ON COMPLEX REFLECTION GROUPS G(M,1,R)
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On Schur Algebras, Doty Coalgebras and Quasi-Hereditary Algebras
CORE Metadata, citation and similar papers at core.ac.uk Provided by White Rose E-theses Online ON SCHUR ALGEBRAS, DOTY COALGEBRAS AND QUASI-HEREDITARY ALGEBRAS Rachel Ann Heaton University of York Department of Mathematics Thesis submitted to the University of York for the degree of Doctor of Philosophy December 2009 1 Abstract Motivated by Doty's Conjecture we study the coalgebras formed from the coefficient spaces of the truncated modules Tr λE. We call these the Doty Coalgebras Dn;p(r). We prove that Dn;p(r) = A(n; r) for n = 2, and also that Dn;p(r) = A(π; r) with π a suitable saturated set, for the cases; i) n = 3, 0 ≤ r ≤ 3p − 1, 6p − 8 ≤ r ≤ n2(p − 1) for all p; ii) p = 2 for all n and all r; iii) 0 ≤ r ≤ p − 1 and nt − (p − 1) ≤ r ≤ nt for all n and all p; iv) n = 4 and p = 3 for all r. The Schur Algebra S(n; r) is the dual of the coalgebra A(n; r), and S(n; r) we know to be quasi-hereditary. Moreover, we call a finite dimensional coal- gebra quasi-hereditary if its dual algebra is quasi-hereditary and hence, in the above cases, the Doty Coalgebras Dn;p(r) are also quasi-hereditary and thus have finite global dimension. We conjecture that there is no saturated set π such that D3;p(r) = A(π; r) for the cases not covered above, giving our reasons for this conjecture. Stepping away from our main focus on Doty Coalgebras, we also describe an infinite family of quiver algebras which have finite global dimension but are not quasi-hereditary. -
3.4 Finite Reflection Groups In
Chapter 3 Equations of order 2 This chapter is mostly devoted to Fuchsian equations L(y)=0oforder2.For these equations we shall describe all finite monodromy groups that are possible. In particular we discuss the projective monodromy groups of dimension 2. Most of the theory we give is based on the work of Felix Klein and of G.C. Shephard and J.A. Todd. Unless stated otherwise we let L(y)=0beaFuchsiandifferential equation order 2, with differentiation with respect to the variable z. 3.1 Finite subgroups of PGL(2, C) Any Fuchsian differential equation with a basis of algebraic solutions has a finite monodromy group, (and vice versa, see Theorem 2.1.8). In particular this is the case for second order Fuchsian equations, to which we restrict ourselves for now. The monodromy group for such an equation is contained in GL(2, C). Any subgroup G ⊂ GL(2, C) acts on the Riemann sphere P1. More specifically, a matrix γ ∈ GL(2, C)with ab γ := cd has an action on C defined as at + b γ ∗ t := . (3.1) ct + d for all appropriate t ∈ C. The action is extended to P1 by γ ∗∞ = a/c in the case of ac =0and γ ∗ (−d/c)=∞ when c is non-zero. The action of G on P1 factors through to the projective group PG ⊂ PGL(2, C). In other words we have the well-defined action PG : P1 → P1 γ · ΛI2 : t → γ ∗ t. 39 40 Chapter 3. Equations of order 2 PG name |PG| Cm Cyclic group m Dm Dihedral group 2m A4 Tetrahedral group 12 (Alternating group on 4 elements) S4 Octahedral group 24 (Symmetric group on 4 elements) A5 Icosahedral group 60 (Alternating group on 5 elements) Table 3.1: The finite subgroups of PGL(2, C). -
Regular Elements of Finite Reflection Groups
Inventiones math. 25, 159-198 (1974) by Springer-Veriag 1974 Regular Elements of Finite Reflection Groups T.A. Springer (Utrecht) Introduction If G is a finite reflection group in a finite dimensional vector space V then ve V is called regular if no nonidentity element of G fixes v. An element ge G is regular if it has a regular eigenvector (a familiar example of such an element is a Coxeter element in a Weyl group). The main theme of this paper is the study of the properties and applications of the regular elements. A review of the contents follows. In w 1 we recall some known facts about the invariant theory of finite linear groups. Then we discuss in w2 some, more or less familiar, facts about finite reflection groups and their invariant theory. w3 deals with the problem of finding the eigenvalues of the elements of a given finite linear group G. It turns out that the explicit knowledge of the algebra R of invariants of G implies a solution to this problem. If G is a reflection group, R has a very simple structure, which enables one to obtain precise results about the eigenvalues and their multiplicities (see 3.4). These results are established by using some standard facts from algebraic geometry. They can also be used to give a proof of the formula for the order of finite Chevalley groups. We shall not go into this here. In the case of eigenvalues of regular elements one can go further, this is discussed in w4. One obtains, for example, a formula for the order of the centralizer of a regular element (see 4.2) and a formula for the eigenvalues of a regular element in an irreducible representation (see 4.5). -
The Partition Algebras and a New Deformation of the Schur Algebras
JOURNAL OF ALGEBRA 203, 91]124Ž. 1998 ARTICLE NO. JA977164 The Partition Algebras and a New Deformation of the Schur Algebras P. MartinU Department of Mathematics, City Uni¨ersity, Northampton Square, London, EC1V 0H8, View metadata, citation and similar papers at core.ac.ukUnited Kingdom brought to you by CORE provided by Elsevier - Publisher Connector and D. Woodcock² School of Mathematical Sciences, Queen Mary and Westfield College, Mile End Road, London, E1 4NS, United Kingdom Communicated by Gordon James Received August 30, 1996 THIS PAPER IS DEDICATED TO THE MEMORY OF AHMED ELGAMAL P Ž. Z The partition algebras PZw¨ x n are algebras defined over the ring wx¨ of integral polynomials. They are of current interest because of their role in the transfer matrix formulation of colouring problems and Q-state Potts models in statistical mechanicswx 11 . Let k be a Zwx¨ -algebra which is a P Ž.P Ž. field, and let Pk n be the algebra obtained from PZw¨ x n by base change to k, a finite dimensional k-algebra. If char k s 0 the representation theory of PkŽ.n is generically semisimple, and the exceptional cases are completely understoodwxwx 11, 12, 14 . In 15 we showed that if char k ) 0 and the image of ¨ does not lie in the prime subfield of k, PkŽ.n is Morita equivalent to kS 0 = ??? = kS n, a product of group algebras of symmetric groups. In the present paper we show that in the remaining cases in positive characteristic the representation theory of PkŽ.n can be obtained by localisation from that of a suitably chosen classical Schur algebraŽ. -
Combinatorial Complexes, Bruhat Intervals and Reflection Distances
Combinatorial complexes, Bruhat intervals and reflection distances Axel Hultman Stockholm 2003 Doctoral Dissertation Royal Institute of Technology Department of Mathematics Akademisk avhandling som med tillst˚andav Kungl Tekniska H¨ogskolan framl¨ag- ges till offentlig granskning f¨oravl¨aggandeav teknisk doktorsexamen tisdagen den 21 oktober 2003 kl 15.15 i sal E2, Huvudbyggnaden, Kungl Tekniska H¨ogskolan, Lindstedtsv¨agen3, Stockholm. ISBN 91-7283-591-5 TRITA-MAT-03-MA-16 ISSN 1401-2278 ISRN KTH/MAT/DA--03/07--SE °c Axel Hultman, September 2003 Universitetsservice US AB, Stockholm 2003 Abstract The various results presented in this thesis are naturally subdivided into three differ- ent topics, namely combinatorial complexes, Bruhat intervals and expected reflection distances. Each topic is made up of one or several of the altogether six papers that constitute the thesis. The following are some of our results, listed by topic: Combinatorial complexes: ² Using a shellability argument, we compute the cohomology groups of the com- plements of polygraph arrangements. These are the subspace arrangements that were exploited by Mark Haiman in his proof of the n! theorem. We also extend these results to Dowling generalizations of polygraph arrangements. ² We consider certain B- and D-analogues of the quotient complex ∆(Πn)=Sn, i.e. the order complex of the partition lattice modulo the symmetric group, and some related complexes. Applying discrete Morse theory and an improved version of known lexicographic shellability techniques, we determine their homotopy types. ² Given a directed graph G, we study the complex of acyclic subgraphs of G as well as the complex of not strongly connected subgraphs of G. -
Finite Complex Reflection Arrangements Are K(Π,1)
Annals of Mathematics 181 (2015), 809{904 http://dx.doi.org/10.4007/annals.2015.181.3.1 Finite complex reflection arrangements are K(π; 1) By David Bessis Abstract Let V be a finite dimensional complex vector space and W ⊆ GL(V ) be a finite complex reflection group. Let V reg be the complement in V of the reflecting hyperplanes. We prove that V reg is a K(π; 1) space. This was predicted by a classical conjecture, originally stated by Brieskorn for complexified real reflection groups. The complexified real case follows from a theorem of Deligne and, after contributions by Nakamura and Orlik- Solomon, only six exceptional cases remained open. In addition to solving these six cases, our approach is applicable to most previously known cases, including complexified real groups for which we obtain a new proof, based on new geometric objects. We also address a number of questions about reg π1(W nV ), the braid group of W . This includes a description of periodic elements in terms of a braid analog of Springer's theory of regular elements. Contents Notation 810 Introduction 810 1. Complex reflection groups, discriminants, braid groups 816 2. Well-generated complex reflection groups 820 3. Symmetric groups, configurations spaces and classical braid groups 823 4. The affine Van Kampen method 826 5. Lyashko-Looijenga coverings 828 6. Tunnels, labels and the Hurwitz rule 831 7. Reduced decompositions of Coxeter elements 838 8. The dual braid monoid 848 9. Chains of simple elements 853 10. The universal cover of W nV reg 858 11. -
Clifford Group Dipoles and the Enactment of Weyl/Coxeter Group W(E8) by Entangling Gates Michel Planat
Clifford group dipoles and the enactment of Weyl/Coxeter group W(E8) by entangling gates Michel Planat To cite this version: Michel Planat. Clifford group dipoles and the enactment of Weyl/Coxeter group W(E8) by entangling gates. 2009. hal-00378095v2 HAL Id: hal-00378095 https://hal.archives-ouvertes.fr/hal-00378095v2 Preprint submitted on 5 May 2009 (v2), last revised 29 Sep 2009 (v4) HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Clifford group dipoles and the enactment of Weyl/Coxeter group W (E8) by entangling gates Michel Planat Institut FEMTO-ST, CNRS, 32 Avenue de l’Observatoire, F-25044 Besan¸con, France ([email protected]) Abstract. Peres/Mermin arguments about no-hidden variables in quantum mechanics are used for displaying a pair (R,S) of entangling Clifford quantum gates, acting on two qubits. From them, a natural unitary representation of Coxeter/Weyl groups W (D5) and W (F4) emerges, which is also reflected into the splitting of the n-qubit Clifford group ± + n into dipoles n . The union of the three-qubit real Clifford group and the Toffoli C C C3 gate ensures a unitary representation of the Weyl/Coxeter group W (E8), and of its relatives. -
Affine Symmetric Group Joel Brewster Lewis¹*
WikiJournal of Science, 2021, 4(1):3 doi: 10.15347/wjs/2021.003 Encyclopedic Review Article Affine symmetric group Joel Brewster Lewis¹* Abstract The affine symmetric group is a mathematical structure that describes the symmetries of the number line and the regular triangular tesselation of the plane, as well as related higher dimensional objects. It is an infinite extension of the symmetric group, which consists of all permutations (rearrangements) of a finite set. In addition to its geo- metric description, the affine symmetric group may be defined as the collection of permutations of the integers (..., −2, −1, 0, 1, 2, ...) that are periodic in a certain sense, or in purely algebraic terms as a group with certain gen- erators and relations. These different definitions allow for the extension of many important properties of the finite symmetric group to the infinite setting, and are studied as part of the fields of combinatorics and representation theory. Definitions Non-technical summary The affine symmetric group, 푆̃푛, may be equivalently Flat, straight-edged shapes (like triangles) or 3D ones defined as an abstract group by generators and rela- (like pyramids) have only a finite number of symme- tions, or in terms of concrete geometric and combina- tries. In contrast, the affine symmetric group is a way to torial models. mathematically describe all the symmetries possible when an infinitely large flat surface is covered by trian- gular tiles. As with many subjects in mathematics, it can Algebraic definition also be thought of in a number of ways: for example, it In terms of generators and relations, 푆̃푛 is generated also describes the symmetries of the infinitely long by a set number line, or the possible arrangements of all inte- gers (..., −2, −1, 0, 1, 2, ...) with certain repetitive pat- 푠 , 푠 , … , 푠 0 1 푛−1 terns. -
The $ Q $-Difference Noether Problem for Complex Reflection Groups And
THE q-DIFFERENCE NOETHER PROBLEM FOR COMPLEX REFLECTION GROUPS AND QUANTUM OGZ ALGEBRAS JONAS T. HARTWIG Abstract. For any complex reflection group G = G(m,p,n), we prove that the G- invariants of the division ring of fractions of the n:th tensor power of the quantum plane is a quantum Weyl field and give explicit parameters for this quantum Weyl field. This shows that the q-Difference Noether Problem has a positive solution for such groups, generalizing previous work by Futorny and the author [10]. Moreover, the new result is simultaneously a q-deformation of the classical commutative case, and of the Weyl algebra case recently obtained by Eshmatov et al. [8]. Secondly, we introduce a new family of algebras called quantum OGZ algebras. They are natural quantizations of the OGZ algebras introduced by Mazorchuk [18] originating in the classical Gelfand-Tsetlin formulas. Special cases of quantum OGZ algebras include the quantized enveloping algebra of gln and quantized Heisenberg algebras. We show that any quantum OGZ algebra can be naturally realized as a Galois ring in the sense of Futorny-Ovsienko [11], with symmetry group being a direct product of complex reflection groups G(m,p,rk). Finally, using these results we prove that the quantum OGZ algebras satisfy the quan- tum Gelfand-Kirillov conjecture by explicitly computing their division ring of fractions. Contents 1. Introduction and Summary of Main Results 2 1.1. The q-Difference Noether Problem 2 1.2. Quantum OGZ Algebras 3 1.3. The Quantum Gelfand-Kirillov Conjecture 4 2. The q-Difference Noether Problem for Complex Reflection Groups 4 3. -
THE HESSE PENCIL of PLANE CUBIC CURVES 1. Introduction In
THE HESSE PENCIL OF PLANE CUBIC CURVES MICHELA ARTEBANI AND IGOR DOLGACHEV Abstract. This is a survey of the classical geometry of the Hesse configuration of 12 lines in the projective plane related to inflection points of a plane cubic curve. We also study two K3surfaceswithPicardnumber20whicharise naturally in connection with the configuration. 1. Introduction In this paper we discuss some old and new results about the widely known Hesse configuration of 9 points and 12 lines in the projective plane P2(k): each point lies on 4 lines and each line contains 3 points, giving an abstract configuration (123, 94). Through most of the paper we will assume that k is the field of complex numbers C although the configuration can be defined over any field containing three cubic roots of unity. The Hesse configuration can be realized by the 9 inflection points of a nonsingular projective plane curve of degree 3. This discovery is attributed to Colin Maclaurin (1698-1746) (see [46], p. 384), however the configuration is named after Otto Hesse who was the first to study its properties in [24], [25]1. In particular, he proved that the nine inflection points of a plane cubic curve form one orbit with respect to the projective group of the plane and can be taken as common inflection points of a pencil of cubic curves generated by the curve and its Hessian curve. In appropriate projective coordinates the Hesse pencil is given by the equation (1) λ(x3 + y3 + z3)+µxyz =0. The pencil was classically known as the syzygetic pencil 2 of cubic curves (see [9], p. -
Presenting Affine Q-Schur Algebras
Mathematische Zeitschrift manuscript No. (will be inserted by the editor) S. R. Doty R. M. Green · Presenting affine q-Schur algebras Received: date / Revised: date Abstract We obtain a presentation of certain affine q-Schur algebras in terms of generators and relations. The presentation is obtained by adding more relations to the usual presentation of the quantized enveloping algebra of type affine gln. Our results extend and rely on the corresponding result for the q-Schur algebra of the symmetric group, which were proved by the first author and Giaquinto. Mathematics Subject Classification (2000) 17B37, 20F55 Introduction r Let V ′ be a vector space of finite dimension n. On the tensor space (V ′)⊗ we have natural commuting actions of the general linear group GL(V ′) and the symmetric group Sr. Schur observed that the centralizer algebra of each action equals the r image of the other action in End((V ′)⊗ ), in characteristic zero, and Schur and Weyl used this observation to transfer information about the representations of Sr to information about the representations of GL(V ′). That this Schur–Weyl dual- ity holds in arbitrary characteristic was first observed in [4], although a special case was already used in [2]. In recent years, there have appeared various applica- tions of the Schur–Weyl duality viewpoint to modular representations. The Schur algebras S(n,r) first defined in [9] play a fundamental role in such interactions. Jimbo [13] and (independently) Dipper and James [6] observed that the ten- r sor space (V ′)⊗ has a q-analogue in which the mutually centralizing actions of GL(V ′) and Sr become mutually centralizing actions of a quantized enveloping algebra U(gln) and of the Iwahori-Hecke algebra H (Sr) corresponding to Sr. -
Annales Scientifiques De L'é.Ns
ANNALES SCIENTIFIQUES DE L’É.N.S. ARJEH M. COHEN Finite complex reflection groups Annales scientifiques de l’É.N.S. 4e série, tome 9, no 3 (1976), p. 379-436. <http://www.numdam.org/item?id=ASENS_1976_4_9_3_379_0> © Gauthier-Villars (Éditions scientifiques et médicales Elsevier), 1976, tous droits réservés. L’accès aux archives de la revue « Annales scientifiques de l’É.N.S. » (http://www. elsevier.com/locate/ansens), implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/legal.php). Toute utilisation commerciale ou impression systéma- tique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. scient. EC. Norm. Sup., 46 serie t. 9, 1976, p. 379 a 436. FINITE COMPLEX REFLECTION GROUPS BY ARJEH M. COHEN Introduction In 1954 G. C. Shephard and J. A. Todd published a list of all finite irreducible complex reflection groups (up to conjugacy). In their classification they separately studied the imprimitive groups and the primitive groups. In the latter case they extensively used the classification of finite collineation groups containing homologies as worked out by G. Bagnera (1905), H. F. Blichfeldt (1905), and H. H. Mitchell (1914). Furthermore, Shephard and Todd determined the degrees of the reflection groups, using the invariant theory of the corresponding collineation groups in the primitive case. In 1967 H. S. M. Coxeter (cf, [6]) presented a number of graphs connected with complex reflection groups in an attempt to systematize the results of Shephard and Todd.