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Modell<strong>in</strong>g f<strong>in</strong>ancial transaction price movements: a dynamic <strong>in</strong>teger count data model 181<br />

and for HAL all but two correlations lie <strong>in</strong>side the 99% band. The means <strong>of</strong><br />

standardized residuals reported <strong>in</strong> Table 1 are close to zero, which should be expected<br />

from a well specified model. However, the estimated variance–covariance<br />

matrix <strong>of</strong> the standardized residuals deviate slightly from the identity matrix. This<br />

may h<strong>in</strong>t to a distributional misspecification or a misspecification <strong>of</strong> log–odds<br />

ratios Λi, which is not fully compatible with the variation <strong>in</strong> the observed variation<br />

<strong>of</strong> price change direction.<br />

2.3 Dynamics <strong>of</strong> the size <strong>of</strong> price changes<br />

In order to analyze the size <strong>of</strong> the non-zero price changes, we use a GLARMA<br />

(generalized l<strong>in</strong>ear autoregressive mov<strong>in</strong>g average) model based on a truncated-atzero<br />

Negative B<strong>in</strong>omial (Negb<strong>in</strong>) distribution. The choice <strong>of</strong> a Negb<strong>in</strong> <strong>in</strong> favor <strong>of</strong> a<br />

Poisson distribution is motivated by the fact, that the unconditional distributions <strong>of</strong><br />

the non-zero price changes show over-dispersion for both stocks. For JBX (HAL)<br />

the dispersion coefficient 7 is given by 3.770 (2.911). Moreover, note, that an atzero-truncated<br />

Poisson distribution would allow only for under-dispersion.<br />

Similar to the ACM model, the dynamic structure <strong>of</strong> this count data model rests<br />

on a recursion on lagged observable variables. A comprehensive description <strong>of</strong> this<br />

class <strong>of</strong> models can, for <strong>in</strong>stance, be found <strong>in</strong> Davis et al. (2003). Note that the time<br />

scale for absolute price changes (def<strong>in</strong>ed by transactions associated with non-zero<br />

price changes) is different from the one <strong>of</strong> the ACM model for the direction <strong>of</strong> the<br />

price changes, which is def<strong>in</strong>ed on the ticktime scale. Let u be a random variable<br />

follow<strong>in</strong>g a Negb<strong>in</strong> distribution with the p.d.f. 8<br />

fðuÞ ¼<br />

ð þ uÞ<br />

ðÞ ðuþ1Þ þ !<br />

!<br />

! þ<br />

u<br />

; u ¼ 0; 1; 2;:::; (2.19)<br />

with E(u)=ω > 0 and Var(u)=ω+ω 2 /κ. The overdispersion <strong>of</strong> the Negb<strong>in</strong> distribution<br />

depends on parameter κ >0. As κ→∞, the Negb<strong>in</strong> collapses to a Poisson<br />

distribution. The correspond<strong>in</strong>g truncated-at-zero Negb<strong>in</strong> distribution is obta<strong>in</strong>ed<br />

as h(u)=f (u)/[1−f (0)], (u = 1, 2, 3, ...), with f (0) = [κ/(κ+ω)] κ . This flexible class <strong>of</strong><br />

distributions will be used to model the size <strong>of</strong> non-zero price changes conditional<br />

on filtration F i 1 and price direction D i. Thus, for S i∣S i >0,D i, F i 1 we assume<br />

the follow<strong>in</strong>g p.d.f.:<br />

hsijDi; ð F i 1Þ<br />

¼<br />

ð þ siÞ<br />

ðÞ ðsiþ1Þ with the conditional moments:<br />

h<br />

þ<br />

i<br />

!i<br />

1<br />

1<br />

!i<br />

!i þ<br />

!i<br />

ESijSi ½ > 0; Di; F i 1Š<br />

¼ Si ¼<br />

1 #i<br />

7 Computed as variance over mean.<br />

8 See, for example, Cameron and Trivedi (1998) (Ch. 4.2.2.).<br />

si<br />

; si ¼ 1; 2; ...;<br />

(2.20)<br />

(2.21)

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