Samira Hosseinzadeh Alikhalaji, Mojtaba Sedaghatjoo And
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Math 5111 (Algebra 1) Lecture #14 of 24 ∼ October 19Th, 2020
Math 5111 (Algebra 1) Lecture #14 of 24 ∼ October 19th, 2020 Group Isomorphism Theorems + Group Actions The Isomorphism Theorems for Groups Group Actions Polynomial Invariants and An This material represents x3.2.3-3.3.2 from the course notes. Quotients and Homomorphisms, I Like with rings, we also have various natural connections between normal subgroups and group homomorphisms. To begin, observe that if ' : G ! H is a group homomorphism, then ker ' is a normal subgroup of G. In fact, I proved this fact earlier when I introduced the kernel, but let me remark again: if g 2 ker ', then for any a 2 G, then '(aga−1) = '(a)'(g)'(a−1) = '(a)'(a−1) = e. Thus, aga−1 2 ker ' as well, and so by our equivalent properties of normality, this means ker ' is a normal subgroup. Thus, we can use homomorphisms to construct new normal subgroups. Quotients and Homomorphisms, II Equally importantly, we can also do the reverse: we can use normal subgroups to construct homomorphisms. The key observation in this direction is that the map ' : G ! G=N associating a group element to its residue class / left coset (i.e., with '(a) = a) is a ring homomorphism. Indeed, the homomorphism property is precisely what we arranged for the left cosets of N to satisfy: '(a · b) = a · b = a · b = '(a) · '(b). Furthermore, the kernel of this map ' is, by definition, the set of elements in G with '(g) = e, which is to say, the set of elements g 2 N. Thus, kernels of homomorphisms and normal subgroups are precisely the same things. -
Arxiv:0704.2561V2 [Math.QA] 27 Apr 2007 Nttto O Xeln Okn Odtos H Eoda Second the Conditions
DUAL FEYNMAN TRANSFORM FOR MODULAR OPERADS J. CHUANG AND A. LAZAREV Abstract. We introduce and study the notion of a dual Feynman transform of a modular operad. This generalizes and gives a conceptual explanation of Kontsevich’s dual construction producing graph cohomology classes from a contractible differential graded Frobenius alge- bra. The dual Feynman transform of a modular operad is indeed linear dual to the Feynman transform introduced by Getzler and Kapranov when evaluated on vacuum graphs. In marked contrast to the Feynman transform, the dual notion admits an extremely simple presentation via generators and relations; this leads to an explicit and easy description of its algebras. We discuss a further generalization of the dual Feynman transform whose algebras are not neces- sarily contractible. This naturally gives rise to a two-colored graph complex analogous to the Boardman-Vogt topological tree complex. Contents Introduction 1 Notation and conventions 2 1. Main construction 4 2. Twisted modular operads and their algebras 8 3. Algebras over the dual Feynman transform 12 4. Stable graph complexes 13 4.1. Commutative case 14 4.2. Associative case 15 5. Examples 17 6. Moduli spaces of metric graphs 19 6.1. Commutative case 19 6.2. Associative case 21 7. BV-resolution of a modular operad 22 7.1. Basic construction and description of algebras 22 7.2. Stable BV-graph complexes 23 References 26 Introduction arXiv:0704.2561v2 [math.QA] 27 Apr 2007 The relationship between operadic algebras and various moduli spaces goes back to Kontse- vich’s seminal papers [19] and [20] where graph homology was also introduced. -
GROUP ACTIONS 1. Introduction the Groups Sn, An, and (For N ≥ 3)
GROUP ACTIONS KEITH CONRAD 1. Introduction The groups Sn, An, and (for n ≥ 3) Dn behave, by their definitions, as permutations on certain sets. The groups Sn and An both permute the set f1; 2; : : : ; ng and Dn can be considered as a group of permutations of a regular n-gon, or even just of its n vertices, since rigid motions of the vertices determine where the rest of the n-gon goes. If we label the vertices of the n-gon in a definite manner by the numbers from 1 to n then we can view Dn as a subgroup of Sn. For instance, the labeling of the square below lets us regard the 90 degree counterclockwise rotation r in D4 as (1234) and the reflection s across the horizontal line bisecting the square as (24). The rest of the elements of D4, as permutations of the vertices, are in the table below the square. 2 3 1 4 1 r r2 r3 s rs r2s r3s (1) (1234) (13)(24) (1432) (24) (12)(34) (13) (14)(23) If we label the vertices in a different way (e.g., swap the labels 1 and 2), we turn the elements of D4 into a different subgroup of S4. More abstractly, if we are given a set X (not necessarily the set of vertices of a square), then the set Sym(X) of all permutations of X is a group under composition, and the subgroup Alt(X) of even permutations of X is a group under composition. If we list the elements of X in a definite order, say as X = fx1; : : : ; xng, then we can think about Sym(X) as Sn and Alt(X) as An, but a listing in a different order leads to different identifications 1 of Sym(X) with Sn and Alt(X) with An. -
Right Product Quasigroups and Loops
RIGHT PRODUCT QUASIGROUPS AND LOOPS MICHAEL K. KINYON, ALEKSANDAR KRAPEZˇ∗, AND J. D. PHILLIPS Abstract. Right groups are direct products of right zero semigroups and groups and they play a significant role in the semilattice decomposition theory of semigroups. Right groups can be characterized as associative right quasigroups (magmas in which left translations are bijective). If we do not assume associativity we get right quasigroups which are not necessarily representable as direct products of right zero semigroups and quasigroups. To obtain such a representation, we need stronger assumptions which lead us to the notion of right product quasigroup. If the quasigroup component is a (one-sided) loop, then we have a right product (left, right) loop. We find a system of identities which axiomatizes right product quasigroups, and use this to find axiom systems for right product (left, right) loops; in fact, we can obtain each of the latter by adjoining just one appropriate axiom to the right product quasigroup axiom system. We derive other properties of right product quasigroups and loops, and conclude by show- ing that the axioms for right product quasigroups are independent. 1. Introduction In the semigroup literature (e.g., [1]), the most commonly used definition of right group is a semigroup (S; ·) which is right simple (i.e., has no proper right ideals) and left cancellative (i.e., xy = xz =) y = z). The structure of right groups is clarified by the following well-known representation theorem (see [1]): Theorem 1.1. A semigroup (S; ·) is a right group if and only if it is isomorphic to a direct product of a group and a right zero semigroup. -
Ring (Mathematics) 1 Ring (Mathematics)
Ring (mathematics) 1 Ring (mathematics) In mathematics, a ring is an algebraic structure consisting of a set together with two binary operations usually called addition and multiplication, where the set is an abelian group under addition (called the additive group of the ring) and a monoid under multiplication such that multiplication distributes over addition.a[›] In other words the ring axioms require that addition is commutative, addition and multiplication are associative, multiplication distributes over addition, each element in the set has an additive inverse, and there exists an additive identity. One of the most common examples of a ring is the set of integers endowed with its natural operations of addition and multiplication. Certain variations of the definition of a ring are sometimes employed, and these are outlined later in the article. Polynomials, represented here by curves, form a ring under addition The branch of mathematics that studies rings is known and multiplication. as ring theory. Ring theorists study properties common to both familiar mathematical structures such as integers and polynomials, and to the many less well-known mathematical structures that also satisfy the axioms of ring theory. The ubiquity of rings makes them a central organizing principle of contemporary mathematics.[1] Ring theory may be used to understand fundamental physical laws, such as those underlying special relativity and symmetry phenomena in molecular chemistry. The concept of a ring first arose from attempts to prove Fermat's last theorem, starting with Richard Dedekind in the 1880s. After contributions from other fields, mainly number theory, the ring notion was generalized and firmly established during the 1920s by Emmy Noether and Wolfgang Krull.[2] Modern ring theory—a very active mathematical discipline—studies rings in their own right. -
Lecture 1.2: Group Actions
Lecture 1.2: Group actions Matthew Macauley Department of Mathematical Sciences Clemson University http://www.math.clemson.edu/~macaule/ Math 8510, Abstract Algebra I M. Macauley (Clemson) Lecture 1.2: Group actions Math 8510, Abstract Algebra I 1 / 29 The symmetric group Definition The group of all permutations of f1;:::; ng is the symmetric group, denoted Sn. We can concisely describe permutations in cycle notation, e.g., 1 2 3 4 as (1 2 3 4). Observation 1 Every permutation can be decomposed into a product of disjoint cycles, and disjoint cycles commute. We usually don't write 1-cycles (fixed points). For example, in S10, we can write 1 2 3 4 5 6 7 8 9 10 as (1 4 6 5) (2 3) (8 10 9). By convention, we'll read cycles from right-to-left, like function composition. [Note. Many sources read left-to-right.] M. Macauley (Clemson) Lecture 1.2: Group actions Math 8510, Abstract Algebra I 2 / 29 The symmetric group Remarks The inverse of the cycle (1 2 3 4) is (4 3 2 1) = (1 4 3 2). If σ is a k-cycle, then jσj = k. If σ = σ1 ··· σm, all disjoint, then jσj = lcm(jσ1j;:::; jσmj). A 2-cycle is called a transposition. Every cycle (and hence element of Sn) can be written as a product of transpositions: (1 2 3 ··· k) = (1 k) (1 k −1) ··· (1 3) (1 2): We say σ 2 Sn is even if it can be written as a product of an even number of transpositions, otherwise it is odd. -
Single Axioms for Groups and Abelian Groups with Various Operations 1
Single Axioms for Groups and Ab elian Groups with Various Op erations Wil liam W McCune Mathematics and Computer Science Division Argonne National Lab oratory Argonne Illinois USA email mccunemcsanlgov March Abstract This pap er summarizes the results of an investigation into single axioms for groups b oth ordinary and Ab elian with each of following six sets of op erations fpro duct inverseg fdivisiong fdouble division identityg fdouble division inverseg fdivision identityg and fdivision inverseg In all but two of the twelve corresp onding theories we present either the rst single axioms known to us or single axioms shorter than those previously known to us The automated theoremproving program Otter was used extensively to construct sets of candidate axioms and to search for and nd pro ofs that given candidate axioms are in fact single axioms Introduction A single axiom for an equational theory is an equality from which the entire theory can b e derived For example each of the equalities xxxy z xxxz y 1 1 1 1 1 x y x z u y u z 1 is a single axiom for ordinary groups Equation in terms of division was shown to b e a single axiom by G Higman and B H Neumann in and was given by Neumann in Each of and axiomatizes groups in the sense that each generates a theory denitionally equivalent to standard axiomatizations for example the triple e x x 1 x x e x y z x y z where e is the identity This work was supp orted by the Applied Mathematical Sciences subprogram of the Oce of Energy Research US Department -
The Algebraic Theory of Semigroups the Algebraic Theory of Semigroups
http://dx.doi.org/10.1090/surv/007.1 The Algebraic Theory of Semigroups The Algebraic Theory of Semigroups A. H. Clifford G. B. Preston American Mathematical Society Providence, Rhode Island 2000 Mathematics Subject Classification. Primary 20-XX. International Standard Serial Number 0076-5376 International Standard Book Number 0-8218-0271-2 Library of Congress Catalog Card Number: 61-15686 Copying and reprinting. Material in this book may be reproduced by any means for educational and scientific purposes without fee or permission with the exception of reproduction by services that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. This consent does not extend to other kinds of copying for general distribution, for advertising or promotional purposes, or for resale. Requests for permission for commercial use of material should be addressed to the Assistant to the Publisher, American Mathematical Society, P. O. Box 6248, Providence, Rhode Island 02940-6248. Requests can also be made by e-mail to reprint-permissionQams.org. Excluded from these provisions is material in articles for which the author holds copyright. In such cases, requests for permission to use or reprint should be addressed directly to the author(s). (Copyright ownership is indicated in the notice in the lower right-hand corner of the first page of each article.) © Copyright 1961 by the American Mathematical Society. All rights reserved. Printed in the United States of America. Second Edition, 1964 Reprinted with corrections, 1977. The American Mathematical Society retains all rights except those granted to the United States Government. -
On Planar Right Groups Kolja Knauer, Ulrich Knauer
On planar right groups Kolja Knauer, Ulrich Knauer To cite this version: Kolja Knauer, Ulrich Knauer. On planar right groups. Semigroup Forum, Springer Verlag, 2016, 92, pp.142 - 157. 10.1007/s00233-015-9688-2. hal-01457892 HAL Id: hal-01457892 https://hal.archives-ouvertes.fr/hal-01457892 Submitted on 6 Feb 2017 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. On planar right groups Kolja Knauer Ulrich Knauer January 7, 2015 Abstract In 1896 Heinrich Maschke characterized planar finite groups, that is groups which admit a generating system such that the resulting Cayley graph is planar. In our study we consider the question, which finite semi- groups have a planar Cayley graph. Right groups are a class of semigroups relatively close to groups. We present a complete characterization of pla- nar right groups. 1 Introduction Cayley graphs of groups and semigroups enjoy a rich research history and are a classic point of interaction of Graph Theory and Algebra. While on the one hand knowledge about the group or semigroup gives information about the Cayley graph, on the other hand properties of the Cayley graph can be translated back to the algebraic objects and their attributes. -
Some Aspects of Semirings
Appendix A Some Aspects of Semirings Semirings considered as a common generalization of associative rings and dis- tributive lattices provide important tools in different branches of computer science. Hence structural results on semirings are interesting and are a basic concept. Semi- rings appear in different mathematical areas, such as ideals of a ring, as positive cones of partially ordered rings and fields, vector bundles, in the context of topolog- ical considerations and in the foundation of arithmetic etc. In this appendix some algebraic concepts are introduced in order to generalize the corresponding concepts of semirings N of non-negative integers and their algebraic theory is discussed. A.1 Introductory Concepts H.S. Vandiver gave the first formal definition of a semiring and developed the the- ory of a special class of semirings in 1934. A semiring S is defined as an algebra (S, +, ·) such that (S, +) and (S, ·) are semigroups connected by a(b+c) = ab+ac and (b+c)a = ba+ca for all a,b,c ∈ S.ThesetN of all non-negative integers with usual addition and multiplication of integers is an example of a semiring, called the semiring of non-negative integers. A semiring S may have an additive zero ◦ defined by ◦+a = a +◦=a for all a ∈ S or a multiplicative zero 0 defined by 0a = a0 = 0 for all a ∈ S. S may contain both ◦ and 0 but they may not coincide. Consider the semiring (N, +, ·), where N is the set of all non-negative integers; a + b ={lcm of a and b, when a = 0,b= 0}; = 0, otherwise; and a · b = usual product of a and b. -
Introduction to Groups, Rings and Fields
Introduction to Groups, Rings and Fields HT and TT 2011 H. A. Priestley 0. Familiar algebraic systems: review and a look ahead. GRF is an ALGEBRA course, and specifically a course about algebraic structures. This introduc- tory section revisits ideas met in the early part of Analysis I and in Linear Algebra I, to set the scene and provide motivation. 0.1 Familiar number systems Consider the traditional number systems N = 0, 1, 2,... the natural numbers { } Z = m n m, n N the integers { − | ∈ } Q = m/n m, n Z, n = 0 the rational numbers { | ∈ } R the real numbers C the complex numbers for which we have N Z Q R C. ⊂ ⊂ ⊂ ⊂ These come equipped with the familiar arithmetic operations of sum and product. The real numbers: Analysis I built on the real numbers. Right at the start of that course you were given a set of assumptions about R, falling under three headings: (1) Algebraic properties (laws of arithmetic), (2) order properties, (3) Completeness Axiom; summarised as saying the real numbers form a complete ordered field. (1) The algebraic properties of R You were told in Analysis I: Addition: for each pair of real numbers a and b there exists a unique real number a + b such that + is a commutative and associative operation; • there exists in R a zero, 0, for addition: a +0=0+ a = a for all a R; • ∈ for each a R there exists an additive inverse a R such that a+( a)=( a)+a = 0. • ∈ − ∈ − − Multiplication: for each pair of real numbers a and b there exists a unique real number a b such that · is a commutative and associative operation; • · there exists in R an identity, 1, for multiplication: a 1 = 1 a = a for all a R; • · · ∈ for each a R with a = 0 there exists an additive inverse a−1 R such that a a−1 = • a−1 a = 1.∈ ∈ · · Addition and multiplication together: forall a,b,c R, we have the distributive law a (b + c)= a b + a c. -
1 Onesided Inverses for Semigroups
Acta Math. Univ. Comenianae 1 Vol. LXXV, 1(2006), pp. 1–19 ONESIDED INVERSES FOR SEMIGROUPS MARIO PETRICH Abstract. In any semigroup S, we say that elements a and b are left inverses of each other if a = aba, b = bab and a L b, in which case we write a γ b. Right inverses are defined dually with the notation δ. Set τ = δγ. We study the classes of semigroups in which τ has some of the usual properties of a relation. We also consider properties of (maximal) completely simple subsemigroups of S. In terms of the above concepts, we characterize E–solid, central, (almost) L–unipotent and locally (almost) L–unipotent semigroups in many ways. We define these notions for arbitrary semigroups by extending their definitions from regular semigroups. 1. Introduction and summary It is the existence of an inverse for each element which distinguishes a group from a monoid and the existence of an identity which distinguishes a monoid from a semigroup. These differences are attenuated by the possibility of defining an inverse of some elements of an arbitrary semigroup S by the following device. Elements a and b are inverses of each other if a = aba and b = bab. The standard notation for the set of all inverses of a is V (a). Not all elements of S may have an inverse, but those that do are called regular. Hence a semigroup is called regular if all its elements are regular (this is equivalent to the usual definition). Two other important classes of semigroups are distinguished by the properties of inverses of their elements.