Interpretations of Probability First Published Mon Oct 21, 2002; Substantive Revision Mon Dec 19, 2011
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Probability Set-Up.Pdf
CHAPTER 2 The probability set-up 2.1. Basic theory of probability We will have a sample space, denoted by S (sometimes Ω) that consists of all possible outcomes. For example, if we roll two dice, the sample space would be all possible pairs made up of the numbers one through six. An event is a subset of S. Another example is to toss a coin 2 times, and let S = fHH;HT;TH;TT g; or to let S be the possible orders in which 5 horses nish in a horse race; or S the possible prices of some stock at closing time today; or S = [0; 1); the age at which someone dies; or S the points in a circle, the possible places a dart can hit. We should also keep in mind that the same setting can be described using dierent sample set. For example, in two solutions in Example 1.30 we used two dierent sample sets. 2.1.1. Sets. We start by describing elementary operations on sets. By a set we mean a collection of distinct objects called elements of the set, and we consider a set as an object in its own right. Set operations Suppose S is a set. We say that A ⊂ S, that is, A is a subset of S if every element in A is contained in S; A [ B is the union of sets A ⊂ S and B ⊂ S and denotes the points of S that are in A or B or both; A \ B is the intersection of sets A ⊂ S and B ⊂ S and is the set of points that are in both A and B; ; denotes the empty set; Ac is the complement of A, that is, the points in S that are not in A. -
21 on Probability and Cosmology: Inference Beyond Data? Martin Sahl´Ena
21 On Probability and Cosmology: Inference Beyond Data? Martin Sahl´ena Slightly expanded version of contribution to the book `The Philosophy of Cos- mology', Khalil Chamcham, Joseph Silk, John D. Barrow, Simon Saunders (eds.), Cambridge University Press, 2017. 21.1 Cosmological Model Inference with Finite Data In physical cosmology we are faced with an empirical context of gradually diminishing returns from new observations. This is true in a fundamental sense, since the amount of information we can expect to collect through as- tronomical observations is finite, owing to the fact that we occupy a particu- lar vantage point in the history and spatial extent of the Universe. Arguably, we may approach the observational limit in the foreseeable future, at least in relation to some scientific hypotheses (Ellis, 2014). There is no guaran- tee that the amount and types of information we are able to collect will be sufficient to statistically test all reasonable hypotheses that may be posed. There is under-determination both in principle and in practice (Zinkernagel, 2011; Butterfield, 2014; Ellis, 2014). These circumstances are not new, in- deed cosmology has had to contend with this problem throughout history. For example, Whitrow (1949) relates the same concerns, and points back to remarks by Blaise Pascal in the 17th century: \But if our view be arrested there let our imagination pass beyond; ... We may enlarge our conceptions beyond all imaginable space; we only produce atoms in comparison with the reality of things." Already with Thales, epistemological principles of unifor- mity and consistency have been used to structure the locally imaginable into something considered globally plausible. -
Determinism, Indeterminism and the Statistical Postulate
Tipicality, Explanation, The Statistical Postulate, and GRW Valia Allori Northern Illinois University [email protected] www.valiaallori.com Rutgers, October 24-26, 2019 1 Overview Context: Explanation of the macroscopic laws of thermodynamics in the Boltzmannian approach Among the ingredients: the statistical postulate (connected with the notion of probability) In this presentation: typicality Def: P is a typical property of X-type object/phenomena iff the vast majority of objects/phenomena of type X possesses P Part I: typicality is sufficient to explain macroscopic laws – explanatory schema based on typicality: you explain P if you explain that P is typical Part II: the statistical postulate as derivable from the dynamics Part III: if so, no preference for indeterministic theories in the quantum domain 2 Summary of Boltzmann- 1 Aim: ‘derive’ macroscopic laws of thermodynamics in terms of the microscopic Newtonian dynamics Problems: Technical ones: There are to many particles to do exact calculations Solution: statistical methods - if 푁 is big enough, one can use suitable mathematical technique to obtain information of macro systems even without having the exact solution Conceptual ones: Macro processes are irreversible, while micro processes are not Boltzmann 3 Summary of Boltzmann- 2 Postulate 1: the microscopic dynamics microstate 푋 = 푟1, … . 푟푁, 푣1, … . 푣푁 in phase space Partition of phase space into Macrostates Macrostate 푀(푋): set of macroscopically indistinguishable microstates Macroscopic view Many 푋 for a given 푀 given 푀, which 푋 is unknown Macro Properties (e.g. temperature): they slowly vary on the Macro scale There is a particular Macrostate which is incredibly bigger than the others There are many ways more to have, for instance, uniform temperature than not equilibrium (Macro)state 4 Summary of Boltzmann- 3 Entropy: (def) proportional to the size of the Macrostate in phase space (i.e. -
Topic 1: Basic Probability Definition of Sets
Topic 1: Basic probability ² Review of sets ² Sample space and probability measure ² Probability axioms ² Basic probability laws ² Conditional probability ² Bayes' rules ² Independence ² Counting ES150 { Harvard SEAS 1 De¯nition of Sets ² A set S is a collection of objects, which are the elements of the set. { The number of elements in a set S can be ¯nite S = fx1; x2; : : : ; xng or in¯nite but countable S = fx1; x2; : : :g or uncountably in¯nite. { S can also contain elements with a certain property S = fx j x satis¯es P g ² S is a subset of T if every element of S also belongs to T S ½ T or T S If S ½ T and T ½ S then S = T . ² The universal set is the set of all objects within a context. We then consider all sets S ½ . ES150 { Harvard SEAS 2 Set Operations and Properties ² Set operations { Complement Ac: set of all elements not in A { Union A \ B: set of all elements in A or B or both { Intersection A [ B: set of all elements common in both A and B { Di®erence A ¡ B: set containing all elements in A but not in B. ² Properties of set operations { Commutative: A \ B = B \ A and A [ B = B [ A. (But A ¡ B 6= B ¡ A). { Associative: (A \ B) \ C = A \ (B \ C) = A \ B \ C. (also for [) { Distributive: A \ (B [ C) = (A \ B) [ (A \ C) A [ (B \ C) = (A [ B) \ (A [ C) { DeMorgan's laws: (A \ B)c = Ac [ Bc (A [ B)c = Ac \ Bc ES150 { Harvard SEAS 3 Elements of probability theory A probabilistic model includes ² The sample space of an experiment { set of all possible outcomes { ¯nite or in¯nite { discrete or continuous { possibly multi-dimensional ² An event A is a set of outcomes { a subset of the sample space, A ½ . -
Turns in the Evolution of the Problem of Induction*
CARL G. HEMPEL TURNS IN THE EVOLUTION OF THE PROBLEM OF INDUCTION* 1. THE STANDARD CONCEPTION: INDUCTIVE "INFERENCE" Since the days of Hume's skeptical doubt, philosophical conceptions of the problem of induction and of ways in which it might be properly solved or dissolved have undergone a series of striking metamor- phoses. In my paper, I propose to examine some of those turnings, which seem to me to raise particularly important questions about the nature of empirical knowledge and especially scientific knowledge. Many, but by no means all, of the statements asserted by empirical science at a given time are accepted on the basis of previously established evidence sentences. Hume's skeptical doubt reflects the realization that most of those indirectly, or inferentially, accepted assertions rest on evidence that gives them no complete, no logically conclusive, support. This is, of course, the point of Hume's obser- vation that even if we have examined many occurrences of A and have found them all to be accompanied by B, it is quite conceivable, or logically possible, that some future occurrence of A might not be accompanied by B. Nor, we might add, does our evidence guarantee that past or present occurrences of A that we have not observed were- or are- accompanied by B, let alone that all occurrences ever of A are, without exception, accompanied by B. Yet, in our everyday pursuits as well as in scientific research we constantly rely on what I will call the method of inductive ac- ceptance, or MIA for short: we adopt beliefs, or expectations, about empirical matters on logically incomplete evidence, and we even base our actions on such beliefs- to the point of staking our lives on some of them. -
Non-Archimedean Probability (NAP) Theory
Non-Archimedean Probability Vieri Benci∗ Leon Horsten† Sylvia Wenmackers‡ October 29, 2018 Abstract We propose an alternative approach to probability theory closely re- lated to the framework of numerosity theory: non-Archimedean prob- ability (NAP). In our approach, unlike in classical probability theory, all subsets of an infinite sample space are measurable and zero- and unit-probability events pose no particular epistemological problems. We use a non-Archimedean field as the range of the probability func- tion. As a result, the property of countable additivity in Kolmogorov’s axiomatization of probability is replaced by a different type of infinite additivity. Mathematics subject classification. 60A05, 03H05 Keywords. Probability, Axioms of Kolmogorov, Nonstandard models, De Finetti lottery, Non-Archimedean fields. Contents 1 Introduction 2 1.1 Somenotation .......................... 3 2 Kolmogorov’s probability theory 4 2.1 Kolmogorov’saxioms.. .. .. .. .. .. .. 4 2.2 Problems with Kolmogorov’s axioms . 6 3 Non-Archimedean Probability 7 arXiv:1106.1524v1 [math.PR] 8 Jun 2011 3.1 The axioms of Non-Archimedean Probability . 7 3.2 Analysisofthefourthaxiom . 10 3.3 First consequences of the axioms . 11 3.4 Infinitesums ........................... 13 ∗Dipartimento di Matematica Applicata, Universit`adegli Studi di Pisa, Via F. Buonar- roti 1/c, Pisa, ITALY and Department of Mathematics, College of Science, King Saud University, Riyadh, 11451, SAUDI ARABIA. e-mail: [email protected] †Department of Philosophy, University of Bristol, 43 Woodland Rd, BS81UU Bristol, UNITED KINGDOM. e-mail: [email protected] ‡Faculty of Philosophy, University of Groningen, Oude Boteringestraat 52, 9712 GL Groningen, THE NETHERLANDS. e-mail: [email protected] 1 4 NAP-spaces and Λ-limits 14 4.1 Fineideals............................ -
Stat 5101 Lecture Notes
Stat 5101 Lecture Notes Charles J. Geyer Copyright 1998, 1999, 2000 by Charles J. Geyer January 16, 2001 ii Stat 5101 (Geyer) Course Notes Contents 1 Random Variables and Change of Variables 1 1.1 Random Variables .......................... 1 1.1.1 Variables ........................... 1 1.1.2 Functions ........................... 1 1.1.3 Random Variables: Informal Intuition ........... 3 1.1.4 Random Variables: Formal De¯nition ........... 3 1.1.5 Functions of Random Variables ............... 7 1.2 Change of Variables ......................... 7 1.2.1 General De¯nition ...................... 7 1.2.2 Discrete Random Variables . ............... 9 1.2.3 Continuous Random Variables ............... 12 1.3 Random Vectors ........................... 14 1.3.1 Discrete Random Vectors . ............... 15 1.3.2 Continuous Random Vectors . ............... 15 1.4 The Support of a Random Variable . ............... 17 1.5 Joint and Marginal Distributions . ............... 18 1.6 Multivariable Change of Variables . ............... 22 1.6.1 The General and Discrete Cases .............. 22 1.6.2 Continuous Random Vectors . ............... 22 2 Expectation 31 2.1 Introduction .............................. 31 2.2 The Law of Large Numbers ..................... 32 2.3 Basic Properties ........................... 32 2.3.1 Axioms for Expectation (Part I) .............. 32 2.3.2 Derived Basic Properties ................... 34 2.3.3 Important Non-Properties . ............... 36 2.4 Moments ............................... 37 2.4.1 First Moments and Means . ............... 38 2.4.2 Second Moments and Variances ............... 40 2.4.3 Standard Deviations and Standardization ......... 42 2.4.4 Mixed Moments and Covariances .............. 43 2.4.5 Exchangeable Random Variables .............. 50 2.4.6 Correlation .......................... 50 iii iv Stat 5101 (Geyer) Course Notes 2.5 Probability Theory as Linear Algebra .............. -
Probability Disassembled John D
Brit. J. Phil. Sci. 58 (2007), 141–171 Probability Disassembled John D. Norton ABSTRACT While there is no universal logic of induction, the probability calculus succeeds as a logic of induction in many contexts through its use of several notions concerning inductive inference. They include Addition, through which low probabilities represent disbelief as opposed to ignorance; and Bayes property, which commits the calculus to a ‘refute and rescale’ dynamics for incorporating new evidence. These notions are independent and it is urged that they be employed selectively according to needs of the problem at hand. It is shown that neither is adapted to inductive inference concerning some indeterministic systems. 1 Introduction 2 Failure of demonstrations of universality 2.1 Working backwards 2.2 The surface logic 3 Framework 3.1 The properties 3.2 Boundaries 3.2.1 Universal comparability 3.2.2 Transitivity 3.2.3 Monotonicity 4 Addition 4.1 The property: disbelief versus ignorance 4.2 Boundaries 5 Bayes property 5.1 The property 5.2 Bayes’ theorem 5.3 Boundaries 5.3.1 Dogmatism of the priors 5.3.2 Impossibility of prior ignorance 5.3.3 Accommodation of virtues 6 Real values 7 Sufficiency and independence The Author (2007). Published by Oxford University Press on behalf of British Society for the Philosophy of Science. All rights reserved. doi:10.1093/bjps/axm009 For Permissions, please email: [email protected] Advance Access published on May 23, 2007 142 John D. Norton 8 Illustrations 8.1 All properties retained 8.2 Bayes property only retained 8.3 Induction without additivity and Bayes property 9 Conclusion 1 Introduction No single idea about induction1 has been more fertile than the idea that inductive inferences may conform to the probability calculus. -
Chapter 2 Conditional Probability and Independence
CHAPTER 2 CONDITIONAL PROBABILITY AND INDEPENDENCE INTRODUCTION This chapter introduces the important concepts of conditional probability and statistical independence. Conditional probabilities arise when it is known that a certain event has occurred. This knowledge changes the probabilities of events within the sample space of the experiment. Conditioning on an event occurs frequently, and understanding how to work with conditional probabilities and apply them to a particular problem or application is extremely important. In some cases, knowing that a particular event has occurred will not effect the probability of another event, and this leads to the concept of the statistical independence of events that will be developed along with the concept of conditional independence. 2-1 CONDITIONAL PROBABILITY The three probability axioms introduced in the previous chapter provide the foundation upon which to develop a theory of probability. The next step is to understand how the knowledge that a particular event has occurred will change the probabilities that are assigned to the outcomes of an experiment. The concept of a conditional probability is one of the most important concepts in probability and, although a very simple concept, conditional probability is often confusing to students. In situations where a conditional probability is to be used, it is often overlooked or incorrectly applied, thereby leading to an incorrect answer or conclusion. Perhaps the best starting point for the development of conditional probabilities is a simple example that illustrates the context in which they arise. Suppose that we have an electronic device that has a probability pn of still working after n months of continuous operation, and suppose that the probability is equal to 0.5 that the device will still be working after one year (n = 12). -
Scaling Qualitative Probability Mark Burgin University of California, Los Angeles 405 Hilgard Ave
Scaling Qualitative Probability Mark Burgin University of California, Los Angeles 405 Hilgard Ave. Los Angeles, CA 90095 Abstract There are different approaches to qualitative probability, which includes subjective probability. We developed a representation of qualitative probability based on relational systems, which allows modeling uncertainty by probability structures and is more coherent than existing approaches. This setting makes it possible proving that any comparative probability is induced by some probability structure (Theorem 2.1), that classical probability is a probability structure (Theorem 2.2) and that inflated, i.e., larger than 1, probability is also a probability structure (Theorem 2.3). In addition, we study representation of probability structures by classical probability. Keywords: probability, qualitative probability, quantitative probability, axiom, random event, permissible event, set algebra. 1. Introduction Qualitative probability and its particular case - subjective probability – plays important role in psychology, decision making and cognitive sciences. However, the mainstream of probability theory and statistics treats probability as a numeric function or measure with specific properties (cf., for example, (Devore, 2015; Hogg, et al, 2014; Walpole, et al, 2011)). Kolmogorov rigorously represented these properties by a system of axioms treating probability as an additive measure on a system of random events (Kolmogorov, 1933). Later researchers suggested other systems of axioms for the conventional probability theory (cf., for example, (Whittle, 2000)), as well as for extended probability theory, which included negative probabilities (Burgin, 2009; 2016), and for larger than 1 (inflated) probabilities (Burgin and Meissner, 2012). At the same time, to reflect uncertainty and probabilistic aspects of decision-making and other cognitive processes, various researchers developed and applied the theory of qualitative probability as an approach to mathematical modeling and investigation of uncertainty. -
Philosophy of Probability
Philosophy of Probability Aidan Lyon Abstract In the philosophy of probability there are two central questions we are concerned with. The first is: what is the correct formal theory of proba- bility? Orthodoxy has it that Kolmogorov’s axioms are the correct axioms of probability. However, we shall see that there are good reasons to con- sider alternative axiom systems. The second central question is: what do probability statements mean? Are probabilities “out there”, in the world as frequencies, propensities, or some other objective feature of reality, or are probabilities “in the head”, as subjective degrees of belief? We will sur- vey some of the answers that philosophers, mathematicians and physicists have given to these questions. 1. Introduction The famous mathematician Henri Poincaré once wrote of the probability calcu- lus: “if this calculus be condemned, then the whole of the sciences must also be condemned” (Poincaré [1902], p. 186). Indeed, every branch of science makes extensive use of probability in some form or other. Quantum mechanics is well–known for making heavy use of probability. The second law of thermodynamics is a statistical law and, for- mulated one way, states that the entropy of a closed system is most likely to increase. In statistical mechanics, a probability distribution known as the micro–canonical distribution is used to make predictions concerning the macro- properties of gases. In evolutionary theory, the concept of fitness is often de- fined in terms of a probability function (one such definition says that fitness is expected number of offspring). Probability also plays central roles in natural se- lection, drift, and macro-evolutionary models. -
Quantum Probability 1982-2017
Quantum Probability 1982-2017 Hans Maassen, Universities of Nijmegen and Amsterdam Nijmegen, June 23, 2017. 1582: Pope Gregory XIII audaciously replaces the old-fashioned Julian calender by the new Gregorian calender, which still prevails. 1982: A bunch of mathematicians and physicists replaces the old-fashioned Kolmogorovian probability axioms by new ones: quantum probability, which still prevail. Two historic events 1982: A bunch of mathematicians and physicists replaces the old-fashioned Kolmogorovian probability axioms by new ones: quantum probability, which still prevail. Two historic events 1582: Pope Gregory XIII audaciously replaces the old-fashioned Julian calender by the new Gregorian calender, which still prevails. Two historic events 1582: Pope Gregory XIII audaciously replaces the old-fashioned Julian calender by the new Gregorian calender, which still prevails. 1982: A bunch of mathematicians and physicists replaces the old-fashioned Kolmogorovian probability axioms by new ones: quantum probability, which still prevail. Two historic events 1582: Pope Gregory XIII audaciously replaces the old-fashioned Julian calender by the new Gregorian calender, which still prevails. 1982: A bunch of mathematicians and physicists replaces the old-fashioned Kolmogorovian probability axioms by new ones: quantum probability, which still prevail. ∗ 400 years time difference; ∗ They happened in the same hall, in Villa Mondragone, 30 km south-west of Rome, in the Frascati hills. Villa Mondragone First conference in quantum probability, 1982 How are these two events related? ∗ They happened in the same hall, in Villa Mondragone, 30 km south-west of Rome, in the Frascati hills. Villa Mondragone First conference in quantum probability, 1982 How are these two events related? ∗ 400 years time difference; Villa Mondragone First conference in quantum probability, 1982 How are these two events related? ∗ 400 years time difference; ∗ They happened in the same hall, in Villa Mondragone, 30 km south-west of Rome, in the Frascati hills.