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Long memory or long range dependence. ARMA models are characterized by an exponential decay in the autocorrelation structure as the lag goes to infinity. Long memory processes are stationary time series that exhibit a slower decay in the autocorrelation structure
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Long memory or long range dependence • ARMA models are characterized by an exponential decay in the autocorrelation structure as the lag goes to infinity. • Long memory processes are stationary time series that exhibit a slower decay in the autocorrelation structure • The sum of the autocorrelation over all lags is infinite. K. Ensor, STAT 421
Behavior of the spectral density • The spectral density has a special structure as it approaches 0. • The Hurst coefficient is defined as • H close to 1 implies longer memory K. Ensor, STAT 421
Fractionally integrated models A class of models that exhibit this same behavior • |d|>.5 implies r is nonstationary • 0<d<.5 implies r is stationary with long memory also d=H-.5 • -.5<d<0 implies r is stationary with short memory K. Ensor, STAT 421
Prediction • Write as AR() • Requires truncation at p lags • Or re-estimate the filter coefficients based on a lag of p for the given long memory covariance structure • This can be accomplished using the Durbin-Levinson recursive algorithm which takes you from the autocorrelation to the coefficients (and vice versa). • Note similar to the argument we had early on in the autoregessive setting using the Yule-Walker equations to come up with our optimal prediction coefficients. K. Ensor, STAT 421
Long memory extended to GARCH and EGARCH models • Persistence in the volatility can be modeled by extending these long memory constructs to the volatility models such as the GARCH and EGARCH. • See Zivot’s manual for further details. K. Ensor, STAT 421
Testing for persistence • R/S Statistic • Range of deviations from the mean rescaled by the standard deviation. • When rescaled and r’s are iid normal this statistic onverges to the range of a Brownian bridge K. Ensor, STAT 421
GPH Test • Base on the behavior of the spectral density as it approaches 0. • See section 8.3 and 8.4 of Zivot’s manual. K. Ensor, STAT 421