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Specification:

In order to construct the measure we define the set of consecutive loss exceedence events $\Psi^{\pm_{(k,P)}}(c)$ so that:  
 \begin{displaymath}
\Psi^{\pm_{(k,P)}}(c) =
\{t\vert\{t,t-1\}\subset\Phi^{\pm_{(k,P)}}(c),t\in[3,1001]\}.\end{displaymath} (32)
Using sets $\Psi^{\pm_{(k,P)}}(c)$ we can finally specify the serial exceedence ratio measure
\begin{displaymath}
s^{\pm_{(k,P)}}(c) = {{\char93 }(\Psi^{\pm_{(k,P)}}(c))\over1000(1-{c\over100})^2}\end{displaymath} (33)

Finally, as specified by expressions [*] and [*], we construct the univariate average exceedence ratio
\begin{displaymath}
s_u(c) = {1\over20}\left(\sum_{k=1}^{10}s^{+_{(k)}}(c) +
\sum_{k=1}^{10}s^{-_{(k)}}(c)\right)\end{displaymath} (34)
and the multivariate average exceedence ratio
\begin{displaymath}
s_m(c) = {1\over2}\left(s^{+_{(P)}}(c) + s^{-_{(P)}}(c)\right)\end{displaymath} (35)
plotted in figures 3u and 3m respectively for all candidate models.