Finite Subgroups of SL(2,CC)
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
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. -
Arxiv:1702.00823V1 [Stat.OT] 2 Feb 2017
Nonparametric Spherical Regression Using Diffeomorphic Mappings M. Rosenthala, W. Wub, E. Klassen,c, Anuj Srivastavab aNaval Surface Warfare Center, Panama City Division - X23, 110 Vernon Avenue, Panama City, FL 32407-7001 bDepartment of Statistics, Florida State University, Tallahassee, FL 32306 cDepartment of Mathematics, Florida State University, Tallahassee, FL 32306 Abstract Spherical regression explores relationships between variables on spherical domains. We develop a nonparametric model that uses a diffeomorphic map from a sphere to itself. The restriction of this mapping to diffeomorphisms is natural in several settings. The model is estimated in a penalized maximum-likelihood framework using gradient-based optimization. Towards that goal, we specify a first-order roughness penalty using the Jacobian of diffeomorphisms. We compare the prediction performance of the proposed model with state-of-the-art methods using simulated and real data involving cloud deformations, wind directions, and vector-cardiograms. This model is found to outperform others in capturing relationships between spherical variables. Keywords: Nonlinear; Nonparametric; Riemannian Geometry; Spherical Regression. 1. Introduction Spherical data arises naturally in a variety of settings. For instance, a random vector with unit norm constraint is naturally studied as a point on a unit sphere. The statistical analysis of such random variables was pioneered by Mardia and colleagues (1972; 2000), in the context of directional data. Common application areas where such data originates include geology, gaming, meteorology, computer vision, and bioinformatics. Examples from geographical domains include plate tectonics (McKenzie, 1957; Chang, 1986), animal migrations, and tracking of weather for- mations. As mobile devices become increasingly advanced and prevalent, an abundance of new spherical data is being collected in the form of geographical coordinates. -
Limits of Geometries
Limits of Geometries Daryl Cooper, Jeffrey Danciger, and Anna Wienhard August 31, 2018 Abstract A geometric transition is a continuous path of geometric structures that changes type, mean- ing that the model geometry, i.e. the homogeneous space on which the structures are modeled, abruptly changes. In order to rigorously study transitions, one must define a notion of geometric limit at the level of homogeneous spaces, describing the basic process by which one homogeneous geometry may transform into another. We develop a general framework to describe transitions in the context that both geometries involved are represented as sub-geometries of a larger ambi- ent geometry. Specializing to the setting of real projective geometry, we classify the geometric limits of any sub-geometry whose structure group is a symmetric subgroup of the projective general linear group. As an application, we classify all limits of three-dimensional hyperbolic geometry inside of projective geometry, finding Euclidean, Nil, and Sol geometry among the 2 limits. We prove, however, that the other Thurston geometries, in particular H × R and SL^2 R, do not embed in any limit of hyperbolic geometry in this sense. 1 Introduction Following Felix Klein's Erlangen Program, a geometry is given by a pair (Y; H) of a Lie group H acting transitively by diffeomorphisms on a manifold Y . Given a manifold of the same dimension as Y , a geometric structure modeled on (Y; H) is a system of local coordinates in Y with transition maps in H. The study of deformation spaces of geometric structures on manifolds is a very rich mathematical subject, with a long history going back to Klein and Ehresmann, and more recently Thurston. -
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. -
Generating Sequences of PSL(2,P) Which Will Eventually Lead Us to Study How This Group Behaves with Respect to the Replacement Property
Generating Sequences of PSL(2,p) Benjamin Nachmana aCornell University, 310 Malott Hall, Ithaca, NY 14853 USA Abstract Julius Whiston and Jan Saxl [14] showed that the size of an irredundant generating set of the group G = PSL(2,p) is at most four and computed the size m(G) of a maximal set for many primes. We will extend this result to a larger class of primes, with a surprising result that when p 1 mod 10, m(G) = 3 except for the special case p = 7. In addition, we6≡ will ± determine which orders of elements in irredundant generating sets of PSL(2,p) with lengths less than or equal to four are possible in most cases. We also give some remarks about the behavior of PSL(2,p) with respect to the replacement property for groups. Keywords: generating sequences, general position, projective linear group 1. Introduction The two dimensional projective linear group over a finite field with p ele- ments, PSL(2,p) has been extensively studied since Galois, who constructed them and showed their simplicity for p > 3 [15]. One of their nice prop- erties is due to a theorem by E. Dickson, which shows that there are only a small number of possibilities for the isomorphism types of maximal sub- arXiv:1210.2073v2 [math.GR] 4 Aug 2014 groups. There are two possibilities: ones that exist for all p and ones that exist for exceptional primes. A more recent proof of Dickson’s Theorem can be found in [10] and a complete proof due to Dickson is in [3]. -
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. -
2-Arcs of Maximal Size in the Affine and the Projective Hjelmslev Plane Over Z25
Advances in Mathematics of Communications doi:10.3934/amc.2011.5.287 Volume 5, No. 2, 2011, 287{301 2-ARCS OF MAXIMAL SIZE IN THE AFFINE AND THE PROJECTIVE HJELMSLEV PLANE OVER Z25 Michael Kiermaier, Matthias Koch and Sascha Kurz Institut f¨urMathematik Universit¨atBayreuth D-95440 Bayreuth, Germany (Communicated by Veerle Fack) Abstract. It is shown that the maximal size of a 2-arc in the projective Hjelmslev plane over Z25 is 21, and the (21; 2)-arc is unique up to isomorphism. Furthermore, all maximal (20; 2)-arcs in the affine Hjelmslev plane over Z25 are classified up to isomorphism. 1. Introduction It is well known that a Desarguesian projective plane of order q admits a 2-arc of size q + 2 if and only if q is even. These 2-arcs are called hyperovals. The biggest 2-arcs in the Desarguesian projective planes of odd order q have size q + 1 and are called ovals. For a projective Hjelmslev plane over a chain ring R of composition length 2 and size q2, the situation is somewhat similar: In PHG(2;R) there exists a hyperoval { that is a 2-arc of size q2 + q + 1 { if and only if R is a Galois ring of size q2 with q even, see [7,6]. For the case q odd and R not a Galois ring it was recently shown 2 that the maximum size m2(R) of a 2-arc is q , see [4]. In the remaining cases, the situation is less clear. For even q and R not a Galois ring, it is known that the maximum possible size of a 2-arc is lower bounded by q2 + 2 [4] and upper bounded by q2 + q [6]. -
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.