Lattice-Ordered Rings and Function Rings
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On the Lattice Structure of Quantum Logic
BULL. AUSTRAL. MATH. SOC. MOS 8106, *8IOI, 0242 VOL. I (1969), 333-340 On the lattice structure of quantum logic P. D. Finch A weak logical structure is defined as a set of boolean propositional logics in which one can define common operations of negation and implication. The set union of the boolean components of a weak logical structure is a logic of propositions which is an orthocomplemented poset, where orthocomplementation is interpreted as negation and the partial order as implication. It is shown that if one can define on this logic an operation of logical conjunction which has certain plausible properties, then the logic has the structure of an orthomodular lattice. Conversely, if the logic is an orthomodular lattice then the conjunction operation may be defined on it. 1. Introduction The axiomatic development of non-relativistic quantum mechanics leads to a quantum logic which has the structure of an orthomodular poset. Such a structure can be derived from physical considerations in a number of ways, for example, as in Gunson [7], Mackey [77], Piron [72], Varadarajan [73] and Zierler [74]. Mackey [77] has given heuristic arguments indicating that this quantum logic is, in fact, not just a poset but a lattice and that, in particular, it is isomorphic to the lattice of closed subspaces of a separable infinite dimensional Hilbert space. If one assumes that the quantum logic does have the structure of a lattice, and not just that of a poset, it is not difficult to ascertain what sort of further assumptions lead to a "coordinatisation" of the logic as the lattice of closed subspaces of Hilbert space, details will be found in Jauch [8], Piron [72], Varadarajan [73] and Zierler [74], Received 13 May 1969. -
Mathematics 144 Set Theory Fall 2012 Version
MATHEMATICS 144 SET THEORY FALL 2012 VERSION Table of Contents I. General considerations.……………………………………………………………………………………………………….1 1. Overview of the course…………………………………………………………………………………………………1 2. Historical background and motivation………………………………………………………….………………4 3. Selected problems………………………………………………………………………………………………………13 I I. Basic concepts. ………………………………………………………………………………………………………………….15 1. Topics from logic…………………………………………………………………………………………………………16 2. Notation and first steps………………………………………………………………………………………………26 3. Simple examples…………………………………………………………………………………………………………30 I I I. Constructions in set theory.………………………………………………………………………………..……….34 1. Boolean algebra operations.……………………………………………………………………………………….34 2. Ordered pairs and Cartesian products……………………………………………………………………… ….40 3. Larger constructions………………………………………………………………………………………………..….42 4. A convenient assumption………………………………………………………………………………………… ….45 I V. Relations and functions ……………………………………………………………………………………………….49 1.Binary relations………………………………………………………………………………………………………… ….49 2. Partial and linear orderings……………………………..………………………………………………… ………… 56 3. Functions…………………………………………………………………………………………………………… ….…….. 61 4. Composite and inverse function.…………………………………………………………………………… …….. 70 5. Constructions involving functions ………………………………………………………………………… ……… 77 6. Order types……………………………………………………………………………………………………… …………… 80 i V. Number systems and set theory …………………………………………………………………………………. 84 1. The Natural Numbers and Integers…………………………………………………………………………….83 2. Finite induction -
Lattice-Ordered Loops and Quasigroupsl
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOIJRNALOFALGEBRA 16, 218-226(1970) Lattice-Ordered Loops and Quasigroupsl TREVOREVANS Matkentatics Department, Emory University, Atlanta, Georgia 30322 Communicated by R. H, Brwk Received April 16, 1969 In studying the effect of an order on non-associativesystems such as loops or quasigroups, a natural question to ask is whether some order condition which implies commutativity in the group case implies associativity in the corresponding loop case. For example, a well-known theorem (Birkhoff, [1]) concerning lattice ordered groups statesthat if the descendingchain condition holds for the positive elements,then the 1.0. group is actually a direct product of infinite cyclic groups with its partial order induced in the usual way by the linear order in the factors. It is easy to show (Zelinski, [6]) that a fully- ordered loop satisfying the descendingchain condition on positive elements is actually an infinite cyclic group. In this paper we generalize this result and Birkhoff’s result, by showing that any lattice-ordered loop with descending chain condition on its positive elements is associative. Hence, any 1.0. loop with d.c.c. on its positive elements is a free abelian group. More generally, any lattice-ordered quasigroup in which bounded chains are finite, is isotopic to a free abelian group. These results solve a problem in Birkhoff’s Lattice Theory, 3rd ed. The proof uses only elementary properties of loops and lattices. 1. LATTICE ORDERED LOOPS We will write loops additively with neutral element0. -
Noncommutative Unique Factorization Domainso
NONCOMMUTATIVE UNIQUE FACTORIZATION DOMAINSO BY P. M. COHN 1. Introduction. By a (commutative) unique factorization domain (UFD) one usually understands an integral domain R (with a unit-element) satisfying the following three conditions (cf. e.g. Zariski-Samuel [16]): Al. Every element of R which is neither zero nor a unit is a product of primes. A2. Any two prime factorizations of a given element have the same number of factors. A3. The primes occurring in any factorization of a are completely deter- mined by a, except for their order and for multiplication by units. If R* denotes the semigroup of nonzero elements of R and U is the group of units, then the classes of associated elements form a semigroup R* / U, and A1-3 are equivalent to B. The semigroup R*jU is free commutative. One may generalize the notion of UFD to noncommutative rings by taking either A-l3 or B as starting point. It is obvious how to do this in case B, although the class of rings obtained is rather narrow and does not even include all the commutative UFD's. This is indicated briefly in §7, where examples are also given of noncommutative rings satisfying the definition. However, our principal aim is to give a definition of a noncommutative UFD which includes the commutative case. Here it is better to start from A1-3; in order to find the precise form which such a definition should take we consider the simplest case, that of noncommutative principal ideal domains. For these rings one obtains a unique factorization theorem simply by reinterpreting the Jordan- Holder theorem for right .R-modules on one generator (cf. -
14. Least Upper Bounds in Ordered Rings Recall the Definition of a Commutative Ring with 1 from Lecture 3
14. Least upper bounds in ordered rings Recall the definition of a commutative ring with 1 from lecture 3 (Definition 3.2 ). Definition 14.1. A commutative ring R with unity consists of the following data: a set R, • two maps + : R R R (“addition”), : R R R (“multiplication”), • × −→ · × −→ two special elements 0 R = 0 , 1R = 1 R, 0 = 1 such that • ∈ 6 (1) the addition + is commutative and associative (2) the multiplication is commutative and associative (3) distributive law holds:· a (b + c) = ( a b) + ( a c) for all a, b, c R. (4) 0 is an additive identity. · · · ∈ (5) 1 is a multiplicative identity (6) for all a R there exists an additive inverse ( a) R such that a + ( a) = 0. ∈ − ∈ − Example 14.2. The integers Z, the rationals Q, the reals R, and integers modulo n Zn are all commutative rings with 1. The set M2(R) of 2 2 matrices with the usual matrix addition and multiplication is a noncommutative ring with 1 (where× “1” is the identity matrix). The set 2 Z of even integers with the usual addition and multiplication is a commutative ring without 1. Next we introduce the notion of an integral domain. In fact we have seen integral domains in lecture 3, where they were called “commutative rings without zero divisors” (see Lemma 3.4 ). Definition 14.3. A commutative ring R (with 1) is an integral domain if a b = 0 = a = 0 or b = 0 · ⇒ for all a, b R. (This is equivalent to: a b = a c and a = 0 = b = c.) ∈ · · 6 ⇒ Example 14.4. -
The Structure of Residuated Lattices
The Structure of Residuated Lattices Kevin Blount and Constantine Tsinakis May 23, 2002 Abstract A residuated lattice is an ordered algebraic structure L = hL, ∧, ∨, · , e, \ , / i such that hL, ∧, ∨i is a lattice, hL, ·, ei is a monoid, and \ and / are binary operations for which the equivalences a · b ≤ c ⇐⇒ a ≤ c/b ⇐⇒ b ≤ a\c hold for all a, b, c ∈ L. It is helpful to think of the last two operations as left and right division and thus the equivalences can be seen as “di- viding” on the right by b and “dividing” on the left by a. The class of all residuated lattices is denoted by RL. The study of such objects originated in the context of the theory of ring ideals in the 1930’s. The collection of all two-sided ideals of a ring forms a lattice upon which one can impose a natural monoid structure making this object into a residuated lattice. Such ideas were investi- gated by Morgan Ward and R. P. Dilworth in a series of important papers [15], [16],[45], [46], [47] and [48] and also by Krull in [33]. Since that time, there has been substantial research regarding some specific classes of residuated structures, see for example [1], [9], [26] and [38], but we believe that this is the first time that a general structural the- ory has been established for the class RL as a whole. In particular, we develop the notion of a normal subalgebra and show that RL is an “ideal variety” in the sense that it is an equational class in which con- gruences correspond to “normal” subalgebras in the same way that ring congruences correspond to ring ideals. -
A Note on Embedding a Partially Ordered Ring in a Division Algebra William H
proceedings of the american mathematical society Volume 37, Number 1, January 1973 A NOTE ON EMBEDDING A PARTIALLY ORDERED RING IN A DIVISION ALGEBRA WILLIAM H. REYNOLDS Abstract. If H is a maximal cone of a ring A such that the subring generated by H is a commutative integral domain that satisfies a certain centrality condition in A, then there exist a maxi- mal cone H' in a division ring A' and an order preserving mono- morphism of A into A', where the subring of A' generated by H' is a subfield over which A' is algebraic. Hypotheses are strengthened so that the main theorems of the author's earlier paper hold for maximal cones. The terminology of the author's earlier paper [3] will be used. For a subsemiring H of a ring A, we write H—H for {x—y:x,y e H); this is the subring of A generated by H. We say that H is a u-hemiring of A if H is maximal in the class of all subsemirings of A that do not contain a given element u in the center of A. We call H left central if for every a e A and he H there exists h' e H with ah=h'a. Recall that H is a cone if Hn(—H)={0], and a maximal cone if H is not properly contained in another cone. First note that in [3, Theorem 1] the commutativity of the hemiring, established at the beginning of the proof, was only exploited near the end of the proof and was not used to simplify the earlier details. -
Thermodynamic Properties of Coupled Map Lattices 1 Introduction
Thermodynamic properties of coupled map lattices J´erˆome Losson and Michael C. Mackey Abstract This chapter presents an overview of the literature which deals with appli- cations of models framed as coupled map lattices (CML’s), and some recent results on the spectral properties of the transfer operators induced by various deterministic and stochastic CML’s. These operators (one of which is the well- known Perron-Frobenius operator) govern the temporal evolution of ensemble statistics. As such, they lie at the heart of any thermodynamic description of CML’s, and they provide some interesting insight into the origins of nontrivial collective behavior in these models. 1 Introduction This chapter describes the statistical properties of networks of chaotic, interacting el- ements, whose evolution in time is discrete. Such systems can be profitably modeled by networks of coupled iterative maps, usually referred to as coupled map lattices (CML’s for short). The description of CML’s has been the subject of intense scrutiny in the past decade, and most (though by no means all) investigations have been pri- marily numerical rather than analytical. Investigators have often been concerned with the statistical properties of CML’s, because a deterministic description of the motion of all the individual elements of the lattice is either out of reach or uninteresting, un- less the behavior can somehow be described with a few degrees of freedom. However there is still no consistent framework, analogous to equilibrium statistical mechanics, within which one can describe the probabilistic properties of CML’s possessing a large but finite number of elements. -
Algorithmic Semi-Algebraic Geometry and Topology – Recent Progress and Open Problems
Contemporary Mathematics Algorithmic Semi-algebraic Geometry and Topology – Recent Progress and Open Problems Saugata Basu Abstract. We give a survey of algorithms for computing topological invari- ants of semi-algebraic sets with special emphasis on the more recent devel- opments in designing algorithms for computing the Betti numbers of semi- algebraic sets. Aside from describing these results, we discuss briefly the back- ground as well as the importance of these problems, and also describe the main tools from algorithmic semi-algebraic geometry, as well as algebraic topology, which make these advances possible. We end with a list of open problems. Contents 1. Introduction 1 2. Semi-algebraic Geometry: Background 3 3. Recent Algorithmic Results 10 4. Algorithmic Preliminaries 12 5. Topological Preliminaries 22 6. Algorithms for Computing the First Few Betti Numbers 41 7. The Quadratic Case 53 8. Betti Numbers of Arrangements 66 9. Open Problems 69 Acknowledgment 71 References 71 1. Introduction This article has several goals. The primary goal is to provide the reader with a thorough survey of the current state of knowledge on efficient algorithms for computing topological invariants of semi-algebraic sets – and in particular their Key words and phrases. Semi-algebraic Sets, Betti Numbers, Arrangements, Algorithms, Complexity . The author was supported in part by NSF grant CCF-0634907. Part of this work was done while the author was visiting the Institute of Mathematics and its Applications, Minneapolis. 2000 Mathematics Subject Classification Primary 14P10, 14P25; Secondary 68W30 c 0000 (copyright holder) 1 2 SAUGATA BASU Betti numbers. At the same time we want to provide graduate students who intend to pursue research in the area of algorithmic semi-algebraic geometry, a primer on the main technical tools used in the recent developments in this area, so that they can start to use these themselves in their own work. -
Embedding Two Ordered Rings in One Ordered Ring. Part I1
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 2, 341-364 (1966) Embedding Two Ordered Rings in One Ordered Ring. Part I1 J. R. ISBELL Department of Mathematics, Case Institute of Technology, Cleveland, Ohio Communicated by R. H. Bruck Received July 8, 1965 INTRODUCTION Two (totally) ordered rings will be called compatible if there exists an ordered ring in which both of them can be embedded. This paper concerns characterizations of the ordered rings compatible with a given ordered division ring K. Compatibility with K is equivalent to compatibility with the center of K; the proof of this depends heavily on Neumann’s theorem [S] that every ordered division ring is compatible with the real numbers. Moreover, only the subfield K, of real algebraic numbers in the center of K matters. For each Ks , the compatible ordered rings are characterized by a set of elementary conditions which can be expressed as polynomial identities in terms of ring and lattice operations. A finite set of identities, or even iden- tities in a finite number of variables, do not suffice, even in the commutative case. Explicit rules will be given for writing out identities which are necessary and sufficient for a commutative ordered ring E to be compatible with a given K (i.e., with K,). Probably the methods of this paper suffice for deriving corresponding rules for noncommutative E, but only the case K,, = Q is done here. If E is compatible with K,, , then E is embeddable in an ordered algebra over Ks and (obviously) E is compatible with the rational field Q. -
Pacific Journal of Mathematics Vol. 281 (2016)
Pacific Journal of Mathematics Volume 281 No. 2 April 2016 PACIFIC JOURNAL OF MATHEMATICS msp.org/pjm Founded in 1951 by E. F. Beckenbach (1906–1982) and F. Wolf (1904–1989) EDITORS Don Blasius (Managing Editor) Department of Mathematics University of California Los Angeles, CA 90095-1555 [email protected] Paul Balmer Vyjayanthi Chari Daryl Cooper Department of Mathematics Department of Mathematics Department of Mathematics University of California University of California University of California Los Angeles, CA 90095-1555 Riverside, CA 92521-0135 Santa Barbara, CA 93106-3080 [email protected] [email protected] [email protected] Robert Finn Kefeng Liu Jiang-Hua Lu Department of Mathematics Department of Mathematics Department of Mathematics Stanford University University of California The University of Hong Kong Stanford, CA 94305-2125 Los Angeles, CA 90095-1555 Pokfulam Rd., Hong Kong fi[email protected] [email protected] [email protected] Sorin Popa Jie Qing Paul Yang Department of Mathematics Department of Mathematics Department of Mathematics University of California University of California Princeton University Los Angeles, CA 90095-1555 Santa Cruz, CA 95064 Princeton NJ 08544-1000 [email protected] [email protected] [email protected] PRODUCTION Silvio Levy, Scientific Editor, [email protected] SUPPORTING INSTITUTIONS ACADEMIA SINICA, TAIPEI STANFORD UNIVERSITY UNIV. OF CALIF., SANTA CRUZ CALIFORNIA INST. OF TECHNOLOGY UNIV. OF BRITISH COLUMBIA UNIV. OF MONTANA INST. DE MATEMÁTICA PURA E APLICADA UNIV. OF CALIFORNIA, BERKELEY UNIV. OF OREGON KEIO UNIVERSITY UNIV. OF CALIFORNIA, DAVIS UNIV. OF SOUTHERN CALIFORNIA MATH. SCIENCES RESEARCH INSTITUTE UNIV. OF CALIFORNIA, LOS ANGELES UNIV. -
Cayley's and Holland's Theorems for Idempotent Semirings and Their
Cayley's and Holland's Theorems for Idempotent Semirings and Their Applications to Residuated Lattices Nikolaos Galatos Department of Mathematics University of Denver [email protected] Rostislav Horˇc´ık Institute of Computer Sciences Academy of Sciences of the Czech Republic [email protected] Abstract We extend Cayley's and Holland's representation theorems to idempotent semirings and residuated lattices, and provide both functional and relational versions. Our analysis allows for extensions of the results to situations where conditions are imposed on the order relation of the representing structures. Moreover, we give a new proof of the finite embeddability property for the variety of integral residuated lattices and many of its subvarieties. 1 Introduction Cayley's theorem states that every group can be embedded in the (symmetric) group of permutations on a set. Likewise, every monoid can be embedded into the (transformation) monoid of self-maps on a set. C. Holland [10] showed that every lattice-ordered group can be embedded into the lattice-ordered group of order-preserving permutations on a totally-ordered set. Recall that a lattice-ordered group (`-group) is a structure G = hG; _; ^; ·;−1 ; 1i, where hG; ·;−1 ; 1i is group and hG; _; ^i is a lattice, such that multiplication preserves the order (equivalently, it distributes over joins and/or meets). An analogous representation was proved also for distributive lattice-ordered monoids in [2, 11]. We will prove similar theorems for resid- uated lattices and idempotent semirings in Sections 2 and 3. Section 4 focuses on the finite embeddability property (FEP) for various classes of idempotent semirings and residuated lat- tices.