1. Introduction
In the world of univariate conditional volatility models, the ARCH model of Engle [
1] and the generalization to the GARCH model by Bollerslev [
2] are the two most widely estimated symmetric models of time-varying conditional volatility, where symmetry refers to the identical effects on volatility of positive and negative shocks of equal magnitude.
The asymmetric effects on conditional volatility of positive and negative shocks of equal magnitude can be captured in different ways by the exponential GARCH (or EGARCH) model of Nelson [
3,
4], and the GJR (alternatively, asymmetric or threshold) model of Glosten, Jagannathan and Runkle [
5]. These are the two most widely estimated asymmetric univariate models of conditional volatility.
A special case of asymmetry is that of leverage. As defined by Black [
6] in terms of the debt-to-equity ratio, leverage is associated with increases in volatility for negative shocks to returns and decreases in volatility for positive shocks to returns. In short, leverage captures the negative correlation between returns shocks and subsequent shocks to volatility. The EGARCH model is capable of capturing leverage, depending on appropriate restrictions on the parameters of the model.
Although the GJR model can capture asymmetry, leverage is not possible, unless the short run persistence effect (that is, the ARCH parameter) is negative. Such a restriction is not consistent with the standard sufficient condition for conditional volatility to be positive.
The univariate GARCH model has been extended to its multivariate counterpart in, for example, the BEKK model of Baba
et al. [
7] and Engle and Kroner [
8], and the VARMA-GARCH model of Ling and McAleer [
8]. The GJR model has a multivariate counterpart in the VARMA-AGARCH model of McAleer, Hoti and Chan [
10].
However, the EGARCH model has not yet been developed formally for multivariate processes, with appropriate regularity conditions. Kawakatsu [
11] examined a matrix exponential GARCH model and its estimation under alternative multivariate distributions, but did not provide any asymptotic theory.
Although it is not essential, leverage is an attractive feature of the EGARCH model. Since EGARCH is derived as a discrete-time approximation to a continuous-time stochastic volatility process, and is expressed in logarithms, the exponential operator is required to obtain conditional volatility, which is guaranteed to be positive. Therefore, no restrictions are required for conditional volatility to be positive.
However, the statistical properties for the (quasi-) maximum likelihood estimator of the EGARCH parameters are not available under general conditions, but rather only for special cases under highly restrictive and unverifiable conditions. It is often argued heuristically that the reason for the lack of general statistical properties arises from the presence in the model of an absolute value of a function of the parameters, which does not permit analytical derivatives, and hence does not permit (quasi-) maximum likelihood estimation.
Some specific statistical results are available under highly restrictive assumptions that cannot readily be verified. For example, Straumann and Mikosch [
12] assume that conditional volatility models are solutions to stochastic recurrence equations which satisfy a contraction property, and derive some asymptotic results for the EGARCH(1,0), or EARCH(1) model. However, their regularity conditions are difficult to interpret or verify.
Wintenberger [
13] proves consistency using continuous invertibility, which is assumed to hold for the EGARCH(1,1) model, and shows asymptotic normality for the quasi-maximum likelihood estimator of EGARCH(1,1) under “non-verifiable” conditions, and asymptotic normality for the stable quasi-maximum likelihood estimator of an invertible EGARCH(1,1) model. However, the sufficient conditions for invertibility seem to be restrictive on the admissible parameter space, and cannot be verified.
Demos and Kyriakopoulou [
14] present sufficient conditions under which the EGARCH(1,1) processes have bounded first- and second-order variance derivatives, and the expectation of the supremum norm of the second order log-likelihood derivative is finite. These sufficient conditions for asymptotic normality also restrict the admissible parameter space, and are difficult to verify.
It is shown in this paper for the non-leverage case that the EGARCH model can be derived from a random coefficient complex nonlinear moving average (RCCNMA) process, and that the reason for the lack of statistical properties of the estimators of EGARCH under general conditions is that the stationarity and invertibility conditions for the RCCNMA process are not known.
The remainder of the paper is organized as follows. In
Section 2, the EGARCH model is discussed.
Section 3 presents a RCCNMA process, from which EGARCH is derived in
Section 4. Some concluding comments are given in
Section 5.
2. EGARCH
Let the conditional mean of financial returns be given as:
where
yt = Δlog
Pt represents the log-difference in stock prices (
Pt),
It−1 is the information set at time
t−1, and
εt is conditionally heteroskedastic.
The EGARCH specification of Nelson [
3,
4] is given as:
where the standardized shocks,
ηt, are given by
,
ηt ~ iid (0,
ω), |
β|<1 and is the stability condition when log
ht−1 is included in the model. Asymmetry exists if
γ ≠ 0, while leverage exists if
γ < 0 and
γ <
α < −
γ. The specification in Equation (2) is EGARCH(1,1), but this can easily be extended to EGARCH(
p,
q).
As
ηt−1 is a function of both
εt and
, each of which is a function of the parameters through Equations (1) and (2), it is clear that quasi-maximum likelihood estimation of EGARCH is problematic as |
ηt−1| is not differentiable with respect to the parameters. Moreover, invertibility of EGARCH is also problematic because of the presence of the logarithmic transformation as well as the absolute value function.
4. One Line Derivation of EGARCH
It follows from Equation (3) that:
The use of an infinite lag for the RCCNMA process in Equation (3) would yield the EGARCH model in Equation (2).
It is worth noting that the transformation of
ht in Equation (4) is not logarithmic, but the approximation given by:
can be used to replace
ht in Equation (4) with 1 + log
ht.
The interpretation of leverage, whereby γ < 0 and γ < α < −γ, is lost in the above derivation because both α and γ are required to be positive.
More importantly, in terms of interpreting the model, the derivation of EGARCH, albeit without the logarithmic transformation, in Equation (4) shows that the statistical properties of the (quasi-) maximum likelihood estimator of the EGARCH parameters do not exist under general conditions because the model is based on a RCCNMA process, for which the stationarity and invertibility conditions are not known.
5. Conclusion
The paper was concerned with one of the most popular univariate asymmetric conditional volatility models, namely the exponential GARCH (or EGARCH) specification. The EGARCH model is popular, among other reasons, because it can capture both asymmetry, namely the different effects on conditional volatility of positive and negative effects of equal magnitude, and leverage, which is the negative correlation between returns shocks and subsequent shocks to volatility.
The statistical properties for the (quasi-) maximum likelihood estimator of the EGARCH parameters are not available under general conditions, but rather only for special cases under highly restrictive and unverifiable conditions. It is often argued heuristically that the reason for the lack of general statistical properties arises from the presence in the model of an absolute value of a function of the parameters, which does not permit analytical derivatives, and hence does not permit (quasi-) maximum likelihood estimation.
It was shown in the paper for the non-leverage case that the EGARCH model could be derived from a random coefficient complex nonlinear moving average (RCCNMA) process, and that the reason for the lack of statistical properties of the estimators of EGARCH under general conditions is that the stationarity and invertibility conditions for the RCCNMA process are not known.