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8.8 Generalized State-Space Models 303<br />

where αt+1|t and λt+1|t are, for the moment, unspecified functions of y (t) . (The subscript<br />

t +1|t on the parameters is a shorthand way to indicate dependence on the conditional<br />

distribution of Xt+1 given Y (t) .) With this specification of the state densities, the<br />

parameters αt+1|t are related to the best one-step predictor of Yt through the formula<br />

αt+1|t/λt+1|t ˆYt+1 : E Yt+1|y (t) . (8.8.38)<br />

Proof We have from (8.8.7) and (8.8.33) that<br />

E(Yt+1|y (t) ) <br />

∞<br />

∞<br />

<br />

yt+10<br />

∞<br />

−∞<br />

yt+1p(yt+1|xt+1)p<br />

−∞<br />

xt+1|y (t) dxt+1<br />

b ′ (xt+1)p xt+1|y (t) dxt+1.<br />

Addition and subtraction of αt+1|t/λt+1|t then gives<br />

E(Yt+1|y (t) ) <br />

<br />

∞<br />

−∞<br />

∞<br />

−∞<br />

<br />

b ′ (xt+1) − αt+1|t<br />

λt+1|t<br />

<br />

p xt+1|y (t) dxt+1 + αt+1|t<br />

−λ −1<br />

t+1|t p′ xt+1|y (t) dxt+1 + αt+1|t<br />

λt+1|t<br />

−λ −1<br />

t+1|tp xt+1|y (t)xt+1∞ αt+1|t<br />

+<br />

xt+1−∞<br />

λt+1|t<br />

αt+1|t<br />

.<br />

λt+1|t<br />

λt+1|t<br />

Letting At|t−1 A(αt|t−1,λt|t−1), we can write the posterior density of Xt given<br />

Y (t) as<br />

p xt|y (t) exp{ytxt − b(xt) + c(yt)} exp{αt|t−1xt − λt|t−1b(xt)<br />

+ At|t−1}/p yt|y (t−1)<br />

<br />

exp{λt|t αt|txt − b(xt) − At|t},<br />

f(xt; αt,λt),<br />

where we find, by equating coefficients of xt and b(xt), that the coefficients λt and αt<br />

are determined by<br />

λt 1 + λt|t−1, (8.8.39)<br />

αt yt + αt|t−1. (8.8.40)<br />

The family of prior densities in (8.8.37) is called a conjugate family of priors for<br />

the observation equation (8.8.35), since the resulting posterior densities are again<br />

members of the same family.

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