The Nobel Memorial Prize for Robert F. Engle
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Financial Econometrics Lecture Notes
Financial Econometrics Lecture Notes Professor Doron Avramov The Hebrew University of Jerusalem & Chinese University of Hong Kong Introduction: Why do we need a course in Financial Econometrics? 2 Professor Doron Avramov, Financial Econometrics Syllabus: Motivation The past few decades have been characterized by an extraordinary growth in the use of quantitative methods in the analysis of various asset classes; be it equities, fixed income securities, commodities, and derivatives. In addition, financial economists have routinely been using advanced mathematical, statistical, and econometric techniques in a host of applications including investment decisions, risk management, volatility modeling, interest rate modeling, and the list goes on. 3 Professor Doron Avramov, Financial Econometrics Syllabus: Objectives This course attempts to provide a fairly deep understanding of such techniques. The purpose is twofold, to provide research tools in financial economics and comprehend investment designs employed by practitioners. The course is intended for advanced master and PhD level students in finance and economics. 4 Professor Doron Avramov, Financial Econometrics Syllabus: Prerequisite I will assume prior exposure to matrix algebra, distribution theory, Ordinary Least Squares, Maximum Likelihood Estimation, Method of Moments, and the Delta Method. I will also assume you have some skills in computer programing beyond Excel. MATLAB and R are the most recommended for this course. OCTAVE could be used as well, as it is a free software, and is practically identical to MATLAB when considering the scope of the course. If you desire to use STATA, SAS, or other comparable tools, please consult with the TA. 5 Professor Doron Avramov, Financial Econometrics Syllabus: Grade Components Assignments (36%): there will be two problem sets during the term. -
Stationary Processes and Their Statistical Properties
Stationary Processes and Their Statistical Properties Brian Borchers March 29, 2001 1 Stationary processes A discrete time stochastic process is a sequence of random variables Z1, Z2, :::. In practice we will typically analyze a single realization z1, z2, :::, zn of the stochastic process and attempt to esimate the statistical properties of the stochastic process from the realization. We will also consider the problem of predicting zn+1 from the previous elements of the sequence. We will begin by focusing on the very important class of stationary stochas- tic processes. A stochastic process is strictly stationary if its statistical prop- erties are unaffected by shifting the stochastic process in time. In particular, this means that if we take a subsequence Zk+1, :::, Zk+m, then the joint distribution of the m random variables will be the same no matter what k is. Stationarity requires that the mean of the stochastic process be a constant. E[Zk] = µ. and that the variance is constant 2 V ar[Zk] = σZ : Also, stationarity requires that the covariance of two elements separated by a distance m is constant. That is, Cov(Zk;Zk+m) is constant. This covariance is called the autocovariance at lag m, and we will use the notation γm. Since Cov(Zk;Zk+m) = Cov(Zk+m;Zk), we need only find γm for m 0. The ≥ correlation of Zk and Zk+m is the autocorrelation at lag m. We will use the notation ρm for the autocorrelation. It is easy to show that γk ρk = : γ0 1 2 The autocovariance and autocorrelation ma- trices The covariance matrix for the random variables Z1, :::, Zn is called an auto- covariance matrix. -
Methods of Monte Carlo Simulation II
Methods of Monte Carlo Simulation II Ulm University Institute of Stochastics Lecture Notes Dr. Tim Brereton Summer Term 2014 Ulm, 2014 2 Contents 1 SomeSimpleStochasticProcesses 7 1.1 StochasticProcesses . 7 1.2 RandomWalks .......................... 7 1.2.1 BernoulliProcesses . 7 1.2.2 RandomWalks ...................... 10 1.2.3 ProbabilitiesofRandomWalks . 13 1.2.4 Distribution of Xn .................... 13 1.2.5 FirstPassageTime . 14 2 Estimators 17 2.1 Bias, Variance, the Central Limit Theorem and Mean Square Error................................ 19 2.2 Non-AsymptoticErrorBounds. 22 2.3 Big O and Little o Notation ................... 23 3 Markov Chains 25 3.1 SimulatingMarkovChains . 28 3.1.1 Drawing from a Discrete Uniform Distribution . 28 3.1.2 Drawing From A Discrete Distribution on a Small State Space ........................... 28 3.1.3 SimulatingaMarkovChain . 28 3.2 Communication .......................... 29 3.3 TheStrongMarkovProperty . 30 3.4 RecurrenceandTransience . 31 3.4.1 RecurrenceofRandomWalks . 33 3.5 InvariantDistributions . 34 3.6 LimitingDistribution. 36 3.7 Reversibility............................ 37 4 The Poisson Process 39 4.1 Point Processes on [0, )..................... 39 ∞ 3 4 CONTENTS 4.2 PoissonProcess .......................... 41 4.2.1 Order Statistics and the Distribution of Arrival Times 44 4.2.2 DistributionofArrivalTimes . 45 4.3 SimulatingPoissonProcesses. 46 4.3.1 Using the Infinitesimal Definition to Simulate Approx- imately .......................... 46 4.3.2 SimulatingtheArrivalTimes . 47 4.3.3 SimulatingtheInter-ArrivalTimes . 48 4.4 InhomogenousPoissonProcesses. 48 4.5 Simulating an Inhomogenous Poisson Process . 49 4.5.1 Acceptance-Rejection. 49 4.5.2 Infinitesimal Approach (Approximate) . 50 4.6 CompoundPoissonProcesses . 51 5 ContinuousTimeMarkovChains 53 5.1 TransitionFunction. 53 5.2 InfinitesimalGenerator . 54 5.3 ContinuousTimeMarkovChains . -
Wavelet Entropy Energy Measure (WEEM): a Multiscale Measure to Grade a Geophysical System's Predictability
EGU21-703, updated on 28 Sep 2021 https://doi.org/10.5194/egusphere-egu21-703 EGU General Assembly 2021 © Author(s) 2021. This work is distributed under the Creative Commons Attribution 4.0 License. Wavelet Entropy Energy Measure (WEEM): A multiscale measure to grade a geophysical system's predictability Ravi Kumar Guntu and Ankit Agarwal Indian Institute of Technology Roorkee, Hydrology, Roorkee, India ([email protected]) Model-free gradation of predictability of a geophysical system is essential to quantify how much inherent information is contained within the system and evaluate different forecasting methods' performance to get the best possible prediction. We conjecture that Multiscale Information enclosed in a given geophysical time series is the only input source for any forecast model. In the literature, established entropic measures dealing with grading the predictability of a time series at multiple time scales are limited. Therefore, we need an additional measure to quantify the information at multiple time scales, thereby grading the predictability level. This study introduces a novel measure, Wavelet Entropy Energy Measure (WEEM), based on Wavelet entropy to investigate a time series's energy distribution. From the WEEM analysis, predictability can be graded low to high. The difference between the entropy of a wavelet energy distribution of a time series and entropy of wavelet energy of white noise is the basis for gradation. The metric quantifies the proportion of the deterministic component of a time series in terms of energy concentration, and its range varies from zero to one. One corresponds to high predictable due to its high energy concentration and zero representing a process similar to the white noise process having scattered energy distribution. -
Examples of Stationary Time Series
Statistics 910, #2 1 Examples of Stationary Time Series Overview 1. Stationarity 2. Linear processes 3. Cyclic models 4. Nonlinear models Stationarity Strict stationarity (Defn 1.6) Probability distribution of the stochastic process fXtgis invariant under a shift in time, P (Xt1 ≤ x1;Xt2 ≤ x2;:::;Xtk ≤ xk) = F (xt1 ; xt2 ; : : : ; xtk ) = F (xh+t1 ; xh+t2 ; : : : ; xh+tk ) = P (Xh+t1 ≤ x1;Xh+t2 ≤ x2;:::;Xh+tk ≤ xk) for any time shift h and xj. Weak stationarity (Defn 1.7) (aka, second-order stationarity) The mean and autocovariance of the stochastic process are finite and invariant under a shift in time, E Xt = µt = µ Cov(Xt;Xs) = E (Xt−µt)(Xs−µs) = γ(t; s) = γ(t−s) The separation rather than location in time matters. Equivalence If the process is Gaussian with finite second moments, then weak stationarity is equivalent to strong stationarity. Strict stationar- ity implies weak stationarity only if the necessary moments exist. Relevance Stationarity matters because it provides a framework in which averaging makes sense. Unless properties like the mean and covariance are either fixed or \evolve" in a known manner, we cannot average the observed data. What operations produce a stationary process? Can we recognize/identify these in data? Statistics 910, #2 2 Moving Average White noise Sequence of uncorrelated random variables with finite vari- ance, ( 2 often often σw = 1 if t = s; E Wt = µ = 0 Cov(Wt;Ws) = 0 otherwise The input component (fXtg in what follows) is often modeled as white noise. Strict white noise replaces uncorrelated by independent. Moving average A stochastic process formed by taking a weighted average of another time series, often formed from white noise. -
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. -
Biostatistics for Oral Healthcare
Biostatistics for Oral Healthcare Jay S. Kim, Ph.D. Loma Linda University School of Dentistry Loma Linda, California 92350 Ronald J. Dailey, Ph.D. Loma Linda University School of Dentistry Loma Linda, California 92350 Biostatistics for Oral Healthcare Biostatistics for Oral Healthcare Jay S. Kim, Ph.D. Loma Linda University School of Dentistry Loma Linda, California 92350 Ronald J. Dailey, Ph.D. Loma Linda University School of Dentistry Loma Linda, California 92350 JayS.Kim, PhD, is Professor of Biostatistics at Loma Linda University, CA. A specialist in this area, he has been teaching biostatistics since 1997 to students in public health, medical school, and dental school. Currently his primary responsibility is teaching biostatistics courses to hygiene students, predoctoral dental students, and dental residents. He also collaborates with the faculty members on a variety of research projects. Ronald J. Dailey is the Associate Dean for Academic Affairs at Loma Linda and an active member of American Dental Educational Association. C 2008 by Blackwell Munksgaard, a Blackwell Publishing Company Editorial Offices: Blackwell Publishing Professional, 2121 State Avenue, Ames, Iowa 50014-8300, USA Tel: +1 515 292 0140 9600 Garsington Road, Oxford OX4 2DQ Tel: 01865 776868 Blackwell Publishing Asia Pty Ltd, 550 Swanston Street, Carlton South, Victoria 3053, Australia Tel: +61 (0)3 9347 0300 Blackwell Wissenschafts Verlag, Kurf¨urstendamm57, 10707 Berlin, Germany Tel: +49 (0)30 32 79 060 The right of the Author to be identified as the Author of this Work has been asserted in accordance with the Copyright, Designs and Patents Act 1988. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, except as permitted by the UK Copyright, Designs and Patents Act 1988, without the prior permission of the publisher. -
Stationary Processes
Stationary processes Alejandro Ribeiro Dept. of Electrical and Systems Engineering University of Pennsylvania [email protected] http://www.seas.upenn.edu/users/~aribeiro/ November 25, 2019 Stoch. Systems Analysis Stationary processes 1 Stationary stochastic processes Stationary stochastic processes Autocorrelation function and wide sense stationary processes Fourier transforms Linear time invariant systems Power spectral density and linear filtering of stochastic processes Stoch. Systems Analysis Stationary processes 2 Stationary stochastic processes I All probabilities are invariant to time shits, i.e., for any s P[X (t1 + s) ≥ x1; X (t2 + s) ≥ x2;:::; X (tK + s) ≥ xK ] = P[X (t1) ≥ x1; X (t2) ≥ x2;:::; X (tK ) ≥ xK ] I If above relation is true process is called strictly stationary (SS) I First order stationary ) probs. of single variables are shift invariant P[X (t + s) ≥ x] = P [X (t) ≥ x] I Second order stationary ) joint probs. of pairs are shift invariant P[X (t1 + s) ≥ x1; X (t2 + s) ≥ x2] = P [X (t1) ≥ x1; X (t2) ≥ x2] Stoch. Systems Analysis Stationary processes 3 Pdfs and moments of stationary process I For SS process joint cdfs are shift invariant. Whereby, pdfs also are fX (t+s)(x) = fX (t)(x) = fX (0)(x) := fX (x) I As a consequence, the mean of a SS process is constant Z 1 Z 1 µ(t) := E [X (t)] = xfX (t)(x) = xfX (x) = µ −∞ −∞ I The variance of a SS process is also constant Z 1 Z 1 2 2 2 var [X (t)] := (x − µ) fX (t)(x) = (x − µ) fX (x) = σ −∞ −∞ I The power of a SS process (second moment) is also constant Z 1 Z 1 2 2 2 2 2 E X (t) := x fX (t)(x) = x fX (x) = σ + µ −∞ −∞ Stoch. -
Advanced Financial Econometrics
MFE 2013-14 Trinity Term | Advanced Financial Econometrics Advanced Financial Econometrics Kevin Sheppard Department of Economics Oxford-Man Institute of Quantitative Finance Course Site: http://www.kevinsheppard.com/Advanced_Econometrics Weblearn Site: https://weblearn.ox.ac.uk/portal/site/socsci/sbs/mfe2012_2013/ttafe 1 Aims, objectives and intended learning outcomes 1.1 Basic aims This course aims to extend the core tools of Financial Econometrics I & II to some advanced forecasting problems. The first component covers techniques for working with many forecasting models – often referred to as data snoop- ing. The second component covers techniques for handling many predictors – including the case where the number of predictors is much larger than the number of data points available. 1.2 Specific objectives Part I (Week 1 – 4) Revisiting the bootstrap and extensions appropriate for time-series data • Technical trading rules and large number of forecasts • Formalized data-snooping robust inference • False-discovery rates • Detecting sets of models that are statistically indistinguishable • Part I (Week 5 – 8) Dynamic Factor Models and Principal Component Analysis • The Kalman Filter and Expectations-Maximization Algorithm • Partial Least Squares and the 3-pass Regression Filter • Regularized Reduced Rank Regression • 1.3 Intended learning outcomes Following class attendance, successful completion of assigned readings, assignments, both theoretical and empiri- cal, and recommended private study, students should be able to Detect superior performance using methods that are robust to data snooping • Produce and evaluate forecasts in for macro-financial time series in data-rich environments • 1 2 Teaching resources 2.1 Lecturing Lectures are provided by Kevin Sheppard. Kevin Sheppard is an Associate Professor and a fellow at Keble College. -
Testing for Cointegration When Some of The
EconometricTheory, 11, 1995, 984-1014. Printed in the United States of America. TESTINGFOR COINTEGRATION WHEN SOME OF THE COINTEGRATINGVECTORS ARE PRESPECIFIED MICHAELT.K. HORVATH Stanford University MARKW. WATSON Princeton University Manyeconomic models imply that ratios, simpledifferences, or "spreads"of variablesare I(O).In these models, cointegratingvectors are composedof l's, O's,and - l's and containno unknownparameters. In this paper,we develop tests for cointegrationthat can be appliedwhen some of the cointegratingvec- tors are prespecifiedunder the null or underthe alternativehypotheses. These tests are constructedin a vectorerror correction model and are motivatedas Waldtests from a Gaussianversion of the model. Whenall of the cointegrat- ing vectorsare prespecifiedunder the alternative,the tests correspondto the standardWald tests for the inclusionof errorcorrection terms in the VAR. Modificationsof this basictest are developedwhen a subsetof the cointegrat- ing vectorscontain unknown parameters. The asymptoticnull distributionsof the statisticsare derived,critical values are determined,and the local power propertiesof the test are studied.Finally, the test is appliedto data on for- eign exchangefuture and spot pricesto test the stabilityof the forward-spot premium. 1. INTRODUCTION Economic models often imply that variables are cointegrated with simple and known cointegrating vectors. Examples include the neoclassical growth model, which implies that income, consumption, investment, and the capi- tal stock will grow in a balanced way, so that any stochastic growth in one of the series must be matched by corresponding growth in the others. Asset This paper has benefited from helpful comments by Neil Ericsson, Gordon Kemp, Andrew Levin, Soren Johansen, John McDermott, Pierre Perron, Peter Phillips, James Stock, and three referees. -
An Introduction to Financial Econometrics
An introduction to financial econometrics Jianqing Fan Department of Operation Research and Financial Engineering Princeton University Princeton, NJ 08544 November 14, 2004 What is the financial econometrics? This simple question does not have a simple answer. The boundary of such an interdisciplinary area is always moot and any attempt to give a formal definition is unlikely to be successful. Broadly speaking, financial econometrics is to study quantitative problems arising from finance. It uses sta- tistical techniques and economic theory to address a variety of problems from finance. These include building financial models, estimation and inferences of financial models, volatility estimation, risk management, testing financial economics theory, capital asset pricing, derivative pricing, portfolio allocation, risk-adjusted returns, simulating financial systems, hedging strategies, among others. Technological invention and trade globalization have brought us into a new era of financial markets. Over the last three decades, enormous number of new financial products have been created to meet customers’ demands. For example, to reduce the impact of the fluctuations of currency exchange rates on a firm’s finance, which makes its profit more predictable and competitive, a multinational corporation may decide to buy the options on the future of foreign exchanges; to reduce the risk of price fluctuations of a commodity (e.g. lumbers, corns, soybeans), a farmer may enter into the future contracts of the commodity; to reduce the risk of weather exposures, amuse parks (too hot or too cold reduces the number of visitors) and energy companies may decide to purchase the financial derivatives based on the temperature. An important milestone is that in the year 1973, the world’s first options exchange opened in Chicago. -
Big Data for Reliability Engineering: Threat and Opportunity
Reliability, February 2016 Big Data for Reliability Engineering: Threat and Opportunity Vitali Volovoi Independent Consultant [email protected] more recently, analytics). It shares with the rest of the fields Abstract - The confluence of several technologies promises under this umbrella the need to abstract away most stormy waters ahead for reliability engineering. News reports domain-specific information, and to use tools that are mainly are full of buzzwords relevant to the future of the field—Big domain-independent1. As a result, it increasingly shares the Data, the Internet of Things, predictive and prescriptive lingua franca of modern systems engineering—probability and analytics—the sexier sisters of reliability engineering, both statistics that are required to balance the otherwise orderly and exciting and threatening. Can we reliability engineers join the deterministic engineering world. party and suddenly become popular (and better paid), or are And yet, reliability engineering does not wear the fancy we at risk of being superseded and driven into obsolescence? clothes of its sisters. There is nothing privileged about it. It is This article argues that“big-picture” thinking, which is at the rarely studied in engineering schools, and it is definitely not core of the concept of the System of Systems, is key for a studied in business schools! Instead, it is perceived as a bright future for reliability engineering. necessary evil (especially if the reliability issues in question are safety-related). The community of reliability engineers Keywords - System of Systems, complex systems, Big Data, consists of engineers from other fields who were mainly Internet of Things, industrial internet, predictive analytics, trained on the job (instead of receiving formal degrees in the prescriptive analytics field).