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statistique, théorie et gestion de portefeuille - Docs at ISFA

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82 3. Distributions exponentielles étirées contre distributions régulièrement variables<br />

4.3.1 Par<strong>et</strong>o distribution<br />

Figure 5a shows the cumul<strong>at</strong>ive sample distribution function 1 − F(x) for the Dow Jones Industrial Average<br />

in<strong>de</strong>x, and in figure 5b the cumul<strong>at</strong>ive sample distribution function for the Nasdaq Composite in<strong>de</strong>x. The<br />

mism<strong>at</strong>ch b<strong>et</strong>ween the Par<strong>et</strong>o distribution and the d<strong>at</strong>a can be seen with the naked eye: if samples were<br />

taken from a Par<strong>et</strong>o popul<strong>at</strong>ion, the graph in double log-scale should be a straight line. Even in the tails,<br />

this is doubtful. To formalize this impression, we calcul<strong>at</strong>e the Hill and AD estim<strong>at</strong>ors for each threshold u.<br />

Denoting y1 ... ynu the or<strong>de</strong>red sub-sample of values exceeding u where Nu is size of this sub-sample,<br />

the Hill maximum likelihood estim<strong>at</strong>e of param<strong>et</strong>er b is (Hill 1975)<br />

<br />

1<br />

ˆbu =<br />

Nu<br />

The standard <strong>de</strong>vi<strong>at</strong>ions of ˆbu can be estim<strong>at</strong>ed as<br />

Nu<br />

∑ 1<br />

log(yk/u)<br />

−1<br />

. (30)<br />

Std(ˆbu) = ˆbu/ √ Nu, (31)<br />

un<strong>de</strong>r the assumption of iid d<strong>at</strong>a, but very severely un<strong>de</strong>restim<strong>at</strong>e the true standard <strong>de</strong>vi<strong>at</strong>ion when samples<br />

exhibit <strong>de</strong>pen<strong>de</strong>nce, as reported by Kearns and Pagan (1997).<br />

Figure 6a and 6b shows the Hill estim<strong>at</strong>es ˆbu as a function of u for the Dow Jones and for the Nasdaq.<br />

Instead of an approxim<strong>at</strong>ely constant exponent (as would be the case for true Par<strong>et</strong>o samples), the tail in<strong>de</strong>x<br />

estim<strong>at</strong>or increases until u ∼ = 0.04, beyond which it seems to slow its growth and oscill<strong>at</strong>es around a value<br />

≈ 3 − 4 up to the threshold u ∼ = .08. It should be noted th<strong>at</strong> interval [0,0.04] contains 99.12% of the sample<br />

whereas interval [0.04,0.08] contains only 0.64% of the sample. The behavior of ˆbu for the ND shown<br />

in figure 6b is similar: Hill’s estim<strong>at</strong>es ˆbu seem to slow its growth already <strong>at</strong> u ∼ = 0.0013 corresponding<br />

to the 95% quantile. Are these slowdowns of the growth of ˆbu genuine sign<strong>at</strong>ures of a possible constant<br />

well-<strong>de</strong>fined asymptotic value th<strong>at</strong> would qualify a regularly varying function?<br />

As a first answer to this question, table 8 compares the AD-estim<strong>at</strong>es of the tail exponent b with the corresponding<br />

maximum likelihood estim<strong>at</strong>es for the 18 intervals u1 ...u18. Both maximum likelihood and<br />

An<strong>de</strong>rson-Darling estim<strong>at</strong>es of b steadily increase with the threshold u (excepted for the highest quantiles<br />

of the positive tail of the Nasdaq). The corresponding figures for positive and neg<strong>at</strong>ive r<strong>et</strong>urns are very<br />

close each to other and almost never significantly different <strong>at</strong> the usual 95% confi<strong>de</strong>nce level. Some slight<br />

non-monotonicity of the increase for the highest thresholds can be explained by small sample sizes. One can<br />

observe th<strong>at</strong> both MLE and ADS estim<strong>at</strong>es continue increasing as the interval of estim<strong>at</strong>ion is contracting to<br />

the extreme values. It seems th<strong>at</strong> their growth potential has not been exhausted even for the largest quantile<br />

u18, except for the positive tail of the Nasdaq sample. This st<strong>at</strong>ement might be however not very strong<br />

as the standard <strong>de</strong>vi<strong>at</strong>ions of the tail in<strong>de</strong>x estim<strong>at</strong>or also grow when exploring the largest quantiles.<br />

However, the non-exhausted growth is observed for three samples out of four. Moreover, this effect is<br />

seen for several threshold values and we can add th<strong>at</strong> random fluctu<strong>at</strong>ions would distort the b-curve<br />

in a random manner, i.e, now up now down, whearas we note in three cases an increasing curve.<br />

Assuming th<strong>at</strong> the observ<strong>at</strong>ion, th<strong>at</strong> the sample distribution can be approxim<strong>at</strong>ed by a Par<strong>et</strong>o distribution<br />

with a growing in<strong>de</strong>x b, is correct, an important question arises: how far beyond the sample this growth will<br />

continue? Judging from table 8, we can think this growth is still not exhausted. Figure 7 suggests a specific<br />

form of this growth, by plotting the hill estim<strong>at</strong>or ˆbu for all four d<strong>at</strong>a s<strong>et</strong>s (positive and neg<strong>at</strong>ive branches<br />

of the distribution of r<strong>et</strong>urns for the DJ and for the ND) as a function of the in<strong>de</strong>x n = 1,...,18 of the 18<br />

quantiles or standard significance levels q1 ...q18 given in table 6. Similar results are obtained with the AD<br />

estim<strong>at</strong>es. Apart from the positive branch of the ND d<strong>at</strong>a s<strong>et</strong>, all other three branches suggest a continuous<br />

growth of the Hill estim<strong>at</strong>or ˆbu as a function of n = 1,...,18. Since the quantiles q1 ...q18 given in table 6<br />

18

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