Lattices in a Gamma Semiring

Total Page:16

File Type:pdf, Size:1020Kb

Lattices in a Gamma Semiring www.ijcrt.org © 2020 IJCRT | Volume 8, Issue 11 November 2020 | ISSN: 2320-2882 LATTICES IN A GAMMA SEMIRING TILAK RAJ SHARMA Department of Mathematics, Himachal Pradesh University, Regional Centre, Khaniyara, Dharamshala, Himachal Pradesh (India)-176218 Abstract: - In this paper, the efforts are made to characterize some results on lattices of Γ −semirings. Since a complemented element plays an important role in the study of lattices, so we give characterization of some results on lattices, which are analogous to the corresponding results in semirings [2-3]. Keywords: Γ −semiring, simple, additive idempotent and multiplicative Γ −idempotent Γ − semiring, Complemented elements in a Γ − semiring, Lattices. 1. INTRODUCTION From an algebraic point of view, semirings provide the most natural common generalization of the theories of rings and most of the techniques used in analyzing semirings are taken from ring theory and group theory. The set of nonnegative integers ℕ with usual addition and multiplication provides a natural example of a semiring. There are many other examples of semiring such as the positive cone of a totally ordered ring. For a given positive integer 푛, the set of all 푛 × 푛 matrices over a semiring R forms a semiring with usual matrix addition and multiplication over R. But the situations for the set of all non-positive integers and for the set of all 푚 × 푛 matrices over a semiring R are different. They do not form semirings with the above operations, because multiplication in the above sense are no longer binary compositions. This notion provides a new kind of algebraic structure what is known as a Γ − semiring. The concept of Γ −semiring was introduced by M. M. K. Rao in 1995 [6] as a generalization of semiring as well as Γ − ring (it may be recalled here that the notion of “Γ” was first introduced in algebra by N. Nobusawa in 1964). Later it was found that Γ − semiring also provides an algebraic home to the negative cones of totally ordered rings and the sets of rectangular matrices over a semiring. For further study of semirings, Γ −semirings and their generalization, one may referred to [2-3][4-10]. IJCRT2011400 International Journal of Creative Research Thoughts (IJCRT) www.ijcrt.org 3360 www.ijcrt.org © 2020 IJCRT | Volume 8, Issue 11 November 2020 | ISSN: 2320-2882 In this paper, the efforts are made to characterize some results on lattices of Γ − semirings. Furthermore, since a complemented element plays an important role in the study of lattices, so we give characterization of some results on lattices, which are analogous to the corresponding results in semirings [2- 3]. Finally, we define harmony difference of elements of Γ푅⊥(set of all complemented elements) and proved that if d ∶ 훤푅⊥ × 훤푅⊥ → 훤푅⊥ be defined by d ∶ (x, y) → 푥∇y. Then d is metric on 훤푅⊥ with values in R. 2. PRELIMINARIES The following definitions with examples and results are felt to be an inseparable part of this paper. Definition 2.1: Let 푅 and be two additive commutative semigroups. Then 푅 is called a Γ − semiring if there exists a mapping 푅 × × 푅 → 푅 denoted by 푥훼푦 for all 푥, 푦 ∈ 푅 and 훼 ∈ satistifying the following conditions: (i) 푥훼(푦 + 푧) = (푥훼푦) + (푥훼푧). (ii) (푦 + 푧)훼푥 = (푦훼푥) + (푧훼푥). (iii) 푥 (훼 + 훽)푧 = (푥훼푧) + (푥훽푧). (iv) 푥훼(푦훽푧) = (푥훼푦)훽푧 for all 푥, 푦, 푧 ∈ 푅 and 훼, 훽 ∈ Γ. Definition 2.3: A Γ − semiring 푅 is said to have a zero element if 0훾푥 = 0 = 푥훾0 and 푥 + 0 = 푥 = 0 + 푥 for all 푥 ∈ 푅 and 훾 ∈ Γ. Definition 2.4: A non-empty subset 푇 of a Γ − semiring 푅 is said to be a sub Γ − semiring of 푅 if (푇, +) is a subsemigroup of (푅, +) and 푥훾푦 ∈ 푇 for all 푥, 푦 ∈ 푇 and 훾 ∈ Γ. Definition 2.5: A Γ − semiring is said to have identity element if 푥훾1 = 푥 = 1훾푥 for all 푥 ∈ 푅 and ∈ Γ . Definition 2.6: A Γ − semiring 푅 is said to be a commutative if 푥훾푦 = 푦훾푥 for all 푥, 푦 ∈ 푅 and 훾 ∈ Γ . Example 2.7: Let 푅 be the set of all even positive integers and Γ be set of all positive integers divisible by 3. Then with usual addition and multiplication of integers, 푅 is a commutative Γ − semiring. Definition 2.8: An element 푥 of a Γ −semiring 푅 is said to be additive idempotent if and only if 푥 + 푥 = 푥. If every element of 푅 is additive idempotent then 푅 is called additive idempotent Γ − semiring. It is denoted by 퐼+(Γ푅). Definition 2.9: An element 푥 of a Γ − semiring 푅 is said to be multiplicative Γ −idempotent if there exists 훾 ∈ Γ such that 푥 = 푥 훾푥. If every element of 푅 is multiplicative Γ − idempotent then 푅 is called multiplicative Γ − idempotent Γ − semiring. It is denoted by 퐼×(Γ푅). Definition 2.10: A Γ − semiring 푅 is said to be Γ − idempotent if it is both additive idempotent and multiplicative Γ − idempotent. We will denote the set of all Γ −idempotent elements of a Γ −semiring 푅 by 퐼(ΓR). Definition 2.11: A Γ − semiring 푅 with identity is simple if and only if 푥 + 1 = 1 = 1 + 푥 for all 푥 ∈ 푅. Definition 2.12: A Γ − semiring 푅 is centreless if and only if 푥 + 푦 = 0 implies that 푥 = 푦 = 0. IJCRT2011400 International Journal of Creative Research Thoughts (IJCRT) www.ijcrt.org 3361 www.ijcrt.org © 2020 IJCRT | Volume 8, Issue 11 November 2020 | ISSN: 2320-2882 Example 2.13: Let 푅 = ℤ+ be a set of non negative integers and Γ = {1}. Define a mapping 푅 × × 푅 → 푅 by 푥1푦 = 푥푦 for all 푥, 푦 ∈ 푅. Then 푅 is a centreless Γ −semiring.. Definition 2.14: The Centre of a Γ − semiring 푅 is a subset of 푅 consisting of all elements x of 푅 such that 푥훾푦 = 푦훾푥 for all 푦 ∈ 푅 and 훾 ∈ Γ. It is denoted by 퐶(푅). Definition 2.15: Let 푥, 푦 be elements of a Γ − semiring 푅, then 푥 is 횪 − interior 푦 denoted by 풙훁퐲 if and only if there exists an element 푧 휖 푅 such that 푥훾푧 = 푧훾푥 = 0 and 푧 + 푦 = 1 푓표푟 푎푙푙 훾 ∈ Γ. Definition 2.16: An element 푥 is complemented if and only if 푥∇x. That is, there exists an element 푦 ∈ 푅 such that 푥훾푦 = 푦훾푥 = 0 and 푥 + 푦 = 1, 푓표푟 푎푙푙 훾 ∈ Γ. This element 푦 of 푅 is the complement of 푥 in 푅. We will denote complement of 푥 by 푥⊥. Clearly if 푥 is complemented then so is 푥⊥ and 푥⊥⊥ = 푥 . Lemma 2.17[9]: Let 푅 be a Γ − semiring. Then (i) 푅 is simple if and only if 푥 = 푥 + 푥훾푦 for all 푥, 푦 ∈ 푅 and 훾 ∈ Γ. (ii) 푅 is simple if and only if 푥 = 푥 + 푦훾푥 for all 푥, 푦 ∈ 푅 and 훾 ∈ Γ. (iii) 푅 is simple if and only if 푥훾푦 = 푥훾푦 + (푥훽푧)훾푦 for all 푥, 푦, 푧 ∈ 푅 and 훽, 훾 ∈ Γ. Theorem 2.18[9]: Let 푅 be a Γ − semiring. Then every additive idempotent Γ − semiring has a simple sub Γ − semiring. Let us denote the set of all complemented elements of 푹 by 횪푹⊥. Clearly Γ푅⊥ ≠ 휙, since 0⊥=1. Indeed, if 푥 ∈ Γ푅⊥, 훾 ∈ Γ. Then 푥 + 푥⊥ = 1, 푥훾푥⊥ = 푥⊥훾푥 = 0 , for all 훾 ∈ Γ. Therefore 푥 = 푥훾1 = 푥훾(푥 + 푥⊥) = 푥훾푥 + 푥훾푥⊥ = 푥훾푥. Thus Γ푅⊥ is multiplicative Γ − idempotent, that is, Γ푅⊥ ⊆ 퐼×(Γ푅). Again let 푥 ∈ Γ푅⊥ 푎푛푑 훾 ∈ Γ. Set 푥 ⊛ 푦 = 푥 + 푥⊥훾푦, for all ∈ Γ . Then 푥 ⊛ 푥⊥ = 푥 + 푥⊥훾푥⊥ = 푥 + 푥⊥ = 1 for all 푥 ∈ Γ푅⊥. Also, if 푥 + 푦 = 1 then 푥⊥ = 푥⊥훾1 = 푥⊥훾(푥 + 푦) = 푥⊥훾푥 + 푥⊥훾푦 = 푥⊥훾푦. Thus 푥 ⊛ 푦 = 푥 + 푥⊥훾푦 = 푥 + 푥⊥ = 1. Lemma 2.19[10]: Let 푅 be a Γ − semiring such that 푥, 푦 ∈ Γ푅⊥. Then x훾푦, 푥 ⊛ 푦 ∈ Γ푅⊥. Lemma 2.20[10]: Let 푅 be a Γ − semiring and 푥, 푦 ∈ Γ푅⊥. Then 푥훾푦 = 푦훾푥, 푓표푟 푎푙푙 훾 ∈ Γ. Lemma 2.21[10]: Let 푅 be a centreless Γ − semiring. If 푥, 푦 ∈ Γ푅⊥ and β, 훾 ∈ Γ. Then (푥훾푦)훽푥⊥ = (푥⊥훾푦)훽푥 = 0. Theorem 2.22[10]: Let 푅 be a centreless Γ − semiring. Then Γ푅⊥ is Γ − idempotent, commutative, simple Γ − semiring with the mapping ⊛ : Γ푅⊥ × Γ × Γ푅⊥ → Γ푅⊥ defined by 푥 ∗ 훾 ∗ 푦 = 푥훾푦, for all 푥, 푦 ∈ Γ푅⊥, 훾 ∈ Γ. Proposition 2.23[10] Let 푅 be a centreless Γ −semiring. Then Γ푅⊥is a sub Γ −semiring of 푅 if and only if 푥 + 푦, 푥훾푦 ∈ Γ푅⊥, 푥, 푦 ∈ Γ푅⊥. Remark 2.24: Throughout this paper, 푅 will denote a Γ − semiring with zero element ′ퟎ′ and identity element ′ퟏ′ unless otherwise stated. IJCRT2011400 International Journal of Creative Research Thoughts (IJCRT) www.ijcrt.org 3362 www.ijcrt.org © 2020 IJCRT | Volume 8, Issue 11 November 2020 | ISSN: 2320-2882 3. LATTICES IN A GAMMA SEMIRING Complemented elements play an important role in study of lattices. Another major source of inspiration for the theory of Γ − semirings is lattice theory. Definition 3.1: Let 푎 and 푏 be two elements in a partially ordered set (퐴, ≤). An element 푐 is said to be an upper bound of 푎 and 푏 if 푎 ≤ 푐 and 푏 ≤ 푐, and an element 푐 is said to be a least upper bound of 푎 and 푏 if 푐 is an upper bound of 푎 and 푏, and there is no other upper bound 푑 of 푎 and 푏 such that 푑 ≤ 푐.
Recommended publications
  • 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).
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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].
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Smarandache Lattice and Pseudo Complement
    International J.Math. Combin. Vol.4(2014), 120-126 Smarandache Lattice and Pseudo Complement N.Kannappa (Mathematics Department, TBML College, Porayar, Tamil Nadu, India) K.Suresh (Department of Mathematics, Mailam Engineering College, Vilupuram,Tamil Nadu, India) E-mail: [email protected], [email protected] Abstract: In this paper, we introduce Smarandache - 2-algebraic structure of lattice S, namely Smarandache lattices. A Smarandache 2-algebraic structure on a set N means a weak algebraic structure A0 on N such that there exists a proper subset M of N which is embedded with a stronger algebraic structure A1, where a stronger algebraic structure means such a structure which satisfies more axioms, by proper subset one can understands a subset different from the empty set, by the unit element if any, and from the whole set. We obtain some of its characterization through pseudo complemented. Key Words: Lattice, Boolean algebra, Smarandache lattice and Pseudo complemented lattice. AMS(2010): 53C78 §1. Introduction New notions are introduced in algebra to study more about the congruence in number theory by Florentin Smarandache [1]. By <proper subset> of a set A, we consider a set P included in A, different from A, also different from the empty set and from the unit element in A - if any they rank the algebraic structures using an order relationship. The algebraic structures S S if both of them are defined on the same set; all S 1 ≪ 2 1 laws are also S2 laws; all axioms of S1 law are accomplished by the corresponding S2 law; S2 law strictly accomplishes more axioms than S1 laws, or in other words S2 laws has more laws than S .
    [Show full text]
  • L−Fuzzy Ideals in Γ−Semiring
    Annals of Fuzzy Mathematics and Informatics Volume 8, No. x, (mm 2015), pp. 1–xx @FMI ISSN: 2093–9310 (print version) c Kyung Moon Sa Co. ISSN: 2287–6235 (electronic version) http://www.kyungmoon.com http://www.afmi.or.kr L−fuzzy ideals in Γ−semiring M. Murali Krishna Rao and B. Vekateswarlu Received 14 December 2014; Revised 19 January 2015; Accepted 22 January 2015 Abstract. We introduce the notion of a L−fuzzy Γ−subsemiring, L−fuzzy ideal, normal L−fuzzy ideal, L−fuzzy k ideal, L−fuzzy maximal ideal in Γ−semiring, where L is a complemented distributive lattice and study some of their properties. We prove that if µ is a maximal L− fuzzy ideal of Γ−semiring M then Mµ is a maximal ideal of Γ−semiring M. 2010 AMS Classification: 16Y60, 03E72. Keywords: Γ−semiring, L−fuzzy ideal, L−fuzzy k ideal, L − k fuzzy ideal, L−fuzzy maximal ideal. 1. INTRODUCTION The notion of a semiring was first introduced by H. S. Vandiver [16] in 1934 but semirings had appeared in studies on the theory of ideals of rings. In structure, semirings lie between semigroups and rings. The results which hold in rings but not in semigroups hold in semirings since semiring is a generalization of ring. The study of rings shows that multiplicative structure of ring is an independent of additive structure whereas in semiring multiplicative structure of semiring is not an indepen- dent of additive structure of semiring. The additive and the multiplicative structure of a semiring play an important role in determining the structure of a semiring.
    [Show full text]
  • C. C. Chen and G. Grätzer, on the Construction of Complemented
    Reprinted from JOURNAL OF AWE8RA Vol. II, No, 1, January 1969 All Rights Reserved by Academic Pres., New York and London Printed in Belgium On the Construction of Complemented lattices C. C. CHEN AND G. GRATZER* Department of Mathematics, The University of Manitoba, Winnipeg, Canada Department of Mathematics, Nanyang Umversity, Singapore Communicated by Saunders MacLane Received Dec. 3, 1967 1. INTRODUCTION R. P. Dilworth's classical resultl that every lattice can be embedded in a uniquely complemented lattice is well known but the proof itself is in­ accessible to the general reader. The reason for this is a simple one: the proof is too specialized, in the sense that a difficult machinery has to be developed for which no other application has been found. We suggest that all the deeper results developed by Dilworth can be avoided. As the first step of the proof let us observe that it suffices to show that an at most uniquely complemented lattice L o can be embedded in a lattice lv[ of the same type in such a way that 0 and 1 are preserved and such that each element of Lo has a complement in M. The second step consists in applying a method of Dilworth (Theorem 2.2. of UC) for the description of the free lattice L generated by a partially ordered set obtained from Lo by adjoining an unordered set S. Finally, if S is in one-to-one correspondence with the non-complemented elements ofL o , then the method of singular elements used in the final step of Dilworth's proof can be applied directly to yield a subset M ofL, which is a lattice and which has the properties required in the first step.
    [Show full text]
  • G. Grätzer and J. Sichler, on the Endomorphism Semigroup
    PACIFIC JOURNAL OF MATHEMATICS Vol. 35, No.3, 1970 ON THE ENDOMORPHISM SEMIGROUP (AND CATEGORY) OF BOUNDED LATTICES G. GRATZER AND J. SICHLER Recently, a large number of papers have been published on the representations of a semigroup with identity (Le" a monoid) as the endomorphism semigroup of algebras and reo lational systems of various kinds. For instance Z. Redrlin and J. Lambek showed that every monoid can be represented as the endomorphism semigroup of a semigroup. Conspicuously missing from the list of algebras for which theorems of this type can be proved are lattices. The reason for this is that any constant map is a lattice endomorphism, and therefore endomorphism semigroups of lattices are very special. For partially ordered sets one can eliminate constant maps as endomorphisms by considering only those maps ep that satisfy x < y implies xep < yep (Z. Redrlin and R. H. McDowell); however, this would not be a very natural condi­ tion to impose on lattice endomorphisms. The approach of this paper! is to consider bounded lattices only, that is, lattices with smallest element 0 and largest element 1, and as endomorphisms to admit only those lattice endomorphisms that preserve 0 and 1 (Le., keep 0 and 1 fixed; this amounts to considering 0 and 1 as nullary operations). Such endomorphisms are usually called {O, 1}-endomorphisms but they are called simply endomorphisms in this paper. The first result is that every monoid is isomorphic to the monoid of all endomorphisms of a bounded lattice. One can also consider lattices with complementation <L; /\, V, I), where' is a complementation, that is, for every a E L, a /\ a' = 0 and a V a' = 1.
    [Show full text]
  • Complemented 'Lattices
    COMPLEMENTED 'LATTICES By KENNETH L. PERRIN pi' Bachelor of Science Harding College Searcy, Arkansas 1955 Master of Science Kansas State University Manhattan, Kansas 1957 Submitted to the faculty of the Graduate College of the Oklahoma State University in partial fulfillment of the requirements for the degree of DOCTOR OF EDUCATION July, 1967 CCMPLEMENTED LATTICES Thesis Approved: Thesis Adviser ~ Jv~!(I ~ £LP Dean of the Graduate College ii OKLAHOMA STATE UNIVERSITY LIBRARY JAN 16 1968 ACKNOWLEDGMENTS I am indebted to the administration of Harding College for their confidence in me, and for their generous financial support during my two years at Oklahoma State University, It is, also, a pleasure to acknowledge my gratitude to Dr. R, B, Deal for his wise counsel, especially in the planning stages of this thesis, and to the rest of my advisory com.mittee -- Professors Milton· Berg, Vernon Troxel, and John E. Susky. Special thanks go to my wife, Libby, for her tremendous help in connection with this paper. iii Ci59715 TABLE OF CONTENTS Chapter Page I. INTRODUCTION, 1 II. BASIC DEFINITIONS AND EXAMPLES 4 Partially Ordered Sets 4 Diagrams •.. , ... 5 Lattices , , •...• 7 An Alternate Definition. 10 Lattices With First and Last Elements. 15 Properties of Lattices in General •• 21 Modular and Distributive Lattices ..• 22 III. RELATIONSHIPS BETWEEN DIFFERENT TYPES OF LATTICES 32 Venn Diagrams of Lattices. 32 Complete Lattices, 37 IV. COMPLEMENTED LATTICES, 45 Relatively Complemented Lattices. 45 A Modularity Condition . • 50 Lattices With Unique Complements . 51 V. SUMMARY AND EDUCATIONAL IMPLICATIONS 56 Sunnnary. • . , • . 56 Educational Implications . • 57 BIBLIOGRAPHY. , , 59 APPENDIX: INDEX , , 60 iv CHAPTER I INTRODUCTION Until about thirty years ago the area of algebra now called lattice theory was v:i..rtually unknowno Since that time it has emerged as an important area of mathematical study, and rapid progress has marked its development.
    [Show full text]
  • A Sauer–Shelah–Perles Lemma for Lattices
    A Sauer{Shelah{Perles Lemma for Lattices Stijn Cambie∗ Bogdan Chornomaz Department of Mathematics Department of Mathematics Radboud University Vanderbilt University Nijmegen, The Netherlands Nashville, Tennessee, U.S.A. [email protected] [email protected] Zeev Dviry Yuval Filmusz Department of Computer Science Taub Faculty of Computer Science Department of Mathematics Technion | Israel Institute of Technology Princeton University Haifa, Israel Princeton, New Jersey, U.S.A. [email protected] [email protected] Shay Moranx Faculty of Mathematics Technion | Israel Institute of Technology Haifa, Israel [email protected] Submitted: Jan 8, 2020; Accepted: Oct 19, 2020; Published: Oct 30, 2020 c The authors. Released under the CC BY-ND license (International 4.0). Abstract We study lattice-theoretical extensions of the celebrated Sauer{Shelah{Perles Lemma. We conjecture that a general Sauer{Shelah{Perles Lemma holds for a lattice if and only if the lattice is relatively complemented, and prove partial results towards this conjecture. Mathematics Subject Classifications: 06B99, 68Q32 ∗Research supported by a Vidi Grant of the Netherlands Organization for Scientific Research (NWO), grant number 639:032:614. yResearch supported by NSF CAREER award DMS-1451191 and NSF grant CCF-1523816. Work on this paper was done while the author was a Von-Neumann fellow at the Institute for Advanced Study, supported by a Simons foundation fellowship. zTaub Fellow | supported by the Taub Foundations. The research was funded by ISF grant 1337/16. xResearch supported by the Israel Science Foundation (grant No. 1225/20), by an Azrieli Faculty Fellowship, and by a grant from the United States | Israel Binational Science Foundation (BSF).
    [Show full text]