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How large is the character degree sum compared to the character table sum for a finite group?

Arvind Ayyer Arvind Ayyer, Department of Mathematics, Indian Institute of Science, Bangalore 560012, India. [email protected] Hiranya Kishore Dey Hiranya Kishore Dey, Department of Mathematics, Indian Institute of Science, Bangalore 560012, India. [email protected]  and  Digjoy Paul Digjoy Paul, Department of Mathematics, Indian Institute of Science, Bangalore 560012, India. [email protected]
Abstract.

In 1961, Solomon gave upper and lower bounds for the sum of all the entries in the character table of a finite group in terms of elementary properties of the group. In a different direction, we consider the ratio of the character table sum to the sum of the entries in the first column, also known as the character degree sum, in this work. First, we propose that this ratio is at most two for many natural groups. Secondly, we extend a conjecture of Fields to postulate that this ratio is at least one with equality if and only if the group is abelian. We establish the validity of this property and conjecture for all finite irreducible Coxeter groups. In addition, we prove the conjecture for generalized symmetric groups. The main tool we use is that the sum of a column in the character table of an irreducible Coxeter group (resp. generalized symmetric group) is given by the number of square roots (resp. absolute square roots) of the corresponding conjugacy class representative.

As a byproduct of our results, we show that the asymptotics of character table sums is the same as the number of involutions in symmetric, hyperoctahedral and demihyperoctahedral groups. We also derive explicit generating functions for the character table sums for these latter groups as infinite products of continued fractions. In the same spirit, we prove similar generating function formulas for the number of square roots and absolute square roots in nn for the generalized symmetric groups G(r,1,n)G(r,1,n).

Key words and phrases:
finite group, irreducible Coxeter group, character table, symmetric group, hyperoctahedral group, demihyperoctahedral group, absolute square roots, generalized symmetric group, asymptotics, continued fractions
2010 Mathematics Subject Classification:
20C15, 05A15, 05A16, 05A17, 05E10

1. Introduction

For any finite group, it is natural to consider the sum of the entries of the character table. Solomon [Sol61] proved that this is always a nonnegative integer by proving something stronger, namely that all row sums are nonnegative integers. He did so by showing that the sum of the row indexed by an irreducible representation is the multiplicity of that representation in the conjugation representation of that group. He then deduced that the sum of the entries in the character table of a finite group is at most the cardinality of the group and at least the cardinality of a maximal abelian normal subgroup of the group. It was shown that the multiplicities in the regular and conjugacy representations for the symmetric group are close in a certain sense [Fru86, AF87, Roi97].

In this article, we take a different approach to estimating the sum of the entries of the character table by considering column sums instead. It is well known that the column sums are always integers, though not necessarily nonnegative [Isa06, Problem (5.13)]. Alternating groups are an example of a family of groups for which some column sums in the character table are negative. We do not know of a classification of groups for which all column sums are nonnegative integers. However, for groups whose irreducible characters are real, the column sums are given by the number of square roots of conjugacy class representatives by a classical result by Frobenius and Schur [Isa06]. This class of groups is called totally orthogonal (see Remark 2.5). Finite Coxeter groups are well-known examples of such groups. When r3r\geq 3, generalized symmetric groups G(r,1,n)G(r,1,n) are not totally orthogonal, though their column sums are nonnegative integers. This is because these column sums are given by the number of so-called absolute square roots [APR10].

For a finite group GG, let Irr(G)\mathrm{Irr}(G) denote the set of irreducible complex representations upto isomorphism, and Conj(G)\mathrm{Conj}(G) denote the set of conjugacy classes of GG. Let χV\chi_{V} denote the character associated with the representation VV and χV(C)\chi_{V}(C) be the value of the character χV\chi_{V} evaluated at an element of the conjugacy class CC. The character table of GG is a square matrix encoding character values, whose rows are indexed by Irr(G)\mathrm{Irr}(G) and columns are indexed by Conj(G)\mathrm{Conj}(G). Let s(G)s(G) denote the sum of all entries in the character table of GG. Let RVR_{V} (resp. ΓC\Gamma_{C}) be the sum of all the entries in the row (resp. column) of the character table indexed by VV (resp. CC). By convention, the first row is indexed by the trivial character and the first column is indexed by the singleton class containing the identity element ee of GG. Thus, the first column records the dimensions of corresponding irreducible representations and Γe(G)\Gamma_{e}(G) is their sum. It is a standard fact (for instance, see [Isa06, Lemma 2.15]) that Γe|ΓC|\Gamma_{e}\geq|\Gamma_{C}| for any group and any conjugacy class CC. We note that Γe\Gamma_{e} has been used to obtain structural properties of groups. Starting with the work of Magaard–Tong-Viet [MTV11], there is a large literature of works in that direction.

From extensive computations, we observe the following upper bound for the sum of the entries of the character table for many but not all groups.

Property S .

For a finite group GG, we have s(G)2Γe(G)s(G)\leq 2\Gamma_{e}(G).

We know that Property S will not hold in general, but it seems to hold for a large class of natural groups. We have looked at data for all groups of order up to 200200 using the SmallGroups Library in GAP. The first counterexamples occur at order 6464. See Section C.1 for the list of groups indexed according to GAP where Property S fails.

Fields [Fie75] provided two-sided bounds for the total sum in terms of the number (and orders of corresponding centralizers) of conjugacy classes, cardinality of the group and the first column sum. The first inequality in the following conjecture is due to him; see [Fie75, Remark 3 after Theorem 2]. We strengthen his conjecture to propose a characterization of when equality is attained.

Conjecture 1.1.

For all finite groups GG, we have s(G)Γe(G)s(G)\geq\Gamma_{e}(G). In addition, s(G)=Γe(G)s(G)=\Gamma_{e}(G) if and only if GG is abelian.

The equality holds for abelian groups; see Proposition 2.10. Note that the inequality in the conjecture follows immediately for all finite groups GG for which ΓC0\Gamma_{C}\geq 0 for all conjugacy classes CC in GG. Totally orthogonal groups and certain complex reflection groups (see Remark 6.8) are examples of such groups. We prove 1.1 for these groups in Proposition 2.6 and Theorem 6.9 respectively using explicit counting formulas for ΓC\Gamma_{C}. Using Solomon’s result, we also deduce that 1.1 holds for any finite group of nilpotency two; see Corollary 2.2. In addition, we have verified that 1.1 holds for all groups of order up to 200. See Section C.3 for the list of ratios of s(G)/Γe(G)s(G)/\Gamma_{e}(G) in increasing order.

Our main result is for finite irreducible Coxeter groups. Recall that Coxeter groups are abstract generalizations of reflection groups [Hum90]. Every finite Coxeter group is a direct product of finitely many irreducible Coxeter groups. Finite irreducible Coxeter groups consist of four one-parameter familes: symmetric groups SnS_{n} (type AA), hyperoctahedral groups BnB_{n} (type BB), demihyperoctahedral groups DnD_{n} (type DD) and dihedral groups Dih(n)\operatorname{Dih}(n) (type I2(n)I_{2}(n)). There are six more finite irreducible Coxeter groups of type E6,E7,E8,F4,H3,H4E_{6},E_{7},E_{8},F_{4},H_{3},H_{4}, which are called exceptional groups. It is well known that every Weyl group can be realized as a Coxeter group and they are Sn,Bn,Dn,E6,E7,E8,F4S_{n},B_{n},D_{n},E_{6},E_{7},E_{8},F_{4} and G2Dih(6)G_{2}\cong\operatorname{Dih}(6).

Theorem 1.2.

Property S holds for all finite irreducible Coxeter groups.

The irreducibility condition in the statement is necessary; see Proposition 2.9. The proof of Theorem 1.2 follows by a case analysis. In Section 2 we will sketch a proof of Theorem 1.2 for dihedral groups Dih(n)\operatorname{Dih}(n). We will prove Property S for the symmetric, hyperoctahedral and demihyperoctahedral groups in the later sections. By explicit computations, we have verified the result for exceptional irreducible finite Coxeter groups; see Appendix A. None of the counterexamples are simple groups and it is tempting to believe that Property S holds for all finite simple groups. We have not yet done a systematic study in that direction, but we certainly believe the following.

Conjecture 1.3.

Property S holds for all alternating groups.

The plan of the article is as follows. We first present results for general finite groups in Section 2. While proving Theorem 1.2 for the infinite one-parameter families of irreducible Coxeter groups, we also consider the sequence of character table sums for these families. In Section 3, we focus on SnS_{n}. We compute the generating function of the sequence of these character table sums for SnS_{n} in Section 3.1. In Section 3.2, we prove Theorem 1.2 for SnS_{n} and show that the sequence grows as fast as the character degree sum in SnS_{n}. We prove similar results for BnB_{n} in Section 4 and for DnD_{n} in Section 5. We extend the generating function results to G(r,1,n)G(r,1,n) in two ways in Section 6. We first give explicit product formulas for the generating functions for the sum of the number of square roots for conjugacy class representatives in Section 6.1. We then do the same for the number of absolute square roots (which are also column sums) in Section 6.2.

2. Character theory of finite groups

Any finite group GG has two natural representations afforded by the action of GG on itself. The first is the regular representation and is given by left multiplication gx=gxg\cdot x=gx. The second is the conjugation representation and is given by gx=gxg1g\cdot x=gxg^{-1}. The regular representation of a finite group is distinguished by the property that each irreducible representation appears within it with a multiplicity equal to its dimension. Solomon [Sol61] obtained the analogous decomposition for the conjugation representation.

Recall that a group GG is said to be nilpotent of class two if the derived subgroup [G,G][G,G] is contained in the center of GG.

Theorem 2.1 ([Sol61]).

The multiplicity of an irreducible representation VV of a finite group GG in the conjugation representation is the row sum RVR_{V}. Furthermore, if hh is the order of a maximal abelian normal subgroup of GG then hs(G)|G|h\leq s(G)\leq|G|. The equality s(G)=hs(G)=h holds if and only if GG is abelian and the equality s(G)=|G|s(G)=|G| holds if and only if GG is nilpotent of class two.

In particular, the row sums of the character table of a finite group are nonnegative integers. We note in passing that classifying groups for which all the row sums are positive (equivalently, every irreducible representation appears in its conjugation representation) is an active area of research. This class includes symmetric and alternating group as shown by Frumkin [Fru86] (also see [Sun18] for a modern treatment) and most of the finite simple groups of Lie type (see [HSTZ13]).

Corollary 2.2.

1.1 holds for any finite group of nilpotency class two.

Proof.

Suppose GG is nilpotent of class two. Then s(G)=|G|s(G)=|G|, by Theorem 2.1. Let d1,,drd_{1},\ldots,d_{r} be the character degrees of GG. Then, we have Γe(G)=i=1rdii=1rdi2=|G|\Gamma_{e}(G)=\sum^{r}_{i=1}d_{i}\leq\sum^{r}_{i=1}d_{i}^{2}=|G|. Since did_{i}’s are positive integers, the equality s(G)=Γe(G)s(G)=\Gamma_{e}(G) implies that di=1d_{i}=1 for all ii. Therefore, GG must be abelian. ∎

Given U,V,WIrr(G)U,V,W\in\mathrm{Irr}(G), let g(U,V,W)g(U,V,W) be the multiplicity of WW in the tensor product representation UVU\otimes V. In the case of the symmetric group SnS_{n}, where the irreducible representations U,V,WU,V,W are indexed by integer partitions λ,μ,ν\lambda,\mu,\nu of nn, the multiplicity g(U,V,W)g(U,V,W) is the so-called Kronecker coefficient g(λ,μ,ν)g(\lambda,\mu,\nu). Thus, we call g(U,V,W)g(U,V,W) as the generalized Kronecker coefficient.

Remark 2.3.

We have the following character identity due to Frame [Fra47] (later proved by Roth [Rot71, Theorem 1.2] using Solomon’s result):

χconj=UIrr(G)χUχU,\chi_{\text{conj}}=\sum_{U\in\mathrm{Irr}(G)}\chi_{U}\chi_{U^{*}},

where conj is the conjugation representation and UU^{*} is the dual representation of UU. Equating multiplicities of an irreducible character χV\chi_{V} in both sides of the above character identity, we obtain

RV=UIrr(G)g(U,U,V).R_{V}=\sum_{U\in\mathrm{Irr}(G)}g(U,U^{*},V).

Therefore, the sum of all entries in the character table of GG is U,VIrr(G)g(U,U,V)\sum_{U,V\in\mathrm{Irr}(G)}g(U,U^{*},V).

Using Galois theory, one can prove that the column sums of the character table are integers, and in general, these sums can be negative as well, see [Isa06, Problem (5.13)]. However, the following classical result gives a formula for the column sum for certain specific groups in terms of the square root function; see for instance [Isa06].

Given a finite group GG, the Frobenius–Schur index of an irreducible representation VV is defined by

σ(V):=1|G|gGχV(g2).\sigma(V):=\frac{1}{|G|}\sum_{g\in G}\chi_{V}(g^{2}).
Theorem 2.4 ([Isa06, Theorem 4.5]).

For a finite group GG, the following holds:

  1. (1)

    For each gGg\in G, we have

    |{xGx2=g}|=VIrr(G)σ(V)χV(g).|\{x\in G\mid x^{2}=g\}|=\sum_{V\in\mathrm{Irr}(G)}\sigma(V)\chi_{V}(g).
  2. (2)

    For VIrr(G)V\in\mathrm{Irr}(G), we have σ(V)=1,0\sigma(V)=1,0 or 1-1 if χV\chi_{V} is real-valued and VV is realizable over \mathbb{R} (in which case, we say VV is real), χV\chi_{V} is not real-valued (in which case, we say VV is complex), or χV\chi_{V} is real-valued but VV is not realizable over \mathbb{R} (in which case, we say VV is quaternionic), respectively.

Remark 2.5.

A group GG is called totally orthogonal if all its irreducible representations are real. All finite Coxeter groups are included in this class [Hum90, Section 8.10]. Applying Theorem 2.4 for such a group GG, we get

|{xGx2=g}|=VIrr(G)χV(g).|\{x\in G\mid x^{2}=g\}|=\sum_{V\in\mathrm{Irr}(G)}\chi_{V}(g).

Thus, column sums of the character table of totally orthogonal groups are given by the number of square roots of conjugacy class representatives.

Proposition 2.6.

Suppose GG is a finite group such that all column sums in its character table are nonnegative integers. Then

  1. (1)

    s(G)Γe(G)s(G)\geq\Gamma_{e}(G).

  2. (2)

    In addition, if GG is totally orthogonal, 1.1 holds for GG.

Proof.

The first part follows immediately as column sums are nonnegative. Let s(G)=Γe(G)s(G)=\Gamma_{e}(G). Then ΓC(G)=0\Gamma_{C}(G)=0 for any non-trivial conjugacy class CC. If GG is totally orthogonal, by Remark 2.5, we have g2=eg^{2}=e for all gGg\in G. This implies GG is abelian. ∎

Proposition 2.7.

For finite groups G1,G2G_{1},G_{2}, we have s(G1×G2)=s(G1)s(G2)s(G_{1}\times G_{2})=s(G_{1})s(G_{2}) and Γe(G1×G2)=Γe(G1)Γe(G2)\Gamma_{e}(G_{1}\times G_{2})=\Gamma_{e}(G_{1})\Gamma_{e}(G_{2}).

Proof.

The proof follows from the fact that Irr(G1×G2)={V1V2V1Irr(G1),V2Irr(G2)}\mathrm{Irr}(G_{1}\times G_{2})=\{V_{1}\otimes V_{2}\mid V_{1}\in\mathrm{Irr}(G_{1}),V_{2}\in\mathrm{Irr}(G_{2})\} and χV1V2=χV1χV2\chi_{V_{1}\otimes V_{2}}=\chi_{V_{1}}\chi_{V_{2}}. ∎

Corollary 2.8.

If 1.1 holds for G1G_{1} and G2G_{2}, then it holds for G1×G2G_{1}\times G_{2}.

Proposition 2.9.

For an integer m>1m>1, there exists a group GG for which s(G)>mΓe(G)s(G)>m\,\Gamma_{e}(G).

Proof.

Let nn be a positive integer such that 2n>m2^{n}>m. Let HH be any group satisfying s(H)=2Γe(H)s(H)=2\Gamma_{e}(H); a list of such groups up to order 200200 is given in Section C.2. Applying Proposition 2.7 we have s(Hn)=s(H)n=2nΓe(Hn)>mΓe(Hn)s(H^{n})=s(H)^{n}=2^{n}\Gamma_{e}(H^{n})>m\Gamma_{e}(H^{n}). This completes the proof. ∎

By Proposition 2.9, Property S does not also hold for all finite Coxeter groups.

For an abelian group HH, the orthogonality of rows in the character table of HH leads to the vanishing of row sums of all representations except the trivial one. So, we have the following result.

Proposition 2.10.

For an abelian group HH, we have s(H)=Γe(H)s(H)=\Gamma_{e}(H).

Corollary 2.11.

Suppose GG satisfies Property S and HH is an abelian group. Then G×HG\times H also satisfies Property S.

Proof.

As stated above, for an abelian group HH, we know s(H)=|H|=Γe(H)s(H)=|H|=\Gamma_{e}(H). Thus s(G×H)=s(G)s(H)2Γe(G)Γe(H)=2Γe(G×H)s(G\times H)=s(G)s(H)\leq 2\Gamma_{e}(G)\Gamma_{e}(H)=2\Gamma_{e}(G\times H). ∎

Proposition 2.12.

Let GG be a finite group such that all the irreducible characters of GG have degree at most 22. Then GG satisfies Property S.

Proof.

Suppose GG has rr irreducible characters and d1,d2,,drd_{1},d_{2},\dots,d_{r} are the degrees of the irreducible characters of GG. We know that i=1rdi2=|G|\sum_{i=1}^{r}d_{i}^{2}=|G|. Moreover, for each 1ir1\leq i\leq r, we have 1di21\leq d_{i}\leq 2. Therefore, for each 1ir1\leq i\leq r, we have di22did_{i}^{2}\leq 2d_{i}. Thus, we have

i=1rdi22i=1rdi.\sum_{i=1}^{r}d_{i}^{2}\leq 2\sum_{i=1}^{r}d_{i}.

By Theorem 2.1, we have

s(G)|G|2i=1rdi=2Γe(G).s(G)\leq|G|\leq 2\sum_{i=1}^{r}d_{i}=2\Gamma_{e}(G).

This completes the proof. ∎

A characterization of finite groups GG such that all the irreducible characters of GG have degree at most 22 is given in [Ami61].

Lemma 2.13 ([Ser77, p. 25]).

Let AA be an abelian subgroup of a finite group GG. Then each irreducible character of GG has degree |G|/|A|\leq|G|/|A|.

Let n/n\mathbb{Z}_{n}\equiv\mathbb{Z}/n\mathbb{Z} be the cyclic group of order nn. For a finite abelian group HH, the generalized dihedral group Dih(H)\operatorname{Dih}(H) is defined as the semidirect product of HH and 2\mathbb{Z}_{2}, where 2\mathbb{Z}_{2} acts on HH by inverting elements. Thus Dih(H):=2H\operatorname{Dih}(H):=\mathbb{Z}_{2}\ltimes H. The usual dihedral group is thus Dih(n)Dih(n)\operatorname{Dih}(n)\equiv\operatorname{Dih}(\mathbb{Z}_{n}) of order 2n2n. Recall that the standard presentation of Dih(n)\operatorname{Dih}(n) is r,srn=s2=1,srs=r1\langle r,s\mid r^{n}=s^{2}=1,srs=r^{-1}\rangle. The involutions of this group are precisely risrir^{i}sr^{-i} for i=0,1,n1i=0,1,\ldots n-1 for any nn and rn/2r^{n/2} in addition when nn is even. Since Dih(n)\operatorname{Dih}(n) is a finite Coxeter group, by Remark 2.5 the first column sum of its character table is n+1n+1 (resp. n+2n+2) when nn is odd (resp. even). But this sum is more than the sum of the remaining columns, which is at most n1n-1, proving Property S. We note that the character table sum of the dihedral group is given by [Slo, Sequence A085624]

{3n+12n odd,3n+22n2(mod4),3n+42n0(mod4).\begin{cases}\displaystyle\frac{3n+1}{2}&\text{$n$ odd},\\[5.69046pt] \displaystyle\frac{3n+2}{2}&\text{$n\equiv 2\pmod{4}$,}\\[5.69046pt] \displaystyle\frac{3n+4}{2}&\text{$n\equiv 0\pmod{4}$}.\end{cases}

Thus, the ratio s(Dih(n))/Γe(Dih(n))s(\operatorname{Dih}(n))/\Gamma_{e}(\operatorname{Dih}(n)) tends to 3/23/2 as nn tends to infinity.

Let HH be a finite abelian group of order 2n2n and assume tt is a unique element in HH of order 22. Let 4=y\mathbb{Z}_{4}=\langle y\rangle, and let yy act on HH by inverting elements. Then, the generalized quarternion group Q(H)Q(H) is defined as the quotient of the semi-direct product 4H\mathbb{Z}_{4}\ltimes H by the two element central subgroup {1,y2t}\{1,y^{2}t\}. Thus, Q(H):=4H/{1,y2t}Q(H):=\mathbb{Z}_{4}\ltimes H/{\{1,y^{2}t\}} has order 4n4n with the presentation,

Q(H)=H,yy4=1,yhy1=h1 for hH,y2t=1.Q(H)=\left<H,y\mid y^{4}=1,\textup{$yhy^{-1}=h^{-1}$ for $h\in H$},\ y^{2}t=1\right>.

Let H=4H=\mathbb{Z}_{4}, and take ±i\pm i to be the generators of HH and y=jy=j, t=1t=-1. Then Q(H)Q(H) is the usual quaternion group Q8={±1,±i,±j,±k}Q_{8}=\{\pm 1,\pm i,\pm j,\pm k\}.

As an application of Lemma 2.13 and Proposition 2.12, we have the following:

Corollary 2.14.

Let HH be a finite abelian group. Then the generalized dihedral group Dih(H)\operatorname{Dih}(H) satisfies Property S. In addition, if HH has even order, the generalized quaternion group Q(H)Q(H) satisfies Property S.

3. Symmetric groups

Let SnS_{n} be the symmetric group on nn letters. The set of irreducible representations and the conjugacy classes of SnS_{n} are indexed by set of integer partitions λ=(λ1λ2λn)\lambda=(\lambda_{1}\geq\lambda_{2}\geq\cdots\geq\lambda_{n}) of nn, denoted λn\lambda\vdash n. Write a partition in frequency notation as

(1) λ=1m1,,nmn,\lambda=\langle 1^{m_{1}},\dots,n^{m_{n}}\rangle,

here mimi(λ)m_{i}\equiv m_{i}(\lambda) denote the number of parts of length ii in λ\lambda. We are interested in sns_{n}, the sum of the entries of the character table of SnS_{n}. The first twelve terms of the sequence (sn)(s_{n}) for n1n\geq 1 are given by [Slo, Sequence A082733]

1,2,5,13,31,89,259,842,2810,10020,37266,145373.1,2,5,13,31,89,259,842,2810,10020,37266,145373.

No formula is given for this sequence as of this writing. Fix a representative of cycle type λ\lambda by

wλ=(1,2,,λ1)(λ1+1,λ1+2,,λ1+λ2).w_{\lambda}=(1,2,\ldots,\lambda_{1})(\lambda_{1}+1,\lambda_{1}+2,\ldots,\lambda_{1}+\lambda_{2})\cdots.

Let Γλ\Gamma_{\lambda} be the sum of entries of the column indexed by λ\lambda. By Theorem 2.4 we have

(2) Γλ=μnχμ(wλ)=|{xSnx2=wλ}|,\Gamma_{\lambda}=\sum_{\mu\vdash n}\chi_{\mu}(w_{\lambda})=|\{x\in S_{n}\mid x^{2}=w_{\lambda}\}|,

where χμ\chi_{\mu} is the character of the irreducible representation VμV_{\mu} of SnS_{n} associated to μ\mu. In particular, we have in=μndimVμi_{n}=\sum_{\mu\vdash n}\dim V_{\mu}, where ini_{n} is the number of involutions in SnS_{n}.

Remark 3.1.
  1. (1)

    Notice that the function T:SnT:S_{n}\longrightarrow\mathbb{Z} defined by T(w)=|{xSnx2=w}|T(w)=|\{x\in S_{n}\mid x^{2}=w\}| is a character of SnS_{n} and T=μnχμT=\sum_{\mu\vdash n}\chi_{\mu} by (2). One can lift this character identity to the ring of symmetric polynomials via the Frobenius characteristic map. More details can be found in [Sta01, Exercise 7.69].

  2. (2)

    Adin–Postnikov–Roichman [APR08]construct a representation VnV_{n}, based on the involutions in SnS_{n}, whose character χVn=T\chi_{V_{n}}=T, thus proving VnλnVλV_{n}\cong\underset{\lambda\vdash n}{\oplus}V_{\lambda} is a Gelfand model. With this notation, Property S for SnS_{n} is equivalent to

    χVn(e)μnμ(n)χVn(wμ).\chi_{V_{n}}(e)\geq\sum_{\begin{subarray}{c}\mu\vdash n\\ \mu\neq(n)\end{subarray}}\chi_{V_{n}}(w_{\mu}).

Recall that the double factorial of an integer nn is given by n!!=n(n2)n!!=n(n-2)\cdots ending at either 2 or 1 depending on whether nn is even or odd respectively. Define

(3) or(n)=k=0n/2(n2k)(2k1)!!rk.o_{r}(n)=\sum_{k=0}^{\lfloor n/2\rfloor}\binom{n}{2k}(2k-1)!!\,r^{k}.

The following result is present in [APR08], but we give an independent proof.

Proposition 3.2 ([APR08, Corollary 3.2]).

Suppose λn\lambda\vdash n as written in (1). Then the column sum Γλ\Gamma_{\lambda} is 0 unless m2im_{2i} is even for all i{1,,n/2}i\in\{1,\dots,\lfloor n/2\rfloor\}. If that is the case,

Γλ=i=1n/2(m2i1)!!(2i)m2i/2j=0(n1)/2o2j+1(m2j+1).\Gamma_{\lambda}=\prod_{i=1}^{\lfloor n/2\rfloor}(m_{2i}-1)!!\,(2i)^{m_{2i}/2}\prod_{j=0}^{\lfloor(n-1)/2\rfloor}o_{2j+1}(m_{2j+1}).
Proof.

Suppose we write μn\mu\vdash n in frequency notation given by μ=1p1,,npn\mu=\langle 1^{p_{1}},\dots,n^{p_{n}}\rangle, and let πSn\pi\in S_{n} be a permutation with cycle type μ\mu. Observe that when we square π\pi, even cycles will split into two cycles of half their length and odd cycles will remain odd cycles of the same length. Therefore π2\pi^{2} has cycle type

1p1+2p2,22p4,3p3+2p6,42p8,.\langle 1^{p_{1}+2p_{2}},2^{2p_{4}},3^{p_{3}+2p_{6}},4^{2p_{8}},\dots\rangle.

Therefore, a permutation with cycle type λ\lambda written as in (1) has a square root if and only if m2im_{2i} is even for all ii. Now, let us suppose this is the case. First note that cycles of different lengths do not interfere with each other in the sense that the number of square roots of cycles of different length can be computed independently.

We will look at odd and even cycles separately. First consider m2im_{2i} cycles of length 2i2i, where m2im_{2i} is even. Then the square root of a permutation with this cycle type will have m2i/2m_{2i}/2 cycles of length 4i4i, as argued above. This will involve pairing these (2i)(2i)-cycles. This can be done in (m2i1)!!(m_{2i}-1)!! ways. Further, for every pairing, the cycles can be joined in 2i2i ways. To see this, consider a single pair,

(s1,,s2i)and(t1,,t2i).(s_{1},\dots,s_{2i})\quad\text{and}\quad(t_{1},\dots,t_{2i}).

Then a square root merges these cycles with sjs_{j}’s and tjt_{j}’s being present alternately in that order. However, there is a freedom to choose the starting location of t1t_{1} relative to sis_{i}, and there are 2i2i choices. Since this choice is present for each pair, we get another factor of (2i)m2i/2(2i)^{m_{2i}/2}.

Now, consider mm2j+1m\equiv m_{2j+1} cycles of length 2j+12j+1 for j0j\geq 0. We can form square roots of a permutation with this cycle type in two ways. First, by taking the cycle individually, and second, by merging two such cycles as in the even case. Moreover, we have the freedom to choose as many pairs as we like. We can merge kk pairs by first choosing 2k2k cycles, combining them in (2k1)!!(2k-1)!! ways and then choosing the location for merging in 2j+12j+1 ways for each pair. Therefore, the total number of ways of forming square roots is

k=0m/2(m2k)(2k1)!!(2j+1)k.\sum_{k=0}^{m/2}\binom{m}{2k}(2k-1)!!\,(2j+1)^{k}.

Comparing this with (3), we see that this is exactly o2j+1(m)o_{2j+1}(m). Note that the case of j=0j=0 corresponds to involutions. This completes the proof. ∎

Bessenrodt–Olsson [BO04] proved the following conjecture of V. Jovovic [Slo, Sequence A085642].

Corollary 3.3 ([BO04]).

The number of columns in the character table of SnS_{n} that have sum zero is equal to the number of partitions of nn with at least one part congruent to 2(mod4)2\pmod{4}.

We sketch a proof of this conjecture because some of the ideas used here will be replicated later. Let Λ\Lambda be the set of all integer partitions and Λn\Lambda_{n} be the partitions of nn. Define the subsets

(4) Λn1:=\displaystyle\Lambda_{n}^{1}:= {λnm2i(λ) is even i} and\displaystyle\{\lambda\vdash n\mid m_{2i}(\lambda)\text{ is even }\forall i\}\quad\text{ and }
(5) Λn2:=\displaystyle\Lambda_{n}^{2}:= {λnm4i+2(λ)=0i},\displaystyle\{\lambda\vdash n\mid m_{4i+2}(\lambda)=0\,\forall i\},

of Λn\Lambda_{n}.

Proof.

The map f:Λn1Λn2f:\Lambda_{n}^{1}\to\Lambda_{n}^{2} given by

(6) 1m1,22m2,3m3,42m4,𝑓1m1,4m2,3m3,8m4,\langle 1^{m_{1}},2^{2m_{2}},3^{m_{3}},4^{2m_{4}},\dots\rangle\overset{f}{\mapsto}\langle 1^{m_{1}},4^{m_{2}},3^{m_{3}},8^{m_{4}},\dots\rangle

gives a bijection between the two sets. By Proposition 3.2, Λn1\Lambda_{n}^{1} indexes the columns of the character table of SnS_{n} with nonzero sum proving the result. ∎

Bessenrodt–Olsson [BO04] found the following result, which we will also generalize to other groups.

Proposition 3.4 ([BO04]).

The generating function for the number of columns of the character table of SnS_{n} with nonzero sum is

j=11(1q2j1)(1q4j).\prod_{j=1}^{\infty}\frac{1}{(1-q^{2j-1})(1-q^{4j})}.

3.1. Generating function for the total sum of the character table

We will first give some background on generating functions which are expressed as continued fractions. One of the original motivations for this theory is the fact that moments of many families of classical orthogonal polynomials have explicit combinatorial interpretations. For example, the nn’th moment of the nn’th Laguerre polynomial is n!n!. Therefore, it is natural to ask for combinatorial proofs of these results. The enumerative theory of continued fraction started with the influential work of Flajolet [Fla80]. Many results follow as special cases of the following two results. Let xx and ρn,τn\rho_{n},\tau_{n} for n0n\geq 0 be commuting indeterminates and let ρ=(ρn)n0\rho=(\rho_{n})_{n\geq 0} and τ=(τn)n0\tau=(\tau_{n})_{n\geq 0}. Then the Jacobi continued fraction, or J-fraction for short, is given by

(7) J(x;τ,ρ)=11τ0xρ0x21τ1xρ1x2.J(x;\tau,\rho)=\frac{1}{1-\tau_{0}x-\frac{\displaystyle\rho_{0}x^{2}}{\displaystyle 1-\tau_{1}x-\frac{\rho_{1}x^{2}}{\ddots}}}.

A special case of this is the Stieltjes continued fraction, or S-fraction for short, which is

(8) S(x;ρ)=11ρ0x1ρ1x2.S(x;\rho)=\frac{1}{1-\frac{\displaystyle\rho_{0}x}{\displaystyle 1-\frac{\displaystyle\rho_{1}x^{2}}{\ddots}}}.

Recall that a Motzkin path is a path in 2\mathbb{Z}^{2} using steps {(1,1),(1,0),(1,1)}\{(1,1),(1,0),(1,-1)\} starting from the origin, ending on the xx-axis and staying in the first quadrant throughout. Similarly, a Dyck path satisfies the same conditions as above, except that the set of steps is {(1,1),(1,1)}\{(1,1),(1,-1)\}. Consider weighted Motzkin paths where northeast steps (1,1)(1,1) get weight ρi\rho_{i} if they start at row ii and east steps (1,0)(1,0) get weight τi\tau_{i} if they stay at row ii. Similarly, steps in weighted Dyck paths get weight ρi\rho_{i} as above. Define the weight of a path to be the product of its step weights times xx raised to its length.

Theorem 3.5 ([Fla80, Theorem 1]).
  1. (1)

    The generating function for weighted Motzkin paths is the J-fraction J(x;τ,ρ)J(x;\tau,\rho).

  2. (2)

    The generating function for weighted Dyck paths is the S-fraction S(x;ρ)S(x;\rho).

See Goulden–Jackson [GJ83, Chapter 5] and Viennot [Vie85] for many applications of these results.

Recall that sns_{n} denote the sum of the entries of the character table of SnS_{n}. Let 𝒮(x)\mathcal{S}(x) be the (ordinary) generating function of the sequence (sn)(s_{n}), i.e.

(9) 𝒮(x)=n0snxn.\mathcal{S}(x)=\sum_{n\geq 0}s_{n}x^{n}.

To give a formula for 𝒮(x)\mathcal{S}(x), we will need the following generating functions. Recall that an involution in SnS_{n} is a permutation ww which squares to the identity. Let ini_{n} be the number of involutions in SnS_{n}. A special case of the above result, also due to Flajolet [Fla80, Theorem 2(iia)] gives a continued fraction expansion of the generating function (x)\mathcal{I}(x) of involutions in SnS_{n} as the J-fraction

(10) (x)=n0inxn=J(x;(1),(n+1))=11xx21x2x2.\mathcal{I}(x)=\sum_{n\geq 0}i_{n}x^{n}=J(x;(1),(n+1))=\frac{1}{\displaystyle 1-x-\frac{x^{2}}{\displaystyle 1-x-\frac{2x^{2}}{\ddots}}}.

Flajolet also showed in the same theorem [Fla80, Theorem 2(iib)] that the generating function of odd double factorials is the S-fraction,

(11) 𝒟(x)=n0(2n1)!!xn=S(x;(n+1))=11x12x.\mathcal{D}(x)=\sum_{n\geq 0}(2n-1)!!\,x^{n}=S(x;(n+1))=\frac{1}{\displaystyle 1-\frac{x}{\displaystyle 1-\frac{2x}{\ddots}}}.

The quantity or(n)o_{r}(n) (defined in Equation 3) and its generalizations have been studied in [LnMRM12]. Setting t=0,n=0t=0,n=0 and u1=1u_{1}=1 in the same theorem  [Fla80, Theorem 2] we obtain the generating function for or(n)o_{r}(n) as the J-fraction

(12) r(x)=n0or(n)xn=J(x;(1),(r(n+1)))=11xrx21x2rx2.\mathcal{R}_{r}(x)=\sum_{n\geq 0}o_{r}(n)x^{n}=J(x;(1),(r(n+1)))=\frac{1}{\displaystyle 1-x-\frac{rx^{2}}{\displaystyle 1-x-\frac{2rx^{2}}{\ddots}}}.

Let x,x1,x2,x,x_{1},x_{2},\ldots be a family of commuting indeterminates. The following result answers a question of Amdeberhan [Amd].

Theorem 3.6.

The number of square roots of a permutation with cycle type λ\lambda written in frequency notation as in (1), which we denoted Γλ\Gamma_{\lambda}, is the coefficient of x1m1x2m2xnmnx_{1}^{m_{1}}x_{2}^{m_{2}}\dots x_{n}^{m_{n}} in

i1𝒟(2ix2i2)2i1(x2i1).\prod_{i\geq 1}\mathcal{D}(2ix_{2i}^{2})\mathcal{R}_{2i-1}(x_{2i-1}).

Consequently, the generating function of the character table sum is

𝒮(x)=i1𝒟(2ix4i)2i1(x2i1).\mathcal{S}(x)=\prod_{i\geq 1}\mathcal{D}(2ix^{4i})\mathcal{R}_{2i-1}(x^{2i-1}).
Proof.

By Proposition 3.2, the multiplicities of even parts must be even. Therefore, we write λ\lambda as λ=1m1,22m2,3m3,42m4,\lambda=\langle 1^{m_{1}},2^{2m_{2}},3^{m_{3}},4^{2m_{4}},\dots\rangle. Thus

λΓλx1m1x22m2=m1=0m2=0i=1(2m2i1)!!(2i)m2ix2i2m2ij=0o2j+1(m2j+1)x2j+1m2j+1=(m1=0o1(m1)x1m1)(m2=0(2m21)!!2m2x22m2).\sum_{\lambda}\Gamma_{\lambda}x_{1}^{m_{1}}x_{2}^{2m_{2}}\dots=\sum_{m_{1}=0}^{\infty}\sum_{m_{2}=0}^{\infty}\cdots\prod_{i=1}^{\infty}(2m_{2i}-1)!!\,(2i)^{m_{2i}}x_{2i}^{2m_{2i}}\prod_{j=0}^{\infty}o_{2j+1}(m_{2j+1})x_{2j+1}^{m_{2j+1}}\\ =\left(\sum_{m_{1}=0}^{\infty}o_{1}(m_{1})x_{1}^{m_{1}}\right)\left(\sum_{m_{2}=0}^{\infty}(2m_{2}-1)!!2^{m_{2}}x_{2}^{2m_{2}}\right)\cdots.

We then use (11) and (12) to prove the first statement. Now replace xix_{i} by xix^{i}, where xx is an indeterminate. Then the coefficient of xnx_{n} is precisely the sum of columns in the character table of SnS_{n}. ∎

3.2. Proof of Property S

The sequence (in)(i_{n}) satisfies the well-known recurrence relation for n2n\geq 2 given by

(13) in=in1+(n1)in2,i_{n}=i_{n-1}+(n-1)i_{n-2},

with i0=i1=1i_{0}=i_{1}=1.

Lemma 3.7.

For n2n\geq 2, we have 2in1innin12i_{n-1}\leq i_{n}\leq n\ i_{n-1}.

Proof.

Since i1=1i_{1}=1, i2=2i_{2}=2 and i3=4i_{3}=4, the inequalities are valid for n=2,3n=2,3. For n4n\geq 4, we have innin12in1i_{n}\geq\sqrt{n}i_{n-1}\geq 2i_{n-1}, where the first inequality follows from [CHM51, Lemma 2] and the second is obvious. We prove the other inequality by induction on nn. This inequality is valid for n=3n=3, as mentioned above. Using (13), we have by the induction hypothesis,

in\displaystyle i_{n} (n1)in2+(n1)in2\displaystyle\leq(n-1)i_{n-2}+(n-1)i_{n-2}
=2(n1)in2(n1)in1nin1,\displaystyle=2(n-1)i_{n-2}\leq(n-1)i_{n-1}\leq ni_{n-1},

where the second line uses the first part of the statement. This completes the proof. ∎

Recall that derangements are permutations without fixed points. We define another sequence (gn)(g_{n}) by

gn:=λnm1(λ)=0Γλ,n1andg0=1.g_{n}:=\sum_{\begin{subarray}{c}\lambda\vdash n\\ m_{1}(\lambda)=0\end{subarray}}\Gamma_{\lambda},\quad n\geq 1\quad\text{and}\quad g_{0}=1.

Then gng_{n} counts the sum of those columns of the character table of SnS_{n} which are indexed by the conjugacy classes corresponding to derangements.

Lemma 3.8.

For n4n\geq 4, we have ikgnkin1/(n2)i_{k}g_{n-k}\leq{i_{n-1}}/(n-2) for all 0kn3.0\leq k\leq n-3.

Proof.

We use induction on nn. The statement holds for n=4n=4, as we can verify using i3=4,i2=2,i1=1,i0=1,g3=1,g2=0,g1=0,g0=0i_{3}=4,i_{2}=2,i_{1}=1,i_{0}=1,g_{3}=1,g_{2}=0,g_{1}=0,g_{0}=0. We assume the statement to be true for nn and prove this for n+1n+1. When k=n2k=n-2, we have in2g3=in2in/(n1)i_{n-2}g_{3}=i_{n-2}\leq i_{n}/(n-1) by (13). For kn3k\leq n-3, by using (13), the left hand side becomes

ikgn+1k=(ik1+(k1)ik2)gn(k1)=ik1gn(k1)+(k1)ik2gn1(k2).i_{k}g_{n+1-k}=(i_{k-1}+(k-1)i_{k-2}\big{)}g_{n-(k-1)}=i_{k-1}g_{n-(k-1)}+(k-1)i_{k-2}g_{n-1-(k-2)}.

By induction, we have

ikgn+1kin1n2+k1n3in2.i_{k}g_{n+1-k}\leq\frac{i_{n-1}}{n-2}+\frac{k-1}{n-3}i_{n-2}.

By Lemma 3.7, we have in1(n1)in2i_{n-1}\leq(n-1)i_{n-2}, we so we get

(n3)in1(n2)(n1)in2(n2)(n1)((n3)(k1))in2,(n-3)i_{n-1}\leq(n-2)(n-1)i_{n-2}\leq(n-2)(n-1)\big{(}(n-3)-(k-1)\big{)}i_{n-2},

where the last inequality follows as (n3)(k1)1(n-3)-(k-1)\geq 1. We can rewrite this inequality as

(n3)in1+(k1)(n1)(n2)in2(n1)(n2)(n3)in2.(n-3)i_{n-1}+(k-1)(n-1)(n-2)i_{n-2}\leq(n-1)(n-2)(n-3)i_{n-2}.

This implies, by adding (n3)(n2)in1(n-3)(n-2)i_{n-1} to both sides, that

(n3)(n1)in1+(k1)(n1)(n2)in2(n1)(n2)(n3)in2+(n3)(n2)in1.(n-3)(n-1)i_{n-1}+(k-1)(n-1)(n-2)i_{n-2}\leq(n-1)(n-2)(n-3)i_{n-2}+(n-3)(n-2)i_{n-1}.

Now, divide each term by (n1)(n2)(n3)(n-1)(n-2)(n-3) to obtain

(14) in1n2+k1n3in2in2+1n1in1=inn1.\frac{i_{n-1}}{n-2}+\frac{k-1}{n-3}i_{n-2}\leq i_{n-2}+\frac{1}{n-1}i_{n-1}=\frac{i_{n}}{n-1}.

This completes the proof. ∎

The next result is a convolution-type statement involving sn,gns_{n},g_{n} and ini_{n}.

Proposition 3.9.

For a positive integer nn, we have

sn=k=0nikgnk.s_{n}=\sum_{k=0}^{n}i_{k}g_{n-k}.
Proof.

We have

sn=λnΓλ=k=0nλnm1(λ)=kΓλ.s_{n}=\sum_{\lambda\vdash n}\Gamma_{\lambda}=\sum_{k=0}^{n}\sum_{\begin{subarray}{c}\lambda\vdash n\\ m_{1}(\lambda)=k\end{subarray}}\Gamma_{\lambda}.

Given a partition λ=1k,2m2,,nmn\lambda=\langle 1^{k},2^{m_{2}},\dots,n^{m_{n}}\rangle, let ν=2m2,,nmn\nu=\langle 2^{m_{2}},\dots,n^{m_{n}}\rangle, so that λ=1kν\lambda=\langle 1^{k}\rangle\cup\nu. Recall that wλw_{\lambda} is a permutation with cycle type λ\lambda. Then observe that

{xSnx2=wλ}={ySky2=e}×{zS{k+1,,n}z2=wν},\{x\in S_{n}\mid x^{2}=w_{\lambda}\}=\{y\in S_{k}\mid y^{2}=e\}\times\{z\in S_{\{k+1,\ldots,n\}}\mid z^{2}=w_{\nu}\},

where S{k+1,,n}S_{\{k+1,\dots,n\}} denotes the group of bijections on the set {k+1,,n}\{k+1,\dots,n\}. Finally,

k=0nλnm1(λ)=kΓλ=k=0nikνnkm1(ν)=0Γν=k=0nikgnk.\sum_{k=0}^{n}\sum_{\begin{subarray}{c}\lambda\vdash n\\ m_{1}(\lambda)=k\end{subarray}}\Gamma_{\lambda}=\sum_{k=0}^{n}i_{k}\sum_{\begin{subarray}{c}\nu\vdash n-k\\ m_{1}(\nu)=0\end{subarray}}\Gamma_{\nu}=\sum_{k=0}^{n}i_{k}g_{n-k}.

This completes the proof. ∎

Theorem 3.10.

Property S holds for all symmetric groups.

Proof.

It is easy to check the property for S1,S2S_{1},S_{2} and S3S_{3}. We shall prove a more stronger result, namely for n4n\geq 4,

(15) snin+in1.s_{n}\leq i_{n}+i_{n-1}.

By Proposition 3.9, we have

sn=k=0nikgnk=k=0n3ikgnk+in2g2+in1g1+in.s_{n}=\sum_{k=0}^{n}i_{k}g_{n-k}=\sum_{k=0}^{n-3}i_{k}g_{n-k}+i_{n-2}g_{2}+i_{n-1}g_{1}+i_{n}.

Using Lemma 3.8 and the fact that g0=1,g1=g2=0g_{0}=1,g_{1}=g_{2}=0, we get

sn(n2)in1n2+in=in1+in.s_{n}\leq(n-2)\frac{i_{n-1}}{n-2}+i_{n}=i_{n-1}+i_{n}.

Thus, sn2ins_{n}\leq 2i_{n} as in1ini_{n-1}\leq i_{n}. This completes the proof. ∎

We now confirm the observation of user Lucia [Amd].

Corollary 3.11.

The total sum sequence (sn)(s_{n}) grows asymptotically as fast as (in)(i_{n}) and hence

sn(ne)n/2en1/42.s_{n}\sim\left(\frac{n}{e}\right)^{n/2}\frac{e^{\sqrt{n}-1/4}}{\sqrt{2}}.
Proof.

By [CHM51, Lemma 2], we have

in1in1n.\frac{i_{n-1}}{i_{n}}\leq\frac{1}{\sqrt{n}}.

Therefore, from the proof of Theorem 3.10, we have

1snin1+in1in1+1n.1\leq\frac{s_{n}}{i_{n}}\leq 1+\frac{i_{n-1}}{i_{n}}\leq 1+\frac{1}{\sqrt{n}}.

Now, both the sequences (1)(1) and (1+1/n)(1+1/\sqrt{n}) converges to 11. Hence, by the sandwich theorem, the sequence sn/ins_{n}/i_{n} converges to 11. Thus, the sequence (sn)(s_{n}) grows asymptotically as fast as the sequence (in)(i_{n}). The asymptotics of (in)(i_{n}) is derived by Chowla–Herstein–Moore [CHM51, Theorem 8] and is stated above. This completes the proof. ∎

4. Weyl groups of type B

Regard S2nS_{2n} as the group of permutations of the set {±1,,±n}\{\pm 1,\ldots,\pm n\}. For an integer n1n\geq 1, the group BnB_{n} is defined as

Bn:={wS2nw(i)+w(i)=0, for all i, 1in}.B_{n}:=\{w\in S_{2n}\,\mid\,w(i)+w(-i)=0,\text{ for all }i,\,1\leq i\leq n\}.

The group BnB_{n} is known as the hyperoctahedral group or the group of signed permutations.

Remark 4.1.

Instead of treating BnB_{n} as a subgroup of S2nS_{2n}, one can also define it as the wreath product, Bn=2SnB_{n}=\mathbb{Z}_{2}\wr S_{n}. In Section 6, we will describe our results for wreath products rSn\mathbb{Z}_{r}\wr S_{n}, where r1r\in\mathbb{N}_{\geq 1}. Here we have stated the results in the standard terminology for BnB_{n} for the benefit of the reader.

The following facts can be found in the book by Musili [Mus93]. Every element wBnw\in B_{n} can be uniquely expressed as a product of cycles

w=u1u¯1uru¯rv1vs,w=u_{1}\overline{u}_{1}\cdots u_{r}\overline{u}_{r}v_{1}\cdots v_{s},

where for 1jr1\leq j\leq r, uju¯j=(a1,,aλj)(a1,,aλj)u_{j}\overline{u}_{j}=(a_{1},\ldots,a_{\lambda_{j}})(-a_{1},\ldots,-a_{\lambda_{j}}) for some positive integer λj\lambda_{j} and for 1ks1\leq k\leq s, vk=(b1,,bμk,b1,,bμk)v_{k}=(b_{1},\ldots,b_{\mu_{k}},-b_{1},\ldots,-b_{\mu_{k}}) for some positive integer μk\mu_{k}. The element uju¯ju_{j}\overline{u}_{j} is called a positive cycle of length λj\lambda_{j} and vkv_{k} is called a negative cycle of length μk\mu_{k}. This cycle decomposition of ww determines a unique pair of partitions (λμ)(\lambda\mid\mu), where λ=(λ1,,λr)\lambda=(\lambda_{1},\ldots,\lambda_{r}), μ=(μ1,,μs)\mu=(\mu_{1},\ldots,\mu_{s}) and |λ|+|μ|=n|\lambda|+|\mu|=n. The pair (λμ)(\lambda\mid\mu), also known as a bipartition, is the cycle type of ww. We write (λμ)n(\lambda\mid\mu)\models n for such a bipartition of nn.

Theorem 4.2 ([Mus93, Theorem 7.2.5]).

The set of conjugacy classes of BnB_{n} is in natural bijection with the set of bipartitions (λμ)n(\lambda\mid\mu)\models n.

Let Γ(λμ)B\Gamma^{B}_{(\lambda\mid\mu)} be the column sum corresponding to the conjugacy class (λμ)n(\lambda\mid\mu)\models n in the character table of BnB_{n}. By Theorem 2.4, Γ(λμ)B\Gamma^{B}_{(\lambda\mid\mu)} is the number of square roots of an element of cycle type (λμ)(\lambda\mid\mu).

4.1. Generating functions

The following results follow immediately from an analysis of the cycle type of a signed permutation.

Lemma 4.3.
  1. (1)

    The square of a positive or negative cycle of odd length is a positive cycle of the same length.

  2. (2)

    The square of an even positive (resp. negative) cycle is a product of two positive (resp. negative) cycles of half that length.

Proposition 4.4.

The bipartition (λμ)n(\lambda\mid\mu)\models n is the cycle type of a square element of BnB_{n} if and only if each even part of λ\lambda has even multiplicity and each part of μ\mu has even multiplicity.

We now extend the results in Corollary 3.3 and Proposition 3.4 to BnB_{n}.

Corollary 4.5.

The number of columns of the character table of BnB_{n} that have zero sum (i.e. the number of bipartitions (λμ)(\lambda\mid\mu) such that Γ(λμ)B=0\Gamma^{B}_{(\lambda\mid\mu)}=0) is the same as the number of bipartitions (λμ)(\lambda\mid\mu) of nn such that at least one part of λ\lambda is congruent to 2(mod4)2\pmod{4} or μ\mu has at least one odd part.

The next result is a special case of Theorem 6.12.

Theorem 4.6.

The generating function for the number of columns in the character table of BnB_{n} with nonzero sum is

j=11(1q2j1)(1q2j)(1q4j).\prod_{j=1}^{\infty}\frac{1}{(1-q^{2j-1})(1-q^{2j})(1-q^{4j})}.

Let snBs_{n}^{B} be the sum of the entries of the character table of BnB_{n}. Let 𝒮B(x)\mathcal{S}^{B}(x) be the ordinary generating function of (snB)(s_{n}^{B}). Recall the functions 𝒟(x)\mathcal{D}(x) from (11) and r(x)\mathcal{R}_{r}(x) from (12). Let {x1,x2,,y1,y2,}\{x_{1},x_{2},\dots,y_{1},y_{2},\dots\} be a doubly infinite family of commuting indeterminates. The following result is a special case of both Theorem 6.6 and Theorem 6.15.

Theorem 4.7.

Write each partition in the bipartition (λμ)n(\lambda\mid\mu)\models n in frequency notation, with λ=1m1,2m2,,nmn\lambda=\langle 1^{m_{1}},2^{m_{2}},\dots,\allowbreak n^{m_{n}}\rangle and μ=1p1,2p2,,npn\mu=\langle 1^{p_{1}},2^{p_{2}},\dots,n^{p_{n}}\rangle. Then Γ(λμ)B\Gamma^{B}_{(\lambda\mid\mu)} is the coefficient of (x1m1xnmn)(y1p1ynpn)(x_{1}^{m_{1}}\dots x_{n}^{m_{n}})(y_{1}^{p_{1}}\dots y_{n}^{p_{n}}) in

k1(𝒟(4kx2k2)𝒟(4ky2k2)𝒟(2(2k1)y2k12)(2k1)2(2x2k1)).\displaystyle\prod_{k\geq 1}\Big{(}\displaystyle\mathcal{D}(4kx_{2k}^{2})\,\mathcal{D}(4ky_{2k}^{2})\mathcal{D}(2(2k-1)y_{2k-1}^{2})\,\mathcal{R}_{\frac{(2k-1)}{2}}(2x_{2k-1})\Big{)}.

Therefore,

𝒮B(x)=k1(𝒟(4kx4k)𝒟(2kx2k)(2k1)2(2x2k1)).\displaystyle\mathcal{S}^{B}(x)=\prod_{k\geq 1}\Big{(}\displaystyle\mathcal{D}(4kx^{4k})\,\mathcal{D}(2kx^{2k})\,\mathcal{R}_{\frac{(2k-1)}{2}}(2x^{2k-1})\Big{)}.

4.2. Proof of Property S

Let inBi_{n}^{B} be the number of involutions in BnB_{n}. The first nine terms of (inB)(i_{n}^{B}) are given by [Slo, Sequence A000898]

2,6,20,76,312,1384,6512,32400,168992.2,6,20,76,312,1384,6512,32400,168992.

The sequence (inB)(i_{n}^{B}) satisfies the recurrence relation [Cho06, Theorem 2.1]

(16) inB=2in1B+2(n1)in2B,n2,i_{n}^{B}=2i_{n-1}^{B}+2(n-1)i_{n-2}^{B},\quad n\geq 2,

with i0B=1i_{0}^{B}=1 and i1B=2i_{1}^{B}=2.

Lemma 4.8.

For positive integers nn, we have

2ninBin1B2n+2.\sqrt{2n}\leq\frac{i_{n}^{B}}{i_{n-1}^{B}}\leq\sqrt{2n}+2.
Proof.

The proof is by induction on nn. When n=1n=1, 2i1B/i0B=22+2\sqrt{2}\leq i_{1}^{B}/i_{0}^{B}=2\leq 2+\sqrt{2}. So, the result is correct. We assume the result for nn. Since in+1B=2inB+2nin1Bi_{n+1}^{B}=2i_{n}^{B}+2ni_{n-1}^{B} by (16), we have

in+1BinB=2+2ninB/in1B2+2n2n2+2(n+1).\frac{i_{n+1}^{B}}{i_{n}^{B}}=2+\frac{2n}{i_{n}^{B}/i_{n-1}^{B}}\leq 2+\frac{2n}{\sqrt{2n}}\leq 2+\sqrt{2(n+1)}.

On the other side, we have

in+1BinB=2+2ninB/in1B2+2n2n+22+(2n+2+2)(2n+22)2n+22n+2.\frac{i_{n+1}^{B}}{i_{n}^{B}}=2+\frac{2n}{i_{n}^{B}/i_{n-1}^{B}}\geq 2+\frac{2n}{\sqrt{2n}+2}\geq 2+\frac{(\sqrt{2n+2}+2)(\sqrt{2n+2}-2)}{\sqrt{2n}+2}\geq\sqrt{2n+2}.

This proves the inequality for n+1n+1 and completes the proof. ∎

Lemma 4.9.

For positive integers n5n\geq 5, we have 4in1BinBnin1B.4i_{n-1}^{B}\leq i_{n}^{B}\leq n\ i_{n-1}^{B}.

Proof.

We proceed by induction on nn. When n=5n=5, this can be verified. By using (16) repeatedly, we get

inB=2in1B+2(n1)in2B=2(2in2B+2(n2)in3B)+2(n1)in2B=(2n+2)in2B+(4n8)in3B.i_{n}^{B}=2i_{n-1}^{B}+2(n-1)i_{n-2}^{B}=2(2i_{n-2}^{B}+2(n-2)i_{n-3}^{B})+2(n-1)i_{n-2}^{B}=(2n+2)i_{n-2}^{B}+(4n-8)i_{n-3}^{B}.

Subsequently, we rewrite and use induction to get

inB=8in2B+(2n6)in2B+4(n2)in3B8in2B+4(2n6)in3B+4(n2)in3B.=8in2B+4(3n8)in3Bi_{n}^{B}=8i_{n-2}^{B}+(2n-6)i_{n-2}^{B}+4(n-2)i_{n-3}^{B}\\ \geq 8i_{n-2}^{B}+4(2n-6)i_{n-3}^{B}+4(n-2)i_{n-3}^{B}.=8i_{n-2}^{B}+4(3n-8)i_{n-3}^{B}

As n6n\geq 6, we finally have

inB8in2B+(8n8)in3B=4in1B.i_{n}^{B}\geq 8i_{n-2}^{B}+(8n-8)i_{n-3}^{B}=4i_{n-1}^{B}.

The proof of the other inequality directly follows by using Lemma 4.8 and observing that for n6n\geq 6, we have 2n+2n.\sqrt{2n}+2\leq n.

The first nine values of the sequence (snB)(s_{n}^{B}) are

2,8,26,112,410,1860,8074,40376,199050.2,8,26,112,410,1860,8074,40376,199050.

To find the asymptotics of snBs_{n}^{B}, we define

(17) gnB:=(λμ)nm1(λ)=0Γ(λμ)B.g_{n}^{B}:=\sum_{\begin{subarray}{c}(\lambda\mid\mu)\models n\\ m_{1}(\lambda)=0\end{subarray}}\Gamma^{B}_{(\lambda\mid\mu)}.
Lemma 4.10.

For positive integers n6n\geq 6, we have ikBgnkB2in1B/(n2)i_{k}^{B}g_{n-k}^{B}\leq 2i_{n-1}^{B}/(n-2) for all 0kn3.0\leq k\leq n-3.

Proof.

Here also, we proceed by induction on nn. When n=6n=6, we can verify that the statement holds. We assume the statement to be true for nn and prove this for n+1n+1. For kn3k\leq n-3, we have

ikBgn+1kB=(2ik1B+2(k1)ik2B)gn(k1)B=2ik1Bgn(k1)B+2(k1)ik2Bgn1(k2)B.i_{k}^{B}g_{n+1-k}^{B}=\big{(}2i_{k-1}^{B}+2(k-1)i_{k-2}^{B}\big{)}g_{n-(k-1)}^{B}=2i_{k-1}^{B}g_{n-(k-1)}^{B}+2(k-1)i_{k-2}^{B}g_{n-1-(k-2)}^{B}.

By the induction hypothesis, we now have

ikBgn+1kB4in1Bn2+(k1)4in2Bn3.i_{k}^{B}g_{n+1-k}^{B}\leq\frac{4i_{n-1}^{B}}{n-2}+(k-1)\frac{4i_{n-2}^{B}}{n-3}.

For positive integers nn, we have in1B(n1)in2Bi_{n-1}^{B}\leq(n-1)i_{n-2}^{B} by Lemma 4.9. So, we get

(n3)in1B(n2)(n1)in2B(n2)(n1)[(n3)(k1)]in2B,(n-3)i_{n-1}^{B}\leq(n-2)(n-1)i_{n-2}^{B}\leq(n-2)(n-1)[(n-3)-(k-1)]i_{n-2}^{B},

where the last inequality follows because (n3)(k1)1(n-3)-(k-1)\geq 1. We can rewrite it as

(n3)in1B+(k1)(n1)(n2)in2B(n1)(n2)(n3)in2B.(n-3)i_{n-1}^{B}+(k-1)(n-1)(n-2)i_{n-2}^{B}\leq(n-1)(n-2)(n-3)i_{n-2}^{B}.

This implies, by adding (n3)(n2)in1B(n-3)(n-2)i_{n-1}^{B} to both sides, that

(n3)(n1)in1B+(k1)(n1)(n2)in2B(n1)(n2)(n3)in2B+(n3)(n2)in1B.(n-3)(n-1)i_{n-1}^{B}+(k-1)(n-1)(n-2)i_{n-2}^{B}\leq(n-1)(n-2)(n-3)i_{n-2}^{B}+(n-3)(n-2)i_{n-1}^{B}.

Dividing each side by (n1)(n2)(n3)(n-1)(n-2)(n-3) and multiplying by 44, we get

4in1Bn2+(k1)4in2Bn34in1Bn1+4in2B.\frac{4i_{n-1}^{B}}{n-2}+(k-1)\frac{4i_{n-2}^{B}}{n-3}\leq\frac{4i_{n-1}^{B}}{n-1}+4i_{n-2}^{B}.

Therefore, we have by (16),

ikBgn+1kB2inBn1.i_{k}^{B}g_{n+1-k}^{B}\leq\frac{2i_{n}^{B}}{n-1}.

Thus for kn3k\leq n-3, our statement holds. When k=n2k=n-2, we have

in2Bgn+1(n2)B=in2Bg3B=2in2B2inBn1,i_{n-2}^{B}g_{n+1-(n-2)}^{B}=i_{n-2}^{B}g_{3}^{B}=2i_{n-2}^{B}\leq\frac{2i_{n}^{B}}{n-1},

completing the proof. ∎

Here, we have the following counterpart of Proposition 3.9.

Proposition 4.11.

For positive integers nn, we have

snB=k=0nikBgnkB.s_{n}^{B}=\sum_{k=0}^{n}i_{k}^{B}g_{n-k}^{B}.
Proof.

We have

(18) snB=(λμ)nΓ(λμ)B=k=0n(λμ)nm1(λ)=kΓ(λμ)B.s_{n}^{B}=\sum_{(\lambda\mid\mu)\models n}\Gamma^{B}_{(\lambda\mid\mu)}=\sum_{k=0}^{n}\sum_{\begin{subarray}{c}(\lambda\mid\mu)\models n\\ m_{1}(\lambda)=k\end{subarray}}\Gamma^{B}_{(\lambda\mid\mu)}.

Given λ=1k,2m2,,nmn\lambda=\langle 1^{k},2^{m_{2}},\dots,n^{m_{n}}\rangle, let ν=2m2,,nmn\nu=\langle 2^{m_{2}},\dots,n^{m_{n}}\rangle. Then we have (λμ)=(1k)(νμ)(\lambda\mid\mu)=(\langle 1^{k}\rangle\mid\emptyset)\cup(\nu\mid\mu). Let w(λμ)w_{(\lambda\mid\mu)} denote a signed permutation with cycle type (λμ)(\lambda\mid\mu). Let B{k+1,,n}B_{\{k+1,\dots,n\}} be the group of bijections ww on the set {±(k+1),,±n}\{\pm(k+1),\dots,\pm n\} such that w(i)+w(i)=0w(i)+w(-i)=0 for all k+1ink+1\leq i\leq n. Observe that

{xBnx2=w(λμ)}={yBky2=e}×{zB{k+1,,n}z2=w(νμ)}.\{x\in B_{n}\mid x^{2}=w_{(\lambda\mid\mu)}\}=\{y\in B_{k}\mid y^{2}=e\}\times\{z\in B_{\{k+1,\ldots,n\}}\mid z^{2}=w_{(\nu\mid\mu)}\}.

Therefore, Γ(λμ)B=Γ(1k)B×Γ(νμ)B\Gamma^{B}_{(\lambda\mid\mu)}=\Gamma^{B}_{(\langle 1^{k}\rangle\mid\emptyset)}\times\Gamma^{B}_{(\nu\mid\mu)}. Thus, the right hand side of (18) is reduced to

k=0nΓ(1k)B(νμ)nkm1(ν)=0Γ(νμ)B=k=0nikBgnkB.\sum_{k=0}^{n}\Gamma^{B}_{(\langle 1^{k}\rangle\mid\emptyset)}\sum_{\begin{subarray}{c}(\nu\mid\mu)\models n-k\\ m_{1}(\nu)=0\end{subarray}}\Gamma^{B}_{(\nu\mid\mu)}=\sum_{k=0}^{n}i_{k}^{B}g_{n-k}^{B}.

Theorem 4.12.

Property S holds for all hyperoctahedral groups BnB_{n}.

Proof.

For n5n\leq 5, this can be directly verified. For every positive integer n6n\geq 6, we shall prove the following:

(19) snBinB+2in1B+2in2B.s_{n}^{B}\leq i_{n}^{B}+2i_{n-1}^{B}+2i_{n-2}^{B}.

By Proposition 4.11, we have

snB=k=0nikBgnkB=inB+in1Bg1B+in2Bg2B+k=0n3ikBgnkBs_{n}^{B}=\sum_{k=0}^{n}i_{k}^{B}g_{n-k}^{B}=i_{n}^{B}+i_{n-1}^{B}g_{1}^{B}+i_{n-2}^{B}g_{2}^{B}+\sum_{k=0}^{n-3}i_{k}^{B}g_{n-k}^{B}

It is easy to see that g1B=0g_{1}^{B}=0 and g2B=2g_{2}^{B}=2. We now use Lemma 4.10 to get

snBinB+2in2B+(n2)2in1Bn2.s_{n}^{B}\leq i_{n}^{B}+2i_{n-2}^{B}+(n-2)\frac{2i_{n-1}^{B}}{n-2}.

By Lemma 4.9, the proof is now complete for n6n\geq 6. ∎

Corollary 4.13.

The total sum sequence (snB)(s_{n}^{B}) grows asymptotically as fast as (inB)(i_{n}^{B}) and hence

snBe2n2e(2ne)n/2s_{n}^{B}\sim\frac{e^{\sqrt{2n}}}{\sqrt{2e}}\left(\frac{2n}{e}\right)^{n/2}
Proof.

By Lemma 4.8, we have

in1BinB12n.\frac{i_{n-1}^{B}}{i_{n}^{B}}\leq\frac{1}{\sqrt{2n}}.

Therefore, from the proof of Theorem 4.12, we have

1snBinB1+2in2BinB+2in1BinB1+42n.1\leq\frac{s_{n}^{B}}{i_{n}^{B}}\leq 1+\frac{2i_{n-2}^{B}}{i_{n}^{B}}+\frac{2i_{n-1}^{B}}{i_{n}^{B}}\leq 1+\frac{4}{\sqrt{2n}}.

Now, both the sequences (1)(1) and (1+4/2n)(1+4/\sqrt{2n}) converges to 11. Hence, by the sandwich theorem, the sequence snB/inBs_{n}^{B}/i_{n}^{B} converges to 11. Thus, the sequence (snB)(s_{n}^{B}) grows asymptotically as fast as the sequence (inB)(i_{n}^{B}). By using a result of Lin [Lin13, Eq. (5)], we have the asymptotics of inBi^{B}_{n}. This completes the proof. ∎

5. Weyl groups of type D

The Weyl group of type DD, also known as the demihyperoctahedral group DnD_{n}, is defined as the following index two subgroup of BnB_{n}:

Dn:={wBnw(1)w(n)>0}.D_{n}:=\{w\in B_{n}\mid w(1)\cdots w(n)>0\}.
Lemma 5.1.

Let wBnw\in B_{n} have cycle type (λμ)(\lambda\mid\mu). Then wDnw\in D_{n} if and only if the length (μ)\ell(\mu) is even.

For a proof, take r=q=2r=q=2 in [MPS23, Lemma 2.3]. A bipartition (λμ)n(\lambda\mid\mu)\models n with (μ)\ell(\mu) is even, is called split if the associated conjugacy class C(λμ)C_{(\lambda\mid\mu)} in BnB_{n} splits into two conjugacy classes in DnD_{n}. Otherwise, (λμ)(\lambda\mid\mu) is called non-split. The following result characterizes split and non-split bipartitions of nn.

Proposition 5.2 ([Mus93, Theorem 8.2.1]).

Suppose (λμ)(\lambda\mid\mu) is a bipartition of nn with (μ)\ell(\mu) even, and πDn\pi\in D_{n} has cycle type (λμ)(\lambda\mid\mu). Then the associated conjugacy class C(λμ)C_{(\lambda\mid\mu)} in BnB_{n} splits into two conjugacy classes in DnD_{n} if and only if μ=\mu=\emptyset and all the parts of λ\lambda are even. Equivalently, the class C(λμ)C_{(\lambda\mid\mu)} remains a DnD_{n} conjugacy class if and only if either μ\mu\neq\emptyset or else one of the parts of λ\lambda is odd. In particular, for odd nn, no conjugacy class of BnB_{n} splits.

Corollary 5.3.

Conjugacy classes in DnD_{n} are indexed by bipartitions (λμ)(\lambda\mid\mu) of nn where

  • (μ)\ell(\mu) is even, and

  • if μ=\mu=\emptyset and λ\lambda contains only even parts, then there are two kinds of bipartitions (λ+)(\lambda_{+}\mid\emptyset) and (λ)(\lambda_{-}\mid\emptyset).

5.1. Generating functions

In this section, we give generating functions for the number of columns in the character table of DnD_{n} with nonzero sum as well as the total sum of the character table. We begin by characterizing the existence of square roots of elements in DnD_{n} in terms of their cycle type.

Proposition 5.4.

A bipartition (λμ)n(\lambda\mid\mu)\models n with (μ)\ell(\mu) even is the cycle type of a square element of DnD_{n} if and only if the following holds:

  1. (1)

    all even parts of λ\lambda have even multiplicity,

  2. (2)

    all parts of μ\mu have even multiplicity, and

  3. (3)

    either λ\lambda has an odd part or 4(μ)4\mid\ell(\mu).

Proof.

Let ωDn\omega\in D_{n} have cycle type (λμ)(\lambda\mid\mu). By Proposition 4.4, ω\omega has a square root in BnB_{n} if and only if (1) and (2) hold. Assuming ω\omega has a square root in BnB_{n}, it is enough to show that ω\omega has a square root in DnD_{n} if and only if either λ\lambda has a odd part or 4(μ)4\mid\ell(\mu).

Suppose πDn\pi\in D_{n} such that π2=ω\pi^{2}=\omega. If λ\lambda has an odd part, we are done. If not, observe that π\pi cannot have a negative cycle of odd length. This is because, by Lemma 4.3, the square of an odd negative cycle is a positive cycle of the same length. This is impossible as λ\lambda has no odd part.

Since πDn\pi\in D_{n}, it has an even number of negative cycles. By the last argument, π\pi has even number of negative cycles of even length, and by squaring each of them, we get two negative cycles, concluding the result 4(μ)4\mid\ell(\mu).

For the converse, note that all parts of μ\mu has even multiplicity, by (2). By Lemma 4.3, each pair of negative cycles of length tt in ω\omega can be obtained only by squaring a negative cycle of length 2t2t. Therefore, any square root (in BnB_{n}) of ω\omega must have at least (μ)/2\ell(\mu)/2 negative cycles. Thus there exists an element πBn\pi\in B_{n} such that its positive cycles squares to positive cycles of ω\omega and its negative cycles squares to negative cycles of ω\omega. Then, the number of negative cycles of π\pi is exactly (μ)/2\ell(\mu)/2, which is even if 4(μ)4\mid\ell(\mu).

If 4(μ)4\nmid\ell(\mu), λ\lambda has at least one odd part by (3). Note that the element π\pi constructed in the last paragraph does not belongs to DnD_{n} as (μ)/2\ell(\mu)/2 is odd. But, by Lemma 4.3, an odd length positive cycle can also be obtained by taking the square of a negative cycle of the same length. Since λ\lambda has at least one odd part, we can form a square root of ω\omega by choosing a negative square root for that odd part and proceeding as before for the other parts. The square root so obtained must belongs to DnD_{n} as it has (μ)/2+1\ell(\mu)/2+1 many negative cycles. This concludes the proof. ∎

Using Proposition 5.4, we next obtain the generating function for the number of conjugacy classes in DnD_{n} with non-zero column sums. The sequence of the number of partitions of a positive integer nn into an even number of parts is given in [Slo, Sequence A027187].

Lemma 5.5 ([Fin88, Example 7, Page 39]).

The generating function for the number of partitions of a positive integer nn with an even number of parts is

12(j=111qj+k=111+qk).\frac{1}{2}\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{j}}+\prod_{k=1}^{\infty}\frac{1}{1+q^{k}}\right).

Let n\mathcal{B}_{n} be the set of bipartitions of nn. The following result extend Proposition 3.4 to the group DnD_{n}.

Theorem 5.6.

The generating function for the number of conjugacy classes in DnD_{n} with non-zero column sum is

(i=111q4i)((j=111q2j)(k=011q2k+11)+12(j=111q2j+k=111+q2k)+1)1.\left(\prod_{i=1}^{\infty}\frac{1}{1-q^{4i}}\right)\left(\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}\right)\left(\prod_{k=0}^{\infty}\frac{1}{1-q^{2k+1}}-1\right)+\frac{1}{2}\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}+\prod_{k=1}^{\infty}\frac{1}{1+q^{2k}}\right)+1\right)-1.
Proof.

Let

n1={(λμ)nm2r(λ) and mr(μ) are even for each r and λ has at least one odd part},\mathcal{B}_{n}^{1}=\{(\lambda\mid\mu)\models n\mid m_{2r}(\lambda)\mbox{ and }m_{r}(\mu)\mbox{ are even for each }r\mbox{ and }\lambda\mbox{ has at least one odd part}\},

and

n2={(λμ)nm2r(λ) and mr(μ) are even for each rλ has no odd parts and (μ)0(mod4)}.\mathcal{B}_{n}^{2}=\{(\lambda\mid\mu)\models n\mid m_{2r}(\lambda)\mbox{ and }m_{r}(\mu)\mbox{ are even for each }r\mbox{, }\lambda\mbox{ has no odd parts}\mbox{ and }\ell(\mu)\equiv 0\pmod{4}\}.

Note that n1n2=\mathcal{B}_{n}^{1}\cap\mathcal{B}_{n}^{2}=\emptyset. By Proposition 5.4, a permutation πDn\pi\in D_{n} with cycle type (λμ)(\lambda\mid\mu) is the square of some element if and only if πn1n2\pi\in\mathcal{B}_{n}^{1}\cup\mathcal{B}_{n}^{2}. We now compute the generating functions for the sequences (|n1|)(|\mathcal{B}_{n}^{1}|) and (|n2|)(|\mathcal{B}_{n}^{2}|) separately.

It is easy to see that n1\mathcal{B}_{n}^{1} can be written as n1=n3n4\mathcal{B}_{n}^{1}=\mathcal{B}_{n}^{3}\setminus\mathcal{B}_{n}^{4}, where

n3={(λμ)nm2r(λ) and mr(μ) are even for each r},\mathcal{B}_{n}^{3}=\{(\lambda\mid\mu)\models n\mid m_{2r}(\lambda)\mbox{ and }m_{r}(\mu)\mbox{ are even for each }r\},

and

n4={(λμ)nm2r(λ) and mr(μ) are even for each r and λ has no odd parts}.\mathcal{B}_{n}^{4}=\{(\lambda\mid\mu)\models n\mid m_{2r}(\lambda)\mbox{ and }m_{r}(\mu)\mbox{ are even for each }r\mbox{ and }\lambda\mbox{ has no odd parts}\}.

We next find generating functions for the sequences (|n3|),(|n4|)(|\mathcal{B}_{n}^{3}|),(|\mathcal{B}_{n}^{4}|) and (|n2|)(|\mathcal{B}_{n}^{2}|). To that end, we define the following three sets:

n5=\displaystyle\mathcal{B}_{n}^{5}= {(λμ)nm4r+2(λ)=0 and m2r+1(μ)=0 for each r},\displaystyle\{(\lambda\mid\mu)\models n\mid m_{4r+2}(\lambda)=0\mbox{ and }m_{2r+1}(\mu)=0\mbox{ for each }r\},
n6=\displaystyle\mathcal{B}_{n}^{6}= {(λμ)nm4r+2(λ)=0,m2r+1(λ)=0 and m2r+1(μ)=0 for each r},\displaystyle\{(\lambda\mid\mu)\models n\mid m_{4r+2}(\lambda)=0,m_{2r+1}(\lambda)=0\mbox{ and }m_{2r+1}(\mu)=0\mbox{ for each }r\},
n7=\displaystyle\mathcal{B}_{n}^{7}= {(λμ)nm4r+2(λ)=0,m2r+1(λ)=0,m2r+1(μ)=0 for each r and (μ)0(mod2)}.\displaystyle\{(\lambda\mid\mu)\models n\mid m_{4r+2}(\lambda)=0,m_{2r+1}(\lambda)=0,m_{2r+1}(\mu)=0\mbox{ for each }r\mbox{ and }\ell(\mu)\equiv 0\pmod{2}\}.

Recall from Section 3 that Λn\Lambda_{n} denotes the set of partitions of nn. We also recall the subsets Λn1\Lambda^{1}_{n} and Λn2\Lambda^{2}_{n} from (4) and (5) respectively, and the bijection f:Λn1Λn2f:\Lambda^{1}_{n}\to\Lambda^{2}_{n} from (6). We will think of ff as a map from Λn1Λn\Lambda^{1}_{n}\to\Lambda_{n}. Now define another subset of Λn\Lambda_{n}

Λn3={λΛnλ=12m1,22m2,32m3,42m4,},\Lambda_{n}^{3}=\{\lambda\in\Lambda_{n}\mid\lambda=\langle 1^{2m_{1}},2^{2m_{2}},3^{2m_{3}},4^{2m_{4}},\dots\rangle\},

and another map g:Λn3Λng:\Lambda_{n}^{3}\rightarrow\Lambda_{n} as

(20) g(12m1,22m2,32m3,42m4,)=2m1,4m2,6m3,8m4,.g(\langle 1^{2m_{1}},2^{2m_{2}},3^{2m_{3}},4^{2m_{4}},\dots\rangle)=\langle 2^{m_{1}},4^{m_{2}},6^{m_{3}},8^{m_{4}},\dots\rangle.

We now observe that the map h(λμ)=(f(λ)g(μ))h(\lambda\mid\mu)=(f(\lambda)\mid g(\mu)) is a bijection from n3\mathcal{B}_{n}^{3} to n5\mathcal{B}_{n}^{5}. Therefore, we have

(21) n=0|n3|qn=n=0|n5|qn=i=11(1q2i1)(1q4i)(1q2i).\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{3}|q^{n}=\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{5}|q^{n}=\prod_{i=1}^{\infty}\frac{1}{(1-q^{2i-1})(1-q^{4i})(1-q^{2i})}.

Moreover, the same map hh is also a bijection from n4\mathcal{B}_{n}^{4} to n6\mathcal{B}_{n}^{6}. This gives us

(22) n=0|n4|qn=n=0|n6|qn=i=11(1q4i)(1q2i).\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{4}|q^{n}=\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{6}|q^{n}=\prod_{i=1}^{\infty}\frac{1}{(1-q^{4i})(1-q^{2i})}.

Finally, the same map hh is a bijection from n2\mathcal{B}_{n}^{2} to n7\mathcal{B}_{n}^{7}. By Lemma 5.5, the generating function for the number of partitions of a positive integer nn such that every part is even and the number of parts is also even, is

12(j=111q2j+k=111+q2k).\frac{1}{2}\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}+\prod_{k=1}^{\infty}\frac{1}{1+q^{2k}}\right).

Therefore, we have

(23) n=0|n2|qn=n=0|n7|qn=12(i=111q4i)(j=111q2j+k=111+q2k).\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{2}|q^{n}=\sum_{n=0}^{\infty}|\mathcal{B}_{n}^{7}|q^{n}=\frac{1}{2}\left(\prod_{i=1}^{\infty}\frac{1}{1-q^{4i}}\right)\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}+\prod_{k=1}^{\infty}\frac{1}{1+q^{2k}}\right).

Using (21), (22), and (23), we get

(24) n=0(|n1|+|n2|)qn=n=0(|n3||n4|+|n5|)qn=(i=111q4i)((j=111q2j)(k=011q2k+11)+12(j=111q2j+k=111+q2k)).\sum_{n=0}^{\infty}(|\mathcal{B}_{n}^{1}|+|\mathcal{B}_{n}^{2}|)q^{n}=\sum_{n=0}^{\infty}(|\mathcal{B}_{n}^{3}|-|\mathcal{B}_{n}^{4}|+|\mathcal{B}_{n}^{5}|)q^{n}\\ =\left(\prod_{i=1}^{\infty}\frac{1}{1-q^{4i}}\right)\left(\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}\right)\left(\prod_{k=0}^{\infty}\frac{1}{1-q^{2k+1}}-1\right)+\frac{1}{2}\left(\prod_{j=1}^{\infty}\frac{1}{1-q^{2j}}+\prod_{k=1}^{\infty}\frac{1}{1+q^{2k}}\right)\right).

By Proposition 5.2, a given bipartition (λμ)n(\lambda\mid\mu)\models n is split if and only if μ=\mu=\emptyset and all the parts of λ\lambda are even. Therefore, each of the bipartitions (λμ)n(\lambda\mid\mu)\models n with μ=ϕ\mu=\phi, λ\lambda having no odd parts and having even parts with even multiplicity will contribute 22 to the number of conjugacy classes with nonzero column sum in DnD_{n}. Therefore, we need to further add the generating function

i=111q4i1\prod_{i=1}^{\infty}\frac{1}{1-q^{4i}}-1

to (24). This completes the proof. ∎

For a positive integer nn, we consider all the set partitions of [n][n]. For any fixed partition of [n][n], we write all the parts in increasing order and for any part, all the elements other than the lowest and the highest of that part are said to be transient elements of that part. For any partition, an element is called transient if it is a transient element of some part. For example, let n=11n=11 and we consider the following set partition of {1,2,,11}={{1,2,6},{3,9,10,11},{4,5},{7},{8}}.\{1,2,\dots,11\}=\{\{1,2,6\},\{3,9,10,11\},\{4,5\},\{7\},\{8\}\}. There are two parts with size more than 22 and the transient elements of these two parts are 22 and 9,109,10 respectively. Therefore, the transient elements of the partition are 2,9,102,9,10. A set partition of [n][n] has no transient element if and only if all parts are either singletons or doubletons.

Theorem 5.7.

([Fla80, Theorem 2]) Let βn1,n2,s\beta_{n_{1},n_{2},s} be the number of partitions having n1n_{1} singleton classes, n2n_{2} classes of cardinality 2\geq 2 and ss non-singleton transient elements. Then the generating function

β(u1,u2,t,x)=n1,n2,s0βn1,n2,su1n1u2n2tsxs+n1+2n2\beta(u_{1},u_{2},t,x)=\sum_{n_{1},n_{2},s\geq 0}\beta_{n_{1},n_{2},s}u_{1}^{n_{1}}u_{2}^{n_{2}}t^{s}x^{s+n_{1}+2n_{2}}

is given by the J-fraction

β(u1,u2,t,x)=J(x;(u1+nt),((n+1))u2)=11u1xu2x21(u1+t)x2u2x21(u1+2t)x3u2x2.\beta(u_{1},u_{2},t,x)=J(x;(u_{1}+nt),((n+1))u_{2})=\frac{1}{\displaystyle 1-u_{1}x-\frac{u_{2}x^{2}}{\displaystyle 1-(u_{1}+t)x-\frac{2u_{2}x^{2}}{\displaystyle 1-(u_{1}+2t)x-\frac{3u_{2}x^{2}}{\dots}}}}.

Before going to the next proposition, we generalize the sequence or(n)o_{r}(n) from (3) and its generating function r(x)\mathcal{R}_{r}(x) we defined in (12) to two variables. For brevity, we will use the same symbol for both. Let

(25) or(m,y)=j=0m/2i=0m2j(m2j)(m2ji)(2j1)!!rjyi.o_{r}(m,y)=\sum_{j=0}^{\lfloor m/2\rfloor}\sum_{i=0}^{m-2j}\binom{m}{2j}\binom{m-2j}{i}(2j-1)!!\,r^{j}y^{i}.

Note that or(n,0)or(n)o_{r}(n,0)\equiv o_{r}(n). Similarly, define the J-fraction

(26) r(x,y)=J(x;(1+y),((n+1)r))=11(1+y)xrx21(1+y)x2rx2.\mathcal{R}_{r}(x,y)=J(x;(1+y),((n+1)r))=\frac{1}{\displaystyle 1-(1+y)x-\frac{rx^{2}}{\displaystyle 1-(1+y)x-\frac{2rx^{2}}{\ddots}}}.

Note that r(x,0)r(x)\mathcal{R}_{r}(x,0)\equiv\mathcal{R}_{r}(x).

Proposition 5.8.

The ordinary generating function of or(m,y)o_{r}(m,y) is

m=0or(m,y)xm=r(x,y).\sum_{m=0}^{\infty}o_{r}(m,y)x^{m}=\mathcal{R}_{r}(x,y).
Proof.

By using Theorem 5.7, we observe that r(x,y)=β(1+y,r,0,x)\mathcal{R}_{r}(x,y)=\beta(1+y,r,0,x). Therefore, it is sufficient to show that

(27) m=0or(m,y)xm=n1,n20βn1,n2,0(1+y)n1rn2xn1+2n2.\sum_{m=0}^{\infty}o_{r}(m,y)x^{m}=\sum_{n_{1},n_{2}\geq 0}\beta_{n_{1},n_{2},0}(1+y)^{n_{1}}r^{n_{2}}x^{n_{1}+2n_{2}}.

We compare the coefficient of xmx^{m} in both sides of (27). The coefficient of xmx^{m} in the left hand side is

j=0m/2i=0m2j(m2j)(m2ji)(2j1)!!rjyi,\sum_{j=0}^{m/2}\sum_{i=0}^{m-2j}\binom{m}{2j}\binom{m-2j}{i}(2j-1)!!\,r^{j}y^{i},

whereas the coefficient of xmx^{m} in the right hand side of (27) is

n1,n20,n1+2n2=mβn1,n2,0(1+y)n1rn2.\sum_{n_{1},n_{2}\geq 0,n_{1}+2n_{2}=m}\beta_{n_{1},n_{2},0}(1+y)^{n_{1}}r^{n_{2}}.

Therefore, it is sufficient to show that

(28) j=0m/2i=0m2j(m2j)(m2ji)(2j1)!!rjyi=n1,n20,n1+2n2=mβn1,n2,0(1+y)n1rn2.\sum_{j=0}^{m/2}\sum_{i=0}^{m-2j}\binom{m}{2j}\binom{m-2j}{i}(2j-1)!!\,r^{j}y^{i}=\sum_{n_{1},n_{2}\geq 0,n_{1}+2n_{2}=m}\beta_{n_{1},n_{2},0}(1+y)^{n_{1}}r^{n_{2}}.

The coefficient of yirn2y^{i}r^{n_{2}} in the left hand side and the right hand side of (28) is respectively (m2n2)(m2n2i)(2n21)!!\binom{m}{2n_{2}}\binom{m-2n_{2}}{i}(2n_{2}-1)!! and βn1,n2,0(n1i)\beta_{n_{1},n_{2},0}\binom{n_{1}}{i}. As n1+2n2=mn_{1}+2n_{2}=m, the quantity βn1,n2,0\beta_{n_{1},n_{2},0} is the number of partitions of n1+2n2n_{1}+2n_{2} into n1n_{1} singletons and n2n_{2} doubletons and therefore βn1,n2,0=(m2n2)(2n21)!!.\beta_{n_{1},n_{2},0}=\binom{m}{2n_{2}}(2n_{2}-1)!!. This completes the proof. ∎

Let Γ(λμ)D\Gamma^{D}_{(\lambda\mid\mu)} be the sum of entries of the column indexed by (λμ)(\lambda\mid\mu) in the character table of DnD_{n}. By Theorem 2.4, Γ(λμ)D\Gamma^{D}_{(\lambda\mid\mu)} is the number of square roots of an element of cycle type (λμ)(\lambda\mid\mu).

Proposition 5.9.

For elements in DnD_{n} whose cycle type contains a single cycle, the following results hold.

  1. (1)

    Γ((2k)2m2k)D=(2m2k1)!!(2k)m2k\displaystyle\Gamma^{D}_{((2k)^{2m_{2k}}\mid\emptyset)}=(2m_{2k}-1)!!\,(2k)^{m_{2k}},

  2. (2)

    Γ((2k+1)m2k+1))D=o2k+1(m2k+1,1)\Gamma^{D}_{((2k+1)^{m_{2k+1}})\mid\emptyset)}=o_{2k+1}(m_{2k+1},1),

  3. (3)

    Γ((k)2m2k)D=(2m2k1)!!(k)m2k\Gamma^{D}_{(\emptyset\mid(k)^{2m_{2k}})}=(2m_{2k}-1)!!\,(k)^{m_{2k}}.

Proof.

By Lemma 5.1, elements in the first two cases belong to DnD_{n}; for the third case however, m2km_{2k} must also be even.

By Lemma 4.3(2), the square root of a pair of positive cycles of length 2k2k is a positive cycle of length 4k4k. We can pair the 2m2k2m_{2k} cycles in (2m2k1)!!(2m_{2k}-1)!! ways and merge each pair in 2k2k ways. This proves the first part. A similar argument proves the third part.

By Lemma 4.3(1) the square root of positive odd cycles can be formed in multiple ways. They can be positive or negative cycles of the same length. If there are two such cycles, their square root can be formed by pairing them into a positive cycle of double the length. In general, we can pair jj of these cycles, where 2jm2k+12j\leq m_{2k+1}, in (2j1)!!(2j-1)!! ways and merge each pair in 2k+12k+1 ways. Among the m2k+12jm_{2k+1}-2j remaining cycles, we can arbitrarily choose ii of them, where im2k+12ji\leq m_{2k+1}-2j, to have a square root with a negative cycle. Summing over ii and jj gives the formula in (25) with r=2k+1r=2k+1 and y=1y=1, completing the proof. ∎

Let snDs_{n}^{D} denote the sum of the entries of the character table of DnD_{n}. Let 𝒮D(x)\mathcal{S}^{D}(x) be the ordinary generating function of (snD)(s_{n}^{D}). Recall the generating function 𝒟(x)\mathcal{D}(x) for double factorials in (11). Let {xi,yii}\{x_{i},y_{i}\mid i\in\mathbb{N}\} be a family of commuting indeterminates.

Theorem 5.10.

The number of square roots of an element in DnD_{n} with cycle type (λμ)(\lambda\mid\mu), where they are written in frequency notation as

λ=1m1,2m2,,nmnandμ=1p1,2p2,,npn,\lambda=\langle 1^{m_{1}},2^{m_{2}},\dots,n^{m_{n}}\rangle\quad\text{and}\quad\mu=\langle 1^{p_{1}},2^{p_{2}},\dots,n^{p_{n}}\rangle,

namely Γ(λμ)D\Gamma^{D}_{(\lambda\mid\mu)}, is the coefficient of x1m1x2m2xnmny1p1y2p2ynpnx_{1}^{m_{1}}x_{2}^{m_{2}}\dots x_{n}^{m_{n}}y_{1}^{p_{1}}y_{2}^{p_{2}}\dots y_{n}^{p_{n}} after setting all even powers of zz to 11 and odd powers of zz to 0 in

k1(𝒟(4kx2k2)𝒟(2kzyk2)2k1(x2k1,z))+k1𝒟(4kx2k2)1.\prod_{k\geq 1}\left(\mathcal{D}(4kx_{2k}^{2})\mathcal{D}(2kzy_{k}^{2})\mathcal{R}_{2k-1}(x_{2k-1},z)\right)+\prod_{k\geq 1}\mathcal{D}(4kx_{2k}^{2})-1.

Therefore, the generating function of the sum of the entries in the character table of DnD_{n} is

𝒮D(x)=(k1(𝒟(4kx4k)𝒟(2kzx2k)2k1(x2k1,z))+k1𝒟(4kx4k)1)|z2k1,z2k10k.\mathcal{S}^{D}(x)=\Bigg{(}\prod_{k\geq 1}\left(\mathcal{D}(4kx^{4k})\mathcal{D}(2kzx^{2k})\mathcal{R}_{2k-1}(x^{2k-1},z)\right)+\prod_{k\geq 1}\mathcal{D}(4kx^{4k})-1\Bigg{)}\Bigg{|}_{z_{2k}\to 1,z_{2k-1}\to 0\forall k}.
Proof.

Square elements in DnD_{n} are classified in Proposition 5.4. The idea of this proof is similar to that of Theorem 3.6. However, there are three additional complications. First, we will have to take care that the square roots satisfy Lemma 5.1, i.e. the number of negative cycles must be even. Secondly, we have to ensure that Proposition 5.4(3) is satisfied, which couples positive and negative cycles. And thirdly, we have to account for two kinds of conjugacy classes when there are no negative cycles and only even positive cycles according to Corollary 5.3.

The generating function of even positive cycles of length 2k2k is 𝒟(4kx2k2)\mathcal{D}(4kx_{2k}^{2}) using Proposition 5.9(1) as before, and all square roots have positive cycles. The generating function of negative cycles of length kk is 𝒟(2kyk2)\mathcal{D}(2ky_{k}^{2}) using Proposition 5.9(3) and all are negative cycles. We now introduce the auxiliary variable zz which keeps track of the number of negative cycles in the square root. That is to say, if there are ii negative cycles in the square root, we keep an additional factor of ziz^{i}. Therefore, the latter generating function is 𝒟(2kzyk2)\mathcal{D}(2kzy_{k}^{2}). By the arguments in the proof of Proposition 5.9(2), the generating function of odd positive cycles of length 2k12k-1 is 2k1(x2k1,z)\mathcal{R}_{2k-1}(x_{2k-1},z). The product of these three terms over all kk gives the first product in the generating function. By setting all odd powers of zz to 0 and even powers of zz to 11 ensures that the first condition in the paragraph above is satisfied.

Now suppose we count the number of square roots for an element of cycle type (λμ)(\lambda\mid\mu). If λ\lambda has an odd part, the second condition is automatically satisfied. If not, then the factor 2k1(x2k1,z)\mathcal{R}_{2k-1}(x_{2k-1},z) does not contribute for any value of kk. We know by Lemma 5.1 that μ\mu has an even number of parts, and for each part, we get a factor of zz from the factor 𝒟(2kzyk2)\mathcal{D}(2kzy_{k}^{2}). Since only even powers of zz contribute, μ\mu has length divisible by 44, proving the second condition. Finally, suppose μ=\mu=\emptyset and λ\lambda contains only even parts. As argued above, we only get a contribution from k𝒟(4kx2k2)\prod_{k}\mathcal{D}(4kx_{2k}^{2}) in that case. But we have two distinct conjugacy classes in that case by Corollary 5.3 with the same number of square roots. Therefore, we need another such factor, which explains the second product. This now satisfies the third condition. The last term, 1-1, is present to make sure the constant term is 11.

Replacing xkx_{k} and yky_{k} by xkx^{k} gives the generating function of column sums and completes the proof. ∎

5.2. Proof of Property S

Recall the following result (see Corollary 7.9.6 and Theorem 8.3.1 of [Mus93]]) about irreducible characters of DnD_{n}.

Theorem 5.11.

Let χαβ\chi^{\alpha\mid\beta} denote the irreducible character of BnB_{n} corresponding to the bipartition (αβ)n(\alpha\mid\beta)\models n. Then the following hold:

  1. (1)

    χαβ=χβαξ\chi^{\alpha\mid\beta}=\chi^{\beta\mid\alpha}\otimes\xi, where ξ:Bn{1,1}\xi:B_{n}\rightarrow\{1,-1\} is the multiplicative character whose kernel is DnD_{n}.

  2. (2)

    If χαβ\chi^{\alpha\mid\beta}\downarrow is the restriction of χαβ\chi^{\alpha\mid\beta} to DnD_{n}, then χαβ=χβα=χαβ\chi^{\alpha\mid\beta}\downarrow=\chi^{\beta\mid\alpha}\downarrow=\chi^{\alpha\mid\beta} if and only if αβ\alpha\neq\beta, and χαα=χ+αα+χαα\chi^{\alpha\mid\alpha}\downarrow=\chi^{\alpha\mid\alpha}_{+}+\chi^{\alpha\mid\alpha}_{-}. In the latter case, χ±αα\chi^{\alpha\mid\alpha}_{\pm} are irreducible characters of DnD_{n} of equal dimension.

Let inDi_{n}^{D} denote the number of involutions in DnD_{n}. Recall that Γ(λμ)D\Gamma^{D}_{(\lambda\mid\mu)} (resp. Γ(λμ)B\Gamma^{B}_{(\lambda\mid\mu)}) is the sum of entries of the column indexed by (λμ)(\lambda\mid\mu) in the character table of DnD_{n} (resp. BnB_{n}). Our next result relates the character sum of BnB_{n} with that of DnD_{n} when nn is odd.

Proposition 5.12.

For an odd positive integer nn and (λμ)n(\lambda\mid\mu)\models n, we have

Γ(λμ)B={2Γ(λμ)D(μ) even,0(μ) odd.\Gamma^{B}_{(\lambda\mid\mu)}=\begin{cases}\displaystyle 2\Gamma^{D}_{(\lambda\mid\mu)}&\text{$\ell(\mu)$ even},\\ 0&\text{$\ell(\mu)$ odd}.\end{cases}

Therefore, we have snB=2snDs_{n}^{B}=2s_{n}^{D}.

Proof.

Assume that nn is odd throughout the proof. Then there are no irreducible representations of type (αα)(\alpha\mid\alpha) in BnB_{n}. So

Irr(Bn)={(αβ),(βα)n|αβ} and Irr(Dn)={(αβ)n|αβ}.\mathrm{Irr}(B_{n})=\{(\alpha\mid\beta),(\beta\mid\alpha)\models n\bigm{|}\alpha\neq\beta\}\text{ and }\mathrm{Irr}(D_{n})=\{(\alpha\mid\beta)\models n\bigm{|}\alpha\neq\beta\}.

By Lemma 5.1 an element wBnw\in B_{n} with cycle type (λμ)n(\lambda\mid\mu)\models n belongs to DnD_{n} if and only if (μ)\ell(\mu) is even. Then, Theorem 5.11(1) implies that

χβα((λμ))={χαβ((λμ))(μ) even,χαβ((λμ))(μ) odd.\chi^{\beta\mid\alpha}((\lambda\mid\mu))=\begin{cases}\displaystyle\chi^{\alpha\mid\beta}((\lambda\mid\mu))&\ell(\mu)\text{ even},\\ \displaystyle-\chi^{\alpha\mid\beta}((\lambda\mid\mu))&\ell(\mu)\text{ odd}.\end{cases}

Now, when (λμ)n(\lambda\mid\mu)\models n and (μ)\ell(\mu) is even, by Theorem 5.11(2) we get

Γ(λμ)B=(αβ)nαβ(χαβ((λμ))+χβα((λμ)))=(αβ)nαβ2χαβ((λμ))=2Γ(λμ)D.\Gamma^{B}_{(\lambda\mid\mu)}=\sum_{\begin{subarray}{c}(\alpha\mid\beta)\models n\\ \alpha\neq\beta\end{subarray}}\Big{(}\chi^{\alpha\mid\beta}((\lambda\mid\mu))+\chi^{\beta\mid\alpha}((\lambda\mid\mu))\Big{)}=\sum_{\begin{subarray}{c}(\alpha\mid\beta)\models n\\ \alpha\neq\beta\end{subarray}}2\chi^{\alpha\mid\beta}\downarrow((\lambda\mid\mu))=2\Gamma^{D}_{(\lambda\mid\mu)}.

Similarly, if (λμ)n(\lambda\mid\mu)\models n and (μ)\ell(\mu) is odd, then Γ(λμ)B=0\Gamma^{B}_{(\lambda\mid\mu)}=0. Note that the latter statement also follows directly from Proposition 4.4.

The second part follows easily from the first part and the observation that there are no split conjugacy classes in DnD_{n} when nn is odd. ∎

When nn is even, it seems difficult to estimate the difference of respective column sums in the character table of BnB_{n} and DnD_{n} using direct computation of character values. However, the difference of the first column sum, which is precisely the number of involutions in BnB_{n} which do not belong to DnD_{n}, turns out to have a nice formula. We have not been able to find the following result in the literature. It would be interesting to find a combinatorial proof.

Lemma 5.13.

We have

2inDinB={0n odd,2n/2(n1)!!=n!(n/2)!n even.2i_{n}^{D}-i_{n}^{B}=\begin{cases}0&\text{$n$ odd},\\ \displaystyle 2^{n/2}(n-1)!!=\frac{n!}{(n/2)!}&\text{$n$ even}.\end{cases}

Therefore, for all positive integers nn, inDinB2inDi_{n}^{D}\leq i_{n}^{B}\leq 2i_{n}^{D}.

Proof.

The result for odd nn follows directly from Proposition 5.12, but we give a unified algebraic proof for all nn. By [Cho06, Theorems 2.1 and 3.2], we have

(29) n0inBxnn!=ex2+2x,\sum_{n\geq 0}i_{n}^{B}\frac{x^{n}}{n!}=e^{x^{2}+2x},

and

(30) n0inDxnn!=ex2e2x+12.\sum_{n\geq 0}i_{n}^{D}\frac{x^{n}}{n!}=e^{x^{2}}\frac{e^{2x}+1}{2}.

Subtracting (30) from (29), we get

(31) n0(inBinD)xnn!=ex2e2x12.\sum_{n\geq 0}(i_{n}^{B}-i_{n}^{D})\frac{x^{n}}{n!}=e^{x^{2}}\frac{e^{2x}-1}{2}.

Finally, subtracting (31) from (30) gives ex2e^{x^{2}}. Thus, there are no odd powers, proving the equation for odd nn. Extracting the coefficient of x2n/(2n)!x^{2n}/(2n)! proves the result for even nn.

For the second part, it is clear that all the involutions in DnD_{n} also belong to BnB_{n}, proving the first inequality. The second inequality follows from the first part, completing the proof. ∎

Recall the definition of gnBg_{n}^{B} from (17).

Lemma 5.14.

For positive integers nn, snDinD+(snBinB)+gnBs_{n}^{D}\leq i_{n}^{D}+(s_{n}^{B}-i_{n}^{B})+g_{n}^{B}.

Proof.

By Proposition 5.2, we have

snD=(λμ)n non-splitΓ(λμ)D+(λμ)n split(Γ(λ+)D+Γ(λ)D).s_{n}^{D}=\sum_{(\lambda\mid\mu)\models n\text{ non-split}}\Gamma^{D}_{(\lambda\mid\mu)}+\sum_{(\lambda\mid\mu)\models n\text{ split}}(\Gamma^{D}_{(\lambda_{+}\mid\emptyset)}+\Gamma^{D}_{(\lambda_{-}\mid\emptyset)}).

Since (1n)(\langle 1^{n}\rangle\mid\emptyset) represents the trivial conjugacy class of DnD_{n} and Γ(1n)D=inD\Gamma^{D}_{(\langle 1^{n}\rangle\mid\emptyset)}=i_{n}^{D}, we can write

(32) snD=(inD+(λμ)n non-split(λμ)(1n)Γ(λμ)D)+(λμ)n splitΓ(λ+)D+(λμ)n splitΓ(λ)D.s_{n}^{D}=\left(i_{n}^{D}+\sum_{\begin{subarray}{c}(\lambda\mid\mu)\models n\text{ non-split}\\ (\lambda\mid\mu)\neq(\langle 1^{n}\rangle\mid\emptyset)\end{subarray}}\Gamma^{D}_{(\lambda\mid\mu)}\right)+\sum_{(\lambda\mid\mu)\models n\text{ split}}\Gamma^{D}_{(\lambda_{+}\mid\emptyset)}+\sum_{(\lambda\mid\mu)\models n\text{ split}}\Gamma^{D}_{(\lambda_{-}\mid\emptyset)}.

Since the number of square roots of an element with cycle type (λμ)(\lambda\mid\mu) in DnD_{n} is less than or equal to the number of square roots of an element with cycle type (λμ)(\lambda\mid\mu) in BnB_{n}, we have Γ(λμ)DΓ(λμ)B\Gamma^{D}_{(\lambda\mid\mu)}\leq\Gamma^{B}_{(\lambda\mid\mu)}, the (λμ)(\lambda\mid\mu)’th column sum in the character table of BnB_{n}. Applying this upper bound for the second and third summand (of the right hand side) of 32, we get

(33) snDinD+(λμ)n and (λμ)(1n)Γ(λμ)B+(λμ)n is splitΓ(λ)D.s_{n}^{D}\leq i_{n}^{D}+\sum_{\begin{subarray}{c}(\lambda\mid\mu)\models n\text{ and }\\ (\lambda\mid\mu)\neq(\langle 1^{n}\rangle\mid\emptyset)\end{subarray}}\Gamma^{B}_{(\lambda\mid\mu)}+\sum_{(\lambda\mid\mu)\models n\text{ is split}}\Gamma^{D}_{(\lambda_{-}\mid\emptyset)}.

The second sum of the right hand side of (33) is clearly equal to snBinBs_{n}^{B}-i_{n}^{B}. By Proposition 5.2, if (λμ)n(\lambda\mid\mu)\models n is a split bipartition, then μ=\mu=\emptyset and all parts of λ\lambda are even. In particular, a split bipartition (λμ)(\lambda\mid\mu) has the property m1(λ)=0m_{1}(\lambda)=0. Thus, the last sum of (33) is at most gnBg_{n}^{B} . Therefore, we have the desired inequality. ∎

Theorem 5.15.

Property S holds for all demihyperoctahedral groups.

Proof.

By Proposition 5.12 and Lemma 5.13, Property S holds for DnD_{n} when nn is odd. However we will not use this fact for our proof strategy.

First we consider the case when n16n\geq 16. Using (19) in Lemma 5.14 we have,

(34) snDinD2(in1B+in2B)+gnB.s_{n}^{D}-i_{n}^{D}\leq 2(i_{n-1}^{B}+i_{n-2}^{B})+g_{n}^{B}.

Setting k=1k=1 in Lemma 4.10 (since n5n\geq 5), we have

(35) snDinD2in1B+2in2B+inBn1.s_{n}^{D}-i_{n}^{D}\leq 2i_{n-1}^{B}+2i_{n-2}^{B}+\frac{i_{n}^{B}}{n-1}.

Now apply the first inequality of Lemma 4.8 to the second term of the right hand side of (35) to get

(36) snDinD2in1B+2in1B2n2+inBn1(2+230)in1B+inB15,s_{n}^{D}-i_{n}^{D}\leq 2i_{n-1}^{B}+\frac{2i_{n-1}^{B}}{\sqrt{2n-2}}+\frac{i_{n}^{B}}{n-1}\leq\left(2+\frac{2}{\sqrt{30}}\right)i_{n-1}^{B}+\frac{i_{n}^{B}}{15},

where we have used n16n\geq 16 for the last inequality. For n16n\geq 16, again using the first inequality of Lemma 4.8, we have in1BinB/2ninB/32i_{n-1}^{B}\leq i_{n}^{B}/\sqrt{2n}\leq i_{n}^{B}/\sqrt{32}. Using this fact along with the inequality inB2inDi_{n}^{B}\leq 2i_{n}^{D} from Lemma 5.13 in (36), we get

snDinD2(230+2)3032inD+215inDinD,s_{n}^{D}-i_{n}^{D}\leq 2\frac{(2\sqrt{30}+2)}{\sqrt{30\cdot 32}}i_{n}^{D}+\frac{2}{15}i_{n}^{D}\leq i_{n}^{D},

where the last inequality follows because

2(230+2)3032+2150.96951.2\frac{(2\sqrt{30}+2)}{\sqrt{30\cdot 32}}+\frac{2}{15}\approx 0.9695\leq 1.

This completes the proof for n16n\geq 16. For n15n\leq 15, the validity of the statement holds by the direct computation shown in Appendix B. Thus, we have proved the result for all positive integers nn. ∎

Corollary 5.16.

For positive integers nn, we have

snDe2n22e(2ne)n/2.s_{n}^{D}\sim\frac{e^{\sqrt{2n}}}{2\sqrt{2e}}\left(\frac{2n}{e}\right)^{n/2}.
Proof.

This follows immediately by using Corollary 4.13 and Lemma 5.13. ∎

6. Generalized symmetric groups

We follow [MPS23, Section 2] for the notational background used in this section. For nonnegative integers r,nr,n, let r={0¯,1¯,,r1¯}\mathbb{Z}_{r}=\{\overline{0},\overline{1},\ldots,\overline{r-1}\} be the additive cyclic group of order rr, where we use bars to distinguish these elements from those in the symmetric group. Then define the generalized symmetric group

G(r,1,n)=rSn:={(z1,,zn;σ)zir,σSn}.G(r,1,n)=\mathbb{Z}_{r}\wr S_{n}:=\{(z_{1},\dots,z_{n};\sigma)\mid z_{i}\in\mathbb{Z}_{r},\sigma\in S_{n}\}.

We remark here that the complex reflection group G(r,q,n)G(r,q,n) is an index qq subgroup of G(r,1,n)G(r,1,n); see Section 6.2 for details. If π=(z1,z2,,zn;σ)\pi=(z_{1},z_{2},\ldots,z_{n};\sigma) and π=(z1,z2,,zn;σ)\pi^{\prime}=(z_{1}^{\prime},z_{2}^{\prime},\ldots,z_{n}^{\prime};\sigma^{\prime}), then their product is given by

(37) ππ=(z1+zσ1(1),,zn+zσ1(n);σσ),\pi\,\pi^{\prime}=(z_{1}+z_{\sigma^{-1}(1)}^{\prime},\ldots,z_{n}+z_{\sigma^{-1}(n)}^{\prime};\sigma\sigma^{\prime}),

where σσ\sigma\sigma^{\prime} is the standard product of permutations in SnS_{n}.

The group G(r,1,n)G(r,1,n) can also be realized as a subgroup of the symmetric group SrnS_{rn}. In this interpretation G(r,1,n)G(r,1,n) consists of all permutations π\pi of the set {k¯+i0kr1,1in}\{\overline{k}+i\mid 0\leq k\leq r-1,1\leq i\leq n\} satisfying π(k¯+i)=k¯+π(i)\pi(\overline{k}+i)=\overline{k}+\pi(i) for all allowed kk and ii. For convenience, we identify the letters 0¯+i\overline{0}+i with ii for 1in1\leq i\leq n. Given a permutation πG(r,1,n)\pi\in G(r,1,n), its values at 1,,n1,\ldots,n determine π\pi uniquely.

The two definitions above are identified using the bijective map ϕ\phi defined on the window [1,,n][1,\dots,n] by

ϕ((z1,,zn;σ))=[12nzσ(1)+σ(1)zσ(2)+σ(2)zσ(n)+σ(n)].\phi((z_{1},\ldots,z_{n};\sigma))=\begin{bmatrix}1&2&\cdots&n\\ z_{\sigma(1)}+\sigma(1)&z_{\sigma(2)}+\sigma(2)&\cdots&z_{\sigma(n)}+\sigma(n)\end{bmatrix}.

This map satisfies ϕ(ππ)=ϕ(π)ϕ(π)\phi(\pi\,\pi^{\prime})=\phi(\pi)\circ\phi(\pi^{\prime}), where \circ is the usual composition of permutations in SrnS_{rn}.

Let π=(z1,,zn;σ)G(r,1,n)\pi=(z_{1},\ldots,z_{n};\sigma)\in G(r,1,n) and (u1),,(ut)(u_{1}),\ldots,(u_{t}) be the cycles of σ\sigma. Let (ui)=(ui,1,,ui,i)(u_{i})=(u_{i,1},\ldots,u_{i,{\ell_{i}}}) where i\ell_{i} is the length of the cycle (ui)(u_{i}). Define the color of a cycle (ui)(u_{i}) as z(ui):=zui,1+zui,2++zui,irz(u_{i}):=z_{u_{i,1}}+z_{u_{i,2}}+\ldots+z_{u_{i,\ell_{i}}}\in\mathbb{Z}_{r}. For j{0,,r1}j\in\{0,\ldots,r-1\}, let λj\lambda^{j} be the partition formed by the lengths of color jj cycles of σ\sigma. Note that 𝑗|λj|=n\underset{j}{\sum}|\lambda^{j}|=n. The rr-tuple of partitions 𝝀=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1}) is called the cycle type of π\pi. We refer to such an rr-tuple of partitions as an r-partite partition of size nn, denoted λrn\lambda\models_{r}n.

For example, the cycle type of the element

(2¯,1¯,1¯,1¯,0¯,2¯;(123)(45)(6))G(3,1,6)(\overline{2},\overline{1},\overline{1},\overline{1},\overline{0},\overline{2};\,(123)(45)(6))\in G(3,1,6)

is ((3,2)(1))(\emptyset\mid(3,2)\mid(1)).

The following theorem asserts that the conjugacy classes of G(r,1,n)G(r,1,n) are indexed by rr-partite partitions of nn.

Theorem 6.1.

[Mac95, p. 170] Two elements π1\pi_{1} and π2\pi_{2} in G(r,1,n)G(r,1,n) are conjugate if and only if their corresponding cycle types are equal.

Lemma 6.2.

Let π=(z1,,zd;σ)G(r,1,d)\pi=(z_{1},\ldots,z_{d};\sigma)\in G(r,1,d) with a single cycle of color tt.

  1. (1)

    When dd is even, π2\pi^{2} is a product of two color tt cycles each of length d/2d/2.

  2. (2)

    When dd is odd, π2\pi^{2} is a single cycle of length dd and color 2t2t.

Proof.

Let π=(z1,,zd;σ)G(r,1,d)\pi=(z_{1},\ldots,z_{d};\sigma)\in G(r,1,d) where σ=(d,d1,,1)\sigma=(d,d-1,\ldots,1). Then, π2=(z1+z2,,zd+z1;σ2)\pi^{2}=(z_{1}+z_{2},\ldots,z_{d}+z_{1};\sigma^{2}). When dd is even, σ2=(d,d2,,4,2)(d1,d3,,3,1)\sigma^{2}=(d,d-2,\ldots,4,2)(d-1,d-3,\ldots,3,1). Note that the color of each cycle of σ2\sigma^{2} is z1++zdz_{1}+\cdots+z_{d}. Thus the first statement follows. When dd is odd, σ2=(d,d2,,3,1,d1,d3,,2)\sigma^{2}=(d,d-2,\ldots,3,1,d-1,d-3,\ldots,2) and the color of π2\pi^{2} is (z1+z2)++(zd+z1)=2(z1++zd)(z_{1}+z_{2})+\cdots+(z_{d}+z_{1})=2(z_{1}+\cdots+z_{d}). This concludes the proof. ∎

Proposition 6.3.

An rr-partite partition 𝛌=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1}) is the cycle-type of a square element of G(r,1,n)G(r,1,n) if and only if the following conditions hold:

  1. (1)

    each even part in each partition λt\lambda^{t} has even multiplicity, and

  2. (2)

    when rr is even, odd parts in λ1,λ3,,λr1\lambda^{1},\lambda^{3},\ldots,\lambda^{r-1} have even multiplicity.

Proof.

Let π\pi have cycle type 𝝀=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1}) and ww be a square root of π\pi. The first part follows directly from Lemma 6.2(1). When rr is even, a single odd length cycle of π\pi with color 2k12k-1, where k=1,2,,r/2k=1,2,\ldots,r/2, cannot be obtained by squaring any single cycle (of any color) of ww. This is because, if a cycle of color tt of ww squares to a cycle of color 2k12k-1 of π\pi, then 2t=2k12t=2k-1 by Lemma 6.2(2). But this equation has no solution in r\mathbb{Z}_{r} when rr is even. Thus, all odd parts in λ1,λ3,,λr1\lambda^{1},\lambda^{3},\ldots,\lambda^{r-1} must come from squaring even length cycles of the same color, enforcing the even multiplicity condition.

The converse part follows by applying Lemma 6.2. A detailed construction of such a square root is demonstrated in the proof of Proposition 6.4. ∎

6.1. Generating function for number of square roots

We now count the number of square roots for elements satisfying Proposition 6.3. We say π=(z1,,zd;σ)G(r,1,d)\pi=(z_{1},\ldots,z_{d};\sigma)\in G(r,1,d) is a single cycle of color tt if σSd\sigma\in S_{d} is a dd-cycle with color z(σ)=tz(\sigma)=t.

Proposition 6.4.
  1. (1)

    Let πG(r,1,d)\pi\in G(r,1,d) be a single cycle of color tt with dd odd. Then the number of square roots of π\pi is

    {1r odd,2r even and t even,0r even and t odd.\begin{cases}1&\text{$r$ odd},\\ 2&\text{$r$ even and $t$ even},\\ 0&\text{$r$ even and $t$ odd}.\end{cases}
  2. (2)

    Let πG(r,1,2d)\pi\in G(r,1,2d) be a product of two disjoint cycles, both having color tt and length dd. Then the number of square roots of π\pi is drdr.

Proof.

Without loss of generality, let π=(t,0,,0;σ=(d,d2,,1,d1,d3,,2))\pi=(t,0,\ldots,0;\sigma=(d,d-2,\dots,1,d-1,d-3,\ldots,2)), which has cycle type λt=(d)\lambda^{t}=(d), with all other λi\lambda^{i}’s being empty. When dd is odd, the cycle σ\sigma has the unique square root (d,d1,,1)(d,d-1,\ldots,1) in SdS_{d}. Let (z1,,zd;(d,d1,,1))(z_{1},\ldots,z_{d};(d,d-1,\ldots,1)) be a square root of π\pi. This gives the following system of equations:

z1+z2=t,z2+z3=0,,zd1+zd=0,zd+z1=0.z_{1}+z_{2}=t,z_{2}+z_{3}=0,\ldots,z_{d-1}+z_{d}=0,z_{d}+z_{1}=0.

Solving this system, we get 2z2=t2z_{2}=t. When rr is odd, 2z2=t2z_{2}=t has a unique solution in r\mathbb{Z}_{r}, and thus π\pi has unique square root. When rr is even, the equation 2z2=t2z_{2}=t in r\mathbb{Z}_{r} has no solution if tt is odd and has exactly two solutions if tt is even. This proves the first part.

Finally, let π=(t,0,,0,t;σ)G(r,1,2d)\pi=(t,0,\ldots,0,t;\sigma)\in G(r,1,2d) where σ=(2d,2d2,,4,2)(2d1,2d3,,3,1)\sigma=(2d,2d-2,\ldots,4,2)(2d-1,2d-3,\ldots,3,1). Note that σ\sigma has dd square roots in S2dS_{2d}, one of which is (2d,2d1,,1)(2d,2d-1,\dots,1). Let (z1,,z2d;(2d,2d1,,1))(z_{1},\ldots,z_{2d};(2d,2d-1,\ldots,1)) be a square root of π\pi. Then we get the following system of equations:

z1+z2=t,z2+z3=0,,z2d1+z2d=0,z2d+z1=t.z_{1}+z_{2}=t,z_{2}+z_{3}=0,\ldots,z_{2d-1}+z_{2d}=0,z_{2d}+z_{1}=t.

Observe that the above system has rr solutions as every choice of z1z_{1} is valid and fixes all other values. For each choice of square root of σ\sigma, we have rr square roots of π\pi. This concludes the proof. ∎

Proposition 6.5.

Given a positive integer rr and tt such that 0tr10\leq t\leq r-1, the number of square roots of elements whose cycles all have the same length \ell and color tt is as follows.

  1. (1)

    When =2k\ell=2k and there are 2m2m cycles, this is given by

    (38) (2m1)!!(2k)mrm.(2m-1)!!(2k)^{m}r^{m}.
  2. (2)

    When =2k+1\ell=2k+1, rr is odd and there are mm cycles, this is given by

    (39) j=0m2(m2j)(2j1)!!(2k+1)jrj.\sum_{j=0}^{\lfloor\frac{m}{2}\rfloor}\binom{m}{2j}(2j-1)!!(2k+1)^{j}r^{j}.
  3. (3)

    When =2k+1\ell=2k+1, both rr and tt are even and there are mm cycles, this is given by

    (40) j=0m2(m2j)(2j1)!!(2k+1)jrj2m2j.\sum_{j=0}^{\lfloor\frac{m}{2}\rfloor}\binom{m}{2j}(2j-1)!!(2k+1)^{j}r^{j}2^{m-2j}.
  4. (4)

    When =2k+1\ell=2k+1, rr is even, tt is odd and there are mm cycles, this is given by

    (41) (2m1)!!(2k+1)mrm.(2m-1)!!(2k+1)^{m}r^{m}.
Proof.

We want to consider all elements π\pi whose square is an element π\pi^{\prime} whose cycle type has only cycles of length \ell with color tt. Let the cycle type of π\pi be 𝝀=(λ0λr1)\bm{\lambda}=(\lambda^{0}\mid\dots\mid\lambda^{r-1}).

First suppose =2k\ell=2k, and there are 2m2m cycles. By Lemma 6.2(1), the square roots of such element will necessarily arise from elements whose cycle type λt\lambda^{t} contains (4k)m(4k)^{m} by combining cycles in pairs and choosing the color in one of rr ways as in Proposition 6.4(3). The number of ways of doing this is given in (38).

Now suppose =2k+1\ell=2k+1. Then this calculation depends on whether rr is odd or even, and in the latter case, whether tt is odd or even. The simplest case is when rr is odd, and if so, suppose there are mm cycles. By Lemma 6.2(1) and (2), the square roots of this element can either contain (2k+1)(2k+1) cycles in the partition λt/2\lambda^{t/2}, (where t/2t/2 is well-defined in r\mathbb{Z}_{r} because rr is odd) or (4k+2)(4k+2) cycles in the partition λt\lambda^{t} (by pairing cycles and coloring each of them in rr ways). Any combination of singletons and pairs gives a valid way of creating a square root. The number of ways of doing this is given in (39).

When rr and tt are both even, suppose again that there are mm cycles. The calculation is very similar to the above case, except that there are two choices for t/2t/2 in r\mathbb{Z}_{r} as shown in Proposition 6.4(2). Therefore, we get an extra power of 22 proving (40).

Lastly, when rr is even, tt is odd and there are 2m2m cycles, the situation is much simpler. In this case, t/2t/2 does not exist in r\mathbb{Z}_{r} and therefore the square root cannot contain (2k+1)(2k+1) cycles in λt/2\lambda^{t/2} as shown in Proposition 6.4(2). Thus, the cycles will have to pair up just as in the first case of even cycles and the square root has to contain (4k+2)m(4k+2)^{m} in λt\lambda^{t}. The number of ways of pairing these cycles is thus (41), completing the proof. ∎

Recall the generating functions 𝒟(x)\mathcal{D}(x) from (11) and r(x)\mathcal{R}_{r}(x) from (12). Let x,{xt,j0tr1,j}x,\{x_{t,j}\mid 0\leq t\leq r-1,j\in\mathbb{N}\} be a family of commuting indeterminates.

Theorem 6.6.

Write each partition in the rr-partite partition 𝛌=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1}) of size nn in frequency notation, with λt=1mt,1,2mt,2,,nmt,n\lambda^{t}=\langle 1^{m_{t,1}},2^{m_{t,2}},\dots,n^{m_{t,n}}\rangle. Then the number of square roots of an element in G(r,1,n)G(r,1,n) with cycle type 𝛌\bm{\lambda} is the coefficient of

(x0,1m0,1x0,nm0,n)(xr1,1mr1,1xr1,nmr1,n)(x_{0,1}^{m_{0,1}}\dots x_{0,n}^{m_{0,n}})\dots(x_{r-1,1}^{m_{r-1,1}}\dots x_{r-1,n}^{m_{r-1,n}})

in

{k1t=0r1(𝒟(2krxt,2k2)r(2k1)(xt,2k1))r odd,k1(t=0r1𝒟(2krxt,2k2)t=0toddr1𝒟((2k1)rxt,2k12)t=0tevenr1r(2k1)4(2xt,2k1))r even.\begin{cases}\displaystyle\prod_{k\geq 1}\prod_{t=0}^{r-1}\left(\displaystyle\mathcal{D}(2krx_{t,2k}^{2})\,\mathcal{R}_{r(2k-1)}(x_{t,2k-1})\right)&r\text{ odd},\\ \displaystyle\prod_{k\geq 1}\left(\displaystyle\prod_{t=0}^{r-1}\mathcal{D}(2krx_{t,2k}^{2})\,\prod_{\begin{subarray}{c}t=0\\ t\,\text{odd}\end{subarray}}^{r-1}\mathcal{D}((2k-1)rx_{t,2k-1}^{2})\,\prod_{\begin{subarray}{c}t=0\\ t\,\text{even}\end{subarray}}^{r-1}\mathcal{R}_{\frac{r(2k-1)}{4}}(2x_{t,2k-1})\right)&r\text{ even}.\end{cases}

Therefore, the generating function (in nn) for the sum of the number of square roots of all the conjugacy class representatives in G(r,1,n)G(r,1,n) is

{k1(𝒟(2krx4k)rr(2k1)(x2k1)r)r odd,k1(𝒟(2krx4k)r𝒟((2k1)rx4k2)r/2r(2k1)4(2x2k1)r/2)r even.\begin{cases}\displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{D}(2krx^{4k})^{r}\,\mathcal{R}_{r(2k-1)}(x^{2k-1})^{r}\right)&r\text{ odd},\\ \displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{D}(2krx^{4k})^{r}\,\mathcal{D}((2k-1)rx^{4k-2})^{r/2}\,\mathcal{R}_{\frac{r(2k-1)}{4}}(2x^{2k-1})^{r/2}\right)&r\text{ even}.\end{cases}
Proof.

Suppose 𝝀=(λ0λ1λr1)rn\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1})\models_{r}n and π\pi is an element with cycle type 𝝀\bm{\lambda}. Then Proposition 6.3 gives the conditions under which π\pi has a square root. Thus, write each of these partitions in frequency notation as

(42) λt={1mt,1,22mt,2,3mt,3,42mt,4,r is odd, or both r and t are even,12mt,1,22mt,2,32mt,3,42mt,4,r is even and t is odd.\lambda^{t}=\begin{cases}\langle 1^{m_{t,1}},2^{2m_{t,2}},3^{m_{t,3}},4^{2m_{t,4}},\dots\rangle&\text{$r$ is odd, or both $r$ and $t$ are even},\\ \langle 1^{2m_{t,1}},2^{2m_{t,2}},3^{2m_{t,3}},4^{2m_{t,4}},\dots\rangle&\text{$r$ is even and $t$ is odd}.\end{cases}

If only one of the mt,jm_{t,j}’s is non-zero, the number of square roots is given by Proposition 6.5.

We now have to argue that the square roots for the cycles in π\pi of colour tt can be formed independently of other cycles of different lengths or colors. When the cycles are paired up to form an even cycle, they remain of color tt by Lemma 6.2(1). But if a cycle stays of the same size under the square root operation, and that can only happen if the cycle is odd, then it changes color (unless t=0t=0) to t/2t/2 by Lemma 6.2(2). In either case, the nature of this cycle in the square root is unaffected by the other cycles. Therefore, the number of square roots for π\pi can be computed by taking a product over all colors and all cycle lengths independently.

By the previous paragraph, the generating function of the number of square roots is the product of those for different cycles of different colors. Even cycles (2k)(2k) of color tt with multiplicity 2mt,2k2m_{t,2k} contribute xt,2k2mt,2kx_{t,2k}^{2m_{t,2k}} to the generating function and we get, by summing over mt,2km_{t,2k} and using Proposition 6.5(1) and (11), a factor of 𝒟(2krxt,2k2)\mathcal{D}(2krx_{t,2k}^{2}) for each tt. This does not depend on the parity of rr.

When rr is odd, odd cycles (2k1)(2k-1) of color tt with multiplicity mt,2k1m_{t,2k-1} contribute xt,2k1mt,2k1x_{t,2k-1}^{m_{t,2k-1}} to the generating function. By summing over mt,2k1m_{t,2k-1} and using Proposition 6.5(2) and (12), we get a factor of r(2k1)(xt,2k1)\mathcal{R}_{r(2k-1)}(x_{t,2k-1}) for each tt. This proves the formula when rr is odd.

Suppose now that both rr and the color tt are even. Then odd cycles (2k1)(2k-1) of color tt with multiplicity mt,2k1m_{t,2k-1} contribute xt,2k1mt,2k1x_{t,2k-1}^{m_{t,2k-1}} to the generating function. From the formula in Proposition 6.5(3), the part of the summand with exponent jj is r(2k1)/4r(2k-1)/4 and we have an extra factor of 2mt,2k12^{m_{t,2k-1}}. Therefore, summing over mt,2k1m_{t,2k-1} and using (12) will give us r(2k1)/4(2xt,2k1)\mathcal{R}_{r(2k-1)/4}(2x_{t,2k-1}) for every even tt.

The last case is when rr is even and the color tt is odd. Then odd cycles (2k1)(2k-1) of color tt with multiplicity 2mt,2k12m_{t,2k-1} contribute xt,2k12mt,2k1x_{t,2k-1}^{2m_{t,2k-1}} to the generating function. This calculation is very similar to the case of even cycles. Comparing Proposition 6.5(1) and Proposition 6.5(4), we obtain a factor of 𝒟((2k1)rxt,2k12)\mathcal{D}((2k-1)rx_{t,2k-1}^{2}) for each even tt. This explains all the factors in the case when rr is even.

To obtain the generating function, replace each xt,kx_{t,k} by xkx^{k}, completing the proof. ∎

6.2. Generating function for character table sums

In contrast with the case of SnS_{n}, the square root function does not give column sums for character table of G(r,1,3)G(r,1,3), r>2r>2 as the group has non-real irreducible characters [APR10]. Given π=(z1,z2,,zn;σ)G(r,1,n)\pi=(z_{1},z_{2},\ldots,z_{n};\sigma)\in G(r,1,n), define the bar operation as

π¯:=(z1,,zn;σ).\overline{\pi}:=(-z_{1},\ldots,-z_{n};\sigma).

An element gG(r,1,n)g\in G(r,1,n) is said to have an absolute square root if there exists πG(r,1,n)\pi\in G(r,1,n) such that ππ¯=g\pi\,\overline{\pi}=g. We will call the element ππ¯\pi\,\overline{\pi} the absolute square of π\pi. Note that π¯π=(ππ¯)¯\overline{\pi}\,\pi=\overline{(\pi\,\overline{\pi})}. The next result describes columns sum for G(r,1,n)G(r,1,n) in terms of absolute square roots.

Theorem 6.7.

[APR10, Theorem 3.4] Let {χ𝛌𝛌rn}\{\chi_{\bm{\lambda}}\mid\bm{\lambda}\models_{r}n\} be the set of irreducible characters of G(r,1,n)G(r,1,n). Then

𝝀rnχ𝝀(g)=|{πG(r,1,n)ππ¯=g}|gG(r,1,n).\sum_{\bm{\lambda}\models_{r}n}\chi_{\bm{\lambda}}(g)=|\{\pi\in G(r,1,n)\mid\pi\,\overline{\pi}=g\}|\quad\forall g\in G(r,1,n).

Let r,q,nr,q,n are positive integers such that qrq\mid r. Then the complex reflection group G(r,q,n)G(r,q,n) is defined by

G(r,q,n):={π=(z1,,zn;σ)G(r,1,n)i=1nzi0 mod q}.G(r,q,n):=\left\{\pi=(z_{1},\ldots,z_{n};\sigma)\in G(r,1,n)\mid\sum_{i=1}^{n}z_{i}\equiv 0\text{ mod }q\right\}.

The group G(r,q,n)G(r,q,n) is a normal subgroup of G(r,1,n)G(r,1,n) with index qq. Special cases of G(r,q,n)G(r,q,n) where q2q\geq 2 include the demioctahedral groups Dn=G(2,2,n)D_{n}=G(2,2,n) and the dihedral groups Dih(n)=G(n,n,2)\operatorname{Dih}(n)=G(n,n,2).

Remark 6.8.

By Theorem 6.7, all the column sums are nonnegative integers for G(r,1,n)G(r,1,n). The same is not true for all G(r,q,n)G(r,q,n). For example, there are six columns in the character table of G(9,3,3)G(9,3,3) with column sum 6-6. Caselli [Cas10, Section 4] building on work of Bump–Ginzburg [BG04] proved that

(43) VIrr(G(r,q,n))χV(g)=|{πG(r,q,n)ππ¯=g}|gG(r,q,n)\sum_{V\in\mathrm{Irr}(G(r,q,n))}\chi_{V}(g)=|\{\pi\in G(r,q,n)\mid\pi\,\overline{\pi}=g\}|\quad\forall g\in G(r,q,n)

if and only if gcd(q,n)2\gcd(q,n)\leq 2. This result completely classifies complex reflection groups whose column sums are given by absolute square roots.

Theorem 6.9.

Suppose r,q,nr,q,n are positive integers such that qrq\mid r and gcd(q,n)2\gcd(q,n)\leq 2. Then 1.1 holds for G(r,q,n)G(r,q,n).

Proof.

By Remark 6.8, the column sums are nonnegative integers for G=G(r,q,n)G=G(r,q,n). Thus, s(G)Γe(G)s(G)\geq\Gamma_{e}(G). For the remaining part, assume that s(G)=Γe(G)s(G)=\Gamma_{e}(G). We will show that GG must be abelian.

Since s(G)=Γe(G)s(G)=\Gamma_{e}(G), by (43) we have ππ¯=e\pi\,\overline{\pi}=e for all π=(z1,,zn;σ)G\pi=(z_{1},\ldots,z_{n};\sigma)\in G, where e=(0,,0;12n)e=(0,\ldots,0;12\dots n) is the identity element in GG and 12n12\dots n is the identity in SnS_{n} in one-line notation. By (37), we have σ2=12n\sigma^{2}=12\dots n for all σSn\sigma\in S_{n}. Thus, SnS_{n} is abelian and this happens only when n2n\leq 2.

If n=1n=1, then GG is an index qq subgroup of the cyclic group r\mathbb{Z}_{r} and so GG is abelian. Let n=2n=2. If r=1r=1, then G=G(1,1,2)G=G(1,1,2) is the abelian group S2S_{2}. If r=2r=2, GG is either G(2,1,2)=Dih(4)G(2,1,2)=\operatorname{Dih}(4) or G(2,2,2)=Dih(2)G(2,2,2)=\operatorname{Dih}(2). For the former nonabelian group, the inequality can be verified directly. The latter is an abelian group.

Finally, consider the case of G=G(r,q,2)G=G(r,q,2) with r>2r>2. Observe that the element π=(r1,1;(1,2))G\pi=(r-1,1;(1,2))\in G is an absolute square root of g=(r2,2;12)g=(r-2,2;12), that is ππ¯=g\pi\,\overline{\pi}=g. Since r2r\neq 2, gg is not the identity element. Now, by (43) we conclude that the column sum corresponding to gg is positive and thus s(G)>Γe(G)s(G)>\Gamma_{e}(G). ∎

By analyzing absolute square roots, we will provide generating functions for number of columns with zero sums and the character table sums of G(r,1,n)G(r,1,n).

Lemma 6.10.
  1. (1)

    The absolute square of a cycle of odd length dd (of any color) is a cycle of the same length of color 0.

  2. (2)

    The absolute square of a cycle of even length dd (of any color) is a product of two cycles, each of length d/2d/2, such that sum of their colors is zero.

Proof.

Let π=(z1,,zd;σ)G(r,1,d)\pi=(z_{1},\ldots,z_{d};\sigma)\in G(r,1,d) where σ=(d,d1,,1)\sigma=(d,d-1,\ldots,1). Then, its absolute square is ππ¯=(z1z2,,zd1zd,zdz1;σ2)\pi\,\overline{\pi}=(z_{1}-z_{2},\ldots,z_{d-1}-z_{d},z_{d}-z_{1};\sigma^{2}).

When dd is odd, σ2=(d,d2,,3,1,d1,d3,,2)\sigma^{2}=(d,d-2,\ldots,3,1,d-1,d-3,\ldots,2) and the color of σ2\sigma^{2} is zero as (z1z2)++(zd1zd)+(zdz1)=0(z_{1}-z_{2})+\cdots+(z_{d-1}-z_{d})+(z_{d}-z_{1})=0. Similarly, when dd is even, σ2=(d,d2,,4,2)(d1,d3,,3,1)\sigma^{2}=(d,d-2,\ldots,4,2)(d-1,d-3,\ldots,3,1). In this case notice that the sum of the colors of both cycles is zero. ∎

The following result characterizes columns of the character table of G(r,1,n)G(r,1,n) having non-zero sums.

Proposition 6.11.

An rr-partite partition 𝛌=(λ0λ1λr1)rn\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1})\models_{r}n is the cycle type of an absolute square in G(r,1,n)G(r,1,n) if and only if the following hold:

  1. (1)

    each even part in λ0\lambda^{0} has even multiplicity,

  2. (2)

    λt=λrt\lambda^{t}=\lambda^{r-t} for all 1t<r/21\leq t<r/2, and

  3. (3)

    each part in λr/2\lambda^{r/2} has even multiplicity when rr is even.

Proof.

Let π\pi be an absolute square having cycle type 𝝀=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1}). By Lemma 6.10, all even parts in λ0\lambda^{0} must come in pairs, enforcing the even multiplicity condition. For the same reason, all parts in λr/2\lambda^{r/2} must come in pairs when rr is even. This proves the first and the third part. The second part follows directly from Lemma 6.10(2). For the converse, we can use Lemma 6.10 to construct an explicit absolute square root of a given element π\pi with cycle type 𝝀\bm{\lambda} satisfying conditions (1),(2) and (3). This construction is demonstrated in the proof of Lemma 6.13. ∎

The following result extends Bessenrodt–Olsson’s result Proposition 3.4 from SnS_{n} to G(r,1,n)G(r,1,n).

Theorem 6.12.

The generating function for the number of conjugacy classes of G(r,1,n)G(r,1,n) with nonzero column sum is

{i=11(1q2i1)(1q4i)(1qi)(r1)/2r odd, i=11(1q2i1)(1q4i)(1q2i)(1qi)(r2)/2r even. \begin{cases}\displaystyle\prod_{i=1}^{\infty}\frac{1}{(1-q^{2i-1})(1-q^{4i})(1-q^{i})^{(r-1)/2}}&r\text{ odd, }\\ \displaystyle\prod_{i=1}^{\infty}\frac{1}{(1-q^{2i-1})(1-q^{4i})(1-q^{2i})(1-q^{i})^{(r-2)/2}}&r\text{ even. }\end{cases}
Proof.

We first consider the case when rr is odd. Let

U1(n)={𝝀=(λ0λ1λr1)rnm2j(λ0) is even for each j,λi=λri for each 1i(r1)/2}.U_{1}(n)=\{\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\dots\mid\lambda^{r-1})\models_{r}n\mid m_{2j}(\lambda^{0})\mbox{ is even for each }j,\lambda^{i}=\lambda^{r-i}\mbox{ for each }1\leq i\leq(r-1)/2\}.

By Proposition 6.11, an element πG(r,1,n)\pi\in G(r,1,n) with cycle type 𝝀=(λ0λ1λr1)\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\dots\mid\lambda^{r-1}) is the absolute square of some element if and only if 𝝀U1(n)\bm{\lambda}\in U_{1}(n). To determine the generating function for U1(n)U_{1}(n), we define the set

U2(n)={𝝀=(λ0λ1λr1)rnm4j+2(λ0)=0 for each j,λi=λri for each 1i(r1)/2}.U_{2}(n)=\{\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\dots\mid\lambda^{r-1})\models_{r}n\mid m_{4j+2}(\lambda^{0})=0\mbox{ for each }j,\lambda^{i}=\lambda^{r-i}\mbox{ for each }1\leq i\leq(r-1)/2\}.

Recall the map ff defined in (6). Using that, we define the map f:U1(n)U2(n)f^{*}:U_{1}(n)\mapsto U_{2}(n) as

f(λ0λ1λr1)=(f(λ0)λ1λr1).f^{*}(\lambda^{0}\mid\lambda^{1}\mid\dots\mid\lambda^{r-1})=(f(\lambda^{0})\mid\lambda^{1}\mid\dots\mid\lambda^{r-1}).

By Corollary 3.3, the map ff^{*} maps U1(n)U_{1}(n) to U2(n)U_{2}(n) bijectively. Therefore, the generating function for the number of partitions in λ0\lambda^{0} is

i=11(1q2i1)(1q4i)\prod_{i=1}^{\infty}\frac{1}{(1-q^{2i-1})(1-q^{4i})}

Moreover, as there is no restriction on the number of parts of λi\lambda^{i} for 1i(r1)/21\leq i\leq(r-1)/2, the generating function for the number of partitions for each such λi\lambda^{i} is

(44) i=111qi.\prod_{i=1}^{\infty}\frac{1}{1-q^{i}}.

As λi=λri\lambda^{i}=\lambda^{r-i}, we have

n=0|U1(n)|qn=n=0|U2(n)|qn=i=11(1q2i1)(1q4i)(1qi)(r1)/2.\sum_{n=0}^{\infty}|U_{1}(n)|q^{n}=\sum_{n=0}^{\infty}|U_{2}(n)|q^{n}=\displaystyle\prod_{i=1}^{\infty}\frac{1}{(1-q^{2i-1})(1-q^{4i})(1-q^{i})^{(r-1)/2}}.

This completes the proof for odd rr.

When rr is even, we get an extra factor because of λr/2\lambda^{r/2}. From Proposition 6.11(3), we know that each part of λr/2\lambda^{r/2} has even multiplicity. Therefore, using the map gg defined in (20), we have that the generating function for the number of partitions in λr/2\lambda^{r/2} is also

i=111q2i,\prod_{i=1}^{\infty}\frac{1}{1-q^{2i}},

completing the proof. ∎

Lemma 6.13.

[APR10, Observation 4.2]

  1. (1)

    Suppose dd is odd. Consider an element πG(r,1,d)\pi\in G(r,1,d) with cycle type 𝝀\bm{\lambda} such that λ0=(d)\lambda^{0}=(d). Then π\pi has rr absolute square roots.

  2. (2)

    Consider an element πG(r,1,2d)\pi\in G(r,1,2d) with cycle type 𝝀\bm{\lambda} such that λi=λri=(d)\lambda^{i}=\lambda^{r-i}=(d) for some ii. Then π\pi has rdrd absolute square roots.

Proof.

Let π=(0,,0;σ)\pi=(0,\ldots,0;\sigma), where σ=(d,d2,,1,d1,d3,,4,2))G(r,1,d)\sigma=(d,d-2,\ldots,1,d-1,d-3,\ldots,4,2))\in G(r,1,d). Since dd is odd, σ\sigma has a unique square root (d,d1,,1)(d,d-1,\ldots,1). Let (z1,,zd;(d,d1,,1))(z_{1},\ldots,z_{d};(d,d-1,\ldots,1)) be an absolute square root of π\pi. By definition, we have zizi+1=0z_{i}-z_{i+1}=0 for 1id11\leq i\leq d-1 and zdz1=0z_{d}-z_{1}=0. Therefore any choice of z1z_{1} is valid and fixes all other ziz_{i}’s. Therefore, we have rr possible absolute square roots of π\pi.

Next, let π=(t1,0,,0,t2;σ)\pi=(t_{1},0,\ldots,0,t_{2};\sigma), where σ=(2d,2d2,,4,2)(2d1,2d3,,3,1))\sigma=(2d,2d-2,\ldots,4,2)(2d-1,2d-3,\ldots,3,1)) such that t1+t2=0t_{1}+t_{2}=0. In S2dS_{2d}, σ\sigma has dd square roots. Let (z1,,z2d;(2d,2d1,,1))(z_{1},\ldots,z_{2d};(2d,2d-1,\ldots,1)) be an absolute square root of π\pi. Then we get the following system of linear equations:

z1z2=t1,z2z3=0,,z2d1z2d=0,z2dz1=t2.z_{1}-z_{2}=t_{1},z_{2}-z_{3}=0,\ldots,z_{2d-1}-z_{2d}=0,z_{2d}-z_{1}=t_{2}.

Observe that the above system has rr solutions because every choice of z2z_{2} is valid and fixes all other values. For each square root of σ\sigma, we have rr absolute square roots of π\pi. This concludes the proof. ∎

Proposition 6.14.

Given a positive integer rr and tt such that 0tr10\leq t\leq r-1, the number of absolute square roots of an element π\pi whose cycles all have the same length \ell is as follows.

  1. (1)

    When =2k\ell=2k and there are 2m2m cycles of color 0, this is given by (2m1)!!(2kr)m(2m-1)!!\,(2kr)^{m}.

  2. (2)

    When =2k+1\ell=2k+1 and there are mm cycles of color 0, this is given by

    j=0m2(m2j)(2j1)!!(2k+1)jrmj.\sum_{j=0}^{\lfloor\frac{m}{2}\rfloor}\binom{m}{2j}\,(2j-1)!!\,(2k+1)^{j}\,r^{m-j}.
  3. (3)

    When =k\ell=k and there are mm cycles of colors tt and rtr-t each (where ar/2a\neq r/2), this is given by m!(kr)mm!\,(kr)^{m}.

  4. (4)

    For even rr, when =k\ell=k and there are 2m2m cycles of color r/2r/2, this is given by (2m1)!!(kr)m(2m-1)!!\,(kr)^{m}.

Proof.

First suppose =2k\ell=2k,and there are 2m2m cycles of color 0. Any absolute square root of π\pi will have mm cycles of length 4k4k and any cycle of length 4k4k comes from pairing two cycles of length 2k2k. This pairing can be done in (2m1)!!(2m-1)!! ways. Moreover, for every pairing, the cycles can be merged in 2k2k ways and by Lemma 6.13, the color of the (4k)(4k)-cycle can be any t[0,r1]t\in[0,r-1]. This completes the proof of (1). The proof of (4) follows via a very similar argument.

Now suppose =2k+1\ell=2k+1 and there are mm cycles of color 0. Note that any absolute square root of π\pi has some cycles of length 2k+12k+1 of any color, and some cycles of length 4k+24k+2 of any color by Lemma 6.10. We get a factor of rr for the color of every (2k+1)(2k+1)-cycle. Any cycle of length 4k+24k+2 again comes from pairing two cycles of length 2k+12k+1. So, we can merge jj pairs by first choosing 2j2j cycles of length 2k+12k+1 and then we can combine them in (2j1)!!(2j-1)!! ways and then merge them in 2k+12k+1 ways each. Moreover, for every pairing, by Lemma 6.13(2), the color of the (4k+2)(4k+2)-cycle can be chosen arbitrarily. This completes the proof of (2).

The proof of (3) follows by the observation that we have to match one cycle of color tt to another cycle of color rtr-t and then merge them. The number of matchings is clearly m!m! and the number of ways of merging is kmk^{m} and finally by Lemma 6.13(2), the color of the (2k)(2k)-cycle can be chosen in rr ways. This completes the proof. ∎

Adin–Postnikov–Roichman [APR10, Corollary 4.3] also give a formula to count the number of absolute square roots of any element in G(r,1,n)G(r,1,n). Using Proposition 6.14, we extend their result to determine the sum of the character table in terms of generating functions. To do so, we also need the classic generating function for the factorials as an S-fraction due to Euler [Eul60] given by

(45) (x)=S(x;(n+12))=n0n!xn=11x1x12x12x.\mathcal{F}(x)=S\left(x;\left(\left\lceil\frac{n+1}{2}\right\rceil\right)\right)=\sum_{n\geq 0}n!\,x^{n}=\frac{1}{\displaystyle 1-\frac{x}{\displaystyle 1-\frac{x}{\displaystyle 1-\frac{2x}{1-\frac{2x}{\ddots}}}}}.

Let 𝝀=(λ0λr1)rn\bm{\lambda}=(\lambda^{0}\mid\dots\mid\lambda^{r-1})\models_{r}n be an rr-partite partition and Γ𝝀\Gamma_{\bm{\lambda}} be the column sum in the character table corresponding to the cycle type 𝝀\bm{\lambda}. By Theorem 6.7, Γ𝝀\Gamma_{\bm{\lambda}} is the number of absolute square roots of an element with cycle type 𝝀\bm{\lambda}. Also, let 𝒮r(x)\mathcal{S}^{r}(x) be the ordinary generating function of the sequence of character table sums (s(G(r,1,n)))n0(s(G(r,1,n)))_{n\geq 0}. Note that 𝒮2(x)=𝒮B(x)\mathcal{S}^{2}(x)=\mathcal{S}^{B}(x).

Theorem 6.15.

Write each partition in the rr-partite partition 𝛌=(λ0λ1λr1)rn\bm{\lambda}=(\lambda^{0}\mid\lambda^{1}\mid\ldots\mid\lambda^{r-1})\models_{r}n in frequency notation, with λt=1mt,1,2mt,2,\lambda^{t}=\langle 1^{m_{t,1}},2^{m_{t,2}},\dots\rangle for 0tr/20\leq t\leq r/2 and λt=λrt\lambda^{t}=\lambda^{r-t} for r/2<tr1r/2<t\leq r-1. Then Γ𝛌\Gamma_{\bm{\lambda}} is the coefficient of

(x0,1m0,1x0,nm0,n)(xr1,1mr1,1xr1,nmr1,n)(x_{0,1}^{m_{0,1}}\dots x_{0,n}^{m_{0,n}})\dots(x_{r-1,1}^{m_{r-1,1}}\dots x_{r-1,n}^{m_{r-1,n}})

in

{k1(𝒟(2krx0,2k2)(2k1)/r(rx2k1)t=1(r1)/2(krxt,k2))r odd,k1(𝒟(2krx0,2k2)𝒟(rkxr/2,k2)(2k1)/r(rx2k1)t=1(r2)/2(krxt,k2))r even.\begin{cases}\displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{D}(2krx_{0,2k}^{2})\,\mathcal{R}_{(2k-1)/r}(rx_{2k-1})\,\prod_{t=1}^{(r-1)/2}\mathcal{F}(krx_{t,k}^{2})\right)&r\text{ odd},\\[14.22636pt] \displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{D}(2krx_{0,2k}^{2})\,\mathcal{D}(rkx_{r/2,k}^{2})\,\mathcal{R}_{(2k-1)/r}(rx_{2k-1})\,\prod_{t=1}^{(r-2)/2}\mathcal{F}(krx_{t,k}^{2})\right)&r\text{ even}.\end{cases}

Therefore,

𝒮r(x)={k1((krx2k)(r1)/2𝒟(2krx4k)(2k1)/r(rx2k1))r odd,k1((krx2k)(r2)/2𝒟(2krx4k)𝒟(rkx2k)(2k1)/r(rx2k1))r even.\mathcal{S}^{r}(x)=\begin{cases}\displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{F}(krx^{2k})^{(r-1)/2}\,\mathcal{D}(2krx^{4k})\,\mathcal{R}_{(2k-1)/r}(rx^{2k-1})\right)&r\text{ odd},\\ \displaystyle\prod_{k\geq 1}\left(\displaystyle\mathcal{F}(krx^{2k})^{(r-2)/2}\,\mathcal{D}(2krx^{4k})\,\mathcal{D}(rkx^{2k})\,\mathcal{R}_{(2k-1)/r}(rx^{2k-1})\right)&r\text{ even}.\end{cases}
Proof.

The strategy is similar to that in the proof of Theorem 6.6. Suppose 𝝀=(λ0λr1)\bm{\lambda}=(\lambda^{0}\mid\dots\mid\lambda^{r-1}) is the rr-partite partition indexing a conjugacy class in G(r,1,n)G(r,1,n) and π\pi be an element with cycle type 𝝀\bm{\lambda}. Then Proposition 6.11 gives the conditions under which π\pi has an absolute square root. Thus, write each of these partitions in frequency notation as

(46) λt={1m0,1,22m0,2,3m0,3,42m0,4,t=0,1mt,1,2mt,2,1t<r/2λrtr/2<tr1,12mr/2,1,22mr/2,2,r is even and t=r/2.\lambda^{t}=\begin{cases}\langle 1^{m_{0,1}},2^{2m_{0,2}},3^{m_{0,3}},4^{2m_{0,4}},\dots\rangle&t=0,\\ \langle 1^{m_{t,1}},2^{m_{t,2}},\dots\rangle&1\leq t<r/2\\ \lambda^{r-t}&r/2<t\leq r-1,\\ \langle 1^{2m_{r/2,1}},2^{2m_{r/2,2}},\dots\rangle&\text{$r$ is even and $t=r/2$}.\end{cases}

As before, the number of square roots is given by Proposition 6.14 if only one of the mt,jm_{t,j}’s is non-zero.

We again have to argue that absolute square roots of cycles of different lengths and colors in λ\lambda can be formed independently. For odd cycles, they just change color and for even cycles, they pair up and change color to form the absolute square root in specific ways. In either case, they do not depend on other cycles or colors.

The argument is very similar now to the proof of Theorem 6.6. Even (resp. odd) cycles of length 2k2k (resp. 2k12k-1) in λ0\lambda^{0} give 𝒟(2krx0,2k2)\mathcal{D}(2krx_{0,2k}^{2}) (resp. (2k1)/r(rx2k1)\mathcal{R}_{(2k-1)/r}(rx_{2k-1})) using Proposition 6.14(1) (resp. (2)). Cycles in λt=λrt\lambda^{t}=\lambda^{r-t} of length kk give (krxt,k2)\mathcal{F}(krx_{t,k}^{2}), one for each tt, by Proposition 6.14(3). Lastly, when rr is even and the cycle is of length 2k2k, we get another factor of 𝒟(krxr/2,k2)\mathcal{D}(krx_{r/2,k}^{2}) by Proposition 6.14(4).

To obtain the generating function 𝒮r(x)\mathcal{S}^{r}(x), replace each xt,kx_{t,k} by xkx^{k}. ∎

Remark 6.16.

When r=2r=2, absolute square roots are exactly the usual square roots. Thus the generating function for (snB)(s_{n}^{B}) can be obtained by setting r=2r=2 in either Theorem 6.6 or Theorem 6.15.

Acknowledgements

We thank Jyotirmoy Ganguly for helpful discussions. This work benefited immensely from Sagemath [The23] and GAP [GAP22]. We acknowledge support from the DST FIST program - 2021 [TPN - 700661]. The first author (AA) was partially supported by SERB Core grant CRG/2021/001592.

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  • [The23] The Sage Developers. SageMath, the Sage Mathematics Software System (Version 9.4), 2023. https://www.sagemath.org.
  • [Vie85] Gérard Viennot. A combinatorial theory for general orthogonal polynomials with extensions and applications. In Orthogonal polynomials and applications (Bar-le-Duc, 1984), volume 1171 of Lecture Notes in Math., pages 139–157. Springer, Berlin, 1985.

Appendix A Exceptional irreducible Coxeter groups

For each of the exceptional simple Lie groups, we list the total sum and the first column sum of their Weyl groups below.

GG Γe(G)\Gamma_{e}(G) s(G)s(G)
E6E_{6} 892 995
E7E_{7} 10,208 10,734
E8E_{8} 199,952 220,772
F4F_{4} 140 200
G2G_{2} 8 10
H2H_{2} 32 40
H3H_{3} 572 770

Note that the Weyl group of G2G_{2} is the dihedral group of order 12. In each case, it is easy to check that the group satisfied Property S.

Appendix B Small demioctahedral groups

For small demioctahedral groups, we have the following table:

GG Γe(G)\Gamma_{e}(G) s(G)s(G)
D6D_{6} 752 930
D7D_{7} 3,256 4,037
D8D_{8} 17,040 21,796
D9D_{9} 84,496 99,525
D10D_{10} 475,712 542,616
D11D_{11} 2,611,104 2,961,697
D12D_{12} 15,687,872 18,040,858
D13D_{13} 93,376,960 103,201,617
D14D_{14} 594,638,592 647,826,742
D15D_{15} 3,786,534,784 4,109,646,977

Appendix C Data for small groups

Using the SmallGroups library in GAP within SageMath, we looked at all finite groups of order up to 200. We found groups where Property S fails (listed in Section C.1) and groups where the first column sum equals the sum of the other columns (listed in Section C.2). We also found that the list of ratios s(G)/Γe(G)s(G)/\Gamma_{e}(G) among all these groups is quite small. We have listed these ratios in Section C.3.

C.1. Groups GG where s(G)>2Γe(G)s(G)>2\Gamma_{e}(G)

There are very few groups where the sum of the entries of the character table of a finite group is more than twice the sum of dimensions of its irreducible representations and we list them below. The only orders where equality holds up to order 200200 are 64,125,16264,125,162 and 192192 and there are 5,2,542,25,2,542,2 and 210210 nonisomorphic groups of these orders respectively. We list the index in the SmallGroups library for each of these orders below.

  1. 64

    : 241,242,243,244,245.241,242,243,244,245.

  2. 125

    : 3,4.3,4.

  3. 128

    : 36,37,38,39,40,41,71,72,73,74,87,88,138,139,144,145,242,243,244,245,246,247,265,266,267,36,37,38,39,40,41,71,72,73,74,87,88,138,139,144,145,242,243,244,245,246,247,265,266,267,

    268,269,287,288,289,290,291,292,293,387,388,389,390,391,392,393,394,395,396,417,418,419,268,269,287,288,289,290,291,292,293,387,388,389,390,391,392,393,394,395,396,417,418,419,

    420,421,422,423,424,425,426,427,428,429,430,431,432,433,434,435,436,527,528,560,561,562,420,421,422,423,424,425,426,427,428,429,430,431,432,433,434,435,436,527,528,560,561,562,

    560,561,562,634,635,636,637,641,642,643,644,645,646,647,740,741,764,780,781,801,802,813,560,561,562,634,635,636,637,641,642,643,644,645,646,647,740,741,764,780,781,801,802,813,

    814,836,853,854,855,859,860,861,865,866,867,912,913,922,923,931,932,933,934,935,970,971,814,836,853,854,855,859,860,861,865,866,867,912,913,922,923,931,932,933,934,935,970,971,

    1107,1108,1109,1110,1111,1112,1113,1114,1115,1345,1346,1347,1348,1349,1350,1351,1352,1353,1107,1108,1109,1110,1111,1112,1113,1114,1115,1345,1346,1347,1348,1349,1350,1351,1352,1353,

    1354,1355,1356,1357,1358,1359,1360,1361,1362,1363,1364,1365,1366,1367,1368,1369,1370,1371,1354,1355,1356,1357,1358,1359,1360,1361,1362,1363,1364,1365,1366,1367,1368,1369,1370,1371,

    1372,1373,1374,1375,1376,1377,1378,1379,1380,1381,1382,1383,1384,1385,1386,1387,1388,1389,1372,1373,1374,1375,1376,1377,1378,1379,1380,1381,1382,1383,1384,1385,1386,1387,1388,1389,

    1390,1391,1392,1393,1394,1395,1396,1397,1398,1399,1400,1401,1402,1403,1404,1405,1406,1407,1390,1391,1392,1393,1394,1395,1396,1397,1398,1399,1400,1401,1402,1403,1404,1405,1406,1407,

    1408,1409,1410,1411,1412,1413,1414,1415,1416,1417,1418,1419,1420,1421,1422,1423,1424,1425,1408,1409,1410,1411,1412,1413,1414,1415,1416,1417,1418,1419,1420,1421,1422,1423,1424,1425,

    1426,1427,1428,1429,1430,1431,1432,1433,1434,1435,1436,1437,1438,1439,1440,1441,1442,1443,1426,1427,1428,1429,1430,1431,1432,1433,1434,1435,1436,1437,1438,1439,1440,1441,1442,1443,

    1444,1445,1446,1447,1448,1449,1450,1451,1452,1453,1454,1455,1456,1457,1458,1459,1460,1461,1444,1445,1446,1447,1448,1449,1450,1451,1452,1453,1454,1455,1456,1457,1458,1459,1460,1461,

    1462,1463,1464,1465,1466,1467,1468,1469,1470,1471,1472,1473,1474,1475,1476,1477,1478,1479,1462,1463,1464,1465,1466,1467,1468,1469,1470,1471,1472,1473,1474,1475,1476,1477,1478,1479,

    1480,1481,1482,1483,1484,1485,1486,1487,1488,1489,1490,1491,1492,1493,1494,1495,1496,1497,1480,1481,1482,1483,1484,1485,1486,1487,1488,1489,1490,1491,1492,1493,1494,1495,1496,1497,

    1498,1499,1500,1501,1502,1503,1504,1505,1506,1507,1508,1509,1510,1511,1512,1513,1514,1515,1498,1499,1500,1501,1502,1503,1504,1505,1506,1507,1508,1509,1510,1511,1512,1513,1514,1515,

    1516,1517,1518,1519,1520,1521,1522,1523,1524,1525,1526,1527,1528,1529,1530,1531,1532,1533,1516,1517,1518,1519,1520,1521,1522,1523,1524,1525,1526,1527,1528,1529,1530,1531,1532,1533,

    1534,1535,1536,1537,1538,1539,1540,1541,1542,1543,1544,1545,1546,1547,1548,1549,1550,1551,1534,1535,1536,1537,1538,1539,1540,1541,1542,1543,1544,1545,1546,1547,1548,1549,1550,1551,

    1552,1553,1554,1555,1556,1557,1558,1559,1560,1561,1562,1563,1564,1565,1566,1567,1568,1569,1552,1553,1554,1555,1556,1557,1558,1559,1560,1561,1562,1563,1564,1565,1566,1567,1568,1569,

    1570,1571,1572,1573,1574,1575,1576,1577,1710,1712,1719,1727,1751,1752,1753,1754,1758,1759,1570,1571,1572,1573,1574,1575,1576,1577,1710,1712,1719,1727,1751,1752,1753,1754,1758,1759,

    1760,1800,1801,1924,1925,1926,1927,1928,1929,1930,1931,1932,1933,1934,1935,1936,1945,1946,1760,1800,1801,1924,1925,1926,1927,1928,1929,1930,1931,1932,1933,1934,1935,1936,1945,1946,

    1947,1948,1949,1950,1951,1952,1953,1954,1955,1956,1957,1966,1967,1968,1969,1970,1971,1972,1947,1948,1949,1950,1951,1952,1953,1954,1955,1956,1957,1966,1967,1968,1969,1970,1971,1972,

    1973,1974,1975,1976,1983,1984,1985,1986,1987,1988,1989,1990,1991,1992,1993,1994,1995,1996,1973,1974,1975,1976,1983,1984,1985,1986,1987,1988,1989,1990,1991,1992,1993,1994,1995,1996,

    1997,1998,1999,2000,2001,2002,2003,2004,2005,2006,2007,2008,2009,2010,2020,2021,2038,2039,1997,1998,1999,2000,2001,2002,2003,2004,2005,2006,2007,2008,2009,2010,2020,2021,2038,2039,

    2040,2041,2042,2043,2044,2045,2046,2047,2048,2049,2050,2051,2052,2053,2054,2055,2056,2057,2040,2041,2042,2043,2044,2045,2046,2047,2048,2049,2050,2051,2052,2053,2054,2055,2056,2057,

    2058,2059,2060,2061,2062,2063,2064,2065,2075,2076,2077,2078,2079,2080,2081,2082,2083,2084,2058,2059,2060,2061,2062,2063,2064,2065,2075,2076,2077,2078,2079,2080,2081,2082,2083,2084,

    2085,2086,2087,2088,2089,2098,2099,2100,2101,2102,2103,2104,2105,2106,2107,2108,2109,2116,2085,2086,2087,2088,2089,2098,2099,2100,2101,2102,2103,2104,2105,2106,2107,2108,2109,2116,

    2117,2118,2119,2120,2121,2122,2129,2130,2131,2132,2133,2134,2135,2257,2258,2259,2260,2261,2117,2118,2119,2120,2121,2122,2129,2130,2131,2132,2133,2134,2135,2257,2258,2259,2260,2261,

    2262,2263,2264,2265,2266,2267,2268,2269,2270,2271,2272,2273,2274,2275,2276,2277,2278,2279,2262,2263,2264,2265,2266,2267,2268,2269,2270,2271,2272,2273,2274,2275,2276,2277,2278,2279,

    2280,2281,2282,2283,2284,2285,2286,2287,2288,2289,2290,2291,2298,2299,2300.2280,2281,2282,2283,2284,2285,2286,2287,2288,2289,2290,2291,2298,2299,2300.

  4. 162

    : 35,162.35,162.

  5. 192

    : 30,31,32,33,34,35,36,37,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,30,31,32,33,34,35,36,37,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,

    323,324,339,341,353,356,371,375,415,424,426,435,445,470,473,474,477,598,601,608,611,614,323,324,339,341,353,356,371,375,415,424,426,435,445,470,473,474,477,598,601,608,611,614,

    617,619,623,626,628,630,633,640,641,645,648,713,718,726,733,735,748,749,757,758,759,760,617,619,623,626,628,630,633,640,641,645,648,713,718,726,733,735,748,749,757,758,759,760,

    761,762,763,764,1146,1148,1149,1150,1151,1152,1153,1154,1156,1157,1158,1160,1161,1162,1163,761,762,763,764,1146,1148,1149,1150,1151,1152,1153,1154,1156,1157,1158,1160,1161,1162,1163,

    1164,1166,1167,1168,1169,1170,1171,1172,1173,1174,1175,1176,1177,1178,1179,1180,1182,1184,1164,1166,1167,1168,1169,1170,1171,1172,1173,1174,1175,1176,1177,1178,1179,1180,1182,1184,

    1187,1188,1189,1190,1191,1192,1193,1194,1195,1196,1197,1198,1199,1200,1201,1202,1203,1204,1187,1188,1189,1190,1191,1192,1193,1194,1195,1196,1197,1198,1199,1200,1201,1202,1203,1204,

    1205,1206,1207,1209,1210,1212,1213,1214,1216,1217,1218,1219,1220,1221,1222,1223,1224,1225,1205,1206,1207,1209,1210,1212,1213,1214,1216,1217,1218,1219,1220,1221,1222,1223,1224,1225,

    1226,1228,1229,1230,1231,1233,1234,1235,1236,1237,1238,1240,1241,1242,1243,1244,1245,1248,1226,1228,1229,1230,1231,1233,1234,1235,1236,1237,1238,1240,1241,1242,1243,1244,1245,1248,

    1249,1251,1252,1253,1254,1255,1256,1257,1258,1259,1260,1261,1263,1264,1266,1267,1268,1269,1249,1251,1252,1253,1254,1255,1256,1257,1258,1259,1260,1261,1263,1264,1266,1267,1268,1269,

    1270,1271,1272,1274,1276,1277,1278,1279,1280,1281,1283,1285,1286,1288,1289,1290,1291,1292,1270,1271,1272,1274,1276,1277,1278,1279,1280,1281,1283,1285,1286,1288,1289,1290,1291,1292,

    1293,1294,1331,1332,1333,1334,1335,1336,1337,1338,1449,1450,1451,1452,1453.1293,1294,1331,1332,1333,1334,1335,1336,1337,1338,1449,1450,1451,1452,1453.

C.2. Groups GG where s(G)=2Γe(G)s(G)=2\Gamma_{e}(G)

There are very few groups where the sum of the entries of the character table of a finite group is equal to twice the sum of dimensions of its irreducible representations and we list them below. The only orders where equality holds up to order 200 are 64,128,16064,128,160 and 192192 and there are 23,642,423,642,4 and 135135 nonisomorphic groups of these orders respectively. We list the index in the SmallGroups library for each of these orders below.

  1. 64

    : 18,19,28,149,150,151,170,171,172,177,178,182,215,216,217,218,219,220,221,222,223,224,22518,19,28,149,150,151,170,171,172,177,178,182,215,216,217,218,219,220,221,222,223,224,225.

  2. 128

    : 6,7,16,17,18,19,20,21,22,23,24,25,45,107,130,194,195,196,197,198,199,200,201,202,203,2046,7,16,17,18,19,20,21,22,23,24,25,45,107,130,194,195,196,197,198,199,200,201,202,203,204,

    205,227,228,229,301,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340205,227,228,229,301,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340,

    341,342,343,344,345,346,347,348,349,350,446,447,448,449,450,451,452,453,454,455,462,463341,342,343,344,345,346,347,348,349,350,446,447,448,449,450,451,452,453,454,455,462,463,

    479,513,514,515,516,517,531,532,533,541,543,544,545,551,552,553,554,559,565,568,570,573479,513,514,515,516,517,531,532,533,541,543,544,545,551,552,553,554,559,565,568,570,573,

    579,581,626,627,629,630,631,632,633,667,668,670,675,676,678,691,692,693,695,696,697,698579,581,626,627,629,630,631,632,633,667,668,670,675,676,678,691,692,693,695,696,697,698,

    699,703,704,705,707,724,725,727,728,729,730,734,735,736,737,738,739,742,749,750,751,752699,703,704,705,707,724,725,727,728,729,730,734,735,736,737,738,739,742,749,750,751,752,

    753,754,759,760,761,762,763,769,770,771,772,776,777,778,779,782,783,784,785,792,793,794753,754,759,760,761,762,763,769,770,771,772,776,777,778,779,782,783,784,785,792,793,794,

    795,796,810,811,812,821,822,823,830,834,835,841,842,897,898,950,951,952,975,976,977,982795,796,810,811,812,821,822,823,830,834,835,841,842,897,898,950,951,952,975,976,977,982,

    983,987,1040,1041,1042,1043,1044,1045,1046,1047,1048,1049,1050,1051,1052,1053,1054,1055983,987,1040,1041,1042,1043,1044,1045,1046,1047,1048,1049,1050,1051,1052,1053,1054,1055,

    1056,1057,1058,1059,1060,1061,1062,1063,1064,1065,1066,1067,1068,1069,1135,1136,1137,11381056,1057,1058,1059,1060,1061,1062,1063,1064,1065,1066,1067,1068,1069,1135,1136,1137,1138,

    1139,1140,1141,1142,1143,1144,1145,1146,1147,1148,1149,1150,1151,1152,1153,1154,1155,11561139,1140,1141,1142,1143,1144,1145,1146,1147,1148,1149,1150,1151,1152,1153,1154,1155,1156,

    1157,1158,1159,1160,1161,1162,1163,1164,1165,1166,1167,1168,1169,1170,1171,1172,1173,11741157,1158,1159,1160,1161,1162,1163,1164,1165,1166,1167,1168,1169,1170,1171,1172,1173,1174,

    1175,1176,1177,1178,1179,1180,1181,1182,1183,1184,1185,1186,1187,1188,1189,1190,1191,11921175,1176,1177,1178,1179,1180,1181,1182,1183,1184,1185,1186,1187,1188,1189,1190,1191,1192,

    1193,1194,1195,1196,1197,1198,1199,1200,1201,1202,1203,1204,1205,1206,1207,1208,1209,12101193,1194,1195,1196,1197,1198,1199,1200,1201,1202,1203,1204,1205,1206,1207,1208,1209,1210,

    1211,1212,1213,1214,1215,1216,1217,1218,1219,1220,1221,1222,1223,1224,1225,1226,1227,12281211,1212,1213,1214,1215,1216,1217,1218,1219,1220,1221,1222,1223,1224,1225,1226,1227,1228,

    1229,1230,1231,1232,1233,1234,1235,1236,1237,1238,1239,1240,1241,1242,1243,1244,1245,12461229,1230,1231,1232,1233,1234,1235,1236,1237,1238,1239,1240,1241,1242,1243,1244,1245,1246,

    1247,1248,1249,1250,1251,1252,1253,1254,1255,1256,1257,1258,1259,1260,1261,1262,1263,12641247,1248,1249,1250,1251,1252,1253,1254,1255,1256,1257,1258,1259,1260,1261,1262,1263,1264,

    1265,1266,1267,1268,1269,1270,1271,1272,1273,1274,1275,1276,1277,1278,1279,1280,1281,12821265,1266,1267,1268,1269,1270,1271,1272,1273,1274,1275,1276,1277,1278,1279,1280,1281,1282,

    1283,1284,1285,1286,1287,1288,1289,1290,1291,1292,1293,1294,1295,1296,1297,1298,1299,13001283,1284,1285,1286,1287,1288,1289,1290,1291,1292,1293,1294,1295,1296,1297,1298,1299,1300,

    1301,1302,1303,1304,1305,1306,1307,1308,1309,1310,1311,1312,1313,1314,1315,1316,1317,13181301,1302,1303,1304,1305,1306,1307,1308,1309,1310,1311,1312,1313,1314,1315,1316,1317,1318,

    1319,1320,1321,1322,1323,1324,1325,1326,1327,1328,1329,1330,1331,1332,1333,1334,1335,13361319,1320,1321,1322,1323,1324,1325,1326,1327,1328,1329,1330,1331,1332,1333,1334,1335,1336,

    1337,1338,1339,1340,1341,1342,1343,1344,1611,1615,1616,1620,1621,1637,1653,1655,1662,16641337,1338,1339,1340,1341,1342,1343,1344,1611,1615,1616,1620,1621,1637,1653,1655,1662,1664,

    1693,1699,1705,1707,1708,1713,1715,1717,1721,1724,1725,1735,1736,1737,1738,1739,1740,17411693,1699,1705,1707,1708,1713,1715,1717,1721,1724,1725,1735,1736,1737,1738,1739,1740,1741,

    1742,1743,1744,1745,1768,1769,1770,1771,1772,1773,1774,1775,1776,1777,1778,1783,1784,17851742,1743,1744,1745,1768,1769,1770,1771,1772,1773,1774,1775,1776,1777,1778,1783,1784,1785,

    1786,1787,1788,1789,1790,1791,1792,1793,1794,1795,1809,1810,1811,1812,1813,1814,1815,18161786,1787,1788,1789,1790,1791,1792,1793,1794,1795,1809,1810,1811,1812,1813,1814,1815,1816,

    1824,1825,1826,1827,1828,1829,1830,1831,1841,1842,1843,1844,1845,1846,1847,1848,1849,18501824,1825,1826,1827,1828,1829,1830,1831,1841,1842,1843,1844,1845,1846,1847,1848,1849,1850,

    1851,1852,1853,1854,1855,1856,1857,1858,1859,1864,1865,1866,1867,1868,1869,1870,1871,18721851,1852,1853,1854,1855,1856,1857,1858,1859,1864,1865,1866,1867,1868,1869,1870,1871,1872,

    1873,1874,1880,1881,1882,1883,1884,1885,1886,1887,1888,1893,1894,1895,1896,1897,1898,19031873,1874,1880,1881,1882,1883,1884,1885,1886,1887,1888,1893,1894,1895,1896,1897,1898,1903,

    1904,1905,1906,1907,1908,1909,1910,1911,1912,1913,1914,1915,1916,1917,1918,1919,1920,19211904,1905,1906,1907,1908,1909,1910,1911,1912,1913,1914,1915,1916,1917,1918,1919,1920,1921,

    1922,1923,1937,1938,1939,1940,1941,1942,1943,1944,1958,1959,1960,1961,1962,1963,1964,19651922,1923,1937,1938,1939,1940,1941,1942,1943,1944,1958,1959,1960,1961,1962,1963,1964,1965,

    1977,1978,1979,1980,1981,1982,2177,2178,2179,2180,2181,2182,2183,2184,2185,2186,2187,21881977,1978,1979,1980,1981,1982,2177,2178,2179,2180,2181,2182,2183,2184,2185,2186,2187,2188,

    2189,2190,2191,2192,2193,2216,2217,2218,2219,2220,2221,2222,2223,2224,2225,2226,2227,22282189,2190,2191,2192,2193,2216,2217,2218,2219,2220,2221,2222,2223,2224,2225,2226,2227,2228,

    2229,2230,2231,2232,2233,2234,2235,2236,2237,2238,2239,2240,2241,2242,2243,2244,2245,22462229,2230,2231,2232,2233,2234,2235,2236,2237,2238,2239,2240,2241,2242,2243,2244,2245,2246,

    2247,2248,2249,2250,2251,2252,2253,2254,2255,2256,2317,2318.2247,2248,2249,2250,2251,2252,2253,2254,2255,2256,2317,2318.

  3. 160

    : 132,135,136,139.132,135,136,139.

  4. 192

    : 25,71,90,116,119,143,144,153,261,262,271,272,273,274,381,384,385,386,455,456,457,592,59325,71,90,116,119,143,144,153,261,262,271,272,273,274,381,384,385,386,455,456,457,592,593,

    594,595,596,599,602,603,604,605,606,609,613,616,622,625,631,634,642,643,646,649,650,653594,595,596,599,602,603,604,605,606,609,613,616,622,625,631,634,642,643,646,649,650,653,

    693,694,696,719,736,751,800,801,802,803,804,805,901,902,903,922,923,924,929,930,934,1042693,694,696,719,736,751,800,801,802,803,804,805,901,902,903,922,923,924,929,930,934,1042,

    1052,1053,1059,1069,1074,1077,1078,1084,1085,1093,1094,1119,1120,1121,1123,1141,1142,11451052,1053,1059,1069,1074,1077,1078,1084,1085,1093,1094,1119,1120,1121,1123,1141,1142,1145,

    1147,1155,1159,1163,1165,1181,1183,1185,1186,1208,1211,1215,1227,1232,1239,1246,1247,12501147,1155,1159,1163,1165,1181,1183,1185,1186,1208,1211,1215,1227,1232,1239,1246,1247,1250,

    1262,1265,1273,1275,1282,1284,1287,1363,1364,1375,1384,1389,1392,1394,1395,1396,1397,14231262,1265,1273,1275,1282,1284,1287,1363,1364,1375,1384,1389,1392,1394,1395,1396,1397,1423,

    1424,1425,1426,1427,1428,1429,1430,1431,1432,1433,1524,1525,1526,1527.1424,1425,1426,1427,1428,1429,1430,1431,1432,1433,1524,1525,1526,1527.

C.3. Set of distinct ratios s(G)/Γe(G)s(G)/\Gamma_{e}(G) up to order 200200

Among all nonisomorphic groups of order up to 200200, of which there are 60656065, we find only 176176 distinct ratios of s(G)/Γe(G)s(G)/\Gamma_{e}(G). These are listed in increasing order below:

1,31/28,7/6,19/16,31/26,11/9,5/4,19/15,51/40,13/10,37/28,4/3,11/8,25/18,7/5,17/12,10/7,23/16,1,31/28,7/6,19/16,31/26,11/9,5/4,19/15,51/40,13/10,37/28,4/3,11/8,25/18,7/5,17/12,10/7,23/16,

13/9,29/20,16/11,35/24,19/13,41/28,22/15,47/32,25/17,53/36,28/19,59/40,31/21,65/44,34/23,71/48,13/9,29/20,16/11,35/24,19/13,41/28,22/15,47/32,25/17,53/36,28/19,59/40,31/21,65/44,34/23,71/48,

37/25,77/52,40/27,83/56,43/29,89/60,46/31,95/64,49/33,101/68,52/35,107/72,55/37,113/76,58/39,37/25,77/52,40/27,83/56,43/29,89/60,46/31,95/64,49/33,101/68,52/35,107/72,55/37,113/76,58/39,

119/8061/41,125/84,64/43,131/88,67/45,137/92,70/47,143/96,73/49,149/100,76/51,3/2,41/27,38/25,119/8061/41,125/84,64/43,131/88,67/45,137/92,70/47,143/96,73/49,149/100,76/51,3/2,41/27,38/25,

32/21,26/17,23/15,20/13,37/24,17/11,31/20,14/9,25/16,47/30,11/7,19/12,73/46,35/22,43/27,51/32,32/21,26/17,23/15,20/13,37/24,17/11,31/20,14/9,25/16,47/30,11/7,19/12,73/46,35/22,43/27,51/32,

8/5,53/33,71/44,21/13,34/21,73/45,13/8,83/51,44/27,103/63,18/11,23/14,43/26,53/32,73/44,5/3,8/5,53/33,71/44,21/13,34/21,73/45,13/8,83/51,44/27,103/63,18/11,23/14,43/26,53/32,73/44,5/3,

67/40,57/34,47/28,37/22,59/35,27/16,22/13,61/36,39/23,17/10,29/17,41/24,12/7,79/46,55/32,19/11,67/40,57/34,47/28,37/22,59/35,27/16,22/13,61/36,39/23,17/10,29/17,41/24,12/7,79/46,55/32,19/11,

26/15,33/19,40/23,7/4,51/29,23/13,85/48,62/35,55/31,16/9,25/14,34/19,43/24,115/64,9/5,101/56,26/15,33/19,40/23,7/4,51/29,23/13,85/48,62/35,55/31,16/9,25/14,34/19,43/24,115/64,9/5,101/56,

65/36,47/26,29/16,20/11,53/29,64/35,11/6,35/19,24/13,13/7,28/15,47/25,32/17,17/9,121/64,36/19,65/36,47/26,29/16,20/11,53/29,64/35,11/6,35/19,24/13,13/7,28/15,47/25,32/17,17/9,121/64,36/19,

19/10,99/52,40/21,23/12,25/13,52/27,31/16,33/17,35/18,37/19,2,65/32,35/17,29/14,25/12,23/11,19/10,99/52,40/21,23/12,25/13,52/27,31/16,33/17,35/18,37/19,2,65/32,35/17,29/14,25/12,23/11,

21/10,40/19,36/17,17/8,28/13,13/6,35/16,11/5,20/9,9/4,25/11,16/7,7/3,40/17,8/3,25/9.21/10,40/19,36/17,17/8,28/13,13/6,35/16,11/5,20/9,9/4,25/11,16/7,7/3,40/17,8/3,25/9.