Representation Theory and the Mckay Correspondence
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The Classification and the Conjugacy Classesof the Finite Subgroups of The
Algebraic & Geometric Topology 8 (2008) 757–785 757 The classification and the conjugacy classes of the finite subgroups of the sphere braid groups DACIBERG LGONÇALVES JOHN GUASCHI Let n 3. We classify the finite groups which are realised as subgroups of the sphere 2 braid group Bn.S /. Such groups must be of cohomological period 2 or 4. Depend- ing on the value of n, we show that the following are the maximal finite subgroups of 2 Bn.S /: Z2.n 1/ ; the dicyclic groups of order 4n and 4.n 2/; the binary tetrahedral group T ; the binary octahedral group O ; and the binary icosahedral group I . We give geometric as well as some explicit algebraic constructions of these groups in 2 Bn.S / and determine the number of conjugacy classes of such finite subgroups. We 2 also reprove Murasugi’s classification of the torsion elements of Bn.S / and explain 2 how the finite subgroups of Bn.S / are related to this classification, as well as to the 2 lower central and derived series of Bn.S /. 20F36; 20F50, 20E45, 57M99 1 Introduction The braid groups Bn of the plane were introduced by E Artin in 1925[2;3]. Braid groups of surfaces were studied by Zariski[41]. They were later generalised by Fox to braid groups of arbitrary topological spaces via the following definition[16]. Let M be a compact, connected surface, and let n N . We denote the set of all ordered 2 n–tuples of distinct points of M , known as the n–th configuration space of M , by: Fn.M / .p1;:::; pn/ pi M and pi pj if i j : D f j 2 ¤ ¤ g Configuration spaces play an important roleˆ in several branches of mathematics and have been extensively studied; see Cohen and Gitler[9] and Fadell and Husseini[14], for example. -
A Symplectic Resolution for the Binary Tetrahedral Group
A SYMPLECTIC RESOLUTION FOR THE BINARY TETRAHEDRAL GROUP MANFRED LEHN & CHRISTOPH SORGER Abstract. We describe an explicit symplectic resolution for the quo- tient singularity arising from the four-dimensional symplectic represen- ation of the binary tetrahedral group. Let G be a nite group with a complex symplectic representation V . The symplectic form σ on V descends to a symplectic form σ¯ on the open regular part of V=G. A proper morphism f : Y ! V=G is a symplectic resolution if Y is smooth and if f ∗σ¯ extends to a symplectic form on Y . It turns out that symplectic resolutions of quotient singularities are a rare phenomenon. By a theorem of Verbitsky [9], a necessary condition for the existence of a symplectic resolution is that G be generated by symplectic reections, i.e. by elements whose x locus on V is a linear subspace of codimension 2. Given an arbitrary complex representation V0 of a nite group G, we obtain a symplectic representation on ∗, where ∗ denotes the contragradient V0 ⊕V0 V0 representation of V0. In this case, Verbitsky's theorem specialises to an earlier theorem of Kaledin [7]: For ∗ to admit a symplectic resolution, the V0 ⊕ V0 =G action of G on V0 should be generated by complex reections, in other words, V0=G should be smooth. The complex reection groups have been classied by Shephard and Todd [8], the symplectic reection groups by Cohen [2]. The list of Shephard and Todd contains as a sublist the nite Coxeter groups. The question which of these groups G ⊂ Sp(V ) admits a symplectic res- olution for V=G has been solved for the Coxeter groups by Ginzburg and Kaledin [3] and for arbitrary complex reection groups most recently by Bellamy [1]. -
Maximal Subgroups of the Coxeter Group W(H4) and Quaternions
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Linear Algebra and its Applications 412 (2006) 441–452 www.elsevier.com/locate/laa Maximal subgroups of the Coxeter group W(H4) and quaternions Mehmet Koca a, Ramazan Koç b,∗, Muataz Al-Barwani a, Shadia Al-Farsi a aDepartment of Physics, College of Science, Sultan Qaboos University, P.O. Box 36, Al-Khod 123, Muscat, Oman bDepartment of Physics, Faculty of Engineering, Gaziantep University, 27310 Gaziantep, Turkey Received 9 October 2004; accepted 17 July 2005 Available online 12 September 2005 Submitted by H. Schneider Abstract The largest finite subgroup of O(4) is the non-crystallographic Coxeter group W(H4) of order 14,400. Its derived subgroup is the largest finite subgroup W(H4)/Z2 of SO(4) of order 7200. Moreover, up to conjugacy, it has five non-normal maximal subgroups of orders 144, two 240, 400 and 576. Two groups [W(H2) × W(H2)]Z4 and W(H3) × Z2 possess non- crystallographic structures with orders 400 and 240 respectively. The groups of orders 144, 240 and 576 are the extensions of the Weyl groups of the root systems of SU(3) × SU(3), SU(5) and SO(8) respectively. We represent the maximal subgroups of W(H4) with sets of quaternion pairs acting on the quaternionic root systems. © 2005 Elsevier Inc. All rights reserved. AMS classification: 20G20; 20F05; 20E34 Keywords: Structure of groups; Quaternions; Coxeter groups; Subgroup structure ∗ Corresponding author. Tel.: +90 342 360 1200; fax: +90 342 360 1013. -
Platonic Solids Generate Their Four-Dimensional Analogues.', Acta Crystallographica Section A., 69 (6)
Durham Research Online Deposited in DRO: 26 January 2014 Version of attached le: Published Version Peer-review status of attached le: Peer-reviewed Citation for published item: Dechant, Pierre-Philippe (2013) 'Platonic solids generate their four-dimensional analogues.', Acta crystallographica section A., 69 (6). pp. 592-602. Further information on publisher's website: http://dx.doi.org/10.1107/S0108767313021442 Publisher's copyright statement: Additional information: Published on behalf of the International Union of Crystallography. Use policy The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that: • a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders. Please consult the full DRO policy for further details. Durham University Library, Stockton Road, Durham DH1 3LY, United Kingdom Tel : +44 (0)191 334 3042 | Fax : +44 (0)191 334 2971 https://dro.dur.ac.uk electronic reprint Acta Crystallographica Section A Foundations of Crystallography ISSN 0108-7673 Platonic solids generate their four-dimensional analogues Pierre-Philippe Dechant Acta Cryst. (2013). A69, 592–602 Copyright c International Union of Crystallography Author(s) of this paper may load this reprint on their own web site or institutional repository provided that this cover page is retained. Republication of this article or its storage in electronic databases other than as specified above is not permitted without prior permission in writing from the IUCr. -
Platonic Solids Generate Their Four-Dimensional Analogues
This is a repository copy of Platonic solids generate their four-dimensional analogues. White Rose Research Online URL for this paper: https://eprints.whiterose.ac.uk/85590/ Version: Accepted Version Article: Dechant, Pierre-Philippe orcid.org/0000-0002-4694-4010 (2013) Platonic solids generate their four-dimensional analogues. Acta Crystallographica Section A : Foundations of Crystallography. pp. 592-602. ISSN 1600-5724 https://doi.org/10.1107/S0108767313021442 Reuse Items deposited in White Rose Research Online are protected by copyright, with all rights reserved unless indicated otherwise. They may be downloaded and/or printed for private study, or other acts as permitted by national copyright laws. The publisher or other rights holders may allow further reproduction and re-use of the full text version. This is indicated by the licence information on the White Rose Research Online record for the item. Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request. [email protected] https://eprints.whiterose.ac.uk/ 1 Platonic solids generate their four-dimensional analogues PIERRE-PHILIPPE DECHANT a,b,c* aInstitute for Particle Physics Phenomenology, Ogden Centre for Fundamental Physics, Department of Physics, University of Durham, South Road, Durham, DH1 3LE, United Kingdom, bPhysics Department, Arizona State University, Tempe, AZ 85287-1604, United States, and cMathematics Department, University of York, Heslington, York, YO10 5GG, United Kingdom. E-mail: [email protected] Polytopes; Platonic Solids; 4-dimensional geometry; Clifford algebras; Spinors; Coxeter groups; Root systems; Quaternions; Representations; Symmetries; Trinities; McKay correspondence Abstract In this paper, we show how regular convex 4-polytopes – the analogues of the Platonic solids in four dimensions – can be constructed from three-dimensional considerations concerning the Platonic solids alone. -
Remarks on the Cohomology of Finite Fundamental Groups of 3–Manifolds
Geometry & Topology Monographs 14 (2008) 519–556 519 arXiv version: fonts, pagination and layout may vary from GTM published version Remarks on the cohomology of finite fundamental groups of 3–manifolds SATOSHI TOMODA PETER ZVENGROWSKI Computations based on explicit 4–periodic resolutions are given for the cohomology of the finite groups G known to act freely on S3 , as well as the cohomology rings of the associated 3–manifolds (spherical space forms) M = S3=G. Chain approximations to the diagonal are constructed, and explicit contracting homotopies also constructed for the cases G is a generalized quaternion group, the binary tetrahedral group, or the binary octahedral group. Some applications are briefly discussed. 57M05, 57M60; 20J06 1 Introduction The structure of the cohomology rings of 3–manifolds is an area to which Heiner Zieschang devoted much work and energy, especially from 1993 onwards. This could be considered as part of a larger area of his interest, the degrees of maps between oriented 3– manifolds, especially the existence of degree one maps, which in turn have applications in unexpected areas such as relativity theory (cf Shastri, Williams and Zvengrowski [41] and Shastri and Zvengrowski [42]). References [1,6,7, 18, 19, 20, 21, 22, 23] in this paper, all involving work of Zieschang, his students Aaslepp, Drawe, Sczesny, and various colleagues, attest to his enthusiasm for these topics and the remarkable energy he expended studying them. Much of this work involved Seifert manifolds, in particular, references [1, 6, 7, 18, 20, 23]. Of these, [6, 7, 23] (together with [8, 9]) successfully completed the programme of computing the ring structure H∗(M) for any orientable Seifert manifold M with 1 2 3 3 G := π1(M) infinite. -
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. -
Half-Bps M2-Brane Orbifolds 3
HALF-BPS M2-BRANE ORBIFOLDS PAUL DE MEDEIROS AND JOSÉ FIGUEROA-O’FARRILL Abstract. Smooth Freund–Rubin backgrounds of eleven-dimensional supergravity of the form AdS X7 and preserving at least half of the supersymmetry have been recently clas- 4 × sified. Requiring that amount of supersymmetry forces X to be a spherical space form, whence isometric to the quotient of the round 7-sphere by a freely-acting finite subgroup of SO(8). The classification is given in terms of ADE subgroups of the quaternions embed- dedin SO(8) as the graph of an automorphism. In this paper we extend this classification by dropping the requirement that the background be smooth, so that X is now allowed to be an orbifold of the round 7-sphere. We find that if the background preserves more than half of the supersymmetry, then it is automatically smooth in accordance with the homo- geneity conjecture, but that there are many half-BPS orbifolds, most of them new. The classification is now given in terms of pairs of ADE subgroups of quaternions fibred over the same finite group. We classify such subgroups and then describe the resulting orbi- folds in terms of iterated quotients. In most cases the resulting orbifold can be described as a sequence of cyclic quotients. Contents List of Tables 2 1. Introduction 3 How to use this paper 5 2. Spherical orbifolds 7 2.1. Spin orbifolds 8 2.2. Statement of the problem 9 3. Finite subgroups of the quaternions 10 4. Goursat’s Lemma 12 arXiv:1007.4761v3 [hep-th] 25 Aug 2010 4.1. -
Convex Polytopes and Tilings with Few Flag Orbits
Convex Polytopes and Tilings with Few Flag Orbits by Nicholas Matteo B.A. in Mathematics, Miami University M.A. in Mathematics, Miami University A dissertation submitted to The Faculty of the College of Science of Northeastern University in partial fulfillment of the requirements for the degree of Doctor of Philosophy April 14, 2015 Dissertation directed by Egon Schulte Professor of Mathematics Abstract of Dissertation The amount of symmetry possessed by a convex polytope, or a tiling by convex polytopes, is reflected by the number of orbits of its flags under the action of the Euclidean isometries preserving the polytope. The convex polytopes with only one flag orbit have been classified since the work of Schläfli in the 19th century. In this dissertation, convex polytopes with up to three flag orbits are classified. Two-orbit convex polytopes exist only in two or three dimensions, and the only ones whose combinatorial automorphism group is also two-orbit are the cuboctahedron, the icosidodecahedron, the rhombic dodecahedron, and the rhombic triacontahedron. Two-orbit face-to-face tilings by convex polytopes exist on E1, E2, and E3; the only ones which are also combinatorially two-orbit are the trihexagonal plane tiling, the rhombille plane tiling, the tetrahedral-octahedral honeycomb, and the rhombic dodecahedral honeycomb. Moreover, any combinatorially two-orbit convex polytope or tiling is isomorphic to one on the above list. Three-orbit convex polytopes exist in two through eight dimensions. There are infinitely many in three dimensions, including prisms over regular polygons, truncated Platonic solids, and their dual bipyramids and Kleetopes. There are infinitely many in four dimensions, comprising the rectified regular 4-polytopes, the p; p-duoprisms, the bitruncated 4-simplex, the bitruncated 24-cell, and their duals. -
2011 Volume 4
2011 Volume 4 The Journal on Advanced Studies in Theoretical and Experimental Physics, including Related Themes from Mathematics PROGRESS IN PHYSICS “All scientists shall have the right to present their scientific research results, in whole or in part, at relevant scientific conferences, and to publish the same in printed scientific journals, electronic archives, and any other media.” — Declaration of Academic Freedom, Article 8 ISSN 1555-5534 The Journal on Advanced Studies in Theoretical and Experimental Physics, including Related Themes from Mathematics PROGRESS IN PHYSICS A quarterly issue scientific journal, registered with the Library of Congress (DC, USA). This journal is peer reviewed and included in the abs- tracting and indexing coverage of: Mathematical Reviews and MathSciNet (AMS, USA), DOAJ of Lund University (Sweden), Zentralblatt MATH (Germany), Scientific Commons of the University of St. Gallen (Switzerland), Open-J-Gate (India), Referativnyi Zhurnal VINITI (Russia), etc. Electronic version of this journal: October 2011 VOLUME 4 http://www.ptep-online.com CONTENTS Editorial Board Dmitri Rabounski, Editor-in-Chief [email protected] Minasyan V. and Samoilov V. Ultracold Fermi and Bose gases and Spinless Bose Florentin Smarandache, Assoc. Editor ChargedSoundParticles.......................................................3 [email protected] Minasyan V. and Samoilov V. Superfluidity Component of Solid 4He and Sound Par- Larissa Borissova, Assoc. Editor ticleswithSpin1.............................................................8 [email protected] Quznetsov G. Fermion-Antifermion Asymmetry . 13 Editorial Team Tank H. K. An Insight into Planck’s Units: Explaining the Experimental-Observa- Gunn Quznetsov tions of Lack of Quantum Structure of Space-Time . 17 [email protected] Ries A. and Fook M.V.L. Excited Electronic States of Atoms described by the Model Andreas Ries [email protected] ofOscillationsinaChainSystem..............................................20 Chifu Ebenezer Ndikilar Ogiba F. -
4D Pyritohedral Symmetry
SQU Journal for Science, 2016, 21(2), 150-161 © 2016 Sultan Qaboos University 4D Pyritohedral Symmetry Nazife O. Koca*, Amal J.H. Al Qanobi and Mehmet Koca Department of Physics, College of Science, Sultan Qaboos University, P.O. Box 36, Al-Khoud 123, Muscat, Sultanate of Oman,* Email: [email protected]. ABSTRACT: We describe an extension of the pyritohedral symmetry in 3D to 4-dimensional Euclidean space and construct the group elements of the 4D pyritohedral group of order 576 in terms of quaternions. It turns out that it is a maximal subgroup of both the rank-4 Coxeter groups W (F4) and W (H4), implying that it is a group relevant to the crystallographic as well as quasicrystallographic structures in 4-dimensions. We derive the vertices of the 24 pseudoicosahedra, 24 tetrahedra and the 96 triangular pyramids forming the facets of the pseudo snub 24- cell. It turns out that the relevant lattice is the root lattice of W (D4). The vertices of the dual polytope of the pseudo snub 24-cell consists of the union of three sets: 24-cell, another 24-cell and a new pseudo snub 24-cell. We also derive a new representation for the symmetry group of the pseudo snub 24-cell and the corresponding vertices of the polytopes. Keywords: Pseudoicosahedron; Pyritohedron; Lattice; Coxeter groups and Quaternions. تماثل متعدد اﻷوجه ذو التركيب المشابه لمعدن البايريت في الفضاء اﻻقليدي ذو اﻷبعاد اﻷربعة نظيفة كوجا، أمل القنوبي و محمد كوجا مستخلص: وصفنا امتدادا لتماثل تركيب متعددات اﻷوجه من النوع المشابه لبلورة معدن البايرايت )pyritohedral( - و الذي يمكن صياغته -
From the Icosahedron to E8
From the Icosahedron to E8 John C. Baez Department of Mathematics University of California Riverside, California 92521, USA and Centre for Quantum Technologies National University of Singapore Singapore 117543 [email protected] December 22, 2017 Abstract The regular icosahedron is connected to many exceptional objects in mathematics. Here we describe two constructions of the E8 lattice from the icosahedron. One uses a subring of the quaternions called the \icosians", while the other uses du Val's work on the resolution of Kleinian singularities. Together they link the golden ratio, the quaternions, the quintic equation, the 600- cell, and the Poincar´ehomology 3-sphere. We leave it as a challenge to the reader to find the connection between these two constructions. In mathematics, every sufficiently beautiful object is connected to all others. Many exciting adven- tures, of various levels of difficulty, can be had by following these connections. Take, for example, the icosahedron|that is, the regular icosahedron, one of the five Platonic solids. Starting from this it is just a hop, skip and a jump to the E8 lattice, a wonderful pattern of points in 8 dimensions! As we explore this connection we shall see that it also ties together many other remarkable entities: the golden ratio, the quaternions, the quintic equation, a highly symmetrical 4-dimensional shape called the 600-cell, and a manifold called the Poincar´ehomology 3-sphere. Indeed, the main problem with these adventures is knowing where to stop. The story we shall tell is just a snippet of a longer one involving the McKay correspondence and quiver representations.