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182<br />

JBX HAL<br />

Fig. 6 Autocorrelation function <strong>of</strong> the non-zero absolute price changes Si|Si > 0 for Jack <strong>in</strong> the<br />

Box Inc. (JBX) and Halliburton p ffiffi Company (HAL). The dashed l<strong>in</strong>es mark the approximate 99%<br />

confidence <strong>in</strong>terval 2:58 = en , where ñ is the number <strong>of</strong> non-zero price changes<br />

VSi ½ jSi > 0; Di; F i 1Š ¼ 2 !i<br />

¼ Si 1 #i<br />

! 2 i<br />

ð1 #iÞ<br />

2 #i<br />

1 #i<br />

; (2.22)<br />

where #i ¼ ð þ !iÞ<br />

: In this specification, both mean and variance are monotonic<br />

<strong>in</strong>creas<strong>in</strong>g functions <strong>of</strong> the variable ωi that is assumed to capture the variation<br />

<strong>of</strong> the conditional distribution depend<strong>in</strong>g on Di and F i 1 .<br />

As noted above, volatility cluster<strong>in</strong>g <strong>of</strong> asset returns is a well-known property,<br />

which also occurs at <strong>high</strong> frequencies. This is confirmed by the autocorrelation<br />

function <strong>of</strong> the nonzero absolute price changes shown <strong>in</strong> Fig. 6, which reveals a<br />

significant autocorrelation <strong>of</strong> this specific volatility measure. For the less frequently<br />

traded stock JBX, the correlations die out quicker than for HAL where<br />

significant but small correlations can be observed even after more than 25 trades.<br />

In order to take <strong>in</strong>to account the dynamics <strong>of</strong> Si we follow Rydberg and<br />

Shephard (2002) and impose a GLARMA structure on ln ωi as follows: 9<br />

ln !i ¼ 0 d Di þ Pm<br />

with i ¼ 0 þ S ð ; ; KÞþ<br />

Pp<br />

l¼1<br />

l¼0<br />

BlZ S i l þ i<br />

l i lþ Pq<br />

l¼1<br />

l"i 1þ Pr<br />

l¼1<br />

l j"ilj: R. Liesenfeld et al.<br />

(2.23)<br />

S<strong>in</strong>ce it is a well-known stylized fact for <strong>high</strong> frequent f<strong>in</strong>ancial data that there<br />

exists <strong>in</strong>traday seasonality <strong>in</strong> price volatility, we <strong>in</strong>troduce the seasonal component<br />

S(ν, τ, K)=ν 0τ +∑ K k=1ν 2k −1s<strong>in</strong> (2π(2k−1)τ)+ν 2k cos (2π(2k)τ). This Fourier flexible<br />

form is to capture <strong>in</strong>traday seasonality <strong>in</strong> the absolute price changes, where τ is<br />

9 Similar to the alternative specification discussed <strong>in</strong> the context <strong>of</strong> the ACM model one could<br />

also specify a dynamic latent process for ωi. See Zeger (1988) and Jung and Liesenfeld (2001) for<br />

examples.

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