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,j
eijω, 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 EZt
EZt 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,j
eijω, 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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