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232 J. M. Rodríguez-Poo et al.<br />

where<br />

V � t ′ 0 ,η� =<br />

� K 2 (u)du<br />

I � t ′ 0 ,η� �<br />

∂<br />

= E<br />

∂φ<br />

f(t ′ 0 )I � t ′ 0 ,η�,<br />

�<br />

�<br />

log p (d; φ,η)2�<br />

� t′ = t ′ �<br />

0<br />

and f(t ′ 0 ) is the marg<strong>in</strong>al density function <strong>of</strong> t′ ,asn tends to <strong>in</strong>f<strong>in</strong>ity.<br />

(16)<br />

(17)<br />

This theorem is very appeal<strong>in</strong>g s<strong>in</strong>ce it allows us to make <strong>in</strong>ference on the<br />

parametric and nonparametric components. However, the result depends on the<br />

correct specification <strong>of</strong> the conditional density function <strong>of</strong> the error term. In Section<br />

2.1 we weaken certa<strong>in</strong> assumptions about the error density function and show that<br />

our result rema<strong>in</strong>s valid.<br />

2.1 The GLM Approach<br />

As po<strong>in</strong>ted out <strong>in</strong> Engle and Russell (1998) and Engle (2000), it is <strong>of</strong> <strong>in</strong>terest<br />

to have estimation techniques available that do not rely on the knowledge<br />

<strong>of</strong> the functional form <strong>of</strong> the conditional density function. Two alternative<br />

approaches that allow for consistent estimation <strong>of</strong> the parameters <strong>of</strong> <strong>in</strong>terest<br />

without specify<strong>in</strong>g the conditional density are quasi maximum likelihood techniques,<br />

QML, (see Gouriéroux, Monfort and Trognon (1984)) and generalized<br />

l<strong>in</strong>ear models, GLM, (see McCullagh and Nelder (1989)). In both approaches it<br />

is assumed that di, conditional on ¯di−1 and ¯yi−1, depends on a scalar parameter<br />

θ = h � ¯di−1, ¯yi−1,t ′ �<br />

i−1 ; ϑ1,ϑ2 , and its distribution belongs to a one-dimensional<br />

exponential family with conditional density<br />

q � di| ¯di−1, ¯yi−1; θ � = exp (diθ − b(θ) + c(di)) ,<br />

where b(·) and c(·) are known functions. The ma<strong>in</strong> difference between the QML<br />

and the GLM approaches is simply a different parameterization. We adopt the GLM<br />

approach for the sake <strong>of</strong> convenience. By adopt<strong>in</strong>g the GLM parametrization, it is<br />

straightforward � to see that the ML estimator <strong>of</strong> θ solves the first order conditions<br />

ni=1 �<br />

di − b ′ (θ) � = 0. The ML estimator <strong>of</strong> θ can also be obta<strong>in</strong>ed from the<br />

solution <strong>of</strong> the follow<strong>in</strong>g equation<br />

n�<br />

i=1<br />

�<br />

di − ϕ � ψ(¯di−1, ¯yi−1; ϑ1), φ(t ′ i−1 ; ϑ2) �� ϕ ′ � ψ(¯di−1, ¯yi−1; ϑ1), φ(t ′ �<br />

i−1 ; ϑ2)<br />

V � ϕ � ψ(¯di−1, ¯yi−1; ϑ1), φ(t ′ �� = 0.<br />

i−1 ; ϑ2)<br />

(18)<br />

The parameter <strong>of</strong> <strong>in</strong>terest θ (the so-called canonical parameter) can be estimated without<br />

specify<strong>in</strong>g the whole conditional distribution function. It is only necessary to specify the<br />

functional form <strong>of</strong> the conditional mean, ϕ(·), and <strong>of</strong> the conditional variance V(·), but<br />

not the whole distribution.<br />

The relationship between the predictors <strong>in</strong> Eq. (7) and the canonical parameter is<br />

given by the l<strong>in</strong>k function. This function depends on the member <strong>of</strong> the exponential

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