Proof.

Given an intersecting set AGA\subset G, we note that AK:={ak:aA&kK}AK:=\{ak\ :\ a\in A\ \&\ k\in K\} is also an intersecting set. So any maximum intersecting set in GG must be a union of KK-cosets. Let s1,s2,srGs_{1},s_{2},\ldots s_{r}\in G be such that 𝒮=siK\mathcal{S}=\bigcup s_{i}K is a maximum intersecting subset of GG. We see that π(𝒮)={siK: 1ir}\pi(\mathcal{S})=\{s_{i}K\ :\ 1\leq i\leq r\} is an intersecting set in G/KG/K.

Now consider a maximum intersecting set 𝒯={tiK: 1is}\mathcal{T}=\{t_{i}K\ :\ 1\leq i\leq s\} of G/KG/K. It is clear that π1(𝒯)=tiKG\pi^{-1}(\mathcal{T})=\bigcup t_{i}K\subset G is an intersecting set. So we have |𝒯||K|=|π1(𝒯)||𝒮||\mathcal{T}||K|=|\pi^{-1}(\mathcal{T})|\leq|\mathcal{S}|, and |𝒮|/|K|=|π(𝒮)||𝒯||\mathcal{S}|/|K|=|\pi(\mathcal{S})|\leq|\mathcal{T}|. This shows that π(𝒮)\pi(\mathcal{S}) (respectively π1(𝒯)\pi^{-1}(\mathcal{T})) is a maximum intersecting set of G/KG/K (respectively GG). ∎

As an immediate consequence, we get the following corollary.

Corollary 2.2.

Let GG be a finite transitive group on Ω\Omega with kernel K=G(Ω)K=G_{(\Omega)}, and let π:GG/K\pi:G\to G/K be the natural quotient map. Then the following hold:

  1. (i)

    GG satisfies the EKR (respectively strict-EKR) property if and only if G/KG/K satisfies the EKR (respectively strict-EKR);

  2. (ii)

    GG satisfies the EKR-module property if and only if G/KG/K satisfies the EKR-module property.

Proof.

Set Q:=G/KQ:=G/K. We note that for all ωΩ\omega\in\Omega and gGg\in G, we have π(g)Qω=π(gGω)\pi(g)Q_{\omega}=\pi(gG_{\omega}) and gGω=π1(π(g)Qω)gG_{\omega}=\pi^{-1}(\pi(g)Q_{\omega}). The proof now follows from Lemma 2.1. ∎

For any gGg\in G, we denote by HgH^{g} the subgroup gHg1gHg^{-1}. Given α=aHΩ\alpha=aH\in\Omega, we have Gα=HaG_{\alpha}=H^{a}. Thus, with respect to this action, we see that the set {aHb:a,bG}\{aH^{b}\ :\ a,b\in G\} is the set of canonical intersecting sets. By G(Ω)\mathfrak{I}_{G}(\Omega), we denote the subspace of G\mathbb{C}G spanned by the set {𝐯aHb:a,bG}\{\mathbf{v}_{aH^{b}}\ :\ a,b\in G\} of the characteristic vectors of the canonical intersecting sets. By the definition of the EKR-module property, the action of GG on Ω\Omega satisfies the EKR-module property if and only if 𝐯𝒮G(Ω)\mathbf{v}_{\mathcal{S}}\in\mathfrak{I}_{G}(\Omega) for every maximum intersecting set 𝒮\mathcal{S} in GG.

We observe that for every a,b,g,hGa,\ b,\ g,\ h\in G, we have g𝐯aHbh=𝐯gahHh1bg\mathbf{v}_{aH^{b}}h=\mathbf{v}_{gahH^{h^{-1}b}}. Therefore, G(Ω)\mathfrak{I}_{G}(\Omega) is a two-sided ideal of the group algebra G\mathbb{C}G. The two-sided ideals of complex group algebras are characterized by the Artin-Wedderburn decomposition.

We will now recall some basic facts on group algebra, proofs of which can be found in any standard text on representation theory such as [19]. Let Irr(G){\rm Irr}(G) be the set of irreducible complex characters of GG. For χIrr(G)\chi\in{\rm Irr}(G), we define Mχ:=i=1χ(1)WiM_{\chi}:=\sum\limits_{i=1}^{\chi(1)}W_{i}, where {W1,W2,Wχ(1)}\{W_{1},W_{2},\ldots W_{\chi(1)}\} are the right submodules of G\mathbb{C}G that afford the character χ\chi. By Maschke’s theorem, we have the decomposition

G=χIrr(G)Mχ.\mathbb{C}G=\bigoplus\limits_{\chi\in{\rm Irr}(G)}M_{\chi}.

For each χIrr(G)\chi\in{\rm Irr}(G), we have dim(Mχ)=χ(1)2\mathrm{dim}_{\mathbb{C}}(M_{\chi})=\chi(1)^{2} and that MχM_{\chi} is a minimal two-sided ideal containing the primitive central idempotent

eχ=χ(1)|G|gGχ(g1)g.e_{\chi}=\dfrac{\chi(1)}{|G|}\sum\limits_{g\in G}\chi(g^{-1})g.

By orthogonality relations among characters, we have

(1) eχeψ={1,  if χ=ψ,0,  otherwise.e_{\chi}e_{\psi}=\begin{cases}1\ \text{,\ \ if $\chi=\psi$,}\\ 0\ \text{,\ \ otherwise.}\end{cases}

Using the fact that G\mathbb{C}G is a semi-simple algebra, we now get the following description of two-sided ideals of G\mathbb{C}G

Lemma 2.3.

Given a two-sided ideal 𝔍\mathfrak{J} of G\mathbb{C}G, there is a subset Y𝔍Irr(G)Y_{\mathfrak{J}}\subseteq{\rm Irr}(G) such that 𝔍=χY𝔍eχ\mathfrak{J}=\bigoplus\limits_{\chi\in Y_{\mathfrak{J}}}\left\langle e_{\chi}\right\rangle.

Our investigation of the EKR-module property of the action of GG on Ω\Omega, will benefit from the description of G(Ω)\mathfrak{I}_{G}(\Omega) as a direct sum of simple ideals of G\mathbb{C}G. We recall that G(Ω)\mathfrak{I}_{G}(\Omega), is the subspace of G\mathbb{C}G spanned by the set {𝐯aHb:a,bG}\{\mathbf{v}_{aH^{b}}\ :\ a,b\in G\}. We also showed that it is a two-sided ideal.

Lemma 2.4.

Let GG be a finite group, H<GH<G a subgroup, and Ω=[G:H]\Omega=[G:H] be the space of left cosets of HH. Let YH={χIrr(G):χ(𝐯H)0}Y_{H}=\{\chi\in{\rm Irr}(G)\ :\ \chi(\mathbf{v}_{H})\neq 0\}. Then, the linear span G(Ω)\mathfrak{I}_{G}(\Omega) of {𝐯aHg:a,gG}\{\mathbf{v}_{aH^{g}}\ :\ a,g\in G\} decomposes as the sum χYHeχ\bigoplus\limits_{\chi\in Y_{H}}\left\langle e_{\chi}\right\rangle of simple ideals of G\mathbb{C}G.

Proof.

For any subset SGS\subset G and ψIrr(G)\psi\in{\rm Irr}(G), we have

|G|ψ(1)eψ𝐯S\displaystyle\frac{|G|}{\psi(1)}e_{\psi}\mathbf{v}_{S} =|G|ψ(1)sSeψs\displaystyle=\frac{|G|}{\psi(1)}\sum\limits_{s\in S}e_{\psi}s
=sSgGψ(sg1)g\displaystyle=\sum\limits_{s\in S}\sum\limits_{g\in G}\psi(sg^{-1})g
=gGgsSψ(sg1)\displaystyle=\sum\limits_{g\in G}g\sum\limits_{s\in S}\psi(sg^{-1})
=gGψ(𝐯Sg1)g.\displaystyle=\sum\limits_{g\in G}\psi(\mathbf{v}_{Sg^{-1}})g.

Therefore for any χYH\chi\in Y_{H}, we have 0eχ𝐯HeχG(Ω)G(Ω)0\neq e_{\chi}\mathbf{v}_{H}\in\left\langle e_{\chi}\right\rangle\cap\mathfrak{I}_{G}(\Omega)\subset\mathfrak{I}_{G}(\Omega). As eχ\left\langle e_{\chi}\right\rangle is a minimal ideal, we conclude that eχG(Ω)\left\langle e_{\chi}\right\rangle\subset\mathfrak{I}_{G}(\Omega).

Now consider θIrr(G)YH\theta\in{\rm Irr}(G)\setminus Y_{H}. In this case, we have θ(𝐯Hg)=θ(𝐯H)=0\theta(\mathbf{v}_{H^{g}})=\theta(\mathbf{v}_{H})=0. Let Θ:GGLθ(1)()\Theta:G\to\mathrm{GL}_{\theta(1)}(\mathbb{C}) be a unitary representation affording θ\theta as its character. Given a subset SGS\subset G, we define MS:=sSΘ(s)M_{S}:=\sum\limits_{s\in S}\Theta(s). As Θ\Theta is a unitary representation, we have MS1=MSM_{S^{-1}}=M_{S}^{\dagger}, that is, MS1M_{S^{-1}} is the conjugate transpose of MSM_{S}. Now given a,gHa,g\in H, we have

MHga1MaHg=x,yHgΘ(x)Θ(y)=x,yHgΘ(xy)=|H|MHg.M_{H^{g}a^{-1}}M_{aH^{g}}=\sum\limits_{x,y\in H^{g}}\Theta(x)\Theta(y)=\sum\limits_{x,y\in H^{g}}\Theta(xy)=|H|M_{H^{g}}.

As θ(𝐯Hg)=0\theta(\mathbf{v}_{H^{g}})=0, we have 0=Tr(MaHg)=Tr(MHga1MaHg)0=\mathrm{Tr}(M_{aH^{g}})=\mathrm{Tr}(M_{H^{g}a^{-1}}M_{aH^{g}}). Since MHga1=MaHgM_{H^{g}a^{-1}}=M_{aH^{g}}^{\dagger}, this can only happen when MaHg=0M_{aH^{g}}=0. Therefore, θ(𝐯aHg)=0\theta(\mathbf{v}_{aH^{g}})=0, and we conclude that eθ𝐯aHg=0e_{\theta}\mathbf{v}_{aH^{g}}=0. Thus eθe_{\theta} annihilates G(Ω)\mathfrak{I}_{G}(\Omega). As eθ2=10e_{\theta}^{2}=1\neq 0, eθe_{\theta} cannot be an element of the ideal G(Ω)\mathfrak{I}_{G}(\Omega). Now the result follows by applying Lemma 2.3 and equation (1). ∎

As an immediate application, we obtain a significantly shorter proof of Lemma 4.1 and Lemma 4.2 of [2]. The content of these two results is presented as the following corollary. We will use the following technical result in the proof of Theorem 1.7. We would like to mention that it was a key result that led to the “Module Method” described in [2].

Corollary 2.5.

Let GSym(Ω)G\leq\mathrm{Sym}(\Omega) be a 22-transitive permutation group with πIrr(G)\pi\in{\rm Irr}(G) such that 1+π1+\pi is the corresponding permutation character. Given α,βΩ\alpha,\beta\in\Omega, set 𝐯α,β:={gG:gα=β}g\mathbf{v}_{\alpha,\beta}:=\sum\limits_{\{g\in G\ :\ g\cdot\alpha=\beta\}}g and 𝐯G:=gGg\mathbf{v}_{G}:=\sum\limits_{g\in G}g. Then

  1. (1)

    G(Ω)=e1+eπ\mathfrak{I}_{G}(\Omega)=\left\langle e_{1}\right\rangle+\left\langle e_{\pi}\right\rangle is a vector space of dimension 1+(|Ω|1)21+(|\Omega|-1)^{2};

  2. (2)

    and the set

    Bω:={𝐯G}{𝐯α,β:(α,β)(Ω{ω})2},B_{\omega}:=\{\mathbf{v}_{G}\}\cup\ \{\mathbf{v}_{\alpha,\ \beta}\ :\ (\alpha,\beta)\in\left(\Omega\setminus\{\omega\}\right)^{2}\},

    is a basis set of G(Ω)\mathfrak{I}_{G}(\Omega) for any ωΩ\omega\in\Omega.

Proof.

Part (1) follows immediately from Lemma 2.4.

We observe that for αΩ\alpha\in\Omega, we have 𝐯α,ω=𝐯Gβω𝐯α,β\mathbf{v}_{\alpha,\omega}=\mathbf{v}_{G}-\sum\limits_{\beta\neq\omega}\mathbf{v}_{\alpha,\ \beta}. Therefore, every vector of the form 𝐯γ,δ\mathbf{v}_{\gamma,\ \delta} is in the linear span of the elements of BωB_{\omega}, and thus BωB_{\omega} spans G(Ω)\mathfrak{I}_{G}(\Omega). Linear independence follows as G(Ω)\mathfrak{I}_{G}(\Omega) is a |Bω||B_{\omega}|-dimensional subspace. ∎

We are now ready to prove Theorem 1.5.

Proof of Theorem 1.5: Given χC={χIrr(G):χ(𝐯H)=0}\chi\in C=\{\chi\in{\rm Irr}(G)\ :\ \chi(\mathbf{v}_{H})=0\}, by Lemma 2.4 and (1), we have eχx=0e_{\chi}x=0, for all xG(Ω)x\in\mathfrak{I}_{G}(\Omega). By the definition of the EKR-module property, for any maximum intersecting set 𝒮\mathcal{S}, we have 𝐯𝒮G(Ω)\mathbf{v}_{\mathcal{S}}\in\mathfrak{I}_{G}(\Omega). The equality χ(𝐯𝒮)=0\chi(\mathbf{v}_{\mathcal{S}})=0 follows from eχ𝐯𝒮=0e_{\chi}\mathbf{v}_{\mathcal{S}}=0.

We now prove the other direction. Suppose that for any χC\chi\in C and any maximum intersecting set 𝒮\mathcal{S}, we have χ(𝐯𝒮)=0\chi(\mathbf{v}_{\mathcal{S}})=0. Fix a maximum intersecting set 𝒮\mathcal{S}. If 𝒮\mathcal{S} is a maximum intersecting set, then so is 𝒮g1\mathcal{S}g^{-1}, for all gGg\in G. Therefore, χ(𝐯𝒮g1)=0\chi(\mathbf{v}_{\mathcal{S}g^{-1}})=0, for all χC\chi\in C and all gGg\in G. Thus |G|χ(1)eχ𝐯𝒮=gGχ(𝐯𝒮g1)g=0\frac{|G|}{\chi(1)}e_{\chi}\mathbf{v}_{\mathcal{S}}=\sum\limits_{g\in G}\chi(\mathbf{v}_{\mathcal{S}g^{-1}})g=0, for all χC\chi\in C. Further, by the equality ψIrr(G)eψ=1\sum\limits_{\psi\in{\rm Irr}(G)}e_{\psi}=1, we have

𝐯𝒮\displaystyle\mathbf{v}_{\mathcal{S}} =(ψIrr(G)eψ)×𝐯𝒮=(ψCeψ)×𝐯𝒮.\displaystyle=\left(\sum\limits_{\psi\in{\rm Irr}(G)}e_{\psi}\right)\times\mathbf{v}_{\mathcal{S}}=\left(\sum\limits_{\psi\notin C}e_{\psi}\right)\times\mathbf{v}_{\mathcal{S}}.

By Lemma 2.4, ψCeψG(Ω)\sum\limits_{\psi\notin C}e_{\psi}\in\mathfrak{I}_{G}(\Omega). Since G(Ω)\mathfrak{I}_{G}(\Omega) is an ideal, we have 𝐯𝒮G(Ω)\mathbf{v}_{\mathcal{S}}\in\mathfrak{I}_{G}(\Omega). Thus the EKR-module property is satisfied. ∎

We note that if 𝒮\mathcal{S} is a maximum intersecting set, then for any t𝒮t\in\mathcal{S}, the set 𝒮t1\mathcal{S}t^{-1} is a maximum intersecting set that contains the identity element. So every maximum intersecting set is a “translate” of an intersecting set containing the identity. The following corollary shows that, as far as the EKR-module property is concerned, we can restrict ourselves to maximum intersecting sets containing the identity.

Corollary 2.6.

Let GG be a finite group with the identity 1G1_{G}, H<GH<G, and Ω=[G:H]\Omega=[G:H]. Let C={χIrr(G):χ(𝐯H)=0}C=\{\chi\in{\rm Irr}(G):\ \chi(\mathbf{v}_{H})=0\}, and

𝔖0={𝒮0:𝒮0is a maximum intersecting set with 1G𝒮0}.\mathfrak{S}_{0}=\{\mathcal{S}_{0}\ :\ \mathcal{S}_{0}\ \text{is a maximum intersecting set with $1_{G}\in\mathcal{S}_{0}$}\}.

Then GG on Ω\Omega satisfies the EKR-module property if and only if χ(𝐯𝒮0)=0\chi(\mathbf{v}_{\mathcal{S}_{0}})=0 for any 𝒮0𝔖0\mathcal{S}_{0}\in\mathfrak{S}_{0} and any χC\chi\in C.

Proof.

At first, we assume that χ(𝐯𝒮0)=0\chi(\mathbf{v}_{\mathcal{S}_{0}})=0, for all 𝒮0𝔖\mathcal{S}_{0}\in\mathfrak{S} and χC\chi\in C. Fix a χC\chi\in C and a maximum intersecting set 𝒮\mathcal{S} . Let P:GGLn()P:G\to\mathrm{GL}_{n}(\mathbb{C}) be a unitary representation affording χ\chi as its character. Given a set XGX\subset G, define MX:=xXP(x)M_{X}:=\sum\limits_{x\in X}P(x). We observe that M𝒮M𝒮1=t𝒮M𝒮t1M_{\mathcal{S}}M_{\mathcal{S}^{-1}}=\sum\limits_{t\in\mathcal{S}}M_{\mathcal{S}t^{-1}}. Then Tr(M𝒮t1)=χ(𝐯𝒮t1)Tr(M_{\mathcal{S}t^{-1}})=\chi(\mathbf{v}_{\mathcal{S}t^{-1}}). As PP is a unitary representation, M𝒮1M_{\mathcal{S}^{-1}} is the conjugate transpose of M𝒮M_{\mathcal{S}}, and thus

(2) Tr(M𝒮M𝒮)=t𝒮χ(𝐯𝒮t1).Tr\left(M_{\mathcal{S}}M_{\mathcal{S}}^{\dagger}\right)=\sum\limits_{t\in\mathcal{S}}\chi(\mathbf{v}_{\mathcal{S}t^{-1}}).

For any t𝒮t\in\mathcal{S}, the set 𝒮t1\mathcal{S}t^{-1} is a maximum intersecting set containing the identity 1G1_{G}. Therefore, we have χ(𝐯𝒮t1)=χ(𝐯H)=0\chi(\mathbf{v}_{\mathcal{S}t^{-1}})=\chi(\mathbf{v}_{H})=0, for all t𝒮t\in\mathcal{S}. Thus by (2), we have Tr(M𝒮M𝒮)=0Tr(M_{\mathcal{S}}M_{\mathcal{S}}^{\dagger})=0. As M𝒮M_{\mathcal{S}}^{\dagger} is the conjugate transpose of M𝒮M_{\mathcal{S}}, the matrix M𝒮M𝒮M_{\mathcal{S}}M_{\mathcal{S}}^{\dagger} is a diagonal matrix whose entries are the norms of rows of M𝒮M_{\mathcal{S}}. Thus, Tr(M𝒮M𝒮)=0Tr(M_{\mathcal{S}}M_{\mathcal{S}}^{\dagger})=0 implies that M𝒮=0M_{\mathcal{S}}=0. We can now conclude that χ(𝐯𝒮)=Tr(M𝒮)=0\chi(\mathbf{v}_{\mathcal{S}})=Tr(M_{\mathcal{S}})=0. By Theorem 1.5, the action of GG on Ω\Omega satisfies the EKR-module property.

The other direction follows directly from Theorem 1.5. ∎

3. EKR-module property and Spectral graph theory.

Results from spectral graph theory have proved useful in characterizing maximum intersecting sets in some permutation groups (for instance, see [25], [26], [27]). Let GG be a group acting on Ω=[G:H]\Omega=[G:H], for some HGH\leq G. An element gGg\in G is called a derangement if it does not fix any point in Ω\Omega. Let Der(G,Ω)Der(G,\Omega) denote the set of derangements in GG. It is easy to see that Der(G,Ω)=GgGgHg1Der(G,\Omega)=G\setminus\bigcup\limits_{g\in G}gHg^{-1}. By ΓG,Ω\Gamma_{G,\Omega}, we denote the Cayley graph on GG, with Der(G,Ω)Der(G,\Omega) as the “connection set”. We now observe that intersecting sets in GG are the same as independent sets/co-cliques in ΓG,Ω\Gamma_{G,\Omega}. This observation enables us to use some popular spectral bounds on sizes of independent sets in regular graphs. Before describing these, we recall some standard definitions.

For graph XX on nn vertices, a real symmetric matrix MM whose rows and columns are indexed by the vertex set of XX, is said to be compatible with XX, if Mu,v=0M_{u,v}=0 whenever uu is not adjacent to vv in XX. Clearly, the adjacency matrix of XX is compatible with XX. Given a subset SS of the vertex set, by 𝐯S\mathbf{v}_{S}, we denote the characteristic vector of SS. We now state the following famous result which is referred to as either the Delsarte-Hoffman bound or the ratio bound.

Lemma 3.1.

([17, Theorem 2.4.2]) Let MM be a real symmetric matrix with constant row sum dd, which is compatible with a graph XX on nn vertices. If the least eigenvalue of MM is τ\tau, then for any independent set SS in XX,

|S|n(τ)dτ,|S|\leq\frac{n(-\tau)}{d-\tau},

and if equality holds, then

𝐯S|S|n𝐯X\mathbf{v}_{S}-\frac{|S|}{n}\mathbf{v}_{X}

is a τ\tau-eigenvector for MM.

The application of the above lemma on clever choices of ΓG,Ω\Gamma_{G,\Omega}-compatible matrices, proved useful in characterization of maximum intersecting sets for many permutation groups (for instance see [26] and [27]). We will now describe these in detail.

Definition 3.2.

Let GG be a group acting transitively on a set Ω\Omega. A (G,Ω)(G,\Omega)-compatible class function is a real valued class function f:Gf:G\to\mathbb{R} such that: (i) f(g)=0f(g)=0 for all gDer(G,Ω)g\notin Der(G,\Omega); and (ii) f(d)=f(d1)f(d)=f(d^{-1}) for all dDer(G,Ω)d\in Der(G,\Omega).

Let ff be a (G,Ω)(G,\Omega)-compatible class function . Consider the matrix MfM^{f} indexed by G×GG\times G, that satisfies Mg,hf=f(gh1)M^{f}_{g,h}=f(gh^{-1}) for all (g,h)G×G(g,h)\in G\times G. Clearly MfM^{f} is a ΓG,Ω\Gamma_{G,\Omega}-compatible matrix. We now describe the spectra of such matrices. The description of spectra of matrices of the form MfM^{f} is a special case of well-know results by Babai ([5]) and Diaconis-Shahshahani ([10]). The following lemma, which is a special case of Lemma 5 of [10], describes the spectra of matrices of the form MfM^{f}.

Lemma 3.3.

(Babai, Diaconis-Shahshahani) Let GG be a permutation group on Ω\Omega, with Der(G,Ω)GDer(G,\Omega)\subset G being the set of derangements. Let f:Gf:G\to\mathbb{R} be (G,Ω)(G,\Omega)-compatible class function. Define MfG×GM^{f}\in\mathbb{C}^{G\times G} to be the matrix satisfying Mg,hf=f(g1h)M^{f}_{g,\ h}=f(g^{-1}h), for all g,hGg,h\in G. Then MfM^{f} is a ΓG,Ω=Cay(G,Der(G,Ω))\Gamma_{G,\Omega}=Cay(G,Der(G,\Omega))-compatible matrix with spectrum Spec(Mf):={λχ,f:χIrr(G)}\mathrm{Spec}(M^{f}):=\{\lambda_{\chi,f}\ :\ \chi\in{\rm Irr}(G)\}, where

λχ,f=1χ(1)gGf(g)χ(g).\lambda_{\chi,f}=\frac{1}{\chi(1)}\sum\limits_{g\in G}f(g)\chi(g).

Given νSpec(Mf)\nu\in\mathrm{Spec}(M^{f}), the ν\nu-eigenspace in G\mathbb{C}{G} is the two-sided ideal

{χ:χIrr(G)andλχ,f=ν}eχ.\sum\limits_{\{\chi\ :\ \chi\in{\rm Irr}(G)\ \text{and}\ \lambda_{\chi,f}=\nu\}}\left\langle e_{\chi}\right\rangle.

We are now ready to give a sufficient condition for EKR-module property in terms of spectra of ΓG,Ω\Gamma_{G,\Omega}-compatible matrices. Let f:Gf:G\to\mathbb{R} be a (G,Ω)(G,\Omega)-compatible class function. Then the row sum of MfM^{f} is rf:=gGf(g)r_{f}:=\sum\limits_{g\in G}f(g). Let τ\tau be the least eigenvalue of MfM^{f}. By Lemma 3.1, for any intersecting set SS, we have

|S||G|(τ)rfτ.|S|\leqslant\frac{|G|(-\tau)}{r_{f}-\tau}.

Let us assume that equality holds for some intersecting set 𝒮\mathcal{S}. By Lemmas 3.1 and 3.3, if 𝒮\mathcal{S} is an maximum intersecting set, then 𝐯𝒮\mathbf{v}_{\mathcal{S}} is in the 22-sided ideal

e1+{χ:χIrr(G)andλχ,f=τ}eχ.\left\langle e_{1}\right\rangle+\sum\limits_{\{\chi\ :\ \chi\in{\rm Irr}(G)\ \text{and}\ \lambda_{\chi,f}=\tau\}}\left\langle e_{\chi}\right\rangle.

Now by application of Lemma 2.4, we obtain the following sufficient condition for EKR-module property.

Theorem 3.4.

Let GG be a group acting on the set Ω\Omega of left cosets of a subgroup HH. Assume that there is an intersecting set SS and a (G,Ω)(G,\Omega)-compatible class function f:Gf:G\to\mathbb{R} such that |S|=|G|(τ)dτ|S|=\dfrac{|G|(-\tau)}{d-\tau}, where d=gGf(g)d=\sum\limits_{g\in G}f(g) and τ\tau is the least eigenvalue of MfM^{f}. Then

(a) |S||S| is the size of a maximum intersecting set in GG; and

(b) the action of GG on Ω\Omega satisfies the EKR-module property if

{χIrr(G):1χ(1)gGf(g)χ(g)=τ}{χIrr(G):χ(𝐯H)0}.\left\{\chi\in{\rm Irr}(G)\ :\ \frac{1}{\chi(1)}\sum\limits_{g\in G}f(g)\chi(g)=\tau\right\}\subseteq\left\{\chi\in{\rm Irr}(G)\ :\ \chi(\mathbf{v}_{H})\neq 0\right\}.

At this point, we remark that the proofs of EKR ([27]) and EKR-module properties ([25]) of 22-transitive groups, involved finding a class function that satisfies the conditions of Theorem 3.4.

4. Proof of Theorem 1.6

In this section, we prove Theorem 1.6. By Corollary 2.2, we can restrict ourselves to permutation groups that contain a regular normal subgroup. Let AA be a finite group and HAut(A)H\leqslant Aut(A). We consider the permutation action of G:=AHG:=A\rtimes H on AA, defined by (a,σ)b=aσ(b)(a,\sigma)\cdot b=a\sigma(b), for all a,bAa,b\in A and σH\sigma\in H. It is well-known that any permutation group with a regular normal subgroup, is of the form GSym(A)G\leqslant\mathrm{Sym}(A). By [1, Corollary 2.2], permutation groups which contain a regular subgroup, satisfy the EKR property. Thus the action of GG on AA satisfies the EKR property.

Before starting the proof, we prove an elementary result that we will use later. Every element of GG is of the form (a,σ)(a,\sigma), where aAa\in A and σH\sigma\in H. Note that (a,σ)(b,π)=(aσ(b),σπ)(a,\sigma)(b,\pi)=(a\sigma(b),\sigma\pi). We need the following well-known result for technical reasons.

Lemma 4.1.

Consider g=(a,σ)Gg=(a,\sigma)\in G, with aAa\in A and σH\sigma\in H. If gg fixes a point then

(i) gg is conjugate to σ\sigma via an element of AA; and

(ii) σ\sigma is the unique AA-conjugate of gg in HH.

Proof.

For convenience, given xAx\in A, we identify (x, 1H)G(x,\ 1_{H})\in G with xAx\in A. Given any bAb\in A, we have (a,σ)b=aσ(b)(a,\sigma)\cdot b=a\sigma(b). So (a,σ)(a,\sigma) fixes bb if and only if a=bσ(b1)a=b\sigma(b^{-1}).

Now for cAc\in A, we have c1(bσ(b1),σ)(c)=(c1bσ(bc1),σ)c^{-1}(b\sigma(b^{-1}),\sigma)(c)=(c^{-1}b\sigma(bc^{-1}),\sigma). Thus(c1bσ(bc1),σ)H(c^{-1}b\sigma(bc^{-1}),\sigma)\in H if and only if c1bσ(bc1)=1Gc^{-1}b\sigma(bc^{-1})=1_{G}. Then the proof follows from setting c=bc=b. ∎

We will now prove the theorem by using Corollary 2.6. Let 𝒮0\mathcal{S}_{0} be any maximum intersecting set with 1G𝒮01_{G}\in\mathcal{S}_{0}. As 𝒮0\mathcal{S}_{0} is an intersecting set, for all s𝒮0s\in\mathcal{S}_{0}, the element s=s1G1s=s1^{-1}_{G} fixes some point. Thus by Lemma 4.1, given s𝒮0s\in\mathcal{S}_{0}, there exists a unique element σsH\sigma_{s}\in H and an element asAa_{s}\in A, such that as1sas=σsHa_{s}^{-1}sa_{s}=\sigma_{s}\in H. We now claim that {σs:s𝒮0}=H\{\sigma_{s}\ :\ s\in\mathcal{S}_{0}\}=H. Since GG satisfies the EKR property, we have |𝒮0|=|H||\mathcal{S}_{0}|=|H|. Therefore, {σs:s𝒮0}=H\{\sigma_{s}:\ s\in\mathcal{S}_{0}\}=H is equivalent to injectivity of the map sσss\mapsto\sigma_{s}.

Suppose that for some s,r𝒮0s,r\in\mathcal{S}_{0}, we have σs=σr\sigma_{s}=\sigma_{r}. Then, we have

sr1=asσsas1arσr1ar1=asσs(as1ar)σs1ar1A.sr^{-1}=a_{s}\sigma_{s}a_{s}^{-1}a_{r}\sigma_{r}^{-1}a_{r}^{-1}=a_{s}\sigma_{s}(a_{s}^{-1}a_{r})\sigma_{s}^{-1}a_{r}^{-1}\in A.

As 𝒮0\mathcal{S}_{0} is an intersecting set, sr1Asr^{-1}\in A fixes a point. Since AA acts regularly, we must have sr1=1sr^{-1}=1. Thus sσss\mapsto\sigma_{s} is injective, and {σs:s𝒮0}=H\{\sigma_{s}:\ s\in\mathcal{S}_{0}\}=H. As s𝒮0s\in\mathcal{S}_{0} is conjugate to σs\sigma_{s}, for any ψIrr(G)\psi\in{\rm Irr}(G), we have ψ(𝐯𝒮0)=s𝒮0ψ(σs)=ψ(𝐯H)\psi(\mathbf{v}_{\mathcal{S}_{0}})=\sum\limits_{s\in\mathcal{S}_{0}}\psi(\sigma_{s})=\psi(\mathbf{v}_{H}). Therefore, if χ{ψ:ψIrr(G)&ψ(𝐯H)=0}\chi\in\{\psi:\ \psi\in{\rm Irr}(G)\ \&\ \psi(\mathbf{v}_{H})=0\} and 𝒮0\mathcal{S}_{0} is a maximum intersecting set containing 1G1_{G}, we have χ(𝐯𝒮0)=0\chi(\mathbf{v}_{\mathcal{S}_{0}})=0. Now, by Corollary 2.6, Theorem 1.6 is proved. ∎

5. EKR-module property for primitive rank 3 group actions.

In this section, we study the EKR-module property for primitive permutation groups of rank 3, and prove Theorem 1.7. Let GG be a primitive permutation group on Ω\Omega of rank 3. To prove Theorem 1.7, we may assume that GG is not an almost simple group. Then either

  1. (a)

    GG is affine, so that GG has a regular normal subgroup, or

  2. (b)

    GG is in product action, and GTS2G\leqslant T\wr S_{2} on Ω2\Omega^{2}, where TSym(Ω)T\leqslant\mathrm{Sym}(\Omega) is 22-transitive.

If GG is affine, then GG indeed has the EKR-module property by Theorem 1.6. We thus assume further that GG is in product action in the rest of this section.

Let TSym(Ω)T\leqslant\mathrm{Sym}(\Omega) be a 22-transitive group, and let H=Tω<TH=T_{\omega}<T, where ωΩ\omega\in\Omega. Let G=TS2G=T\wr S_{2}, and M=HS2M=H\wr S_{2}. Then GG naturally acts on Ω2\Omega^{2}, with M=G(ω,ω)M=G_{(\omega,\omega)}. Obviously,

{(ω,ω)}\{(\omega,\ \omega)\}, (Ω{ω})×(Ω{ω})\left(\Omega\setminus\{\omega\}\right)\times\left(\Omega\setminus\{\omega\}\right), and ((Ω{ω})×{ω})({ω}×(Ω{ω}))\left(\left(\Omega\setminus\{\omega\}\right)\times\{\omega\}\right)\bigcup\left(\{\omega\}\times\left(\Omega\setminus\{\omega\}\right)\right)

are the orbits of M=G(ω,ω)M=G_{(\omega,\omega)} on Ω2\Omega^{2}. Thus GG is of rank 33.

In view of Corollary 2.6, it is beneficial to obtain descriptions of the set Irr(G){\rm Irr}(G) of irreducible characters of GG, and of the maximum intersecting sets in GG containing the identity. As one would expect, the 22-transitive action TT on Ω\Omega plays a major role. Before going any further, we establish some notation. In G=TS2=(T×T)S2G=T\wr S_{2}=(T\times T)\rtimes S_{2}, by π\pi, we denote the unique 22-cycle in S2S_{2}. Elements of G(T×T)G\setminus(T\times T) are of the form (s,r)π(s,r)\pi, where s,rTs,r\in T. By (s,r)π(s,r)\pi, we denote the product of elements (s,r)(s,r) and π\pi of GG.

We start by describing Irr(G){\rm Irr}(G). The subgroup N:=T×TN:=T\times T of GG is a normal subgroup of index 22. By Clifford theory ([19, 6.19]), restriction of any irreducible character νIrr(G)\nu\in{\rm Irr}(G) to NN is either an irreducible GG-invariant character of NN, or the sum of two GG-conjugate irreducible characters of NN. From well-known results on characters of direct products, we have

Irr(N)={χ×λ:χ,λIrr(T)}.{\rm Irr}(N)=\{\chi\times\lambda\ :\chi,\lambda\in\ {\rm Irr}(T)\}.

Let χ,λ\chi,\lambda be two distinct irreducible characters of TT, then the inertia subgroup in GG of χ×λ\chi\times\lambda is NN, and therefore σχ,λ:=IndNG(χ×λ)\sigma_{\chi,\lambda}:=Ind^{G}_{N}(\chi\times\lambda) is an irreducible character of GG, with ResNG(σχ,λ)=χ×λ+λ×χRes^{G}_{N}(\sigma_{\chi,\lambda})=\chi\times\lambda+\lambda\times\chi. Now consider an irreducible character of NN, of the form χ×χ\chi\times\chi. Let P:TGL(V)P:T\to\mathrm{GL}(V) be a representation affording χ\chi as its character. Then PP:NGL(VV)P\otimes P:N\to\mathrm{GL}(V\otimes V) is a representation of NN that affords χ×χ\chi\times\chi as its character. Let π\pi be the unique 22-cycle in S2S_{2}. Define Ψ:GGL(VV)\Psi:G\to\mathrm{GL}(V\otimes V) to be the representation such that Ψ|N=PP\Psi\lvert_{N}=P\otimes P and Ψ(π)(vw)=wv\Psi(\pi)(v\otimes w)=w\otimes v for all v,wVv,w\in V. The character ρχ\rho_{\chi} afforded by Ψ\Psi is an irreducible character of GG that extends χ×χ\chi\times\chi. We also have ρχ((s,r)π))=χ(rs)\rho_{\chi}((s,r)\pi))=\chi(rs) for all r,sTr,s\in T. By a result of Gallagher ([19, 6.17]), there is exactly one other irreducible character of GG whose restriction to NN is χ×χ\chi\times\chi, namely βρχ\beta\rho_{\chi}, where β\beta is the unique non-trivial linear character with kernel NN. Therefore by Clifford theory any irreducible character is one of the characters defined above.

Lemma 5.1.

The set

{ρχ:χIrr(T)}{βρχ:χIrr(T)}{σχ,λ:χ,λIrr(T)&χλ}\{\rho_{\chi}\ :\ \chi\in{\rm Irr}(T)\}\cup\{\beta\rho_{\chi}\ :\ \chi\in{\rm Irr}(T)\}\cup\{\sigma_{\chi,\ \lambda}\ :\ \chi,\lambda\in{\rm Irr}(T)\ \&\ \chi\neq\lambda\}

is the complete set of irreducible characters of GG.

We now describe the permutation character for the action GG on Ω2\Omega^{2}. As TT is a 22-transitive group, there is ψIrr(T)\psi\in{\rm Irr}(T) be such that 1+ψ1+\psi is the permutation character for TT. Computation shows that Λ:=1+ρψ+σψ,1\Lambda:=1+\rho_{\psi}+\sigma_{\psi,1} is the permutation character for GG.

The next lemma follows from the proof of Lemma 3.5 of [18], which is essentially the same as Lemma 4.2 of [3].

Lemma 5.2.

Every maximum intersecting set for the action of T×TT\times T on Ω2\Omega^{2} is of the form S×RS\times R, where SS and RR are maximum intersecting sets with respect to the action of TT on Ω\Omega

We now give the following characterization of maximum intersecting sets in G=TS2G=T\wr S_{2}.

Lemma 5.3.

The action of GG on Ω2\Omega^{2} satisfies the EKR property. If 𝒮\mathcal{S} is a maximum intersecting set in GG that contains the identity, then there are maximum intersecting sets XX, WW, ZZ in TT such that:

  1. (i)

    𝒮=(W×Z)(X×X1)π\mathcal{S}=(W\times Z)\cup(X\times X^{-1})\pi, and

  2. (ii)

    WW and ZZ contain the identity of TT.

Proof.

As TT is a 22-transitive group, by the main results of [27] and [25], the action of TT on Ω\Omega satisfies both EKR and EKR-module properties. By Lemma 5.2, a maximum intersecting set for the action of N:=T×TN:=T\times T on Ω2\Omega^{2} is of the form S×RS\times R, where SS and RR are maximum intersecting sets in TT. Therefore, the action of NN on Ω2\Omega^{2} also satisfies the EKR property. The subgroup NN of GG is a transitive subgroup satisfying the EKR property, and so by Lemma 3.3 of [27], we see that the action of GG also satisfies the EKR property.

We consider a maximum intersecting set 𝒮\mathcal{S} with respect to the action of GG on Ω2\Omega^{2}. We further assume that 𝒮\mathcal{S} contains the identity element. With this assumption, every element of 𝒮\mathcal{S} must fix a point in Ω2\Omega^{2}. Now 𝒮N\mathcal{S}\cap N and (𝒮Nπ)π1(\mathcal{S}\cap N\pi)\pi^{-1} are intersecting sets with respect to the action of NN on Ω2\Omega^{2}. We note that H×HNH\times H\leq N is a point stabilizer for this action. Since the action of NN on Ω2\Omega^{2} satisfies the EKR property, we have |H×H||(𝒮N)||H\times H|\geq|(\mathcal{S}\cap N)| and |H×H||(𝒮Nπ)π1||H\times H|\geq|(\mathcal{S}\cap N\pi)\pi^{-1}|. Now since the action of GG on Ω2\Omega^{2} satisfies the EKR property, MM is a point stabilizer, and 𝒮\mathcal{S} is a maximum intersecting set in GG, we have 2|H×H|=|M|=|𝒮|=|(𝒮Nπ)π1|+|(𝒮N)|2|H\times H|=|M|=|\mathcal{S}|=|(\mathcal{S}\cap N\pi)\pi^{-1}|+|(\mathcal{S}\cap N)|. Therefore, both 𝒮N\mathcal{S}\cap N and (𝒮Nπ)π1(\mathcal{S}\cap N\pi)\pi^{-1} are maximum intersecting sets in NN. Using Lemma 5.2, we see that there are maximum intersecting sets WW, ZZ, XX, YY in TT, such that (i) 𝒮N=W×Z\mathcal{S}\cap N=W\times Z; and (ii) (𝒮Nπ)=(X×Y)π(\mathcal{S}\cap N\pi)=(X\times Y)\pi. As 𝒮N\mathcal{S}\cap N contains the identity of NN, WW and ZZ must contain the identity of TT. We will now show that X1=YX^{-1}=Y.

Given xXx\in X and yYy\in Y, consider the element (x,y)π(𝒮Nπ)𝒮(x,y)\pi\in(\mathcal{S}\cap N\pi)\subset\mathcal{S}. As we assume that 𝒮\mathcal{S} contains the identity, (x,y)π(x,y)\pi must fix a point. That is to say, 0Λ((x,y)π)=1+ψ(xy)0\neq\Lambda((x,y)\pi)=1+\psi(xy), where Λ\Lambda and ψ\psi are as described prior to the statement of the lemma. As 1+ψ1+\psi is the permutation character for the action of TT on Ω\Omega, 1+ψ(xy)01+\psi(xy)\neq 0 if and only if xyTxy\in T fixes a point of Ω\Omega. Thus for for a given yYy\in Y, the set X{y1}X\cup\{y^{-1}\} is an intersecting set in TT. As XX is a maximum intersecting set in TT, we must have y1Xy^{-1}\in X. This shows that Y=X1Y=X^{-1}. ∎

We recall that Λ=1+ρψ+σψ,1\Lambda=1+\rho_{\psi}+\sigma_{\psi,1} is the permutation character for the action of GG on Ω2\Omega^{2}, where ψIrr(T)\psi\in{\rm Irr}(T) is such that 1+ψ1+\psi is the permutation character for the action of TT on Ω\Omega. By Corollary 2.6, EKR-module property of GG is equivalent to showing that ν(𝐯𝒮)=0\nu(\mathbf{v}_{\mathcal{S}})=0 for all maximum intersecting sets 𝒮\mathcal{S} that contain the identity and νIrr(G){1,σψ,1,ρψ}\nu\in{\rm Irr}(G)\setminus\{1,\sigma_{\psi,1},\ \rho_{\psi}\}. Let 𝒮0\mathcal{S}_{0} be a maximum intersecting set in GG such that 1G𝒮01_{G}\in\mathcal{S}_{0}. By Lemma 5.3, there are maximum intersecting sets X,W,ZX,W,Z in TT such that : ZZ and WW contain the identity of TT; and 𝒮0=W×Z(Z×Z1)π\mathcal{S}_{0}=W\times Z\cup\left(Z\times Z^{-1}\right)\pi. For any distinct pair χ,λIrr(T)\chi,\lambda\in{\rm Irr}(T), we can compute the following character sums:

  1. (I)

    ρχ(𝐯𝒮0)=χ(𝐯W)χ(𝐯Z)+r,sZχ(r1s)=χ(𝐯W)χ(𝐯Z)+rZχ(𝐯r1Z)\rho_{\chi}(\mathbf{v}_{\mathcal{S}_{0}})=\chi(\mathbf{v}_{W})\chi(\mathbf{v}_{Z})+\sum\limits_{r,s\in Z}\chi(r^{-1}s)=\chi(\mathbf{v}_{W})\chi(\mathbf{v}_{Z})+\sum\limits_{r\in Z}\chi(\mathbf{v}_{r^{-1}Z});

  2. (II)

    βρχ(𝐯𝒮0)=χ(𝐯W)χ(𝐯Z)r,sZχ(r1s)=χ(𝐯W)χ(𝐯Z)rZχ(𝐯r1Z)\beta\rho_{\chi}(\mathbf{v}_{\mathcal{S}_{0}})=\chi(\mathbf{v}_{W})\chi(\mathbf{v}_{Z})-\sum\limits_{r,s\in Z}\chi(r^{-1}s)=\chi(\mathbf{v}_{W})\chi(\mathbf{v}_{Z})-\sum\limits_{r\in Z}\chi(\mathbf{v}_{r^{-1}Z}); and

  3. (III)

    σχ,λ(𝐯𝒮0)=χ(𝐯W)λ(𝐯Z)+λ(𝐯W)χ(𝐯Z)\sigma_{\chi,\ \lambda}(\mathbf{v}_{\mathcal{S}_{0}})=\chi(\mathbf{v}_{W})\lambda(\mathbf{v}_{Z})+\lambda(\mathbf{v}_{W})\chi(\mathbf{v}_{Z}).

We need to compute χ(𝐯S)\chi(\mathbf{v}_{S}), for all χIrr(T)\chi\in{\rm Irr}(T) and all maximum intersecting sets SS in TT. To do so, we use the EKR and EKR-module properties of 22-transitive groups.

Lemma 5.4.

Let TSym(Ω)T\leq\mathrm{Sym}(\Omega) be a 22-transitive group with HGH\leq G being the point stabilizer. Let ψIrr(T)\psi\in{\rm Irr}(T) be such that 1+ψ1+\psi is the permutation character. If SS is an maximum intersecting set in TT, then

  1. (i)

    ψ(S)=|H|\psi(S)=|H|, when 1S1\in S;

  2. (ii)

    ψ(S)=|H|/ψ(1)\psi(S)=-|H|/\psi(1), provided 1S1\notin S; and

  3. (iii)

    ν(S)=0\nu(S)=0 for all irreducible characters ν{1,ψ}\nu\notin\ \{1,\ \psi\}.

Proof.

As TT is 2-transitive, it satisfies both the EKR and EKR-module properties. By Corollary 2.5, 𝐯𝒮\mathbf{v}_{\mathcal{S}} is in the ideal J=e1+eψJ=\left\langle e_{1}\right\rangle+\left\langle e_{\psi}\right\rangle. By the orthogonality relations among primitive central idempotents, we see that left multiplication by e1+eψe_{1}+e_{\psi} is a projection onto JJ. That is (e1+eψ)(𝐯𝒮)=𝐯𝒮(e_{1}+e_{\psi})(\mathbf{v}_{\mathcal{S}})=\mathbf{v}_{\mathcal{S}}. Writing both sides as a linear combination of the elements in the basis set {tT}\{t\in T\} of the group algebra T\mathbb{C}T, and equating the coefficients of the identity element on both sides, yields the first two formulae.

Part (iii) is a direct consequence of Corollary 2.6. ∎

Pick a maximum intersecting set 𝒮0\mathcal{S}_{0} in GG such that 1G𝒮01_{G}\in\mathcal{S}_{0}, and let νIrr(G){1,σψ,1,ρψ,βρψ}\nu\in{\rm Irr}(G)\setminus\{1,\ \sigma_{\psi,1},\ \rho_{\psi},\ \beta\rho_{\psi}\}. Now applying Lemma 5.4 (ii) and the character sum formulas (I) (II) and (III) given above yields that ν(𝐯𝒮0)=0\nu(\mathbf{v}_{\mathcal{S}_{0}})=0. As 1,σψ,1,ρψ1,\ \sigma_{\psi,1},\ \rho_{\psi} are the only irreducibles that contribute to the permutation character for the action of GG on Ω2\Omega^{2}, in view of Corollary 2.6, we need to show that βρψ(𝐯𝒮0)=0\beta\rho_{\psi}(\mathbf{v}_{\mathcal{S}_{0}})=0. This is indeed true by Lemma 5.4, and then Theorem 1.7 follows from an application of Corollary 2.6. ∎

6. Some groups satisfying the EKR-module property.

In this section, we study groups satisfying the EKR-module property. Recall (from Definition 1.8) that a finite group GG satisfies the EKR-module property if every transitive action of GG satisfies the EKR-module property. We first prove Theorem 1.9, and then prove the smallest non-abelian simple group A5A_{5} satisfies the EKR-module property.

6.1. Proof of Theorem 1.9.

In this subsection, we consider transitive actions of nilpotent groups of nilpotency class 22. By [6, Theorem 3], all transitive actions of nilpotent groups satisfy the EKR property. In the same paper, it was also shown that there are examples of class-22 nilpotent groups that do not satisfy the strict-EKR property. We will show that all transitive actions of class-22 nilpotent groups satisfy the EKR-module property. Our proof is a proof by contradiction.

Recall the following well-known result from character theory.

Lemma 6.1.

Let GG be a group, ψ\psi an irreducible complex character of GG, and zz an element of the centre of GG. Then for all gGg\in G, we have ψ(gz)=ψ(g)ψ(z)\psi(gz)=\psi(g)\psi(z).

Proof.

Let ρ:GGL(V)\rho:G\to\mathrm{GL}(V) be a representation affording ψ\psi as its character. As zz is in the centre, the map ρ(z):VV\rho(z):V\to V is a GG-module homomorphism. Thus, by Schur’s lemma, ρ(z)\rho(z) acts like a scalar matrix, and thus ψ(gz)=Tr(ρ(gz))=Tr(ρ(g))Tr(ρ(z))=ψ(g)ψ(z)\psi(gz)=Tr(\rho(gz))=Tr(\rho(g))Tr(\rho(z))=\psi(g)\psi(z). ∎

Assume that Theorem 1.9 is false. Let NN be a class-22 nilpotent group NN, and HNH\leqslant N such that the action of NN on Ω=[N:H]\Omega=[N:H] does not satisfy the EKR-module property. We may further assume that |N|+|Ω||N|+|\Omega| is as small as possible. By the minimality of (N,Ω)(N,\Omega) and by Corollary 2.2, the action of NN on Ω\Omega must be a permutation action. In other words, HH is core-free, that is, nNnHn1={1N}\bigcap\limits_{n\in N}nHn^{-1}=\{1_{N}\}. As the action of NN on Ω\Omega does not satisfy the EKR-module property, by Theorem 1.5, there is a character χ{ψ:ψIrr(N)&ψ(𝐯H)=0}\chi\in\{\psi:\ \psi\in{\rm Irr}(N)\ \&\ \psi(\mathbf{v}_{H})=0\} and a maximum intersecting set 𝒮\mathcal{S} such that χ(𝐯𝒮)0\chi(\mathbf{v}_{\mathcal{S}})\neq 0. We fix one such pair χ,𝒮\chi,\mathcal{S}.

As NN is nilpotent, it has a non-trivial centre, which we denote by ZZ. Given a character ψ\psi of NN, we denote its kernel, {nN:ψ(n)=ψ(1)}\{n\in N:\ \psi(n)=\psi(1)\}, by ker(ψ)ker(\psi). As every non-trivial normal subgroup of a nilpotent group intersects non-trivially with the centre, we either have ker(χ)Z{1N}ker(\chi)\cap Z\neq\{1_{N}\}, or that χ\chi is a faithful character.

We first assume that χ\chi is faithful. As NN is a class-22 nilpotent group, we have Z[N,N]Z\supset[N,N]. Since NN is non-abelian, given yNZy\in N\setminus Z, we can pick xNx\in N be such that z:=xyx1y11Nz:=xyx^{-1}y^{-1}\neq 1_{N}. As χ\chi is faithful, we have χ(z)1\chi(z)\neq 1. Since xyx1=zyxyx^{-1}=zy, we have χ(y)=χ(xyx1)=χ(yz)\chi(y)=\chi(xyx^{-1})=\chi(yz). As zz is a central element, by Lemma 6.1, we have χ(y)=χ(y)χ(z)\chi(y)=\chi(y)\chi(z). As χ(z)1\chi(z)\neq 1, we must have χ(y)=0\chi(y)=0 for all yNZy\in N\setminus Z. Recall that HH is core-free, and thus HZ={1N}H\cap Z=\{1_{N}\}. We can now conclude that χ(𝐯H)=χ(1)0\chi(\mathbf{v}_{H})=\chi(1)\neq 0. This contradicts our initial condition that χ(𝐯H)=0\chi(\mathbf{v}_{H})=0, and therefore χ\chi cannot be faithful.

Now we are left with the case when χ\chi is not faithful. By ker(χ)ker(\chi), we denote the kernel of a corresponding representation. We set Zχ=ker(χ)ZZ_{\chi}=ker(\chi)\cap Z. We note that ZχZ_{\chi} is a non-trivial normal subgroup of NN. As HH is a core-free subgroup, we have ZχnHn1={1N}Z_{\chi}\cap nHn^{-1}=\{1_{N}\}, for all nNn\in N. Thus the action of ZχZ_{\chi} on Ω\Omega is semi-regular. If the action of ZχZ_{\chi} is regular, then it is a regular normal subgroup, and thus by Theorem 1.6, the action of NN on Ω\Omega must satisfy the EKR-module property. As this contradicts our assumption, the action of ZχZ_{\chi} on Ω\Omega must be semi-regular and intransitive. As ZχNZ_{\chi}\lhd N, the set Ω~\tilde{\Omega} of ZχZ_{\chi} orbits on Ω\Omega, is a block system for the action of NN on Ω\Omega. Since ZχZ_{\chi} acts intransitively, we have |Ω~||Ω||\tilde{\Omega}|\lneqq|\Omega|, and thus |N|+|Ω~||N|+|Ω||N|+|\tilde{\Omega}|\lneqq|N|+|\Omega|. We now consider the transitive action of NN on Ω~\tilde{\Omega}. The elements of HZχHZ_{\chi} fix the ZχZ_{\chi}-orbit containing the element HΩH\in\Omega. Observing that |N|/|HZχ|=|N|/|H||Zχ|=|Ω|/|Zχ|=|Ω~||N|/|HZ_{\chi}|=|N|/|H||Z_{\chi}|=|\Omega|/|Z_{\chi}|=|\tilde{\Omega}|, we can conclude that HZχHZ_{\chi} is a stabilizer for the action of NN on Ω~\tilde{\Omega}. As 𝒮\mathcal{S} is an intersecting set with respect to the action of NN on Ω\Omega, the set 𝒮Zχ\mathcal{S}Z_{\chi} is an intersecting set with respect to the action of NN on Ω~\tilde{\Omega}. Since ZχZ_{\chi} is a central semi-regular subgroup in NSym(Ω)N\leq\mathrm{Sym}(\Omega) and 𝒮\mathcal{S} is an intersecting set, we can conclude that |𝒮Zχ|=|𝒮||Zχ||\mathcal{S}Z_{\chi}|=|\mathcal{S}||Z_{\chi}|. As we mentioned above, transitive actions of nilpotent groups satisfy the EKR property, and thus since 𝒮\mathcal{S} is a maximum intersecting set with respect to the action of NN on Ω\Omega, we have |𝒮|=|H||\mathcal{S}|=|H|, and therefore |𝒮Zχ|=|HZχ||\mathcal{S}Z_{\chi}|=|HZ_{\chi}|. We can now see that 𝒮Zχ\mathcal{S}Z_{\chi} is a maximum intersecting set with respect to the action of NN on Ω~\tilde{\Omega}. As Zχker(χ)Z_{\chi}\leq ker(\chi) is a central subgroup, by using Lemma 6.1, we have χ(𝐯𝒮Zχ)=|Zχ|×χ(𝐯𝒮)\chi(\mathbf{v}_{\mathcal{S}Z_{\chi}})=|Z_{\chi}|\times\chi(\mathbf{v}_{\mathcal{S}}) and χ(𝐯HZχ)=|Zχ|×χ(𝐯H)\chi(\mathbf{v}_{HZ_{\chi}})=|Z_{\chi}|\times\chi(\mathbf{v}_{H}). By our choice of χ\chi and 𝒮\mathcal{S}, χ(𝐯H)=0\chi(\mathbf{v}_{H})=0 and χ(𝐯𝒮)0\chi(\mathbf{v}_{\mathcal{S}})\neq 0. Therefore 𝒮Zχ\mathcal{S}Z_{\chi} is a maximum intersecting set with respect to the action of NN on Ω~\tilde{\Omega} and χ\chi is a character in {ψIrr(G):ψ(𝐯HZχ)=0}\{\psi\in{\rm Irr}(G)\ :\ \psi(\mathbf{v}_{HZ_{\chi}})=0\}, such that χ(𝐯𝒮Zχ)0\chi(\mathbf{v}_{\mathcal{S}Z_{\chi}})\neq 0. So by Theorem 1.5, the action of NN on Ω~\tilde{\Omega} does not satisfy the EKR-module property. Now since |N|+|Ω~||N|+|Ω||N|+|\tilde{\Omega}|\lneqq|N|+|\Omega|, this conclusion contradicts the minimality of (N,Ω)(N,\ \Omega). Therefore our assumption that χ\chi is not faithful must be false.

Both cases return contradictions, and hence our initial assumption that Theorem 1.9 fails, must be false. This concludes the proof. ∎

Theorem 1.9 and Theorem 3 of [6] establish the existence of infinitely many groups that satisfy the EKR and EKR-module property, but not the strict-EKR property. Theorem 2 of [6] shows that groups that satisfy the EKR property are necessarily solvable. However, the EKR-module property is not so restrictive.

6.2. A group satisfying the EKR-module property is not necessarily solvable

Lemma 6.2.

The simple group A5A_{5} satisfies the EKR-module property.

Proof.

Let HH be a subgroup of A5A_{5}. We need to show that the action of A5A_{5} on ΩH=[A5:H]\Omega_{H}=[A_{5}:H] satisfies the EKR-module property. Assume that HH is a subgroup satisfying

(3) {χIrr(A5):χ(𝐯H)0}=Irr(A5).\{\chi\in{\rm Irr}(A_{5})\ :\ \chi(\mathbf{v}_{H})\neq 0\}={\rm Irr}(A_{5}).

Then by Theorem 1.5, the action of A5A_{5} on ΩH\Omega_{H} satisfies the EKR-module property. Computation shows that the relation (3) fails if and only if HH is isomorphic to one of the groups:

22,5,S3,D10,A4.\mathbb{Z}^{2}_{2},\ \mathbb{Z}_{5},\ S_{3},\ D_{10},\ A_{4}.

(Here D10D_{10} denotes the dihedral group of order 10.) We will deal with groups separately.

When HH is isomorphic to one of D10D_{10} or A4A_{4}, the action of GG on ΩH\Omega_{H} is 22-transitive. Hence by the main result of [25], these group actions satisfy the EKR-module property.

Consider a subgroup H15H_{1}\cong\mathbb{Z}_{5}. We will use Theorem 3.4 to show that the action of A5A_{5} on ΩH1\Omega_{H_{1}} satisfies the EKR-module property. For this, we need the character table of A5A_{5}, which is given as Table 1.

Table 1. Character table of A5A_{5}.
class ()(\ ) C1C_{1} C2C_{2} C3C_{3} C4C_{4}
size 11 1515 2020 1212 1212
ρ1\rho_{1} 11 11 11 11 11
ρ2\rho_{2} 33 1-1 0 1+52\frac{1+\sqrt{5}}{2} 152\frac{1-\sqrt{5}}{2}
ρ3\rho_{3} 33 1-1 0 152\frac{1-\sqrt{5}}{2} 1+52\frac{1+\sqrt{5}}{2}
ρ4\rho_{4} 44 0 11 1-1 1-1
ρ5\rho_{5} 55 11 1-1 0 0

In this case, the set Der(G,ΩH1)Der(G,\Omega_{H_{1}}), of derangements, is the union of the conjugacy class C1C_{1} containing (1,2)(3,4)(1,2)(3,4) and the conjugacy class C2C_{2} containing (1,2,3)(1,2,3). Let f1f_{1} be the (G,ΩH1)(G,\Omega_{H_{1}})-compatible class function satisfying f1((1,2)(3,4))=1f_{1}((1,2)(3,4))=1 and f1((1,2,3))=2f_{1}((1,2,3))=2. Now application of Theorem 3.4 by setting f=f1f=f_{1} and 𝒮=H1\mathcal{S}=H_{1}, yields that this action satisfies the EKR-module property.

Next, we consider a subgroup H222H_{2}\cong\mathbb{Z}^{2}_{2} in A5A_{5} and the action of A5A_{5} on ΩH2\Omega_{H_{2}}. The set Der(G,ΩH2)Der(G,\Omega_{H_{2}}), of derangements, is the union of the conjugacy class C2C_{2} containing (1,2,3)(1,2,3), the conjugacy class C3C_{3} containing (1,2,3,4,5)(1,2,3,4,5), and the conjugacy class C4C_{4} containing (1,5,4,3,2,1)(1,5,4,3,2,1). Let f2f_{2} be be the (G,ΩH2)(G,\Omega_{H_{2}})-compatible class function satisfying f2((1,2,3))=1f_{2}((1,2,3))=1 and f2((1,2,3,4,5))=f2((1,5,4,3,2,1))=3/2f_{2}((1,2,3,4,5))=f_{2}((1,5,4,3,2,1))=3/2. Now application of Theorem 3.4, by setting 𝒮=H2\mathcal{S}=H_{2} and f=f2f=f_{2}, yields that this action satisfies the EKR-module property.

Finally, we consider a subgroup H3S3H_{3}\cong S_{3} in A5A_{5} and the action of A5A_{5} on ΩH3\Omega_{H_{3}}. The set Der(G,ΩH2)Der(G,\Omega_{H_{2}}), of derangements, is the union of conjugacy classes C3C_{3} and C4C_{4}. Let f3f_{3} be be the (G,ΩH3)(G,\Omega_{H_{3}})-compatible class function satisfying f3((1,2,3,4,5))=f3((1,5,4,3,2,1))=1f_{3}((1,2,3,4,5))=f_{3}((1,5,4,3,2,1))=1. Let KA4K\cong A_{4} be a subgroup of A5A_{5}. As KK1=KgGH3gKK^{-1}=K\subset\bigcup\limits_{g\in G}H_{3}^{g}, we see that KK is an intersecting set with respect to this action. Now, setting 𝒮=K\mathcal{S}=K and f=f3f=f_{3}, Theorem 3.4 yields that this action satisfies the EKR-module property. ∎

7. EKR-module property in Strongly Regular Graphs

In the section, we consider maximum cliques in the Peisert-type strongly regular graphs defined in [4]. These are a subclass of strongly regular graphs found in [7]. Consider a strongly regular graph XX, with a prescribed set 𝒞\mathcal{C} of “naturally” occurring cliques. Cliques in 𝒞\mathcal{C} will be called canonical cliques. We say that XX satisfies the EKR-module property with respect to 𝒞\mathcal{C} if the characteristic vector of every maximum clique in XX is a linear combination of characteristic vectors of the cliques in 𝒞\mathcal{C}. We now define Peisert-type graphs.

Definition 7.1.

Let qq be an odd prime power. Then a Peisert-type graph of type (m,q)(m,q) is a Cayley graph on the additive group of 𝔽q2\mathbb{F}_{q^{2}} with its “connection” set SS being a union of mm cosets of 𝔽q×\mathbb{F}^{\times}_{q} in 𝔽q2×\mathbb{F}^{\times}_{q^{2}} such that 𝔽q×S\mathbb{F}^{\times}_{q}\subset S.

Given a Peisert-type graph of type (m,q)(m,q), with connection set SS. For any sSs\in S and x𝔽q2x\in\mathbb{F}_{q^{2}}, the set s𝔽q+xs\mathbb{F}_{q}+x is a naturally occurring clique. By a canonical clique in a Peiset-type graph, we mean a clique of the form s𝔽q+xs\mathbb{F}_{q}+x, where sSs\in S and x𝔽q2x\in\mathbb{F}_{q^{2}}. The main result of [4] is the following shows that Peiser-type graphs satisfy EKR-module property. In this section, we give a shorter and different proof of the same.

Theorem 7.2.

([4, Theorem 1.3]) The characteristic vector of a maximum clique in a Peisert-type graph is a linear combination of characteristic vectors of its canonical cliques.

We now collect some results about Peisert-type graphs and some general results about strongly regular graphs. The main result of [7] shows that Peisert-type graphs are strongly regular. A different proof of the same is given in [4]. We will give a proof using a standard technique of finding eigenvalues of an abelian Cayley graph.

Lemma 7.3.

Peisert-type graph of type (m,q)(m,q) is strongly regular with eigenvalues k:=m(q1)k:=m(q-1) with multiplicity 1, qmq-m with multiplicity m(q1)m(q-1), and m-m with multiplicity q21m(q1)q^{2}-1-m(q-1).

Proof.

Let XX a Peisert-type graph of type (m,q)(m,q) whose connection set is S=i=0m1ci𝔽q×S=\bigcup\limits_{i=0}^{m-1}c_{i}\mathbb{F}^{\times}_{q} (with c0=1c_{0}=1). Let AA be the adjacency matrix of XX. Considering an additive character of χ\chi of 𝔽q\mathbb{F}_{q} as a column vector, we see that Aχ=χ(𝐯S)χA\chi=\chi(\mathbf{v}_{S})\chi, where χ(𝐯S)=sSχ(s)\chi(\mathbf{v}_{S})=\sum\limits_{s\in S}\chi(s).

If χ\chi is not the trivial character, Ker(χ)𝔽q2Ker(\chi)\neq\mathbb{F}_{q^{2}}, and so at most one of {ci𝔽q: 0im1}\{c_{i}\mathbb{F}_{q}\ :\ 0\leq i\leq m-1\} can be a subgroup of Ker(χ)Ker(\chi). Thus if ci𝔽qKer(χ)c_{i}\mathbb{F}_{q}\subset Ker(\chi) for some ii, then the restriction χ|cj𝔽q\chi|_{c_{j}\mathbb{F}_{q}} of χ\chi onto the subgroup cj𝔽qc_{j}\mathbb{F}_{q}, is a non-trivial character whenever jij\neq i. Otherwise, Ker(χ)Ker(\chi) will have two 11-dimensional subspaces of 𝔽q2\mathbb{F}_{q^{2}} and thus must be equal to 𝔽q2\mathbb{F}_{q^{2}}.

Assume that χ\chi is a non-trivial character with ci𝔽qKer(χ)c_{i}\mathbb{F}_{q}\subseteq Ker(\chi). As the sum of values of a non-trivial character are zero, in this case, we have

χ(𝐯S)\displaystyle\chi(\mathbf{v}_{S}) =xci𝔽q×χ(x)+jixcj𝔽q×χ(x)\displaystyle=\sum\limits_{x\in c_{i}\mathbb{F}^{\times}_{q}}\chi(x)+\sum\limits_{j\neq i}\sum\limits_{x\in c_{j}\mathbb{F}^{\times}_{q}}\chi(x)
=q1(m1)=qm.\displaystyle=q-1-(m-1)=q-m.

The set on non-trivial characters χ\chi with ci𝔽qKer(χ)c_{i}\mathbb{F}_{q}\subset Ker(\chi) is in one-one correspondence with the non-trivial characters of 𝔽q2/ci𝔽q\mathbb{F}_{q^{2}}/c_{i}\mathbb{F}_{q}. Thus there are atleast m(q1)m(q-1) characters χ\chi such that Aχ=(qm)χA\chi=(q-m)\chi. As distinct characters are orthogonal the dimension of the (qm)(q-m)-eigenspace of AA is atleast m(q1)m(q-1).

Similarly, if χ\chi is a non-trivial character with ci𝔽qKer(χ)c_{i}\mathbb{F}_{q}\not\subseteq Ker(\chi) for all 0im10\leq i\leq m-1, we have χ(𝐯S)=m\chi(\mathbf{v}_{S})=-m. Thus there are atleast q21m(q1)q^{2}-1-m(q-1) characters χ\chi such that Aχ=(m)χA\chi=(-m)\chi. As distinct characters are orthogonal the dimension of the (m)(-m)-eigenspace of AA is atleast q21m(q1)q^{2}-1-m(q-1).

If χ\chi is the trivial character χ0\chi_{0}, we have Aχ0=|S|χ0A\chi_{0}=|S|\chi_{0}. With this, we have found all the eigenvalues of AA and their corresponding eigenspaces. As AA has exactly three distinct eigenvalues, it is a strongly regular graph. ∎

Let XX be a strongly regular graph with parameters (v,k,λ,μ)(v,\ k,\ \lambda,\ \mu), which is a kk-regular graph on vv vertices such that

  1. (i)

    any two adjacent vertices have exactly λ\lambda common neighbours, and

  2. (ii)

    any two non-adjacent vertices have exactly μ\mu common neighbours.

We further assume that XX is primitive, that is, both XX and its complement are connected. It is well known ([16, Lemma 10.2.1]) that the adjacency matrix AA of XX has exactly three distinct eigenvalue. As XX is kk-regular and connected, kk is an eigenvalue of AA with multiplicity 11. Let r,sr,s with r>sr>s be the other eigenvalues.

Our proof uses some results on graphs in association schemes. For a quick introduction to the preliminaries on graphs in association schemes, we refer the reader to Chapter 3 of [17]. We first recall the following well-known result linking strongly regular graphs with association schemes. By JJ and II, we denote the all-one matrix and the identity matrix respectively.

Lemma 7.4.

([17, Lemma 5.1.1]) Let XX be a graph with AA as its adjacency matrix. Then XX is strongly regular if and only if 𝒜X:={I,A,A¯:=JIA}\mathcal{A}_{X}:=\{I,\ A,\ \overline{A}:=J-I-A\} is an association scheme.

By [𝒜X]\mathbb{C}[\mathcal{A}_{X}], we denote the linear span of matrices in 𝒜X\mathcal{A}_{X}. This is referred to as the Bose-Mesner algebra. By a well-known result ([17, Theorem 3.4.4]), the projections onto eigenspaces of AA is an orthogonal basis of idempotents of [𝒜X]\mathbb{C}[\mathcal{A}_{X}]. The matrix JJ is the projection onto the kk-eigenspace. We denote ErE_{r} and EsE_{s} to be the projections onto the rr-eigenspace and the ss-eigenspace respectively. We have A=kJ+rEr+sEsA=kJ+rE_{r}+sE_{s}, I=Jn+Er+EsI=\frac{J}{n}+E_{r}+E_{s}, and so {Jn,Er,Es}\{\frac{J}{n},\ E_{r},\ E_{s}\} is an orthogonal basis of idempotents of [𝒜X]\mathbb{C}[\mathcal{A}_{X}]. We now mention a bound by Delsarte (see equation (3.25)(3.25) of [9]) on cliques in strongly regular graphs. We state the formulation of this result as given in [17, Corollary 3.7.2].

Lemma 7.5.

Let XX be kk-regular strongly regular graph with ss as the least eigenvalue of its adjacency matrix. If CC is a clique in XX, then |C|1ks|C|\leqslant 1-\frac{k}{s}.

Moreover, if CC is a clique that meets the bound with equality, then the characteristic vector 𝐯C\mathbf{v}_{C} is orthogonal to the ss-eigenspace.

Given a subset BB of the vertex set of XX, by 𝐯B\mathbf{v}_{B}, we denote the characteristic vector of BB, and by 𝟏\mathbf{1}, the all-one vector. Consider the \mathbb{C}-linear span VmaxV_{max} of characteristic vectors of maximum cliques in XX. By the above lemma, we have |C|1ks|C|\leq 1-\frac{k}{s}, for any clique CC. Assume that there is a clique CC of size 1ks1-\frac{k}{s}, then by the above Lemma, VmaxV_{max} is orthogonal to the ss-eigenspace. We will now show that VmaxV_{max} is in the image of Jn+Er\frac{J}{n}+E_{r}.

Lemma 7.6.

Let XX be kk-regular strongly regular graph on nn vertices with {k,r,s}\{k,\ r,\ s\} with r>sr>s as set of distinct eigenvalues of its adjacency matrix. If XX has a clique of size 1ks1-\frac{k}{s}, then 𝐯C|C|n𝟏\mathbf{v}_{C}-\frac{|C|}{n}\mathbf{1} is an rr-eigenvector.

Proof.

From Lemma 7.5, we have Es𝐯S=0E_{s}\mathbf{v}_{S}=0. As 𝟏\mathbf{1} is a kk-eigenvector, it is also orthogonal to the ss-eigenspace. Since J𝐯C=|C|𝟏J\mathbf{v}_{C}=|C|\mathbf{1}, the vector 𝐯C|C|n𝟏\mathbf{v}_{C}-\frac{|C|}{n}\mathbf{1} is orthogonal to both the kk-eigenspace and the ss-eigenspace, and so must lie in the rr-eigenspace. ∎

We are now ready to prove Theorem 7.2.

Proof of Theorem 7.2: Let XX be a Peisert-type graph of type (m,q)(m,q) whose connection set is S=i=0m1ci𝔽q×S=\bigcup\limits_{i=0}^{m-1}c_{i}\mathbb{F}^{\times}_{q} (with c0=1c_{0}=1). By Lemmas 7.3, 7.5 and 7.6, we obtain the next result.

Lemma 7.7.

If CC is a maximum clique in XX, then |C|=q|C|=q and 𝐯C1q𝟏\mathbf{v}_{C}-\frac{1}{q}\mathbf{1} is a (qm)(q-m)-eigenvector.

Thus, given x𝔽q2x\in\mathbb{F}_{q^{2}} and 0im10\leq i\leqslant m-1, the canonical clique ci𝔽q+xc_{i}\mathbb{F}_{q}+x is a maximum clique and 𝐯ci,x:=𝐯ci𝔽q+x1q𝟏\mathbf{v}_{c_{i},x}:=\mathbf{v}_{c_{i}\mathbb{F}_{q}+x}-\frac{1}{q}\mathbf{1} is a (qm)(q-m)-eigenevector. By Lemma 7.3, the dimension of the (qm(q-m)-eigenspace is m(q1)m(q-1). Using the above Lemma, we can now deduce that Theorem 7.2 follows from showing that {𝐯ci,x:x𝔽q2& 0im1}\{\mathbf{v}_{c_{i},x}\ :\ x\in\mathbb{F}_{q^{2}}\ \&\ 0\leqslant i\leqslant m-1\} spans an m(q1)m(q-1) dimensional vector space.

Given an additive character χ\chi of 𝔽q2\mathbb{F}_{q^{2}}, we set 𝐯χ:=z𝔽q2χ(z)z\mathbf{v}_{\chi}:=\sum\limits_{z\in\mathbb{F}_{q^{2}}}\chi(z)z. In the proof of Lemma 7.3, we see that the (qm)(q-m)-eigenspace VqmV_{q-m}, is spanned by

{𝐯χ: χ is non-trivial and ci𝔽qKer(χ) for some 0im1}.\{\mathbf{v}_{\chi}:\ \text{ $\chi$ is non-trivial and $c_{i}\mathbb{F}_{q}\subseteq\ Ker(\chi)$ for some $0\leqslant i\leqslant m-1$}\}.

Let Ei={vχ:𝔽q2Ker(χ)ci𝔽q}E_{i}=\left\langle\{v_{\chi}\ :\ \mathbb{F}_{q^{2}}\supsetneq Ker(\chi)\supset c_{i}\mathbb{F}_{q}\}\right\rangle. Then we have

Vqm=Ei.V_{q-m}=\bigoplus E_{i}.

By [,]\left[\ ,\ \right], we denote the natural orthogonal form on [𝔽q2]\mathbb{C}[\mathbb{F}_{q^{2}}]. With respect to this form, we have Ei=jiEjE^{\perp}_{i}=\bigoplus\limits_{j\neq i}E_{j}. If χ\chi is a non-trivial character, then

[𝐯χ,𝐯ci,x]=χ(x)zci𝔽qχ(z).\left[\mathbf{v}_{\chi},\mathbf{v}_{c_{i},x}\right]=\chi(x)\sum\limits_{z\in c_{i}\mathbb{F}_{q}}\chi(z).

Therefore, 𝐯ci,xEi\mathbf{v}_{c_{i},x}\in E_{i} for all x𝔽q2x\in\mathbb{F}_{q^{2}}. We will now show that vectors of the form 𝐯ci,x\mathbf{v}_{c_{i},x} span EiE_{i}. Considering x𝔽q2×x\in\mathbb{F}^{\times}_{q^{2}} and fi,x:=𝐯ci, 0𝐯ci,x=𝐯ci𝔽q𝐯ci𝔽q+xf_{i,x}:=\mathbf{v}_{c_{i},\ 0}-\mathbf{v}_{c_{i},\ x}=\mathbf{v}_{c_{i}\mathbb{F}_{q}}-\mathbf{v}_{c_{i}\mathbb{F}_{q}+x}. As the set {𝐯ciFq+x:x𝔽q2}\{\mathbf{v}_{c_{i}F_{q}+x}\ :\ x\in\mathbb{F}_{q^{2}}\} is a set of qq orthogonal vectors, the set {fi,x:x0}\{f_{i,x}:\ x\neq 0\} spans a q1q-1 dimensional vector space. Therefore {𝐯ci,x:x𝔽q2}\{\mathbf{v}_{c_{i},x}:\ x\in\mathbb{F}_{q^{2}}\} spans EiE_{i}. Thus {𝐯ci,x:x𝔽q2& 0im1}\{\mathbf{v}_{c_{i},x}:\ x\in\mathbb{F}_{q^{2}}\ \&\ 0\leqslant i\leqslant m-1\} spans Vqm=EiV_{q-m}=\bigoplus E_{i}. This concludes the proof of Theorem 7.2. ∎

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