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statistique, théorie et gestion de portefeuille - Docs at ISFA

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2.2. Des bulles r<strong>at</strong>ionnelles aux krachs 53<br />

50 D. Sorn<strong>et</strong>te, Y. Malevergne / Physica A 299 (2001) 40–59<br />

distribution of each of the components of the vector X is asymptotically a power<br />

law with exponent .<br />

Eq. (22) d<strong>et</strong>ermining the tail exponent reduces to (8) in the one-dimensional case,<br />

which is simple to handle. In the multi-dimensional case, the novel fe<strong>at</strong>ure is the<br />

non-diagonal n<strong>at</strong>ure of the multiplic<strong>at</strong>ion of m<strong>at</strong>rices which does not allow in general<br />

for an explicit equ<strong>at</strong>ion similar to (8).<br />

It is important to stress th<strong>at</strong> the tails of the distribution of r<strong>et</strong>urns for all the components<br />

of the bubble <strong>de</strong>crease with the same tail in<strong>de</strong>x . This mo<strong>de</strong>l thus provi<strong>de</strong>s<br />

a n<strong>at</strong>ural s<strong>et</strong>ting for r<strong>at</strong>ionalizing the well-documented empirical observ<strong>at</strong>ion th<strong>at</strong> the<br />

exponent is found to be approxim<strong>at</strong>ely the same for most ass<strong>et</strong>s. The constraint on<br />

its value discussed in the next paragraph does not diminish the value of this remark,<br />

as explained in Section 5.<br />

3.5. Constraint on the tail in<strong>de</strong>x<br />

The rst conclusion of the theorem above shows th<strong>at</strong> the tail in<strong>de</strong>x of the process<br />

(Xt) is driven by the behavior of the m<strong>at</strong>rices (At). We will then st<strong>at</strong>e a proposition<br />

in which we give a major<strong>at</strong>ion of the tail in<strong>de</strong>x.<br />

Proposition 2. A necessary condition to have ¿1 is th<strong>at</strong> the spectral radius (largest<br />

eigenvalue) of EP[A] be smaller than 1:<br />

¿1 ⇒ (EP[A]) ¡ 1 : (23)<br />

The proof is given in Ref. [32]. This proposition, put tog<strong>et</strong>her with Proposition 1 above,<br />

allows us to <strong>de</strong>rive our main result. We have seen in Section 3.3 from Proposition 1<br />

th<strong>at</strong>, as a result of the no-arbitrage condition, the spectral radius of the m<strong>at</strong>rix EP[A]<br />

is gre<strong>at</strong>er than 1. As a consequence, by applic<strong>at</strong>ion of the converse of Proposition 2,<br />

we nd th<strong>at</strong> the tail in<strong>de</strong>x of the distribution of (X) is smaller than 1. This result<br />

does not rely on the diagonal property of the m<strong>at</strong>rices EP[At] but only on the value<br />

of the spectral radius imposed by the no-arbitrage condition.<br />

This result generalizes to arbitrary d-dimensional processes the result of Ref. [15]. As<br />

a consequence, d-dimensional r<strong>at</strong>ional expect<strong>at</strong>ion bubbles linking several ass<strong>et</strong>s su er<br />

from the same discrepancy compared to empirical d<strong>at</strong>a as the one-dimensional bubbles.<br />

It would therefore appear th<strong>at</strong> exogenous r<strong>at</strong>ional bubbles are hardly reconcilable with<br />

some of the most fundamental stylized facts of nancial d<strong>at</strong>a <strong>at</strong> a very elementary level.<br />

At this stage, we have to ask the question: wh<strong>at</strong> is wrong with the mo<strong>de</strong>l of r<strong>at</strong>ional<br />

bubbles? Two altern<strong>at</strong>ive answers are explored below: either we believe in the standard<br />

valu<strong>at</strong>ion formula and we are led to extend the restricted framework <strong>de</strong>scribed by the<br />

Blanchard and W<strong>at</strong>son’s mo<strong>de</strong>l; or we believe in the existence of the bubbles within<br />

their framework and we have to generalize the valu<strong>at</strong>ion formula. In the next two<br />

sections, we will discuss these two points of view.

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