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

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3.2. CHOICE OF THE PRIOR 101<br />

twice to the same s<strong>et</strong> of option prices using prior mo<strong>de</strong>ls that were differ<strong>en</strong>t but close to each<br />

other (see Section 3.5.3 for the <strong>de</strong>scription of the calibration algorithm). Namely, in the test A<br />

we used Merton mo<strong>de</strong>l with diffusion volatility σ = 0.2, zero mean jump size, jump standard<br />

<strong>de</strong>viation of 0.1 and int<strong>en</strong>sity λ = 3, whereas in the test B all the param<strong>et</strong>ers except int<strong>en</strong>sity<br />

had the same values and the int<strong>en</strong>sity was equal to 2. The result of the test is shown in<br />

Figure 3.1. The solid curves correspond to calibrated measures and the dotted ones <strong>de</strong>pict<br />

the prior measures. Notice that there is very little differ<strong>en</strong>ce b<strong>et</strong>we<strong>en</strong> the calibrated measures,<br />

which means that, in harmony with Theorem 3.2, the result of calibration is robust to minor<br />

variations of the param<strong>et</strong>ers of prior measure, as long as its qualitative shape remains the same.<br />

12<br />

10<br />

Test A<br />

8<br />

6<br />

4<br />

Test B<br />

2<br />

0<br />

−1.2 −1 −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6<br />

Figure 3.1: Lévy measures calibrated to the same data s<strong>et</strong> using two prior measures similar to<br />

each other. Solid curves correspond to calibrated measures and dotted ones <strong>de</strong>pict the priors.<br />

In the second series of tests we have again calibrated the Lévy measure twice to the same<br />

s<strong>et</strong> of option prices, this time taking two radically differ<strong>en</strong>t priors. Namely, in test A we used<br />

Merton mo<strong>de</strong>l with diffusion volatility σ = 0.2, zero mean jump size, jump standard <strong>de</strong>viation<br />

of 0.1 and int<strong>en</strong>sity λ = 2, whereas in test B we took a uniform Lévy measure on the interval<br />

[−1, 0.5] with int<strong>en</strong>sity λ = 2. The calibrated measures (solid lines in Figure 3.2) are still similar<br />

but exhibit much more differ<strong>en</strong>ces than in the first series of tests. Not only they are differ<strong>en</strong>t

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