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78<br />

As 0 < a m < 1; L ð Þ ¼ 1 a<br />

mL is a stationary polynomial <strong>in</strong> L. Then,<br />

ðatmtÞ ¼ ðLÞ 1 Ax;tðLÞ 0 xt þ ðLÞ 1 EC<br />

a st 1 þ ðLÞ 1 " a t : (A.1)<br />

Let Δ=(1−L) be the first differenc<strong>in</strong>g operator. Pre-multiply<strong>in</strong>g <strong>in</strong> (A.1) by Δ,<br />

and lett<strong>in</strong>g ðLÞ 1 Ax;tðLÞ ¼ eAx;t ðLÞ and ðLÞ 1 EC ¼ eECð Þ we obta<strong>in</strong><br />

a<br />

a L<br />

at ¼ mt þ eAx;t ðLÞ 0 xt þ ~ EC<br />

a L ð Þst1 þ ðLÞ" a t ; (A.2)<br />

where θ(L)" t a =(1−L)(1−αm a L)"t a which can be approximated by a mov<strong>in</strong>g<br />

average polynomial <strong>of</strong> f<strong>in</strong>ite order, say q, ðLÞ" a t<br />

eðLÞ" a t ¼ 1 e1<br />

aL e2<br />

aL2 eq<br />

aLqÞ" a t . Similar expansions are made with eAx;t ðLÞ and eEC a L ð Þ. Substitut<strong>in</strong>g<br />

Eq. (3.1) <strong>in</strong> (A.2) we have<br />

at ¼ eAx;t ðLÞ 0 xt þ e EC<br />

a L ð Þst1 þ a t : (A.3)<br />

The error term a t ¼ eðLÞ" a t þ BvB 2;t þ SvS 2;t þ v1;t has an <strong>in</strong>vertible mov<strong>in</strong>g<br />

average (MA) representation. Invert<strong>in</strong>g the MA or alternatively add<strong>in</strong>g longenough<br />

dynamics <strong>of</strong> the regressors <strong>of</strong> (A.3), Δat and also Δbt (s<strong>in</strong>ce they are<br />

<strong>high</strong>ly correlated), the mov<strong>in</strong>g average structure disappears. Therefore, Eq. (A.3)<br />

could parsimoniously be approximated by<br />

at ¼ e EC<br />

a L ð Þst1 þ AaaðLÞ at 1 þ AabðLÞ bt 1 þ eAx;t ðLÞ 0 xt þ u a t : (A.4)<br />

The errors are white noise, E(u t a )=0 and E(ut a ,ut−k a )=0∀k ≠0, with the<br />

autoregressive polynomials A ij(L) hav<strong>in</strong>g all roots outside the unit circle. Let,<br />

ð Þ 0 xt ¼ A B aB L<br />

B<br />

ð Þf ð Þx B t þ ASaS L<br />

S<br />

ð Þf ð Þx S t :<br />

eAx;t L<br />

aB MCt 1; Dt 1<br />

Equation (A.4) can now be written as<br />

aS MCt 1; Dt 1<br />

at ¼ e EC<br />

a L ð Þst1 þ AaaðLÞ at 1 þ AabðLÞ bt 1 þ AaB;tðLÞx B t<br />

þAaS;tðLÞx S t þ uat ;<br />

(A.5)<br />

which is the first equation <strong>of</strong> the system Eq. (3.7).<br />

The correspond<strong>in</strong>g equation for Δbt is similarly obta<strong>in</strong>ed by repeat<strong>in</strong>g the<br />

previous steps for Eq. (3.3) obta<strong>in</strong><strong>in</strong>g the equivalent expression <strong>of</strong> Eq. (A.3) for bt<br />

bt ¼ eBx;t ðLÞ 0 xt þ e EC<br />

b L ð Þst1 þ b t : (A.6)<br />

Notice that ξ t a and ξt b have a component <strong>in</strong> common ( B v2,t B + S v2,t S +v1,t) and,<br />

therefore, they are mutually correlated. This correlation depends on the importance<br />

<strong>of</strong> the idiosyncratic components <strong>in</strong> each <strong>of</strong> the residuals. From the same arguments,<br />

we can obta<strong>in</strong> the equivalent model to (A.5) for Δb t with white noise errors<br />

bt ¼ e EC<br />

b L ð Þst1 þ AbaðLÞ at 1 þ AbbðLÞ bt 1 þ AbB;tðLÞx B t<br />

þAbS;tðLÞx S t þ ubt :<br />

A. Escribano and R. Pascual<br />

(A.7)

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