statistique, théorie et gestion de portefeuille - Docs at ISFA
statistique, théorie et gestion de portefeuille - Docs at ISFA
statistique, théorie et gestion de portefeuille - Docs at ISFA
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248 9. Mesure <strong>de</strong> la dépendance extrême entre <strong>de</strong>ux actifs financiers<br />
the Brazilian case, the estim<strong>at</strong>es of the correl<strong>at</strong>ion coefficient will be particularly noisy and thus of weak<br />
st<strong>at</strong>istical value.<br />
We have checked th<strong>at</strong> the f<strong>at</strong> tailness of the in<strong>de</strong>xes expressed in US dollar comes from the impact of the<br />
exchange r<strong>at</strong>es. Thus, an altern<strong>at</strong>ive should be to consi<strong>de</strong>r the in<strong>de</strong>xes in local currency, following (Longin<br />
and Solnik 1995) and (Longin and Solnik 2001)’s m<strong>et</strong>hodology, but it would lead to focus on the linkages<br />
b<strong>et</strong>ween mark<strong>et</strong>s only and to neglect the impact of the <strong>de</strong>valu<strong>at</strong>ions, which is precisely the main concern of<br />
many studies about the contagion in L<strong>at</strong>in America.<br />
Figures 2, 4 and 6 give the conditional correl<strong>at</strong>ion coefficient ρ +,−<br />
v<br />
(plain thick line) for the pairs Ar-<br />
gentina / Brazil, Brazil / Chile and Chile / Mexico while figures 3, 5 and 7 show the conditional correl<strong>at</strong>ion<br />
coefficient ρ s v for the same pairs. For each figure, the dashed thick line gives the theor<strong>et</strong>ical curve obtained<br />
un<strong>de</strong>r the bivari<strong>at</strong>e Gaussian assumption whose analytical expressions can be found in appendices A.1.1<br />
and A.1.2. The unconditional correl<strong>at</strong>ion coefficient of the Gaussian mo<strong>de</strong>l is s<strong>et</strong> to the empirically estim<strong>at</strong>ed<br />
unconditional correl<strong>at</strong>ion coefficent. The two dashed thin lines represent the interval within which<br />
we cannot reject, <strong>at</strong> the 95% confi<strong>de</strong>nce level, the hypothesis according to which the estim<strong>at</strong>ed conditional<br />
correl<strong>at</strong>ion coefficient is equal to the theor<strong>et</strong>ical one. This confi<strong>de</strong>nce interval has been estim<strong>at</strong>ed using the<br />
Fisher’s st<strong>at</strong>istics. Similarly, the thick dotted curve graphs the theor<strong>et</strong>ical curve obtained un<strong>de</strong>r the bivari<strong>at</strong>e<br />
Stu<strong>de</strong>nt’s assumption with ν = 3 <strong>de</strong>grees of freedom (whose expressions are given in appendices B.3<br />
and B.4) and the two thin dotted lines are its 95% confi<strong>de</strong>nce level. Here, the Fisher’s st<strong>at</strong>istics cannot be<br />
applied, since it requires <strong>at</strong> least th<strong>at</strong> the fourth moment of the distribution exists. In fact, (Meerschaert and<br />
Scheffler 2001) have shown th<strong>at</strong>, in such a case, the distribution of the sample correl<strong>at</strong>ion converges to a<br />
stable law with in<strong>de</strong>x 3/2, which justifies why the confi<strong>de</strong>nce interval for the Stu<strong>de</strong>nt’s mo<strong>de</strong>l with three<br />
<strong>de</strong>gres of freedom is much larger than the confi<strong>de</strong>nce interval for the Gaussian mo<strong>de</strong>l. In the present study,<br />
we have used a bootstrap m<strong>et</strong>hod to <strong>de</strong>rive this confi<strong>de</strong>nce interval since the scale factor intervening in the<br />
stable law is difficult to calcul<strong>at</strong>e.<br />
In figures 2, 4 and 6, we observe th<strong>at</strong> the change in the conditional correl<strong>at</strong>ion coefficients ρ +,−<br />
v<br />
are not sig-<br />
nificantly different, <strong>at</strong> the 95% confi<strong>de</strong>nce level, from those obtained with a bivari<strong>at</strong>e Stu<strong>de</strong>nt’s mo<strong>de</strong>l with<br />
three <strong>de</strong>grees of freedom. In contrast, the Gaussian mo<strong>de</strong>l is often rejected. In fact, similar results hold (but<br />
are not <strong>de</strong>picted here) for the three others pairs Argentina / Chile, Argentina / Mexico and Brazil / Mexico.<br />
Thus, these observ<strong>at</strong>ions should lead us to conclu<strong>de</strong> th<strong>at</strong>, in these cases, no change in the correl<strong>at</strong>ions, and<br />
therefore no contagion mechanism, needs to be invoked to explain the d<strong>at</strong>a, since they are comp<strong>at</strong>ible with<br />
a Stu<strong>de</strong>nt’s mo<strong>de</strong>l with constant correl<strong>at</strong>ion.<br />
L<strong>et</strong> us now discuss the results obtained for the correl<strong>at</strong>ion coefficient conditioned on the vol<strong>at</strong>ility. Figures<br />
3 and 7 show th<strong>at</strong> the estim<strong>at</strong>ed correl<strong>at</strong>ion coefficients conditioned on vol<strong>at</strong>ility remain consistent with the<br />
Stu<strong>de</strong>nt’s mo<strong>de</strong>l with three <strong>de</strong>gres of freedom, while they still reject the Gaussian mo<strong>de</strong>l. In contrast, figure<br />
5 shows th<strong>at</strong> the increase of the correl<strong>at</strong>ion cannot be explained by any of the Gaussian or Stu<strong>de</strong>nt mo<strong>de</strong>ls,<br />
when conditioning on the Mexican in<strong>de</strong>x vol<strong>at</strong>ilty. In<strong>de</strong>ed, when the Mexican in<strong>de</strong>x vol<strong>at</strong>ility becomes larger<br />
than 2.5 times its standard <strong>de</strong>vi<strong>at</strong>ion, none of our mo<strong>de</strong>ls can account for the increase of the correl<strong>at</strong>ion. The<br />
same discrepancy is observed for the pairs Argentina / Chile, Argentina / Mexico and Brazil / Mexico which<br />
have not been represented here. In each case, the Chilean or the Mexican mark<strong>et</strong> have an impact on the<br />
Argentina or the Brazilian mark<strong>et</strong> which cannot be accounted for by neither the Gaussian or Stu<strong>de</strong>nt mo<strong>de</strong>ls<br />
with constant correl<strong>at</strong>ion.<br />
To conclu<strong>de</strong> this empirical part, there is no significant increase in the real correl<strong>at</strong>ion b<strong>et</strong>ween Argentina<br />
and Brazil in the one hand and b<strong>et</strong>ween Chile and Mexico in the other hand, when the vol<strong>at</strong>ility or the<br />
r<strong>et</strong>urns exhibit large moves. But, in period of high vol<strong>at</strong>ility, the Chilean and Mexican mark<strong>et</strong> may have an<br />
genuine impact on the Argentina and Brazilian mark<strong>et</strong>s. Thus, a priori, this should lead us to conclu<strong>de</strong> on<br />
the existence of a contagion across these mark<strong>et</strong>s. However, this conclusion is based on the investig<strong>at</strong>ion of<br />
10