Stabilisers of eigenvectors in complex reflection groups
Sinead Wilson B.Sc. (Hons), M.Sc.
A thesis submitted for the degree of Master of Philosophy at The University of Queensland in 2018 School of Mathematics and Physics Abstract
Eigenvectors of elements of real and complex reflection groups have been studied by Coxeter, Kostant, Springer, Lehrer and Bessis amongst others, due to their rich geometry, and the extensive information that they yield about the structure of the reflection group and related objects in Lie theory and braid theory. Recently, Kamgarpour proved that if G is an irreducible finite real reflection group of rank n, x is an eigenvector of any element of G with eigenvalue a primitive dth root of unity, and Φ and Φx denote the root systems of G and StabG(x) respectively, then |Φ| − |Φx| ≥ dn, with equality if and only if d is the Coxeter number. In this thesis, we prove the following generalisation of Kamgarpour’s inequality. If G is an irreducible complex reflection group of rank n and x is any eigenvector of an element of G with eigenvalue a primitive dth root of unity, then we have
`(π) − `(π x) ≥ dn, with equality if and only if G is well-generated and d = h. Here, π is the generator of the centre of the pure braid group of G, π x is the generator of the centre of the pure braid group of the stabiliser of x, and ` denotes the length function on the braid group of G. Our proof is case-by-case using the Shephard–Todd classification of complex reflection groups. We also investigate the case where `(π) − `(π x) − dn is as small as possible while still being positive, as well as a possible braid-theoretic explanation of our result. Declaration by author
This thesis is composed of my original work, and contains no material previously published or written by another person except where due reference has been made in the text. I have clearly stated the contribution by others to jointly-authored works that I have included in my thesis. I have clearly stated the contribution of others to my thesis as a whole, including statistical assistance, survey design, data analysis, significant technical procedures, professional editorial advice, financial support and any other original research work used or reported in my thesis. The content of my thesis is the result of work I have carried out since the commencement of my higher degree by research candidature and does not include a substantial part of work that has been submitted to qualify for the award of any other degree or diploma in any university or other tertiary institution. I have clearly stated which parts of my thesis, if any, have been submitted to qualify for another award. I acknowledge that an electronic copy of my thesis must be lodged with the University Library and, subject to the policy and procedures of The University of Queensland, the thesis be made available for research and study in accordance with the Copyright Act 1968 unless a period of embargo has been approved by the Dean of the Graduate School. I acknowledge that copyright of all material contained in my thesis resides with the copyright holder(s) of that material. Where appropriate I have obtained copyright permission from the copyright holder to reproduce material in this thesis and have sought permission from co-authors for any jointly authored works included in the thesis. Publications included in this thesis
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Submitted manuscripts included in this thesis
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Other publications during candidature
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Contributions by others to the thesis
The uniform proof of Kamgarpour’s inequality (1.1.1) at the end of Section 4.7 (pp. 42–43) and the formulation of Conjecture 1.2 are due to Jean Michel.
Statement of parts of the thesis submitted to qualify for the award of another degree
No works submitted towards another degree have been included in this thesis.
Research involving human or animal subjects
No animal or human subjects were involved in this research. Acknowledgments
I am deeply grateful to my advisors, Masoud Kamgarpour and Ole Warnaar, for their extensive feedback and patience, and to Kamgarpour for suggesting this fascinating topic. I would also like to thank Jean Michel for our meeting in Sydney, and in particular, for pointing out the problem with [9], for showing me—and giving me permission to reproduce—the proofs in Section 4.7, and for suggesting Conjecture 1.2. This work was funded by a Research Training Scheme scholarship from the Australian Research Council. Financial support
This research was supported by an Australian Government Research Training Program Scholarship
Keywords complex reflection groups, eigenvectors of reflection group elements, parabolic subgroups, braid groups
Australian and New Zealand Standard Research Classifications (ANZSRC)
ANZSRC code: 010101 Algebra and Number Theory, 50% ANZSRC code: 010105 Group Theory and Generalisations , 50%
Fields of Research (FoR) Classification
FoR code: 0101, Pure Mathematics, 100% Contents
Abstract ...... ii
Contents vii
List of figures x
List of tables xi
1 Introduction 1 1.1 Stabilisers of eigenvectors in complex reflection groups ...... 1
2 Real reflection groups 5 2.1 Definition and examples ...... 5 2.2 Root systems ...... 7 2.3 Length ...... 8 2.4 Coxeter groups ...... 9 2.5 Classification ...... 10 2.6 Invariant theory ...... 11 2.6.1 The fundamental degrees ...... 12 2.7 Coxeter elements and exponents ...... 13
3 Complex reflection groups 17 3.1 Introduction ...... 17 3.2 Definitions and notation ...... 18 3.3 Example: generalised permutation matrices ...... 18 3.4 Classification ...... 19 3.5 Invariant theory ...... 20 3.5.1 M-exponents ...... 21
vii viii CONTENTS
3.5.2 The discriminant ...... 22 3.6 Braid groups ...... 22 3.6.1 Braid reflections ...... 24 3.6.2 Artin groups ...... 25 3.6.3 Length in braid groups ...... 26 3.6.4 The centres of P and B ...... 26 3.7 Parabolic subgroups ...... 28 3.7.1 Classification of parabolics in real reflection groups ...... 29 3.7.2 Classification of parabolics in complex reflection groups ...... 30 3.7.3 Parabolic subgroups of braid groups ...... 32
4 Eigenvectors of reflection group elements 35 4.1 Eigenvalues and fundamental degrees ...... 35 4.2 Regular elements ...... 36 4.3 Well-generated reflection groups and Coxeter elements ...... 37 4.4 Statement of the main theorem ...... 38 4.5 Necessity of conditions ...... 39 4.6 Braid group formulation ...... 40 4.7 The case of real reflection groups ...... 40 4.8 Cases where equality almost holds in (4.6.1) ...... 43 4.9 Towards a uniform proof ...... 44
5 Proof of the main theorem 47 5.1 The case G = G(m,1,1) ...... 47
5.2 The case G = G(1,1,n + 1) = Sn ...... 47 5.3 The groups G(m, p,n): structure of the stabiliser ...... 48 5.4 The groups G(m, p,n): proof of the inequality ...... 52 5.5 The exceptional groups ...... 55 5.5.1 Exceptional groups of rank 2 ...... 55 5.5.2 Exceptional groups of higher rank ...... 56 5.6 The case d = h ...... 57
Bibliography 59
A Sage code 63 CONTENTS ix
B Tables 67 List of figures
2.1 The symmetric group S3 as a reflection group...... 6 2.2 The dihedral groups of orders 10 and 12 as reflection groups...... 7
3.1 Some elements of B3 ...... 24 reg 3.2 The (unique) distinguished braid reflection in B(µm), as a path in V (left), and as a loop in V reg/G (right)...... 25
3.3 The generator π = β of Z(P3) = Z(B3)...... 27
3.4 A subdiagram of type A3 × A1 in the Coxeter diagram of type E6...... 29
x List of tables
2.1 Coxeter graphs of irreducible real reflection groups ...... 11
B.1 Groups of rank 2 ...... 67 B.2 Groups of higher rank ...... 68
xi
Chapter 1
Introduction
1.1 Stabilisers of eigenvectors in complex reflection groups
Finite real reflection groups play an important role in many areas of mathematics, arising for example, as Weyl groups of semisimple Lie algebras. Complex reflection groups are a generalisation of the more familiar real reflection groups, arising naturally in the study of eigenspaces of real reflection group elements, and also as automorphism groups of certain polytopes. The eigenspaces of elements of complex reflection groups reveal a rich pattern, studied exten- sively by Springer [34]. In this thesis, we continue in that direction by looking at the stabiliser of an eigenvector (which, by a theorem of Steinberg [35], is also a complex reflection group). Specifically, we prove the following theorem.
Theorem 1.1. Let (G,V) be an irreducible complex reflection group with dimV = n, w ∈ G any element, and x ∈ V an eigenvector of w with eigenvalue a primitive dth root of unity. Write N ∗ ∗ (respectively Nx) for the number of reflections and N (respectively Nx ) for the number of reflecting hyperplanes of G (respectively, of the stabiliser of x). Then, we have,
∗ ∗ N + N − Nx − Nx ≥ dn with equality if and only if G can be generated by n reflections and d is the largest degree of G.
Formally, a complex reflection group is a finite group G which acts on a finite-dimensional hermitian vector space V by pseudo-reflections—that is, finite-order unitary transformations that stabilise a complex hyperplane. Complex reflection groups arise, for example, as quotients of normalisers of maximal eigenspaces of elements of real reflection groups by the centralisers of the same eigenspaces. Thus, they can be considered a natural generalisation of real reflection groups
1 2 CHAPTER 1. INTRODUCTION
(which correspond to the case of an eigenvalue of 1). For example, if G = Smn, w is a product of n disjoint cycles of length m, and E is the eigenspace of w with eigenvalue exp(2πi/m), then the normaliser NG(E) acts on E as the group G(m,1,n) of generalised permutation matrices; see the beginning of Chapter 3 for a more detailed discussion. As with finite real reflection groups, there is a classification of complex reflection groups— namely, if G is irreducible, then it either belongs to the infinite series G(m, p,n), which consist of generalised permutation matrices, or it is one of 34 exceptions, G4 through G37. An important characterisation of complex reflection groups is the Chevalley–Shephard–Todd Theorem, which states that for G a finite subgroup of GL(V), G is a complex reflection group if G and only if the invariant algebra C[V] is generated by algebraically independent elements, whose degrees d1,...,dn are independent of the choice of generators. These numbers are called the degrees, and they contain a considerable amount of information about G. The study of eigenspaces of reflection group elements has a long history, going back at least as far as the discovery by Coxeter [15] and Coleman [14] of a relationship between the degrees of a real reflection group and the eigenvalues of what are now known as Coxeter elements. Later, a systematic study of eigenspaces of arbitrary elements was undertaken by Springer [34], who showed that there is a close relationship between the degrees and the orders of eigenvalues of elements. Springer also explored the case where an eigenvector is regular—that is, when it does not lie on any reflecting hyperplane—showing that certain properties of Coxeter elements are special cases of a more general pattern. In particular, we note that Springer’s work recovers the earlier result of Kostant [26], that if G is an irreducible real reflection group, then in the above setting the number of roots |Φ| is at least dn, with equality if and only if w is a Coxeter element. An interesting strengthening of this inequality was recently discovered by Kamgarpour [24], who proved that
|Φ| − |Φx| ≥ dn, (1.1.1) with equality if and only if w is a Coxeter element. Here, Φx denotes the set of roots of the stabiliser ∗ Gx of x in G. Notice that for G a real reflection group, we have |Φ| = N + N ; hence, (1.1.1) is a special case of Theorem 1.1. We can restate (1.1.1) more conceptually as follows. For any complex reflection group G, let V reg denote the complement of the hyperplane arrangement of G in V. Since by definition, G acts freely on V reg, the quotient space V reg/G is a manifold, and there is an exact sequence,
1 → P → B → G → 1, 1.1. STABILISERS OF EIGENVECTORS IN COMPLEX REFLECTION GROUPS 3
where the pure braid group P is defined to be the fundamental group of V reg and the braid group B is defined to be the fundamental group of V reg/G. Braid groups were studied extensively by Broue,´ Malle and Rouquier [9], who introduced a length function ` : B → Z generalising the length function on a real reflection group. They also show the pure braid group Px and the braid group Bx of Gx inject into P and B respectively, compatibly with the length functions. It was conjectured by [9], and proven by Digne, Marin and Michel [18], that the centre of P is a cyclic group generated by an element π of length N + N∗. Combining these results, it follows that Kamgarpour’s inequality can be restated as,
`(π) − `(π x) ≥ dn, where π x denotes the generator of Z(Px) of positive length. As this inequality makes sense for any irreducible complex reflection group, it is a natural question to ask whether it holds in this greater generality—a question that Theorem 1.1 answers in the affirmative. The braid-theoretic nature of the above inequality also raises the more difficult question (which we have been unable to answer) of whether there is a uniform proof of Theorem 1.1, for example using the topology of the hyperplane arrangement instead of the Shephard–Todd classification. However, as we show in Section 4.9, Theorem 1.1 is closely related to the following conjecture, which was suggested to us by Jean Michel.
Conjecture 1.2 (Michel, private communication [29]). In the setting of Theorem 1.1, there exists a d −e lift w of some element of Gxw to B such that w = ππππ x for some e ≥ 0.
We prove Theorem 1.1 via the classification of irreducible complex reflection groups. For the infinite series G(m, p,n), the key idea is to associate to x a G-invariant “characteristic polynomial”. ∗ We are then able to bound Nx +Nx by studying the action of Gx on the roots of this polynomial. For all but five of the 34 exceptional cases, Theorem 1.1 can be proven by comparing the largest value ∗ that Nx + Nx can take (which is easily deduced from the classification of parabolics by Taylor [37]), with the largest degree (which bounds d, by the work of Springer). However, the three cases G25,
G31 and G32 required an exhaustive verification using the computer algebra system SageMath [38]. This thesis is structured as follows. Background on real reflection groups is introduced in Chapter 2, while complex reflection groups and their braid groups are discussed in Chapter 3. In Chapter 4, we review previous work on eigenvalues and eigenvectors of reflection group elements, state the main theorem and its braid-theoretic interpretation, and discuss the prospects for a uniform proof using braid theory. Finally, in Chapter 5, we present our proof of Theorem 1.1 using the case-by-case approach sketched above.
Chapter 2
Real reflection groups
Finite real reflection groups have been studied extensively due to the pivotal role that they play in Lie theory. Here we give an overview of important facts about these groups. For a more detailed exposition, see [22] or [5].
2.1 Definition and examples
Definition 2.1. (i). Let V be a real vector space equipped with an inner product, (·,·).A reflection
in V is a transformation of the form rα : V → V defined by
(v,α) r (v) = v − 2 α, α (α,α)
def ⊥ for some α ∈ V. Notice that rα fixes the hyperplane Hα = α , which is called the reflecting
hyperplane, and that rα sends α to −α.
(ii). A (finite) real reflection group is a pair (G,V) consisting of a Euclidean space V and a finite subgroup G of the orthogonal group O(V) generated by reflections.
(iii). G is said to be irreducible if we cannot write V = V1 ⊥ V2 and G = G1 × G2 with Gi < O(Vi).
(iv). The rank of G is the codimension of V G in V.
Example 2.2. The symmetric group Sn can be realised as an irreducible real reflection group as n follows. Let Sn act on R by permuting the coordinates. The elements of Sn are then given by permutation matrices, that is, matrices with entries in {0,1} with a unique nonzero entry in each
5 6 CHAPTER 2. REAL REFLECTION GROUPS
row and column. For example, 0 1 0 0 0 0 0 1 1 0 0 0 0 0 1 0 is the permutation matrix corresponding to the permutation (1342). This action restricts to an action on the subspace, n V = (x1,...,xn) ∈ R | x1 + ··· + xn = 0 , so the rank of Sn is n − 1. For example, the S3 case is depicted in Figure 2.1. To see that this is a reflection group, recall that Sn is generated by the transpositions (i,i + 1) for 1 ≤ i < j ≤ n.
Geometrically, any transposition (i, j) acts via the reflection rei−e j , where ei is the ith standard unity n vector in R .
s1
α2 α1 + α2
s1s2s1 = s2s1s2 s2
−α1 α1
−α1 − α2 −α2
Figure 2.1: The symmetric group S3 as a reflection group.
Example 2.3. For any integer m ≥ 3 let D2m (or I2(m)) denote the dihedral group of order 2m, i.e. the group of symmetries of a regular m-gon. This can be realised as an irreducible real reflection group of rank 2 as follows. Suppose that the vertices of the m-gon are (cos(2kπ/m),sin(2kπ/m)), and let s1 be the reflection about the x-axis, and s2 be the reflection through the line generated be the vector (cos(π/m),sin(π/m)), as depicted in Figure 2.2 (notice the different behaviours for even and odd m). Then, one can check that s2 ◦ s1 is a rotation by 2π/m, so that s1 and s2 generate D2m. 2.2. ROOT SYSTEMS 7
s2 s2 s 1 s1
Figure 2.2: The dihedral groups of orders 10 and 12 as reflection groups.
2.2 Root systems
Following [22], we define a root system as follows. Note that this is not the only definition in the literature: see Remark 2.5.
Definition 2.4. A (reduced) root system in a Euclidean vector space V is a finite subset Φ ⊂ V \{0} such that:
(i). The rα for α ∈ Φ permute Φ,
(ii). For all α ∈ Φ, we have Rα ∩ Φ = {±α}.
To any root system Φ we can associate a reflection group hrα | α ∈ Φi. On the other hand, we can associate to each reflection group G a root system Φ as the set of unit normal vectors to the reflecting hyperplanes of V. For example, a root system for S3 is given in Figure 2.1. Similarly, a root system for the dihedral group of order 2m is given by
kπ kπ −sin ,cos 0 ≤ k ≤ 2m − 1 . m m
Remark 2.5. Some sources (such as [5]) use a more restrictive definition, which amounts to requiring that for each α ∈ Φ, the linear form1 2(·,α)/(α,α) takes integer values on Φ. Such root systems are called crystallographic. Assuming a crystallographic root system Φ for the group G def exists, it immediately follows that G acts on the lattice Q = hΦiZ.
Let φ : V → R be any linear form such that φ(α) 6= 0 for all α ∈ Φ. Then, we can write
Φ = Φ+ t Φ−, where Φ+ = {α ∈ Φ | φ(α) > 0} and Φ− = −Φ+ = {α ∈ Φ | φ(α) < 0}. Elements of Φ+ are called positive roots.
1In fact, Bourbaki does not fix a Euclidean form, and instead talks about coroots in V ∗. 8 CHAPTER 2. REAL REFLECTION GROUPS
If G is crystallographic, and Φ is a crystallographic root system, the lattice Q has a unique basis + of roots ∆ = {α1,...,αn} ⊂ Φ , called the simple roots such that all positive roots are nonnegative def linear combinations of simple roots; furthermore, the corresponding simple reflections si = rαi generate G [5, Ch. V §3.2]. In the non-crystallographic case, we cannot expect something this strong. Nevertheless, there is a weaker notion of simple roots in this case, which can be found in [22].
Theorem 2.6 ( [22, §1.3, 1.5]). Let Φ be any root system, and Φ+ as above. Then, there exists a unique subset + ∆ = {α1,...,αn} ⊆ Φ , called the set of simple roots, such that for any β ∈ Φ we have n β = ∑ aiαi, i=1
+ def and the ai are nonnegative for β ∈ Φ . Furthermore, the simple reflections si = rαi are a minimal set of generators for G.
Remark 2.7. Notice that (αi,α j) < 0, since otherwise at least one out of si(α j) and s j(αi) will be positive, but not a nonnegative linear combination of simple roots.
2.3 Length
Definition 2.8. For any element w ∈ G, denote by `(w) the shortest length of a word for w in the simple reflections. Then, `(w) is called the length of w, and any word for w of length `(w) is called a reduced word.
We have the following standard facts about the length function ` : G → Z≥0.
Proposition 2.9 (Exchange relation, [5, Ch. 4, §1, Prop. 4]). Let w ∈ G and α ∈ ∆, and let w = si1 ···sik be a reduced word. Then,
(i). `(rα w) = k ± 1,
(ii). If `(rα w) = k + 1, then rα si1 ···sik is a reduced word.
(iii). If `(rα w) = k − 1, then there exists 1 ≤ j ≤ k such that
rα w = si1 ···si j−1 si j+1 ···sik
is a reduced word. 2.4. COXETER GROUPS 9
Proposition 2.10 ( [22, §1.7]). For any w ∈ G, `(w) is equal to the number of positive roots α such that w(α) is negative.
+ Proposition 2.11 ( [22, §1.8]). There is a unique element w0 ∈ G of length |Φ |, called the longest element. The order of w0 is 2.
The terminology longest element is justified by Proposition 2.10, in that the length of an element cannot exceed |Φ+|. Furthermore, we can define a partial order ≤ on G by declaring2 that for w1,w2 ∈ G, we have w1 ≤ w2 if and only if there exists g ∈ G such that gw1 = w2 and
`(g) + `(w2) = `(w2). The element w0 is then the unique maximal element with respect to ≤. There is a second length function on G: the reflection length. We define T to be the collection of all reflections. Since T is stable under G-conjugation, we see that G has a presentation given by the generators T modulo all relations of the form st = tu; this is called the Steinberg presentation.
Definition 2.12. The reflection length `T : G → Z≥0 is defined by taking w ∈ G to the minimal length of any word for w in T.
Proposition 2.13 was proven by Carter in [10, §2 Lemma 3] in the context of Weyl groups, but as observed by Bessis in [2], Carter’s proof works more generally.
Proposition 2.13 (Carter). For any w ∈ G, we have,