are independent. Thus it can capture any type of pairwise cross-dependence between fZtg and j,j > 0g over various lags (including those with zero autocorrelation). In this spirit, fZYω,u,v can capture various linear and nonlinear cross-dependencies.[11] Another important advantage of using the characteristic function is that it requires no moment condition on fZtg and fYtg, and so it does not suffer from the potential problem when the moment condition fails, which is often found in high-frequency economic and financial time series (e.g., Pagan and Schwert, 1990). Moreover, the generalized spectrum shares a nice feature of the conventional spectral approach—it incorporates information on serial dependence from virtually all lags. This will ensure to capture serial dependence at higher lag orders, and hence enhance good power for tests against the alternatives involving a persistent dependence structure (i.e., serial dependence decays to zero slowly as j ! 1).
It is important to point out that the generalized cross-spectrum fZYω,u,v itself is not suitable for testing the null hypotheses 0 in (2) and (4), because the generalized spectrum fZYω,u,v encompasses all pairwise cross-dependencies in various conditional moments of both fZtg and j,j > 0g. Fortunately, fZYω,u,v can be differentiated to reveal possible specific patterns of cross-dependence in various conditional moments, thanks to the use of the characteristic function.
In particular, one can use the generalized cross-spectral density derivative
fZY0,m,lω,u, ∂u∂mmC∂vl l fZYω,u, 2 jD1 ZY,jm,lu,ijω, m,l ½ 0 7
By varying the combination of the derivative orders m,l, the generalized cross-spectral derivative fZY0,m,lω,u,v can capture various specific aspects of cross-dependence between fZtg and fYtj,j > 0g. For example, to test the null hypothesis 0 of (2): EZt EZt a.s. (with Zt D Ztc), we can use the (1, 0)th order generalized cross-spectral derivative
fZY0,1,0ω, ZY,jeijω, ω ,] 8
2 jD1
where
ZY,j1,0ZY,ju, coviZt,eivY
The measure ZY,j1,00,v checks correlations between Zt and all moments of Yt, and is thus suitable for testing whether EZtEZt for all j.[12]
As in Hong and Chung (2006), we consider a stepwise procedure for hypothesis testing, which begins by examining directional predictability using fZY0,1,0ω,0,v, then proceeds for separate inferences on various sources such as time-varying conditional mean, volatility clustering and conditional skewness or other higher-order conditional moments. Once directional predictability is detected, this stepwise testing procedure will reveal useful information in making inferences on the nature of directional predictability and thus the modeling of directional forecasts.14 In particular, we use the following higher-order generalized cross-spectral derivative with the choice of l D 1,2,3,4 respectively:
1
fZY0,1,lω, ZY,jeijω, ω ,] 9
2
where
ZY,j1,l l ZY,ju,cov[iZt,iY l , l ½ 1
∂u∂v
As expected, ZY1,l0,0 will be proportional to cross-covariance covZt,Yl and, as a consequence, fZY0,1,lω,0,0 for l D 1,2,3,4 can be used to test whether Zt is predictable using the level of past changes , past volatility, past skewness and past kurtosis
, respectively.
Following Hong (1999, Theorem 1), we can consistently estimate the above generalized crossspectral density derivative by a smoothed kernel estimator:
fO ZY0,1,lω,/T1/2kj/p ZY,j eijω, ω ,], 10
T
where OZY,j1,lu, l ZY,ju,ZY,ju,ZYj,u,ZYj,u,ZYj,0,v is the
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