From Semirings to Residuated Kleene Lattices
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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. -
ON F-DERIVATIONS from SEMILATTICES to LATTICES
Commun. Korean Math. Soc. 29 (2014), No. 1, pp. 27–36 http://dx.doi.org/10.4134/CKMS.2014.29.1.027 ON f-DERIVATIONS FROM SEMILATTICES TO LATTICES Yong Ho Yon and Kyung Ho Kim Abstract. In this paper, we introduce the notion of f-derivations from a semilattice S to a lattice L, as a generalization of derivation and f- derivation of lattices. Also, we define the simple f-derivation from S to L, and research the properties of them and the conditions for a lattice L to be distributive. Finally, we prove that a distributive lattice L is isomorphic to the class SDf (S,L) of all simple f-derivations on S to L for every ∧-homomorphism f : S → L such that f(x0) ∨ f(y0) = 1 for ∼ some x0,y0 ∈ S, in particular, L = SDf (S,L) for every ∧-homomorphism f : S → L such that f(x0) = 1 for some x0 ∈ S. 1. Introduction In some of the literature, authors investigated the relationship between the notion of modularity or distributivity and the special operators on lattices such as derivations, multipliers and linear maps. The notion and some properties of derivations on lattices were introduced in [10, 11]. Sz´asz ([10, 11]) characterized the distributive lattices by multipliers and derivations: a lattice is distributive if and only if the set of all meet- multipliers and of all derivations coincide. In [5] it was shown that every derivation on a lattice is a multiplier and every multiplier is a dual closure. Pataki and Sz´az ([9]) gave a connection between non-expansive multipliers and quasi-interior operators. -
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. -
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. -
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. -
Semilattice Sums of Algebras and Mal'tsev Products of Varieties
Mathematics Publications Mathematics 5-20-2020 Semilattice sums of algebras and Mal’tsev products of varieties Clifford Bergman Iowa State University, [email protected] T. Penza Warsaw University of Technology A. B. Romanowska Warsaw University of Technology Follow this and additional works at: https://lib.dr.iastate.edu/math_pubs Part of the Algebra Commons The complete bibliographic information for this item can be found at https://lib.dr.iastate.edu/ math_pubs/215. For information on how to cite this item, please visit http://lib.dr.iastate.edu/ howtocite.html. This Article is brought to you for free and open access by the Mathematics at Iowa State University Digital Repository. It has been accepted for inclusion in Mathematics Publications by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. Semilattice sums of algebras and Mal’tsev products of varieties Abstract The Mal’tsev product of two varieties of similar algebras is always a quasivariety. We consider when this quasivariety is a variety. The main result shows that if V is a strongly irregular variety with no nullary operations, and S is a variety, of the same type as V, equivalent to the variety of semilattices, then the Mal’tsev product V ◦ S is a variety. It consists precisely of semilattice sums of algebras in V. We derive an equational basis for the product from an equational basis for V. However, if V is a regular variety, then the Mal’tsev product may not be a variety. We discuss examples of various applications of the main result, and examine some detailed representations of algebras in V ◦ S. -
Steps in the Representation of Concept Lattices and Median Graphs Alain Gély, Miguel Couceiro, Laurent Miclet, Amedeo Napoli
Steps in the Representation of Concept Lattices and Median Graphs Alain Gély, Miguel Couceiro, Laurent Miclet, Amedeo Napoli To cite this version: Alain Gély, Miguel Couceiro, Laurent Miclet, Amedeo Napoli. Steps in the Representation of Concept Lattices and Median Graphs. CLA 2020 - 15th International Conference on Concept Lattices and Their Applications, Sadok Ben Yahia; Francisco José Valverde Albacete; Martin Trnecka, Jun 2020, Tallinn, Estonia. pp.1-11. hal-02912312 HAL Id: hal-02912312 https://hal.inria.fr/hal-02912312 Submitted on 5 Aug 2020 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. Steps in the Representation of Concept Lattices and Median Graphs Alain Gély1, Miguel Couceiro2, Laurent Miclet3, and Amedeo Napoli2 1 Université de Lorraine, CNRS, LORIA, F-57000 Metz, France 2 Université de Lorraine, CNRS, Inria, LORIA, F-54000 Nancy, France 3 Univ Rennes, CNRS, IRISA, Rue de Kérampont, 22300 Lannion, France {alain.gely,miguel.couceiro,amedeo.napoli}@loria.fr Abstract. Median semilattices have been shown to be useful for deal- ing with phylogenetic classication problems since they subsume me- dian graphs, distributive lattices as well as other tree based classica- tion structures. Median semilattices can be thought of as distributive _-semilattices that satisfy the following property (TRI): for every triple x; y; z, if x ^ y, y ^ z and x ^ z exist, then x ^ y ^ z also exists. -
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. -
LATTICE THEORY of CONSENSUS (AGGREGATION) an Overview
Workshop Judgement Aggregation and Voting September 9-11, 2011, Freudenstadt-Lauterbad 1 LATTICE THEORY of CONSENSUS (AGGREGATION) An overview Bernard Monjardet CES, Université Paris I Panthéon Sorbonne & CAMS, EHESS Workshop Judgement Aggregation and Voting September 9-11, 2011, Freudenstadt-Lauterbad 2 First a little precision In their kind invitation letter, Klaus and Clemens wrote "Like others in the judgment aggregation community, we are aware of the existence of a sizeable amount of work of you and other – mainly French – authors on generalized aggregation models". Indeed, there is a sizeable amount of work and I will only present some main directions and some main results. Now here a list of the main contributors: Workshop Judgement Aggregation and Voting September 9-11, 2011, Freudenstadt-Lauterbad 3 Bandelt H.J. Germany Barbut, M. France Barthélemy, J.P. France Crown, G.D., USA Day W.H.E. Canada Janowitz, M.F. USA Mulder H.M. Germany Powers, R.C. USA Leclerc, B. France Monjardet, B. France McMorris F.R. USA Neumann, D.A. USA Norton Jr. V.T USA Powers, R.C. USA Roberts F.S. USA Workshop Judgement Aggregation and Voting September 9-11, 2011, Freudenstadt-Lauterbad 4 LATTICE THEORY of CONSENSUS (AGGREGATION) : An overview OUTLINE ABSTRACT AGGREGATION THEORIES: WHY? HOW The LATTICE APPROACH LATTICES: SOME RECALLS The CONSTRUCTIVE METHOD The federation consensus rules The AXIOMATIC METHOD Arrowian results The OPTIMISATION METHOD Lattice metric rules and the median procedure The "good" lattice structures for medians: Distributive lattices Median semilattice Workshop Judgement Aggregation and Voting September 9-11, 2011, Freudenstadt-Lauterbad 5 ABSTRACT CONSENSUS THEORIES: WHY? "since Arrow’s 1951 theorem, there has been a flurry of activity designed to prove analogues of this theorem in other contexts, and to establish contexts in which the rather dismaying consequences of this theorem are not necessarily valid. -
Problems and Comments on Boolean Algebras Rosen, Fifth Edition: Chapter 10; Sixth Edition: Chapter 11 Boolean Functions
Problems and Comments on Boolean Algebras Rosen, Fifth Edition: Chapter 10; Sixth Edition: Chapter 11 Boolean Functions Section 10. 1, Problems: 1, 2, 3, 4, 10, 11, 29, 36, 37 (fifth edition); Section 11.1, Problems: 1, 2, 5, 6, 12, 13, 31, 40, 41 (sixth edition) The notation ""forOR is bad and misleading. Just think that in the context of boolean functions, the author uses instead of ∨.The integers modulo 2, that is ℤ2 0,1, have an addition where 1 1 0 while 1 ∨ 1 1. AsetA is partially ordered by a binary relation ≤, if this relation is reflexive, that is a ≤ a holds for every element a ∈ S,it is transitive, that is if a ≤ b and b ≤ c hold for elements a,b,c ∈ S, then one also has that a ≤ c, and ≤ is anti-symmetric, that is a ≤ b and b ≤ a can hold for elements a,b ∈ S only if a b. The subsets of any set S are partially ordered by set inclusion. that is the power set PS,⊆ is a partially ordered set. A partial ordering on S is a total ordering if for any two elements a,b of S one has that a ≤ b or b ≤ a. The natural numbers ℕ,≤ with their ordinary ordering are totally ordered. A bounded lattice L is a partially ordered set where every finite subset has a least upper bound and a greatest lower bound.The least upper bound of the empty subset is defined as 0, it is the smallest element of L. -
Measure Algebras of Semilattices with Finite Breadth
Pacific Journal of Mathematics MEASURE ALGEBRAS OF SEMILATTICES WITH FINITE BREADTH JIMMIE DON LAWSON,JOHN ROBIE LIUKKONEN AND MICHAEL WILLIAM MISLOVE Vol. 69, No. 1 May 1977 PACIFIC JOURNAL OF MATHEMATICS Vol. 69, No. 1, 1977 MEASURE ALGEBRAS OF SEMILATTIGES WITH FINITE BREADTH J. D. LAWSON, J. R. LIUKKONEN AND M. W. MlSLOVE The main result of this paper is that if S is a locally compact semilattice of finite breadth, then every complex homomorphism of the measure algebra M(S) is given by integration over a Borel filter (subsemilattice whose comple- ment is an ideal), and that consequently M(S) is a P-algebra in the sense of S. E. Newman. More generally it is shown that if S is a locally compact Lawson semilattice which has the property that every bounded regular Borel measure is concentrated on a Borel set which is the countable union of compact finite breadth subsemilattices, then M(S) is a P-algebra. Furthermore, complete descriptions of the maxi- mal ideal space of M(S) and the structure semigroup of M(S) are given in terms of S, and the idempotent and invertible measures in M(S) are identified. In earlier work Baartz and Newman have shown that if S is the finite product of totally ordered locally compact semilattices, then every complex homomorphism is given by integration over a Borel subsemilattice whose complement is an ideal [1, Th. 3.15], and consequently, the structure semigroup of M(S) in the sense of Taylor [10] is itself a semilattice [9, Th. 3]. In both papers it is shown that such results do not hold for the infinite dimensional cube S — Iω, and Newman conjectures that what is needed for these results to hold is a "finite dimensionality" condition.