The Bernoulli Process and Discrete Distributions Math 217 Probability
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Partnership As Experimentation: Business Organization and Survival in Egypt, 1910–1949
Yale University EliScholar – A Digital Platform for Scholarly Publishing at Yale Discussion Papers Economic Growth Center 5-1-2017 Partnership as Experimentation: Business Organization and Survival in Egypt, 1910–1949 Cihan Artunç Timothy Guinnane Follow this and additional works at: https://elischolar.library.yale.edu/egcenter-discussion-paper-series Recommended Citation Artunç, Cihan and Guinnane, Timothy, "Partnership as Experimentation: Business Organization and Survival in Egypt, 1910–1949" (2017). Discussion Papers. 1065. https://elischolar.library.yale.edu/egcenter-discussion-paper-series/1065 This Discussion Paper is brought to you for free and open access by the Economic Growth Center at EliScholar – A Digital Platform for Scholarly Publishing at Yale. It has been accepted for inclusion in Discussion Papers by an authorized administrator of EliScholar – A Digital Platform for Scholarly Publishing at Yale. For more information, please contact [email protected]. ECONOMIC GROWTH CENTER YALE UNIVERSITY P.O. Box 208269 New Haven, CT 06520-8269 http://www.econ.yale.edu/~egcenter Economic Growth Center Discussion Paper No. 1057 Partnership as Experimentation: Business Organization and Survival in Egypt, 1910–1949 Cihan Artunç University of Arizona Timothy W. Guinnane Yale University Notes: Center discussion papers are preliminary materials circulated to stimulate discussion and critical comments. This paper can be downloaded without charge from the Social Science Research Network Electronic Paper Collection: https://ssrn.com/abstract=2973315 Partnership as Experimentation: Business Organization and Survival in Egypt, 1910–1949 Cihan Artunç⇤ Timothy W. Guinnane† This Draft: May 2017 Abstract The relationship between legal forms of firm organization and economic develop- ment remains poorly understood. Recent research disputes the view that the joint-stock corporation played a crucial role in historical economic development, but retains the view that the costless firm dissolution implicit in non-corporate forms is detrimental to investment. -
3.2.3 Binomial Distribution
3.2.3 Binomial Distribution The binomial distribution is based on the idea of a Bernoulli trial. A Bernoulli trail is an experiment with two, and only two, possible outcomes. A random variable X has a Bernoulli(p) distribution if 8 > <1 with probability p X = > :0 with probability 1 − p, where 0 ≤ p ≤ 1. The value X = 1 is often termed a “success” and X = 0 is termed a “failure”. The mean and variance of a Bernoulli(p) random variable are easily seen to be EX = (1)(p) + (0)(1 − p) = p and VarX = (1 − p)2p + (0 − p)2(1 − p) = p(1 − p). In a sequence of n identical, independent Bernoulli trials, each with success probability p, define the random variables X1,...,Xn by 8 > <1 with probability p X = i > :0 with probability 1 − p. The random variable Xn Y = Xi i=1 has the binomial distribution and it the number of sucesses among n independent trials. The probability mass function of Y is µ ¶ ¡ ¢ n ¡ ¢ P Y = y = py 1 − p n−y. y For this distribution, t n EX = np, Var(X) = np(1 − p),MX (t) = [pe + (1 − p)] . 1 Theorem 3.2.2 (Binomial theorem) For any real numbers x and y and integer n ≥ 0, µ ¶ Xn n (x + y)n = xiyn−i. i i=0 If we take x = p and y = 1 − p, we get µ ¶ Xn n 1 = (p + (1 − p))n = pi(1 − p)n−i. i i=0 Example 3.2.2 (Dice probabilities) Suppose we are interested in finding the probability of obtaining at least one 6 in four rolls of a fair die. -
A Model of Gene Expression Based on Random Dynamical Systems Reveals Modularity Properties of Gene Regulatory Networks†
A Model of Gene Expression Based on Random Dynamical Systems Reveals Modularity Properties of Gene Regulatory Networks† Fernando Antoneli1,4,*, Renata C. Ferreira3, Marcelo R. S. Briones2,4 1 Departmento de Informática em Saúde, Escola Paulista de Medicina (EPM), Universidade Federal de São Paulo (UNIFESP), SP, Brasil 2 Departmento de Microbiologia, Imunologia e Parasitologia, Escola Paulista de Medicina (EPM), Universidade Federal de São Paulo (UNIFESP), SP, Brasil 3 College of Medicine, Pennsylvania State University (Hershey), PA, USA 4 Laboratório de Genômica Evolutiva e Biocomplexidade, EPM, UNIFESP, Ed. Pesquisas II, Rua Pedro de Toledo 669, CEP 04039-032, São Paulo, Brasil Abstract. Here we propose a new approach to modeling gene expression based on the theory of random dynamical systems (RDS) that provides a general coupling prescription between the nodes of any given regulatory network given the dynamics of each node is modeled by a RDS. The main virtues of this approach are the following: (i) it provides a natural way to obtain arbitrarily large networks by coupling together simple basic pieces, thus revealing the modularity of regulatory networks; (ii) the assumptions about the stochastic processes used in the modeling are fairly general, in the sense that the only requirement is stationarity; (iii) there is a well developed mathematical theory, which is a blend of smooth dynamical systems theory, ergodic theory and stochastic analysis that allows one to extract relevant dynamical and statistical information without solving -
POISSON PROCESSES 1.1. the Rutherford-Chadwick-Ellis
POISSON PROCESSES 1. THE LAW OF SMALL NUMBERS 1.1. The Rutherford-Chadwick-Ellis Experiment. About 90 years ago Ernest Rutherford and his collaborators at the Cavendish Laboratory in Cambridge conducted a series of pathbreaking experiments on radioactive decay. In one of these, a radioactive substance was observed in N = 2608 time intervals of 7.5 seconds each, and the number of decay particles reaching a counter during each period was recorded. The table below shows the number Nk of these time periods in which exactly k decays were observed for k = 0,1,2,...,9. Also shown is N pk where k pk = (3.87) exp 3.87 =k! {− g The parameter value 3.87 was chosen because it is the mean number of decays/period for Rutherford’s data. k Nk N pk k Nk N pk 0 57 54.4 6 273 253.8 1 203 210.5 7 139 140.3 2 383 407.4 8 45 67.9 3 525 525.5 9 27 29.2 4 532 508.4 10 16 17.1 5 408 393.5 ≥ This is typical of what happens in many situations where counts of occurences of some sort are recorded: the Poisson distribution often provides an accurate – sometimes remarkably ac- curate – fit. Why? 1.2. Poisson Approximation to the Binomial Distribution. The ubiquity of the Poisson distri- bution in nature stems in large part from its connection to the Binomial and Hypergeometric distributions. The Binomial-(N ,p) distribution is the distribution of the number of successes in N independent Bernoulli trials, each with success probability p. -
5 Stochastic Processes
5 Stochastic Processes Contents 5.1. The Bernoulli Process ...................p.3 5.2. The Poisson Process .................. p.15 1 2 Stochastic Processes Chap. 5 A stochastic process is a mathematical model of a probabilistic experiment that evolves in time and generates a sequence of numerical values. For example, a stochastic process can be used to model: (a) the sequence of daily prices of a stock; (b) the sequence of scores in a football game; (c) the sequence of failure times of a machine; (d) the sequence of hourly traffic loads at a node of a communication network; (e) the sequence of radar measurements of the position of an airplane. Each numerical value in the sequence is modeled by a random variable, so a stochastic process is simply a (finite or infinite) sequence of random variables and does not represent a major conceptual departure from our basic framework. We are still dealing with a single basic experiment that involves outcomes gov- erned by a probability law, and random variables that inherit their probabilistic † properties from that law. However, stochastic processes involve some change in emphasis over our earlier models. In particular: (a) We tend to focus on the dependencies in the sequence of values generated by the process. For example, how do future prices of a stock depend on past values? (b) We are often interested in long-term averages,involving the entire se- quence of generated values. For example, what is the fraction of time that a machine is idle? (c) We sometimes wish to characterize the likelihood or frequency of certain boundary events. -
1 Normal Distribution
1 Normal Distribution. 1.1 Introduction A Bernoulli trial is simple random experiment that ends in success or failure. A Bernoulli trial can be used to make a new random experiment by repeating the Bernoulli trial and recording the number of successes. Now repeating a Bernoulli trial a large number of times has an irritating side e¤ect. Suppose we take a tossed die and look for a 3 to come up, but we do this 6000 times. 1 This is a Bernoulli trial with a probability of success of 6 repeated 6000 times. What is the probability that we will see exactly 1000 success? This is de…nitely the most likely possible outcome, 1000 successes out of 6000 tries. But it is still very unlikely that an particular experiment like this will turn out so exactly. In fact, if 6000 tosses did produce exactly 1000 successes, that would be rather suspicious. The probability of exactly 1000 successes in 6000 tries almost does not need to be calculated. whatever the probability of this, it will be very close to zero. It is probably too small a probability to be of any practical use. It turns out that it is not all that bad, 0:014. Still this is small enough that it means that have even a chance of seeing it actually happen, we would need to repeat the full experiment as many as 100 times. All told, 600,000 tosses of a die. When we repeat a Bernoulli trial a large number of times, it is unlikely that we will be interested in a speci…c number of successes, and much more likely that we will be interested in the event that the number of successes lies within a range of possibilities. -
Bernoulli Random Forests: Closing the Gap Between Theoretical Consistency and Empirical Soundness
Proceedings of the Twenty-Fifth International Joint Conference on Artificial Intelligence (IJCAI-16) Bernoulli Random Forests: Closing the Gap between Theoretical Consistency and Empirical Soundness , , , ? Yisen Wang† ‡, Qingtao Tang† ‡, Shu-Tao Xia† ‡, Jia Wu , Xingquan Zhu ⇧ † Dept. of Computer Science and Technology, Tsinghua University, China ‡ Graduate School at Shenzhen, Tsinghua University, China ? Quantum Computation & Intelligent Systems Centre, University of Technology Sydney, Australia ⇧ Dept. of Computer & Electrical Engineering and Computer Science, Florida Atlantic University, USA wangys14, tqt15 @mails.tsinghua.edu.cn; [email protected]; [email protected]; [email protected] { } Traditional Bernoulli Trial Controlled Abstract Tree Node Splitting Tree Node Splitting Random forests are one type of the most effective ensemble learning methods. In spite of their sound Random Attribute Bagging Bernoulli Trial Controlled empirical performance, the study on their theoreti- Attribute Bagging cal properties has been left far behind. Recently, several random forests variants with nice theoreti- Random Structure/Estimation cal basis have been proposed, but they all suffer Random Bootstrap Sampling Points Splitting from poor empirical performance. In this paper, we (a) Breiman RF (b) BRF propose a Bernoulli random forests model (BRF), which intends to close the gap between the theoreti- Figure 1: Comparisons between Breiman RF (left panel) vs. cal consistency and the empirical soundness of ran- the proposed BRF (right panel). The tree node splitting of dom forests classification. Compared to Breiman’s Breiman RF is deterministic, so the final trees are highly data- original random forests, BRF makes two simplifi- dependent. Instead, BRF employs two Bernoulli distributions cations in tree construction by using two indepen- to control the tree construction. -
Contents-Preface
Stochastic Processes From Applications to Theory CHAPMAN & HA LL/CRC Texts in Statis tical Science Series Series Editors Francesca Dominici, Harvard School of Public Health, USA Julian J. Faraway, University of Bath, U K Martin Tanner, Northwestern University, USA Jim Zidek, University of Br itish Columbia, Canada Statistical !eory: A Concise Introduction Statistics for Technology: A Course in Applied F. Abramovich and Y. Ritov Statistics, !ird Edition Practical Multivariate Analysis, Fifth Edition C. Chat!eld A. A!!, S. May, and V.A. Clark Analysis of Variance, Design, and Regression : Practical Statistics for Medical Research Linear Modeling for Unbalanced Data, D.G. Altman Second Edition R. Christensen Interpreting Data: A First Course in Statistics Bayesian Ideas and Data Analysis: An A.J.B. Anderson Introduction for Scientists and Statisticians Introduction to Probability with R R. Christensen, W. Johnson, A. Branscum, K. Baclawski and T.E. Hanson Linear Algebra and Matrix Analysis for Modelling Binary Data, Second Edition Statistics D. Collett S. Banerjee and A. Roy Modelling Survival Data in Medical Research, Mathematical Statistics: Basic Ideas and !ird Edition Selected Topics, Volume I, D. Collett Second Edition Introduction to Statistical Methods for P. J. Bickel and K. A. Doksum Clinical Trials Mathematical Statistics: Basic Ideas and T.D. Cook and D.L. DeMets Selected Topics, Volume II Applied Statistics: Principles and Examples P. J. Bickel and K. A. Doksum D.R. Cox and E.J. Snell Analysis of Categorical Data with R Multivariate Survival Analysis and Competing C. R. Bilder and T. M. Loughin Risks Statistical Methods for SPC and TQM M. -
Probability Theory
Probability Theory Course Notes — Harvard University — 2011 C. McMullen March 29, 2021 Contents I TheSampleSpace ........................ 2 II Elements of Combinatorial Analysis . 5 III RandomWalks .......................... 15 IV CombinationsofEvents . 24 V ConditionalProbability . 29 VI The Binomial and Poisson Distributions . 37 VII NormalApproximation. 44 VIII Unlimited Sequences of Bernoulli Trials . 55 IX Random Variables and Expectation . 60 X LawofLargeNumbers...................... 68 XI Integral–Valued Variables. Generating Functions . 70 XIV RandomWalkandRuinProblems . 70 I The Exponential and the Uniform Density . 75 II Special Densities. Randomization . 94 These course notes accompany Feller, An Introduction to Probability Theory and Its Applications, Wiley, 1950. I The Sample Space Some sources and uses of randomness, and philosophical conundrums. 1. Flipped coin. 2. The interrupted game of chance (Fermat). 3. The last roll of the game in backgammon (splitting the stakes at Monte Carlo). 4. Large numbers: elections, gases, lottery. 5. True randomness? Quantum theory. 6. Randomness as a model (in reality only one thing happens). Paradox: what if a coin keeps coming up heads? 7. Statistics: testing a drug. When is an event good evidence rather than a random artifact? 8. Significance: among 1000 coins, if one comes up heads 10 times in a row, is it likely to be a 2-headed coin? Applications to economics, investment and hiring. 9. Randomness as a tool: graph theory; scheduling; internet routing. We begin with some previews. Coin flips. What are the chances of 10 heads in a row? The probability is 1/1024, less than 0.1%. Implicit assumptions: no biases and independence. 10 What are the chance of heads 5 out of ten times? ( 5 = 252, so 252/1024 = 25%). -
Notes on Stochastic Processes
Notes on stochastic processes Paul Keeler March 20, 2018 This work is licensed under a “CC BY-SA 3.0” license. Abstract A stochastic process is a type of mathematical object studied in mathemat- ics, particularly in probability theory, which can be used to represent some type of random evolution or change of a system. There are many types of stochastic processes with applications in various fields outside of mathematics, including the physical sciences, social sciences, finance and economics as well as engineer- ing and technology. This survey aims to give an accessible but detailed account of various stochastic processes by covering their history, various mathematical definitions, and key properties as well detailing various terminology and appli- cations of the process. An emphasis is placed on non-mathematical descriptions of key concepts, with recommendations for further reading. 1 Introduction In probability and related fields, a stochastic or random process, which is also called a random function, is a mathematical object usually defined as a collection of random variables. Historically, the random variables were indexed by some set of increasing numbers, usually viewed as time, giving the interpretation of a stochastic process representing numerical values of some random system evolv- ing over time, such as the growth of a bacterial population, an electrical current fluctuating due to thermal noise, or the movement of a gas molecule [120, page 7][51, page 46 and 47][66, page 1]. Stochastic processes are widely used as math- ematical models of systems and phenomena that appear to vary in a random manner. They have applications in many disciplines including physical sciences such as biology [67, 34], chemistry [156], ecology [16][104], neuroscience [102], and physics [63] as well as technology and engineering fields such as image and signal processing [53], computer science [15], information theory [43, page 71], and telecommunications [97][11][12]. -
Random Walk in Random Scenery (RWRS)
IMS Lecture Notes–Monograph Series Dynamics & Stochastics Vol. 48 (2006) 53–65 c Institute of Mathematical Statistics, 2006 DOI: 10.1214/074921706000000077 Random walk in random scenery: A survey of some recent results Frank den Hollander1,2,* and Jeffrey E. Steif 3,† Leiden University & EURANDOM and Chalmers University of Technology Abstract. In this paper we give a survey of some recent results for random walk in random scenery (RWRS). On Zd, d ≥ 1, we are given a random walk with i.i.d. increments and a random scenery with i.i.d. components. The walk and the scenery are assumed to be independent. RWRS is the random process where time is indexed by Z, and at each unit of time both the step taken by the walk and the scenery value at the site that is visited are registered. We collect various results that classify the ergodic behavior of RWRS in terms of the characteristics of the underlying random walk (and discuss extensions to stationary walk increments and stationary scenery components as well). We describe a number of results for scenery reconstruction and close by listing some open questions. 1. Introduction Random walk in random scenery is a family of stationary random processes ex- hibiting amazingly rich behavior. We will survey some of the results that have been obtained in recent years and list some open questions. Mike Keane has made funda- mental contributions to this topic. As close colleagues it has been a great pleasure to work with him. We begin by defining the object of our study. Fix an integer d ≥ 1. -
Generalized Bernoulli Process with Long-Range Dependence And
Depend. Model. 2021; 9:1–12 Research Article Open Access Jeonghwa Lee* Generalized Bernoulli process with long-range dependence and fractional binomial distribution https://doi.org/10.1515/demo-2021-0100 Received October 23, 2020; accepted January 22, 2021 Abstract: Bernoulli process is a nite or innite sequence of independent binary variables, Xi , i = 1, 2, ··· , whose outcome is either 1 or 0 with probability P(Xi = 1) = p, P(Xi = 0) = 1 − p, for a xed constant p 2 (0, 1). We will relax the independence condition of Bernoulli variables, and develop a generalized Bernoulli process that is stationary and has auto-covariance function that obeys power law with exponent 2H − 2, H 2 (0, 1). Generalized Bernoulli process encompasses various forms of binary sequence from an independent binary sequence to a binary sequence that has long-range dependence. Fractional binomial random variable is dened as the sum of n consecutive variables in a generalized Bernoulli process, of particular interest is when its variance is proportional to n2H , if H 2 (1/2, 1). Keywords: Bernoulli process, Long-range dependence, Hurst exponent, over-dispersed binomial model MSC: 60G10, 60G22 1 Introduction Fractional process has been of interest due to its usefulness in capturing long lasting dependency in a stochas- tic process called long-range dependence, and has been rapidly developed for the last few decades. It has been applied to internet trac, queueing networks, hydrology data, etc (see [3, 7, 10]). Among the most well known models are fractional Gaussian noise, fractional Brownian motion, and fractional Poisson process. Fractional Brownian motion(fBm) BH(t) developed by Mandelbrot, B.