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On the Hurwitz action in finite Coxeter groups

  • Barbara Baumeister EMAIL logo , Thomas Gobet , Kieran Roberts and Patrick Wegener
Published/Copyright: June 15, 2016

Abstract

We provide a necessary and sufficient condition on an element of a finite Coxeter group to ensure the transitivity of the Hurwitz action on its set of reduced decompositions into products of reflections. We show that this action is transitive if and only if the element is a parabolic quasi-Coxeter element. We call an element of the Coxeter group parabolic quasi-Coxeter element if it has a factorization into a product of reflections that generate a parabolic subgroup. We give an unusual definition of a parabolic subgroup that we show to be equivalent to the classical one for finite Coxeter groups.

1 Introduction

This paper is concerned with the so-called dual approach to Coxeter groups. A dual Coxeter system is a Coxeter group together with a generating set consisting of all the reflections in the group, that is, the set of conjugates of all the elements of a simple system.

There are several motivations for studying dual Coxeter systems. They were introduced by Bessis [3] and independently by Brady and Watt [8, 10]. The dual Coxeter systems are crucial in the theory of dual braid monoids, which are alternative braid monoids embedding in the Artin–Tits group attached to a finite Coxeter group (that is, a spherical Artin–Tits group) and providing an alternative Garside structure of it. The latter allows a new presentation of the group and thereby for instance to get better solutions to the word problem in the spherical Artin–Tits groups (see [5, 3]). Each dual braid monoid depends on a choice of a Coxeter element and its poset of simple elements ordered by left-divisibility is isomorphic to the generalized noncrossing partition lattice with respect to that Coxeter element (see [3]).

Bessis [4] later generalized these notions to complex reflections groups and their braid groups where the dual approach is natural. Indeed, there is in general no canonical choice of a simple system for a complex reflection group.

Having replaced the set of simple generators of a Coxeter group by the whole set of reflections in the Coxeter group (and in the Artin–Tits group), one needs to find new sets of relations between these new generators that define the respective groups. The idea is to take the so-called dual braid relations [3]. Unlike the classical braid relations, a dual braid relation can involve three generators and has the form ab=ca (or ba=ac), where a,b and c are reflections.

In the classical case Matsumoto’s Lemma [30] allows one to pass from any reduced decomposition of an element to any other one by successive applications of braid relations. The same question can be asked for reduced decompositions with respect to the new set of generators, and can be studied using the so-called Hurwitz action on reduced decompositions.

Let us say a bit more on this action. Let G be an arbitrary group, n2. There is an action of the braid group n on n strands on Gn where the standard generator σin which exchanges the i-th and (i+1)-th strands acts as

σi(g1,,gn):=(g1,,gi-1,gigi+1gi-1,gi,gi+2,,gn).

Notice that the product of the entries stays unchanged and that all the tuples in a given orbit generate the same subgroup of the Coxeter group. This action is called the Hurwitz action since it was first studied by Hurwitz in 1891 ([23]) in the case where G=𝔖n.

Two elements g,hGn are called Hurwitz equivalent if there is a braid βn such that βg=h. It has been shown by Liberman and Teicher (see [29]) that the question of whether two elements in Gn are Hurwitz equivalent or not is undecidable in general. Nevertheless, there are results in many cases (see for instance [19] and [35]). The Hurwitz action also plays a role in algebraic geometry, more precisely in the braid monodromy of a projective curve (e.g., see [28, 11] or [25]).

In the case of finite Coxeter groups, the Hurwitz action can be restricted to the set of minimal length decompositions of a given fixed element w into products of reflections. Given a reduced decomposition (t1,,tk) of w where t1,,tk are reflections (that is, w=t1tk with k minimal), the generator σin then acts as

σi(t1,,tk):=(t1,,ti-1,titi+1ti,ti,ti+2,,tk).

The right-hand side is again a reduced decomposition of w. In fact, we see that the braid group generator σi acts on the i-th and (i+1)-th entries by replacing (ti,ti+1) by (titi+1ti,ti) which corresponds exactly to a dual braid relation. Hence determining whether one can pass from any reduced decomposition of an element to any other just by applying a sequence of dual braid relations is equivalent to determining whether the Hurwitz action on the set of reduced decompositions of the element is transitive.

The transitivity of the Hurwitz action on the set of reduced decompositions has long been known to be true for a family of elements commonly called parabolic Coxeter elements (note that there are several inequivalent definitions of these in the literature). For more on the topic we refer to [2], and the references therein, where a simple proof of the transitivity of the Hurwitz action was shown for (suitably defined) parabolic Coxeter elements in a (not necessarily finite) Coxeter group. See also [24]. The Hurwitz action in Coxeter groups has also been studied outside the context of parabolic Coxeter elements (see [37, 22, 31] – be aware that there are mistakes in [22]).

The aim of this paper is to provide a necessary and sufficient condition on an element of a finite Coxeter group to ensure the transitivity of the Hurwitz action on its set of reduced decompositions. We call an element of a Coxeter group a parabolic quasi-Coxeter element if it admits a reduced decomposition which generates a parabolic subgroup. A quasi-Coxeter element is an element admitting a reduced decomposition which generates the whole Coxeter group.

The main result of this paper is the following characterization.

Theorem 1.1

Let (W,T) be a finite, dual Coxeter system of rank n and let wW. The Hurwitz action on RedT(w) is transitive if and only if w is a parabolic quasi-Coxeter element for (W,T).

The following theorem is an immediate consequence.

Theorem 1.2

Let (W,T) be a finite, dual Coxeter system of rank n and let wW. If w is a quasi-Coxeter element for (W,T), then for each(t1,,tn)RedT(w) one has W=t1,,tn.

The proof that being a parabolic quasi-Coxeter element is a necessary condition to ensure the transitivity of the Hurwitz action is uniform. The other direction is case-by-case. In the simply laced types we first prove Theorem 1.2 (see Theorem 6.1) and use it to prove the second direction of Theorem 1.1.

Another consequence of Theorem 1.1 and of work of Dyer [16, Theorem 3.3] is the following.

Corollary 1.3

Let (W,T) be a dual Coxeter system and let wW. Further, let (t1,,tm)RedT(w), set W:=t1,,tm and T:=WT. If W is finite, then the Hurwitz action on RedT(w) is transitive.

It is an open question whether this statement remains true if there is no finiteness assumption on W.

The structure of the paper is as follows. We adopt the approach and terminology introduced in [2] (see Section 2). In particular, we use an unusual definition of parabolic subgroup, which we show in Section 4 (after recalling some well-known facts on root systems in Section 3) to be equivalent to the classical definition for finite Coxeter groups and (as a consequence of results in [18]) for a large family of irreducible infinite Coxeter groups, the so-called irreducible 2-spherical Coxeter groups. As a byproduct, we obtain some results on parabolic subgroups of finite Coxeter groups. In particular, we show the following:

Proposition 1.4

Let (W,S) be a finite Coxeter system and ST such that (W,S) is a simple system. Then the parabolic subgroups with respect to S coincide with those with respect to S.

Given a root subsystem Φ of a given root system Φ, we discuss in Section 5 the relationship between the corresponding Coxeter groups and root lattices, especially in the simply laced types. These results are needed later in Section 6. It is known for the Coxeter groups of type An that all the elements are parabolic Coxeter elements in the sense of [2]. For types Bn and I2(m), the sets of parabolic Coxeter elements and parabolic quasi-Coxeter elements coincide as it is shown in Section 6. In particular, Theorem 1.1 is true for An,Bn and I2(m) as a consequence of [2]. For the other types it is in general false that parabolic quasi-Coxeter elements coincide with parabolic Coxeter elements. In Section 6 we also show:

Theorem 1.5

Let w be a quasi-Coxeter element in a finite dual Coxeter system (W,T) of rank n and (t1,,tn)RedT(w) such that W=t1,,tn. Then the reflection subgroup W:=t1,,tn-1 is parabolic.

The proof of this theorem is uniform for the simply laced types, but case-by-case for the other ones. As a corollary we obtain a new characterization of the maximal parabolic subgroups of a finite dual Coxeter system (see Corollary 6.10). Moreover, it follows from Theorem 1.5 that an element is a parabolic quasi-Coxeter element if and only if it is a prefix of a quasi-Coxeter element (see Corollary 6.11).

Theorem 1.5 allows us to argue by induction to prove the main theorem. For type Dn we need to show that every two maximal parabolic subgroups intersect non-trivially provided that n6 (see Section 7) which then allows us to conclude Theorem 1.1 by induction. For the types E6,E7 and E8 we first check by computer that every reflection occurs in the Hurwitz orbit of every reduced decomposition of a quasi-Coxeter element, and then argue by induction. Theorem 1.1 is verified for types F4, H3 and H4 by computer. All this is done in Section 8.

2 Dual Coxeter systems and Hurwitz action

2.1 Dual Coxeter systems

Let (W,T) be a dual Coxeter system of finite rank n in the sense of [3]. This is to say that there is a subset ST with |S|=n such that (W,S) is a (not necessarily finite) Coxeter system, and T={wsw-1wW,sS} is the set of reflections for the Coxeter system (W,S) (unlike Bessis, we specify no Coxeter element). We call (W,S) a simple system for (W,T) and S a set of simple reflections. If ST is such that (W,S) is a Coxeter system, then {wsw-1wW,sS}=T (see [9, Lemma 3.7]). Hence a set ST is a simple system for (W,T) if and only if (W,S) is a Coxeter system. The rank of (W,T) is defined as |S| for a simple system S. This is well-defined by [9, Theorem 3.8]. It is equal to the rank of the corresponding root system.

Simple systems for (W,T) have been studied by several authors (see [18]). Clearly, if S is a simple system for (W,T), then so is wSw-1 for any wW. Moreover, it is shown in [18] that for an important class of infinite Coxeter groups including the irreducible affine Coxeter groups, all simple systems for (W,T) are conjugate to one another in this sense.

The following result is well known and follows from [16].

Proposition 2.1

Let (W,S) be a (not necessarily finite) Coxeter system of rank n. Then W cannot be generated by less than n reflections.

Proof.

Assume that W=t1,,tk, with kn. Following [16], write

χ(W)={tT{uT(ut)<(t)}={t}}

for the set of canonical Coxeter generators of W where is the length function in (W,S). It follows from [16, Corollary 3.1 (i)] that |χ(W)|k. But since W is of rank n the set χ(W) contains S hence we have |χ(W)|n, which concludes the proof. ∎

A reflection subgroupW is a subgroup of W generated by reflections. It is well known that (W,WT) is again a dual Coxeter system (see [16]). For wW, a reduced T-decomposition of w is a shortest length decomposition of w into reflections, and we denote by RedT(w) the set of all such reduced T-decompositions. When the context is clear, we drop the T and elements of RedT(w) are referred to as reduced decompositions of w. The length of any element in RedT(w) is called the reflection length (or absolute length) of w and we denote it by T(w). The absolute length function T:W0 can be used to define the absolute orderT on W as follows. For u,vW:

uTv if and only if T(u)+T(u-1v)=T(v).

The reflection subgroup generated by {s1,,sm} is called a parabolic subgroup for (W,T) if there is a simple system S={s1,,sn} for (W,T) with mn. Notice that this differs from the usual notion of a parabolic subgroup generated by a conjugate of a subset of a fixed simple system S (see [21, Section 1.10]). However we prove in Section 4 the equivalence of the definitions for finite Coxeter groups.

2.2 Coxeter and quasi-Coxeter elements

We now define (parabolic) Coxeter elements and (parabolic) quasi-Coxeter elements. The second item of the definition below is borrowed from [2]. The third one is a generalization of Voigt’s original definition in [37], see also Remark 2.8.

Definition 2.2

Let (W,T) be a dual Coxeter system and S={s1,,sn} be a simple system for (W,T).

  1. We say that cW is a classical Coxeter element if c is conjugate to some sπ(1)sπ(n) for π a permutation of the symmetric group 𝔖n. An element wW is a classical parabolic Coxeter element if wTc for some classical Coxeter element c.

  2. An element cW is called a Coxeter element if there exists a simple system S={s1,,sn} for (W,T) such that c=s1sn. An element wW is a parabolic Coxeter element if there exists a simple system S={s1,,sn} for (W,T) such that w=s1sm for some mn.

  3. An element wW is called a quasi-Coxeter element for (W,T) if there exists (t1,,tn)RedT(w) such that W=t1,,tn. An element wW is a parabolic quasi-Coxeter element for (W,T) if there is a simple system S={s1,,sn} and (t1,,tm)RedT(w) such that

    t1,,tm=s1,,sm

    for some mn.

Remark 2.3

Let us point out a few facts about these definitions.

  1. An element of the form sπ(1)sπ(n) obtained as product of elements of a fixed simple system in some order as in Definition 2.2 (a) is usually called a standard Coxeter element. In the case where the Dynkin diagram of the Coxeter system is a tree, every two standard Coxeter elements are conjugate to each other by a sequence of cyclic conjugations (see [7, V, 6.1, Lemme 1]). Hence the set of classical Coxeter elements forms in that case a single conjugacy class. In particular, this holds for all the finite Coxeter groups.

  2. If the Coxeter group is finite, then an element wW is a parabolic Coxeter element if and only if wTc for some Coxeter element c (see [14, Corollary 3.6]).

  3. It is clear that a classical Coxeter element is a Coxeter element and hence it follows from Remark 2.3 (b) that a classical parabolic Coxeter element is a parabolic Coxeter element. The difference between classical Coxeter elements and Coxeter elements is somewhat subtle. For finite Weyl groups (see Section 3 for the definition), the two definitions are equivalent, as a consequence of [34, Theorem 1.8 (ii) and Remark 1.10]. It seems however that no case-free proof of this fact is known. An example where these two definitions differ is the dihedral group I2(5) (see [2, Remark 1.1]).

  4. We will show in Corollary 6.11 the same statement as the one given in Remark 2.3 (b) but for parabolic quasi-Coxeter elements, namely that wW is a parabolic quasi-Coxeter element if and only if there exists a quasi-Coxeter element wW such that wTw.

Example 2.4

In type D4 with simple system {s0,s1,s2,s3} where s2 does not commute with any other simple reflection, the element

c:=s1(s2s1s2)(s2s0s2)s3

is a quasi-Coxeter element. It has a reduced decomposition generating the whole group since if we write

(t1,,t4)=(s1,s2s1s2,s2s0s2,s3)

we have that t1t2t1=s2 and s2t3s2=s0. Using the permutation model for a group of type D4 (see Section 7), it can be shown that there is no reduced decomposition of this element yielding a simple system for the group. By computer we checked that the poset {wWwTc} has 54 elements and is not a lattice. There is a single conjugacy class of quasi-Coxeter elements which are not Coxeter elements in that case. Therefore we can not define a new Garside structure on the Artin–Tits group of type D4 by replacing the Coxeter element by a quasi-Coxeter element.

2.3 Rigidity

Finite Coxeter groups are reflection rigid, that is, if (W,S) and (W,S) are simple systems for (W,T), then both systems determine the same diagram (see [9, Theorem 3.10]). We define (W,T) to be irreducible if (W,S) is irreducible and its type to be the type of (W,S) for some (equivalently each) simple system ST. In most cases, the type is determined by the group itself. There are only two exceptions, namely

WB2k+1WA1×WD2k+1(k1),
WI2(4k+2)WA1×WI2(2k+1)(k1),

which follows from the classification of the finite irreducible Coxeter groups and [32, Theorem 2.17, Lemma 2.18 and Theorem 3.3].

We say that a reflection group is strongly reflection rigid if whenever (W,S) and (W,S) are simple systems for (W,T), then S and S are conjugate in W. Notice that (W,T) is strongly reflection rigid if and only if every Coxeter element is a classical Coxeter element. Hence in particular let us point out that Remark 2.3 (c) implies:

Remark 2.5

The finite Weyl groups are strongly reflection rigid.

2.4 Hurwitz action on reduced decompositions

The braid group on n strands denoted n is the group with generators σ1,,σn-1 subject to the relations

σiσj=σjσifor |i-j|>1,
σiσi+1σi=σi+1σiσi+1for i=1,,n-2.

It acts on the set Tn of n-tuples of reflections as

σi(t1,,tn)=(t1,,ti-1,titi+1ti,ti,ti+2,,tn),
σi-1(t1,,tn)=(t1,,ti-1,ti+1,ti+1titi+1,ti+2,,tn).

We call this action of n on Tn the Hurwitz action and an orbit of this action an Hurwitz orbit.

Lemma 2.6

Lemma 2.6 ([2, Lemma 1.2])

Let W be a reflection subgroup of W and let T=TW be the set of reflections in W. For an element wW such that T(w)=n, the braid group on n strands acts on RedT(w).

We now give the main result of [2].

Theorem 2.7

Let (W,T) be a dual Coxeter system of finite rank n and let c=s1sm be a parabolic Coxeter element in W. The Hurwitz action on RedT(c) is transitive. In symbols, for each (t1,,tm)Tm such that c=t1tm, there is a braid βBm such that

β(t1,,tm)=(s1,,sm).

Hence in the case where W is finite, Theorem 1.1 generalizes Theorem 2.7.

Remark 2.8

For the case where (W,T) is simply laced and w is a quasi-Coxeter element in W, Voigt observed in his thesis [37] that the Hurwitz action on RedT(w) is transitive. His definition of a quasi-Coxeter element is slightly different. Let Φ be the root system associated to W (see Sections 3 and 5 for definitions and notations on root systems and lattices), then Voigt defined w=sα1sαnW to be quasi-Coxeter if span(α1,,αn) is equal to the root lattice of Φ. The connection with our definition will be explained in Section 5.

3 Root systems and geometric representation

In this section we fix some notation, and for the convenience of the reader we recall some facts on root systems and the geometric representation of a Coxeter group as can be found for example in [21] or [7]. Let V be a finite-dimensional Euclidean vector space with positive definite symmetric bilinear form (--). For 0αV, let sα:VV be the reflection in the hyperplane orthogonal to α, that is, the map defined by

vv-2(vα)(αα)α.

Then sα is an involution and sαO(V), the orthogonal group of V with respect to (--).

Definition 3.1

A finite subset ΦV of nonzero vectors is called root system in V if

  1. span(Φ)=V,

  2. sα(Φ)=Φ for all αΦ,

  3. Φα={±α} for all αΦ.

The root system is called crystallographic if in addition

  1. β,α:=2(βα)(αα) for all α,βΦ.

The rankrk(Φ) of Φ is the dimension of V. The group WΦ=sααΦ associated to the root system Φ is a Coxeter group. In the case where the root system is crystallographic, WΦ is a (finite) Weyl group. A subset ΦΦ is called a root subsystem if Φ is a root system in span(Φ).

Conversely, to any finite Coxeter group one can associate a root system. For an infinite Coxeter system (W,S), one can still associate a set of vectors (again called a root system) with slightly relaxed conditions (see for instance [21, Section 5.3–5.7]). In the following, when dealing with root systems it will always be in the sense of the above definition unless otherwise specified since this paper primarily concerns finite Coxeter groups. When results generalize to arbitrary Coxeter groups, we will mention that we work with the generalized root systems.

Let Φ be a root system. Then Φ is reducible if Φ=˙Φ1Φ2 where Φ1, Φ2 are nonempty root systems such that (αβ)=0 whenever αΦ1, βΦ2. Otherwise Φ is irreducible. For an irreducible crystallographic root system Φ, the set {(αα)αΦ} has at most two elements (see [21, Section 2.9]). If this set has only one element, up to rescaling we can assume it to be 2 and call Φ simply laced. It follows from the classification of irreducible root systems that simply laced root systems are crystallographic. Simply laced root systems have types An (n1), Dn (n4) or En (n{6,7,8}) in the classification. We will sometimes use the notation WXn for the Coxeter group with corresponding root system of type Xn for convenience. For more on the topic we refer the reader to [21].

4 Equivalent definitions of parabolic subgroups

In this section, we show one direction of Theorem 1.1 with a case-free argument. To this end, we show Proposition 1.4, that is, we show that for finite Coxeter groups, the definition of parabolic subgroups given in Section 2 coincides with the usual one. We also mention that they coincide for a large class of infinite Coxeter groups.

Let (W,S) be a finite Coxeter system with root system Φ and V:=span(Φ). We say that a subgroup generated by a conjugate of a subset of S is parabolic in the classical sense. It is well known that these are exactly the subgroups of the form

CW(E):={wWw(v)=vfor all vE}

where EV is any set of vectors (see for instance [26, Section 5-2]).

Definition 4.1

Given a subset 𝒜W, the parabolic closureP𝒜 of 𝒜 is the intersection of all the parabolic subgroups in the classical sense containing 𝒜. It is again a parabolic subgroup in the classical sense (see [36, 12.2–12.5] or [33]).

We denote by Fix(𝒜) the subspace of vectors in V which are fixed by every element of 𝒜. If 𝒜={w}, then we simply write Fix(w) for Fix(𝒜)=ker(w-1) and Pw for P𝒜. For convenience we also set Mov(w):=im(w-1). Note that V=Fix(w)Mov(w) (see [1, Definition 2.4.6]). It follows from the above description that P𝒜=CW(Fix(𝒜)).

In this section we give a case-free proof that for finite Coxeter groups, the parabolic subgroups as defined in Section 2.1 coincide with the parabolic subgroups in the classical sense. As a consequence we are able to show one direction of Theorem 1.1. We first recall the following result

Lemma 4.2

Lemma 4.2 ([3, Lemma 1.2.1 (i)], [1, Theorem 2.4.7] after [12])

Let wW, tT. Then

Fix(w)Fix(t)if and only if tTw.

Notice that Lemma 4.2 implies [2, Theorem 1.4] if W is finite.

Proposition 4.3

Let (W,S) be a finite Coxeter system, T=wWwSw-1 and wW. If the Hurwitz action on RedT(w) is transitive, then the subgroup generated by the reflections in any reduced decomposition of w is equal to Pw.

Proof.

We prove the contrapositive of the statement. Let (t1,,tm)RedT(w) and assume that W:=t1,,tm is not equal to Pw. Since tiTw for each i, we have tiPw for all i=1,,m by Lemma 4.2. It follows that WPw. Since both W and Pw are reflection subgroups of W, there exists a reflection tPw with tW. It follows that Fix(w)Fix(t), hence also that tTw by Lemma 4.2. In particular, there exists (q1,,qm)RedT(w) with q1=t. Since the Hurwitz orbit of (t1,,tm) remains in W and tW, the Hurwitz action on RedT(w) can therefore not be transitive. ∎

Corollary 4.4

Let (W,S) be a finite Coxeter system and T=wWwSw-1. A subgroup PW is parabolic if and only if it is parabolic in the classical sense. In particular, if ST is such that (W,S) is a simple system, then the parabolic subgroups in the classical sense defined by S coincide with those defined by S.

Proof.

If P is parabolic, then P=s1,,sm where {s1,,sn}=ST is a simple system for W and mn. By [2, Theorem 1.3], the Hurwitz action on RedT(w) where w=s1s2sm is transitive. By Proposition 4.3, it follows that P is parabolic in the classical sense.

Conversely, if P is parabolic in the classical sense, then P is generated by a conjugate of a subset of S, and a conjugate of S is again a simple system for W. Hence P is parabolic. ∎

As a corollary we get a proof of one direction of Theorem 1.1:

Corollary 4.5

Let (W,T) be a finite, dual Coxeter system of rank n and let wW. If the Hurwitz action on RedT(w) is transitive, then w is a parabolic quasi-Coxeter element for (W,T).

Proof.

Let w=t1tmRedT(w). By Proposition 4.3, W:=t1,,tm is parabolic in the classical sense. By Corollary 4.4, it follows that W is parabolic and hence w is a parabolic quasi-Coxeter element. ∎

If (W,S) is of type A~1, i.e. if W is a dihedral group of infinite order, then the non-trivial parabolic subgroups are precisely those subgroups that are generated by a reflection. Therefore parabolic subgroups in the classical sense coincide with parabolic subgroups in this case. As an immediate consequence of a theorem of Franzsen, Howlett and Mühlherr [18] we also get the equivalence of the definitions for a large family of infinite Coxeter groups (including the irreducible affine Coxeter groups):

Proposition 4.6

Let (W,S) be an infinite irreducible 2-spherical Coxeter system, that is, S is finite, and ss has finite order for every s,sS. Then a subgroup of W is parabolic if and only if it is parabolic in the classical sense.

Proof.

Under these assumptions, if (W,S) is a Coxeter system (without assuming ST), it follows from [18, Theorem 1 b)] that there exists wW such that S=wSw-1, hence any parabolic subgroup is a parabolic subgroup in the classical sense. ∎

Question 4.7

Do parabolic subgroups always coincide with parabolic subgroups in the classical sense?

5 Root lattices

In this section, we study root lattices and their sublattices. The results will be needed for the better understanding of quasi-Coxeter elements in the simply laced types. Parts of this section have been inspired by [37].

Definition 5.1

Let V be a Euclidean vector space with symmetric bilinear form (--). A latticeL in V is the integral span of a basis of V. The lattice L is called integral if (αβ) for all α,βL and even if (αα)=2 for all basis elements α.

For a set of vectors ΦV we set L(Φ):=span(Φ).

Remark 5.2

If Φ is a root system, then L(Φ) is a lattice, called the root lattice. If Φ is a crystallographic root system, then L(Φ) is an integral lattice.

Proposition 5.3

For an even lattice L the set Φ(L):={αL(αα)=2} is a simply laced, crystallographic root system in spanR(L).

Proof.

The set Φ(L) is contained in the ball around 0 with radius 2, therefore bounded, thus finite. The rest of the proof is straightforward. ∎

Definition 5.4

Let Φ be a crystallographic root system in V. The weight latticeP(Φ) of Φ is defined by P(Φ):={xVx,α for all αΦ}. By [7, VI, 1.9] it is again a lattice containing L(Φ) and the group P(Φ)/L(Φ) is finite. We call its order the connection index of Φ and denote it by i(Φ).

Note that if Φ is simply laced, the weight lattice is equal to the dual root lattice, namely,

P(Φ)=L*(Φ):={xV(xy) for all yL(Φ)}.

Proposition 5.5

Let Φ be a simply laced root system and let C be the Cartan matrix of Φ. Then

i(Φ)=det(C).

Proof.

Let Δ={α1,,αm}Φ be a basis of the root system Φ. Then Δ is a basis of L(Φ). Denote by M the Gram matrix of L(Φ) with respect to Δ. By general lattice theory (see for instance [17, Section 1.1]) one has

|L*(Φ):L(Φ)|=det(M).

Since Φ is simply laced, we have L*(Φ)=P(Φ) and hence

i(Φ)=|L*(Φ):L(Φ)|.

Again since Φ is simply laced, we have C=M, which concludes the proof. ∎

We list i(Φ) for the irreducible, simply laced root systems. These can be found in [7, Planches I, IV , V, VI, VII].

Type of ΦAnDnE6E7E8
i(Φ)n+14321

As a consequence we obtain the following result.

Proposition 5.6

Let Φ be an irreducible, simply laced root system. Then Φ is determined by the pair (rk(Φ),i(Φ)).

The following lemma seems to be folklore, but we could not find a proof in the literature, hence we state it here.

Lemma 5.7

Let Φ be a simply laced root system. Then the root lattice determines the root system, that is,

Φ(L(Φ))=Φ.

Proof.

By the previous proposition, we have to show that the rank and connection indices of Φ and Φ(L(Φ)) coincide. Since ΦΦ(L(Φ)), we have

rk(Φ)rk(Φ(L(Φ))).

On the other hand, the rank of Φ(L(Φ)) is bounded above by the dimension of the ambient vector space which equals rk(Φ).

In the proof of Proposition 5.5, we used the fact that the Cartan matrix of a root system and the Gram matrix of the corresponding root lattice coincide. Denote by CΦ the Cartan matrix with respect to Φ. Then

det(CΦ)=vol(L(Φ))=vol(L(Φ(L(Φ))))=det(CΦ(L(Φ))),

which yields i(Φ)=i(Φ(L(Φ))) by Proposition 5.5. ∎

Lemma 5.8

Let Φ be as in Lemma 5.7 and let ΦΦ be a root subsystem. Then L(Φ)Φ=Φ.

Proof.

We have the equalities

L(Φ)Φ=L(Φ){αL(Φ)(αα)=2}by Lemma 5.7
={αL(Φ)(αα)=2}
=Φby Lemma 5.7.

Notation 5.9

Let Φ be a finite root system and RΦ a set of roots. We denote by WR the group sr|rR.

Note that this is consistent with the notation introduced in Definition 3.1 in the case where R=Φ.

Proposition 5.10

Let Φ be a crystallographic root system, let ΦΦ be a root subsystem, and let R:={β1,,βk}Φ be a set of roots. The following statements are equivalent:

  1. The root subsystem Φ is the smallest root subsystem of Φ containing R (i.e., the intersection of all root subsystems containing R).

  2. Φ=WR(R).

  3. WΦ=WR.

Moreover, if any of the above equivalent conditions is satisfied, then

  1. L(Φ)=L(R).

Proof.

Obviously, WR(R) is a root system with RWR(R). Thus if (a) holds, then ΦWR(R). As WR(R)WΦ(Φ)=Φ, it follows that (a) implies (b). The converse direction follows from the definition of a root subsystem.

Statement (b) implies that RΦ and therefore we have WRWΦ. We show that in this case WΦWR. To this end, let αΦ=WR(R). Then α=w(βi) for some wWR and 1ik. Then

sα=sw(βi)=wsβiw-1WR,

which shows the claim. Thus (b) implies (c).

Assume (c) and let Φ′′ be the smallest root subsystem of Φ containing R. Then WΦ=WRWΦ′′. By the definition of Φ′′ we have Φ′′Φ. If Φ′′Φ, then WΦ′′WΦ, a contradiction. Hence Φ′′=Φ, which shows (a).

It remains to show that (c) implies (d). So assume (c) and let ti:=sβi, 1ik. Let TΦ be the set of reflections in WΦ. By [16, Corollary 3.11 (ii)], we have TΦ={wtiw-11ik,wWΦ}. In particular, any root in Φ has the form w(βi) for some wWΦ, 1ik. Since WΦ=t1,,tk, we can write w=ti1tim with 1ijk for each 1jm. Since Φ is crystallographic, it follows that w(βi)=ti1tim(βi) is an integral linear combination of the roots βj, hence that ΦL(R). Since RΦ, we get L(R)=L(Φ), which proves (d). ∎

Remark 5.11

Notice that condition (d) in Proposition 5.10 is in general not equivalent to conditions (a)–(c). For example, if Φ is of type B2, then one can choose two orthogonal roots α and β generating a proper root subsystem of type A1×A1 while one has L({α,β})=L(Φ). Nevertheless, one has the equivalence for simply laced root systems:

Lemma 5.12

Let Φ,Φ,R be as in Proposition 5.10 and assume in addition that Φ is simply laced. Then condition (d) in Proposition 5.10 is equivalent to any of conditions (a)–(c).

Proof.

Since conditions (a)–(c) are equivalent, it suffices to show that condition (d) implies (a). Assume that there exists a root subsystem Φ′′ of Φ with Φ′′Φ and RΦ′′. It follows that L(Φ)=L(R)L(Φ′′). One then has

Φ=L(Φ)ΦL(Φ′′)Φ=Φ′′

by Lemma 5.8. Hence Φ=Φ′′, which concludes the proof. ∎

The following two results are useful tools for the next section. The following proposition and its proof are borrowed from [37, Proposition 1.5.2].

Proposition 5.13

Let Φ be a simply laced root system and let ΦΦ be a root subsystem with rk(Φ)=m=rk(Φ). Then:

  1. |L(Φ):L(Φ)|=|P(Φ):P(Φ)|,

  2. |L(Φ):L(Φ)|=i(Φ)i(Φ)-1.

Proof.

Since Φ and Φ have the same rank, there is a lattice isomorphism

:L(Φ)L(Φ),

hence |L(Φ):L(Φ)|=|det()| (see [17, Section 1.1]). Furthermore, we have

P(Φ)={xV(xy) for all yL(Φ)}
={xV(x(v)) for all vL(Φ)}
={xV(t(x)v) for all vL(Φ)}
={xVt(x)P(Φ)}
=(t)-1(P(Φ)).

Thus [P(Φ):P(Φ)]=|det(t)|=|det()|, which shows (a). We have

L(Φ)L(Φ)P(Φ)P(Φ).

It follows that

|L(Φ):L(Φ)||P(Φ):L(Φ)|=i(Φ)|P(Φ):P(Φ)|=|L(Φ):L(Φ)|=|P(Φ):L(Φ)|=i(Φ),

which concludes the proof. ∎

For a simply laced root system Φ we extend the definition of connection index to subsets of Φ. For an arbitrary subset RΦ we define i(R):=|L*(R):L(R)|. Note that i(R) is well-defined by Proposition 5.10, because i(R)=i(Φ), where Φ is the smallest root subsystem of Φ in span(R) containing R.

The following theorem is part of the Diploma thesis of Kluitmann [27].

Theorem 5.14

Let Φ be a simply laced root system. Further, let wWΦ and let (sα1,,sαk), (sβ1,,sβk)RedT(w), where αi,βiΦ, for 1ik. Then for R:={α1,,αk} and Q:={β1,,βk} we have

i(R)=i(Q).

Proof.

Consider L(R) and L*(R) (respectively L(Q) and L*(Q)) as lattices in V:=span(R) (respectively in V′′:=span(Q)). By [12, Lemma 3] the set R is a basis for L(R). Let {α1*,,αk*} be the basis of L*(R) dual to R. In particular, sαj(αi*)=αi* for ij and sαi(αi*)=αi*-αi. Therefore

θi:=(w-1)(αi*)=-sα1sαi-1(αi)L(R)Φ.

Note that θ1=-α1, θ2-α2+span(α1), and more generally

θi-αi+span(α1,,αi-1).

It follows that {θ1,,θk} is a basis of V and that the map

(w-1)|V:L*(R)L(R)

is bijective.

Thus we have i(R)=|det(w-1)|V|. The same argument with Q instead of R yields that i(Q)=|det(w-1)|V′′|. By the proof of [1, Theorem 2.4.7] we have that R and Q are both bases for Mov(w), hence V=V′′=Mov(w) and hence i(R)=i(Q). ∎

6 Reflection subgroups related to prefixes of quasi-Coxeter elements

In this section, we prove Theorem 1.2 for simply laced dual Coxeter systems, see Theorem 6.1. Further we show that the reflections in a reduced T-decomposition of an element wW generate a parabolic subgroup whenever wTw for some quasi-Coxeter element w. Last but not least we demonstrate that parabolic quasi-Coxeter elements coincide with parabolic Coxeter elements in types An, Bn and I2(m).

Recall that for wW, we denote by Pw the parabolic closure of w (see Definition 4.1) and that Pw=CW(Fix(w)).

Theorem 6.1

Let (W,T) be a simply laced dual Coxeter system of rank n. If wW is a parabolic quasi-Coxeter element, then the reflections in any reduced T-decomposition of w generate the parabolic subgroup Pw. That is, for each (t1,,tm)RedT(w) we have Pw=t1,,tm.

Proof.

By the definition of a parabolic quasi-Coxeter element, there exists an element (t1,,tm)RedT(w) such that P:=t1,,tm is a parabolic subgroup. By Lemma 4.2, we have PCW(Fix(w))=Pw. Since wP, we have by definition of the parabolic closure that P=Pw. Let (q1,,qm)RedT(w). Then for all 1im we have qiTw, which yields that qi is in CW(Fix(w))=Pw. Thus W:=q1,,qm is a subgroup of Pw. Let Φ be the root system of Pw and βiΦ be such that qi=sβi, for 1im. Then L(β1,,βm) is a sublattice of L(Φ) and Φ=L(β1,,βm)Φ is the smallest root subsystem of Φ that contains β1,,βm. Therefore Theorem 5.14 yields that i(Φ)=i(Φ). This implies L(Φ)=L(Φ) by Proposition 5.13. Thus W=Pw by Lemma 5.12. ∎

We will show in Corollary 6.11 that the following property of parabolic quasi-Coxeter elements does in fact characterize them.

Proposition 6.2

Let (W,T) be a finite dual Coxeter system. If wW is a parabolic quasi-Coxeter element, then there exists a quasi-Coxeter element wW such that wTw.

Proof.

Let wW be a parabolic quasi-Coxeter element. By definition, there exists a simple system S={s1,,sn} for W and a T-reduced decomposition w=t1tm such that

t1,,tm=s1,,sm,

with mn. Set w:=t1tmsm+1sn. It is clear that

t1,,tm,sm+1,,sn=W.

Moreover, we have that T(w)=n, hence w is a quasi-Coxeter element with wTw. ∎

Lemma 6.3

Let (W,T) be a dual Coxeter system of type An. Then each wW is a classical parabolic Coxeter element.

Proof.

In type An, the set of (n+1)-cycles forms a single conjugacy class. Hence the set of classical Coxeter elements is exactly the set of (n+1)-cycles (see Remark 2.3 (a)). The assertion follows with Remark 2.3 (b) as for every element wW, we have wTw for at least one (n+1)-cycle w. ∎

Lemma 6.4

Let (W,T) be a dual Coxeter system of type Bn. Then every parabolic quasi-Coxeter element wW for (W,T) is a classical parabolic Coxeter element.

Proof.

For the proof we use the combinatorial description of WBn as given in [6, Section 8.1]. Therefore let S-n,n be the group of permutations of

[-n,n]={-n,-n+1,,-1,1,,n}

and define

W=WBn:={wS-n,nw(-i)=-w(i) for all i[-n,n]},

also known as the hyperoctahedral group. Then (W,S) is a Coxeter system of type Bn with

S={(1,-1),(1,2)(-1,-2),,(n-1,n)(-n+1,-n)}.

The set of reflections T for this choice of S is given by

T={(i,-i)i[n]}{(i,j)(-i,-j)1i<|j|n}.

We show that every quasi-Coxeter element for (W,T) is a classical Coxeter element. If w is a parabolic quasi-Coxeter element, then by Proposition 6.2, there exists a quasi-Coxeter element wW such that wTw. Hence if w is a classical Coxeter element, then wTw implies that w is a classical parabolic Coxeter element.

Let R={r1,,rn}T be such that R=W. It suffices to show that r1r2rn is in fact a classical Coxeter element.

The group W cannot be generated only by reflections of type (i,j)(-i,-j), i±j. Therefore there exists i[n] with (i,-i)R. If there exists j[n], ji, with (j,-j)R, then R cannot generate the whole group W. Since classical Coxeter elements are closed under conjugation, we can conjugate the set R with (1,i)(-1,-i) (if necessary) and assume (1,-1)R.

Since R generates the whole group W, there does not exist j[n] which is fixed by each rR. Thus for each k[n],k1, we can find ik[±n] with k±ik such that (k,ik)(-k,-ik)R. Therefore

R={(1,-1),(2,i2)(-2,-i2),,(n,in)(-n,-in)}.

Note that some ij has to equal ±1, because otherwise (1,-1) would commute with any element of W. By conjugating R with (j,2)(-j,-2) respectively (j,-2)(-j,2) (if necessary) we can assume that i2=1. Hence after rearrangement we can assume that R is of the form

R={(1,-1),(2,1)(-2,-1),(3,i3)(-3,-i3),,(n,in)(-n,-in)}.

Similarly to what we did above, there exists j3 with ij{±1,±2}. By conjugating R with (j,3)(-j,-3) respectively (j,-3)(-j,3) (if necessary) we can assume that i3{1,2}. Continuing in this manner we obtain

R={(1,-1),(2,i2)(-2,-i2),,(n,in)(-n,-in)}

with ij{1,,j-1} for each j{2,,n}. A direct computation shows that c:=r1r2rn is a 2n-cycle and thus a classical Coxeter element. Indeed, there is a single conjugacy class of 2n-cycles in W. ∎

Remark 6.5

Notice that by Remark 2.3 (c), it is already known that classical Coxeter elements and Coxeter elements must coincide in type Bn. Moreover, it follows from [12, Lemma 8, Theorem A] that every quasi-Coxeter element is actually a Coxeter element. Hence one can derive Lemma 6.4 from these two observations. However since both of them rely on sophisticated methods, we preferred to give here a direct proof using the combinatorics of the hyperoctahedral group.

Remark 6.6

In type An, we even have that every element w such that T(w)=n is a classical Coxeter element (thus quasi-Coxeter), because such an element is necessarily an (n+1)-cycle. Notice that this fails in type Bn. For instance, the product (1,-1)(2,-2)(n,-n) in WBn has reflection length equal to n, but it is not a quasi-Coxeter element.

The following is well known (see [7, IV, 1.2, Proposition 2]):

Proposition 6.7

A group W is a dihedral group if and only if it is generated by two elements s, t of order 2, in which case {s,t} is a simple system for W.

Corollary 6.8

Let (W,T) be a dual Coxeter system of type I2(m), m3. Then w is a quasi-Coxeter element in W if and only if w is a Coxeter element in W. It follows that wW is a parabolic quasi-Coxeter element if and only if w is a parabolic Coxeter element.

Note that Coxeter elements and classical Coxeter elements do not coincide in general in dihedral type (see Remark 2.3 (c)).

Theorem 1.5

Let w be a quasi-Coxeter element in a finite dual Coxeter system (W,T) of rank n and (t1,,tn)RedT(w) such that W=t1,,tn. Then the reflection subgroup W:=t1,,tn-1 is parabolic.

Proof.

The reduction to the case where W is irreducible is immediate. The proof is uniform for the simply laced types and case-by-case for the non-simply laced types.

Dihedral type. The claim is obvious in that case.

Simply laced types. Let Φ be a root system for (W,T) with ambient vector space V. Let PW be the parabolic closure of W. For 1in, let βiΦ be a root corresponding to ti and let Φ be the smallest root subsystem of Φ containing R:={β1,,βn-1} so that WR=WΦ=W (see Proposition 5.10). Let ΨΦ be the root subsystem of Φ associated to PW. By [12, Lemma 3] the set R{βn} is a basis of V.

Let U be the ambient vector space for Ψ. As the linear independent set R is a subset of Ψ, the dimension of U is at least n-1. Since PW is the parabolic closure of t1tn-1 it has to be the centralizer of a line in V and therefore dimU=n-1. It follows that U=span(β1,,βn-1).

By Proposition 5.10 we have that

L(Φ)=L({β1,,βn-1})andL(Φ)=L({β1,,βn}).

Since V=Uβn, we have that L(Φ)U=L({β1,,βn-1})=L(Φ). As L(Ψ)U, it follows that L(Ψ)L(Φ). But since ΦΨ, we get that L(Φ)L(Ψ) and therefore L(Φ)=L(Ψ). Thus W=PW by Lemma 5.12.

Type Bn. By Lemma 6.4 the element w is a classical Coxeter element. It follows that wtn is a classical parabolic Coxeter element, hence a parabolic Coxeter element (see Remark 2.3 (c)). It follows that W is parabolic.

Type F4. By [15, Table 6], the group WF4 cannot be generated by just adding one reflection to one of its non-parabolic rank 3 reflection subgroups.

Types H3 and H4. We refer to [15, Tables 8 and 9], where the reflection subgroups of WH3 and WH4 and their parabolic closures are determined.

  1. Each rank 2 reflection subgroup of the group WH3 is already parabolic.

  2. The only rank 3 reflection subgroup of WH4 that is not parabolic has type A1×A1×A1. Taking a set of three reflections generating such a reflection subgroup, we checked using [38] that this set cannot be completed to obtain a generating set for WH4 by adding a single reflection.∎

Remark 6.9

Theorem 1.5 is not true in general. It can even fail if w is a Coxeter element, as the following example borrowed from [20, Example 5.7] shows: Let W=s,t,u be of affine type A~2, and let w=stu. Then we have s(tut)Tc, but W=s,tut is an infinite dihedral group, hence it is not a parabolic subgroup in the classical sense since proper parabolic subgroups of W are finite. We mentioned in Section 4 that for affine Coxeter groups parabolic subgroups in the classical sense also coincide with parabolic subgroups as defined in Section 2.1.

Corollary 6.10

Let (W,T) be a finite dual Coxeter system of rank n and let W be a reflection subgroup of rank n-1. Then W is a parabolic subgroup if and only if there exists tT such that W,t=W.

Proof.

The necessary condition is clear by the definition of parabolic subgroup. The sufficient condition is a direct consequence of Theorem 1.5. ∎

We also derive a characterization of parabolic quasi-Coxeter elements analogous to that of parabolic Coxeter elements (see Remark 2.3 (b)).

Corollary 6.11

Let (W,T) be a finite dual Coxeter system and wW. Then w is a parabolic quasi-Coxeter element if and only if there exists a quasi-Coxeter element wW such that wTw.

Proof.

The forward direction is given by Proposition 6.2. Now let wTw where wW is a quasi-Coxeter element. Using Theorem 1.5 inductively we get that w is a parabolic quasi-Coxeter element in W. ∎

Remark 6.12

Corollary 6.11 does not hold for infinite Coxeter groups as it fails for the Coxeter element given in Remark 6.9.

7 Intersection of maximal parabolic subgroups in type Dn

The aim of this section is to show the following result which will be needed in the next section in the proof of Theorem 1.1.

Proposition 7.1

Let (W,S) be a Coxeter system of type Dn (n6). Then the intersection of two maximal parabolic subgroups is non-trivial.

Remark 7.2

This statement is not true in general, not even in the simply laced case. In particular, it fails in types D4,D5,E7 and E8. For example:

  1. Let (W,S) be of type D4 where S={s0,s1,s2,s3} with s2 commuting with no other simple reflection, then both P:=s0,s1,s3 and s2Ps2 are maximal parabolic subgroups of type A1×A1×A1 and have trivial intersection.

  2. Let (W,S) be of type E7 where S={s1,,s7} labelled as in [7, Planche VI]. Let I={s1,s2,s3,s4,s6,s7} and J={s1,s2,s3,s5,s6,s7}. Then the non-conjugate parabolic subgroups WJ and wWIw-1 intersect trivially, where

    w=s6s2s4s5s3s4s1s3s2s4s5s6s7s4s5s6s4s5s3s4s1s3s2s4s5s4s3s2s4s1.

    This was checked using [38].

For the rest of this section we work with the combinatorial realization of W as a subgroup (which we denote by WDn) of the hyperoctahedral group WBn (see Section 6). To this end, set

s0=(1,-2)(-1,2),
si=(i,i+1)(-i,-(i+1))for i[n-1].

Then {s0,s1,,sn-1} is a simple system for a Coxeter group WDn of type Dn. The set of reflections is given by T={(i,j)(-i,-j)i,j[-n,n],i±j}. Notice that W is a subgroup of the group WBn of type Bn; indeed, the above generators are clearly contained in WBn. Given A[-n,n], write Stab(A) for the subgroup of WDn of elements preserving the set A. Notice that since WDnWBn, we have Stab(A)=Stab(-A). The maximal standard parabolic subgroups of WDn are then described as follows (see [6, Proposition 8.2.4]). Let i{0,1,,n-1} and I=S{si}. Then WI=Stab(AI), where

AI:={[i+1,n]if i1,{-1,2,3,,n}if i=1.

Since WI stabilizes both AI and -AI, it stabilizes also the complement AI0 of AI(-AI) in [-n,n]. Notice that AI0=-AI0.

From this description we can easily achieve a description of maximal parabolic subgroups:

Lemma 7.3

If WJ=Stab(AJ) is a maximal standard parabolic subgroup and wW, then wWJw-1=Stab(w(AJ)).

Proof.

Clear. ∎

Proof of Proposition 7.1.

It is enough to show that WIwWJw-1{id} for two subsets I,JS with |I|=|J|=n-1 and wW. We therefore assume that WIwWJw-1={id} for some I,JS with |I|=|J|=n-1 and wW and show that this implies that n5. Consider the intersections AIw(AJ) and AI(-w(AJ)). If one of these intersections contains at least two elements, say k and l, then (k,l)(-k,-l)WIwWJw-1 since

AI(-AI)==w(AJ)(-w(AJ)).

Therefore we can assume that |AIw(AJ)|1 and |AI-w(AJ)|1. Now if |AI|4, then |AIw(AJ)0|2, and since AI(-AI)=, it follows that there exist k,AIw(AJ)0 with k±, and we then have that

(k,)(-k,-)WIwWJw-1.

Hence we can furthermore assume that |AI|<4. It follows that |AI0|2n-6.

But arguing similarly we can also assume that |AI0w(AJ)0|<4, hence we have |AI0w(AJ)0|2 since it has to be even and |AI0w(AJ)|1. It follows that |AI0|4. Together with the inequality above we get 2n-6|AI0|4, hence n5. ∎

8 The proof of Theorem 1.1

The aim of this section is to prove the sufficient condition for the transitive Hurwitz action as stated in Theorem 1.1. The proof is a case-by-case analysis.

Let (W,T) be a finite dual Coxeter system and let wW. For two elements (t1,,tm),(r1,,rm)RedT(w) we write (t1,,tm)(r1,,rm) if both factorizations lie in the same Hurwitz orbit. Furthermore, note that if w is a parabolic quasi-Coxeter element in (W,T), then each conjugate of w is also a parabolic quasi-Coxeter element in (W,T). Since the Hurwitz operation commutes with conjugation, we can restrict ourselves to check transitivity for one representative of each conjugacy class of parabolic quasi-Coxeter elements of W. The proof of the following is easy:

Lemma 8.1

Let (Wi,Ti), i=1,2, be dual Coxeter systems and let wiWi, i=1,2. Then (W1×W2,T:=(T1×{1})({1}×T2)) is a dual Coxeter system. Furthermore, if the Hurwitz action is transitive on RedTi(wi), i=1,2, then the Hurwitz action is transitive on RedT((w1,w2)).

8.1 Types An, Bn and I2(m)

In all these cases every parabolic quasi-Coxeter element is already a parabolic Coxeter element by Lemmas 6.3, 6.4 and Corollary 6.8. Therefore the assertion follows with [2, Theorem 1.3].

Remark 8.2

Notice that in types An and Bn, parabolic quasi-Coxeter elements, classical parabolic Coxeter elements and parabolic Coxeter elements coincide. In type I2(m), parabolic quasi-Coxeter elements and parabolic Coxeter elements coincide, but parabolic Coxeter elements and classical parabolic Coxeter elements do not (see Remark 2.3(c)).

8.2 The simply laced types

We now treat the parabolic quasi-Coxeter elements in an irreducible, finite, simply laced dual Coxeter system (W,T) of rank n. As we already dealt with the type An, it remains to consider the types Dn, n4 and E6,E7,E8.

We only need to show the assertion for quasi-Coxeter elements. Indeed, let w be a parabolic quasi-Coxeter element in (W,T) and let (t1,,tm)RedT(w). Then W=t1,,tm is by Theorem 6.1 a parabolic subgroup of (W,T), in fact W=Pw.

Therefore, it follows from Lemma 4.2 that all the reflections in any reduced factorization of w are in W. The latter group is a direct product of irreducible Coxeter groups of simply laced type. If we know that the Hurwitz action is transitive on RedT(w~) for all the quasi-Coxeter elements w~ in the irreducible Coxeter groups of simply laced type, then the Hurwitz action on RedT(w) is transitive as well by Lemma 8.1.

The strategy to prove the theorem is as follows: we first show by induction on the rank n (with n4) that the Hurwitz action is transitive on the set of reduced decompositions of quasi-Coxeter elements of type Dn; for this we will need to use the result for parabolic subgroups, but since they are (products) of groups of type A with groups of type D of smaller rank, the result holds for groups of type A by Section 8.1 and they hold for groups of type Dk, k<n by induction.

Using the fact that it holds for type Dn, n4, we then prove the result for the groups E6, E7 and E8. Similarly as for type Dn, parabolic subgroups of type E are of type A, D or E. It was previously shown to hold for types A and D and holds for type E by induction.

We then prove by computer that the result holds for the remaining exceptional groups.

Let w be a quasi-Coxeter element and let (t1,,tn)RedT(w).

8.2.1 Type Dn

For types D4 and D5 the assertion is checked directly using [38]. Therefore assume n6. Let (r1,,rn)RedT(w) be a second reduced factorization of w. By Theorem 6.1 and Theorem 1.5 the groups t1,,tn-1 and r1,,rn-1 are maximal parabolic subgroups and since T(wtn)=n-1=T(wrn), it follows that CW(Vwtn)=Pwtn=t1,,tn-1, CW(Vwrn)=Pwrn=r1,,rn-1. By Proposition 7.1 there exists a reflection t in their intersection. It follows by Lemma 4.2 that tTwtn,wrn. Hence there exists t2,,tn-1,r2,,rn-1T such that (t,t2,,tn-1)RedT(wtn) and (t,r2,,rn-1)RedT(wrn). In particular, we get

(t2,,tn-1,tn),(r2,,rn-1,rn)RedT(tw).

By Theorem 1.5 the element tw is quasi-Coxeter in the parabolic subgroup

Ptw=t2,,tn-1,tn.

It follows from Lemma 4.2 that the reflections r2,,rn-1,rn are in Ptw since riTtw for each i. As Ptw is a direct product of irreducible Coxeter groups of type A and D of smaller rank, we have by induction together with Lemma 8.1 that

(t2,,tn-1,tn)(r2,,rn-1,rn),

as well as

(t,t2,,tn-1)(t1,,tn-1)and(t,r2,,rn-1)(r1,,rn-1).

This implies

(t1,,tn)(t,t2,,tn-1,tn)
(t,r2,,rn-1,rn)(r1,,rn)RedT(w),

which concludes the proof.

8.2.2 Types E6,E7 and E8

First we calculated representatives of the conjugacy classes of quasi-Coxeter elements using [38], see also Remark 8.3 (b) below. Then given a quasi-Coxeter element w we checked, again using [38], that there is a reduced factorization (t1,,tn) of w such that for every reflection t in T there exists an element (t1,,tn-1,t)RedT(w) with (t1,,tn)(t1,,tn-1,t).

Let (r1,,rn)RedT(w). By our computations in GAP there exists an element (t1,,tn-1,rn)RedT(w) with (t1,,tn)(t1,,tn-1,rn). Then

wrn=t1tn-1=r1rn-1

are reduced factorizations. Further, wrn is a quasi-Coxeter element in (W,T) where W:=t1,,tn-1 and T:=TW. By Theorem 1.5 we have that W is a equal to the parabolic closure Pt1tn-1 of t1tn-1 and therefore r1,,rn-1 are elements of W by Lemma 4.2. Thus (t1,,tn-1) and (r1,,rn-1) are reduced factorizations of a quasi-Coxeter element in a dual, simply laced Coxeter system of rank n-1. By induction and by Lemma 8.1 we get

(t1,,tn-1)(r1,,rn-1),

thus

(t1,,tn)(t1,,tn-1,rn)(r1,,rn).

8.3 The types F4, H3 and H4

For these cases we again calculated representatives of the conjugacy classes of quasi-Coxeter elements using [38] and then we checked Theorem 1.1 directly for each representative using [38].

Remark 8.3

(a) The computer programs that we used can be found at www.math.uni-bielefeld.de/~baumeist/Dual-Coxeter/dual-Coxeter.html.

(b) For the convenience of the reader we briefly describe Carter’s classification of the conjugacy classes in finite Weyl groups by means of so-called admissible diagrams [12]. Due to [12, Lemma 8, Theorem A], we obtain the following description of conjugacy classes of quasi-Coxeter elements (in the notation of [12]):

  1. For the infinite families the conjugacy classes correspond to the admissible diagrams

    An,Bn,Dn,Dn(a1),Dn(a2),,Dn(a12n-1).

    In particular, in types An and Bn the conjugacy class of the Coxeter element is the only quasi-Coxeter class (see Lemmata 6.3 and 6.4).

  2. For the exceptional types the conjugacy classes correspond to the admissible diagrams

    E6,E6(a1),E6(a2),E7,E7(a1),,E7(a4),E8,E8(a1),,E8(a8),F4,F4(a1),G2.

For the remaining non-crystallographic types we found by computer:

  1. For the type H3 respectively H4 there are three respectively eleven conjugacy classes of quasi-Coxeter elements.

Note that there might be more than one admissible diagram for the same conjugacy class (e.g., the class E7(a2) might also be parametrized by the diagram E7(b2)). For (W,T) irreducible and crystallographic, the conjugacy classes of quasi-Coxeter elements are precisely described by the connected admissible diagrams with number of nodes equal to the rank of (W,T). In [13] such a class is called semi-Coxeter class.


Communicated by Gunter Malle


Award Identifier / Grant number: CRC 701

Funding statement: The work was done while the third author held a position at the CRC 701 within the project C13 ”The geometry and combinatorics of groups”. The other authors wish to thank the DFG for its support through CRC 701 as well. The fourth author also thanks Bielefeld University for financial support through a scholarship by the rectorship.

Acknowledgements

We thank Joel Lewis as well as the referee for helpful comments and Christian Stump for fruitful discussions.

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Received: 2016-1-27
Revised: 2016-5-4
Published Online: 2016-6-15
Published in Print: 2017-1-1

© 2017 by De Gruyter

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