Abstract INTRODUCTION 2 INDEPENDENCE STRUCTURES

Abstract INTRODUCTION 2 INDEPENDENCE STRUCTURES

583 Generating Graphoids from Generalised Conditional Probability Nic Wilson Department of Computer Science Queen Mary and Westfield College Mile End Rd., London El 4NS, UK [email protected] Abstract This means that then independence assumptions can be propagated using the graphoid inference rules, and We take a general approach to uncertainty can be represented and propagated using the (both on product spaces, and give sufficient condi­ directed and undirected) graphical methods of [Pearl, 88]. tions for the independence structures of un­ certainty measures to satisfy graphoid prop­ erties. Since these conditions are arguably In section 2 we define independence structures, semi­ more intuitive than some of the graphoid graphoids and graphoids. GCPPs are defined in sec­ properties, they can be viewed as explana­ tion 3, with examples and we show how they give rise tions why probability and certain other for­ to independence structures. Section 4 considers the malisms generate graphoids. The conditions Intersection property. In the literature it seems to be include a sufficient condition for the Inter­ generally assumed that this only holds for probability section property which can still apply even if distributions which are always non-zero; we show here there is a strong logical relationship between that it holds much more generally, a sufficient con­ the variables. We indicate how these results dition being a connectivity property on the non-zero can be used to produce theories of qualita­ values of the probability; exactly the same condition tive conditional probability which are semi­ is sufficient for other GCPPs to satisfy Intersection. graphoids and graphoids. Section 5 considers different sufficient conditions for GCPPs to give rise to semi-graphoids. These are use­ Keywords: Graphoids, Conditional Inde­ ful for constructing uncertainty calculi which generate pendence, Qualitative Probability. graphoids and might also be used for showing that an uncertainty calculus gives rise to a graphoid. 1 INTRODUCTION In section 6 we consider another view of GCPPs: as qualitative conditional probabilities. This view allows The importance of the qualitative features of prob­ graphoids to be constructed from qualitative compar­ abilistic reasoning has often been emphasised in the ative judgements of probability. Section 7 briefly con­ 8 recent AI literature, especially by Judea Pearl. An siders computation of GCPPs, and section highlights important qualitative aspect of probability is given by some areas for further study. the graphoid properties, defined in [Pearl, 88] (see also [Dawid, 79; Smith, 90]) which sum up many of the properties of probabilistic conditional independence. 2 INDEPENDENCE STRUCTURES In this paper we look at the reasons why probabil­ ity obeys these properties, with an eye to generating Let U be a finite set. An independence structure I on other uncertainty theories which share much of the U is defined to be a set of triples (X, Z, Y) where X, Y same structure as probability, but represent different and Z are disjoint1 subsets of U. We write I(X, Z, Y) types of information, perhaps of a more qualitative for (X, Z, Y) E I. For disjoint subsets X, Y � U, their nature. union XU Y will be written XY. A fairly general family of uncertainty calculi on prod­ U is intended to be a set of variables, and I(X, Z, Y) is uct spaces is introduced, which we call Generalised intended to mean that variables X are independent of Conditional Probability on Product Spaces (GCPP), variables Y given we know the values of the variables and define two different types of conditional indepen­ z. dence for GCPPs. We show that under simple (and apparently fairly weak) conditions, conditional inde­ 1 A collection A of sets is sa.id to be disjoint if for ea.ch pendence for GCPPs satisfies the graphoid properties. X, Y E A, X n Y = 0. 584 Wilson The Graphoid Properties of Independence disjoint X, Y � U, an element of XY may be written Structures xy for x EX, y E Y. For disjoint X, Y � U we define XIY to be the set of all pairs {xly : x EX, y E Y}. I(X, Z, 0) (Trivial Independence) The set ]1 is defined to be a singleton {T}. An element. If I(X, Z, Y) then I(Y, Z, X) (Symmetry) xiT of X I� will usually be abbreviated to x (we are identifying Xl]l. with X). If I(X,Z, YW) then I(X, Z, Y) (Decomposition) The set u· is defined to be X IY. If I(X,Z, YW) then I(X, ZY, W) (Weak Union) u X,YCU - XnY =� If I(X,ZY, W) and I(X,Z, Y) then I(X,Z, YW) (Contraction) A GCPP p over set of variables U is defined to be a function p: u• _. D for some set D containing differ­ If I{X, ZY, W) and I( X, ZW, Y) then I(X Z, YW) , ent distinguished elements 0 and oo such that for any (Intersection) disjoint X, Y � U and x EX, where W, Y, are arbitrary disjoint subsets of U X, Z (i) p(x) = 0 if and only if for all y E Y, p(xy) = 0, (so, for example, I satisfies symmetry if and only if and the above property holds for all disjoint X, Y and Z). (ii) for any y E Y, p(xlv) = oo if and only if p(y) = 0. If an independence structure satisfies all these proper­ ties then it is said to be a graphoid; if it satisfies the GCPPs will be viewed as measures of uncertainty; first five (i.e, all except Intersection) then it is said to p(xly) may be thought of as some sort of measure be a semi-graphoid. As we shall see in section 5, prob­ of how plausible it is that the composite variable X abilistic conditional independence is a semi-graphoid, takes the value x, given that Y takes the value y. The and in certain situations a graphoid. assignment p( x IY) = 0 is intended to mean that :c is impossible given i.e., cannot take the value :1: if The definitions given here for semi-graphoid and y, X Y takes the value The inclusion of element oo in graphoid differ from that given in [Pearl, 88], in that y. D is not strictly necessary; it is used as a notational we require Trivial Independence to hold. However, our convenience, and can be read as 'undefined'. We re­ definition seems to be what Pearl intended2; it is not quire (i) because: x is possible if and only if there is implied by other properties (consider the empty inde­ some value of which is possible when X takes the pendence structure) and it is satisfied by probabilis­ Y value x. We require (ii) because: if y is impossible tic conditional independence so it is a (rather triv­ then conditioning on doesn't make much sense. ial) counter-example to the Completeness Conjecture3 y [Pearl, 88]; also without Trivial Independence, Markov Note that no structure on Dis assumed; for example, boundaries don't necessarily exist (consider the empty we do not assume that D \ { oo} � IR, or even that D independence structure again) which makes Theorem has an ordering on it. 4 of [Pearl, 88] incorrect. The definition implies that p(T) ::}; 0, oo and that for The intersection of a family of (semi-)graphoids is a any X� U and x EX, p(J.;)::}; oo. (semi-)graphoid. Hence, for any independence struc­ ture I, there is a unique smallest (semi-)graphoid con­ Definition taining I. For GCPP p over U and disjoint X, Y � U define pXIY to be p restricted to X IY and define px to be pXI0. 3 GENERALISED CONDITIONAL For Z � U and z E Z define Pz: (U \ Z)" -> D by, PROBABILITY ON PROD UCT for disjoint X, Y � U \ Z, x E X, y E Y, Pz(xly) = SPACES (GCPPs) p(xlyz). For disjoint X, Y � U \ Z, p;'JY is defined to be Pz restricted to X IY, and P7 is defined to be p;'10. Uncertainty measures are usually defined on boolean GCPP over U is said to be a full GCPP over U if algebras. However, for our purposes of studying in­ p for every � U and z Z such that a dependence structures generated by the uncertainty Z E p(z)::}; 0, p, is GCPP over U measure, a different domain is natural. \ Z. The function P.z may be thought of as p conditioned THE BASIC DEFINITIONS 3.1 on Z = z. It turns out that, for GCPP p, p is a full GCPP if and only if for all disjoint X, Y � U, x E X, U = {X1, ... , Xn} is said to be a set of variables if = 0 ¢::=::> p(xy) = 0 and p(y) 0]. associated with each variable X; E U is a finite set of y E Y, [p(xly) ::}; values X;. For X� U defineX to be Il ,E X;. For x X 3.2 EXAMPLES OF GCPPS 2See, for example, the sentence before Theorem 4, p97 of [Pearl, 88]. A probability function over set of variables U is de­ 3 Fatal counter-examples are given in [Studeny, 92]. fined to be a function p: u· - [ 0, 1] u { 00} such that Generating Graphoids from Generalised Conditional Probability 585 for xJy E U*, (i) P(xJy) oo ¢::::::} P(y) == 0; include a maximal element in the range of OCFs be­ (ii) if P(y) # 0, P(xJy) P(xy)/P(y); and (iii) cause he desired belief change to be reversible [Spohn, P(x)::: LweU\X P(xw).

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