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A detailed overview of autocorrelation functions (acf) and their applications in time series analysis. It covers key concepts such as the j-th order autocorrelation function, correlograms, and estimation methods for stationary ergodic processes. The document also explains testing for autocorrelation using box-pierce and ljung-box statistics, along with their implementation in r. Furthermore, it delves into arma models, gaussian white noise, and moving average processes (ma), including ma(1), ma(q), and ma(infinity). The stationarity and ergodicity conditions for these processes are thoroughly examined, making it a valuable resource for students and practitioners in statistics and econometrics.
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The j-th order autocorrelation function is defined as - correct answer rho(j) = gamma(j)/gamma(0) = ([E(X(t)-mew)E(X(t-j)-mew)])/(E[(X(t) - mew)^2]) = (Cov(X(t),X(t-j))/Var(X(t) for j = 0,1,2,... with -1 <= rho(j) <= 1 The plot of rho(j) against j = 0,1,2,... is called - correct answer the correlogram For a stationary ergodic process, the ACF can be estimated by the sample moments as follows - correct answer y bar = (1/T) * Summation from t=1 to T of y(t) sigma hat^2 = (1/T) * Summation from t=1 to T of (y(t) - y bar)^ for each j: r(j) = (Summation from t=j+1 to T of (y(t)-y bar)(y(t-j)-y bar))/(Summation from t=1 to T of (y(t)-y bar)^2) Sample variance of r(j): Var(r(j)) = T^-1 for j= Var(r(j)) = T^-1 * (1+2*summation from k=1 to j-1 of (r(k)^2)) for j > 1 Testing for autocorrelation - correct answer Also known as testing the null hypothesis that autocorrelations are significantly different from zero H(0): r(j) = 0 for j = 1,2,3,...,k and k < T **Can be done with Box and Pierce (1970) or Ljung-Box (1978)
Autocorrelation - correct answer In a longitudinal design, the correlation of one variable with itself, measured at two different times. Box-Pierce (1970) statistic - correct answer Q = T * Summation from j=1 to k of r(j)^ Q ~ X^2(k) under H(0) Ljung-Box (1978) statistic - correct answer Q = T(T+2) * Summation from j=1 to k of r(j)^2 / (T - j) Q ~ X^2(k) under H(0) Box-Pierce and Ljung-Box in R - correct answer Examining null hypothesis of independence in a given time series ('portmanteau tests') Box.test(x, lag=1, type=c("Box-Pierce","Ljung-Box") fitdf=0) x = numeric vector or univariate time series lag = statistic based on lag autocorrelation coefficients type = test to be performed: partial matching used fitdf = number of degrees of freedom to be subtracted if x is series of residuals **Sometimes applied to the residuals from an ARMA (p, q) fit, in which case the references suggest a better approximation to the null-hypothesis distribution is obtained by setting fitdf = p+q, provided lag > fitdf --> Gives value = a list with class "htest" and following components: -statistic = value of test statistic
Moving average processes - correct answer 1. MA(1)-process
The higher order covariances of MA(1) are all - correct answer zero gamma(j) = Cov(Y(t), Y(t-j)) = 0, inverted A j > 1 -> {Y(t)} of MA(1) is (covariance) stationary The MA(1)-process is stationary and - correct answer ergodic *Ergodic based on: Summation from j=0 to infinity |gamma(j)| = (1+theta(1)^2)sigma^2 + |theta(1)| *sigma^2 < infinity The autocorrelations for the MA(1)-process are given by - correct answer rho(j) = gamma(j) / gamma(0) for j = 0,1,2,... **Therefore rho(0) = 1 (always) and for the MA(1)-process we have: rho(1) = theta(1) / (1 + theta(1)^2) with rho(1) > 0 for theta(1) > 0 and rho(1) < 0 for theta(1) < 0 *For j > 1 : gamma(j) = 0 and rho(j) = 0 --> thus autocorrelations are useful to identify the process MA(q)-process - correct answer Y(t) = mew + theta(0)Epsilon(t-1) + ... + theta(q)Epsilon(t-1) **Normally with theta(0) = 1
= 1 / 1 - phi, if |phi| < 1 + MA(infinity)-process Y(t) = mew + Epsilon(t) + phiEpsilon(t-1) + phi^2(Epsilon(t-2)) + ... with E(Y(t) = mew = c / 1 - phi Applying AR(1)-process |phi| < 1 condition to stationarity and ergodicity of an MA(infinity)-process - correct answer Summation from j=0 to infinity of |psi(j)| = Summation from j=0 to infinity of |phi^j| = 1 / (1 - |phi|) < infinity if |phi| < 1 Applying AR(1)-process |phi| < 1 condition to variance of an MA(infinity)-process - correct answer gamma(0) = E[(Y(t) - mew)^2] = E[(Epsilon(t) + phiEpsilon(t-1) + phi^2Epsilon(t-2) + ...)^2] = (1 + phi^2 + phi^4 + phi^6 + ...)sigma^ = 1/(1-phi^2)sigma^2 (if |phi| < 1) Applying AR(1)-process |phi| < 1 condition to autocovariance - correct answer gamma(j) = E[(Y(t) - mew)(Y(t-j) - mew)] = E[(Epsilon(t) + phiEpsilon(t-1) + phi^2Epsilon(t-2) + ...)(Epsilon(t-j) + phiEpsilon(t-j-1) + phi^2Epsilon(t-j-2) + ...)] -> gamma(1) = (phi + phi^3 + phi^5 + ...)sigma^ = phi(1 + phi^2 + phi^4 + ...)sigma^ = (phi / (1 - phi^2))sigma^
AR(2)-process written with lag operator - correct answer (1 - phi(1)L - phi(2)L^2)Y(t) = c + Epsilon(t) With factorization: (1 - lambda(1)L)(1-lambda(2)L)Y(t) = c + Epsilon(t) Only stable if eigenvalues lambda(1) and lambda(2) of F matrix (phi(1),phi(2),1,0) [solutions lambda(1) and lambda(2) of characteristic polynomial lambda^2 - phi(1)lambda - phi(2) = 0] lie inside unit circle (i.e., are less than 1 in modulus for complex numbers) Can also be checked by seeing if solutions z(1) and z(2) of lag polynomial 1- phi(1)z-phi(2)z^2=0 le outside unit circle (i.e., are greater than 1 in modulus) As AR(2)-process is a second-order stochastic linear difference equation, those conditions must be fulfilled for the AR(2)-process to be stationary Expression for (1 - phi(1)L - phi(2)L^2)^-1 so that the AR(2)-process can be written as an MA(infinity)-process - correct answer Y(t) = (1-phi(1)L-phi(2)L^2)^- 1 c + (1-phi(1)L - phi(2)L^2)^-1Epsilon(t) where: (1-phi(1)L - phi(2)L^2)^-1 = (1-lambda(2)L)^-1(1-lambda(1)L)^- = (1+lambda(2)L + lambda(2)^2L^ +...)(1+lambda(1)L+lambda(1)^2L^2+...) = 1+psi(1)L+psi(2)L^2+... =phi(L)
with phi(1) = lambda(1) + lambda(2) phi(2) = lambda(1)^2 + lambda(2)^2 + lambda(1) * lambda(2) MA(infinity)-representation of the AR(2)-process is given by - correct answer Y(t) = c/(1-phi(1)-phi(2) + Epsilon(t) + psi(1)Epsilon(t-1) + psi(2)Epsilon(t-2)+... with E(Y(t)) = mew = c/(1-phi(1)-phi(2)) and psi(j) = c(1)lambda(1)^j + c(2)lambda(2)^j where c(1) + c(2) = 1 Therefore, MA representation of AR(2)-process can be written shortly as: Y(t) = mew + psi(L)Epsilon(t) Showing that the autocovariances follow the same second-order difference equation as the process for Y(t) - correct answer Substituting c=mew(1-phi(1)-phi(2)), we get Y(t) = mew(1-phi(1)-phi(2)) + phi(1)Y(t-1) + phi(2)Y(t-2) + Epsilon(t) Y(t) - mew = psi(1)(Y(t-1)-mew)+psi(2)(Y(t-2)-mew)+Epsilon(t) Multiplying by (Y(t-j)-mew) and taking expectations results in: E[(Y(t)-mew)(Y(t-j)-mew)] = psi(1)E[(Y(t-1)-mew)(Y(t-j)-mew)] + psi(2)E[(Y(t-2)- mew)(Y(t-j)-mew)]+E[Epsilon(t)(Y(t-j)-mew)]
where (1 - phi(1)L - phi(2)L^2 - ... - phi(P)L^P)^- = (1 - lambda(P)L)^-1 ... (1-lambda(1)L)^- = (1 + lambda(P)L + lambda(P)^2L^2 + ...)...(1 + lambda(1)L + lambda(1)^2L^2 + ...) = 1 + psi(1)L + psi(2)*L^2 + ... = psi(L)
Also shown that psi(j) = c(1)lambda(1)^j + c(2)lambda(2)^j + ... + c(P)lambda(P)^j with Summation from i=1 to P of c(i) = 1 --> MA(infinity) of AR(p) given by: Y(t) = c/(1-phi(1)-...-phi(P)) + Epsilon(t) + psi(1)Epsilon(t-1) + psi(2)*Epsilon(t-2)
Writing MA(infinity) representation of AR(p) shortly - correct answer Y(t) = mew + psiLEpsilon(t) **As for stationary AR(p) process Summation from j=0 to infinity of |psi(j)| < infinity the process is also ergodic Showing that the autocovariances of AR(p) follow same pth-order difference equation as the process for Y(t) - correct answer -Substituting c = mew(1 - phi(1)
-> gamma(j) = phi(1)gamma(j-1) + phi(2)gamma(j-2) + ... + phi(p)*gamma(j-p) for j > q **For j <= q, the MA part also affects the autocovariances, thus the autocovariances and the autocorrelations of the ARMA process have more complicated characteristics than those of an AR(p) or MA(q) process