2.3 Conjugacy in Symmetric Groups
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On the Permutations Generated by Cyclic Shift
1 2 Journal of Integer Sequences, Vol. 14 (2011), 3 Article 11.3.2 47 6 23 11 On the Permutations Generated by Cyclic Shift St´ephane Legendre Team of Mathematical Eco-Evolution Ecole Normale Sup´erieure 75005 Paris France [email protected] Philippe Paclet Lyc´ee Chateaubriand 00161 Roma Italy [email protected] Abstract The set of permutations generated by cyclic shift is studied using a number system coding for these permutations. The system allows to find the rank of a permutation given how it has been generated, and to determine a permutation given its rank. It defines a code describing structural and symmetry properties of the set of permuta- tions ordered according to generation by cyclic shift. The code is associated with an Hamiltonian cycle in a regular weighted digraph. This Hamiltonian cycle is conjec- tured to be of minimal weight, leading to a combinatorial Gray code listing the set of permutations. 1 Introduction It is well known that any natural integer a can be written uniquely in the factorial number system n−1 a = ai i!, ai ∈ {0,...,i}, i=1 X 1 where the uniqueness of the representation comes from the identity n−1 i · i!= n! − 1. (1) i=1 X Charles-Ange Laisant showed in 1888 [2] that the factorial number system codes the permutations generated in lexicographic order. More precisely, when the set of permutations is ordered lexicographically, the rank of a permutation written in the factorial number system provides a code determining the permutation. The code specifies which interchanges of the symbols according to lexicographic order have to be performed to generate the permutation. -
4. Groups of Permutations 1
4. Groups of permutations 1 4. Groups of permutations Consider a set of n distinguishable objects, fB1;B2;B3;:::;Bng. These may be arranged in n! different ways, called permutations of the set. Permu- tations can also be thought of as transformations of a given ordering of the set into other orderings. A convenient notation for specifying a given permutation operation is 1 2 3 : : : n ! , a1 a2 a3 : : : an where the numbers fa1; a2; a3; : : : ; ang are the numbers f1; 2; 3; : : : ; ng in some order. This operation can be interpreted in two different ways, as follows. Interpretation 1: The object in position 1 in the initial ordering is moved to position a1, the object in position 2 to position a2,. , the object in position n to position an. In this interpretation, the numbers in the two rows of the permutation symbol refer to the positions of objects in the ordered set. Interpretation 2: The object labeled 1 is replaced by the object labeled a1, the object labeled 2 by the object labeled a2,. , the object labeled n by the object labeled an. In this interpretation, the numbers in the two rows of the permutation symbol refer to the labels of the objects in the ABCD ! set. The labels need not be numerical { for instance, DCAB is a well-defined permutation which changes BDCA, for example, into CBAD. Either of these interpretations is acceptable, but one interpretation must be used consistently in any application. The particular application may dictate which is the appropriate interpretation to use. Note that, in either interpre- tation, the order of the columns in the permutation symbol is irrelevant { the columns may be written in any order without affecting the result, provided each column is kept intact. -
Mathematics of the Rubik's Cube
Mathematics of the Rubik's cube Associate Professor W. D. Joyner Spring Semester, 1996{7 2 \By and large it is uniformly true that in mathematics that there is a time lapse between a mathematical discovery and the moment it becomes useful; and that this lapse can be anything from 30 to 100 years, in some cases even more; and that the whole system seems to function without any direction, without any reference to usefulness, and without any desire to do things which are useful." John von Neumann COLLECTED WORKS, VI, p. 489 For more mathematical quotes, see the first page of each chapter below, [M], [S] or the www page at http://math.furman.edu/~mwoodard/mquot. html 3 \There are some things which cannot be learned quickly, and time, which is all we have, must be paid heavily for their acquiring. They are the very simplest things, and because it takes a man's life to know them the little new that each man gets from life is very costly and the only heritage he has to leave." Ernest Hemingway (From A. E. Hotchner, PAPA HEMMINGWAY, Random House, NY, 1966) 4 Contents 0 Introduction 13 1 Logic and sets 15 1.1 Logic................................ 15 1.1.1 Expressing an everyday sentence symbolically..... 18 1.2 Sets................................ 19 2 Functions, matrices, relations and counting 23 2.1 Functions............................. 23 2.2 Functions on vectors....................... 28 2.2.1 History........................... 28 2.2.2 3 × 3 matrices....................... 29 2.2.3 Matrix multiplication, inverses.............. 30 2.2.4 Muliplication and inverses............... -
Spatial Rules for Capturing Qualitatively Equivalent Configurations in Sketch Maps
Preprints of the Federated Conference on Computer Science and Information Systems pp. 13–20 Spatial Rules for Capturing Qualitatively Equivalent Configurations in Sketch maps Sahib Jan, Carl Schultz, Angela Schwering and Malumbo Chipofya Institute for Geoinformatics University of Münster, Germany Email: sahib.jan | schultzc | schwering | mchipofya|@uni-muenster.de Abstract—Sketch maps are an externalization of an indi- such as representations for the topological relations [6, 23], vidual’s mental images of an environment. The information orderings [1, 22, 25], directions [10, 24], relative position of represented in sketch maps is schematized, distorted, generalized, points [19, 20, 24] and others. and thus processing spatial information in sketch maps requires plausible representations based on human cognition. Typically In our previous studies [14, 15, 16, 27], we propose a only qualitative relations between spatial objects are preserved set of plausible representations and their coarse versions to in sketch maps, and therefore processing spatial information on qualitatively formalize key sketch aspects. We use several a qualitative level has been suggested. This study extends our qualifiers to extract qualitative constraints from geometric previous work on qualitative representations and alignment of representations of sketch and geo-referenced maps [13] in sketch maps. In this study, we define a set of spatial relations using the declarative spatial reasoning system CLP(QS) as an the form of Qualitative Constraint Networks (QCNs). QCNs approach to formalizing key spatial aspects that are preserved are complete graphs representing spatial objects and relations in sketch maps. Unlike geo-referenced maps, sketch maps do between them. However, in order to derive more cognitively not have a single, global reference frame. -
Higher-Order Intersections in Low-Dimensional Topology
Higher-order intersections in SPECIAL FEATURE low-dimensional topology Jim Conanta, Rob Schneidermanb, and Peter Teichnerc,d,1 aDepartment of Mathematics, University of Tennessee, Knoxville, TN 37996-1300; bDepartment of Mathematics and Computer Science, Lehman College, City University of New York, 250 Bedford Park Boulevard West, Bronx, NY 10468; cDepartment of Mathematics, University of California, Berkeley, CA 94720-3840; and dMax Planck Institute for Mathematics, Vivatsgasse 7, 53111 Bonn, Germany Edited by Robion C. Kirby, University of California, Berkeley, CA, and approved February 24, 2011 (received for review December 22, 2010) We show how to measure the failure of the Whitney move in dimension 4 by constructing higher-order intersection invariants W of Whitney towers built from iterated Whitney disks on immersed surfaces in 4-manifolds. For Whitney towers on immersed disks in the 4-ball, we identify some of these new invariants with – previously known link invariants such as Milnor, Sato Levine, and Fig. 1. (Left) A canceling pair of transverse intersections between two local Arf invariants. We also define higher-order Sato–Levine and Arf sheets of surfaces in a 3-dimensional slice of 4-space. The horizontal sheet invariants and show that these invariants detect the obstructions appears entirely in the “present,” and the red sheet appears as an arc that to framing a twisted Whitney tower. Together with Milnor invar- is assumed to extend into the “past” and the “future.” (Center) A Whitney iants, these higher-order invariants are shown to classify the exis- disk W pairing the intersections. (Right) A Whitney move guided by W tence of (twisted) Whitney towers of increasing order in the 4-ball. -
Classification of 3-Manifolds with Certain Spines*1 )
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 205, 1975 CLASSIFICATIONOF 3-MANIFOLDSWITH CERTAIN SPINES*1 ) BY RICHARD S. STEVENS ABSTRACT. Given the group presentation <p= (a, b\ambn, apbq) With m, n, p, q & 0, we construct the corresponding 2-complex Ky. We prove the following theorems. THEOREM 7. Jf isa spine of a closed orientable 3-manifold if and only if (i) \m\ = \p\ = 1 or \n\ = \q\ = 1, or (") (m, p) = (n, q) = 1. Further, if (ii) holds but (i) does not, then the manifold is unique. THEOREM 10. If M is a closed orientable 3-manifold having K^ as a spine and \ = \mq — np\ then M is a lens space L\ % where (\,fc) = 1 except when X = 0 in which case M = S2 X S1. It is well known that every connected compact orientable 3-manifold with or without boundary has a spine that is a 2-complex with a single vertex. Such 2-complexes correspond very naturally to group presentations, the 1-cells corre- sponding to generators and the 2-cells corresponding to relators. In the case of a closed orientable 3-manifold, there are equally many 1-cells and 2-cells in the spine, i.e., equally many generators and relators in the corresponding presentation. Given a group presentation one is motivated to ask the following questions: (1) Is the corresponding 2-complex a spine of a compact orientable 3-manifold? (2) If there are equally many generators and relators, is the 2-complex a spine of a closed orientable 3-manifold? (3) Can we say what manifold(s) have the 2-complex as a spine? L. -
Algebras Assigned to Ternary Relations
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Repository of the Academy's Library Miskolc Mathematical Notes HU e-ISSN 1787-2413 Vol. 14 (2013), No 3, pp. 827-844 DOI: 10.18514/MMN.2013.507 Algebras assigned to ternary relations Ivan Chajda, Miroslav Kola°ík, and Helmut Länger Miskolc Mathematical Notes HU e-ISSN 1787-2413 Vol. 14 (2013), No. 3, pp. 827–844 ALGEBRAS ASSIGNED TO TERNARY RELATIONS IVAN CHAJDA, MIROSLAV KOLARˇ IK,´ AND HELMUT LANGER¨ Received 19 March, 2012 Abstract. We show that to every centred ternary relation T on a set A there can be assigned (in a non-unique way) a ternary operation t on A such that the identities satisfied by .A t/ reflect relational properties of T . We classify ternary operations assigned to centred ternaryI relations and we show how the concepts of relational subsystems and homomorphisms are connected with subalgebras and homomorphisms of the assigned algebra .A t/. We show that for ternary relations having a non-void median can be derived so-called median-likeI algebras .A t/ which I become median algebras if the median MT .a;b;c/ is a singleton for all a;b;c A. Finally, we introduce certain algebras assigned to cyclically ordered sets. 2 2010 Mathematics Subject Classification: 08A02; 08A05 Keywords: ternary relation, betweenness, cyclic order, assigned operation, centre, median In [2] and [3], the first and the third author showed that to certain relational systems A .A R/, where A ¿ and R is a binary relation on A, there can be assigned a certainD groupoidI G .A/¤ .A / which captures the properties of R. -
Chapter 3: Transformations Groups, Orbits, and Spaces of Orbits
Preprint typeset in JHEP style - HYPER VERSION Chapter 3: Transformations Groups, Orbits, And Spaces Of Orbits Gregory W. Moore Abstract: This chapter focuses on of group actions on spaces, group orbits, and spaces of orbits. Then we discuss mathematical symmetric objects of various kinds. May 3, 2019 -TOC- Contents 1. Introduction 2 2. Definitions and the stabilizer-orbit theorem 2 2.0.1 The stabilizer-orbit theorem 6 2.1 First examples 7 2.1.1 The Case Of 1 + 1 Dimensions 11 3. Action of a topological group on a topological space 14 3.1 Left and right group actions of G on itself 19 4. Spaces of orbits 20 4.1 Simple examples 21 4.2 Fundamental domains 22 4.3 Algebras and double cosets 28 4.4 Orbifolds 28 4.5 Examples of quotients which are not manifolds 29 4.6 When is the quotient of a manifold by an equivalence relation another man- ifold? 33 5. Isometry groups 34 6. Symmetries of regular objects 36 6.1 Symmetries of polygons in the plane 39 3 6.2 Symmetry groups of some regular solids in R 42 6.3 The symmetry group of a baseball 43 7. The symmetries of the platonic solids 44 7.1 The cube (\hexahedron") and octahedron 45 7.2 Tetrahedron 47 7.3 The icosahedron 48 7.4 No more regular polyhedra 50 7.5 Remarks on the platonic solids 50 7.5.1 Mathematics 51 7.5.2 History of Physics 51 7.5.3 Molecular physics 51 7.5.4 Condensed Matter Physics 52 7.5.5 Mathematical Physics 52 7.5.6 Biology 52 7.5.7 Human culture: Architecture, art, music and sports 53 7.6 Regular polytopes in higher dimensions 53 { 1 { 8. -
Finiteness of $ Z $-Classes in Reductive Groups
FINITENESS OF z-CLASSES IN REDUCTIVE GROUPS SHRIPAD M. GARGE. AND ANUPAM SINGH. Abstract. Let k be a perfect field such that for every n there are only finitely many field extensions, up to isomorphism, of k of degree n. If G is a reductive algebraic group defined over k, whose characteristic is very good for G, then we prove that G(k) has only finitely many z-classes. For each perfect field k which does not have the above finiteness property we show that there exist groups G over k such that G(k) has infinitely many z-classes. 1. Introduction Let G be a group. A G-set is a non-empty set X admitting an action of the group G. Two G-sets X and Y are called G-isomorphic if there is a bijection φ : X → Y which commutes with the G-actions on X and Y . If the G-sets X and Y are transitive, say X = Gx and Y = Gy for some x ∈ X and y ∈ Y , then X and Y are G-isomorphic if and only if the stabilizers Gx and Gy of x and y, respectively, in G are conjugate as subgroups of G. One of the most important group actions is the conjugation action of a group G on itself. It partitions the group G into its conjugacy classes which are orbits under this action. However, from the point of view of G-action, it is more natural to partition the group G into sets consisting of conjugacy classes which are G- arXiv:2001.06359v1 [math.GR] 17 Jan 2020 isomorphic to each other. -
Math 3230 Abstract Algebra I Sec 3.7: Conjugacy Classes
Math 3230 Abstract Algebra I Sec 3.7: Conjugacy classes Slides created by M. Macauley, Clemson (Modified by E. Gunawan, UConn) http://egunawan.github.io/algebra Abstract Algebra I Sec 3.7 Conjugacy classes Abstract Algebra I 1 / 13 Conjugation Recall that for H ≤ G, the conjugate subgroup of H by a fixed g 2 G is gHg −1 = fghg −1 j h 2 Hg : Additionally, H is normal iff gHg −1 = H for all g 2 G. We can also fix the element we are conjugating. Given x 2 G, we may ask: \which elements can be written as gxg −1 for some g 2 G?" The set of all such elements in G is called the conjugacy class of x, denoted clG (x). Formally, this is the set −1 clG (x) = fgxg j g 2 Gg : Remarks −1 In any group, clG (e) = feg, because geg = e for any g 2 G. −1 If x and g commute, then gxg = x. Thus, when computing clG (x), we only need to check gxg −1 for those g 2 G that do not commute with x. Moreover, clG (x) = fxg iff x commutes with everything in G. (Why?) Sec 3.7 Conjugacy classes Abstract Algebra I 2 / 13 Conjugacy classes Proposition 1 Conjugacy is an equivalence relation. Proof Reflexive: x = exe−1. Symmetric: x = gyg −1 ) y = g −1xg. −1 −1 −1 Transitive: x = gyg and y = hzh ) x = (gh)z(gh) . Since conjugacy is an equivalence relation, it partitions the group G into equivalence classes (conjugacy classes). Let's compute the conjugacy classes in D4. -
Arxiv:1711.04390V1 [Math.LO]
A FAMILY OF DP-MINIMAL EXPANSIONS OF Z; ( +) MINH CHIEU TRAN, ERIK WALSBERG Abstract. We show that the cyclically ordered-abelian groups expanding (Z; +) contain a continuum-size family of dp-minimal structures such that no two members define the same subsets of Z. 1. Introduction In this paper, we are concerned with the following classification-type question: What are the dp-minimal expansions of Z; ? ( +) For a definition of dp-minimality, see [Sim15, Chapter 4]. The terms expansion and reduct here are as used in the sense of definability: If M1 and M2 are structures with underlying set M and every M1-definable set is also definable in M2, we say that M1 is a reduct of M2 and that M2 is an expansion of M1. Two structures are definably equivalent if each is a reduct of the other. A very remarkable common feature of the known dp-minimal expansions of Z; ( +) is their “rigidity”. In [CP16], it is shown that all proper stable expansions of Z; ( +) have infinite weight, hence infinite dp-rank, and so in particular are not dp-minimal. The expansion Z; , , well-known to be dp-minimal, does not have any proper ( + <) dp-minimal expansion [ADH+16, 6.6], or any proper expansion of finite dp-rank, or even any proper strong expansion [DG17, 2.20]. Moreover, any reduct Z; , ( + <) expanding Z; is definably equivalent to Z; or Z; , [Con16]. Recently, it ( +) ( +) ( + <) is shown in [Ad17, 1.2] that Z; , is dp-minimal for all primes p where be ( + ≺p) ≺p the partial order on Z given by declaring k l if and only if v k v l with ≺p p( ) < p( ) v the p-adic valuation on Z. -
A STUDY on the ALGEBRAIC STRUCTURE of SL 2(Zpz)
A STUDY ON THE ALGEBRAIC STRUCTURE OF SL2 Z pZ ( ~ ) A Thesis Presented to The Honors Tutorial College Ohio University In Partial Fulfillment of the Requirements for Graduation from the Honors Tutorial College with the degree of Bachelor of Science in Mathematics by Evan North April 2015 Contents 1 Introduction 1 2 Background 5 2.1 Group Theory . 5 2.2 Linear Algebra . 14 2.3 Matrix Group SL2 R Over a Ring . 22 ( ) 3 Conjugacy Classes of Matrix Groups 26 3.1 Order of the Matrix Groups . 26 3.2 Conjugacy Classes of GL2 Fp ....................... 28 3.2.1 Linear Case . .( . .) . 29 3.2.2 First Quadratic Case . 29 3.2.3 Second Quadratic Case . 30 3.2.4 Third Quadratic Case . 31 3.2.5 Classes in SL2 Fp ......................... 33 3.3 Splitting of Classes of(SL)2 Fp ....................... 35 3.4 Results of SL2 Fp ..............................( ) 40 ( ) 2 4 Toward Lifting to SL2 Z p Z 41 4.1 Reduction mod p ...............................( ~ ) 42 4.2 Exploring the Kernel . 43 i 4.3 Generalizing to SL2 Z p Z ........................ 46 ( ~ ) 5 Closing Remarks 48 5.1 Future Work . 48 5.2 Conclusion . 48 1 Introduction Symmetries are one of the most widely-known examples of pure mathematics. Symmetry is when an object can be rotated, flipped, or otherwise transformed in such a way that its appearance remains the same. Basic geometric figures should create familiar examples, take for instance the triangle. Figure 1: The symmetries of a triangle: 3 reflections, 2 rotations. The red lines represent the reflection symmetries, where the trianlge is flipped over, while the arrows represent the rotational symmetry of the triangle.