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"Frontmatter". In: Analysis of Financial Time Series

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NONLINEARITY TESTS 153idea behind various nonlinearity tests. <strong>In</strong> particular, some <strong>of</strong> the nonlinearity testsare designed to check for possible violation in quadratic forms <strong>of</strong> the underlyingtime series.4.2.1.1 Q-Statistic <strong>of</strong> Squared ResidualsMcLeod and Li (1983) apply the Ljung–Box statistics to the squared residuals <strong>of</strong> anARMA(p, q) model to check for model inadequacy. The test statistic isQ(m) = T (T + 2)m∑i=1ˆρ 2 i (a2 t )T − i ,where T is the sample size, m is a properly chosen number <strong>of</strong> autocorrelationsused in the test, a t denotes the residual series, and ˆρ i (at 2) is the lag-i ACF <strong>of</strong> a2 t .If the entertained linear model is adequate, Q(m) is asymptotically a chi-squaredrandom variable with m − p − q degrees <strong>of</strong> freedom. As mentioned in Chapter 3,the prior Q-statistic is useful in detecting conditional heteroscedasticity <strong>of</strong> a t and isasymptotically equivalent to the Lagrange multiplier test statistic <strong>of</strong> Engle (1982)for ARCH models; see subsection 3.3.3. The null hypothesis <strong>of</strong> the statistics isH o : β 1 =···=β m = 0, where β i is the coefficient <strong>of</strong> at−i 2 in the linear regressiona 2 t = β 0 + β 1 a 2 t−1 +···+β ma 2 t−m + e tfor t = m + 1,...,T . Because the statistic is computed from residuals (not directlyfrom the observed returns), the number <strong>of</strong> degrees <strong>of</strong> freedom is m − p − q.4.2.1.2 Bispectral TestThis test can be used to test for linearity and Gaussianity. It depends on the resultthat a properly normalized bispectrum <strong>of</strong> a linear time series is constant over allfrequencies and that the constant is zero under normality. The bispectrum <strong>of</strong> a timeseries is the Fourier transform <strong>of</strong> its third-order moments. For a stationary time seriesx t in Eq. (4.1), the third-order moment is defined asc(u,v)= g∞∑k=−∞ψ k ψ k+u ψ k+v , (4.35)where u and v are integers, g = E(a 3 t ), ψ 0 = 1, and ψ k = 0fork < 0. TakingFourier transforms <strong>of</strong> Eq. (4.35), we haveb 3 (w 1 ,w 2 ) =g4π 2 Ɣ[−(w 1 + w 2 )]Ɣ(w 1 )Ɣ(w 2 ), (4.36)where Ɣ(w) = ∑ ∞u=0 ψ u exp(−iwu) with i = √ −1, and w i are frequencies. Yet thespectral density function <strong>of</strong> x t is given by

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