Review from last time Time Series Analysis, Fall 2007 Professor Anna Mikusheva Paul Schrimpf, scribe October 23, 2007.
|
|
- Darrell Gerald Mosley
- 6 years ago
- Views:
Transcription
1 Review fro last tie 4384 ie Series Analsis, Fall 007 Professor Anna Mikusheva Paul Schrif, scribe October 3, 007 Lecture 3 Unit Roots Review fro last tie Let t be a rando walk t = ρ t + ɛ t, ρ = where ɛ t is a artingale difference sequence (E[ɛ t I t] = 0, with E[ɛ It ] σ as and E ɛ 4 t t < K < hen {ɛ t } satisf a functional central liit theore, ξ (τ = [τ ] ɛt t= σ ( e showed last tie that: σ (td (t σ (t 0 σ (t t ɛ t 3/ t t 0 0 and our OLS estiator and t-statistic have non-standard distributions: d ( ρˆ ρ d t his is quite different fro the case with ρ < If x t = ρx t + ɛ t, ρ < then, xt ɛ t x 3/ t x t σ N(0, 4 ρ Ex t = 0 Ex t = σ ρ and the OLS estiate and t-stat converge to noral distributions: (ρˆ ρ N(0, ( ρ t N(0, Cite as: Anna Mikusheva, course aterials for 4384 ie Series Analsis, Fall 007 MI OenCourseare (htt://ocwitedu, Massachusetts Institute of echnolog Downloaded on [DD Month YYYY]
2 Adding a constant Adding a constant Suose we add a constant to our OLS regression of t his is equivalent to running OLS on deeaned t Let t = t ȳ hen, ρˆ = t ɛ t ( t Consider the nuerator: t ɛ t = ( t ȳɛ t = t ɛ t ȳɛ ȳɛ = 3/ t ɛ t e know that t σ, and 3/ we know that t ɛ t σ d Cobining this, we have: ( t ɛ t σ (sd (s ( ɛt σ ( Also, fro before (t e can think of this as the integral of a deeaned Brownian otion, ( (sd (s ( (t = (s (t d (s = (sd (s he liiting distributions of all statistics (ρˆ, t, etc would change In ost cases, the change is onl in relacing b one also can include a linear trend in the regression, then the liiting distribution would deend on a detrended Brownian otion Liiting Distribution Let s R return to the case without a constant he liiting distribution of the OLS esitate is (ρˆ R d his distribution is skewed and shifted to the left If we include a constant, the distribution is even ore shifted If we also include a trend, the distribution shifts et ore For exale, the 5%-tile without a constant is -05, with a constant is -69, and with a trend is -5 he 975%-tiles are 6, 04, and -8, resectivel hus, estiates of ρ have bias of order his bias is quite large in sall sales he distribution of the t-statistic is also shifted to the left and skewed, but less so than the distribution of the OLS estiate he 5%-tiles are -3, -3, -366 and of the 975%-tiles are 6, 03, and -066 for no constant, with a constant, and with a trend, resectivel Allowing Auto-correlation So far, we have assued that ɛ t are not correlated his assution is too strong for eirical work Let, t = t + v t where v t is a zero-ean stationar rocess with an MA reresentation, v t = c j ɛ j j=0 Cite as: Anna Mikusheva, course aterials for 4384 ie Series Analsis, Fall 007 MI OenCourseare (htt://ocwitedu, Massachusetts Institute of echnolog Downloaded on [DD Month YYYY]
3 Augented Dicke Fuller 3 where ɛ j is white noise Now we need to look at the liiting distributions of each of the ters we looked at before ( v t, t v t, t, etc v t is a ter we alread encountered in HAC estiation: where ω is the long-ter variance, vt N(0, ω t= ω = γj = σ c( ω j= For linearl deendent rocess, v t, we have the following central liit theore: ξ (τ = [ τ] vt t= ω ( his can be roven b using the Beveridge-Nelson decoosition All the other ters converge to things siilar to the uncorrelated case, excet with σ relaced b ω For exale, An excetion is: = ξ (t/ ω (t/ 3/ t ω (sds t v t = his leads to an extra constant in the distribution of ρˆ: t v (ω ( σ v ω ω d + σ v (ρˆ d ω σ v ω so it is iossible to just look u critical values in a table Phillis & Perron (988 suggested corrected statistics: ωˆ σˆv d (ρˆ + where ωˆ t is an estiate of the long-run variance, sa Newe-est, and σˆv is the variance of the residuals Augented Dicke Fuller Another aroach is the augented Dicke-Fuller test Suose, t = a j t j + ɛ t j= Cite as: Anna Mikusheva, course aterials for 4384 ie Series Analsis, Fall 007 MI OenCourseare (htt://ocwitedu, Massachusetts Institute of echnolog Downloaded on [DD Month YYYY]
4 Augented Dicke Fuller 4 where z = is a root, Suose we factor a(l as a j z j =0 j= with b(l = j j= β jl e can write the odel as his suggests estiating: = a j a j L j = ( Lb(L j t = β j t + ɛ t i= t = ρ t + β j t + ɛ t j i= and testing whether ρ = to see if we have a unit root his is another wa of allowing auto-correlation because we can write the odel as: a(l t =ɛ t b(l t =ɛ t t = t + v t t =b(l ɛ t where v t = b(l ɛ t is auto-correlated he nice thing about the augeented Dicke-Fuller test is that the coefficients on t j each converge to a noral distribution at rate, and the coefficient on t converges to a non-standard distribution without nuisance araeters o see this, let x t = [ t, t,, t + ] and let θ = [ρ, β,, β ] Consider: θˆ θ = (X X (X ɛ e need to noralize this so that it converges Our noralizing atrix will be Q = 0 Multiling b Q gives: ˆ Q(θ θ =(Q (X X Q (Q X ɛ he denoinator is: Q (X X Q = t t 3/ t t 3/ t X X Cite as: Anna Mikusheva, course aterials for 4384 ie Series Analsis, Fall 007 MI OenCourseare (htt://ocwitedu, Massachusetts Institute of echnolog Downloaded on [DD Month YYYY]
5 Other ests 5 Note that t 3/ t j 0 Also, we know that t ω, so ω 0 Q (X X Q 0 EX X Siilarl, ( Q X ɛ = ( t ɛ t σω d t j ɛ t N(0, E[X X]σ hus, or ωˆ (ρˆ σˆ σ d (ρˆ ω (ρˆ = d βˆ j Other ests Sargan-Bhargrava (983 look at: For a non-stationar rocess, the variance of t grows with tie, so we could when ɛ t is an ds, this converges to a distribution, converges to 0 in robabilit t t P t P t ( For a stationar rocess, this Range (Mandelbrot and coauthors You could also look at the range of t, this should blow u for non-stationar rocesses for a rando walk, we have: est Coarison (ax t in t su (λ t λ inf (λ λ he Sargan-Bhargrava (983 test has otial astotic ower against local alternatives, but has bad size distortions in sall sales, eseciall if errors are negativel autocorrelated he augented Dicke-Fuller test with the BIC used to choose lag-length has overall good size in finite sales Cite as: Anna Mikusheva, course aterials for 4384 ie Series Analsis, Fall 007 MI OenCourseare (htt://ocwitedu, Massachusetts Institute of echnolog Downloaded on [DD Month YYYY]
13.2 Fully Polynomial Randomized Approximation Scheme for Permanent of Random 0-1 Matrices
CS71 Randoness & Coputation Spring 018 Instructor: Alistair Sinclair Lecture 13: February 7 Disclaier: These notes have not been subjected to the usual scrutiny accorded to foral publications. They ay
More informationChange-point detection for recursive Bayesian geoacoustic inversion
Change-oint detection for recursive Baesian geoacoustic inversion Bien Aik Tan Peter Gerstoft Caglar Yardi and Willia S. Hodgkiss Universit of California San Diego htt://www.l.ucsd.edu/eole/btan/ Overview
More information[95/95] APPROACH FOR DESIGN LIMITS ANALYSIS IN VVER. Shishkov L., Tsyganov S. Russian Research Centre Kurchatov Institute Russian Federation, Moscow
[95/95] APPROACH FOR DESIGN LIMITS ANALYSIS IN VVER Shishkov L., Tsyganov S. Russian Research Centre Kurchatov Institute Russian Federation, Moscow ABSTRACT The aer discusses a well-known condition [95%/95%],
More informationBinomial and Poisson Probability Distributions
Binoial and Poisson Probability Distributions There are a few discrete robability distributions that cro u any ties in hysics alications, e.g. QM, SM. Here we consider TWO iortant and related cases, the
More informationSome simple continued fraction expansions for an in nite product Part 1. Peter Bala, January ax 4n+3 1 ax 4n+1. (a; x) =
Soe sile continued fraction exansions for an in nite roduct Part. Introduction The in nite roduct Peter Bala, January 3 (a; x) = Y ax 4n+3 ax 4n+ converges for arbitrary colex a rovided jxj
More informationA Simple Regression Problem
A Siple Regression Proble R. M. Castro March 23, 2 In this brief note a siple regression proble will be introduced, illustrating clearly the bias-variance tradeoff. Let Y i f(x i ) + W i, i,..., n, where
More information1 Brownian motion and the Langevin equation
Figure 1: The robust appearance of Robert Brown (1773 1858) 1 Brownian otion and the Langevin equation In 1827, while exaining pollen grains and the spores of osses suspended in water under a icroscope,
More informationModi ed Local Whittle Estimator for Long Memory Processes in the Presence of Low Frequency (and Other) Contaminations
Modi ed Local Whittle Estiator for Long Meory Processes in the Presence of Low Frequency (and Other Containations Jie Hou y Boston University Pierre Perron z Boston University March 5, 203; Revised: January
More informationQuestions and Answers on Unit Roots, Cointegration, VARs and VECMs
Questions and Answers on Unit Roots, Cointegration, VARs and VECMs L. Magee Winter, 2012 1. Let ɛ t, t = 1,..., T be a series of independent draws from a N[0,1] distribution. Let w t, t = 1,..., T, be
More informationTime Series Analysis Fall 2008
MIT OpenCourseWare http://ocw.mit.edu 14.384 Time Series Analysis Fall 008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. Introduction 1 14.384 Time
More informationTEST OF HOMOGENEITY OF PARALLEL SAMPLES FROM LOGNORMAL POPULATIONS WITH UNEQUAL VARIANCES
TEST OF HOMOGENEITY OF PARALLEL SAMPLES FROM LOGNORMAL POPULATIONS WITH UNEQUAL VARIANCES S. E. Ahed, R. J. Tokins and A. I. Volodin Departent of Matheatics and Statistics University of Regina Regina,
More information1 Introduction to Generalized Least Squares
ECONOMICS 7344, Spring 2017 Bent E. Sørensen April 12, 2017 1 Introduction to Generalized Least Squares Consider the model Y = Xβ + ɛ, where the N K matrix of regressors X is fixed, independent of the
More informationQuadratic Reciprocity. As in the previous notes, we consider the Legendre Symbol, defined by
Math 0 Sring 01 Quadratic Recirocity As in the revious notes we consider the Legendre Sybol defined by $ ˆa & 0 if a 1 if a is a quadratic residue odulo. % 1 if a is a quadratic non residue We also had
More informationRandom Process Review
Rando Process Review Consider a rando process t, and take k saples. For siplicity, we will set k. However it should ean any nuber of saples. t () t x t, t, t We have a rando vector t, t, t. If we find
More informationBlock designs and statistics
Bloc designs and statistics Notes for Math 447 May 3, 2011 The ain paraeters of a bloc design are nuber of varieties v, bloc size, nuber of blocs b. A design is built on a set of v eleents. Each eleent
More informationRisk & Safety in Engineering. Dr. Jochen Köhler
Risk & afety in Engineering Dr. Jochen Köhler Contents of Today's Lecture Introduction to Classical Reliability Theory tructural Reliability The fundaental case afety argin Introduction to Classical Reliability
More informationPlasma-Wall Interaction: Sheath and Pre-sheath
Plasa-Wall Interaction: Sheath and Pre-sheath Under ost conditions, a very thin negative sheath appears in the vicinity of walls, due to accuulation of electrons on the wall. This is in turn necessitated
More information1 Proof of learning bounds
COS 511: Theoretical Machine Learning Lecturer: Rob Schapire Lecture #4 Scribe: Akshay Mittal February 13, 2013 1 Proof of learning bounds For intuition of the following theore, suppose there exists a
More information5. Dimensional Analysis. 5.1 Dimensions and units
5. Diensional Analysis In engineering the alication of fluid echanics in designs ake uch of the use of eirical results fro a lot of exerients. This data is often difficult to resent in a readable for.
More informationEE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng
EE59 Spring Parallel LSI AD Algoriths Lecture I interconnect odeling ethods Zhuo Feng. Z. Feng MTU EE59 So far we ve considered only tie doain analyses We ll soon see that it is soeties preferable to odel
More informationVariance Decomposition
Variance Decomposition 1 14.384 Time Series Analysis, Fall 2007 Recitation by Paul Schrimpf Supplementary to lectures given by Anna Mikusheva October 5, 2007 Recitation 5 Variance Decomposition Suppose
More informationMachine Learning Basics: Estimators, Bias and Variance
Machine Learning Basics: Estiators, Bias and Variance Sargur N. srihari@cedar.buffalo.edu This is part of lecture slides on Deep Learning: http://www.cedar.buffalo.edu/~srihari/cse676 1 Topics in Basics
More informationThe Schrödinger Equation and the Scale Principle
Te Scrödinger Equation and te Scale Princile RODOLFO A. FRINO Jul 014 Electronics Engineer Degree fro te National Universit of Mar del Plata - Argentina rodolfo_frino@aoo.co.ar Earlier tis ear (Ma) I wrote
More informationCSE525: Randomized Algorithms and Probabilistic Analysis May 16, Lecture 13
CSE55: Randoied Algoriths and obabilistic Analysis May 6, Lecture Lecturer: Anna Karlin Scribe: Noah Siegel, Jonathan Shi Rando walks and Markov chains This lecture discusses Markov chains, which capture
More information1. (2.5.1) So, the number of moles, n, contained in a sample of any substance is equal N n, (2.5.2)
Lecture.5. Ideal gas law We have already discussed general rinciles of classical therodynaics. Classical therodynaics is a acroscoic science which describes hysical systes by eans of acroscoic variables,
More informationESTIMATING AND FORMING CONFIDENCE INTERVALS FOR EXTREMA OF RANDOM POLYNOMIALS. A Thesis. Presented to. The Faculty of the Department of Mathematics
ESTIMATING AND FORMING CONFIDENCE INTERVALS FOR EXTREMA OF RANDOM POLYNOMIALS A Thesis Presented to The Faculty of the Departent of Matheatics San Jose State University In Partial Fulfillent of the Requireents
More informationarxiv: v1 [math.ds] 19 Jun 2012
Rates in the strong invariance rincile for ergodic autoorhiss of the torus Jérôe Dedecker a, Florence Merlevède b and Françoise Pène c 1 a Université Paris Descartes, Sorbonne Paris Cité, Laboratoire MAP5
More informationEstimating Parameters for a Gaussian pdf
Pattern Recognition and achine Learning Jaes L. Crowley ENSIAG 3 IS First Seester 00/0 Lesson 5 7 Noveber 00 Contents Estiating Paraeters for a Gaussian pdf Notation... The Pattern Recognition Proble...3
More informationW-BASED VS LATENT VARIABLES SPATIAL AUTOREGRESSIVE MODELS: EVIDENCE FROM MONTE CARLO SIMULATIONS
W-BASED VS LATENT VARIABLES SPATIAL AUTOREGRESSIVE MODELS: EVIDENCE FROM MONTE CARLO SIMULATIONS. Introduction When it coes to applying econoetric odels to analyze georeferenced data, researchers are well
More informationarxiv: v2 [math.st] 11 Dec 2018
esting for high-diensional network paraeters in auto-regressive odels arxiv:803659v [aths] Dec 08 Lili Zheng and Garvesh Raskutti Abstract High-diensional auto-regressive odels provide a natural way to
More informationKeywords: Estimator, Bias, Mean-squared error, normality, generalized Pareto distribution
Testing approxiate norality of an estiator using the estiated MSE and bias with an application to the shape paraeter of the generalized Pareto distribution J. Martin van Zyl Abstract In this work the norality
More informationOnline Supplement. and. Pradeep K. Chintagunta Graduate School of Business University of Chicago
Online Suppleent easuring Cross-Category Price Effects with Aggregate Store Data Inseong Song ksong@usthk Departent of arketing, HKUST Hong Kong University of Science and Technology and Pradeep K Chintagunta
More informationP (t) = P (t = 0) + F t Conclusion: If we wait long enough, the velocity of an electron will diverge, which is obviously impossible and wrong.
4 Phys520.nb 2 Drude theory ~ Chapter in textbook 2.. The relaxation tie approxiation Here we treat electrons as a free ideal gas (classical) 2... Totally ignore interactions/scatterings Under a static
More informationSUPPORTING INFORMATION FOR. Mass Spectrometrically-Detected Statistical Aspects of Ligand Populations in Mixed Monolayer Au 25 L 18 Nanoparticles
SUPPORTIG IFORMATIO FOR Mass Sectroetrically-Detected Statistical Asects of Lig Poulations in Mixed Monolayer Au 25 L 8 anoarticles Aala Dass,,a Kennedy Holt, Joseh F. Parer, Stehen W. Feldberg, Royce
More informationA method to determine relative stroke detection efficiencies from multiplicity distributions
A ethod to deterine relative stroke detection eiciencies ro ultiplicity distributions Schulz W. and Cuins K. 2. Austrian Lightning Detection and Inoration Syste (ALDIS), Kahlenberger Str.2A, 90 Vienna,
More informationThus, the formula weight per C-atom is: 1*12 (g/mol) +1.85*1(g/mol)+0.55*16 (g/mol)+0.13*14(g/mol)=24.5 g/mol.
Proble. a. C: H: O: N47.6%/: 7.%/: (-47.6%-7.%-7.%-.%)/6: 7.%/4:.85:.55:. Therefore, the eleental coposition for the ash-free bioass is CH.85 O.55 N.. Thus, the forula weight per C-ato is: * (g/ol).85*(g/ol).55*6
More informationPseudo-marginal Metropolis-Hastings: a simple explanation and (partial) review of theory
Pseudo-arginal Metropolis-Hastings: a siple explanation and (partial) review of theory Chris Sherlock Motivation Iagine a stochastic process V which arises fro soe distribution with density p(v θ ). Iagine
More informationGeneral Physical Chemistry I
General Physical Cheistry I Lecture 12 Aleksey Kocherzhenko Aril 2, 2015" Last tie " Gibbs free energy" In order to analyze the sontaneity of cheical reactions, we need to calculate the entroy changes
More informationIntroduction to Robotics (CS223A) (Winter 2006/2007) Homework #5 solutions
Introduction to Robotics (CS3A) Handout (Winter 6/7) Hoework #5 solutions. (a) Derive a forula that transfors an inertia tensor given in soe frae {C} into a new frae {A}. The frae {A} can differ fro frae
More informationExtension of CSRSM for the Parametric Study of the Face Stability of Pressurized Tunnels
Extension of CSRSM for the Paraetric Study of the Face Stability of Pressurized Tunnels Guilhe Mollon 1, Daniel Dias 2, and Abdul-Haid Soubra 3, M.ASCE 1 LGCIE, INSA Lyon, Université de Lyon, Doaine scientifique
More informationRandom Process Examples 1/23
ando Process Eaples /3 E. #: D-T White Noise Let ] be a sequence of V s where each V ] in the sequence is uncorrelated with all the others: E{ ] ] } 0 for This DEFINES a DT White Noise Also called Uncorrelated
More informationPattern Recognition and Machine Learning. Artificial Neural networks
Pattern Recognition and Machine Learning Jaes L. Crowley ENSIMAG 3 - MMIS Fall Seester 2016 Lessons 7 14 Dec 2016 Outline Artificial Neural networks Notation...2 1. Introduction...3... 3 The Artificial
More informationVibrations: Two Degrees of Freedom Systems - Wilberforce Pendulum and Bode Plots
.003J/.053J Dynaics and Control, Spring 007 Professor Peacock 5/4/007 Lecture 3 Vibrations: Two Degrees of Freedo Systes - Wilberforce Pendulu and Bode Plots Wilberforce Pendulu Figure : Wilberforce Pendulu.
More informationMore Empirical Process Theory
More Empirical Process heory 4.384 ime Series Analysis, Fall 2008 Recitation by Paul Schrimpf Supplementary to lectures given by Anna Mikusheva October 24, 2008 Recitation 8 More Empirical Process heory
More informationBayesian inference for stochastic differential mixed effects models - initial steps
Bayesian inference for stochastic differential ixed effects odels - initial steps Gavin Whitaker 2nd May 2012 Supervisors: RJB and AG Outline Mixed Effects Stochastic Differential Equations (SDEs) Bayesian
More informationAutomated Frequency Domain Decomposition for Operational Modal Analysis
Autoated Frequency Doain Decoposition for Operational Modal Analysis Rune Brincker Departent of Civil Engineering, University of Aalborg, Sohngaardsholsvej 57, DK-9000 Aalborg, Denark Palle Andersen Structural
More informationSTOPPING SIMULATED PATHS EARLY
Proceedings of the 2 Winter Siulation Conference B.A.Peters,J.S.Sith,D.J.Medeiros,andM.W.Rohrer,eds. STOPPING SIMULATED PATHS EARLY Paul Glasseran Graduate School of Business Colubia University New Yor,
More informationAN ACCURACY OF ASYMPTOTIC FORMULAS IN CALCULATIONS OF A RANDOM NETWORK RELIABILATY. Tsitsiashvili G.Sh., Losev A.S.
Tsitsiashvili G, Losev A AN ACCUACY OF ASYMPTOTIC FOMULAS IN CALCULATIONS OF A ANDOM NETWOK ELIABILATY &ATA # 3 (Vol) 009, Seteber AN ACCUACY OF ASYMPTOTIC FOMULAS IN CALCULATIONS OF A ANDOM NETWOK ELIABILATY
More informationCourse Notes for EE227C (Spring 2018): Convex Optimization and Approximation
Course Notes for EE7C (Spring 018: Convex Optiization and Approxiation Instructor: Moritz Hardt Eail: hardt+ee7c@berkeley.edu Graduate Instructor: Max Sichowitz Eail: sichow+ee7c@berkeley.edu October 15,
More informationPrinciples of Optimal Control Spring 2008
MIT OpenCourseWare http://ocw.it.edu 16.323 Principles of Optial Control Spring 2008 For inforation about citing these aterials or our Ters of Use, visit: http://ocw.it.edu/ters. 16.323 Lecture 10 Singular
More informationSome Proofs: This section provides proofs of some theoretical results in section 3.
Testing Jups via False Discovery Rate Control Yu-Min Yen. Institute of Econoics, Acadeia Sinica, Taipei, Taiwan. E-ail: YMYEN@econ.sinica.edu.tw. SUPPLEMENTARY MATERIALS Suppleentary Materials contain
More informationProblem Set 2 Due Sept, 21
EE6: Rando Processes in Sstes Lecturer: Jean C. Walrand Proble Set Due Sept, Fall 6 GSI: Assane Guee This proble set essentiall reviews notions of conditional epectation, conditional distribution, and
More informationGeneralized Method of Moments (GMM) Estimation
Econometrics 2 Fall 2004 Generalized Method of Moments (GMM) Estimation Heino Bohn Nielsen of29 Outline of the Lecture () Introduction. (2) Moment conditions and methods of moments (MM) estimation. Ordinary
More informationOPENING THE NEURAL NETWORK BLACKBOX: AN ALGORITHM FOR EXTRACTING RULES FROM FUNCTION APPROXIMATING ARTIFICIAL NEURAL NETWORKS
OENING THE NEURAL NETWORK BLACKBOX: AN ALGORITHM FOR EXTRACTING RULES FROM FUNCTION AROXIMATING ARTIFICIAL NEURAL NETWORKS Rud Setiono Wee Kheng Leow National Universit of Singaore Singaore Jaes Y.L. Thong
More informationPERIODIC STEADY STATE ANALYSIS, EFFECTIVE VALUE,
PERIODIC SEADY SAE ANALYSIS, EFFECIVE VALUE, DISORSION FACOR, POWER OF PERIODIC CURRENS t + Effective value of current (general definition) IRMS i () t dt Root Mean Square, in Czech boo denoted I he value
More informationSeismic Analysis of Structures by TK Dutta, Civil Department, IIT Delhi, New Delhi.
Seisic Analysis of Structures by K Dutta, Civil Departent, II Delhi, New Delhi. Module 5: Response Spectru Method of Analysis Exercise Probles : 5.8. or the stick odel of a building shear frae shown in
More informationQuestions and Answers on Heteroskedasticity, Autocorrelation and Generalized Least Squares
Questions and Answers on Heteroskedasticity, Autocorrelation and Generalized Least Squares L Magee Fall, 2008 1 Consider a regression model y = Xβ +ɛ, where it is assumed that E(ɛ X) = 0 and E(ɛɛ X) =
More informationClassical systems in equilibrium
35 Classical systes in equilibriu Ideal gas Distinguishable particles Here we assue that every particle can be labeled by an index i... and distinguished fro any other particle by its label if not by any
More informationThe proofs of Theorem 1-3 are along the lines of Wied and Galeano (2013).
A Appendix: Proofs The proofs of Theore 1-3 are along the lines of Wied and Galeano (2013) Proof of Theore 1 Let D[d 1, d 2 ] be the space of càdlàg functions on the interval [d 1, d 2 ] equipped with
More informationOptimal Jackknife for Discrete Time and Continuous Time Unit Root Models
Optial Jackknife for Discrete Tie and Continuous Tie Unit Root Models Ye Chen and Jun Yu Singapore Manageent University January 6, Abstract Maxiu likelihood estiation of the persistence paraeter in the
More informationSymmetrization and Rademacher Averages
Stat 928: Statistical Learning Theory Lecture: Syetrization and Radeacher Averages Instructor: Sha Kakade Radeacher Averages Recall that we are interested in bounding the difference between epirical and
More informationarxiv: v1 [math.pr] 17 May 2009
A strong law of large nubers for artingale arrays Yves F. Atchadé arxiv:0905.2761v1 [ath.pr] 17 May 2009 March 2009 Abstract: We prove a artingale triangular array generalization of the Chow-Birnbau- Marshall
More informationUfuk Demirci* and Feza Kerestecioglu**
1 INDIRECT ADAPTIVE CONTROL OF MISSILES Ufuk Deirci* and Feza Kerestecioglu** *Turkish Navy Guided Missile Test Station, Beykoz, Istanbul, TURKEY **Departent of Electrical and Electronics Engineering,
More informationarxiv: v4 [math.st] 9 Aug 2017
PARALLELIZING SPECTRAL ALGORITHMS FOR KERNEL LEARNING GILLES BLANCHARD AND NICOLE MÜCKE arxiv:161007487v4 [athst] 9 Aug 2017 Abstract We consider a distributed learning aroach in suervised learning for
More informationStatistical Techniques II
Statistical Techniques II EST705 Regression with atrix Algebra 06a_atrix SLR atrix Algebra We will not be doing our regressions with matrix algebra, except that the computer does employ matrices. In fact,
More informationA GENERAL THEORY OF PARTICLE FILTERS IN HIDDEN MARKOV MODELS AND SOME APPLICATIONS. By Hock Peng Chan National University of Singapore and
Subitted to the Annals of Statistics A GENERAL THEORY OF PARTICLE FILTERS IN HIDDEN MARKOV MODELS AND SOME APPLICATIONS By Hock Peng Chan National University of Singaore and By Tze Leung Lai Stanford University
More informationCS Lecture 13. More Maximum Likelihood
CS 6347 Lecture 13 More Maxiu Likelihood Recap Last tie: Introduction to axiu likelihood estiation MLE for Bayesian networks Optial CPTs correspond to epirical counts Today: MLE for CRFs 2 Maxiu Likelihood
More informationLinear Regression with Time Series Data
u n i v e r s i t y o f c o p e n h a g e n d e p a r t m e n t o f e c o n o m i c s Econometrics II Linear Regression with Time Series Data Morten Nyboe Tabor u n i v e r s i t y o f c o p e n h a g
More informationGeneralized eigenfunctions and a Borel Theorem on the Sierpinski Gasket.
Generalized eigenfunctions and a Borel Theore on the Sierpinski Gasket. Kasso A. Okoudjou, Luke G. Rogers, and Robert S. Strichartz May 26, 2006 1 Introduction There is a well developed theory (see [5,
More informationSolutions of some selected problems of Homework 4
Solutions of soe selected probles of Hoework 4 Sangchul Lee May 7, 2018 Proble 1 Let there be light A professor has two light bulbs in his garage. When both are burned out, they are replaced, and the next
More informationA Sequential Tracking Filter without Requirement of Measurement Decorrelation
A Sequential racing Filter without Requient of Measuent Decorlation Gongjian Zhou, Changjun Yu, aifan Quan Deartent of Electronic Engineering Harbin Institute of echnology Harbin, China zhougj@hit.edu.cn
More informationLecture 3: October 2, 2017
Inforation and Coding Theory Autun 2017 Lecturer: Madhur Tulsiani Lecture 3: October 2, 2017 1 Shearer s lea and alications In the revious lecture, we saw the following stateent of Shearer s lea. Lea 1.1
More information3.3 Variational Characterization of Singular Values
3.3. Variational Characterization of Singular Values 61 3.3 Variational Characterization of Singular Values Since the singular values are square roots of the eigenvalues of the Heritian atrices A A and
More informationChapter 8 Markov Chains and Some Applications ( 馬哥夫鏈 )
Chater 8 arkov Chains and oe Alications ( 馬哥夫鏈 Consider a sequence of rando variables,,, and suose that the set of ossible values of these rando variables is {,,,, }, which is called the state sace. It
More informationLecture 21. Interior Point Methods Setup and Algorithm
Lecture 21 Interior Point Methods In 1984, Kararkar introduced a new weakly polynoial tie algorith for solving LPs [Kar84a], [Kar84b]. His algorith was theoretically faster than the ellipsoid ethod and
More informationThe Distribution of the Covariance Matrix for a Subset of Elliptical Distributions with Extension to Two Kurtosis Parameters
journal of ultivariate analysis 58, 96106 (1996) article no. 0041 The Distribution of the Covariance Matrix for a Subset of Elliptical Distributions with Extension to Two Kurtosis Paraeters H. S. Steyn
More informationOrder Recursion Introduction Order versus Time Updates Matrix Inversion by Partitioning Lemma Levinson Algorithm Interpretations Examples
Order Recursion Introduction Order versus Tie Updates Matrix Inversion by Partitioning Lea Levinson Algorith Interpretations Exaples Introduction Rc d There are any ways to solve the noral equations Solutions
More informationWeek 5 Quantitative Analysis of Financial Markets Characterizing Cycles
Week 5 Quantitative Analysis of Financial Markets Characterizing Cycles Christopher Ting http://www.mysmu.edu/faculty/christophert/ Christopher Ting : christopherting@smu.edu.sg : 6828 0364 : LKCSB 5036
More informationSlide10. Haykin Chapter 8: Principal Components Analysis. Motivation. Principal Component Analysis: Variance Probe
Slide10 Motivation Haykin Chapter 8: Principal Coponents Analysis 1.6 1.4 1.2 1 0.8 cloud.dat 0.6 CPSC 636-600 Instructor: Yoonsuck Choe Spring 2015 0.4 0.2 0 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 How can we
More informationTopic 5a Introduction to Curve Fitting & Linear Regression
/7/08 Course Instructor Dr. Rayond C. Rup Oice: A 337 Phone: (95) 747 6958 E ail: rcrup@utep.edu opic 5a Introduction to Curve Fitting & Linear Regression EE 4386/530 Coputational ethods in EE Outline
More informationBroadband Synthetic Aperture Matched Field Geoacoustic Inversion
Broadband Snthetic Aerture Matched Field Geoacoustic Inversion PhD Candidate: Bien Aik Tan htt://www.l.ucsd.edu/eole/btan/ PhD Coittee: Prof. Willia Hodgkiss Chair Prof. Peter Gerstoft Co-chair Prof. Willia
More informationModel Mis-specification
Model Mis-specification Carlo Favero Favero () Model Mis-specification 1 / 28 Model Mis-specification Each specification can be interpreted of the result of a reduction process, what happens if the reduction
More informationParallelizing Spectrally Regularized Kernel Algorithms
Journal of Machine Learning Research 19 (2018) 1-29 Subitted 11/16; Revised 8/18; Published 8/18 Parallelizing Sectrally Regularized Kernel Algoriths Nicole Mücke nicole.uecke@atheatik.uni-stuttgart.de
More informationFundamentals of Astrodynamics and Applications 3 rd Ed
Fundaentals of Astrodynaics and Alications 3 rd Ed Errata June 0, 0 This listing is an on-going docuent of corrections and clarifications encountered in the book. I areciate any coents and questions you
More informationNumerical Method for Obtaining a Predictive Estimator for the Geometric Distribution
British Journal of Matheatics & Couter Science 19(5): 1-13, 2016; Article no.bjmcs.29941 ISSN: 2231-0851 SCIENCEDOMAIN international www.sciencedoain.org Nuerical Method for Obtaining a Predictive Estiator
More informationApproximation by Piecewise Constants on Convex Partitions
Aroxiation by Piecewise Constants on Convex Partitions Oleg Davydov Noveber 4, 2011 Abstract We show that the saturation order of iecewise constant aroxiation in L nor on convex artitions with N cells
More informationLearnability of Gaussians with flexible variances
Learnability of Gaussians with flexible variances Ding-Xuan Zhou City University of Hong Kong E-ail: azhou@cityu.edu.hk Supported in part by Research Grants Council of Hong Kong Start October 20, 2007
More informationCOS 424: Interacting with Data. Written Exercises
COS 424: Interacting with Data Hoework #4 Spring 2007 Regression Due: Wednesday, April 18 Written Exercises See the course website for iportant inforation about collaboration and late policies, as well
More informationQuantum algorithms (CO 781, Winter 2008) Prof. Andrew Childs, University of Waterloo LECTURE 15: Unstructured search and spatial search
Quantu algoriths (CO 781, Winter 2008) Prof Andrew Childs, University of Waterloo LECTURE 15: Unstructured search and spatial search ow we begin to discuss applications of quantu walks to search algoriths
More informationFunctions: Review of Algebra and Trigonometry
Sec. and. Functions: Review o Algebra and Trigonoetry A. Functions and Relations DEFN Relation: A set o ordered pairs. (,y) (doain, range) DEFN Function: A correspondence ro one set (the doain) to anther
More informationThe degree of a typical vertex in generalized random intersection graph models
Discrete Matheatics 306 006 15 165 www.elsevier.co/locate/disc The degree of a typical vertex in generalized rando intersection graph odels Jerzy Jaworski a, Michał Karoński a, Dudley Stark b a Departent
More informationProc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES
Proc. of the IEEE/OES Seventh Working Conference on Current Measureent Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Belinda Lipa Codar Ocean Sensors 15 La Sandra Way, Portola Valley, CA 98 blipa@pogo.co
More informationNon-Stationary Time Series and Unit Root Testing
Econometrics II Non-Stationary Time Series and Unit Root Testing Morten Nyboe Tabor Course Outline: Non-Stationary Time Series and Unit Root Testing 1 Stationarity and Deviation from Stationarity Trend-Stationarity
More informationCHAPTER 2 THERMODYNAMICS
CHAPER 2 HERMODYNAMICS 2.1 INRODUCION herodynaics is the study of the behavior of systes of atter under the action of external fields such as teerature and ressure. It is used in articular to describe
More information1 Bounding the Margin
COS 511: Theoretical Machine Learning Lecturer: Rob Schapire Lecture #12 Scribe: Jian Min Si March 14, 2013 1 Bounding the Margin We are continuing the proof of a bound on the generalization error of AdaBoost
More informationAnalyzing Simulation Results
Analyzing Siulation Results Dr. John Mellor-Cruey Departent of Coputer Science Rice University johnc@cs.rice.edu COMP 528 Lecture 20 31 March 2005 Topics for Today Model verification Model validation Transient
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.436J/15.085J Fall 2008 Lecture 11 10/15/2008 ABSTRACT INTEGRATION I
MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.436J/15.085J Fall 2008 Lecture 11 10/15/2008 ABSTRACT INTEGRATION I Contents 1. Preliinaries 2. The ain result 3. The Rieann integral 4. The integral of a nonnegative
More informationHeteroskedasticity and Autocorrelation Consistent Standard Errors
NBER Summer Institute Minicourse What s New in Econometrics: ime Series Lecture 9 July 6, 008 Heteroskedasticity and Autocorrelation Consistent Standard Errors Lecture 9, July, 008 Outline. What are HAC
More information2 Q 10. Likewise, in case of multiple particles, the corresponding density in 2 must be averaged over all
Lecture 6 Introduction to kinetic theory of plasa waves Introduction to kinetic theory So far we have been odeling plasa dynaics using fluid equations. The assuption has been that the pressure can be either
More informationMulti-Dimensional Hegselmann-Krause Dynamics
Multi-Diensional Hegselann-Krause Dynaics A. Nedić Industrial and Enterprise Systes Engineering Dept. University of Illinois Urbana, IL 680 angelia@illinois.edu B. Touri Coordinated Science Laboratory
More information