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Processus de Lévy en Finance - Laboratoire de Probabilités et ...

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4.1. INTRODUCTION 137<br />

distribution at time t for any fixed t > 0, the <strong>de</strong>p<strong>en</strong><strong>de</strong>nce structure of a multidim<strong>en</strong>sional<br />

Lévy process X ≡ {X i t} i=1...d<br />

t≥0<br />

can be param<strong>et</strong>rized by the copula C t of the random vector<br />

{X i t} i=1...d for some t > 0. However, this approach has a number of drawbacks. First, for giv<strong>en</strong><br />

infinitely divisible one-dim<strong>en</strong>sional laws µ 1 t , . . . , µ d t , it is unclear, which copulas C t will yield a<br />

d-dim<strong>en</strong>sional infinitely divisible law. Second, the copula C t may <strong>de</strong>p<strong>en</strong>d on t and C s for some<br />

s ≠ t cannot in g<strong>en</strong>eral be computed from C t alone; to compute it one also needs to know the<br />

marginal distributions at time t and at time s. We will now construct an explicit example of a<br />

Lévy process with nonconstant copula.<br />

Example 4.1. L<strong>et</strong> Z := {Z t } t≥0 be a 2-dim<strong>en</strong>sional Cauchy process, that is, a Lévy process with<br />

characteristic tripl<strong>et</strong> (0, ν Z , 0), where ν Z has a <strong>de</strong>nsity, also <strong>de</strong>noted by ν Z , giv<strong>en</strong> by<br />

ν Z (x, y) =<br />

1<br />

(x 2 + y 2 ) 3/2 .<br />

The probability distribution of Z t for every t > 0 has a <strong>de</strong>nsity<br />

p Z t (x, y) = 1 t<br />

2π {(x 2 + y 2 ) 2 + t 2 } 3/2 .<br />

The copula of Z t does not <strong>de</strong>p<strong>en</strong>d on time and can be computed explicitly:<br />

⎧ ⎫<br />

C Z (u, v) = − 1 4 + u 2 + v 2 + 1 ⎨<br />

2π arctan tan π(u − 1 2 ) tan π(v − 1 2 ) ⎬<br />

⎩<br />

√1 + tan 2 π(u − 1 2 ) + tan2 π(v − 1 2 ) ⎭ ,<br />

which is clearly differ<strong>en</strong>t from the in<strong>de</strong>p<strong>en</strong><strong>de</strong>nce copula C ⊥ (u, v) = uv.<br />

L<strong>et</strong> W := {W t } t≥0 be a standard planar Brownian motion, in<strong>de</strong>p<strong>en</strong><strong>de</strong>nt from Z. Since the<br />

compon<strong>en</strong>ts of W are in<strong>de</strong>p<strong>en</strong><strong>de</strong>nt, the copula of W t for each t > 0 is the in<strong>de</strong>p<strong>en</strong><strong>de</strong>nce copula<br />

C ⊥ (u, v) = uv. For every t, l<strong>et</strong> X t = Z t + W t . {X t } t≥0 is a Lévy process with characteristic<br />

tripl<strong>et</strong> (Id 2 , ν Z , 0).<br />

X t √t<br />

Since Z is a 1-stable process and W is 1 2 -stable, X t<br />

t<br />

d = Z √<br />

t<br />

+ W 1 . Therefore, the random variable Xt<br />

t<br />

d<br />

= Z 1 + W 1/t and<br />

is infinitely divisible with characteristic<br />

tripl<strong>et</strong> ( 1 t Id 2, 0, ν Z ) and the random variable Xt √<br />

t<br />

is infinitely divisible with characteristic tripl<strong>et</strong><br />

(Id 2 , 0, √ tν Z ). From Proposition 1.7 it follows that Xt d<br />

t<br />

−−−→ Z 1 and Xt d<br />

√<br />

t→∞<br />

t<br />

−−→ W 1 . Since the<br />

t→0<br />

copula is invariant with respect to transformations of margins by strictly increasing functions,<br />

X t , Xt √<br />

t<br />

and Xt<br />

t<br />

have the same copula. Therefore, Theorem 2.1 in [64] implies that the copula<br />

C t of X t has the following properties<br />

∀u, v, C t (u, v) → C Z (u, v) as t → ∞,<br />

∀u, v, C t (u, v) → C ⊥ (u, v) as t → 0.

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