On Quadruply Transitive Groups Dissertation
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Generating the Mathieu Groups and Associated Steiner Systems
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Discrete Mathematics 112 (1993) 41-47 41 North-Holland Generating the Mathieu groups and associated Steiner systems Marston Conder Department of Mathematics and Statistics, University of Auckland, Private Bag 92019, Auckland, New Zealand Received 13 July 1989 Revised 3 May 1991 Abstract Conder, M., Generating the Mathieu groups and associated Steiner systems, Discrete Mathematics 112 (1993) 41-47. With the aid of two coset diagrams which are easy to remember, it is shown how pairs of generators may be obtained for each of the Mathieu groups M,,, MIz, Mz2, M,, and Mz4, and also how it is then possible to use these generators to construct blocks of the associated Steiner systems S(4,5,1 l), S(5,6,12), S(3,6,22), S(4,7,23) and S(5,8,24) respectively. 1. Introduction Suppose you land yourself in 24-dimensional space, and are faced with the problem of finding the best way to pack spheres in a box. As is well known, what you really need for this is the Leech Lattice, but alas: you forgot to bring along your Miracle Octad Generator. You need to construct the Leech Lattice from scratch. This may not be so easy! But all is not lost: if you can somehow remember how to define the Mathieu group Mz4, you might be able to produce the blocks of a Steiner system S(5,8,24), and the rest can follow. In this paper it is shown how two coset diagrams (which are easy to remember) can be used to obtain pairs of generators for all five of the Mathieu groups M,,, M12, M22> Mz3 and Mz4, and also how blocks may be constructed from these for each of the Steiner systems S(4,5,1 I), S(5,6,12), S(3,6,22), S(4,7,23) and S(5,8,24) respectively. -
MATHEMATISCH CENTRUM 2E BOERHAA VESTR.AA T 49 AMSTERDAM
STICHTING MATHEMATISCH CENTRUM 2e BOERHAA VESTR.AA T 49 AMSTERDAM zw 1957 - ~ 03 ,A Completeness of Holomor:phs W. Peremans 1957 KONJNKL. :'\lBDl~HL. AKADE:lllE \'A:'\l WETE:NI-ICHAl'PEN . A:\II-ITEKUA:\1 Heprintod from Procoeding,;, Serie,;.; A, 60, No. fi nnd fndag. Muth., 19, No. 5, Hl/57 MATHEMATICS COMPLE1'ENE:-:l:-:l OF HOLOMORPH8 BY W. l'l~RBMANS (Communicated by Prof. J. F. KOKSMA at tho meeting of May 25, 1957) l. lntroduct-ion. A complete group is a group without centre and without outer automorphisms. It is well-known that a group G is complete if and only if G is a direct factor of every group containing G as a normal subgroup (cf. [6], p. 80 and [2]). The question arises whether it is sufficient for a group to be complete, that it is a direct factor in its holomorph. REDEI [9] has given the following necessary condition for a group to be a direct factor in its holomorph: it is complete or a direct product of a complete group and a group of order 2. In section 2 I establish the following necessary and sufficient condition: it is complete or a direct product of a group of order 2 and a complete group without subgroups of index 2. Obviously a group of order 2 is a trivial exam1)le of a non-complete group which is a direct factor of its holomorph (trivial, because the group coincides with its holomorph). For non-trivial examples we need non trivial complete groups without subgroups of index 2. -
Group Theory
Group Theory Hartmut Laue Mathematisches Seminar der Universit¨at Kiel 2013 Preface These lecture notes present the contents of my course on Group Theory within the masters programme in Mathematics at the University of Kiel. The aim is to introduce into concepts and techniques of modern group theory which are the prerequisites for tackling current research problems. In an area which has been studied with extreme intensity for many decades, the decision of what to include or not under the time limits of a summer semester was certainly not trivial, and apart from the aspect of importance also that of personal taste had to play a role. Experts will soon discover that among the results proved in this course there are certain theorems which frequently are viewed as too difficult to reach, like Tate’s (4.10) or Roquette’s (5.13). The proofs given here need only a few lines thanks to an approach which seems to have been underestimated although certain rudiments of it have made it into newer textbooks. Instead of making heavy use of cohomological or topological considerations or character theory, we introduce a completely elementary but rather general concept of normalized group action (1.5.4) which serves as a base for not only the above-mentioned highlights but also for other important theorems (3.6, 3.9 (Gasch¨utz), 3.13 (Schur-Zassenhaus)) and for the transfer. Thus we hope to escape the cartesian reservation towards authors in general1, although other parts of the theory clearly follow well-known patterns when a major modification would not result in a gain of clarity or applicability. -
Symmetries and Exotic Smooth Structures on a K3 Surface WM Chen University of Massachusetts - Amherst, [email protected]
University of Massachusetts Amherst ScholarWorks@UMass Amherst Mathematics and Statistics Department Faculty Mathematics and Statistics Publication Series 2008 Symmetries and exotic smooth structures on a K3 surface WM Chen University of Massachusetts - Amherst, [email protected] S Kwasik Follow this and additional works at: https://scholarworks.umass.edu/math_faculty_pubs Part of the Physical Sciences and Mathematics Commons Recommended Citation Chen, WM and Kwasik, S, "Symmetries and exotic smooth structures on a K3 surface" (2008). JOURNAL OF TOPOLOGY. 268. Retrieved from https://scholarworks.umass.edu/math_faculty_pubs/268 This Article is brought to you for free and open access by the Mathematics and Statistics at ScholarWorks@UMass Amherst. It has been accepted for inclusion in Mathematics and Statistics Department Faculty Publication Series by an authorized administrator of ScholarWorks@UMass Amherst. For more information, please contact [email protected]. SYMMETRIES AND EXOTIC SMOOTH STRUCTURES ON A K3 SURFACE WEIMIN CHEN AND SLAWOMIR KWASIK Abstract. Smooth and symplectic symmetries of an infinite family of distinct ex- otic K3 surfaces are studied, and comparison with the corresponding symmetries of the standard K3 is made. The action on the K3 lattice induced by a smooth finite group action is shown to be strongly restricted, and as a result, nonsmoothability of actions induced by a holomorphic automorphism of a prime order ≥ 7 is proved and nonexistence of smooth actions by several K3 groups is established (included among which is the binary tetrahedral group T24 which has the smallest order). Concerning symplectic symmetries, the fixed-point set structure of a symplectic cyclic action of a prime order ≥ 5 is explicitly determined, provided that the action is homologically nontrivial. -
The Group of Automorphisms of the Holomorph of a Group
Pacific Journal of Mathematics THE GROUP OF AUTOMORPHISMS OF THE HOLOMORPH OF A GROUP NAI-CHAO HSU Vol. 11, No. 3 BadMonth 1961 THE GROUP OF AUTOMORPHISMS OF THE HOLOMORPH OF A GROUP NAI-CHAO HSU l Introduction* If G = HK where H is a normal subgroup of the group G and where K is a subgroup of G with the trivial intersection with H, then G is said to be a semi-direct product of H by K or a splitting extension of H by K. We can consider a splitting extension G as an ordered triple (H, K; Φ) where φ is a homomorphism of K into the automorphism group 2I(if) of H. The ordered triple (iϊ, K; φ) is the totality of all ordered pairs (h, k), he H, he K, with the multiplication If φ is a monomorphism of if into §I(if), then (if, if; φ) is isomorphic to (iϊ, Φ(K); c) where c is the identity mapping of φ(K), and therefore G is the relative holomorph of if with respect to a subgroup φ(-K) of Sί(ίf). If φ is an isomorphism of K onto Sί(iϊ), then G is the holomorph of if. Let if be a group, and let G be the holomorph of H. We are con- sidering if as a subgroup of G in the usual way. GoΓfand [1] studied the group Sί^(G) of automorphisms of G each of which maps H onto itself, the group $(G) of inner automorphisms of G, and the factor group SIff(G)/$5(G). -
Notes on Finite Group Theory
Notes on finite group theory Peter J. Cameron October 2013 2 Preface Group theory is a central part of modern mathematics. Its origins lie in geome- try (where groups describe in a very detailed way the symmetries of geometric objects) and in the theory of polynomial equations (developed by Galois, who showed how to associate a finite group with any polynomial equation in such a way that the structure of the group encodes information about the process of solv- ing the equation). These notes are based on a Masters course I gave at Queen Mary, University of London. Of the two lecturers who preceded me, one had concentrated on finite soluble groups, the other on finite simple groups; I have tried to steer a middle course, while keeping finite groups as the focus. The notes do not in any sense form a textbook, even on finite group theory. Finite group theory has been enormously changed in the last few decades by the immense Classification of Finite Simple Groups. The most important structure theorem for finite groups is the Jordan–Holder¨ Theorem, which shows that any finite group is built up from finite simple groups. If the finite simple groups are the building blocks of finite group theory, then extension theory is the mortar that holds them together, so I have covered both of these topics in some detail: examples of simple groups are given (alternating groups and projective special linear groups), and extension theory (via factor sets) is developed for extensions of abelian groups. In a Masters course, it is not possible to assume that all the students have reached any given level of proficiency at group theory. -
Lifting a 5-Dimensional Representation of $ M {11} $ to a Complex Unitary Representation of a Certain Amalgam
Lifting a 5-dimensional representation of M11 to a complex unitary representation of a certain amalgam Geoffrey R. Robinson July 16, 2018 Abstract We lift the 5-dimensional representation of M11 in characteristic 3 to a unitary complex representation of the amalgam GL(2, 3) ∗D8 S4. 1 The representation It is well known that the Mathieu group M11, the smallest sporadic simple group, has a 5-dimensional (absolutely) irreducible representation over GF(3) (in fact, there are two mutually dual such representations). It is clear that this does not lift to a complex representation, as M11 has no faithful complex character of degree less than 10. However, M11 is a homomorphic image of the amalgam G = GL(2, 3) D8 S4, ∗ and it turns out that if we consider the 5-dimension representation of M11 as a representation of G, then we may lift that representation of G to a complex representation. We aim to do that in such a way that the lifted representation Z 1 is unitary, and we realise it over [ √ 2 ], so that the complex representation admits reduction (mod p) for each odd− prime. These requirements are stringent enough to allow us explicitly exhibit representing matrices. It turns out that reduction (mod p) for any odd prime p other than 3 yields either a 5-dimensional arXiv:1502.00520v3 [math.RT] 8 Feb 2015 special linear group or a 5-dimensional special unitary group, so it is only the behaviour at the prime 3 which is exceptional. We are unsure at present whether the 5-dimensional complex representation of G is faithful (though it does have free kernel), so we will denote the image of Z 1 G in SU(5, [ √ 2 ]) by L, and denote the image of L under reduction (mod p) − by Lp. -
K3 Surfaces, N= 4 Dyons, and the Mathieu Group
K3 Surfaces, =4 Dyons, N and the Mathieu Group M24 Miranda C. N. Cheng Department of Physics, Harvard University, Cambridge, MA 02138, USA Abstract A close relationship between K3 surfaces and the Mathieu groups has been established in the last century. Furthermore, it has been observed recently that the elliptic genus of K3 has a natural inter- pretation in terms of the dimensions of representations of the largest Mathieu group M24. In this paper we first give further evidence for this possibility by studying the elliptic genus of K3 surfaces twisted by some simple symplectic automorphisms. These partition functions with insertions of elements of M24 (the McKay-Thompson series) give further information about the relevant representation. We then point out that this new “moonshine” for the largest Mathieu group is con- nected to an earlier observation on a moonshine of M24 through the 1/4-BPS spectrum of K3 T 2-compactified type II string theory. This insight on the symmetry× of the theory sheds new light on the gener- alised Kac-Moody algebra structure appearing in the spectrum, and leads to predictions for new elliptic genera of K3, perturbative spec- arXiv:1005.5415v2 [hep-th] 3 Jun 2010 trum of the toroidally compactified heterotic string, and the index for the 1/4-BPS dyons in the d = 4, = 4 string theory, twisted by elements of the group of stringy K3N isometries. 1 1 Introduction and Summary Recently there have been two new observations relating K3 surfaces and the largest Mathieu group M24. They seem to suggest that the sporadic group M24 naturally acts on the spectrum of K3-compactified string theory. -
Group Theory
Algebra Math Notes • Study Guide Group Theory Table of Contents Groups..................................................................................................................................................................... 3 Binary Operations ............................................................................................................................................................. 3 Groups .............................................................................................................................................................................. 3 Examples of Groups ......................................................................................................................................................... 4 Cyclic Groups ................................................................................................................................................................... 5 Homomorphisms and Normal Subgroups ......................................................................................................................... 5 Cosets and Quotient Groups ............................................................................................................................................ 6 Isomorphism Theorems .................................................................................................................................................... 7 Product Groups ............................................................................................................................................................... -
A Chemist Looks at the Structure of Symmetry Groups
A CHEMIST LOOKS AT THE STRUCTURE OF SYMMETRY GROUPS On a generic scheme of important point groups for rigid molecular frames H. P. Fritzer Institut fur Physikalische und Theoretische Chemie, Technical University, A-8010 Graz, Austria Abstract A practical method for generating larger symmetry groups from smaller ones is presented. It is based upon the con- struction of the abstract-unique group H(G) called the holomorph of a given starting group G. The extension of G by its full automorphism group A(G) is given in great detail as permutation realizations for both the cyclic and the abelian group of order 4. A selection of point groups generated by this method of the holomorph is given for some important symmetries. Contribution for the Proceedings of the %th International Colloquium on "Group Theorebical Methods In Physics", University of Nijmegen, The Netherlands, 1975. 349 ~,Introduction Symmetry considerations have always been important in various branches of chemistry from both qualitative (or geo- metrical) and quantitative (i.e. group theoretical) points of view. It is the concept of structural symmetry or (mentioning L. Pauling's words about)the "architecture of molecules", resp., that is relating experimental observations like optical spectra, dipole moments, electric and magnetic susceptibilities, optical activity and chirality, etc., to theoretical calculations based upon quantum mechanics. Therefore, group theory is connecting very efficiently the world of problems in chemical statics and dynamics to the world of abstractly operating computational machinery supplied by physics and mathematics. The traditional interest of chemists in group theory stems from areas as classification of molecules by means of point groups, normal vibrations analysis, MO theory, crystal and/or ligand field theory (a terrible semantics since these topics have nothing to do with a physical "field theory"), selection rules, and so forth. -
The Mathieu Group M24 As We Knew It
Cambridge University Press 978-1-108-42978-8 — The Mathieu Groups A. A. Ivanov Excerpt More Information 1 The Mathieu Group M24 As We Knew It In this chapter we start by reviewing the common way to describe the Math- ieu group G = M24 as the automorphism group of the binary Golay code and of the Steiner system formed by the minimal codewords in the Golay code. This discussion will lead us to the structure of the octad–trio–sextet stabiliz- ers {G1, G2, G3}. The starting point is the observation that, when forming a similar triple {H1, H2, H3} comprised of the stabilizers of one-, two- and three-dimensional subspaces in H = L5(2),wehave 4 6 G1 =∼ H1 =∼ 2 : L4(2), G2 =∼ H2 =∼ 2 : (L3(2) × S3), [G1 : G1 ∩ G2]=[H1 : H1 ∩ H2]=15, [G2 : G1 ∩ G2]=[H2 : H1 ∩ H1]=3, so that the amalgams {G1, G2} and {H1, H2} have the same type according to Goldschmidt’s terminology, although they are not isomorphic and differ by a twist performed by an outer automorphism of 3 3 H1 ∩ H2 =∼ G1 ∩ G2 =∼ (2 × 2 ) : (L3(2) × 2), which permutes conjugacy classes of L3(2)-subgroups. This observation led us to the construction of M24 as the universal completion of a twisted L5(2)- amalgam. 1.1 The Golay Code Commonly the Mathieu group M24 is defined as the automorphism group of the Golay code, which by definition is a (a) binary (b) linear code (c) of length 24, which is (d) even, (e) self-dual and (f) has no codewords of weight 4. -
A UTOMORPHISMS of the DIHEDRAL GROUPS the Group Of
368 MA THEMA TICS: G. A. MILLER PROc. N. A. S. A UTOMORPHISMS OF THE DIHEDRAL GROUPS BY G. A. MILLER DEPARTMENT OF MATHEMATICS, UNIVERSITY OF ILLINOIS Communicated July 24, 1942 The group of inner automorphisms of a dihedral group whose order is twice an odd number is obviously the group itself while the group of inner automorphisms of a dihedral group whose order is divisible by 4 is the quotient group of this dihedral group with respect to its invariant subgroup of order 2 when the dihedral group is not the four group. It is well known that the four group is the only abelian dihedral group and that its group of automorphisms is the symmetric group of order 6. All of these automor- phisms except the identity are outer automorphisms but this symmetric group admits no outer automorphisms. In fact, we shall prove that it is the only dihedral group which does not admit any outer automorphisms. To emphasize this fact it may be noted here that on page 152 of the Survey of Modern Algebra by Birkhoff and MacLane (1941) it is stated that the group of symmetries of the square, which is also a dihedral group, admits no outer automorphisms. This is obviously not in agreement with the theorem noted above. To prove that the symmetric group of order 6, which is also the group of movements of the equilateral triangle, is the only dihedral group which does not admit any outer automorphisms it may first be noted that if a dihedral group whose order is twice an odd number admits no outer auto- morphisms its cyclic subgroup of index 2 cannot have an order which exceeds 3 since in the group of automorphisms of a cyclic group every operator of highest order corresponds to every other such operator and every operator may correspond to its inverse.