A-P Congruences on Baer Semigroups
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Topological Duality and Lattice Expansions Part I: a Topological Construction of Canonical Extensions
TOPOLOGICAL DUALITY AND LATTICE EXPANSIONS PART I: A TOPOLOGICAL CONSTRUCTION OF CANONICAL EXTENSIONS M. ANDREW MOSHIER AND PETER JIPSEN 1. INTRODUCTION The two main objectives of this paper are (a) to prove topological duality theorems for semilattices and bounded lattices, and (b) to show that the topological duality from (a) provides a construction of canonical extensions of bounded lattices. The paper is first of two parts. The main objective of the sequel is to establish a characterization of lattice expansions, i.e., lattices with additional operations, in the topological setting built in this paper. Regarding objective (a), consider the following simple question: Is there a subcategory of Top that is dually equivalent to Lat? Here, Top is the category of topological spaces and continuous maps and Lat is the category of bounded lattices and lattice homomorphisms. To date, the question has been answered positively either by specializing Lat or by generalizing Top. The earliest examples are of the former sort. Tarski [Tar29] (treated in English, e.g., in [BD74]) showed that every complete atomic Boolean lattice is represented by a powerset. Taking some historical license, we can say this result shows that the category of complete atomic Boolean lattices with complete lat- tice homomorphisms is dually equivalent to the category of discrete topological spaces. Birkhoff [Bir37] showed that every finite distributive lattice is represented by the lower sets of a finite partial order. Again, we can now say that this shows that the category of finite distributive lattices is dually equivalent to the category of finite T0 spaces and con- tinuous maps. -
Advanced Discrete Mathematics Mm-504 &
1 ADVANCED DISCRETE MATHEMATICS M.A./M.Sc. Mathematics (Final) MM-504 & 505 (Option-P3) Directorate of Distance Education Maharshi Dayanand University ROHTAK – 124 001 2 Copyright © 2004, Maharshi Dayanand University, ROHTAK All Rights Reserved. No part of this publication may be reproduced or stored in a retrieval system or transmitted in any form or by any means; electronic, mechanical, photocopying, recording or otherwise, without the written permission of the copyright holder. Maharshi Dayanand University ROHTAK – 124 001 Developed & Produced by EXCEL BOOKS PVT. LTD., A-45 Naraina, Phase 1, New Delhi-110 028 3 Contents UNIT 1: Logic, Semigroups & Monoids and Lattices 5 Part A: Logic Part B: Semigroups & Monoids Part C: Lattices UNIT 2: Boolean Algebra 84 UNIT 3: Graph Theory 119 UNIT 4: Computability Theory 202 UNIT 5: Languages and Grammars 231 4 M.A./M.Sc. Mathematics (Final) ADVANCED DISCRETE MATHEMATICS MM- 504 & 505 (P3) Max. Marks : 100 Time : 3 Hours Note: Question paper will consist of three sections. Section I consisting of one question with ten parts covering whole of the syllabus of 2 marks each shall be compulsory. From Section II, 10 questions to be set selecting two questions from each unit. The candidate will be required to attempt any seven questions each of five marks. Section III, five questions to be set, one from each unit. The candidate will be required to attempt any three questions each of fifteen marks. Unit I Formal Logic: Statement, Symbolic representation, totologies, quantifiers, pradicates and validity, propositional logic. Semigroups and Monoids: Definitions and examples of semigroups and monoids (including those pertaining to concentration operations). -
Chain Based Lattices
Pacific Journal of Mathematics CHAIN BASED LATTICES GEORGE EPSTEIN AND ALFRED HORN Vol. 55, No. 1 September 1974 PACIFIC JOURNAL OF MATHEMATICS Vol. 55, No. 1, 1974 CHAIN BASED LATTICES G. EPSTEIN AND A. HORN In recent years several weakenings of Post algebras have been studied. Among these have been P0"lattices by T. Traezyk, Stone lattice of order n by T. Katrinak and A. Mitschke, and P-algebras by the present authors. Each of these system is an abstraction from certain aspects of Post algebras, and no two of them are comparable. In the present paper, the theory of P0-lattices will be developed further and two new systems, called Pi-lattices and P2-lattices are introduced. These systems are referred to as chain based lattices. P2-lattices form the intersection of all three weakenings mentioned above. While P-algebras and weaker systems such as L-algebras, Heyting algebras, and P-algebras, do not require any distinguished chain of elements other than 0, 1, chain based lattices require such a chain. Definitions are given in § 1. A P0-lattice is a bounded distributive lattice A which is generated by its center and a finite subchain con- taining 0 and 1. Such a subchain is called a chain base for A. The order of a P0-lattice A is the smallest number of elements in a chain base of A. In § 2, properties of P0-lattices are given which are used in later sections. If a P0-lattice A is a Heyting algebra, then it is shown in § 3, that there exists a unique chain base 0 = e0 < ex < < en_x — 1 such that ei+ί —* et = et for all i > 0. -
Lattices: an Introduction
Lattices: An Introduction Felix Gotti [email protected] UC Berkeley Student Combinatorics Seminar Felix Gotti [email protected] Lattices: An Introduction Outline General Lattices Modular Lattices Distributive Lattices Felix Gotti [email protected] Lattices: An Introduction Joins and Meets Definition (Joins and Meets) Let P be a poset. I If S ⊆ P a join (or supremum) of S, denoted by _ s; s2S is an element of u 2 P that is an upper bound of S satisfying that if u0 is any other upper bound of S, then u ≤ u0. I The definition of a meet (or infimum) of S ⊆ P, denoted by ^ s; s2S is dual to the definition of join. Remark: Note that if a join (resp., meet) exists then it is unique. Felix Gotti [email protected] Lattices: An Introduction Definition of Lattice Definition I A join-semilattice (resp., meet-semilattice) is a poset such that any pair of elements have a join (resp., meet). I A lattice is a poset that is both a join-semilattice and a meet-semilattice. I If L is a lattice and S ⊂ L such that r _ s; r ^ s 2 S for all r; s 2 S, we say that S is a sublattice of L. Example of lattices: I Every totally ordered set is a lattice. ∗ I If L and M are lattices, so are L ; L ⊕ M, and L × M. While L + M is not a lattice, at least L or M is empty, (L + M) [ f0^; 1^g is always a lattice. I The lattices L and M are sublattices of L ⊕ M and (L + M) [ f0^; 1^g. -
COMPLETE HOMOMORPHISMS BETWEEN MODULE LATTICES Patrick F. Smith 1. Introduction in This Paper We Continue the Discussion In
International Electronic Journal of Algebra Volume 16 (2014) 16-31 COMPLETE HOMOMORPHISMS BETWEEN MODULE LATTICES Patrick F. Smith Received: 18 October 2013; Revised: 25 May 2014 Communicated by Christian Lomp For my good friend John Clark on his 70th birthday Abstract. We examine the properties of certain mappings between the lattice L(R) of ideals of a commutative ring R and the lattice L(RM) of submodules of an R-module M, in particular considering when these mappings are com- plete homomorphisms of the lattices. We prove that the mapping λ from L(R) to L(RM) defined by λ(B) = BM for every ideal B of R is a complete ho- momorphism if M is a faithful multiplication module. A ring R is semiperfect (respectively, a finite direct sum of chain rings) if and only if this mapping λ : L(R) !L(RM) is a complete homomorphism for every simple (respec- tively, cyclic) R-module M. A Noetherian ring R is an Artinian principal ideal ring if and only if, for every R-module M, the mapping λ : L(R) !L(RM) is a complete homomorphism. Mathematics Subject Classification 2010: 06B23, 06B10, 16D10, 16D80 Keywords: Lattice of ideals, lattice of submodules, multiplication modules, complete lattice, complete homomorphism 1. Introduction In this paper we continue the discussion in [7] concerning mappings, in particular homomorphisms, between the lattice of ideals of a commutative ring and the lattice of submodules of a module over that ring. A lattice L is called complete provided every non-empty subset S has a least upper bound _S and a greatest lower bound ^S. -
Algebraic Lattices in QFT Renormalization
Algebraic lattices in QFT renormalization Michael Borinsky∗ Institute of Physics, Humboldt University Newton Str. 15, D-12489 Berlin, Germany Abstract The structure of overlapping subdivergences, which appear in the perturbative expan- sions of quantum field theory, is analyzed using algebraic lattice theory. It is shown that for specific QFTs the sets of subdivergences of Feynman diagrams form algebraic lattices. This class of QFTs includes the Standard model. In kinematic renormalization schemes, in which tadpole diagrams vanish, these lattices are semimodular. This implies that the Hopf algebra of Feynman diagrams is graded by the coradical degree or equivalently that every maximal forest has the same length in the scope of BPHZ renormalization. As an application of this framework a formula for the counter terms in zero-dimensional QFT is given together with some examples of the enumeration of primitive or skeleton diagrams. Keywords. quantum field theory, renormalization, Hopf algebra of Feynman diagrams, algebraic lattices, zero-dimensional QFT MSC. 81T18, 81T15, 81T16, 06B99 1 Introduction Calculations of observable quantities in quantum field theory rely almost always on perturbation theory. The integrals in the perturbation expansions can be depicted as Feynman diagrams. Usually these integrals require renormalization to give meaningful results. The renormalization procedure can be performed using the Hopf algebra of Feynman graphs [10], which organizes the classic BPHZ procedure into an algebraic framework. The motivation for this paper was to obtain insights on the coradical filtration of this Hopf algebra and thereby on the structure of the subdivergences of the Feynman diagrams in the perturbation expansion. The perturbative expansions in QFT are divergent series themselves as first pointed out by [12]. -
Pseudocomplemented Semilattices, Boolean Algebras, and Compatible Products1
Journal of Algebra 242, 60᎐91Ž. 2001 doi:10.1006rjabr.2001.8807, available online at http:rrwww.idealibrary.com on Pseudocomplemented Semilattices, Boolean Algebras, and Compatible Products1 Antonio Fernandez´´ Lopez and Marıa ´ Isabel Tocon ´ Barroso View metadata, citationDepartamento and similar papers de Algebra, at core.ac.uk Geometrıa´´ y Topologıa, Facultad de Ciencias, brought to you by CORE Uni¨ersidad de Malaga,´´ 29071 Malaga, Spain provided by Elsevier - Publisher Connector E-mail: [email protected], [email protected] Communicated by Georgia Benkart Received November 19, 1999 DEDICATED TO PROFESSOR J. MARSHALL OSBORN Pseudocomplemented semilattices are studied here from an algebraic point of view, stressing the pivotal role played by the pseudocomplements and the relation- ship between pseudocomplemented semilattices and Boolean algebras. Following the pattern of semiprime ring theory, a notion of Goldie dimension is introduced for complete pseudocomplemented lattices and calculated in terms of maximal uniform elements if they exist in abundance. Products in lattices with 0-element are studied and questions about the existence and uniqueness of compatible products in pseudocomplemented lattices, as well as about the abundance of prime elements in lattices with a compatible product, are discussed. Finally, a Yood decomposition theorem for topological rings is extended to complete pseudocom- plemented lattices. ᮊ 2001 Academic Press Key Words: pseudocomplemented semilattice; Boolean algebra; compatible product. INTRODUCTION A pseudocomplemented semilattice is aŽ. meet semilattice S having a least element 0 and is such that, for each x in S, there exists a largest element x H such that x n x Hs 0. In spite of what the name could suggest, a complemented lattice need not be pseudocomplemented, as is easily seen by considering the lattice of all subspaces of a vector space of dimension greater than one. -
Lattices and the Geometry of Numbers
Lattices and the Geometry of Numbers Lattices and the Geometry of Numbers Sourangshu Ghosha, aUndergraduate Student ,Department of Civil Engineering , Indian Institute of Technology Kharagpur, West Bengal, India 1. ABSTRACT In this paper we discuss about properties of lattices and its application in theoretical and algorithmic number theory. This result of Minkowski regarding the lattices initiated the subject of Geometry of Numbers, which uses geometry to study the properties of algebraic numbers. It has application on various other fields of mathematics especially the study of Diophantine equations, analysis of functional analysis etc. This paper will review all the major developments that have occurred in the field of geometry of numbers. In this paper we shall first give a broad overview of the concept of lattice and then discuss about the geometrical properties it has and its applications. 2. LATTICE Before introducing Minkowski’s theorem we shall first discuss what is a lattice. Definition 1: A lattice 흉 is a subgroup of 푹풏 such that it can be represented as 휏 = 푎1풁 + 푎2풁 + . + 푎푚풁 풏 Here {푎푖} are linearly independent vectors of the space 푹 and 푚 ≤ 푛. Here 풁 is the set of whole numbers. We call these vectors {푎푖} the basis of the lattice. By the definition we can see that a lattice is a subgroup and a free abelian group of rank m, of the vector space 푹풏. The rank and dimension of the lattice is 푚 and 푛 respectively, the lattice will be complete if 푚 = 푛. This definition is not only limited to the vector space 푹풏. -
Lattice Theory
Chapter 1 Lattice theory 1.1 Partial orders 1.1.1 Binary Relations A binary relation R on a set X is a set of pairs of elements of X. That is, R ⊆ X2. We write xRy as a synonym for (x, y) ∈ R and say that R holds at (x, y). We may also view R as a square matrix of 0’s and 1’s, with rows and columns each indexed by elements of X. Then Rxy = 1 just when xRy. The following attributes of a binary relation R in the left column satisfy the corresponding conditions on the right for all x, y, and z. We abbreviate “xRy and yRz” to “xRyRz”. empty ¬(xRy) reflexive xRx irreflexive ¬(xRx) identity xRy ↔ x = y transitive xRyRz → xRz symmetric xRy → yRx antisymmetric xRyRx → x = y clique xRy For any given X, three of these attributes are each satisfied by exactly one binary relation on X, namely empty, identity, and clique, written respectively ∅, 1X , and KX . As sets of pairs these are respectively the empty set, the set of all pairs (x, x), and the set of all pairs (x, y), for x, y ∈ X. As square X × X matrices these are respectively the matrix of all 0’s, the matrix with 1’s on the leading diagonal and 0’s off the diagonal, and the matrix of all 1’s. Each of these attributes holds of R if and only if it holds of its converse R˘, defined by xRy ↔ yRx˘ . This extends to Boolean combinations of these attributes, those formed using “and,” “or,” and “not,” such as “reflexive and either not transitive or antisymmetric”. -
7. Varieties of Lattices
7. Varieties of Lattices Variety is the spice of life. A lattice equation is an expression p ≈ q where p and q are lattice terms. Our intuitive notion of what it means for a lattice L to satisfy p ≈ q (that p(x1,...,xn)= q(x1,...,xn) whenever elements of L are substituted for the variables) is captured by the formal definition: L satisfies p ≈ q if h(p)=h(q) for every homomorphism h : W (X) →L.WesaythatLsatisfies a set Σ of equations if L satisfies every equation in Σ. As long as we are dealing entirely with lattices, there is no loss of generality in replacing p and q by the corresponding elements of FL(X), and in practice it is often more simple and natural to do so (as in Theorem 7.2 below). A variety (or equational class) of lattices is the class of all lattices satisfying some set Σ of lattice equations. You are already familiar with several lattice varieties: (1) the variety T of one-element lattices, satisfying x ≈ y (not very exciting); (2) the variety D of distributive lattices, satisfying x ∧ (y ∨ z) ≈ (x ∧ y) ∨ (x ∧ z); (3) the variety M of modular lattices, satisfying (x∨y)∧(x∨z) ≈ x∨(z∧(x∨y)); (4) the variety L of all lattices, satisfying x ≈ x. If K is any class of lattices, we say that a lattice F is K-freely generated by its subset X if (1) F∈K, (2) X generates F, (3) for every lattice L∈K,everymaph0 :X→Lcan be extended to a homomorphism h : F→L. -
The Lattice of Equational Classes of Ldempotent Semigroups*
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURN.AL OP ALGEBRA 15, 195-224 (1970) The Lattice of Equational Classes of ldempotent Semigroups* J. A. GERHARD Department of Mathematics, The University of Manitoba, Winnipeg, Cnmdn Comnzmicated by D. Rees Received April IO, 1969 The concept of an equational class was introduced by Birkhoff [2] in 1935, and has been discussed by several authors (see for example Tarski [22]). Recently there has been much interest in the subject, and especially in the lattice of equational classes of lattices [l], [8], [I 11, [12], [17]. However, until now the only nontrivial lattice of equational classes to be completely described was the lattice of equational classes of algebras with one unary operation (Jacobs and Schwabauer [IO]). The problem of describing the lattice of equational classes of algebras with a single binary operation, i.e., groupoids. is much more difficult. Kalicki [13] h as shown that there are uncountably many atoms in the lattice of equational classes of groupoids. The lattice of equational classes of semigroups (associative groupoids) is uncountable (Evans [5]) and has been investigated by Kalicki and Scott [14], who listed its countably many atoms. There are only two equational classes of commutative idempotent semi- groups, but the removal of either commutativity or idempotence gives rise to a non-trivial lattice. Partial results have been obtained for the lattice of equa- tional classes of commutative semigroups [19], [20]. In the case of idempotent semigroups it is relatively easy to show that the lattice of equational classes has three atoms, and in fact the sublattice generated by the atoms has been shown by Tamura [21] to be the eight-element Boolean lattice. -
The Lattice of Equational Classes of Commutative Semigroups AUTHOR: Evelyn M
THE LATTICE OF EQUATIONAL CLASSES 01! COMMlJTA'I'IVE SEMIGROUPS THE LATTICE OF EQUATIONAL CLASSES OF COMMUTATIVE SEMIGROUPS by EVELYN M. NELSON, B.Sc •• M.Sc. A Thesis Submitted to the School of Graduate Studies in Partial Fulfilment of the Requirements for the Degree Doctor of Philosophy McMaster University May 1970 DOCTOR OF PHILOSOPHY (1970) McMASTER UNIVERSITY (Mathematics) Hamilton, Ontario. TITLE: The Lattice of Equational Classes of Commutative Semigroups AUTHOR: Evelyn M. Nelson, B. Sc. (McMaster University) M. Sc. (McMaster University) SUPERVISOR: Professor G. Bruns NUMBER OF PAGES: vii, 48 SCOPE AND CONTENTS: CoLunutative semigroup equations are described, and rules of inference for them are given. Then a skeleton sublattice of the lattice of equational classes of commutative semigroups is described, and a partial description is given of the way in which the rest of the lattice hangs on the skeleton. (ii) ACKNOWLEDGEMENTS I would like to express my sincerest appreciation to my supervisor, Dr. Gunter Bruns, for the invaluable guidance and good counsel he has given me throughout my mathematical career, and for his patience and advice during the preparation of this thesis. Thanks are also due to the National Research Council of Canada and to McMaster University for financial support. (iii) TABLE OF CONTENTS INTRODUCTION (v) CHAPTER 1. BASIC CONCEPTS 1 Section 1. Equations and Completeness 1 Section 2. The Free Commutative Semigroups Satisfying 6 ((r), (r + n)) Section 3. Definition of the Invariants D,V,L,U 7 Section 4. Elementary Properties of D,V,LtU 8 CHAPTER 2. THE SKELETON SUBLATTICE CONSISTING OF THE CLASSES 13 0 r,s,n Section 1.