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"Frontmatter". In: Analysis of Financial Time Series

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374 MULTIVARIATE VOLATILITY MODELŜΣ 888 (1) =[ ]71.09 21.83,21.83 17.79where the covariance is obtained by using the constant correlation coefficient 0.614.For the time-varying correlation model in Eqs. (9.24) and (9.25), we have a 1,888 =3.287, a 2,888 = 4.950, σ 11,888 = 83.35, σ 22,888 = 28.56, and ρ 888 = 0.546. The1-step ahead forecast for the covariance matrix iŝΣ 888 (1) =[ ]75.15 23.48,23.48 24.70where the forecast <strong>of</strong> the correlation coefficient is 0.545.<strong>In</strong> the second method, we use the Cholesky decomposition <strong>of</strong> Σ t to modeltime-varying correlations. For the bivariate case, the parameter vector is Ξ t =(g 11,t , g 22,t , q 21,t ) ′ ; see Eq. (9.13). A simple GARCH(1, 1)-type model for a t isg 11,t = α 10 + α 11 b 2 1,t−1 + β 11g 11,t−1q 21,t = γ 0 + γ 1 q 21,t−1 + γ 2 a 2,t−1 (9.26)g 22,t = α 20 + α 21 b1,t−1 2 + α 22b2,t−1 2 + β 21g 11,t−1 + β 22 g 22,t−1 ,where b 1t = a 1t and b 2t = a 2t −q 21,t a 1t . Thus, b 1t assumes a univariate GARCH(1,1) model, b 2t uses a bivariate GARCH(1, 1) model, and q 21,t is auto-correlated anduses a 2,t−1 as an additional explanatory variable. The probability density functionrelevant to maximum likelihood estimation is given in Eq. (9.15) with k = 2.Example 9.2. (continued). Again we use the monthly log returns <strong>of</strong> IBMstock and the S&P 500 index to demonstrate the volatility model in Eq. (9.26).Using the same specification as before, we obtain the fitted mean equations asr 1t = 1.364 + 0.075r 1,t−1 − 0.058r 2,t−2 + a 1tr 2t = 0.643 + a 2t ,where standard errors <strong>of</strong> the parameters in the first equation are 0.219, 0.027, and0.032, respectively, and that <strong>of</strong> the parameter in the second equation is 0.154. Thesetwo mean equations are close to what we obtained before. The fitted volatility modelisg 11,t = 3.714 + 0.113b 2 1,t−1 + 0.804g 11,t−1q 21,t = 0.0029 + 0.9915q 21,t−1 − 0.0041a 2,t−1 (9.27)g 22,t = 1.023 + 0.021b1,t−1 2 + 0.052b2 2,t−1 − 0.040g 11,t−1 + 0.937g 22,t−1 ,

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