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statistique, théorie et gestion de portefeuille - Docs at ISFA

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In the sequel, we will first evalu<strong>at</strong>e the moments, which turns out to be easier, and then using eq (66) we<br />

will be able to calcul<strong>at</strong>e the cumulants.<br />

8.2 Symm<strong>et</strong>ric ass<strong>et</strong>s<br />

We start with the expression of the distribution of the weighted sum of N ass<strong>et</strong>s :<br />

<br />

PS(s) =<br />

R N<br />

447<br />

N<br />

dx P (x)δ( wixi − s) , (67)<br />

where δ(·) is the Dirac distribution. Using the change of variable (40), allowing us to go from the ass<strong>et</strong><br />

r<strong>et</strong>urns Xi’s to the transformed r<strong>et</strong>urns Yi’s, we g<strong>et</strong><br />

1<br />

PS(s) =<br />

(2π) N/2 <br />

d<strong>et</strong>(V )<br />

R N<br />

i=1<br />

1<br />

−<br />

dy e 2 ytV −1y δ(<br />

Taking its Fourier transform ˆ PS(k) = dsPS(s)eiks , we obtain<br />

ˆPS(k)<br />

1<br />

=<br />

(2π) N/2 <br />

d<strong>et</strong>(V )<br />

where ˆ PS is the characteristic function of PS.<br />

R N<br />

N<br />

wisgn(yi)f −1 (y 2 i ) − s) . (68)<br />

i=1<br />

1<br />

−<br />

dy e 2 ytV −1y+ikN i=1 wisgn(yi)f −1 (y2 i ) , (69)<br />

In the particular case of interest here where the marginal distributions of the variables Xi’s are the modified<br />

Weibull pdf,<br />

f −1 (yi) = χi| yi<br />

√2 | qi (70)<br />

with<br />

the equ<strong>at</strong>ion (69) becomes<br />

ˆPS(k)<br />

1<br />

=<br />

(2π) N/2 <br />

d<strong>et</strong>(V )<br />

R N<br />

qi = 2/ci , (71)<br />

1<br />

−<br />

dy e 2 ytV −1y+ikN i=1 wisgn(yi)χi| y √2 i | qi . (72)<br />

The task in front of us is to evalu<strong>at</strong>e this expression through the d<strong>et</strong>ermin<strong>at</strong>ion of the moments and/or<br />

cumulants.<br />

8.2.1 Case of in<strong>de</strong>pen<strong>de</strong>nt ass<strong>et</strong>s<br />

In this case, the cumulants can be obtained explicitely (Sorn<strong>et</strong>te <strong>et</strong> al. 2000b). In<strong>de</strong>ed, the expression (72)<br />

can be expressed as a product of integrals of the form<br />

We obtain<br />

+∞<br />

0<br />

C2n =<br />

u2<br />

− 2 du e +ikwiχiu i<br />

√2q<br />

. (73)<br />

N<br />

c(n, qi)(χiwi) 2n , (74)<br />

i=1<br />

23

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