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Research Articles

Non-induced modular representations of cyclic groups

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Pages 2346-2357 | Received 17 Jan 2023, Accepted 14 Nov 2023, Published online: 17 Jan 2024

Abstract

We compute the ring of non-induced representations for a cyclic group, Cn, over an arbitrary field and show that it has rank φ(n), where φ is Euler’s totient function—independent of the characteristic of the field. Along the way, we obtain a “pick-a-number” trick; expressing an integer n as a sum of products of p-adic digits of related integers.

2020 MATHEMATICS SUBJECT CLASSIFICATION:

1 Introduction

Given a finite group G and a field k of characteristic p0, we may study the representation theory of G over k via the representation ring RkG, whose elements are (isomorphism classes of) kG modules, {V}. Here, and throughout, the representations of G over k will be identified with kG-modules. The addition and multiplication operations on the representation ring correspond to taking the direct sum and tensor product of modules. That is; {V}+{U}={VU} and {V}·{U}={VkU}.

Observe that the representation ring differs from the Grothendieck ring, as in the Grothendieck ring we have {V}+{U}={W} whenever there is a short exact sequence 0VWU0. We shall abuse notation when working in the representation ring and write V for the isomorphism class {V}.

Recall that if H is a subgroup of G, and V is a kG-module, then we may consider V as a kH-module, simply by only considering the action of the elements in kH. This module will be denoted by VHG, or often just VH, and is called the restriction of V to H. It is clear that if KHG, then VHGKH=VKG,which is to say that restriction is transitive.

On the other hand, if HG and V is a kH-module, then VHG=kGkHVis the kG-module induced from H to G. Here, the G action is given by left multiplication on the first factor. We call this process induction and say that VHG is an induced module. Induction is also transitive, which is to say if KHG, then VKHHG=VKG.

Since (VU)  HG V  HGU  HG, induction gives rise to a well defined (additive) group homomorphism of the representation rings, which we denote IndHG:RkHRkG.

Lemma 1.

[Citation6, Corollary 4.3.8 (4)] The image IndHG(RkH) is an ideal in RkG.

The quotient of the representation ring by this ideal gives a measure of the kG-modules which are not induced from kH-modules. We shall now turn our attention to the kG-modules which are not induced from any proper subgroup. That is, we study the quotient RkGH<GIndHGRkH,which we shall refer to as the ring of non-induced representations. This was considered for cyclic groups by Srihari in [Citation4], where the following is proved:

Theorem 2.

Let G be a cyclic group of order n and k an algebraically closed field of characteristic 0. Then RkGH<GIndHGRkHZ[Y](Φn(Y)),where Φn is the nth cyclotomic polynomial. In particular, rank(RkGH<GIndHGRkH)=φ(n), where φ(n) is the number of integers less than n coprime to n.

The main goal of this paper is to prove an analogous result over fields of positive characteristic. We first shall observe that the proof of Theorem 2 provided in [Citation4] actually shows:

Corollary 3.

Let G be a cyclic group of order n and k an algebraically closed field of characteristic p such that p∤n. Then RkGH<GIndHGRkHZ[X](Φn(X)).

In particular the rank of the ring of non-induced representations is φ(n).

In Theorem 24 we will expand this result on cyclic groups to a field of arbitrary characteristic and see that the rank of the ring is unchanged at φ(n). Along the way we will discover a convenient, fractal-like basis (see ) of the representation ring which lifts to a basis of the quotient.

Fig. 1 The change of basis matrix, expressing Vi in terms of Uj over characteristic p = 3. Here i increases downwards along rows and j to the right along columns and a cell is filled if the coefficient is 1 and empty if it is 0. Notice, for example that V i = Ui whenever i=apk with 1a<p. This picture appears also in [Citation5, Figure 2], where it shows the Weyl-Cartan matrix counting the decomposition multiplicities of simple sl2-modules in Weyl sl2-modules over characteristic p.

Fig. 1 The change of basis matrix, expressing Vi in terms of Uj over characteristic p = 3. Here i increases downwards along rows and j to the right along columns and a cell is filled if the coefficient is 1 and empty if it is 0. Notice, for example that V i = Ui whenever i=apk with 1≤a<p. This picture appears also in [Citation5, Figure 2], where it shows the Weyl-Cartan matrix counting the decomposition multiplicities of simple sl2-modules in Weyl sl2-modules over characteristic p.

2 Cyclic p-groups

Throughout this section, let k be an algebraically closed field of characteristic p > 0. Let q=pα and denote by G=Cq the cyclic group of order q generated by element g.

2.1 The representation ring

Lemma 4.

[Citation1, Proposition 1.1] For k and G as above,

  1. there is a ring isomorphism kGk[X]/(Xq), defined by sending g to 1+X,

  2. under this isomorphism, a complete set of (pairwise non-isomorphic) indecomposable kG-modules is given by

    {Vr:=k[X]/(Xr):1rq},

  3. the trivial module, V1, is the unique irreducible kG-module.

To understand RkG, we first need to understand the structure of multiplication. In other words we need to understand the decomposition of the tensor product VrVs into indecomposable parts. The decomposition rule was known to Littlewood, and has been discussed by a number of authors. The following multiplication table is given in the lecture notes of Almkvist and Fossum [Citation1] and is derived by Green [Citation2]:

Proposition 5.

For each k<α and spk+1 we have the following decompositions. If spk, then Vpk1·Vs=(s1)Vpk+VpksVpk+1·Vs=(s1)Vpk+Vpk+s.

Otherwise, if pk<spk+1 then write s=s0pk+s1 with 0s1<pk. Then Vpk1·Vs=(s11)V(s0+1)pk+V(s0+1)pks1+(pks11)Vs0pk.

If s0<p1, then Vpk+1·Vs=(s11)V(s0+1)pk+V(s0+1)pks1+(pks11)Vs0pk+Vs+pk+Vspkwhile if s0=p1, Vpk+1·Vs=(s1+1)Vpk+1+(pks11)V(p1)pk+V(p2)pk+s1, and if s0=p and s1=0, Vpk+1·Vs=Vpk+1+(pk1)Vpk+1+V(p1)pk.

This suggests the construction in [Citation1] which defines, for 0k<α, elements in RkG denoted χk=Vpk+1Vpk1 (where V0 is interpreted as the zero representation—the zero in RkG) so that (1) χk·Vs={Vs+pkVpks1spkVs+pk+Vspkpk<s<(p1)pkVspk+2Vpk+1V2pk+1(s+pk)(p1)pks<pk+1(1)

In particular, if 1j<p then χk·Vjpk=V(j1)pk+V(j+1)pk.

To complete the multiplication rule, Renaud [Citation3] gives a reduction theorem which allows us to express Vr·Vs in terms of the tensor product of smaller modules:

Theorem 6

(Reduction Theorem). For 1rspβ+1, with r=r0pβ+r1,s=s0pβ+s1, where 1β<α, and 0(r1,s1)<pβ: Vr·Vs=c1Vpβ+1+|r1s1|i=1d1V(s0r0+2i)pβ+max(0,r1s1)V(s0r0)pβ+(pβs1r1)i=1d2V(s0r0+2i1)pβ+j=1laj[i=1d1(V(s0r0+2i)pβ+bj+V(s0r0+2i)pβbj)+V(s0r0)pβ+bj],where c1={0 if r0+s0<p,r+spβ+1 if r0+s0p,d1={r0 if r0+s0<p,ps01 if r0+s0p,d2={r0 if r0+s0<p,ps0 if r0+s0p, and Vr1·Vs1=j=1lajVbj.

This allows a general tensor product to be reduced to the tensor product of smaller modules, which can be calculated via repeated applications of Theorem 6, and finally Proposition 5, or similar multiplication rules appearing in [Citation3].

To aid in exposing the structure of RkG, we adjoin elements μk±1 for 0k<α subject to χk=μk+μk1. If so, then for each 0<s<p, we have that μks+μks=Vspk+1Vspk1. With this set up Alkvist and Fossum are able to completely determine the structure of RkG by identifying RkG with a quotient of a polynomial ring. Before we can state their result, we will first state some identities involving the χi and then define some families of polynomials.

Lemma 7.

Let i < j and 0<s<p, then we have χis=ν=0s12(sν)(V(s2ν)pi+1V(s2ν)pi1)+{(ss/2)s even0s oddand χiχj=Vpj+pi+1Vpjpi1Vpj+pi1+Vpjpi+1.

Proof.

The first fact can be verified by considering the expansion of (μi+μi1)s, while the second is obtained from applications of Proposition 5. □

Now, still following [Citation1], we define some families of polynomials. These are easier to state if we allow ourselves to use the language of quantum numbers which are briefly introduced here.

Definition 8.

The quantum number, [n] for nZ, are polynomials in Z[X] that satisfy [0]=0,[1]=1,[2]=X, and [n]=[2][n1][n2]. We shall write [n]x for the nth quantum number evaluated at X = x.

The first quantum numbers are

Notice that the coefficients are such that [n]2=n. We can also write [n]=i=0n/2(1)i(n1ii)Xn12i.

In this formulation, [n+1]q+q1=qn+qn2++qn+2+qn.

Consider the polynomials in Z[X0,,Xα1], Fj=(Xj2[p]Xj12[p1]Xj1)[p]Xj,where 1j<α, together with F0=(X02)[p]X0. We are now ready to state a structure theorem for RkG.

Theorem 9.

[Citation1, Proposition 1.6] The map Z[X0,,Xα1]RkG defined by Xiχi induces a ring isomorphism Z[X0,,Xα1](F0,F1,,Fα1)RkG.

2.2 Induced representations

The subgroups of G are all cyclic p groups generated by some power of g. Consider H=gpαβ, the subgroup of G of order pβ. The group algebra kHkG is identified, under the isomorphism in Lemma 4, with k[Xpαβ]/(Xpα). Its indecomposable representations are again each of the form Wi=k[Xpαβ]/(Xipαβ) for 1i<pβ. Inducing to obtain a kG-module we get:

Lemma 10.

We have an isomorphism of kG-modules WrHG Vrpαβ.

Proof.

Note kGkHWr is cyclic as a kG-module, generated by e1 and has dimension rpαβ. □

Thus IndHGRkH consists of all kG-modules Vi such that i is divisible by pβ. Hence, since G has a unique maximal subgroup, and induction is transitive, H<GIndHGRkH consists of all the kG-modules Vi such that i is divisible by p. We have thus shown:

Proposition 11.

Let G=Cq the cyclic group of order q=pα and let k be a field of characteristic p. Then H<GIndHGRkH={Vi:p|i}Z.

To describe the ring of non-induced representations, RkGH<GIndHGRkH,via the isomorphism in Theorem 9 we would aim to write the kG-modules Vi where p|i in terms of the χi. Instead, we shall change basis and give an alternative description of the ideal H<GIndHGRkH in terms of modules which are easier to describe by polynomials in the χi.

2.3 Change of basis

Our new basis for RkG shall use the language of quantum numbers and cousins. Observe, from Proposition 5, that tensoring with V2 satisfies a similar relation to the quantum numbers.

Lemma 12.

For r < p, Vr·V2=Vr+1+Vr1.

Moreover,

Lemma 13.

For 0k and a{0,1,,p1}, (2) [a]χk[p]χk1[p]χk2[p]χ0=Vapk.(2)

Proof.

The case a = 0 is trivial. By Lemma 12, for r < p, we know that χ0·Vr=V2·Vr=Vr+1+Vr1. Since this are the defining relation for [r]χ0 the result is shown for k = 0. Equivalently it holds for k = 1 and a = 1. We now induct on k, with the key observation that, for 1ap and 1spk, (3) [a]χk·Vs=(V(a1)pk+sV(a1)pks)+(V(a3)pk+sV(a3)pks)++{Vpk+sVpksa evenVsa odd(3) from which the desired result follows by the substitution s=pk.

To prove EquationEq. (3) we induct on a. The base case of a = 1 is trivial, and the case a = 2 is covered by the first line of EquationEq. (1). Now, assuming EquationEq. (3) holds for a1<p, we can apply the second line of EquationEq. (1) to obtain [2]χk[a1]χk·Vs=(Vapk+s+V(a2)pk+sVapksV(a2)pks)+(V(a2)pk+s+V(a4)pk+sV(a2)pksV(a4)pks)++{V2pk+s+VsVsa evenVpk+sVpksa odd

from which we can subtract [a2]χk·Vs to obtain EquationEq. (3). □

This relationship motivates defining a new basis.

Definition 14.

Let r<q=pα and write r1=i=0α1ripi with ri{0,1,,p1}. Set Ur:=i=0α1[ri+1]χi.

Of course, each UjRkG can be written in terms of the indecomposable modules Vi using repeated applications of Theorem 9 and Proposition 5. The largest indecomposable appearing in this expression for Ur comes from the term i=0α1χiri. This largest module appearing in this term corresponds to the largest term in i=0α1Vpi+1ri. Using the reduction theorem, Theorem 9, again we see that largest module appearing in our expression for Ur is Vr. In particular, the set {Uj:0<j<q} is a basis for RkG and the change-of-basis matrix is lower triangular (see ).

We have a ring homomorphism from RkG to Z simply by taking dimensions. As χi is the difference of the indecomposable modules Vpi+1 and Vpi1, this homomorphism sends χi to 2. In particular, the image of Ur under the dimension homomorphism can be realized by evaluating the polynomials at χi=2. As observed earlier, the quantum polynomials are such that [r]2=r, thus the “dimension” of Ur is i=0α1(ri+1).

Example 15.

Let p = 5, α = 3. We then have that U12=[1]χ2[3]χ1[2]χ0=(1)(χ121)(χ0)=(V11V9+1)·V2=V12V8+V2,where the third equality follows from the identity χ12=V2p+1+V2p1+2, and the final equality follows from Proposition 5, which shows V11·V2=V12+V10 and V9·V2=V10+V8. Observe that if p = 5 then U12=V12V8+V2 for any α2 as the factors [1]χi for i2 make no contribution. Observe that the image of U12 under the dimension map is 128+2=(1)·(3)·(2)=6.

In fact, we are able to give a closed form for the Vr in terms of the Uj. See for a visual representation of this proposition. In order to describe this change of basis, we will introduce a few number theoretic concepts.

Definition 16.

Let n=nkpk+nk1pk1++n0 be the p-adic expansion of n. We define the cousins of n as cous(n)={nkpk±nk1pk1±±n0},and for α>k, the α-anti-cousins of n as acousα(n)={j:pαncous(pαj)}.

Note that the cousins of n are at most n, and hence the anti-cousins of n are also at most n.

Now, if jpα, then cous(pα+1j)=cous((p1)pα+(pαj))=(p1)pα±cous(pαj).

Hence if pα+1rcous(pα+1j) then pαrcous(pαj). However, the reverse inclusion also holds, so in fact acousα+1(r)=acousα(r). Hence we may talk about the anti-cousins of r.

We can now state and prove the change of basis theorem.

Proposition 17.

We have that Vr=jacousrUj.

Proof.

We note that Uapk=Vapk by Lemma 13. Further acous(apk)=acousk+1(apk)={j:pk+1jcous((pa)pk)}={j:pk+1j{pk+1apk}}={apk}and thus the result holds for r=apk.

Now, suppose the equation holds for s < r, and write r=pβ+r for some β such that r<pβ+1. Note that we may permit r>pβ. In fact we will take two cases:

  1. Case rpβ: If r=0 or r=pβ we are done as r=pβ or r=2pβ which is handled above. Otherwise, by induction Vr can be written as a sum of Uj with j<r. Moreover we can write, using EquationEq. (1)

    Vr=χβ·Vr+Vpβr=jacous(r)χβUj+jacous(pβr)Uj=jacous(r)Upβ+j+jacous(pβr)Uj.

    Here we have used the fact that χβUj=[2]βUj=Upβ+j for all j<pβ. The result will follow given the claim that

    1. if r<pβ, then acous(r+pβ)=(acous(r)+pβ)acous(pβr)

  2. Case pβ<r(p1)pβ: If r=(p1)pβ then r=pβ+1 and we are done by the base case. Otherwise, again, using the second case of EquationEq. (1),

    Vr=χβ·VrVrpβ=jacous(r)(Upβ+j+Ujpβ)jacous(rpβ)Uj

    and again the claims bellow will show that most terms cancel and those that remain are what is desired:

    1. if pβ<r<(p1)pβ, then acous(r)pβ=acous(rpβ), and

    2. if pβ<r<(p1)pβ, then acous(r)+pβ=acous(r+pβ)=acous(r)

We thus need to show the three claims, which is an exercise in dealing with cousins and anti-cousins.

  1. Firstly note that the union is disjoint as the first set is larger than pβ and the second set is smaller. Then notice that

    jacous(pβr)rcous(pβj)pβ+1r(p1)pβ+cous(pβj)pβ+1rcous(pβ+1j)jacous(r),

    where we have used the fact that cous(pβ+1j)=cous((p1)pβ+(pβj)) which can be written as (p1)pβ±cous(pβj). If j<pβ then

    jacous(r)(p1)pβrcous((p1)pβ+(pβj))(p1)pβr(p1)pβcous(pβj)rcous(pβj)jacous(pβr),

    and we have shown that acous(r+pβ){0,1,,pβ}=acous(pβr).

    On the other hand, if

    jacous(r)+pβpβ+1+pβrcous(pβ+1+pβj)pβ+1+pβrcous((p1)pβ+(2pβj))pβ+1r(p2)pβ±cous(2pβj)pβ+1rcous(pβ+1j)jacous(r),

    and if pβ<j<2pβ then

    jacous(r)pβ+1pβrcous(pβ+1j)pβ+1pβrcous((p1)pβ(jpβ))(p1)pβr(p1)pβ±cous(jpβ)pβ+1rpβ+1±cous(jpβ)pβ+1rcous(pβ+1(pβj))jacous(r)+pβ.

  2. Suppose that j<(p2)pβ and write j=j0pβ+j1 for 0j1<pβ and hence 0<j0<p2. Then

    jacous(rpβ)pβ+1+pβrcous(pβ+1j)pβ+1+pβrcous((p1j0)pβ+(pβj1))pβ+1+pβr(p1j0)pβ±cous(pβj1)pβ+1r(p2j0)pβ±cous(pβj1)pβ+1rcous(pβ+1jpβ)jacous(r)pβ.

  3. Write j=j0pβ+j1 for 0j1<pβ and 0<j0<p1. Then

    jacous(r)+pβpβ+1+pβrcous(pβ+1+pβj)pβ+1+pβrcous((pj0)pβ+(pβj1))pβ+1+pβr(pj0)pβ±cous(pβj1)pβ+1r(pj01)pβ±cous(pβj1)pβ+1rcous(pβ+1j)jacous(r).

In particular, note that the Vr are multiplicity-free in the Uj. We can alternatively express Vr=Urα where we define Uri as below.

Definition 18.

Let r<q=pα and let βα. Write r=mpβ+j for j<pβ. Set Ur0=Ur and define Urβ={Umpβ+jβ1+Umpβjβ1p∤mUrβ1else.

Example 19.

For example, if p = 5 and α = 3 then V62=U623=U622 where U622=U621+U381=U62+U58+U38+U32.

Remark 20.

The aforementioned dimension map enables us to play a number theoretic game. Indeed, recall this map sends Vrr and Uj to some product of its digits plus one.

Thus select a prime p and natural number n. Compute all of the Uj appearing in Unβ for β such that pβ>n. Let all the appearing j be collected in a set J. Then for each such jJ, write out the p-adic digits of j – 1 as (j0,,jk). Finally, n=jJ(j0+1)(j1+1)(jk+1).

This is reminiscent of the “pick-a-number” trick played by schoolchildren. In fact, we may relax the condition that p is prime in Definition 18 and the trick still works, in particular we may use the usual base 10 expansion. In this situation, however, we lose the representation theoretic interpretation of this fact.

Example 19

(continued). Continuing from our example above where p = 5, α = 3, and n = 62 then J={62,58,38,32}.

We then write 621=2·52+2·51+1·50=2215581=2·52+1·51+2·50=2125381=1·52+2·51+2·50=1225321=1·52+1·51+1·50=1115.

Observe that 62=(3)(3)(2)+(3)(2)(3)+(2)(3)(3)+(2)(2)(2),as claimed.

The purpose of this basis, apart from Theorem 9, is that it allows us to write down the ideal of induced modules very simply.

Proposition 21.

The ideal of induced modules is principal. To be exact, H<GIndHGRkH=Uj:p|jZ=(Up).

Proof.

Let I=H<GIndHGRkH. Note Up=VpI and each Ump=U(m1)p+1·Up by definition. Hence Uj:p|jZ(Up)=(Vp)I=Vj:p|jZ

where the last equality is by Proposition 11. But these have the same rank and hence we have equality. □

We are thus able to give an explicit structure to the non-induced representation ring, analogous to Theorem 2.

Corollary 22.

The ring of non-induced representations of Cq over a field of characteristic p is isomorphic to Z[X0,,Xα1]([p]χ0,F1,,Fα1)and thus has rank φ(q).

3 General cyclic groups

In general a cyclic group is of the form G:=Cn=Cm×Cq, where q=pα and n=m·q with p∤m. Let k be an algebraically closed filed of characteristic p. It is well known that the representation ring RkCn is the tensor product of the representation rings RkCm and RkCq, so our task is to understand the ideal generated by induced representations. Subgroups of G are of the form H=H1×H2 where H1Cm and H2Cq. In particular, H1=Cm for some m|m and H2=Cpβ for some βα. An indecomposable kH-module N is of the form N1kN2 where Ni is a kHi module. Inducing we get NHG=N1H1CmkN2H2Cq. In particular:

Proposition 23.

Let G be a cyclic group and k a field of characteristic p. Suppose G is of order n = mq, where q=pα and p∤m. Let {Vi:0<i<m} be the complete set of indecomposable kCm-modules and let {Vi:0<i<q} be the complete set of indecomposable kCq-modules. Then H<GIndHGRkH=VikVj:0<i<m,0<j<q,p|j or i|m,which is the ideal generated by H<CmIndHCmRkH and H<CqIndHCqRkH.

It follows then that:

Theorem 24.

Let G be a cyclic group of order n = mq, where q=pα and m∤p. The ring of non-induced representations is isomorphic to Z[Y](Φm(Y))ZZ[X0,,Xα1]([p]χ0,F1,,Fα1),or equivalently Z[X0,,Xα1,Y](Φm(Y),[p]χ0,F1,,Fα1).

In particular, rank(RkGH<GIndHGRkH)=φ(m)×φ(pα)=φ(n).

Note that the ranks of both the ring of non-induced representations and the ideal of induced representations are independent of the characteristic of the field, even though these sets may differ from field to field.

Acknowledgments

The authors are grateful to Dr. Stuart Martin for his guidance and support and to the reviewer for insightful and detailed comments on an earlier draft of this paper.

Additional information

Funding

The work of the first author was supported by the Woolf Fisher Trust and the Cambridge Commonwealth and International Trust. The work of the second author was supported by an EPSRC DTP Scholarship from the University of Cambridge.

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