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9.1. Les différentes mesures <strong>de</strong> dépendances extrêmes 253<br />

3.1 Definition<br />

The concept of tail <strong>de</strong>pen<strong>de</strong>nce is appealing by its simplicity. By <strong>de</strong>finition, the (upper) tail <strong>de</strong>pen<strong>de</strong>nce<br />

coefficient is:<br />

−1<br />

λ = lim<br />

(u)|Y > F (u)] , (19)<br />

Pr[X > F<br />

u→1 −1<br />

X<br />

and quantifies the probability to observe a large X, assuming th<strong>at</strong> Y is large itself. For a survey of the<br />

properties of the tail <strong>de</strong>pen<strong>de</strong>nce coefficient, the rea<strong>de</strong>r is refered to (Coles <strong>et</strong> al. 1999, Embrechts <strong>et</strong> al.<br />

2001, Lindskog 1999), for instance. In words, given th<strong>at</strong> Y is very large (which occurs with probability<br />

1 − u), the probability th<strong>at</strong> X is very large <strong>at</strong> the same probability level u <strong>de</strong>fines asymptotically the tail<br />

<strong>de</strong>pen<strong>de</strong>nce coefficient λ. As an example, consi<strong>de</strong>ring th<strong>at</strong> X and Y represent the vol<strong>at</strong>ility of two different<br />

n<strong>at</strong>ional mark<strong>et</strong>s, the coefficient of tail <strong>de</strong>pen<strong>de</strong>nce λ gives the probabilty th<strong>at</strong> both mark<strong>et</strong>s exhibit tog<strong>et</strong>her<br />

very high vol<strong>at</strong>ility.<br />

One of the appeal of this <strong>de</strong>finition of tail <strong>de</strong>pen<strong>de</strong>nce is th<strong>at</strong> it is a pure copula property, i.e., it is in<strong>de</strong>pen<strong>de</strong>nt<br />

of the margins of X and Y . In<strong>de</strong>ed, l<strong>et</strong> C be the copula of the variables X and Y , then if the bivari<strong>at</strong>e copula<br />

C is such th<strong>at</strong><br />

Y<br />

1 − 2u + C(u, u)<br />

log C(u, u)<br />

lim<br />

= lim 2 − = λ (20)<br />

u→1 1 − u<br />

u→1 log u<br />

exists, then C has an upper tail <strong>de</strong>pen<strong>de</strong>nce coefficient λ (see (Coles <strong>et</strong> al. 1999, Embrechts <strong>et</strong> al. 2001,<br />

Lindskog 1999)).<br />

If λ > 0, the copula presents tail <strong>de</strong>pen<strong>de</strong>nce and large events tend to occur simultaneously, with the<br />

probability λ. On the contrary, when λ = 0, the copula has no tail <strong>de</strong>pen<strong>de</strong>nce and the variables X and Y<br />

are said asymptotically in<strong>de</strong>pen<strong>de</strong>nt. There is however a subtl<strong>et</strong>y in this <strong>de</strong>finition (19) of tail <strong>de</strong>pen<strong>de</strong>nce.<br />

To make it clear, first consi<strong>de</strong>r the case where for large X and Y the cumul<strong>at</strong>ive distribution function H(x, y)<br />

factorizes such th<strong>at</strong><br />

F (x, y)<br />

lim<br />

= 1 , (21)<br />

x,y→∞ FX(x)FY (y)<br />

where FX(x) and FY (y) are the margins of X and Y respectively. This means th<strong>at</strong>, for X and Y sufficiently<br />

large, these two variables can be consi<strong>de</strong>red as in<strong>de</strong>pen<strong>de</strong>nt. It is then easy to show th<strong>at</strong><br />

lim<br />

u→1 Pr{X > FX −1 (u)|Y > FY −1 (u)} = lim 1 − FX(FX<br />

u→1 −1 (u)) (22)<br />

= lim<br />

u→1 1 − u = 0, (23)<br />

so th<strong>at</strong> in<strong>de</strong>pen<strong>de</strong>nt variables really have no tail <strong>de</strong>pen<strong>de</strong>nce λ = 0, as one can expect.<br />

However, the result λ = 0 does not imply th<strong>at</strong> the multivari<strong>at</strong>e distribution can be autom<strong>at</strong>ically factorized<br />

asymptotically, as shown by the Gaussian example. In<strong>de</strong>ed, the Gaussian multivari<strong>at</strong>e distribution does not<br />

have a factorizable multivari<strong>at</strong>e distribution, even asymptotically for extreme values, since the non-diagonal<br />

term of the quadr<strong>at</strong>ic form in the exponential function does not become negligible in general as X and Y go<br />

to infinity. Therefore, in a weaker sense, there may still be a <strong>de</strong>pen<strong>de</strong>nce in the tail even when λ = 0.<br />

To make this st<strong>at</strong>ement more precise, following (Coles <strong>et</strong> al. 1999), l<strong>et</strong> us introduce the coefficient<br />

¯λ = lim<br />

u→1<br />

2 log Pr{X > FX −1 (u)}<br />

log Pr{X > FX −1 (u), Y > FY −1 (u)}<br />

− 1 (24)<br />

2 log(1 − u)<br />

= lim<br />

− 1 . (25)<br />

u→1 log[1 − 2u + C(u, u)]<br />

It can be shown th<strong>at</strong> the coefficient ¯ λ = 1 if and only if the coefficient of tail <strong>de</strong>pen<strong>de</strong>nce λ > 0, while ¯ λ<br />

takes values in [−1, 1) when λ = 0, allowing us to quantify the strength of the <strong>de</strong>pen<strong>de</strong>nce in the tail in such<br />

15

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