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Published online by Cambridge University Press: 22 August 2005
Strong consistency and asymptotic normality are established for the quasi-maximum likelihood estimator for a class of ARCH(q) models. The conditions are that the ARCH process is geometrically ergodic with a moment of arbitrarily small order. Furthermore for consistency, we assume that the second-order moment exists for the nondegenerate rescaled errors and, similarly, that the fourth-order moment exists for asymptotic normality to hold. Contrary to existing literature on (G)ARCH models the parameter space is not assumed to be compact; we only impose a lower bound for the constant term in our parameterization of the conditional variance. It is demonstrated that the general conditions are satisfied for a range of specific models.We are grateful to the editor and the referees for their very helpful and detailed suggestions, which, we believe, improved the paper substantially. We thank Søren T. Jensen for stimulating discussions and Jonathan Dennis for helpful research assistance. Rahbek acknowledges continuing financial support from the Danish Social Sciences Research Council. Kristensen received funding from the Danish Research Agency and the Financial Markets Group, LSE, during this research.
Since the introduction of the autoregressive conditional heteroskedastic (ARCH) model by Engle (1982), the basic model has been extended and generalized in various ways; see, e.g., Bera and Higgins (1993). One of the most popular estimators for this class of models is the quasi-maximum likelihood estimator (QMLE) where the Gaussian likelihood is used for the true but possibly unknown likelihood. We derive the asymptotic properties of the QMLE for a class of parametric univariate ARCH(q) models, which includes many of the models in the literature; for example, the linear ARCH model (Engle, 1982) and various asymmetric ARCH models (Guegan and Diebolt, 1994; Glosten, Jegannathan, and Runke, 1993; Gourieroux and Monfort, 1992). Except for the linear ARCH model, none of these models has been treated explicitly before.
We show that the QMLE for this class is consistent and asymptotically normally distributed under weak conditions: we require the existence of an arbitrarily small (log) order moment of the ARCH process itself; only the second-order moment of the rescaled errors is required for consistency, whereas the fourth moment is needed for asymptotic normality. Furthermore, in contrast to most of the existing work, the parameter space is not assumed to be compact. Also, we allow for no ARCH in the proof of consistency; to establish asymptotic normality we assume that ARCH is present, however, because the proof is based on a standard Taylor expansion.
As a further condition we assume that the ARCH process is geometrically ergodic, which is verified for the previously mentioned models under weak conditions. See, e.g., An, Chen, and Huang (1997); Basrak, Davis, and Mikosch (2002); Carrasco and Chen (2002); Lu and Jiang (2001); and Masry and Tjøstheim (1995) for further results on geometric ergodicity in ARCH models. In general, a Markov process

is geometrically ergodic with associated invariant probability measure π, if, for some ρ < 1 and all

, ∥Qn(·|x) − π(·)∥ ≤ Mx ρn for some Mx > 0. Here ∥·∥ denotes the total variation norm and Qn the n-step transition probability (for details, see Meyn and Tweedie, 1993). In particular, if X1 ∼ π then {Xt} is stationary and ergodic. Geometric ergodicity implies that the stationary version is β-mixing with exponentially decaying mixing coefficients (see Davydov, 1973; Doukhan, 1994). Importantly, the strong law of large numbers (LLN) holds for any given initial distribution of the geometrically ergodic process (cf. Meyn and Tweedie, 1993, Thm. 17.0.1), which is used repeatedly in the proofs.
Finally, it should be noted that we consider a global QMLE, in contrast to much of the existing literature where local properties are derived. Our consistency proof is based on Huber (1967) and Pfanzagl (1969). Jeantheau (1998) applies Pfanzagl (1969) also to give conditions for consistency of the QMLE in a broad class of (G)ARCH models but assumes that the stationary version of the process is observed and that the parameter space is compact, contrary to here.
Although the QMLE is often used in empirical studies, its asymptotic properties have mainly been derived for the linear (G)ARCH model. Weiss (1986) proved consistency and asymptotic normality for the QMLE in the linear ARCH(q) model requiring the existence of the fourth-order moment of the ARCH process, which contradicts empirical work. The moment conditions were weakened in Lee and Hansen (1994) and Lumsdaine (1996); both of these studies considered the linear GARCH(1,1) model. Lee and Hansen (1994) require a stationary solution to the model and the existence of fourth-order moment of the rescaled errors, whereas the parameter space is assumed to be compact and restricted further. Lumsdaine (1996) considers GARCH processes with second-order moments and the I-GARCH process and assumes that the rescaled errors have 32nd-order moments in addition to restrictions on the parameter space. In Berkes, Horvarth, and Kokoszka (2003), the results are extended to hold for the linear stationary GARCH(p,q) model under weaker conditions on the rescaled errors. Jensen and Rahbek (2004a, 2004b) establish that the asymptotic results hold for the entire parameter region, including the nontationary explosive case, for ARCH(1) and GARCH(1,1) models. Finally, Ling and Li (1998) investigate asymptotics for unit-root ARMA-GARCH models. All of the aforementioned assumes that the parameter space is compact or addresses local consistency.
In the following section we present the model and the assumptions applied. In Section 3 we state the consistency result, and the asymptotic distribution of the QMLE is in Section 4. In Section 5, we go through various popular parametrizations, and show that they satisfy the assumptions made in the general model. We conclude in Section 6. All proofs together with technical lemmas are found in Appendixes A and B, respectively. Appendix C contains two propositions.
Throughout the paper we will use the following notation. For any function

, we shall write the partial derivative w.r.t. θ as Df (x,θ) = (Dj(fi x,θ))i,j where Dj fi = (∂fi(x,θ)/∂θj); the second-order partial derivatives are written as D2f (x,θ) = (Djk fi(x,θ))i,j,k where Djk fi = (∂2fi(x,θ)/∂θj∂θk). Also, C and Ci, i = 1,2,…, will denote generic constants. For any process Xt, use {Xt} to denote the infinite sequence X1,X2,….
Assume that we have observed (yt,xt−1)t=1,…,n with

given by the ARCH model,


with parameter

and where x0 is fixed.
1The following results can be extended to allow for x0 being random as long as its distribution does not depend on θ.
Some of the parametrizations that fall within our framework are given in Table 1: linear ARCH (Engle, 1982), β-ARCH (Guegan and Diebolt, 1994) for known β > 0, μ-ARCH (Engle and Bollerslev, 1986) for known μ > 0, threshold or GJR-ARCH (Glosten et al., 1993; Li and Li, 1996; Zakoian, 1994), SD-ARCH (Schwert, 1990), and TARCH (Gourieroux and Monfort, 1992).
Examples of parametrizations
For the asymptotic analysis, we assume that for θ at the true value θ0 there exists a stationary solution to equations (1)–(2) and denote this {(yt*,xt−1*)}. However, the process {(yt,xt−1)} may be nonstationary as x0, and hence y1, need not be initiated from the stationary distribution. To emphasize this, in the following discussion let h0t = ω0 + α0′xt−1 and h0t* = ω0 + α0′xt−1* denote the true conditional variance process corresponding to {(yt,xt−1)} and {(yt*,xt−1*)}, respectively. Correspondingly, write ht = ω + α′xt−1 and ht* for any θ ≠ θ0.
The following conditions are assumed to hold.
C.1. The innovations {zt} are i.i.d.(0,1) with E [|log(zt2)|] < ∞.
C.2. The parameter space is given by

for some fixed ω > 0.
C.3. For all t ≥ 1, (i) xi,t−1 ≥ 0, 1 ≤ i ≤ m, (ii) xt−1 is measurable w.r.t.

for some finite q ≥ 1, and (iii) P(β′xt−1* ≠ c) > 0 for any

.
C.4. (i) {(yt,xt−1)} is geometrically ergodic such that for the true parameter θ0 ∈ Θ a stationary solution {(yt*,xt−1*)} exists with (ii) E [|log(xi,t*)|] < ∞, 1 ≤ i ≤ m.
The assumptions made in C.1 about the rescaled errors are fairly standard, where we note that the i.i.d. assumption is needed to obtain the Markov property of {(yt,xt−1)}. Lee and Hansen (1994) assumed that {zt} was a stationary martingale difference sequence. It is possible here to introduce limited dependence in the {zt} process without removing the Markov property, e.g., by assuming that {(zt,…,zt−p)} is a geometrically ergodic Markov chain for some finite p ≥ 0 and satisfying

where

includes the lagged zt's too. For simplicity, we maintain the i.i.d. assumption however.
Condition C.2 defines the noncompact parameter space Θ for the statistical analysis; i.e., the quasi-likelihood function defined subsequently is maximized over θ ∈ Θ. Condition C.2 implies—together with C.3(i) and (ii)—that ht > 0 for all θ ∈ Θ.
Note that the only real restriction on the parameter space Θ is the requirement that the constant term, ω, is bounded from below by some ω > 0. It is used when deriving a uniform lower bound for the quasi-likelihood function in the proof of Lemma 4 and appears difficult to avoid.
For the asymptotics, or the probability analysis, condition C.4(i) of geometric ergodicity restricts the possible values of the true value θ0 in Θ. As noted geometric ergodicity implies that the strong LLN holds for {(yt,xt−1)} irrespective of initial values. Explicit conditions for which C.4 holds in some leading examples are given in Section 5, Theorem 3 and Corollary 1. The assumption of geometric ergodicity can be exchanged with the weaker condition that there exists a version of {(yt,xt−1)} that is stationary and ergodic. But then one needs to either (i) assume that it is the stationary version that has been observed (see Jeantheau, 1998) or (ii) show that the observed quasi-likelihood function converges uniformly toward the stationary version of it (see Lee and Hansen, 1994).
Condition C.3(iii) is a nondegeneracy condition that is used in the proof of identification of θ0. A sufficient, but stronger, condition for C.3(iii) would be that E [xt−1*xt−1*′] is nonsingular, which however requires that the moment exists. For example, in the linear ARCH model we would have to require that E [yt*4] < ∞, contradicting empirical findings.
Finally note that it can be shown that a simple condition for the moment in C.4(ii) to exist is E [∥xt*∥p] < ∞ for some p > 0. And if one assumes that Θ is compact, the log-moment condition in C.1 can be removed and C.4(ii) weakened to E [|log(h0t*)|] < ∞; cf. the proof of Lemma 4.
Our first main result is that the QMLE

is strongly consistent, where

Here

We furthermore define the moment function

which takes values on the extended real line

. This is well defined by Lemma 1. To allow for noncompact Θ when proving consistency, we use the strategy of Huber (1967). The idea is to find a compact set

, as defined in (B.2) in Appendix B, for which

and such that

for some ε > 0. It then follows that

, and we can apply a consistency result of Pfanzagl (1969) on the compact set

. This involves showing that L(θ) is well defined, that θ0 is identified by L(θ), and that θ [map ] L(θ) is continuous.
THEOREM 1. Under C.1–C.4, the QMLE defined by (3) satisfies

.
In this section we show that the QMLE is asymptotically Gaussian. To prove this result, we impose the following assumptions in addition to C.1–C.4.
N.1. For θ0 = (ω0,α0), ω0 > ω and α0,i > 0 for i = 1,…,m.
N.2. κ4 = E [(zt2 − 1)2] ∈ (0,∞).
Assumption N.1, or equivalently θ0 ∈ intΘ, is needed for a Taylor expansion of the quasi-likelihood function around θ0. The case of no ARCH, α0 = 0, is not straightforward (see, e.g., Andrews, 1999) and will be left for future work. The second condition, N.2, ensures that the asymptotic variance of the QMLE exists.
The proof of asymptotic normality is standard (see, e.g., Basawa, Feigin, and Heyde, 1976), based on a Taylor expansion of the score,

around θ0. In particular, we show in Lemma 9 that

where

and furthermore in Lemma 8 that uniformly over θ in a compact set containing θ0,

THEOREM 2. Under C.1–C.4 and N.1 and N.2,

where V(θ0) and H(θ0) are given in (6) and (7), both are positive definite. Furthermore,


are strongly consistent estimators of V(θ0) and H(θ0), respectively.
Remark 1. In the case where zt ∼ N(0,1), the result collapses to the standard maximum likelihood estimator (MLE) result with κ4 = 2 and H(θ0) being the information matrix multiplied by 2.
In this section we consider the models shown in Table 1 and demonstrate that under suitable conditions they satisfy C.2–C.4, which are the only assumptions made on the actual parametrization. The remaining assumptions concern the error structure (C.1 and N.2) and the location of θ0 in the parameter space (C.2 and N.1).
To do so we consider a specific subclass of models of (1)–(2) given by

which contains the models in Table 1 as special cases, except the SD-ARCH because of the cross-product terms. This is treated separately as part of Corollary 1, which follows. In (10),

such that the dimension of xt−1 is m = qp. For this class, we address the two questions, identification, C.3, and geometric ergodicity, C.4, in turn. Specifically, we make the following assumptions about g.
G.1.

is measurable, j = 1,…,p.
G.2. For any

.
G.3. There exist constants a0(i) > 0, a1(i) ≥ 0, i = 1,…,q, with

, such that for

as |y| → ∞.
Note that by Lemma 10, G.1 and G.2 imply C.3. The proof exploits that as yt−i = ht−i1/2zt−i, G.2 can be seen as a conditional (on ht−i1/2 = h) version of C.3(iii) when xt−1 takes the form (11). The condition G.3 implies that C.4 holds by using the so-called drift criterion from Markov chain theory.
THEOREM 3. Assume (i) that C.1, C.2, N.1, and N.2 hold with zt ∼ fz·λ, where fz > 0 is a lower semicontinuous density w.r.t. the Lebesgue measure λ. Assume further (ii) that α′xt−1 is given by (10) and that G.1–G.3 hold. Then the QMLE is strongly consistent and asymptotically Gaussian.
As a corollary we state the results specifically for the models in Table 1.
COROLLARY 1. Assume that the assumptions of Theorem 3 hold. Assume further at the true parameter value for the linear ARCH(q), Σi=1qα0,i < 1; for the β-ARCH, β ∈ (0,2); for the μ-ARCH, μ ∈ (0,2); for the GJR-ARCH, Σi=1q{α0,1i + α0,2i} < 1; for the SD-ARCH, Σi=1qα0,2ii + 2Σi=1qΣj=i+1qα0,2ij < 1; and for the TARCH,

. Then the QMLE for each model is strongly consistent and asymptotically Gaussian.
Remark 2. Apart from the TARCH case, the last conditions in Corollary 1 are only needed to establish geometric ergodicity. So if weaker conditions for this property can be found, then under these conditions the results remain valid. For example, in the linear ARCH(1) model, we may weaken the preceding condition, α0 = α0,1 < 1, to log(α0) < −E [log(zt2)] (see Lemma 11). Note that this condition is necessary and sufficient for stationarity and ergodicity (see Nelson, 1990).
Remark 3. The condition given for the TARCH model is used to establish identification. It might be possible to find weaker conditions for this property to hold.
We have shown consistency and asymptotic normality for the QMLE in a general class of ARCH models under relatively weak conditions. Several extensions are of interest: GARCH models other than the linear one, more general ARCH(q) models that are not linear in the parameters, and multivariate models. The latter has already been investigated by Comte and Lieberman (2003) and Ling and McAleer (2003), but it could be interesting to consider other parametrizations than the ones they work with and perhaps weaken the restrictions they impose.
Proof of Theorem 1. We first establish that

where

is the compact set given in (B.2) in Lemma 4 with

. Observe first that by the strong LLN,

where L(θ0) < ∞ by Lemma 3. Next, applying Lemma 4 and the definition of l(yt|xt−1) therein, together with the strong LLN gives

Combining (A.1) and (A.2), we obtain that

. Hence we can restrict attention to

and redefine

. The set

is compact, and we can apply Proposition 2: l(yt|xt−1;θ) = log(ht) + yt2/ht is continuous in θ for all (yt,xt−1); by Lemma 1, L(θ) > −∞, so the moment is well defined; identification of θ0 holds by Lemma 3. Finally, for any compact subset

by Lemma 1. We can therefore conclude that

as desired. █
Proof of Theorem 2. The result is obtained by the following standard Taylor expansion of

in (5). Note first that by Lemma 5, Sn(θ) is well defined for all θ ∈ Θ. By N.1, there exists a ball B(θ0,δ) ⊆ Θ. We then choose the compact

such that

,

where ω ≤ ωl < ωu and 0 < αil < αiu, i = 1,…,m. As

by Theorem 1, such that

by the definition of

and hence,

where Hn(θ) is given in (7) and

because

. Lemmas 8 and 9 then imply

To prove that

, define

and use the following inequality:

By Lemma 7(ii)

with V(θ) continuous. Thus,

implies

. Similarly,

, by Lemma 8. █
Proof of Theorem 3. The result follows by showing that C.3 and C.4 hold. C.3(i) and (ii) hold by G.1 and G.2; C.3(iii) holds by Lemma 10; and finally, C.4 holds by Lu (1998, Thm. 3.1 with s(y) = |y|). █
Proof of Corollary 1. The result follows for all models but the SD-ARCH by establishing G.1–G.3. Assumption G.1 trivially holds, and G.3 is simple to verify for each model in question under the assumptions of the corollary. Next, turn to G.2.
For the linear and μ-ARCH cases, note that h|zt|μ ≠ b, a.s. for μ > 0, and hence G.2 holds. Regarding the β and the GJR-ARCH cases, note likewise that

For the TARCH case note that the variance of the discrete variable

is positive as for any

and, finally, that zt has a positive density. For the SD-ARCH case, note first that geometric ergodicity follows by Lu (1998, Thm. 3.1). This implies that the Markov chain has the Lebesgue measure, λ, as an irreducibility measure. This again implies, by the Lebesgue decomposition, that the invariant measure has a component that has a strictly positive density w.r.t. λ. Thus, P((yt*,…,yt−q+1*) ∈ A) > 0 for any set with λ(A) > 0. In particular,

because

is a continuous nonconstant function. █
LEMMA 1. Under C.1–C.4, L(θ) = E [l(yt*|xt−1*;θ)] > −∞. Furthermore, it holds that for any set

.
Proof. By C.2, l(yt*|xt−1*;θ) ≥ log(ht*) ≥ log(ω) ≥ log(ω), for any θ ∈ Θ, implying

Hence, L(θ) is well defined and bounded from below. The first inequality also implies that

. █
LEMMA 2. Under C.1–C.4, ht* = h0t* a.s. ⇒ θ = θ0.
Proof. Assume that ht* = h0t* a.s., or equivalently,

To prove that θ = θ0, assume first α = α0, which implies ω = ω0. If α ≠ α0, (α − α0)′xt−1* = −(ω − ω0), which contradicts C.3(iii). █
LEMMA 3. Under C.1–C.4, L(θ0) < ∞ and L(θ0) ≤ L(θ) with equality if and only if ht* = h0t* a.s. In particular, L(θ0) < L(θ) for all θ ≠ θ0.
Proof. First observe that L(θ0) < ∞. Because

it follows by C.1 and C.4(ii) that

Let θ ≠ θ0 be given. Then by Lemma 1 either (i) L(θ) = ∞ or (ii) L(θ) ∈ (−∞,∞). If (i) holds, L(θ0) < ∞ = L(θ). If (ii) holds, the following calculations are allowed:

where we made use of C.1. From the last equality,

with equality if and only if h0t* = ht* a.s. Then by Lemma 2, L(θ) = L(θ0) if and only if θ = θ0. █
LEMMA 4. Under C.1–C.4, there exist a compact set

, and a function l such that

where E [l(yt*|xt−1*)] = L(θ0) + ε for some ε > 0.
Proof. Choose

as

for some δ > 0 specified subsequently. Let

be given; then either (i) ω0 + δ < ω or (ii) α0,i + δ < αi, for at least one i ∈ {1,…,m}. In the first case,

whereas in the second case

Define l(yt|xt−1) = log(δ) + m(xt−1) where

for some ε > 0. From the preceding inequalities, l(yt|xt−1;θ) ≥ l(yt|xt−1) a.s. Finally, by C.4, (iii) E [|m(xt−1*)|] < ∞ such that

, and

LEMMA 5. Under C.1–C.4, θ [map ] s(y|x;θ) and θ [map ] Ds(y|x;θ) exist and are continuous for all

.
Proof. First observe that θ [map ] ht is twice continuously differentiable, so by the chain rule so is θ [map ] l(yt|xt−1;θ). Next,

where Dht = [1, xt−1′]′ and it has been used that D2ht = O(m+1)×(m+1). █
LEMMA 6. Under C.1–C.4 and N.1 and N.2, there exists a constant C < ∞ that does not depend on θ such that for any

, where

is defined in> (A.3),
(i) 1/ht ≤ C,
(ii) yt2/ht ≤ C(1 + zt2), and
(iii) |Di ht|/ht ≤ C,i = 1,…,m + 1.
Proof. The fact that ht ≥ ω ≥ ω establishes (i). To prove (ii), use that for any

, α > 0, i = 1,…,m, such that
LEMMA 7. The following conditions hold under C.1–C.4 and N.1 and N.2, with

defined in (A.3)
(i)

, where C < ∞ does not depend on θ.
(ii) The moment function θ [map ] V(θ) = E [s(yt*|xt−1*;θ)s(yt*|xt−1*;θ)′] is well defined and continuous for

.
Proof. Using Lemma 6,

To prove (ii), apply the uniform LLN stated in Proposition 1 with

. The conditions stated there hold by the definition of

, Lemma 5, and the bound just derived together with N.2. █
LEMMA 8. The following conditions hold under C.1–C.4 and N.1 and N.2, with

defined in (A.3):
(i)

, where C < ∞ does not depend on θ.
(ii) The moment function θ [map ] H(θ) = E [Ds(yt*|xt−1*;θ)] is well defined and continuous for

.
(iii) The matrix H(θ0) = E [Dh0t*(Dh0t*)′/h0t*2] is nonsingular.
Proof. Applying the bounds established in Lemma 6,

for C < ∞. Because ∥Ds(yt|xt−1;θ)∥2 = [sum ]ij Dj si(yt|xt−1;θ)2, the first part has been shown to hold. The second part follows from Proposition 1 on f = Ds with

. Finally, from (B.3),

by C.1. Now, assume that H(θ0) is not positive definite; then there exists a vector λ = (c,β) ≠ 0 such that λ′Dh0t* = 0 a.s. because h0t* > 0. That is, β′xt−1* = −c a.s., which is ruled out by C.4. █
LEMMA 9. Under C.1–C.4 and N.1 and N.2,

.
Proof. First observe that Sn(θ0) is a martingale w.r.t.

defined in C.3. To see this, first note that by Lemma 7, s0t ≡ s(yt|xt−1;θ0) satisfies

by C.1, whereas E [∥s0t*∥2] = E [∥s(yt*|xt−1*;θ0)∥2] < ∞. Hence by the martingale central limit theorem in, e.g., Brown (1971), the result holds if


where E [s0t*s0t*′] is a positive definite matrix. By Lemma 7, ∥s0t∥ ≤ st ≡ C(1 + zt2), and hence

where the sequence {st} is i.i.d. with a finite second moment by C.1 and N.2. Hence,

Next, as

is a function of (yt,xt−1) with an existing first-order moment (cf. Lemma 7), the strong LLN can be applied, yielding that the averaged sum in (B.5) converges toward

Note that this holds irrespective of the initial distribution. Lemma 8 together with the fact that κ4 > 0 implies that V(θ0) is a positive definite matrix. █
LEMMA 10. Assume that C.1, C.2, and C.4 hold. Then G.1 and G.2 imply C.3.
Proof. Assumption G.1 directly implies C.3(i) and (ii). To prove (iii), let

be given. Without loss of generality β1 ≠ 0, and hence by G.2,

As

, then for any

there exists an h > 0 such that

By definition,

, and choosing

, we obtain from (B.6) that for any

,

for any

. Hence, as P(β′xt* = c) = ∫P(β′xt* = c|(yt−1*,…,yt−q*)) × dP(yt−1*,…,yt−q*), P(β′xt* = c) < 1. █
LEMMA 11. The ARCH(1) process is geometrically ergodic if log(α1) < −E log zt2.
Proof. This follows by Carrasco and Chen (2002, Thm. 1 with A(e) = α1 e2 and B(e) = ω), using Nelson (1990, proof of Thm. 2) together with Nelson (1990, Thms. 3 and 4). █
Here we state a uniform LLN and a consistency result, which are modifications of Tauchen (1985, Lem. 1) and Pfanzagl (1969, Thm. 1.12), respectively. Proofs can be obtained from the authors. In the following discussion {Xt} is a geometrically ergodic Markov chain sequence such that a stationary version {Xt*} exists. Observe that all moments are stated in terms of {Xt*}, whereas convergence takes place w.r.t. the possibly nonstationary version of {Xt}. All functions in the following exposition are assumed to be Borel-measurable.
PROPOSITION 1. Assume that

is a compact set and that the function

satisfies the following conditions.
Then,

where the mapping θ [map ] E [f (Xt*|Xt−1*;θ)] is continuous.
PROPOSITION 2. Make the following assumptions.
Then

is strongly consistent:

as n → ∞.
Examples of parametrizations