Γ(h)=0 h 0. Γ(h)=cov(X 0,X 0-h ). A stationary process is called white noise if its autocovariance

Similar documents
14 Autoregressive Moving Average Models

DYNAMIC ECONOMETRIC MODELS vol NICHOLAS COPERNICUS UNIVERSITY - TORUŃ Józef Stawicki and Joanna Górka Nicholas Copernicus University

OBJECTIVES OF TIME SERIES ANALYSIS

Exercises: Similarity Transformation

White noise processes

Stationary Time Series

Vectorautoregressive Model and Cointegration Analysis. Time Series Analysis Dr. Sevtap Kestel 1

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

10. State Space Methods

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

ODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004

System of Linear Differential Equations

Concourse Math Spring 2012 Worked Examples: Matrix Methods for Solving Systems of 1st Order Linear Differential Equations

Chapter 6. Systems of First Order Linear Differential Equations

Section 4 NABE ASTEF 232

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.

MATH 2050 Assignment 9 Winter Do not need to hand in. 1. Find the determinant by reducing to triangular form for the following matrices.

Licenciatura de ADE y Licenciatura conjunta Derecho y ADE. Hoja de ejercicios 2 PARTE A

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

Methodology. -ratios are biased and that the appropriate critical values have to be increased by an amount. that depends on the sample size.

Announcements: Warm-up Exercise:

Chapter 3 Boundary Value Problem

After the completion of this section the student. Theory of Linear Systems of ODEs. Autonomous Systems. Review Questions and Exercises

2 Univariate Stationary Processes

- The whole joint distribution is independent of the date at which it is measured and depends only on the lag.

STATIONARY LINEAR VECTOR TIME SERIES PROCESSES Richard T Baillie, ( ).

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

Then. 1 The eigenvalues of A are inside R = n i=1 R i. 2 Union of any k circles not intersecting the other (n k)

Two Coupled Oscillators / Normal Modes

2. Nonlinear Conservation Law Equations

Math 334 Fall 2011 Homework 11 Solutions

Financial Econometrics Jeffrey R. Russell Midterm Winter 2009 SOLUTIONS

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

BOX-JENKINS MODEL NOTATION. The Box-Jenkins ARMA(p,q) model is denoted by the equation. pwhile the moving average (MA) part of the model is θ1at

12: AUTOREGRESSIVE AND MOVING AVERAGE PROCESSES IN DISCRETE TIME. Σ j =

Ordinary Differential Equations

Math 315: Linear Algebra Solutions to Assignment 6

Chapter 2. First Order Scalar Equations

Chapter Three Systems of Linear Differential Equations

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

Sample Autocorrelations for Financial Time Series Models. Richard A. Davis Colorado State University Thomas Mikosch University of Copenhagen

Linear Dynamic Models

LAPLACE TRANSFORM AND TRANSFER FUNCTION

Richard A. Davis Colorado State University Bojan Basrak Eurandom Thomas Mikosch University of Groningen

Application 5.4 Defective Eigenvalues and Generalized Eigenvectors

CHAPTER 2 Signals And Spectra

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

Institute for Mathematical Methods in Economics. University of Technology Vienna. Singapore, May Manfred Deistler

2 Some Property of Exponential Map of Matrix

Modeling Economic Time Series with Stochastic Linear Difference Equations

State-Space Models. Initialization, Estimation and Smoothing of the Kalman Filter

Homework 10 (Stats 620, Winter 2017) Due Tuesday April 18, in class Questions are derived from problems in Stochastic Processes by S. Ross.

ST4064. Time Series Analysis. Lecture notes

SOLUTIONS TO ECE 3084

Let ( α, β be the eigenvector associated with the eigenvalue λ i

Distance Between Two Ellipses in 3D

Math 1. Two-Hours Exam December 10, 2017.

Økonomisk Kandidateksamen 2005(II) Econometrics 2. Solution

Generalized Least Squares

Regular Variation and Financial Time Series Models

Box-Jenkins Modelling of Nigerian Stock Prices Data

Quarterly ice cream sales are high each summer, and the series tends to repeat itself each year, so that the seasonal period is 4.

Chapter 5. Heterocedastic Models. Introduction to time series (2008) 1

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

Modal identification of structures from roving input data by means of maximum likelihood estimation of the state space model

Lecture Notes 2. The Hilbert Space Approach to Time Series

STATE-SPACE MODELLING. A mass balance across the tank gives:

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

Linear Response Theory: The connection between QFT and experiments

Chapter #1 EEE8013 EEE3001. Linear Controller Design and State Space Analysis

How to Deal with Structural Breaks in Practical Cointegration Analysis

Homework Solution Set # 3. Thursday, September 22, Textbook: Claude Cohen Tannoudji, Bernard Diu and Franck Lalo, Second Volume Complement G X

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

For example, the comb filter generated from. ( ) has a transfer function. e ) has L notches at ω = (2k+1)π/L and L peaks at ω = 2π k/l,

Differential Equations

Vehicle Arrival Models : Headway

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

KEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)

Math 10B: Mock Mid II. April 13, 2016

Lie Derivatives operator vector field flow push back Lie derivative of

15. Vector Valued Functions

Basilio Bona ROBOTICA 03CFIOR 1

Excel-Based Solution Method For The Optimal Policy Of The Hadley And Whittin s Exact Model With Arma Demand

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS

Tests of Nonlinear Resonse Theory. We compare the results of direct NEMD simulation against Kawasaki and TTCF for 2- particle colour conductivity.

Lecture 20: Riccati Equations and Least Squares Feedback Control

3, so θ = arccos

Y, where. 1 Estimate St.error

EE363 homework 1 solutions

Math Week 14 April 16-20: sections first order systems of linear differential equations; 7.4 mass-spring systems.

Let us start with a two dimensional case. We consider a vector ( x,

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0.

Forecasting optimally

Solutions to Odd Number Exercises in Chapter 6

6.2 Transforms of Derivatives and Integrals.

Introduction D P. r = constant discount rate, g = Gordon Model (1962): constant dividend growth rate.

Transcription:

A family, Z,of random vecors : Ω R k defined on a probabiliy space Ω, A,P) is called a saionary process if he mean vecors E E =E M = M k E and he auocovariance marices are independen of. k cov, -h )=E E ) -h E -h ) he auocovariance funcion of a saionary process is defined by Γh)=cov, -h ). Exercise: Show ha Γh)=Γ h). MS A saionary process is called whie noise if is auocovariance funcion saisfies Γh)= h. Since Γ) does no have o be a diagonal marix, any wo componens of whie noise can be correlaed wih each oher conemporaneously. A saionary process is called a firs order auoregressive process or AR) process) if i can be expressed as φ φk ) M = M O M M + M, k 3 k 4 φ φkk 443 ) k 443 k 3 Φ where is whie noise wih mean vecor. Each componen of an AR) process depends no only on lagged values of iself bu also on lagged values of he oher componens.

Subsiuing in an AR) equaion =Φ - + firs Φ - + - for - and hen Φ -3 + 3 for -, gives =ΦΦ - + - )+ =Φ - +Φ - + =Φ Φ -3 + - )+Φ - + =Φ 3-3 +Φ - +Φ - + M m =Φ m -m + Φ j j Suppose ha Φ is diagonalizable, i.e., here is an inverible marix C such ha Λ=C - ΦC is a diagonal marix. I hen follows from Λ=C - ΦC Φ=CΛC - For example, any Hermiian marix a complex square marix ha is equal o is own conjugae ranspose) is diagonalizable. hus, real symmeric marices are diagonalizable. ha Φ =ΦΦ=CΛC - CΛC - =CΛ C - Φ 3 =Φ Φ=CΛ C - CΛC - =CΛ 3 C - hus, M Φ m =CΛ m C -. λ Φ m =C M m λ =C M λ λ m O O m M λ k M m λ k C - C - will vanish as m only if he no necessarily real numbers λ,,λ k have modulus less han. MR

A k k marix Φ is diagonalizable if and only if i has k linearly independen eigenvecors diagonalizaion heorem). Proof: Suppose ha c,,c k are linearly independen eigenvecors wih eigenvalues λ,,λ k. hen If hen λ Φ = c,,c k ) M O M c,,c k ) -, λ k Φ = Φc,,c k )c,,c k ) - Φc,,Φc k ) = Φc,,c k ) = Φc,,Φc k )c,,c k ) - = λ c,,λ k c k )c,,c k ) - λ = c,,c k ) M O M c,,c k ) -. λk = c,,c k ) λ M = λ c,,λ k c k ). O λ M k MD 3

Exercise: Show ha if a marix Φ has differen eigenvalues λ and λ, he corresponding eigenvecors c and c will be linearly independen. Soluion: Since λ and λ are differen, a leas one of hem, say λ, is no equal o zero. Assuming ha he anihesis is valid, we obain c =νc for some ν Φc =νφc, λ c =νλ c, and c = λ λ νc, Since λ and c, c, his is in conradicion wih he λ anihesis. ME Exercise: Find he eigenvalues λ and λ of he marix Φ=. Hin: If c is an eigenvecor wih eigenvalue λ, i.e., or, equivalenly, Φc=λc λiφ)c=, hen he inveribiliy of he marix λiφ would imply ha c=λiφ) - =, which is inconsisen wih he requiremen ha c mus be a non-zero vecor. he eigenvalues can herefore be found by solving he equaion deλiφ)=. MV 4

If Φ is a k k marix, he characerisic polynomial deλiφ) has degree k. According o he fundamenal heorem of algebra i has herefore k complex) roos, if each roo is couned wih is algebraic mulipliciy. Since eigenvecors corresponding o differen eigenvalues are independen, Φ can only be non-diagonalizable if here exiss an eigenvalue wih algebraic mulipliciy m a > and geomeric mulipliciy m g <m a. he geomeric mulipliciy of an eigenvalue is he number of linearly independen eigenvecors wih ha eigenvalue. Exercise: Show ha he marix MN is non-diagonalizable. Φ= 3 Hin: he eigenvecors corresponding o an eigenvalue λ can be found by solving he equaion λiφ)c= for c. he condiion ha all he eigenvalues of Φ are less han in absolue value, i.e., is equivalen o z deφzi), z de z ΦzI)), z dei z Φ), and z deizφ). Remark: If all roos of he polynomial dei-zφ) lie ouside of he uni circle, he sequence Φ, Φ, Φ 3, is absoluely summable and j j converges componenwise) in mean square o. Φ 5

sing lag-operaor noaion he equaion can also be wrien as Φ - = IΦ) =, where IΦ is a marix-valued polynomial. For example, in he bivariae case we have I Φ) = φ = φ φ φ φ φ φ φ φ) φ = φ + φ) A saionary process is called an auoregressive process of order p or ARp) process) if i can be expressed as or, equivalenly, as =Φ - + +Φ p -p + Φ - Φ p -p =, where is whie noise wih mean vecor. sing lag-operaor noaion, he laer equaion can also be wrien as where Φ) =, Φ)=IΦ Φ p p is a marix-valued polynomial. = φ φ ) ) φ φ ) ). 6

e be a general linear process represened by = Ψ j j, where is whie noise wih E = and var )=Σ. We have and E = Ψ je j = Γ k)=cov, -k )=E Ψ j = Ψ r= r j E = Ψ j+ kσψ j. j k)j Ψ -r -j+ k) Since neiher E nor cov, -k ) depend on, he process is weakly saionary. P Ψ j he specral densiies of and are given by f ω)= π f ω)= π e k= iωk iωk e = π k= Γ k)= Σ, π Ψ i k e ω = π k= j+ k Γ k) ΣΨ j 4443 4 Ψ j ΣΨ iωj e Ψ jσ) k= = π Ψ j e -iωj Σ k= = π Ψ jk Ψ jk e iωj-k) j+ k e iωj+k) Ψ j e -iωj Σ Ψ -iωk k e * ) k=. PD 7

A represenaion IΦ) = of an AR) process is called causal if can be expressed in erms of presen and pas shocks, i.e., = j j Is specral densiy is given by f ω)= π j j Φ ) = Φ. j Φ e -iωj Σ iω = π Φe ) I Σ k= k e -iωk Φ ) * iω ) * I Φe ). Exercise: Derive he sum formula PG n Φ j =IΦ n+ )IΦ) for a geomeric series of marices. Hin: Muliply each side of he equaion by IΦ. Remark: Moreover, if all eigenvalues of Φ have modulus less han, we have = j j Φ =IΦ). Exercise: Show ha PV = j j Φ e -iωj =IΦe -iω ), if all eigenvalues of Φ have modulus less han. Analogously, f ω)= π IΦ e -iω Φ p e -iωp ) - Σ IΦ e -iω Φ p e -iωp ) - ) * is he specral densiy of an ARp) process wih causal represenaion IΦ Φ p p ) =. 8

Exercise: Reexamine he relaionship beween changes in he indusrial producion and changes in he duraion of unemploymen wih parameric mehods. Wrie an R funcion for he calculaion of he specral densiy of a vecor auoregressive process. var.spec <- funcionfr,ar.p) { # fr vecor of frequencies # AR.p ARp) model esimaed by R funcion ar nf <- lenghfr); p <- AR.p$order sigma <- AR.p$var.pred; k <- lenghsigma[,]) Id <- diag,nrow=k,ncol=k) # ideniy marix sp <- arraydim=cnf,k,k)) for w in :nf) { A <- Id for l in :p) A <- A-AR.p$ar[l,,]*exp-i*fr[w]*l) A <- solvea) # inverse of A sp[w,,] <- A%*%sigma%*%ConjA)) } reurnsp/*pi)) } Esimae AR model of order p=3. AR.3 <- arxy,order.max=3,aic=f,demean=) # aic=f order is fixed, no seleced auomaically # AR.3$ar: array of dim 3,,) wih AR coefficiens AR.3$ar[,,] # lag Series Series Series.6357.78465 Series -.59957 -.3733489 AR.3$ar[,,] # lag Series Series Series.44655.994 Series -.46 -.7367764 AR.3$ar[3,,] # lag 3 Series Series Series.76967 -.95759 Series -.466969 -.74439 AR.3$var.pred # variance no explained by AR model Series Series Series 4.437e-5-6.444694e-6 Series -6.444694e-6 3.7668e-3 9

Esimae he univariae specral densiies. parmfrow=c,),mar=c,,,)) p <- spec.pgramxy[,],aper=,der=f,fas=f,plo=f) f <- p$freq**pi; plof,p$spec/*pi),ype="l") sp.3 <- var.specf,ar.3); linesf,sp.3[,,],col="red") p <- spec.pgramxy[,],aper=,der=f,fas=f,plo=f) plof,p$spec/*pi),ype="l") linesf,sp.3[,,],col="red") Esimae he cospecrum. parmfrow=c,)) plof,resp.3[,,]),ype="l") ablineh=,ly="dashed") # dashed horizonal line he overall negaive relaionship beween he wo variables is mainly due o he low frequencies.

Esimae he squared coherency and he phase specrum. parmfrow=c,)) plof,modsp.3[,,])^/sp.3[,,]*sp.3[,,]),ype="l") plof,argsp.3[,,]),ype="l") he squared coherency is large a he low frequencies. here he slope of he phase specrum is approximaely, which indicaes ha changes in he duraion of unemploymen lag wo monhs behind changes in indusrial producion.

A saionary process is called an auoregressive moving average process of order p,q) or ARMAp,q) process) if i can be expressed as =Φ - + +Φ p -p + +Θ - + +Θ q -q or, equivalenly, as Φ - Φ p -p = +Θ - + +Θ q -q, where is whie noise wih mean vecor. sing lag-operaor noaion, he laer equaion can also be wrien as where and Φ) =Θ), Φ)=IΦ Φ p p Θ)=I+Θ + +Θ q q are marix-valued polynomials. An ARMAp,) process is an ARp) process. An ARMA,q) process is also called a moving average process of order q or MAq) process). he ARMAp,q) equaion IΦ Φ p p ) = I+Θ + +Θ q q ) is said o be causal if z deizφ z p Φ p ). I is said o be inverible if z dei+zθ+ +z q Θ q ). Exercise: Show ha he bivariae AR) process 4 ) ) = is causal and inverible. PC

3 Exercise: Show ha he bivariae MA) process = + 3 ) ) + ) ) is causal and inverible. PI Exercise: Show ha he bivariae ARMA,) process ) ) = + 3 5 ) ) is causal and inverible. PA I does no make sense o esimae he parameer marices Φ,,Φ p,θ,,θ q, and Σ of an ARMAp,q) process if hey are no unique. o ensure idenifiabiliy in he univariae case, where Φ) and Θ) are jus scalar polynomials, we mus require, in addiion o causaliy and inveribiliy, ha Φz) and Θz) have no common zeros. For example, he equaion 4 ) =+ ) can be wrien more parsimoniously as ) =, because he polynomials 4 z =+ z) z) and + z have a common zero.

In he mulivariae case, he marix-valued polynomials Φz) and Θz) can have a common lef facor even if deφz)) and deθz)) have no common zero. o avoid he difficulies involved in he idenificaion of mulivariae ARMA processes, many ime series analyss use only mulivariae AR models for he modeling of mulivariae ime series. Exercise: Show ha he equaion P φ + θ ) ) can be wrien more parsimoniously as φ = θ + ) ) = ) ) alhough he polynomials and have no common zero. φ + θ deφz))=dei z) θ deθz))=dei+ z) Hin: Muliply boh Φz) and Θz) by Θ - θz z)=. Remark: he inverse of he marix-valued polynomial Θz) is also a marix-valued polynomial. Is deerminan is a consan unequal o zero. Such a marix-valued polynomial is called unimodular. 4