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Groups whose Chermak–Delgado lattice is a quasi-antichain

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Veröffentlicht/Copyright: 20. Januar 2019

Abstract

A quasi-antichain is a lattice consisting of a maximum, a minimum, and the atoms of the lattice. The width of a quasi-antichain is the number of atoms. For a positive integer w3, a quasi-antichain of width w is denoted by w. In [B. Brewster, P. Hauck and E. Wilcox, Quasi-antichain Chermak–Delgado lattice of finite groups, Arch. Math. 103 2014, 4, 301–311], it is proved that w can be the Chermak–Delgado lattice of a finite group if and only if w=1+pa for some positive integer a and some prime p. Let t be the number of abelian atoms in 𝒞𝒟(G). In this paper, we completely answer the following question: which values of t are possible in quasi-antichain Chermak–Delgado lattices?

1 Introduction

Chermak and Delgado [4] defined a family of functions from the set of subgroups of a finite group into the set of positive integers. They then used these functions to obtain a variety of results, including a proof that every finite group G has a characteristic abelian subgroup N such that |G:N||G:A|2 for any abelian AG. Chermak–Delgado measures are values of one of these functions. For any subgroup H of G, the Chermak–Delgado measure of H (in G) is denoted by mG(H) and defined as mG(H)=|H||CG(H)|. The maximal Chermak–Delgado measure of G is denoted by m*(G). That is, m*(G)=max{mG(H)HG}. Let 𝒞𝒟(G)={HmG(H)=m*(G)}. Then the set 𝒞𝒟(G) forms a sublattice of subgroups of G, which is called the Chermak–Delgado lattice of G. It was first introduced by Chermak and Delgado [4] and revisited by Isaacs [5].

Recall that the Chermak–Delgado lattice of a finite group is always a self-dual lattice. It is natural to ask a question: which types of self-dual lattices can be used as Chermak–Delgado lattices of finite groups? Some special cases of this question are proposed and solved. In [2], it is proved that, for any integer n, a chain of length n can be a Chermak–Delgado lattice of a finite p-group. In [1], general conclusions are given.

Theorem 1.1 ([1]).

If L is a Chermak–Delgado lattice of a finite p-group G such that both G/Z(G) and G are elementary abelian, then so are L+ and L++, where L+ is a mixed 3-string with center component isomorphic to L and the remaining components being m-diamonds (a lattice with subgroups in the configuration of an m-dimensional cube), L++ is a mixed 3-string with center component isomorphic to L and the remaining components being lattice isomorphic to Mp+1 (a quasi-antichain of width p+1; see the following definition).

A quasi-antichain is a lattice consisting of a maximum, a minimum, and the atoms of the lattice. The width of a quasi-antichain is the number of atoms. For a positive integer w3, a quasi-antichain of width w is denoted by w. In [3], it was proved that w can be the Chermak–Delgado lattice of a finite group if and only if w=1+pa for some positive integer a and some prime p. Furthermore, the following result was proved therein.

Theorem 1.2 ([3]).

If a finite group GCD(G) has a quasi-antichain of width w3, then

  1. the group G is nilpotent of class 2 , both G/Z(G) and G are elementary abelian p-groups for some prime p, and G/Z(G) is a direct product of any pair of atoms modulo Z(G);

  2. there exists a non-abelian Sylow p-subgroup P and an abelian Hall p-subgroup Q such that G=P×Q, P𝒞𝒟(G) and 𝒞𝒟(P)𝒞𝒟(G) as lattices;

  3. the number t of abelian atoms is of the form t=pb+1 for some integer b (where t2).

At the end of [3], two questions are proposed definitely:

  1. Which values of t are possible in quasi-antichain Chermak–Delgado lattices of width w=pa+1 when a>1?

  2. Are there examples of groups G with G𝒞𝒟(G) and 𝒞𝒟(G) a quasi-antichain where t=0 and p1 modulo 4?

This paper answers the above questions completely. It is amazing that there are only two possible relations: a=b or a=2b. In the proof, we use the decomposition of a finitely generated torsion module over a principal ideal domain. Examples related to (Q1) and (Q2) are also given.

2 Main theorem

Main theorem.

Suppose that GCD(G)Mw, and there are, in total, t>2 abelian atoms in CD(G). Then there are positive integers a and b and some prime p such that w=pa+1 and t=pb+1, where a=b or a=2b. If

|G/Z(G)|=p2n,

then |an.

Proof.

By Theorem 1.2 (2), we may assume that G is a finite p-group.

Let M1,M2,,Mw be all the atoms of 𝒞𝒟(G), M1=x1,x2,,xnZ(G) and M2=y1,y2,,ynZ(G) such that M1/Z(G) and M2/Z(G) are elementary abelian groups of order pn for some positive integer n. Then, by Theorem 1.2 (1), for k3, Mk=x1y1,x2y2,,xnynZ(G), where

M2=y1,y2,,ynZ(G).

Moreover, there is an invertible matrix Ck=(cij(k))n×n over Fp such that

yji=1nyicij(k)(modZ(G)),j=1,2,,n.

In this paper, the matrix Ck is called the characteristic matrix of Mk relative to (x1,x2,,xn) and (y1,y2,,yn).

Without loss of generality, we may assume that M1, M2 and M3 are abelian atoms. For convenience, the operation of the group G/Z(G) is written as addition. By Theorem 1.2 (1), M3=x1+y1,x2+y2,,xn+ynZ(G) such that

yji=1ncij(3)yi(modZ(G)),j=1,2,,n;

C3=(cij(3))n×n is the characteristic matrix of M3 relative to (x1,x2,,xn) and (y1,y2,,yn). Replacing y1,y2,,yn with y1,y2,,yn respectively, we may assume that C3=In.

Let zij=[xi,yj] and Z=(zij)n×n. Then G=ziji,j=1,2,,n. We have the following formalized calculation (where CT is denoted to the transpose of C):

[((x1,x2,,xn)+(y1,y2,,yn)Ck)T,(x1,x2,,xn)+(y1,y2,,yn)Ck]
=[(x1,x2,,xn)T+CkT(y1,y2,,yn)T,(x1,x2,,xn)+(y1,y2,,yn)Ck]
=[(x1,x2,,xn)T,(y1,y2,,yn)Ck]
   +[CkT(y1,y2,,yn)T,(x1,x2,,xn)]
=ZCk+CkT(-ZT)=ZCk-(ZCk)T.

Hence CG(Mk)=Mk if and only if (ZCk)T=ZCk. In particular, Mk is abelian if and only if ZCk is symmetric. Since M3 is abelian, ZT=Z.

Let 𝕍={Cn(Fp)there existsCn(Fp)such thatCTZ=ZC}. Notice that if C𝕍 and CTZ=ZC, then C𝕍. It is straightforward to prove that 𝕍 is a linear space over Fp. Hence |𝕍|=pa for some positive integer a.

Assume that OnC𝕍 and CTZ=ZC. Let

(s1,s2,,sn)=(x1,x2,,xn)+(y1,y2,,yn)C,
(t1,t2,,tn)=(x1,x2,,xn)+(y1,y2,,yn)C.

Then, by the formalized calculation above, [(s1,s2,,sn)T,(t1,t2,,tn)]=On. Let

N1=s1,s2,,snZ(G)andN2=t1,t2,,tnZ(G).

Then N2CG(N1). Hence |N1||CG(N1)||N1||N2|=|M1|2=m*(G). This implies that N1𝒞𝒟(G), and, there is some k3 such that N1=Mk. Hence 𝕍{On} is the set of Ck where 3kw. Since Ck is invertible, 𝕍 is a division algebra. By Wedderburn’s little theorem, 𝕍 is also a finite field. Now we know that w-2=pa-1. Notice that an (see [3, Theorem 6]). Let A=(aij) be a primitive element of 𝕍, and mA(λ)=k0+k1λ++ka-1λa-1-kaλa the minimal polynomial of A. Then 𝕍={On,A,A2,,Apa-1=In}=Fp(A).

Notice that M2/Z(G) can be regarded as a n-dimensional vector space 𝕍2 over Fp, in which (y1Z(G),y2Z(G),,ynZ(G)) is a basis for 𝕍2. We can make 𝕍2 an Fp[λ]-module by defining the action of any polynomial g(λ)=b0+b1λ++bmλm on any vector y𝕍2 as g(λ)y=b0+b1(𝒜y)++bm(𝒜my), where 𝒜(yjZ(G))=(i=1naijyi)Z(G), j=1,2,,n. By the well-known principal ideal domain theory and linear algebra arguments, 𝕍2 is a direct sum of r=n:a cyclic module. Thus

A=Diag(B,B,,B)r-timeswithB=(00k010k101ka-1).

Suppose that ATZ=ZA1. Since A1𝕍, there is 1kpa-1 such that A1=Ak. Thus ATZ=ZAk. Let

Z=(Z11Z12Z1rZ21Z22Z2rZr1Zr2Zrr),

where Zij are a×a matrices. Since ZT=Z, Zji=ZijT for 1ijr. It follows from ATZ=ZAk that

(2.1)BTZij=ZijBk,
(2.2)BTZji=ZjiBk.

Let

Zij=(Zij(1)Zij(2)Zij(a)).

Then

(2.3)BTZij=(Zij(2)Zij(3)k0Zij(1)+k1Zij(2)++ka-1Zij(a)).

By (2.1) and (2.3),

(2.4)Zij(2)=Zij(1)Bk,Zij(3)=Zij(2)Bk,,Zij(a)=Zij(a-1)Bk,
(2.5)k0Zij(1)+k1Zij(2)++ka-1Zij(a)=Zij(a)Bk.

Hence

Zij(1)(k0+k1Bk++ka-1B(a-1)k-Bak)=0.

That is, Zij(1)mA(Bk)=0. We claim that mA(Bk)=0. Otherwise, mA(Ak)0. Since mA(Ak)𝕍 and 𝕍 is a field, mA(Ak) is invertible. Hence mA(Bk) is also invertible. Notice that if Zij(1)=0 then Zij=Oa by (2.4) and (2.5). Hence we may choose Zij such that Zij(1)0. In this case, Zij(1)mA(Bk)0, a contradiction. Thus mA(Bk)=0 and mA(Ak)=0. Since Ap,Ap2,,Apa=A are all zero points of mA(λ), there exists a 1ea such that k=pe. By easy calculation, (Am)TZ=ZAmpe.

Let 𝕎={C𝕍CTZ=ZC}. Then |𝕎|=t-1 since t is the number of abelian atoms in 𝒞𝒟(G). Since Ampe=Am if and only if |(pa-1)m(pe-1),

𝕎{On}={Am𝕍|(pa-1)m(pe-1)}.

Hence 𝕎{On} is a cyclic group generated by Apa-1(pa-1,pe-1) of order

(pa-1,pe-1)=p(a,e)-1.

Let b=(a,e). Then t=pb+1. By (2.1),

(Bpe)TZij=ZijBp2e

By (2.2),

(Bpe)TZij=ZijB

Hence |(pa-1)(p2e-1). Thus |a2e. It follows that |a2b. Hence a=e=b or a=2e=2b. ∎

3 Examples

The main theorem gives the possible values of t. In this section, we will give examples in which t is exactly such values respectively. The key is to construct the commutator matrices Z=(zij)n×n.

Remark 3.1.

Let F be a field containing pa elements, and let F* be the multiply group of F. Then F* is cyclic with order pa-1. Let F*=b and :fbf be linear transformations over F, where F is regarded as a linear space over the field Fp. Of course, the order of is pa-1. Let p(x) be the minimal polynomial of . It follows from the Cayley–Hamilton theorem that deg(p(x))=ra. Let W={f()f(x)Fp[x]}={f1()f1(x)Fp[x],deg(f1)<r}. Then dimW=deg(p(x))=r and hence |W|=pr. On the other hand,

{1,,2,,pa-1}W,

and hence |W|pa. So we get r=a. Let the minimal polynomial of be

p(x)=xa-ka-1xa-1--k1x-k0.

Then a matrix of is

B=(00k010k101ka-1).

Lemma 3.2.

Let B be the matrix introduced in Remark 3.1. Let Z=(zij) be an a×a matrix. If BTZ=ZB, then Z is symmetric.

Proof.

By calculation, the (u,v)-th entry of BTZ is zu+1,v, while the (u,v)-th entry of ZB is zu,v+1, where 1u,va-1. Hence zu+1,v=zu,v+1, where 1u,va-1. Then, for uv, we have

zu,v+1=zu+1,v=zu+2,v-1==zv,u+1=zv+1,u.

Hence Z is symmetric. ∎

Theorem 3.3.

Suppose that a and r are positive integers. Let n=ar, and let p be a prime. Then there exists a group G such that |G/Z(G)|=p2n, and CD(G) is a quasi-antichain of width w=pa+1, in which the number of abelian atoms is t=pa+1.

Proof.

We construct G=x1,x2,,xn,y1,y2,,yn with defining relationships:

  1. xip=yip=1, [xi,xj]=[yi,yj]=1, [xi,yj]=zij for all i and j such that 1i,jn;

  2. z(u-1)a+1,(v-1)a+jZ(G) for 1uvr and 1ja;

    (In the following, we use the addition operation to denote the multiplication operation.)

  3. Zuv(k)=Zuv(1)Bk-1 for 1uvr and 2ka, where

    Zuv(k):=(z(u-1)a+k,(v-1)a+1,z(u-1)a+k,(v-1)a+2,,z(u-1)a+k,(v-1)a+a);
  4. Zuv=ZvuT for 1v<ur, where

    Zuv=(z(u-1)a+i,(v-1)a+j)=(Zuv(1)Zuv(2)Zuv(a)).

It is easy to see that

G=Z(G)=z(u-1)a+1,(v-1)a+j1uvr, 1ja

is elementary abelian of order pr+12n. Hence |G|=pr+52n.

By relationship (3), BTZuv=ZuvB for 1uvr. By Lemma 3.2, Zuv is symmetric for 1uvr. Hence Zuv=ZvuT=Zvu for 1v<ur. Moreover, ZuvT=ZvuT=Zuv=Zvu for all 1u,vr. Let

Z=(Z11Z12Z1rZ21Z22Z2rZr1Zr2Zrr).

Then ZT=Z. Let X=x1,x2,,xnZ(G) and Y=y1,y2,,ynZ(G).

Assertion (1): CG(x)=X for all xXZ(G). Let x=i=1ncixi+z, where zZ(G). Write Ck=(c(k-1)a+1,c(k-1)a+2,,cka) for 1kr. Since xZ(G), there exists a k0 such that Ck0(0,0,,0). Exchanging

x(k0-1)a+1,y(k0-1)a+1,,xk0a,yk0aandx(r-1)a+1,y(r-1)a+1,,xra,yra,

we have Cr(0,0,,0). Let Hi=[x,y(i-1)a+j]1ja for 1ir. We will prove that H1+H2++Hv is of order pva. Using induction, we may assume that H1+H2++Hv-1 is of order p(v-1)a. By calculation,

([x,y(v-1)a+1],,[x,yva])=k=1nck([xk,y(v-1)a+1],,[xk,yva])=u=1ri=1ac(u-1)a+i([x(u-1)a+i,y(v-1)a+1],,[x(u-1)a+i,yva])=u=1ri=1ac(u-1)a+iZuv(i)=u=1ri=1ac(u-1)a+iZuv(1)Bi-1=u=1rZuv(1)(i=1ac(u-1)a+iBi-1)=u=1r-1Zuv(1)(i=1ac(u-1)a+iBi-1)+Zrv(1)(i=1ac(r-1)a+iBi-1).

Since Cr(0,0,,0),

i=1ac(r-1)a+iBi-1Oa.

By Remark 3.1, i=1ac(r-1)a+iBi-1 is invertible. Hence

Zrv(1)(i=1ac(r-1)a+iBi-1)

is of rank a. It follows that

(H1+H2++Hv-1)Hv=0.

Thus H1+H2++Hv is of order pva.

By the discussion above, H1+H2++Hr is of order pn, and hence |[x,G]|=pn. It follows that

|CG(x)|=|G|/pn=pr+32n.

Since |X|=pr+32n and XCG(x), CG(x)=X.

Similarly, we have CG(y)=Y for all yYZ(G). Then CG(X)=X and CG(Y)=Y, yielding mG(G)=mG(X)=mG(Y)=p(r+3)n.

Assertion (2): m*(G)=p(r+3)n and 𝒞𝒟(G) is a quasi-antichain. Otherwise, by the dual-property of 𝒞𝒟-lattice, there exists H𝒞𝒟(G) such that

H<Gand|H|>p(r+3)2n.

Since

|HX|=|H||X||HX|>p(r+1)2n=|Z(G)|,

there exists xHXZ(G). Hence CG(H)CG(x)=X. Similarly, we have CG(H)Y. Hence CG(H)=Z(G) and mG(H)<mG(G), a contradiction.

The discussion above also gives that 𝒞𝒟(G) is a quasi-antichain, in which every atom is of order p(r+3)2n.

Assertion (3): w=t=1+pa. Now we have G,Z(G),X,Y𝒞𝒟(G). Let M be an atom different from X and Y. Then, by the same reason given in the main theorem, we may let M=w1,w2,,wn and N=CG(M)=v1,v2,,vn, where

(w1,w2,,wn)=(x1,x2,,xn)+(y1,y2,,yn)C,
(v1,v2,,vn)=(x1,x2,,xn)+(y1,y2,,yn)D.

Since [M,N]=0, CTZ=ZD. Let

C=(C11C12C1rC21C22C2rCr1Cr2Crr)andD=(D11D12D1rD21D22D2rDr1Dr2Drr).

Then

(3.1)k=1rCkiTZkj=k=1rZikDkjfor 1i,jr.

Taking ij in equation (3.1) and comparing the two sides, we get Cik=Oa for ik, Dkj=Oa for kj, and

CiiTZij=ZijDjjfor 1i,jrandij.

Taking i=j in equation (3.1) and comparing the two sides, we get

CiiTZii=ZiiDiifor 1ir.

Notice that Zij and Zii have no essential difference, and thus Cii=Cjj and Dii=Djj for ij.

Let 𝕍={Ua(Fp)there existsVa(Fp)such thatUTZ11=Z11V}. Similar to the proof of the main theorem, 𝕍 is a division algebra. Hence 𝕍 has at most pa elements (otherwise, there exists a non-zero matrix in which the elements of the first row are all zero, a contradiction). Notice that BTZ11=Z11B. Hence Bk𝕍, where 1kpa-1. It follows that 𝕍={On,B,B2,,Bpa-1=In}.

Therefore, C=D=Diag(Bk,Bk,,Bk) for some 1kpa-1. Hence w=t=pa+1. ∎

Theorem 3.4.

Suppose that a,b and r are positive integers such that a=2b and r3. Let n=ar. Then there exists a group G such that |G/Z(G)|=p2n, and CD(G) is a quasi-antichain of width w=pa+1, in which the number of abelian atoms is t=pb+1.

Proof.

We construct G=x1,x2,,xn,y1,y2,,yn with defining relationships:

  1. xip=yip=1, [xi,xj]=[yi,yj]=1, [xi,yj]=zij for all i and j such that 1i,jn;

  2. z(u-1)a+1,(v-1)a+jZ(G) for 1uvr and 1ja;

  3. [x(u-1)a+i,y(u-1)a+j]=1 for 1ur and 1i,ja;

    (In the following, we use the addition operation to denote the multiplication operation.)

  4. Zuv(k)=Zuv(1)B(k-1)pb for 1u<vr and 2ka, where

    Zuv(k):=(z(u-1)a+k,(v-1)a+1,z(u-1)a+k,(v-1)a+2,,z(u-1)a+k,(v-1)a+a);
  5. Zuv=ZvuT for 1v<ur, where

    Zuv=(z(u-1)a+i,(v-1)a+j)=(Zuv(1)Zuv(2)Zuv(a)).

It is easy to see that

G=Z(G)=z(u-1)a+1,(v-1)a+j1u<vr, 1ja

is elementary abelian of order pr-12n. Hence |G|=pr+32n.

By relationship (4), BTZuv=ZuvBpb for 1u<vr. In this case, Zuv is not symmetric and ZuvZvu for all 1v<ur. Let

Z=(Z11Z12Z1rZ21Z22Z2rZr1Zr2Zrr).

Then ZT=Z. Let X=x1,x2,,xnZ(G) and Y=y1,y2,,ynZ(G).

Similar to assertion (1) in the proof of Theorem 3.3, we have |[x,Y]|p(r-1)a for all xXZ(G). It follows that |CY(x)||Y|/p(r-1)a=pa|Z(G)|.

Similarly, |CX(y)|pa|Z(G)| for all yYZ(G). It is easy to check that CG(X)=X and CG(Y)=Y, yielding mG(G)=mG(X)=mG(Y)=p(r+1)n.

Assertion (1): m*(G)=p(r+1)n. Otherwise, by the dual-property of the 𝒞𝒟-lattice, there exists H𝒞𝒟(G) such that

H<Gand|H|>p(r+1)2n.

Since

|HX|=|H||X||HX|>p(r-1)2n=|Z(G)|,

there exists xHXZ(G), and hence CG(H)CG(x)=XCY(x). Similarly, there exists yHYZ(G), and hence CG(H)CG(y)=YCX(y). It follows that CG(H)CX(y)CY(x). Hence |CG(H)|p2a|Z(G)|. Obviously, CG(H)>Z(G). Hence there exists xyCG(H)Z(G), where xCX(y), yCY(x). If xZ(G), then |[G,xy]||[Y,x]|p(r-1)a; If yZ(G), then |[G,xy]||[X,y]|p(r-1)a. Whatever, we have

|[G,xy]|p(r-1)a=pn-a.

It follows that |H||CG(xy)|=|G:[G,xy]||G|pn-a=pr+12n+a. Hence mG(H)=|H||CG(H)|prn+3ap(r+1)n, a contradiction.

Assertion (2): 𝒞𝒟(G) is a quasi-antichain. Otherwise, by the dual-property of the 𝒞𝒟-lattice, there exists H𝒞𝒟(G) such that

H<Gand|H|>p(r+1)2n.

By the same argument used within the proof of assertion (1), n=3a, and there exists xHXZ(G) and yHYZ(G) such that CG(H)=CX(y)CY(x), where |CX(y)|=|CY(x)|=pa|Z(G)|. Take

xCX(y)Z(G)andyCY(x)Z(G).

Then HCG(y)CG(x)=CX(y)YXCY(x)=CX(y)CY(x). Hence

|H|p2a|Z(G)|<p(r+1)2n,

a contradiction.

Assertion (3): w=pa+1 and t=pb+1. Let M be an atom different from X and Y. Then, by the same reason given in the main theorem, we may let M=w1,w2,,wn and N=CG(M)=v1,v2,,vn where

(w1,w2,,wn)=(x1,x2,,xn)+(y1,y2,,yn)C,
(v1,v2,,vn)=(x1,x2,,xn)+(y1,y2,,yn)D.

We also have CTZ=ZD. Let

C=(C11C12C1rC21C22C2rCr1Cr2Crr)andD=(D11D12D1rD21D22D2rDr1Dr2Drr).

Then

(3.2)k=1rCkiTZkj=k=1rZikDkjfor 1i,jr.

Taking ij in equation (3.2) and comparing the two sides, we get Cik=Oa for ik, Dkj=Oa for kj, and

CiiTZij=ZijDjjfor 1i,jrandij.

Notice that Zij, Zik and Zki have no essential difference for ki,j. Thus Cii=Ckk and Djj=Dkk for ki,j. Since r3, C11=C22==Crr and D11=D22==Drr.

Let 𝕍={Ua(Fp)there existsVa(Fp)such thatUTZ12=Z12V}. Similar to the proof in the main theorem, 𝕍 is a division algebra. Hence 𝕍 has at most pa elements (otherwise, there exists a non-zero matrix in which the elements of the first row are all zero, a contradiction). Notice that BTZ12=Z12Bpb. Hence Bk𝕍 where 1kpa-1. It follows that

𝕍={On,B,B2,,Bpa-1=In}.

Therefore, C=Diag(Bk,Bk,,Bk) and D=Diag(Bkpb,Bkpb,,Bkpb) for some 1kpa-1. Hence w=pa+1. It is easy to see that M=N if and only if C=D if and only if kpbk(modpa-1=(pb-1)(pb+1)) if and only if |(pb+1)k. Hence M is abelian if and only if

k{pb+1,2(pb+1),,(pb-1)(pb+1)},

and the number of abelian atoms is t=(pb-1)+2=pb+1 (X and Y are also abelian atoms). ∎

In the following, we will give examples in which the number of abelian atoms is less than 3.

Theorem 3.5.

Suppose that a and r are positive integers such that r3. Let n=ar. Then there exists a group G such that |G/Z(G)|=p2n, and CD(G) is a quasi-antichain of width w=pa+1, in which the number of abelian atoms is 1 or 2 for p=2 or p2 respectively.

Proof.

We construct G=x1,x2,,xn,y1,y2,,yn with defining relationships:

  1. xip=yip=1, [xi,yj]=1, [xi,yj]=zij for 1i,jn;

  2. [x(u-1)a+i,x(u-1)a+j]=1 for 1ur and 1i<ja;

  3. [x(u-1)a+i,x(v-1)a+j]=z(u-1)a+i,(v-1)a+j for 1u<vr and 1i,ja;

  4. [yi,yj]=[xj,xi] for 1i<jn;

  5. z(u-1)a+1,(v-1)a+jZ(G) for 1u<vr and 1ja;

    (In the following, we use the addition operation to denote the multiplication operation.)

  6. Zuv(k)=Zuv(1)Bk-1 for 1u<vr and 2ka, where

    Zuv(k):=(z(u-1)a+k,(v-1)a+1,z(u-1)a+k,(v-1)a+2,,z(u-1)a+k,(v-1)a+a).

For 1u,vr, let

Zuv=(z(u-1)a+i,(v-1)a+j)=(Zuv(1)Zuv(2)Zuv(a)).

It is easy to see that Zuv=-ZvuT for 1v<ur,

G=Z(G)=z(u-1)a+1,(v-1)a+j1u<vr, 1ja

is elementary abelian of order pr-12n. Hence |G|=pr+32n.

By relationship (2), Zuu=Oa for 1ur. By relationship (6), BTZuv=ZuvB for 1u<vr. By Lemma 3.2, Zuv is symmetric for 1u<vr. Hence Zuv=-ZvuT=-Zvu for 1v<ur. Moreover, BTZuv=ZuvB for all 1u,vr. Let

Z=(Z11Z12Z1rZ21Z22Z2rZr1Zr2Zrr).

Then ZT=-Z. Let X=x1,x2,,xnZ(G) and Y=y1,y2,,ynZ(G).

Similar to assertion (1) in the proof of Theorem 3.3, we have |[x,X]|p(r-1)a for all xXZ(G). It follows that |CX(x)||X|/p(r-1)a=pa|Z(G)|.

Similarly, |CY(y)|pa|Z(G)| for all yYZ(G). It is easy to check that CG(X)=Y and CG(Y)=X, yielding mG(G)=mG(X)=mG(Y)=p(r+1)n.

Similar to assertion (1) and assertion (2) in the proof of Theorem 3.4, we have m*(G)=p(r+1)n, and 𝒞𝒟(G) is a quasi-antichain.

Let M be an atom different from X and Y. Then, by the same reason given in the main theorem, we may let M=w1,w2,,wn and N=CG(M)=v1,v2,,vn, where

(w1,w2,,wn)=(x1,x2,,xn)+(y1,y2,,yn)C,
(v1,v2,,vn)=(x1,x2,,xn)D+(y1,y2,,yn).

Since [M,N]=0, CTZ=ZD. Let

C=(C11C12C1rC21C22C2rCr1Cr2Crr)andD=(D11D12D1rD21D22D2rDr1Dr2Drr).

Similar to assertion (3) in the proof of Theorem 3.3, we have

C=D=Diag(Bk,Bk,,Bk)for some 1kpa-1.

Hence w=pa+1. It is easy to see that M=N if and only if CD=In if and only if |(pa-1)2k.

If p=2, then (pa-1,2)=1. Hence M is abelian if and only if k=pa-1. In this case, the number of abelian atoms is 1. If p>2, then M is abelian if and only if k=pa-1 or k=pa-12. Hence the number of abelian atoms is 2. ∎

Theorem 3.6.

Suppose that p is an odd prime, a is odd, and r is a positive integer such that r3. Let n=ar. Then there exists a group G with |G/Z(G)|=p2n, and CD(G) is a quasi-antichain of width w=pa+1, in which the number of abelian atoms is t=0.

Proof.

Let G=x1,x2,,xn,y1,y2,,yn with defining relationships similar to that in Theorem 3.5. The unique difference is relationship (4), which is replaced with the following:

  1. [yi,yj]=[xj,xi]ν for 1i<jn, where ν is a fixed quadratic non-residue module p;

Similar to the proof of Theorem 3.5, we have m*(G)=p(r+1)n, 𝒞𝒟(G) is a quasi-antichain, w=pa+1, νC=D=Diag(Bk,Bk,,Bk) for some 1kpa-1, and M=N if and only if νB2k=Ia.

By the definition of B,

Bpa-1p-1=lIa1lp-1.

Since ν is not a square, there exists an odd m such that Bmpa-1p-1=νIa.

If νB2k=Ia, then

|(pa-1)2k+mpa-1p-1.

Notice that m and pa-1p-1=1+p++pa-1 are all odd. There is no integer k such that νB2k=Ia. Hence the number of abelian atoms is t=0. ∎


Communicated by Evgenii I. Khukhro


Award Identifier / Grant number: 11471198

Award Identifier / Grant number: 11771258

Funding statement: This work was supported by NSFC (No. 11471198 & 11771258).

Acknowledgements

I cordially thank the referee for their detailed reading and helpful comments, which helped me to improve the whole paper considerably.

References

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Received: 2018-01-19
Revised: 2018-12-05
Published Online: 2019-01-20
Published in Print: 2019-05-01

© 2019 Walter de Gruyter GmbH, Berlin/Boston

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