Enumerating Chambers of Hyperplane Arrangements with Symmetry

Total Page:16

File Type:pdf, Size:1020Kb

Enumerating Chambers of Hyperplane Arrangements with Symmetry ENUMERATING CHAMBERS OF HYPERPLANE ARRANGEMENTS WITH SYMMETRY TAYLOR BRYSIEWICZ, HOLGER EBLE, AND LUKAS KUHNE¨ Abstract. We introduce a new algorithm for enumerating chambers of hyperplane arrangements which exploits their underlying symmetry groups. Our algorithm counts the chambers of an arrangement as a byproduct of computing its characteristic polynomial. We showcase our julia implementation, based on OSCAR, on examples coming from hyper- plane arrangements with applications to physics and computer science. Keywords. Hyperplane arrangement, chambers, algorithm, symmetry, resonance arrangement, separability 1. Introduction The problem of enumerating chambers of hyperplane arrangements is a well-known challenge in computational discrete geometry [19, 28, 33, 42]. We develop a novel chamber-counting algorithm which takes advantage of the combinatorial symmetries of an arrangement. This count is derived from the computation of other important combinatorial invariants: Betti numbers and characteristic polynomials [1, 20, 29, 37, 43, 45]. While most arrangements admit few combinatorial symmetries [39], most arrangements of interest do [18, 40, 46]. We implemented our algorithm in julia [3] and published it as the pack- age CountingChambers.jl1. Our implementation relies heavily on the cor- nerstones of the new computer algebra system OSCAR [38] for group theory computations (GAP [16]) and the ability to work over number fields (Hecke and Nemo [15]). To the best of our knowledge, it is the first publicly available software for counting chambers which uses symmetry. We showcase our algorithm and its implementation on a number of well- known examples, such as the resonance and discriminantal arrangements. Additionally, we study sequences of hyperplane arrangements which come from the problem of linearly separating vertices of regular polytopes. In particular, we investigate one corresponding to the hypercube [0; 1]d whose arXiv:2105.14542v2 [math.CO] 25 Jun 2021 chambers are in bijection with linearly separable Boolean functions. In the presence of symmetry, our implementation outperforms the exist- ing software by several orders of magnitude (cf. Table 1). Moreover, its output is guaranteed to be accurate since we compute symbolically over the integers or exact number fields and avoid overflow errors thanks to the package SaferIntegers.jl [41]. 9 The ninth resonance arrangement (511 hyperplanes in R ) approaches the limit of what is possible with our implementation: the computation of its 2010 Mathematics Subject Classification. 52C35, 52B15. 1available at https://mathrepo.mis.mpg.de/CountingChambers 1 2 T. BRYSIEWICZ, H. EBLE, AND L. KUHNE¨ characteristic polynomial took 10 days on 42 processors. Our computation confirms that its chamber-count is 1955230985997140 as independently and concurrently computed by Chroman and Singhar with different methods [9]. We first give background on hyperplane arrangements in Section 2. The ideas outlined in Section 3, regarding deletion and restriction algorithms, form the basic structure of our algorithm. We explain the relevant results regarding symmetries of arrangements in Section 4. The algorithm and its implementation details reside in Section 5. In Section 6 we construct and discuss examples of arrangements exhibiting large symmetry groups. We conclude in Section 7 with timings and comparisons to other software. Acknowledgements We are very grateful to Tommy Hofmann, Christopher Jefferson, and Marek Kaluba for their support regarding the implementation and to Michael Cuntz for initial verifications of our computations. We would also like to thank Michael Joswig for his helpful comments throughout the project and Bernd Sturmfels for suggesting the discriminantal arrangement. 2. Hyperplane arrangements We begin by discussing background on the theory of hyperplane arrange- ments related to the problem of enumerating chambers: the main goal of this article and the associated software. Our notation will mostly follow the textbook by Orlik and Terao [37]. d For any field K, a hyperplane in K is an affine linear space of codi- mension one. Throughout this article, we denote by = H1;:::;Hn a A d f g (hyperplane) arrangement where Hi is a hyperplane in K . d Definition 1. Suppose is an arrangement in R . The connected com- A d S ponents of the complement R H2A H are called chambers of and are denoted ch( ). n A A Example 2. We use the arrangement y x = 1 ; x = 0 ; x + y = 1 ; y = 0 ff| −{z g} |f {z g} |f {z g} |f {z g}g H1 H2 H3 H4 2 in R as a running example. This arrangement is depicted in Figure 1. It has 10 chambers: 2 bounded and 8 unbounded. H1 H3 H2 H4 Figure 1. The arrangement introduced in Example 2. Given a subset I [n] := 1; : : : ; n , we write the set Hi i2I as HI and ⊆ T f g f g its intersection as LI = i2I Hi. The collection of these intersections form ENUMERATING CHAMBERS OF ARRANGEMENTS WITH SYMMETRY 3 the set L( )= LI I [n] ;LI = , a combinatorial shadow of known as its intersectionA f posetj ⊆. This poset6 ;g is ordered by reverse inclusionA and graded by the rank function, r : L( ) Z≥0, where r(LI ) = codim (LI ). A ! As a notational convention, we set r(I) = r(LI ) for I [n] whenever LI = . ⊆ 6 ; 2.1. The characteristic polynomial. Our algorithm counts chambers of an arrangement by computing a more refined count, namely the Betti num- bers. Knowing the Betti numbers of an arrangement is equivalent to knowing its characteristic polynomial. d Definition 3. The characteristic polynomial of an arrangement in K is the polynomial A d X jIj d−r(I) X i d−i (1) χA(t)= ( 1) t = ( 1) bi( )t : − − A I⊆[n]:LI 6=; i=0 d The integers bi( ) i=0, defined via (1), are non-negative and are called the Betti numbersf ofA g. We denote the vector of Betti numbers by b( ). A A The characteristic polynomial and Betti numbers of an arrangement depend only on the intersection poset L( ) and have various interpretationsA A depending on the field K as detailed below. d Real: For an arrangement in R , Zaslavsky [45] proved that A d d X ch( ) = ( 1) χA( 1) = bi( ): j A j − − A i=0 Thus, the Betti numbers are a refined count of the chambers of . They have the following geometric interpretation. Given a genericA d flag • : F0 F1 Fd = R of affine linear subspaces Fi F ⊂ ⊂ · · · ⊂ (where dim(Fi) = i) the number of chambers of which meet Fi A but do not meet Fi−1 is equal to bi( ) [44, Proposition 2.3.2]. Ad Complex: If is an arrangement in C where all hyperplanes contain A the origin, then bi( ) is the i-th topological Betti number of the d S A complement C H with rational coefficients [36]. n H2A Finite: When is an arrangement over a finite field Fq, Crapo and A d S Rota proved that χA(q) = Fq H2A H [11]. Moreover, if is a hy- jd n j A perplane arrangement in Q one may consider its reduction modulo q: Fq = H1 Fq;:::;Hn Fq . When q is sufficiently large, we A ⊗ f ⊗ ⊗ g have that L( ) = L( Fq) and thus computing χA(t) for rational arrangementsA also yieldsA ⊗ the number of points in the complement after reducing modulo large primes. Example 4. Let be the arrangement introduced in Example 2. Its char- A 2 acteristic polynomial is χA(t) = t 4t + 5. Figure 2 shows a generic flag • intersecting this arrangement verifying− that b( ) = (1; 4; 5). F A 3. A deletion-restriction algorithm d To compute the Betti numbers of an arrangement in K , we take ad- A vantage of the behavior of χA(t) under the operations of deletion and re- striction. These operations reduce computations about to computations A 4 T. BRYSIEWICZ, H. EBLE, AND L. KUHNE¨ F2 F1 F0 2 Figure 2. The intersections of a generic flag (purple) in R with the chambers of . The point F0 intersects one cham- A ber, F1 intersects four others, and F2 intersects the remain- ing 5, and so b( ) = (1; 4; 5). A about two smaller arrangements. Thus at its core, our main algorithm is a divide-and-conquer algorithm. Given a hyperplane H , the deletion of H in is the arrangement 2 A A d−1 H . The restriction of H in is the arrangement in H ∼= K defined byAnf Hg= K H K H A. The following lemma provides the basic foundationA f of\ our algorithm.j 2 Anf gg Lemma 5 [37, Corollary 2.57]. Given a hyperplane H , we have that 2 A H χA(t) = χAnfHg(t) χAH (t): In particular, b( ) = b( H ) + 0 b( ) where 0 b means prepending− the vector b with aA zero. Anf g j A j 3.1. A simple deletion-restriction algorithm. Lemma 5 along with the d d+1 fact that the empty arrangement in K has Betti numbers (1; 0;:::; 0) N suggests the following well-known recursive algorithm for computing2b( ). A Algorithm 1: Betti numbers via simple deletion and restriction d Input: A hyperplane arrangement in K Output: The Betti numbers b( ) A BettiNumbers ( ) A A 1 if = then ; 6 A 2 choose H 2 A 3 return BettiNumbers( H ) + 0 BettiNumbers( H ) Anf g j A 4 else 5 return (1; 0;:::; 0) Structurally, Algorithm 1 is a depth-first binary tree algorithm on ar- rangements, rooted at the initial input: one child represents a deletion and the other a restriction, as shown in Figure 3. The implementation of Algorithm 1 is already nontrivial as it is often the case that some hyperplanes become the same after a restriction. Thus, its proper implementation requires care in representing an arrangement on a computer. 3.2. Computationally representing deletions and restrictions. An arrangement coming from via deletions and restrictions may be repre- sented by an encodingB of theA restricted hyperplanes.
Recommended publications
  • JMM 2017 Student Poster Session Abstract Book
    Abstracts for the MAA Undergraduate Poster Session Atlanta, GA January 6, 2017 Organized by Eric Ruggieri College of the Holy Cross and Chasen Smith Georgia Southern University Organized by the MAA Committee on Undergraduate Student Activities and Chapters and CUPM Subcommittee on Research by Undergraduates Dear Students, Advisors, Judges and Colleagues, If you look around today you will see over 300 posters and nearly 500 student presenters, representing a wide array of mathematical topics and ideas. These posters showcase the vibrant research being conducted as part of summer programs and during the academic year at colleges and universities from across the United States and beyond. It is so rewarding to see this session, which offers such a great opportunity for interaction between students and professional mathematicians, continue to grow. The judges you see here today are professional mathematicians from institutions around the world. They are advisors, colleagues, new Ph.D.s, and administrators. We have acknowledged many of them in this booklet; however, many judges here volunteered on site. Their support is vital to the success of the session and we thank them. We are supported financially by Tudor Investments and Two Sigma. We are also helped by the mem- bers of the Committee on Undergraduate Student Activities and Chapters (CUSAC) in some way or other. They are: Dora C. Ahmadi; Jennifer Bergner; Benjamin Galluzzo; Kristina Cole Garrett; TJ Hitchman; Cynthia Huffman; Aihua Li; Sara Louise Malec; Lisa Marano; May Mei; Stacy Ann Muir; Andy Nieder- maier; Pamela A. Richardson; Jennifer Schaefer; Peri Shereen; Eve Torrence; Violetta Vasilevska; Gerard A.
    [Show full text]
  • Matroid Automorphisms of the F4 Root System
    ∗ Matroid automorphisms of the F4 root system Stephanie Fried Aydin Gerek Gary Gordon Dept. of Mathematics Dept. of Mathematics Dept. of Mathematics Grinnell College Lehigh University Lafayette College Grinnell, IA 50112 Bethlehem, PA 18015 Easton, PA 18042 [email protected] [email protected] Andrija Peruniˇci´c Dept. of Mathematics Bard College Annandale-on-Hudson, NY 12504 [email protected] Submitted: Feb 11, 2007; Accepted: Oct 20, 2007; Published: Nov 12, 2007 Mathematics Subject Classification: 05B35 Dedicated to Thomas Brylawski. Abstract Let F4 be the root system associated with the 24-cell, and let M(F4) be the simple linear dependence matroid corresponding to this root system. We determine the automorphism group of this matroid and compare it to the Coxeter group W for the root system. We find non-geometric automorphisms that preserve the matroid but not the root system. 1 Introduction Given a finite set of vectors in Euclidean space, we consider the linear dependence matroid of the set, where dependences are taken over the reals. When the original set of vectors has `nice' symmetry, it makes sense to compare the geometric symmetry (the Coxeter or Weyl group) with the group that preserves sets of linearly independent vectors. This latter group is precisely the automorphism group of the linear matroid determined by the given vectors. ∗Research supported by NSF grant DMS-055282. the electronic journal of combinatorics 14 (2007), #R78 1 For the root systems An and Bn, matroid automorphisms do not give any additional symmetry [4]. One can interpret these results in the following way: combinatorial sym- metry (preserving dependence) and geometric symmetry (via isometries of the ambient Euclidean space) are essentially the same.
    [Show full text]
  • European Journal of Combinatorics a Survey on Spherical Designs And
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector European Journal of Combinatorics 30 (2009) 1392–1425 Contents lists available at ScienceDirect European Journal of Combinatorics journal homepage: www.elsevier.com/locate/ejc A survey on spherical designs and algebraic combinatorics on spheres Eiichi Bannai a, Etsuko Bannai b a Faculty of Mathematics, Graduate School, Kyushu University, Hakozaki 6-10-1, Higashu-ku, Fukuoka, 812-8581, Japan b Misakigaoka 2-8-21, Maebaru-shi, Fukuoka, 819-1136, Japan article info a b s t r a c t Article history: This survey is mainly intended for non-specialists, though we try to Available online 12 February 2009 include many recent developments that may interest the experts as well. We want to study ``good'' finite subsets of the unit sphere. To consider ``what is good'' is a part of our problem. We start with n−1 n the definition of spherical t-designs on S in R : After discussing some important examples, we focus on tight spherical t-designs on Sn−1: Tight t-designs have good combinatorial properties, but they rarely exist. So, we are interested in the finite subsets on Sn−1, which have properties similar to tight t-designs from the various viewpoints of algebraic combinatorics. For example, rigid t-designs, universally optimal t-codes (configurations), as well as finite sets which admit the structure of an association scheme, are among them. We will discuss various results on the existence and the non-existence of special spherical t-designs, as well as general spherical t-designs, and their constructions.
    [Show full text]
  • COXETER GROUPS (Unfinished and Comments Are Welcome)
    COXETER GROUPS (Unfinished and comments are welcome) Gert Heckman Radboud University Nijmegen [email protected] October 10, 2018 1 2 Contents Preface 4 1 Regular Polytopes 7 1.1 ConvexSets............................ 7 1.2 Examples of Regular Polytopes . 12 1.3 Classification of Regular Polytopes . 16 2 Finite Reflection Groups 21 2.1 NormalizedRootSystems . 21 2.2 The Dihedral Normalized Root System . 24 2.3 TheBasisofSimpleRoots. 25 2.4 The Classification of Elliptic Coxeter Diagrams . 27 2.5 TheCoxeterElement. 35 2.6 A Dihedral Subgroup of W ................... 39 2.7 IntegralRootSystems . 42 2.8 The Poincar´eDodecahedral Space . 46 3 Invariant Theory for Reflection Groups 53 3.1 Polynomial Invariant Theory . 53 3.2 TheChevalleyTheorem . 56 3.3 Exponential Invariant Theory . 60 4 Coxeter Groups 65 4.1 Generators and Relations . 65 4.2 TheTitsTheorem ........................ 69 4.3 The Dual Geometric Representation . 74 4.4 The Classification of Some Coxeter Diagrams . 77 4.5 AffineReflectionGroups. 86 4.6 Crystallography. .. .. .. .. .. .. .. 92 5 Hyperbolic Reflection Groups 97 5.1 HyperbolicSpace......................... 97 5.2 Hyperbolic Coxeter Groups . 100 5.3 Examples of Hyperbolic Coxeter Diagrams . 108 5.4 Hyperbolic reflection groups . 114 5.5 Lorentzian Lattices . 116 3 6 The Leech Lattice 125 6.1 ModularForms ..........................125 6.2 ATheoremofVenkov . 129 6.3 The Classification of Niemeier Lattices . 132 6.4 The Existence of the Leech Lattice . 133 6.5 ATheoremofConway . 135 6.6 TheCoveringRadiusofΛ . 137 6.7 Uniqueness of the Leech Lattice . 140 4 Preface Finite reflection groups are a central subject in mathematics with a long and rich history. The group of symmetries of a regular m-gon in the plane, that is the convex hull in the complex plane of the mth roots of unity, is the dihedral group of order 2m, which is the simplest example of a reflection Dm group.
    [Show full text]
  • The Fundamental Group of SO(N) Via Quotients of Braid Groups Arxiv
    The Fundamental Group of SO(n) Via Quotients of Braid Groups Ina Hajdini∗ and Orlin Stoytchevy July 21, 2016 Abstract ∼ We describe an algebraic proof of the well-known topological fact that π1(SO(n)) = Z=2Z. The fundamental group of SO(n) appears in our approach as the center of a certain finite group defined by generators and relations. The latter is a factor group of the braid group Bn, obtained by imposing one additional relation and turns out to be a nontrivial central extension by Z=2Z of the corresponding group of rotational symmetries of the hyperoctahedron in dimension n. 1 Introduction. n The set of all rotations in R forms a group denoted by SO(n). We may think of it as the group of n × n orthogonal matrices with unit determinant. As a topological space it has the structure of a n2 smooth (n(n − 1)=2)-dimensional submanifold of R . The group structure is compatible with the smooth one in the sense that the group operations are smooth maps, so it is a Lie group. The space SO(n) when n ≥ 3 has a fascinating topological property—there exist closed paths in it (starting and ending at the identity) that cannot be continuously deformed to the trivial (constant) path, but going twice along such a path gives another path, which is deformable to the trivial one. For example, if 3 you rotate an object in R by 2π along some axis, you get a motion that is not deformable to the trivial motion (i.e., no motion at all), but a rotation by 4π is deformable to the trivial motion.
    [Show full text]
  • The Strong Symmetric Genus and Generalized Symmetric Groups: Results and a Conjecture
    The strong symmetric genus and generalized symmetric groups: results and a conjecture Michael A. Jackson Grove City College, USA [email protected] Special Session on Group Theory, Actions, and Computation AMS-NZMS Joint Meeting Wellington, New Zealand December, 15 2007 1 Strong Symmetric Genus Given a finite group G, the smallest genus of any closed orientable topological surface on which G acts faithfully as a group of orientation preserving symmetries is called the strong symmetric genus of G. The strong symmetric genus of the group G is denoted σ0(G). By a result of Hurwitz [1893], if σ0(G) > 1 for a finite group 0 |G| G, then σ (G) ≥ 1 + 84 . 2 Known results on the strong symmetric genus All groups G such that σ0(G) ≤ 4 are known. [Broughton, 1991; May and Zimmerman, 2000 and 2005] For each positive integer n, there is exists a finite group G with σ0(G) = n. [May and Zimmerman, 2003] 3 Known results on the strong symmetric genus continued The strong symmetric genus is known for the following groups: • P SL2(q) [Glover and Sjerve, 1985 and 1987] • SL2(q) [Voon, 1993] • the sporadic finite simple groups [Conder, Wilson and Woldar, 1992; Wilson, 1993, 1997 and 2001] 4 Known results on the strong symmetric genus continued The strong symmetric genus is known for the following groups: • alternating and symmetric groups [Conder, 1980 and 1981] • the hyperoctahedral groups [J, 2004] • the remaining finite Coxeter groups [J, 2007] 5 The Generalized Symmetric Groups G(n, m) = Zm o Σn for n > 1 and m ≥ 1.
    [Show full text]
  • Lecture 3 1 Structure of the Automorphism Group
    Hypercube problems Lecture 3 October 24, 2012 Lecturer: Petr Gregor Scribe by: Otakar Trunda Updated: November 8, 2012 1 Structure of the automorphism group In this talk we take a closer look at the structure of Γ = Aut(Qn). We already know that n 8g 2 Γ 9!π 2 Sn 9!a 2 Z2 such that g = rπta where rπ 2 Rn; ta 2 Tn: A subgroup N of a group G is normal (denoted by N C G) if it is invariant under −1 conjugation; that is, gNg = N for every g 2 G. It is easy to see that Tn C Γ for every n ≥ 1 and Rn 6 Γ for every n ≥ 2. Definition 1 Let G, H be groups. The direct product of G and H (denoted by G × H) is the group on f(g; h) j g 2 G; h 2 Hg with the operation defined by (g1; h1)(g2; h2) = (g1g2; h1h2). Note that Γ cannot be expressed as Rn ×Tn since (rπ; ta)(rρ; tb) 6= (rπrρ; tatb). However, we can use a conjugation to express the composition since (rπ; ta)(rρ; tb) = (rπ(rρrρ−1 ); ta)(rρ; tb) = (rπrρ; (rρ−1 tarρ)tb): Definition 2 Let H, N be groups and let ' : H ! Aut(N) be a homomorphism. The semidirect product (external) of H and N with respect to ' (we write H n' N) is the group on −1 f(h; n); h 2 H; n 2 Ng with the operation defined by (h1; n1)(h2; n2) = (h1h2;'(h2 )(n1)n2): If H, N are subgroups of same group and N is normal then we can use the homomorphism −1 ' defined by '(h): n 7! hnh (a conjugation by h).
    [Show full text]
  • Complex Reflection Groups, Their Irreducible Representations, and a Generalized Robinson-Schensted Algorithm
    Complex reflection groups, their irreducible representations, and a generalized Robinson-Schensted algorithm Aba Mbirika Department of Mathematics University of Wisconsin{Eau Claire Eau Claire, WI 54701 email: [email protected] The purpose of this brief overview is to introduce readers to the objects of my research involving complex reflection groups. This introductory material is not intended to provide particular results of my current research. However, it is intended to do the following: (1) Give a brief introduction to complex reflection groups and a variety of ways to view their elements combinatorially. (2) Define the irreducible representations of this infinite family of groups. (3) Explain a generalized Robinson-Schensted algorithm by first looking at an example in the smallest non-trivial case|namely, the hyperoctahedral group. Understanding this simplest setting helps to understand the arbitrary setting introduced next. (4) Give a generalized Robinson-Schensted algorithm for arbitrary complex reflection groups, and provide some related combinatorial implications of this map. 1. Brief introduction to the complex reflection groups G(r; p; n) The family of imprimitive complex reflections groups are defined as follows. Let r; p; n 2 p N 2π −1 with pjr and let ζ = exp r . The groups G(r; p; n) are the subgroups of GLn(C) consisting of matrices such that • the entries are either 0 or powers of ζ, • there is exactly one nonzero entry in each row and column, and • the (r=p)-th power of the product of all nonzero entries is 1. Together with 34 exceptional groups, the groups G(r; p; n) account for all finite groups gen- erated by complex reflections [4].
    [Show full text]
  • Odd Length for Even Hyperoctahedral Groups and Signed Generating Functions 1
    Odd length for even hyperoctahedral groups and signed generating functions 1 Francesco Brenti Dipartimento di Matematica Universit`adi Roma \Tor Vergata" Via della Ricerca Scientifica, 1 00133 Roma, Italy [email protected] Angela Carnevale 2 Fakultat f¨urMathematik Universit¨atBielefeld D-33501 Bielefeld, Germany [email protected] Abstract We define a new statistic on the even hyperoctahedral groups which is a natural analogue of the odd length statistic recently defined and studied on Coxeter groups of types A and B. We compute the signed (by length) generating function of this statistic over the whole group and over its maximal and some other quotients and show that it always factors nicely. We also present some conjectures. 1 Introduction The signed (by length) enumeration of the symmetric group, and other finite Coxeter groups by various statistics is an active area of research (see, e.g., [1, 2, 4, 6, 7, 10, 11, 12, 13, 14, 19]). For example, the signed enumeration of classical Weyl groups by major index was carried out by Gessel-Simion in [19] (type A), by Adin-Gessel-Roichman in [1] (type B) and by Biagioli in [2] (type D), that by descent by Desarmenian-Foata in [7] (type A) and by Reiner in [13] (types B and D), while that by excedance by Mantaci in [11] and independently by Sivasubramanian in [14] (type A) and by Mongelli in [12] (other types). 12010 Mathematics Subject Classification: Primary 05A15; Secondary 05E15, 20F55. 2Partially supported by German-Israeli Foundation for Scientific Research and Development, grant no. 1246. 1 In [9], [17] and [18] two statistics were introduced on the symmetric and hyperoctahe- dral groups, in connection with the enumeration of partial flags in a quadratic space and the study of local factors of representation zeta functions of certain groups, respectively (see [9] and [18], for details).
    [Show full text]
  • Orthogonal Group Matrices of Hyperoctahedral Groups
    ORTHOGONAL GROUP MATRICES OF HYPEROCTAHEDRAL GROUPS J. S. FRAME To the memory of TADASI NAKAYAMA n 1. Introduction. The hyperoctahedral group Gn of order 2 n\ is generated by permutations and sign changes applied to n digits, J= 1, 2, . , n. The n 2 sign changes generate a normal subgroup Σn whose factor group GnlΣn is isomorphic with the symmetric group Sn of order n\. To each irreducible orthogonal representation {λ p) of Gn corresponds an ordered pair of par- titions [_λ~] of / and M of m, where ί+m = n. The faithful representation {n - 1 1} of Gn is the real monomial group Rn of degree n. The representa- tions {λ 0} of Gn with l=n, m = 0, are isomorphic with corresponding irre- ducible representations {λ) of Sn. If the representation {λ μ) maps the λμ λμ element gk of Gn into the real orthogonal matrix M (gk) of degree / , we define the group matrix of {λ μ) to be gk^Gn (l.i) Our purpose is to determine explicitly for each {λ ', μ) the z^-entry of the group matrix of an irreducible orthogonal representation of Gn, and incidentally those of Sn, in the form Wλui = rvEλμσXμΰι (1.2) λμ by describing in the group ring Γ of Gn a suitable pair of ring elements E λμ related to permutations of SΛ, and a related to sign changes of Σn, and also λ a set of invertible ring factors γυ that meet our requirements. Matrices M \τd) for transpositions τd of consecutive digits d, d+\ are to be those of λμ Young's orthogonal representation {λ} of Sn M.
    [Show full text]
  • A Character Relationship Between Symmetric Group and Hyperoctahedral Group
    A CHARACTER RELATIONSHIP BETWEEN SYMMETRIC GROUP AND HYPEROCTAHEDRAL GROUP FRANK LUBECK¨ AND DIPENDRA PRASAD, WITH AN APPENDIX BY ARVIND AYYER ABSTRACT. We relate character theory of the symmetric groups S2n and S2n+1 with n that of the hyperoctahedral group Bn = (Z=2) o Sn, as part of the expectation that the character theory of reductive groups with diagram automorphism and their Weyl groups, is related to the character theory of the fixed subgroup of the diagram automorphism. March 27, 2020 CONTENTS 1. Introduction1 2. A lemma on 2-core and 2-quotient of partitions3 3. Schur-Weyl theory and Frobenius character formula5 4. A theorem of Littlewood9 5. The theorem 14 6. A correspondence between representations of S2n and S2n+1 15 References 17 Appendix A. Proof of Proposition 4.2 by Arvind Ayyer 18 1. INTRODUCTION Let G be either the symmetric group S2n or the symmetric group S2n+1, and H the n hyperoctahedral group Bn = (Z=2) o Sn, sitting naturally inside G (Bn ⊂ S2n ⊂ S2n+1) as the centralizer of a fixed point free involution w0 in S2n. In this paper, we take the symmetric group S2n as acting on the set {±1; ±2; ··· ; ±ng of cardinality 2n, and the symmetric group S2n+1 as acting on the set f0; ±1; ±2; ··· ; ±ng of cardinality 2n + 1. We fix w0 = (1; −1)(2; −2) ··· (n; −n). The paper proves a character relationship be- tween the irreducible representations of the groups G and Bn, closely related to character identities available between (finite dimensional, irreducible, algebraic) representations of the groups GL2n(C), or GL2n+1(C) which are self-dual, i.e., invariant under the invo- lution g ! tg−1, with (finite dimensional, irreducible, algebraic) representations of the groups SO2n+1(C), or Sp2n(C), for which we refer to [KLP].
    [Show full text]
  • THE HYPEROCTAHEDRAL QUANTUM GROUP Introduction
    THE HYPEROCTAHEDRAL QUANTUM GROUP TEODOR BANICA, JULIEN BICHON, AND BENOˆIT COLLINS n Abstract. We consider the hypercube in R , and show that its quantum symmetry group is a q-deformation of On at q = −1. Then we consider the graph formed by n segments, and show that its quantum symmetry group is free in some natural sense. + + + + This latter quantum group, denoted Hn , enlarges Wang’s series Sn ,On ,Un . Introduction The idea of noncommuting coordinates goes back to Heisenberg. Several theories emerged from Heisenberg’s work, most complete being Connes’ noncommutative geom- etry, where the base space is a Riemannian manifold. See [19]. A natural question is about studying algebras of free coordinates on algebraic groups. Given a group G ⊂ Un, the matrix coordinates uij ∈ C(G) commute with each other, and satisfy certain relations R. One can define then the universal algebra generated by abstract variables uij, subject to the relations R. The spectrum of this algebra is an abstract object, called noncommutative version of G. The noncommutative version is not unique, because it depends on R. We have the following examples: (1) Free quantum semigroups. The algebra generated by variables uij with relations making u = (uij) a unitary matrix was considered by Brown [14]. This algebra has a comultiplication and a counit, but no antipode. In other words, the nc corresponding noncommutative version Un is a quantum semigroup. (2) Quantum groups. A remarkable discovery is that for a compact Lie group G, once commutativity is included into the relations R, one can introduce a complex parameter q, as to get deformed relations Rq.
    [Show full text]