Towards a Bohrification of Effect Algebras
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Math Preliminaries
Preliminaries We establish here a few notational conventions used throughout the text. Arithmetic with ∞ We shall sometimes use the symbols “∞” and “−∞” in simple arithmetic expressions involving real numbers. The interpretation given to such ex- pressions is the usual, natural one; for example, for all real numbers x, we have −∞ < x < ∞, x + ∞ = ∞, x − ∞ = −∞, ∞ + ∞ = ∞, and (−∞) + (−∞) = −∞. Some such expressions have no sensible interpreta- tion (e.g., ∞ − ∞). Logarithms and exponentials We denote by log x the natural logarithm of x. The logarithm of x to the base b is denoted logb x. We denote by ex the usual exponential function, where e ≈ 2.71828 is the base of the natural logarithm. We may also write exp[x] instead of ex. Sets and relations We use the symbol ∅ to denote the empty set. For two sets A, B, we use the notation A ⊆ B to mean that A is a subset of B (with A possibly equal to B), and the notation A ( B to mean that A is a proper subset of B (i.e., A ⊆ B but A 6= B); further, A ∪ B denotes the union of A and B, A ∩ B the intersection of A and B, and A \ B the set of all elements of A that are not in B. For sets S1,...,Sn, we denote by S1 × · · · × Sn the Cartesian product xiv Preliminaries xv of S1,...,Sn, that is, the set of all n-tuples (a1, . , an), where ai ∈ Si for i = 1, . , n. We use the notation S×n to denote the Cartesian product of n copies of a set S, and for x ∈ S, we denote by x×n the element of S×n consisting of n copies of x. -
Sets, Functions
Sets 1 Sets Informally: A set is a collection of (mathematical) objects, with the collection treated as a single mathematical object. Examples: • real numbers, • complex numbers, C • integers, • All students in our class Defining Sets Sets can be defined directly: e.g. {1,2,4,8,16,32,…}, {CSC1130,CSC2110,…} Order, number of occurence are not important. e.g. {A,B,C} = {C,B,A} = {A,A,B,C,B} A set can be an element of another set. {1,{2},{3,{4}}} Defining Sets by Predicates The set of elements, x, in A such that P(x) is true. {}x APx| ( ) The set of prime numbers: Commonly Used Sets • N = {0, 1, 2, 3, …}, the set of natural numbers • Z = {…, -2, -1, 0, 1, 2, …}, the set of integers • Z+ = {1, 2, 3, …}, the set of positive integers • Q = {p/q | p Z, q Z, and q ≠ 0}, the set of rational numbers • R, the set of real numbers Special Sets • Empty Set (null set): a set that has no elements, denoted by ф or {}. • Example: The set of all positive integers that are greater than their squares is an empty set. • Singleton set: a set with one element • Compare: ф and {ф} – Ф: an empty set. Think of this as an empty folder – {ф}: a set with one element. The element is an empty set. Think of this as an folder with an empty folder in it. Venn Diagrams • Represent sets graphically • The universal set U, which contains all the objects under consideration, is represented by a rectangle. -
The Structure of the 3-Separations of 3-Connected Matroids
THE STRUCTURE OF THE 3{SEPARATIONS OF 3{CONNECTED MATROIDS JAMES OXLEY, CHARLES SEMPLE, AND GEOFF WHITTLE Abstract. Tutte defined a k{separation of a matroid M to be a partition (A; B) of the ground set of M such that |A|; |B|≥k and r(A)+r(B) − r(M) <k. If, for all m<n, the matroid M has no m{separations, then M is n{connected. Earlier, Whitney showed that (A; B) is a 1{separation of M if and only if A is a union of 2{connected components of M.WhenM is 2{connected, Cunningham and Edmonds gave a tree decomposition of M that displays all of its 2{separations. When M is 3{connected, this paper describes a tree decomposition of M that displays, up to a certain natural equivalence, all non-trivial 3{ separations of M. 1. Introduction One of Tutte’s many important contributions to matroid theory was the introduction of the general theory of separations and connectivity [10] de- fined in the abstract. The structure of the 1–separations in a matroid is elementary. They induce a partition of the ground set which in turn induces a decomposition of the matroid into 2–connected components [11]. Cun- ningham and Edmonds [1] considered the structure of 2–separations in a matroid. They showed that a 2–connected matroid M can be decomposed into a set of 3–connected matroids with the property that M can be built from these 3–connected matroids via a canonical operation known as 2–sum. Moreover, there is a labelled tree that gives a precise description of the way that M is built from the 3–connected pieces. -
Dichotomy Between Deterministic and Probabilistic Models in Countably Additive Effectus Theory
Dichotomy between deterministic and probabilistic models in countably additive effectus theory Kenta Cho National Institute of Informatics, Japan Bas Westerbaan University College London John van de Wetering Radboud University Nijmegen June 6, 2020 such that § hom-sets tf : A Ñ Bu are convex sets, § and the scalars ts : I Ñ I u are the real unit interval r0; 1s Special operations: § States StpAq :“ t! : I Ñ Au § Effects EffpAq :“ tp : A Ñ I u § p ˝ ! is probability that p holds on state ! Generalized Probabilistic Theories GPTs are generalisations of quantum theory. They consist of § systems A; B; C;:::, § the `empty system' I , § operations f : A Ñ B, Special operations: § States StpAq :“ t! : I Ñ Au § Effects EffpAq :“ tp : A Ñ I u § p ˝ ! is probability that p holds on state ! Generalized Probabilistic Theories GPTs are generalisations of quantum theory. They consist of § systems A; B; C;:::, § the `empty system' I , § operations f : A Ñ B, such that § hom-sets tf : A Ñ Bu are convex sets, § and the scalars ts : I Ñ I u are the real unit interval r0; 1s Generalized Probabilistic Theories GPTs are generalisations of quantum theory. They consist of § systems A; B; C;:::, § the `empty system' I , § operations f : A Ñ B, such that § hom-sets tf : A Ñ Bu are convex sets, § and the scalars ts : I Ñ I u are the real unit interval r0; 1s Special operations: § States StpAq :“ t! : I Ñ Au § Effects EffpAq :“ tp : A Ñ I u § p ˝ ! is probability that p holds on state ! Solution: allow more general sets of scalars ts : I Ñ I u. -
Matroids with Nine Elements
Matroids with nine elements Dillon Mayhew School of Mathematics, Statistics & Computer Science Victoria University Wellington, New Zealand [email protected] Gordon F. Royle School of Computer Science & Software Engineering University of Western Australia Perth, Australia [email protected] February 2, 2008 Abstract We describe the computation of a catalogue containing all matroids with up to nine elements, and present some fundamental data arising from this cataogue. Our computation confirms and extends the results obtained in the 1960s by Blackburn, Crapo & Higgs. The matroids and associated data are stored in an online database, arXiv:math/0702316v1 [math.CO] 12 Feb 2007 and we give three short examples of the use of this database. 1 Introduction In the late 1960s, Blackburn, Crapo & Higgs published a technical report describing the results of a computer search for all simple matroids on up to eight elements (although the resulting paper [2] did not appear until 1973). In both the report and the paper they said 1 “It is unlikely that a complete tabulation of 9-point geometries will be either feasible or desirable, as there will be many thousands of them. The recursion g(9) = g(8)3/2 predicts 29260.” Perhaps this comment dissuaded later researchers in matroid theory, because their cata- logue remained unextended for more than 30 years, which surely makes it one of the longest standing computational results in combinatorics. However, in this paper we demonstrate that they were in fact unduly pessimistic, and describe an orderly algorithm (see McKay [7] and Royle [11]) that confirms their computations and extends them by determining the 383172 pairwise non-isomorphic matroids on nine elements (see Table 1). -
Section 3: Equivalence Relations
10.3.1 Section 3: Equivalence Relations • Definition: Let R be a binary relation on A. R is an equivalence relation on A if R is reflexive, symmetric, and transitive. • From the last section, we demonstrated that Equality on the Real Numbers and Congruence Modulo p on the Integers were reflexive, symmetric, and transitive, so we can describe them as equivalence relations. 10.3.2 Examples • What is the “smallest” equivalence relation on a set A? R = {(a,a) | a Î A}, so that n(R) = n(A). • What is the “largest” equivalence relation on a set A? R = A ´ A, so that n(R) = [n(A)]2. Equivalence Classes 10.3.3 • Definition: If R is an equivalence relation on a set A, and a Î A, then the equivalence class of a is defined to be: [a] = {b Î A | (a,b) Î R}. • In other words, [a] is the set of all elements which relate to a by R. • For example: If R is congruence mod 5, then [3] = {..., -12, -7, -2, 3, 8, 13, 18, ...}. • Another example: If R is equality on Q, then [2/3] = {2/3, 4/6, 6/9, 8/12, 10/15, ...}. • Observation: If b Î [a], then [b] = [a]. 10.3.4 A String Example • Let S = {0,1} and denote L(s) = length of s, for any string s Î S*. Consider the relation: R = {(s,t) | s,t Î S* and L(s) = L(t)} • R is an equivalence relation. Why? • REF: For all s Î S*, L(s) = L(s); SYM: If L(s) = L(t), then L(t) = L(s); TRAN: If L(s) = L(t) and L(t) = L(u), L(s) = L(u). -
Parity Systems and the Delta-Matroid Intersection Problem
Parity Systems and the Delta-Matroid Intersection Problem Andr´eBouchet ∗ and Bill Jackson † Submitted: February 16, 1998; Accepted: September 3, 1999. Abstract We consider the problem of determining when two delta-matroids on the same ground-set have a common base. Our approach is to adapt the theory of matchings in 2-polymatroids developed by Lov´asz to a new abstract system, which we call a parity system. Examples of parity systems may be obtained by combining either, two delta- matroids, or two orthogonal 2-polymatroids, on the same ground-sets. We show that many of the results of Lov´aszconcerning ‘double flowers’ and ‘projections’ carry over to parity systems. 1 Introduction: the delta-matroid intersec- tion problem A delta-matroid is a pair (V, ) with a finite set V and a nonempty collection of subsets of V , called theBfeasible sets or bases, satisfying the following axiom:B ∗D´epartement d’informatique, Universit´edu Maine, 72017 Le Mans Cedex, France. [email protected] †Department of Mathematical and Computing Sciences, Goldsmiths’ College, London SE14 6NW, England. [email protected] 1 the electronic journal of combinatorics 7 (2000), #R14 2 1.1 For B1 and B2 in and v1 in B1∆B2, there is v2 in B1∆B2 such that B B1∆ v1, v2 belongs to . { } B Here P ∆Q = (P Q) (Q P ) is the symmetric difference of two subsets P and Q of V . If X\ is a∪ subset\ of V and if we set ∆X = B∆X : B , then we note that (V, ∆X) is a new delta-matroid.B The{ transformation∈ B} (V, ) (V, ∆X) is calledB a twisting. -
Computing Partitions Within SQL Queries: a Dead End? Frédéric Dumonceaux, Guillaume Raschia, Marc Gelgon
Computing Partitions within SQL Queries: A Dead End? Frédéric Dumonceaux, Guillaume Raschia, Marc Gelgon To cite this version: Frédéric Dumonceaux, Guillaume Raschia, Marc Gelgon. Computing Partitions within SQL Queries: A Dead End?. 2013. hal-00768156 HAL Id: hal-00768156 https://hal.archives-ouvertes.fr/hal-00768156 Submitted on 20 Dec 2012 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. Computing Partitions within SQL Queries: A Dead End? Fr´ed´eric Dumonceaux – Guillaume Raschia – Marc Gelgon December 20, 2012 Abstract The primary goal of relational databases is to provide efficient query processing on sets of tuples and thereafter, query evaluation and optimization strategies are a key issue in database implementation. Producing universally fast execu- tion plans remains a challenging task since the underlying relational model has a significant impact on algebraic definition of the operators, thereby on their implementation in terms of space and time complexity. At least, it should pre- vent a quadratic behavior in order to consider scaling-up towards the processing of large datasets. The main purpose of this paper is to show that there is no trivial relational modeling for managing collections of partitions (i.e. -
Partial Ordering Relations • a Relation Is Said to Be a Partial Ordering Relation If It Is Reflexive, Anti -Symmetric, and Transitive
Relations Chang-Gun Lee ([email protected]) Assistant Professor The School of Computer Science and Engineering Seoul National University Relations • The concept of relations is also commonly used in computer science – two of the programs are related if they share some common data and are not related otherwise. – two wireless nodes are related if they interfere each other and are not related otherwise – In a database, two objects are related if their secondary key values are the same • What is the mathematical definition of a relation? • Definition 13.1 (Relation): A relation is a set of ordered pairs – The set of ordered pairs is a complete listing of all pairs of objects that “satisfy” the relation •Examples: – Greater Than Re lat ion = {(2 {(21)(31)(32),1), (3,1), (3,2), ...... } – R = {(1,2), (1,3), (3,0)} (1,2)∈ R, 1 R 2 :"x is related by the relation R to y" Relations • Definition 13.2 (Relation on, between sets) Let R be a relation and let A and B be sets . –We say R is a relation on A provided R ⊆ A× A –We say R is a relation from A to B provided R ⊆ A× B Example Relations •Let A={1,2,3,4} and B={4,5,6,7}. Let – R={(11)(22)(33)(44)}{(1,1),(2,2),(3,3),(4,4)} – S={(1,2),(3,2)} – T={(1,4),(1,5),(4,7)} – U={(4,4),(5,2),(6,2),(7,3)}, and – V={(1,7),(7,1)} • All of these are relations – R is a relation on A. -
Notes for Math 450 Lecture Notes 2
Notes for Math 450 Lecture Notes 2 Renato Feres 1 Probability Spaces We first explain the basic concept of a probability space, (Ω, F,P ). This may be interpreted as an experiment with random outcomes. The set Ω is the collection of all possible outcomes of the experiment; F is a family of subsets of Ω called events; and P is a function that associates to an event its probability. These objects must satisfy certain logical requirements, which are detailed below. A random variable is a function X :Ω → S of the output of the random system. We explore some of the general implications of these abstract concepts. 1.1 Events and the basic set operations on them Any situation where the outcome is regarded as random will be referred to as an experiment, and the set of all possible outcomes of the experiment comprises its sample space, denoted by S or, at times, Ω. Each possible outcome of the experiment corresponds to a single element of S. For example, rolling a die is an experiment whose sample space is the finite set {1, 2, 3, 4, 5, 6}. The sample space for the experiment of tossing three (distinguishable) coins is {HHH,HHT,HTH,HTT,THH,THT,TTH,TTT } where HTH indicates the ordered triple (H, T, H) in the product set {H, T }3. The delay in departure of a flight scheduled for 10:00 AM every day can be regarded as the outcome of an experiment in this abstract sense, where the sample space now may be taken to be the interval [0, ∞) of the real line. -
Arxiv:1711.00219V2 [Math.OA] 9 Aug 2019 R,Fe Rbblt,Glbr Coefficients
CUMULANTS, SPREADABILITY AND THE CAMPBELL-BAKER-HAUSDORFF SERIES TAKAHIRO HASEBE AND FRANZ LEHNER Abstract. We define spreadability systems as a generalization of exchangeability systems in order to unify various notions of independence and cumulants known in noncommutative probability. In particular, our theory covers monotone independence and monotone cumulants which do not satisfy exchangeability. To this end we study generalized zeta and M¨obius functions in the context of the incidence algebra of the semilattice of ordered set partitions and prove an appropriate variant of Faa di Bruno’s theorem. With the aid of this machinery we show that our cumulants cover most of the previously known cumulants. Due to noncommutativity of independence the behaviour of these cumulants with respect to independent random variables is more complicated than in the exchangeable case and the appearance of Goldberg coefficients exhibits the role of the Campbell-Baker-Hausdorff series in this context. In a final section we exhibit an interpretation of the Campbell-Baker-Hausdorff series as a sum of cumulants in a particular spreadability system, thus providing a new derivation of the Goldberg coefficients. Contents 1. Introduction 2 2. Ordered set partitions 4 2.1. Set partitions 4 2.2. Ordered set partitions 5 2.3. Incidence algebras and multiplicative functions 8 2.4. Special functions in the poset of ordered set partitions 10 3. A generalized notion of independence related to spreadability systems 11 3.1. Notation and terminology 11 3.2. Spreadability systems 13 3.3. Examples from natural products of linear maps 14 3.4. E-independence 15 3.5. -
Arxiv:Quant-Ph/0611110 V1 10 Nov 2006
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server COORDINATING QUANTUM AGENTS’ PERSPECTIVES: CONVEX OPERATIONAL THEORIES, QUANTUM INFORMATION, AND QUANTUM FOUNDATIONS H. BARNUM1 1Computer and Computational Sciences Division CCS-3, MS B256, Los Alamos National Laboratory, Los Alamos 87545, USA E-mail: [email protected] In this paper, I propose a project of enlisting quantum information science as a source of task- oriented axioms for use in the investigation of operational theories in a general framework capable of encompassing quantum mechanics, classical theory, and more. Whatever else they may be, quantum states of systems are compendia of probabilities for the outcomes of possible operations we may perform on the systems: “operational theories.” I discuss appropriate general frameworks for such theories, in which convexity plays a key role. Such frameworks are appropriate for investigating what things look like from an “inside view,” i.e. for describing perspectival information that one subsystem of the world can have about another. Understanding how such views can combine, and whether an overall “geometric” picture (“outside view”) coordinating them all can be had, even if this picture is very different in nature from the structure of the perspectives within it, is the key to understanding whether we may be able to achieve a unified, “objective” physical view in which quantum mechanics is the appropriate description for certain perspectives, or whether quantum mechanics is truly telling us we must go beyond this “geometric” conception of physics. The nature of information, its flow and processing, as seen from various operational persepectives, is likely to be key to understanding whether and how such coordination and unification can be achieved.