Why Monte Carlo Simulations Are Inferences and Not Experiments
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Kalman and Particle Filtering
Abstract: The Kalman and Particle filters are algorithms that recursively update an estimate of the state and find the innovations driving a stochastic process given a sequence of observations. The Kalman filter accomplishes this goal by linear projections, while the Particle filter does so by a sequential Monte Carlo method. With the state estimates, we can forecast and smooth the stochastic process. With the innovations, we can estimate the parameters of the model. The article discusses how to set a dynamic model in a state-space form, derives the Kalman and Particle filters, and explains how to use them for estimation. Kalman and Particle Filtering The Kalman and Particle filters are algorithms that recursively update an estimate of the state and find the innovations driving a stochastic process given a sequence of observations. The Kalman filter accomplishes this goal by linear projections, while the Particle filter does so by a sequential Monte Carlo method. Since both filters start with a state-space representation of the stochastic processes of interest, section 1 presents the state-space form of a dynamic model. Then, section 2 intro- duces the Kalman filter and section 3 develops the Particle filter. For extended expositions of this material, see Doucet, de Freitas, and Gordon (2001), Durbin and Koopman (2001), and Ljungqvist and Sargent (2004). 1. The state-space representation of a dynamic model A large class of dynamic models can be represented by a state-space form: Xt+1 = ϕ (Xt,Wt+1; γ) (1) Yt = g (Xt,Vt; γ) . (2) This representation handles a stochastic process by finding three objects: a vector that l describes the position of the system (a state, Xt X R ) and two functions, one mapping ∈ ⊂ 1 the state today into the state tomorrow (the transition equation, (1)) and one mapping the state into observables, Yt (the measurement equation, (2)). -
A Fourier-Wavelet Monte Carlo Method for Fractal Random Fields
JOURNAL OF COMPUTATIONAL PHYSICS 132, 384±408 (1997) ARTICLE NO. CP965647 A Fourier±Wavelet Monte Carlo Method for Fractal Random Fields Frank W. Elliott Jr., David J. Horntrop, and Andrew J. Majda Courant Institute of Mathematical Sciences, 251 Mercer Street, New York, New York 10012 Received August 2, 1996; revised December 23, 1996 2 2H k[v(x) 2 v(y)] l 5 CHux 2 yu , (1.1) A new hierarchical method for the Monte Carlo simulation of random ®elds called the Fourier±wavelet method is developed and where 0 , H , 1 is the Hurst exponent and k?l denotes applied to isotropic Gaussian random ®elds with power law spectral the expected value. density functions. This technique is based upon the orthogonal Here we develop a new Monte Carlo method based upon decomposition of the Fourier stochastic integral representation of the ®eld using wavelets. The Meyer wavelet is used here because a wavelet expansion of the Fourier space representation of its rapid decay properties allow for a very compact representation the fractal random ®elds in (1.1). This method is capable of the ®eld. The Fourier±wavelet method is shown to be straightfor- of generating a velocity ®eld with the Kolmogoroff spec- ward to implement, given the nature of the necessary precomputa- trum (H 5 Ad in (1.1)) over many (10 to 15) decades of tions and the run-time calculations, and yields comparable results scaling behavior comparable to the physical space multi- with scaling behavior over as many decades as the physical space multiwavelet methods developed recently by two of the authors. -
3 Autocorrelation
3 Autocorrelation Autocorrelation refers to the correlation of a time series with its own past and future values. Autocorrelation is also sometimes called “lagged correlation” or “serial correlation”, which refers to the correlation between members of a series of numbers arranged in time. Positive autocorrelation might be considered a specific form of “persistence”, a tendency for a system to remain in the same state from one observation to the next. For example, the likelihood of tomorrow being rainy is greater if today is rainy than if today is dry. Geophysical time series are frequently autocorrelated because of inertia or carryover processes in the physical system. For example, the slowly evolving and moving low pressure systems in the atmosphere might impart persistence to daily rainfall. Or the slow drainage of groundwater reserves might impart correlation to successive annual flows of a river. Or stored photosynthates might impart correlation to successive annual values of tree-ring indices. Autocorrelation complicates the application of statistical tests by reducing the effective sample size. Autocorrelation can also complicate the identification of significant covariance or correlation between time series (e.g., precipitation with a tree-ring series). Autocorrelation implies that a time series is predictable, probabilistically, as future values are correlated with current and past values. Three tools for assessing the autocorrelation of a time series are (1) the time series plot, (2) the lagged scatterplot, and (3) the autocorrelation function. 3.1 Time series plot Positively autocorrelated series are sometimes referred to as persistent because positive departures from the mean tend to be followed by positive depatures from the mean, and negative departures from the mean tend to be followed by negative departures (Figure 3.1). -
The Bayesian Approach to Statistics
THE BAYESIAN APPROACH TO STATISTICS ANTHONY O’HAGAN INTRODUCTION the true nature of scientific reasoning. The fi- nal section addresses various features of modern By far the most widely taught and used statisti- Bayesian methods that provide some explanation for the rapid increase in their adoption since the cal methods in practice are those of the frequen- 1980s. tist school. The ideas of frequentist inference, as set out in Chapter 5 of this book, rest on the frequency definition of probability (Chapter 2), BAYESIAN INFERENCE and were developed in the first half of the 20th century. This chapter concerns a radically differ- We first present the basic procedures of Bayesian ent approach to statistics, the Bayesian approach, inference. which depends instead on the subjective defini- tion of probability (Chapter 3). In some respects, Bayesian methods are older than frequentist ones, Bayes’s Theorem and the Nature of Learning having been the basis of very early statistical rea- Bayesian inference is a process of learning soning as far back as the 18th century. Bayesian from data. To give substance to this statement, statistics as it is now understood, however, dates we need to identify who is doing the learning and back to the 1950s, with subsequent development what they are learning about. in the second half of the 20th century. Over that time, the Bayesian approach has steadily gained Terms and Notation ground, and is now recognized as a legitimate al- ternative to the frequentist approach. The person doing the learning is an individual This chapter is organized into three sections. -
Fourier, Wavelet and Monte Carlo Methods in Computational Finance
Fourier, Wavelet and Monte Carlo Methods in Computational Finance Kees Oosterlee1;2 1CWI, Amsterdam 2Delft University of Technology, the Netherlands AANMPDE-9-16, 7/7/2016 Kees Oosterlee (CWI, TU Delft) Comp. Finance AANMPDE-9-16 1 / 51 Joint work with Fang Fang, Marjon Ruijter, Luis Ortiz, Shashi Jain, Alvaro Leitao, Fei Cong, Qian Feng Agenda Derivatives pricing, Feynman-Kac Theorem Fourier methods Basics of COS method; Basics of SWIFT method; Options with early-exercise features COS method for Bermudan options Monte Carlo method BSDEs, BCOS method (very briefly) Kees Oosterlee (CWI, TU Delft) Comp. Finance AANMPDE-9-16 1 / 51 Agenda Derivatives pricing, Feynman-Kac Theorem Fourier methods Basics of COS method; Basics of SWIFT method; Options with early-exercise features COS method for Bermudan options Monte Carlo method BSDEs, BCOS method (very briefly) Joint work with Fang Fang, Marjon Ruijter, Luis Ortiz, Shashi Jain, Alvaro Leitao, Fei Cong, Qian Feng Kees Oosterlee (CWI, TU Delft) Comp. Finance AANMPDE-9-16 1 / 51 Feynman-Kac theorem: Z T v(t; x) = E g(s; Xs )ds + h(XT ) ; t where Xs is the solution to the FSDE dXs = µ(Xs )ds + σ(Xs )d!s ; Xt = x: Feynman-Kac Theorem The linear partial differential equation: @v(t; x) + Lv(t; x) + g(t; x) = 0; v(T ; x) = h(x); @t with operator 1 Lv(t; x) = µ(x)Dv(t; x) + σ2(x)D2v(t; x): 2 Kees Oosterlee (CWI, TU Delft) Comp. Finance AANMPDE-9-16 2 / 51 Feynman-Kac Theorem The linear partial differential equation: @v(t; x) + Lv(t; x) + g(t; x) = 0; v(T ; x) = h(x); @t with operator 1 Lv(t; x) = µ(x)Dv(t; x) + σ2(x)D2v(t; x): 2 Feynman-Kac theorem: Z T v(t; x) = E g(s; Xs )ds + h(XT ) ; t where Xs is the solution to the FSDE dXs = µ(Xs )ds + σ(Xs )d!s ; Xt = x: Kees Oosterlee (CWI, TU Delft) Comp. -
Efficient Monte Carlo Methods for Estimating Failure Probabilities
Reliability Engineering and System Safety 165 (2017) 376–394 Contents lists available at ScienceDirect Reliability Engineering and System Safety journal homepage: www.elsevier.com/locate/ress ffi E cient Monte Carlo methods for estimating failure probabilities MARK ⁎ Andres Albana, Hardik A. Darjia,b, Atsuki Imamurac, Marvin K. Nakayamac, a Mathematical Sciences Dept., New Jersey Institute of Technology, Newark, NJ 07102, USA b Mechanical Engineering Dept., New Jersey Institute of Technology, Newark, NJ 07102, USA c Computer Science Dept., New Jersey Institute of Technology, Newark, NJ 07102, USA ARTICLE INFO ABSTRACT Keywords: We develop efficient Monte Carlo methods for estimating the failure probability of a system. An example of the Probabilistic safety assessment problem comes from an approach for probabilistic safety assessment of nuclear power plants known as risk- Risk analysis informed safety-margin characterization, but it also arises in other contexts, e.g., structural reliability, Structural reliability catastrophe modeling, and finance. We estimate the failure probability using different combinations of Uncertainty simulation methodologies, including stratified sampling (SS), (replicated) Latin hypercube sampling (LHS), Monte Carlo and conditional Monte Carlo (CMC). We prove theorems establishing that the combination SS+LHS (resp., SS Variance reduction Confidence intervals +CMC+LHS) has smaller asymptotic variance than SS (resp., SS+LHS). We also devise asymptotically valid (as Nuclear regulation the overall sample size grows large) upper confidence bounds for the failure probability for the methods Risk-informed safety-margin characterization considered. The confidence bounds may be employed to perform an asymptotically valid probabilistic safety assessment. We present numerical results demonstrating that the combination SS+CMC+LHS can result in substantial variance reductions compared to stratified sampling alone. -
A Review of Graph and Network Complexity from an Algorithmic Information Perspective
entropy Review A Review of Graph and Network Complexity from an Algorithmic Information Perspective Hector Zenil 1,2,3,4,5,*, Narsis A. Kiani 1,2,3,4 and Jesper Tegnér 2,3,4,5 1 Algorithmic Dynamics Lab, Centre for Molecular Medicine, Karolinska Institute, 171 77 Stockholm, Sweden; [email protected] 2 Unit of Computational Medicine, Department of Medicine, Karolinska Institute, 171 77 Stockholm, Sweden; [email protected] 3 Science for Life Laboratory (SciLifeLab), 171 77 Stockholm, Sweden 4 Algorithmic Nature Group, Laboratoire de Recherche Scientifique (LABORES) for the Natural and Digital Sciences, 75005 Paris, France 5 Biological and Environmental Sciences and Engineering Division (BESE), King Abdullah University of Science and Technology (KAUST), Thuwal 23955, Saudi Arabia * Correspondence: [email protected] or [email protected] Received: 21 June 2018; Accepted: 20 July 2018; Published: 25 July 2018 Abstract: Information-theoretic-based measures have been useful in quantifying network complexity. Here we briefly survey and contrast (algorithmic) information-theoretic methods which have been used to characterize graphs and networks. We illustrate the strengths and limitations of Shannon’s entropy, lossless compressibility and algorithmic complexity when used to identify aspects and properties of complex networks. We review the fragility of computable measures on the one hand and the invariant properties of algorithmic measures on the other demonstrating how current approaches to algorithmic complexity are misguided and suffer of similar limitations than traditional statistical approaches such as Shannon entropy. Finally, we review some current definitions of algorithmic complexity which are used in analyzing labelled and unlabelled graphs. This analysis opens up several new opportunities to advance beyond traditional measures. -
Introduction to Bayesian Inference and Modeling Edps 590BAY
Introduction to Bayesian Inference and Modeling Edps 590BAY Carolyn J. Anderson Department of Educational Psychology c Board of Trustees, University of Illinois Fall 2019 Introduction What Why Probability Steps Example History Practice Overview ◮ What is Bayes theorem ◮ Why Bayesian analysis ◮ What is probability? ◮ Basic Steps ◮ An little example ◮ History (not all of the 705+ people that influenced development of Bayesian approach) ◮ In class work with probabilities Depending on the book that you select for this course, read either Gelman et al. Chapter 1 or Kruschke Chapters 1 & 2. C.J. Anderson (Illinois) Introduction Fall 2019 2.2/ 29 Introduction What Why Probability Steps Example History Practice Main References for Course Throughout the coures, I will take material from ◮ Gelman, A., Carlin, J.B., Stern, H.S., Dunson, D.B., Vehtari, A., & Rubin, D.B. (20114). Bayesian Data Analysis, 3rd Edition. Boco Raton, FL, CRC/Taylor & Francis.** ◮ Hoff, P.D., (2009). A First Course in Bayesian Statistical Methods. NY: Sringer.** ◮ McElreath, R.M. (2016). Statistical Rethinking: A Bayesian Course with Examples in R and Stan. Boco Raton, FL, CRC/Taylor & Francis. ◮ Kruschke, J.K. (2015). Doing Bayesian Data Analysis: A Tutorial with JAGS and Stan. NY: Academic Press.** ** There are e-versions these of from the UofI library. There is a verson of McElreath, but I couldn’t get if from UofI e-collection. C.J. Anderson (Illinois) Introduction Fall 2019 3.3/ 29 Introduction What Why Probability Steps Example History Practice Bayes Theorem A whole semester on this? p(y|θ)p(θ) p(θ|y)= p(y) where ◮ y is data, sample from some population. -
Autocorrelation
Autocorrelation David Gerbing School of Business Administration Portland State University January 30, 2016 Autocorrelation The difference between an actual data value and the forecasted data value from a model is the residual for that forecasted value. Residual: ei = Yi − Y^i One of the assumptions of the least squares estimation procedure for the coefficients of a regression model is that the residuals are purely random. One consequence of randomness is that the residuals would not correlate with anything else, including with each other at different time points. A value above the mean, that is, a value with a positive residual, would contain no information as to whether the next value in time would have a positive residual, or negative residual, with a data value below the mean. For example, flipping a fair coin yields random flips, with half of the flips resulting in a Head and the other half a Tail. If a Head is scored as a 1 and a Tail as a 0, and the probability of both Heads and Tails is 0.5, then calculate the value of the population mean as: Population Mean: µ = (0:5)(1) + (0:5)(0) = :5 The forecast of the outcome of the next flip of a fair coin is the mean of the process, 0.5, which is stable over time. What are the corresponding residuals? A residual value is the difference of the corresponding data value minus the mean. With this scoring system, a Head generates a positive residual from the mean, µ, Head: ei = 1 − µ = 1 − 0:5 = 0:5 A Tail generates a negative residual from the mean, Tail: ei = 0 − µ = 0 − 0:5 = −0:5 The error terms of the coin flips are independent of each other, so if the current flip is a Head, or if the last 5 flips are Heads, the forecast for the next flip is still µ = :5. -
Mild Vs. Wild Randomness: Focusing on Those Risks That Matter
with empirical sense1. Granted, it has been Mild vs. Wild Randomness: tinkered with using such methods as Focusing on those Risks that complementary “jumps”, stress testing, regime Matter switching or the elaborate methods known as GARCH, but while they represent a good effort, Benoit Mandelbrot & Nassim Nicholas Taleb they fail to remediate the bell curve’s irremediable flaws. Forthcoming in, The Known, the Unknown and the The problem is that measures of uncertainty Unknowable in Financial Institutions Frank using the bell curve simply disregard the possibility Diebold, Neil Doherty, and Richard Herring, of sharp jumps or discontinuities. Therefore they editors, Princeton: Princeton University Press. have no meaning or consequence. Using them is like focusing on the grass and missing out on the (gigantic) trees. Conventional studies of uncertainty, whether in statistics, economics, finance or social science, In fact, while the occasional and unpredictable have largely stayed close to the so-called “bell large deviations are rare, they cannot be dismissed curve”, a symmetrical graph that represents a as “outliers” because, cumulatively, their impact in probability distribution. Used to great effect to the long term is so dramatic. describe errors in astronomical measurement by The good news, especially for practitioners, is the 19th-century mathematician Carl Friedrich that the fractal model is both intuitively and Gauss, the bell curve, or Gaussian model, has computationally simpler than the Gaussian. It too since pervaded our business and scientific culture, has been around since the sixties, which makes us and terms like sigma, variance, standard deviation, wonder why it was not implemented before. correlation, R-square and Sharpe ratio are all The traditional Gaussian way of looking at the directly linked to it. -
Random Variables and Applications
Random Variables and Applications OPRE 6301 Random Variables. As noted earlier, variability is omnipresent in the busi- ness world. To model variability probabilistically, we need the concept of a random variable. A random variable is a numerically valued variable which takes on different values with given probabilities. Examples: The return on an investment in a one-year period The price of an equity The number of customers entering a store The sales volume of a store on a particular day The turnover rate at your organization next year 1 Types of Random Variables. Discrete Random Variable: — one that takes on a countable number of possible values, e.g., total of roll of two dice: 2, 3, ..., 12 • number of desktops sold: 0, 1, ... • customer count: 0, 1, ... • Continuous Random Variable: — one that takes on an uncountable number of possible values, e.g., interest rate: 3.25%, 6.125%, ... • task completion time: a nonnegative value • price of a stock: a nonnegative value • Basic Concept: Integer or rational numbers are discrete, while real numbers are continuous. 2 Probability Distributions. “Randomness” of a random variable is described by a probability distribution. Informally, the probability distribution specifies the probability or likelihood for a random variable to assume a particular value. Formally, let X be a random variable and let x be a possible value of X. Then, we have two cases. Discrete: the probability mass function of X specifies P (x) P (X = x) for all possible values of x. ≡ Continuous: the probability density function of X is a function f(x) that is such that f(x) h P (x < · ≈ X x + h) for small positive h. -
Basic Statistics and Monte-Carlo Method -2
Applied Statistical Mechanics Lecture Note - 10 Basic Statistics and Monte-Carlo Method -2 고려대학교 화공생명공학과 강정원 Table of Contents 1. General Monte Carlo Method 2. Variance Reduction Techniques 3. Metropolis Monte Carlo Simulation 1.1 Introduction Monte Carlo Method Any method that uses random numbers Random sampling the population Application • Science and engineering • Management and finance For given subject, various techniques and error analysis will be presented Subject : evaluation of definite integral b I = ρ(x)dx a 1.1 Introduction Monte Carlo method can be used to compute integral of any dimension d (d-fold integrals) Error comparison of d-fold integrals Simpson’s rule,… E ∝ N −1/ d − Monte Carlo method E ∝ N 1/ 2 purely statistical, not rely on the dimension ! Monte Carlo method WINS, when d >> 3 1.2 Hit-or-Miss Method Evaluation of a definite integral b I = ρ(x)dx a h X X X ≥ ρ X h (x) for any x X Probability that a random point reside inside X O the area O O I N' O O r = ≈ O O (b − a)h N a b N : Total number of points N’ : points that reside inside the region N' I ≈ (b − a)h N 1.2 Hit-or-Miss Method Start Set N : large integer N’ = 0 h X X X X X Choose a point x in [a,b] = − + X Loop x (b a)u1 a O N times O O y = hu O O Choose a point y in [0,h] 2 O O a b if [x,y] reside inside then N’ = N’+1 I = (b-a) h (N’/N) End 1.2 Hit-or-Miss Method Error Analysis of the Hit-or-Miss Method It is important to know how accurate the result of simulations are The rule of 3σ’s Identifying Random Variable N = 1 X X n N n=1 From