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statistique, théorie et gestion de portefeuille - Docs at ISFA

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ased on the fact th<strong>at</strong> the quantity<br />

ˆηT = ĉ<br />

<br />

ĉ<br />

u<br />

+ 1<br />

dˆ<br />

goes to b un<strong>de</strong>r the null hypothesis, wh<strong>at</strong>ever c being positive or neg<strong>at</strong>ive. This can be seen from the<br />

asymptotic correspon<strong>de</strong>nce given by (26) and (27). Moreover, it is proved in appendix D th<strong>at</strong> the variable<br />

<br />

ˆηT<br />

ζT = T − 1 , (36)<br />

ˆb<br />

asymptoticaly follows a χ 2 -distribution with one <strong>de</strong>gree of freedom.<br />

The results of this test are given in table 14. They show th<strong>at</strong> H0 is more often rejected for the Dow Jones<br />

than for the Nasdaq. In<strong>de</strong>ed, beyond quantile q12 = 95%, H0 cannot be rejected <strong>at</strong> the 95% confi<strong>de</strong>nce level<br />

for the Nasdaq d<strong>at</strong>a. For the Dow Jones, we must consi<strong>de</strong>r quantiles higher than q18 = 99% in or<strong>de</strong>r not to<br />

reject H0 <strong>at</strong> the 95% significance level. These results are in agreement with the central limit theorem: the<br />

power-law regime (if it really exists) is pushed back to higher quantiles due to time agreg<strong>at</strong>ion (recall th<strong>at</strong><br />

our Dow Jones d<strong>at</strong>a is <strong>at</strong> the daily scale while our Nasdaq d<strong>at</strong>a is <strong>at</strong> the 5 minutes time scale).<br />

In summary, the (SE) mo<strong>de</strong>l encompasses the Par<strong>et</strong>o mo<strong>de</strong>l as soon as one consi<strong>de</strong>rs quantiles higher than<br />

q6 = 50%. On the other hand, the null hypothesis th<strong>at</strong> the true distribution is the Par<strong>et</strong>o distribution is<br />

strongly rejected until quantiles 90% − 95% or so. Thus, within this range, the (SE) mo<strong>de</strong>l seems the best.<br />

But, for the very highest quantiles (above 95% − 98%) we cannot any more reject the hypothesis th<strong>at</strong> the<br />

Par<strong>et</strong>o mo<strong>de</strong>l is the right one. Thus, for these extreme quantiles, this last mo<strong>de</strong>l seems to slightly outperform<br />

the (SE) mo<strong>de</strong>l.<br />

However, recall th<strong>at</strong> section 4.1 has shown th<strong>at</strong> the Par<strong>et</strong>o mo<strong>de</strong>l is r<strong>et</strong>rieved as a limiting case of the (SE)<br />

mo<strong>de</strong>l when the fractional exponent c and the scale factor d go to zero <strong>at</strong> an appropri<strong>at</strong>ed r<strong>at</strong>e. Thus, all the<br />

results above are comp<strong>at</strong>ible with the (SE) mo<strong>de</strong>l in a generalized version. In<strong>de</strong>ed, <strong>de</strong>fining a generalized<br />

Str<strong>et</strong>ched-Exponential mo<strong>de</strong>l as<br />

<br />

¯Fu(x) = exp − xc−uc dc <br />

, c > 0<br />

¯Fu(x) = <br />

u b<br />

x , c = 0 and b = limc→0 c <br />

u c (37)<br />

d = b,<br />

our tests show the relevance of this represent<strong>at</strong>ion and its superiority over all the mo<strong>de</strong>ls consi<strong>de</strong>red here.<br />

In<strong>de</strong>ed, we have shown th<strong>at</strong> it is the best (i.e, the most parcimonious) represent<strong>at</strong>ion of the d<strong>at</strong>a for all<br />

quantiles above q9 = 80%.<br />

6 Discussion and Conclusions<br />

We have presented a st<strong>at</strong>istical analysis of the tail behavior of the distributions of the daily log-r<strong>et</strong>urns of<br />

the Dow Jones Industrial Average and of the 5-minutes log-r<strong>et</strong>urns of the Nasdaq Composite in<strong>de</strong>x. We<br />

have emphasized practical aspects of the applic<strong>at</strong>ion of st<strong>at</strong>istical m<strong>et</strong>hods to this problem. Although the<br />

applic<strong>at</strong>ion of st<strong>at</strong>istical m<strong>et</strong>hods to the study of empirical distributions of r<strong>et</strong>urns seems to be an obvious<br />

approach, it is necessary to keep in mind the existence of necessary conditions th<strong>at</strong> the empirical d<strong>at</strong>a must<br />

obey for the conclusions of the st<strong>at</strong>istical study to be valid. Maybe the most important condition in or<strong>de</strong>r to<br />

speak meaningfully about distribution functions is the st<strong>at</strong>ionarity of the d<strong>at</strong>a, a difficult issue th<strong>at</strong> we have<br />

not consi<strong>de</strong>red here. In particular, the importance of regime switching is now well established (Ramcham<br />

and Susmel 1998, Ang and Bekeart 2001) and should be accounted for.<br />

23<br />

87<br />

(35)

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