recent developments in high frequency financial ... - Index of
recent developments in high frequency financial ... - Index of
recent developments in high frequency financial ... - Index of
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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)