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statistique, théorie et gestion de portefeuille - Docs at ISFA

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9.2. Estim<strong>at</strong>ion du coefficient <strong>de</strong> dépendance <strong>de</strong> queue 313<br />

same tail in<strong>de</strong>x. We can also add th<strong>at</strong>, as asserted by Lor<strong>et</strong>an and Phillips (1994) or Longin (1996),<br />

we cannot reject the hypothesis th<strong>at</strong> the tail in<strong>de</strong>x remains the same over time. Nevertheless, it<br />

seems th<strong>at</strong> during the first period from July 1962 to December 1979, the tail in<strong>de</strong>xes were sightly<br />

larger than during the second period from January 1980 to <strong>de</strong>cember 2000.<br />

3.4 D<strong>et</strong>ermin<strong>at</strong>ion of the coefficient of tail <strong>de</strong>pen<strong>de</strong>nce<br />

Using the just established empirical fact th<strong>at</strong> we cannot reject the hypothesis th<strong>at</strong> the ass<strong>et</strong>s, the<br />

mark<strong>et</strong> and the residues have the same tail in<strong>de</strong>x, we can use the theorem of Appendix A and<br />

its second corollary st<strong>at</strong>ed in section 2. This allows us to conclu<strong>de</strong> th<strong>at</strong> one cannot reject the<br />

hypothesis of a non-vanishing tail <strong>de</strong>pen<strong>de</strong>nce b<strong>et</strong>ween the ass<strong>et</strong>s and the mark<strong>et</strong>.<br />

In addition, the coefficient of tail <strong>de</strong>pen<strong>de</strong>nce is given by equ<strong>at</strong>ions (12) and (13). These equ<strong>at</strong>ions<br />

provi<strong>de</strong> two ways for estim<strong>at</strong>ing the coefficient of tail <strong>de</strong>pen<strong>de</strong>nce: non-param<strong>et</strong>ric with (12) and<br />

param<strong>et</strong>ric with (13). The first one is more general since it only requires the hypothesis of a regular<br />

vari<strong>at</strong>ion, while the second one explicitly assumes th<strong>at</strong> the factor and the residues have distributions<br />

with power law tails.<br />

To estim<strong>at</strong>e the tail <strong>de</strong>pen<strong>de</strong>nce according equ<strong>at</strong>ion (12), we need only to d<strong>et</strong>ermine the constant l<br />

<strong>de</strong>fined (8). Consi<strong>de</strong>r N sorted realiz<strong>at</strong>ions of X and Y <strong>de</strong>noted by x1,N ≥ x2,N ≥ · · · ≥ xN,N and<br />

y1,N ≥ y2,N ≥ · · · ≥ yN,N, the quantile of F −1<br />

−1<br />

X (u) and of FY (u) are estim<strong>at</strong>ed by<br />

−1 −1<br />

FX<br />

ˆ (u) = x[(1−u)·N],N and FY<br />

ˆ (u) = y[(1−u)·N],N, (22)<br />

where [·] <strong>de</strong>notes the integer part. Thus, the constant l is non-param<strong>et</strong>rically estim<strong>at</strong>ed by<br />

ˆ lk = xk,N<br />

yk,N<br />

as k → 0 or N. (23)<br />

As u goes to zero or one (or k goes to zero or N), the number of observ<strong>at</strong>ions <strong>de</strong>creases dram<strong>at</strong>ically.<br />

However, we observe a large interval of small or large k’s such th<strong>at</strong> the r<strong>at</strong>io of the empirical<br />

quantiles remains remarkably stable and thus allows for an accur<strong>at</strong>e estim<strong>at</strong>ion of l. A more<br />

precise estim<strong>at</strong>ion could be performed with a kernel-based quantile estim<strong>at</strong>or (see Shealter and<br />

Marron (1990) or Pagan and Ullah (1999) for instance). A non-param<strong>et</strong>ric estim<strong>at</strong>or for λ is then<br />

obtained by replacing l by its estim<strong>at</strong>ed value in equ<strong>at</strong>ion (12)<br />

ˆλNP =<br />

1<br />

<br />

max 1, ˆ 1<br />

α = <br />

l<br />

ˆβ max 1, xk,N<br />

α . (24)<br />

ˆβ·yk,N<br />

It can also be advantageous to follow a param<strong>et</strong>ric approach, which generally allows for a more<br />

accur<strong>at</strong>e estim<strong>at</strong>ion of (the r<strong>at</strong>io of) the quantiles, provi<strong>de</strong>d th<strong>at</strong> the assumed param<strong>et</strong>ric form of<br />

the distributions is not too far from the true one. For this purpose, we will use formula (13) which<br />

requires the estim<strong>at</strong>ion of the scale factors for the different ass<strong>et</strong>s. To g<strong>et</strong> the scale factors, we<br />

proceed as follows. Consi<strong>de</strong>r a variable X which asymptotically follows a power law distribution<br />

Pr{X > x} ∼ C · x −α . Given a rank or<strong>de</strong>red sample x1,N ≥ x2,N ≥ · · · ≥ xN,N, the scale factor C<br />

can be consistently estim<strong>at</strong>ed from the k largest realiz<strong>at</strong>ions by<br />

Ĉ = k<br />

N · (xk,N) α . (25)<br />

The estim<strong>at</strong>ed value of the scale factor must not <strong>de</strong>pends on the rank k for k large enough, in or<strong>de</strong>r<br />

for the param<strong>et</strong>eriz<strong>at</strong>ion of the distribution in terms of a power law to hold true. Thus, <strong>de</strong>noting<br />

14

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