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234 J. M. Rodríguez-Poo et al.<br />

As an example, set ϕ(u, v) = exp(u+v). Then, the quasi-likelihood function corresponds<br />

to the log-likelihood function from an exponential distribution and a Log-ACD<br />

representation, i.e.,<br />

n�<br />

�<br />

�ψ(¯di−1, − ¯yi−1; ϑ1) + φϑ1 (t′ i−1 )� di<br />

+<br />

exp � ψ(¯di−1, ¯yi−1; ϑ1) + φϑ1 (t′ i−1 )�<br />

�<br />

,<br />

i=1<br />

and, after some derivations, the estimator (19) takes the explicit form<br />

ˆφϑ1 (t′ ⎧<br />

⎪⎨<br />

1 � �<br />

ni=1 t ′<br />

0−t nh K<br />

0 ) = log<br />

⎪⎩<br />

′ �<br />

i di<br />

h exp � ψ(¯di−1,¯yi−1;ϑ1) �<br />

1 � �<br />

ni=1 t ′<br />

0−t nh K<br />

′ ⎫<br />

⎪⎬<br />

�<br />

i ⎪⎭<br />

h<br />

.<br />

The above expressions are obta<strong>in</strong>ed by assum<strong>in</strong>g a seasonal component for a given period<br />

(e.g., daily). But it is also possible to extend this method to cover several seasonal effects.<br />

For example, we may be <strong>in</strong>terested <strong>in</strong> look<strong>in</strong>g at whether the seasonal patterns for each<br />

day <strong>of</strong> the week are different and test the differences us<strong>in</strong>g confidence bands. For sth<br />

day <strong>of</strong> the week, we have for the exponential density and the Log-ACD representation,<br />

ˆφs(t ′<br />

⎧<br />

⎪⎨<br />

� 1 ⌊n/5⌋ �n nh j=1 i=1<br />

0 ) = log<br />

⎪⎩<br />

K<br />

�<br />

t ′<br />

0<br />

−t ′ � �<br />

i I ⌊ h<br />

t−to<br />

�<br />

di + 1⌋=js<br />

tc−to exp{ψ( ¯d i−1 ,¯y i−1 ;ϑ1)} � 1 ⌊n/5⌋ �n nh j=1 i=1 K � t0−t � �<br />

i I ⌊ h<br />

t−to<br />

⎫<br />

⎪⎬<br />

�<br />

+ 1⌋=js<br />

⎪⎭<br />

tc−to<br />

for s = 1,...,5. I(·) is the <strong>in</strong>dicator function and ⌊x⌋ is the <strong>in</strong>teger part <strong>of</strong> x.<br />

The follow<strong>in</strong>g Theorem shows the equivalence <strong>of</strong> statistical results for mak<strong>in</strong>g correct<br />

<strong>in</strong>ference (notation is simplified, as <strong>in</strong> Theorem 1, and the pro<strong>of</strong> is given <strong>in</strong> theAppendix):<br />

Theorem 2:<br />

Appendix then,<br />

Under conditions (A.1) to (A.5), and (B.1) to (B.6), provided <strong>in</strong> the<br />

√ � � �<br />

n ˆϑ1n − ϑ1 →d N 0,� −1<br />

�<br />

, ϑ1<br />

(20)<br />

where<br />

and<br />

where<br />

�ϑ1 =−E<br />

V � t ′ 0 ; η� =<br />

�<br />

∂ 2<br />

∂ϑ1∂ϑ T 1<br />

log q � d,ϕ � ψ(¯d, ¯y; ϑ1), φ(t ′ ) ���<br />

,<br />

√ �<br />

nh ˆφ ˆϑ1 (t′ 0 ) − φ(t′ 0 )<br />

�<br />

→d N � 0,V � t ′ 0 ; η�� , (21)<br />

� K 2 (u)du<br />

×<br />

f(t ′ 0 )<br />

�� d−ϕ(ψ(ϑ1),φ) ∂<br />

E V (ϕ(ψ(ϑ1),φ)) ∂φϕ (ψ(ϑ1),<br />

�2 ��t<br />

φ) ′ = t ′ �<br />

0<br />

�<br />

∂<br />

E × ∂φϕ (ψ(ϑ1), φ) 2 � � ,<br />

2<br />

�t ′ = t ′<br />

0<br />

1<br />

V0(ϕ(ψ(ϑ1),φ))<br />

and f(t ′ 0 ) is the marg<strong>in</strong>al density function <strong>of</strong> t′ ,asn tends to <strong>in</strong>f<strong>in</strong>ity.

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