%Paper: 
%From: NARISON@crnvma.cern.ch
%Date: Fri, 26 Aug 94 10:33:33 SET
%Date (revised): Fri, 26 Aug 94 11:26:52 SET


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\begin{document}
\pagestyle{empty}
\begin{flushright}
{CERN-TH.7405/94}\\
%PM 94/xx
\end{flushright}
 \vspace*{5mm}
\begin{center}
\section*{\bf
A fresh look into the heavy quark-mass values }
%from QCD spectral sum rules}
%\vspace*{0.5cm}
{\bf S. Narison} \\
 \vspace{0.3cm}
Theoretical Physics Division, CERN\\
CH - 1211 Geneva 23, Switzerland\\
and\\
Laboratoire de Physique Math\'ematique\\
Universit\'e de Montpellier II\\
Place Eug\`ene Bataillon\\
34095 - Montpellier Cedex 05, France\\
\vspace*{1cm}
{\bf Abstract} \\ \end{center}
\vspace*{2mm}
\noindent
Using the recent {\it world average}
 $\alpha_s(M^2_Z)= 0.118 \pm 0.006$, we give the
 {\it first direct extraction}
from the $\Psi $ and $ \Upsilon$
data of the values of the
{\it running heavy quark masses} within QCD spectral
sum rules to two-loops in the $\overline {MS}$-scheme:
$\mr_b(M^{PT2}_b)$ = $(4.23~^{+0.03}_{-0.04} \pm 0.02)$ GeV
and $\mr_c(M^{PT2}_c)$ = $(1.23~^{+ 0.02}_{-0.04} \pm 0.03)$ GeV,
(the errors are respectively due to $\alf$ and to the
gluon condensate), and the corresponding value of
the {\it short-distance perturbative pole masses to two-loops}:
$M^{PT2}_b=(4.62 \pm 0.02)$ GeV,	 $M^{PT2}_c=(1.41\pm 0.03)$ GeV,
which we compare with the
 updated values of the {\it non-relativistic
pole masses} re-extracted {\it directly}
from the two-loop non-relativistic sum rules:
$M^{NR}_b= (4.69~^{-0.01}_{+0.02}\pm 0.02)$ GeV and
$M^{NR}_c=(1.44\pm 0.02\pm 0.03)$ GeV. It is also informative
to compare the {\it three-loop} values of the
short-distance pole masses:
$M^{PT3}_b=(4.87\pm 0.05
 \pm 0.02)$ GeV and $M^{PT3}_c=(1.62\pm 0.07 \pm 0.03)$ GeV, with the
{\it dressed mass} $M^{nr}_b =(4.94 \pm 0.10 \pm 0.03)$ GeV,
entering into
the {\it non-relativistic Balmer formula} including higher order $\alf$
corrections. The $small$ mass-differences $M^{NR}_b-M^{PT2}_b
\simeq M^{nr}_b-M^{PT3}_b \simeq 70$ MeV and $M_c^{NR}-M_c^{PT2} \simeq
(30 \pm 20)$ MeV {\it can measure the size}
of the non-perturbative effect induced by {\it renormalon}
type-singularities. An analogous analysis
is pursued for the heavy-light mesons,  where
a simultaneous {\it re-fit} of the $B$ and
$B^*$ masses from relativistic sum rules
leads to:
$M_b^{PT2}= (4.63 \pm 0.08)$ GeV, while the full-QCD
and HQET sum rules in the large mass limit give the {\it meson-quark mass
difference to two-loops}: $(M_B-M^{NR}_b)_{\infty}
 \simeq (0.6 ^{+0.20}_{-0.10})$ GeV. A
comparison of
these $new$ and $accurate$
results with the existing ones in the literature is
done. As a consequence, the {\it updated} values of
the {\it pseudoscalar decay constants to two-loops} are:
$f_D = (1.37\pm 0.04\pm 0.06)f_\pi$ and $f_B=(1.49\pm 0.06\pm 0.05)f_\pi,
$ which lead to $f_B\sqrt{B_B}=(1.49\pm 0.14)f_\pi$.

\vspace*{0.5cm}
\noindent

\begin{flushleft}
CERN-TH.7405/94 \\
August 1994\\
%\today
\end{flushleft}
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\section{Introduction} \par
Present accurate measurements of the QCD coupling $\alpha_s$,
mainly from Z-physics and tau-decay data, motivate
a careful reconsideration of the existing estimates of the standard
model parameters. Among others, of a $prime~importance$ is the one of
the quark masses. However, unlike the electron mass, the definition
of the quark masses needs a theoretical framework due to the complication
implied by confinement. In particular, the notion of the pole mass
from perturbation theory, though gauge independent,
appears to be ambiguous, as the summation of large order perturbation
theory induces a non-perturbative term due to renormalon-type
singularities. However, one can still provide a $good~ definition$ of
this pole mass for a truncated QCD series, which can be used
$consistently$ in a given observable known at the same order of
perturbation theory. Unlike the $pole$ mass,
the $running$ mass of the $\overline{MS}$-scheme does not suffer from
this ambiguity, such that its $direct~ estimate$ from the data without
passing through the pole mass should be very useful.

\nin
In this paper, we shall use
 QCD spectral sum rules (QSSR) in order {\it
 to extract, directly} from the data,
and {\it for the first time},
the value of the $running$ heavy quark mass $\overline{m}_Q$\footnote[1]
{However,
an extraction of the running mass using local duality FESR has been
done in \cite{RAF}.}, which is a useful (and well-defined) quantity for
GUTS and some other phenomenology.
 Indeed, many papers have been devoted in the past,
either to the $direct$
estimate of the $Euclidian$ mass $m_Q(p^2=-m^2_Q)$
or/and  of the $pole$ mass $M_Q(p^2=M^2_Q)$
\cite{SVZ}-\cite{SNB}
while the running mass has been
mainly deduced \cite{LEUT,SN1} from its perturbative relation with the pole
mass \cite{BINET}\footnote[2]{For consistency with the two-loop
expression of the two-point correlator, we shall not use the
three-loop
relation in the sum rule analysis.}:
\beq
M_Q(M_Q^2)
=\overline{m}_Q(M_Q^2)\aga 1+\frac{4}{3}\ga\frac{\alpha_s(M_Q^2)}{\pi}\dr
 +K_Q\ga\frac{\alpha_s(M_Q^2)}{\pi}\dr^2 \adr ,
\eeq
where $K_b \simeq 12.4,~K_c \simeq 13.3$ \cite{SCHILCHER}.
Instead, once, we obtain the running mass from the data, we shall use the
previous relation in order to deduce the short-distance
$perturbative$ pole mass $M^{PT}_Q$,
which we shall compare with the
$non$-$relativistic$ pole mass $M^{NR}_Q$ extracted
directly from the data, using non-relativistic sum rules, and with
the mass $M^{nr}_Q$ entering into the non-relativistic
Balmer formula. We shall interpret
the difference between these two values as a measure of the size of the
renormalon effect into the pole mass definition.

\nin
Finally, in comparing our results for the pole masses with the existing ones
in the literature, we shall test the reliability of these previous results
and look for the possible sources of some eventual differences between these
and
the ones in this paper.

\section{Input values of $\alf$ and matching conditions}
We use the value of $\alf(M_Z)$ in the range given in Table 1, where
the new world average is $0.118\pm 0.006$ \cite{BETHKE}, but we have
also considered a slightly higher value of 0.127 in order to be more
conservative. Then, we run  this value until $M_b=4.6-4.7$ GeV, using
the two-loop relation:
\beq
\frac{\alf}{\pi}= a_s \ga
1-a_s\frac{\beta_2}{\beta_1}\log\log(p^2/\al^2) \dr
\eeq
where:
\beq
 a_s= \frac{2}{-\beta_1\log(p^2/\al^2)}
\eeq
and for $n_f$ flavours:
\beq
\beta_1= -\frac{11}{2}+\frac{n_f}{3}~~~~~~\mbox{and}
{}~~~~~~  \beta_2=-\frac{51}{4}+\frac{19}{12}n_f .
\eeq
Following, Ref.\cite{BERN},
we do the matching condition $\alf^{(5)}=\alf^{(4)}$ at this $b$-mass,
in order to extract $\al$ for 4 flavours. We
continue iteratively this procedure for completing Table 1, which is
one of the basic inputs of our analysis. Notice that doing a similar
procedure at the tree-loop level, we reproduce the value of $\al$ given
in \cite{BETHKE}.
\begin{table}[h]
\begin{center}
\begin{tabular}[h]{||lllllll||}
\hline \hline
 & & & & & & \\
$\alf(M_Z)$&$\Lambda_5$[MeV]&$\alf(M_b)$&
$\Lambda_4$[MeV]&$\alf(M_c)$&$\Lambda_3$[MeV]&$\alf(M_\tau)$\\
 & & & & & & \\
\hline \hline
0.112&160 &0.198&233& 0.299&268& 0.269 \\
0.118&225 &0.217&317& 0.350&345& 0.308 \\
0.124&310 &0.240&420& 0.420&433& 0.356 \\
0.127&360 &0.252&475& 0.493&525& 0.407 \\
\hline \hline
\end{tabular}
\caption{\it Value of $\alf$ and $\Lambda$ to two-loops at different scales and
\end{center}
\end{table}
 \section{ Running masses from the $\Psi$- and
 $\Upsilon$-systems}

In so doing, let us consider
the two-point vector correlator:
\bea
\Pi^{\mu\nu}_b(q^2,M^2_Q) &\equiv& i \int d^4x ~e^{iqx} \
\la 0\vert {\cal T}
J^{\mu}_Q(x)
\ga J^{\nu}_Q(o)\dr ^\dagger \vert 0 \ra \\ \nnb
&=& -\ga g^{\mu\nu}q^2-q^\mu q^\nu \dr \Pi_Q(q^2,M^2_Q),
\eea
where $J^{\mu}_Q(x) \equiv \bar Q \gamma^\mu Q (x)$ is the local vector
current of the heavy quark $Q$. The correlator obeys the well-known
K\"all\`en-Lehmann dispersion relation:
\beq
\Pi_Q(q^2,M^2_Q) = \int_{4M^2_Q}^{\infty} \frac{dt}{t-q^2-i\epsilon}
{}~\frac{1}{\pi}~\mbox{Im}  \Pi_Q(t) \ \ \ + \ \ \ \mbox{subtractions},
\eeq
which expresses in a clear way the {\it duality} between the spectral
function Im$ \ \Pi_Q(t)$, which can be measured experimentally, as here
it is related to the $e^+e^-$ into $\Psi$ or $\Upsilon$-like states total
cross-section or their leptonic widths as:
\beq
\mbox{Im}  \Pi_Q(t) =\frac{3}{4\alpha^2}\frac{1}{Q^2_Q}
\sum_{i}
{\Gamma_i M_i} \delta (t-M^2_i)~~+~~
\Theta (t-t_c) \mbox{Im} \Pi^{QCD}_Q(t).
\eeq
$Q_Q$ is the heavy quark charge in units of e;
$\Gamma_i$ is the electronic width of the resonances with the value
given in PDG 92 \cite{PDG}; $t_c$ is the QCD continuum threshold
which we fix just above the last known radial excitation which is
respectively about (5 GeV$)^2$ and (12 GeV$)^2$ for the $\Psi$ and
$\Upsilon$ families (however, it should be noticed that your result
is not dependent on this choice due to the
almost complete dominance of the lowest ground state at the stability
point).
$\Pi_Q(q^2,M^2_Q)$ can be calculated directly in
QCD, even at $q^2=0$,
provided that $M^2_Q-q^2 \gg \Lambda^2$. For the perturbative part,
we shall use (without expanding in 1/M)
the Schwinger extrapolation formula to two-loops:
\beq
\mbox{Im} \Pi^{pert}_Q(t)
\simeq \frac{3}{12\pi}v_Q\ga \frac{3-v^2_Q}{2} \dr
\aga 1+\frac{4}{3}\alf f(v_Q) \adr ,
\eeq
where:
\beq
v_Q= \sqrt{1-4M^2_Q/t}
\eeq
and:
\beq
f(v_Q)=\frac{\pi}{2v_Q}-\frac{(3+v_Q)}{4}\ga \frac{\pi}{2}-\frac{3}{4\pi}
\dr
\eeq
is the Schwinger function \cite{SCHWI}. We express this
spectral function in terms of the running mass by using Eq. (1)
to two-loops and the
$\alf\log(t/M^2_Q)$-term appearing in Eq. (1) for off-shell quark.
We shall add to this perturbative
expression the lowest dimension $\la \alf G^2 \ra $
non-perturbative effect (it is known \cite{HEAVY} that, for a heavy-heavy quark
correlator, the quark condensate contribution
is already absorbed into the gluon
one)
which among the available higher dimension
condensate-terms can only give a non-negligible contribution. We shall
use the range of values:
\beq
\la \alf G^2 \ra = (0.06 \pm 0.03)~ \mbox{GeV}^4,
\eeq
from different QSSR analysis \cite{SNB}; a value confirmed by the recent
ALEPH measurement of this quantity from tau-decay data \cite{ALEPH},
which, at the same time,
exclude higher values of this condensate advocated sometimes
in the literature.

\nin
QSSR is an improvement of the previous
dispersion relation. For our purpose, we shall consider the ratios:
\beq
{\cal R}_n \equiv \frac{{\cal M}^{(n)}}{{\cal M}^{(n+1)}}~~~~~~~
\mbox{and}~~~~~~~
{\cal R}_\tau \equiv -\frac{d}{d\tau} \log {{\cal L}},
\eeq
and their finite energy sum rule (FESR) variants, which come from
the moment sum rules
(finite number of derivatives and finite values of $q^2$):
\beq
{\cal M}^{(n)} \equiv \frac{1}{n!}\frac{\partial^n \Pi_Q(q^2)}
{\ga \partial q^2\dr^n} \Bigg{\vert} _{q^2=0}
= \int_{4M^2_Q}^{\infty} \frac{dt}{t^{n+1}}
{}~\frac{1}{\pi}~ \mbox{Im}  \Pi_Q(t),
\eeq
or infinite number of derivatives and infinite values of $q^2$, but
keeping their ratio fixed as $\tau \equiv n/q^2$
(Laplace or Borel or exponential sum rules):
\beq
{\cal L}(\tau,M^2_b)
= \int_{4M^2_Q}^{\infty} {dt}~\mbox{exp}(-t\tau)
{}~\frac{1}{\pi}~\mbox{Im} \Pi_Q(t).
\eeq
The ratios of sum rules are
more appropriate for the estimate of the
quark mass as these ratios equate $directly$ the mass squared of
ground state to that of the quark. They also eliminate, to leading order,
some artefact dependence due to the sum rules (exponential weight factor
or number of derivatives).

\nin
In principle, the pairs $(n,t_c)$, $(\tau,t_c)$ are free external
parameters in the analysis, so that the optimal result should be
insensitive to their variations. Stability criteria, which are equivalent
to the variational method, state that the optimal results should
be obtained at the minimas or at the inflexion points in $n$ or $\tau$,
while stability in $t_c$ is useful to control the sensitivity of the
result in the changes of $t_c$-values (in the present case of the
$\Psi$ and $\Upsilon$ systems, $t_c$-stability is manifest due to the
negligible effect of the QCD continuum).
%To these stability criteria are
%added constraints from local duality FESR, which
%correlate the $t_c$-value to those of the ground state mass and
%coupling \cite{FESR}.
Stability criteria have also been tested in
models such as
harmonic oscillator, where the exact and approximate
solutions are known \cite{BERT}. The {\it most conservative
optimization criteria} which include various types of optimizations
in the literature are the following: the
optimal result is obtained in the region,
from the beginning of $\tau / n$ stability (this corresponds in most
of the cases to the so-called plateau discussed often in the literature,
but in my opinion, the interpretation of this nice plateau as a good
sign of a good continuum model is not sufficient, in the sense
that the flatness of the
curve extends in the uninteresting high-energy region where the
properties of the ground state are lost),
until the beginning of the $t_c$
stability, where the value of $t_c$ corresponds to about the one fixed by
FESR duality constraints.
The earlier {\it sum rule window} introduced by SVZ, stating that the
optimal result should be in the region where both the non-perturbative
and continuum contributions are {\it small} is included in the previous
region.
%Our criteria renders the SVZ statement more accurate because it gives a
%precise meaning on the word {\it small}.
 Indeed, at the stability
point, we have an equilibrium between the continuum and non-perturbative
contributions, which are both small,
while the OPE is still convergent  at this point.

\nin
The gluon condensate contribution to the moments ${\cal M}^{(n)}$ and
so to ${\cal R}_n$ can be copied from the original work of SVZ \cite{SVZ}
and reads:
\beq
{\cal M}^{(n)}_G=-{\cal M}^{(n)}_{pert} ~\frac{(n+3)!}{(n-1)!(2n+5)}
\frac {4\pi}{9}\frac{\la \alf G^2 \ra}{\ga 4M_Q^2 \dr^2},
\eeq
where ${\cal M}^{(n)}_{pert}$ is the lowest perturbative expression
of the moments.
The one to the Laplace ratio ${\cal R}_\tau $ can be also
copied from the
original work of Bertlmann \cite{BERT}, which has been expanded
recently in $1/M_Q$ by \cite{DOM}. It reads:
\beq
{\cal R}^G_\tau \simeq (4M^2_Q)\frac{2\pi}{3}\la \alf G^2 \ra \tau^2
\ga 1+\frac{4}{3\omega}-\frac{5}{12\omega^2} \dr ,
\eeq
where $\omega = 4M^2_Q \tau$. Due to the poor accuracy of $\la \alf G^2 \ra$,
we
used the recent two-loop calculation of \cite{BROAD2}.

\nin
We give the results of our analysis in
Fig. 1 from the FESR version of these relativistic
sum rules as we have transferred,
into the QCD side, the QCD continuum contribution, such that in the
ratio, we only remain with the resonance contributions in the RHS
of the sum rule. At the stability point or for large n-values, the
experimental ratio of the sum rules give, with an accuracy better
than 1$^0/_{00}$, the mass squared of the lowest ground state. The
curves in Fig. 1 are
for a given value of $\alf (M_b)=0.217$ and the corresponding
$\alf (M_c)=0.350$. As explained previously, our best solution
is obtained at the minimum of the curve for ${\cal R}_\tau$, while
for ${\cal R}_n$, the curve is flat and insensitive to n. As one can
notice, the reproduction of the resonance mass needs a sharp value of
the running mass, while the moments and Laplace sum rules give
practically the same solution of $\overline {m}_b$. We have also
checked that the result is almost insensitive to the choice of the
subtraction point varying in the range from $\tau^{-1/2}\simeq 1.4$ GeV
to $M_Q$. That is due to the small effect of the radiative corrections
in the sum rule analysis. However, the natural choice of the scale
as dictated by the RGE is $M_b$ for the moments \cite{SNY}
and $\tau^{-1/2}$ for
the Laplace \cite{RAF2}.
It is also clear
due to the smallness of the $c$-quark mass that we cannot use at our
approximation the moments for this channel.
 \section{Non-relativistic
 pole masses from the $\Psi$- and $\Upsilon$-systems}
Let us now extract directly the {\it non-relativistic}
pole masses from the $\Psi$ and $\Upsilon$
data, by using the non-relativistic version of the
previous sum rules. This determination is interesting as a comparison of this
result with the {\it short distance perturbative pole mass}
 from the perturbative expression in Eq. (1) via the running
mass can measure the size of the renormalon contribution discussed in
\cite{REN}

\nin
The non-relativistic Laplace sum rule has been discussed in details
by Bell and Bertlmann \cite{BERT}. In this case the non-relativistic
ratio of moments ${\cal R}^{NR}_{\tau}$ is about $\sqrt{{\cal R}_\tau}$ and
can be deduced from ${\cal R}_\tau$ by the introduction of the non-relativistic
variable:
\beq
\tau_{NR}= 4M_Q\tau .
\eeq
The results of this analysis are shown in Fig. 2 for a given value of $\alf$
and
different values of $M_Q$, where as in Fig. 1, the agreement with the data
gives
constraint on the value of $M_Q$.

\nin
The non-relativistic version of the moments has been
discussed in \cite{VOL,VOL2}, where a summation of the higher order Coulombic
co
has been done. The moment reads \cite{VOL}:
\bea
{\cal M}^{(n)}_{NR} &\equiv &
\int_{4M^2_b}^{\infty} ~dt~ \mbox{exp}\ga \ga1-\frac{t}{4M^2_b}\dr n\dr
\frac{1}{\pi}~\mbox{Im}~\Pi_b(t) \nnb \\
 & = & M^2_b~\ga \frac{3}{4\pi^2} \dr
\frac{\sqrt{\pi}}{n^{3/2}}\ga 1-\frac{16}{3}\frac{\alf}{\pi}\dr\aga
\Phi_s(\gamma)-\frac{\pi}{72}\la \alf G^2\ra \frac{n^3}{M^4_b}X_s(\gamma)\adr
,
\eea
where:
\beq
\gamma = \frac{2}{3} \alf n^{1/2} ~~~~~~~~X_s(\gamma)\simeq
e^{-0.8\gamma}\Phi_s
\eeq
and:
\beq
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
\Phi_s(\gamma)=1+2\sqrt{\pi}\gamma+\frac{2\pi^2}{3}\gamma^2+4\sqrt{\pi}\sum_{i=1
\ga \frac{\gamma}{n} \dr ^3 \mbox{exp}\ga\frac{\gamma}{n}^2\dr\ga 1+\mbox{erf}
\ga\frac{\gamma}{n}\dr\dr
\eeq
with:
\beq
\mbox{erf}(x)= \frac{2}{\sqrt{\pi}}\int_{0}^{x}dt~\mbox{exp}\ga -t^2\dr .
\eeq
The result from this sum rule is also shown in Fig. 2, where we anticipate that
the value $\approx$ 4.8 GeV claimed in \cite{VOL} is not reproduced,
even if we use the same input parameters as \cite{VOL}, though we agree with
the
value of $n \approx 25$ and on the corresponding value of
$\Phi_s(\gamma)\approx
Instead, our result is more
similar to the previous value obtained by the one of the authors \cite{VOL2},
from a similar sum rule.
\section{Conclusions from the $\Psi$- and $\Upsilon$-systems}
We give our complete results  in Table 2 for the $b$ and in
Table 3 for the $c$.

\begin{table}[h]
\begin{center}
\begin{tabular}[h]{||l|llllll||}
\hline \hline
 & & & & & &\\
$\alf(M_b)$&$\overline
{m}_b (M_b)$&$\hat {m}_b$&
$m^{EU}_b$&$M_b^{PT2}$&$M_b^{PT3}$&$M_b^{NR}$\\
 & & & & & &\\
\hline \hline
0.198 &4.26 &8.33& 4.25& 4.62 &4.83&4.68 \\
0.217 &4.23 &7.83& 4.21& 4.62 &4.87&4.69 \\
0.240 &4.19 &7.23& 4.17& 4.62 &4.92&4.71 \\
0.254 &4.17 &7.05& 4.15& 4.62 &4.96&4.71  \\
\hline \hline
\end{tabular}
\caption{\it Two-loop values of the $b$-quark masses for different values of
$\a
for 5 flavours except for $M^{PT}_b$ given also at the tree-loop level.}
\end{center}
\end{table}


\nin

\begin{table}[h]
\begin{center}
\begin{tabular}[h]{||l|llllll||}
\hline \hline
 & & & & & &\\
$\alf(M_c)$&$\overline {m}_c (M_c)$&$\hat {m}_c$&
$m^{EU}_c$&$M_c^{PT2}$&$M_c^{PT3}$&$M_c^{NR}$\\
 & & & & & &\\
\hline \hline
0.299 &1.25 &1.78& 1.24& 1.41&1.56 &1.42 \\
0.350 &1.23 &1.60& 1.22& 1.41&1.62 &1.44 \\
0.420 &1.19 &1.39& 1.18& 1.40&1.69 &1.46 \\
0.493 &1.16 &1.23& 1.15& 1.40&1.78 &1.49  \\
\hline \hline
\end{tabular}
\caption{\it Two-loop values of the $c$-quark masses for different values of
$\a
4 flavours except for $M^{PT}_c$ given also at the tree-loop level.}
\end{center}
\end{table}

\nin
The running mass $\overline{m}_Q$ directly obtained from
the sum rules for different
values of $\alf$ (first column) from Table 1,
is given in the second column. We use the two-loop relation \cite{FLO,SNB}:
\beq
\overline{m}_Q(p^2) = \hat{m}_Q\ga -\beta_1\frac{\alf(p^2)}{\pi}\dr
^{-\gamma_1/\beta_1} \aga 1~+~\frac{\beta_2}{\beta_1}
\ga \frac{\gamma_1}{\beta_1}-\frac{\gamma_2}{\beta_2}\dr
\ga \frac{\alf}{\pi}\dr
\adr ,
\eeq
where $\hat{m}_Q$ is the invariant mass \cite{FLO}(third column); $\gamma_1=2$
and $\gamma_2= 101/12-5n_f/18$
(third column). The gauge-dependent Euclidian mass
$m^{EU}_Q $ (fourth column) reads in the Landau gauge:
\beq
m^{EU}_Q(p^2=-M^2_Q)
=\overline{m}_Q(M_Q)\aga 1+\ga\frac{\alpha_s(M_Q)}{\pi}\dr
\ga -2\log2 +\frac{4}{3} \dr \adr .
\eeq
We use Eq. (1) to get the short distance {\it perturbative} pole mass
$M^{PT}_Q$
and 6th columns).
The pole mass $M^{NR}_b$ directly obtained from non-relativistic sum rules is
given in the last column. We have only considered the one from the Laplace
ratio
${\cal R}^{NR}_{\tau}$, which appears to be more reliable than the
moment  analysis.

\nin
 Using the {\it world average}\cite{BETHKE}: $\alf (M_Z)=0.118 \pm 0.006$,
we obtain, for the $b$-quark mass at the two-loop level, the values, in units
of
\beq
\overline{m}_b(M_b)= 4.23 ~^{+0.03}_{-0.04}~\pm 0.02 ~~~
\hat{m}_b=7.83~^{+0.40}_{-0.60}~\pm 0.04 ~~~
m^{EU}_b=4.21\pm 0.04 \pm 0.02
\eeq
and:
\beq
M^{PT2}_b=4.62 \pm 0.02 ~~~~~~~~~~~~~~~
M^{NR}_b=4.69~^{-0.01}_{+0.02} \pm 0.02.
\eeq

\nin
It is informative to compare this two-loop result with the ones in the existing
which are known at the same level of accuracy.
The value of the invariant mass $\hat {m}_b$ agrees with the one given in
\cite{
while the error is reduced here by a factor of about 2 due to the progress in
th
measurement of $\alf$. The value of the Euclidian mass $m^{EU}_b$ obtained here
the running mass, is compatible with the one extracted directly from the sum
rul
\cite{SVZ}-\cite{BERT}, despite the different values of $\alf$ used in these
pap
which most of  the time are incompatible with the range given
in Table 1. Indeed, the use
of the Euclidian mass in the sum rules, minimizes the size of the radiative
corr
and then the one of $\alf$ in the sum rule estimate of $m^{EU}$. However,
the uncertainty due
to $\alf$ appears when one translates this mass into the pole one $M^{PT2}_b$,
t
\beq
M^{PT2}_Q=m^{EU}_Q(p^2=-M^2_Q)
\aga 1+2\log2\ga\frac{\alpha_s(M_Q)}{\pi}\dr
\adr ,
\eeq
or if one extracts directly the pole mass from relativistic sum rules. One can
a
notice that $M^{PT2}_Q$ is almost constant in the given
range of $\alf$ values, as the change in the running mass is compensated by the
in $\alf$ via Eq. (1). The value of $M^{NR}_b$ agrees
with the one of \cite{BERT,DOM}, while
we have improved the recent re-estimate of \cite{DOM}
by using consistently the value
of $\Lambda$ and the corresponding two-loop expression
 of $\alf$. However, as already stressed, our
analysis using the same non-relativistic
moments in Eq. (18) does not favour the
value $4.8$ GeV claimed by \cite{VOL}.

\nin
It is interesting to compare $M^{NR}_b$, with the {\it dressed mass}
 $M^{nr}_b$ from the
non-relativistic treatment  of the bound state motion, where the leading
non-per
effect is included. For a sufficiently heavy quark, the {\it Balmer formula}
for the lowest ground state reads \cite{GASSER,LEUT}:
\beq
M_{\Upsilon}=2M^{nr}_b\aga 1-\frac{1}{8}
\ga C_F\alf \dr ^2+ {\cal O} \alf^3+
\frac{\pi}{2}~\frac{\la{\alf G^2}\ra}{\ga M^{nr}_b \dr ^4}
\frac{\ga \epsilon_{10}\simeq 1.468 \dr}{\ga C_F\alf \dr ^4} ~ \adr
\eeq
where $C_F =4/3$, from which one
deduces\footnote[3]{The next-to-leading corrections
to this formula have been evaluated in \cite{YND},
 but we have not included them in our estimate in Eq. (28)
in order to have a consistent comparison
with $M^{NR}_b$ obtained at the two-loop level. These higher order
corrections are taken into account in Eq. (29).}:
\beq
M^{nr}_b = (4.57\pm 0.09\pm 0.14)~\mbox{GeV},
\eeq
 where the errors are due to $\alf$ and $\la \alf G^2 \ra $.
 The difference of the central value
with the one ($4.76 \pm 0.10 \pm 0.05$) GeV
obtained in \cite{LEUT,YND} is mainly due to the different value of
$\alf$ and of the gluon condensate used there. However, the error
 due to the latter has been underestimated in \cite{YND}. The large
role of the gluon condensate also indicates that the $b$-quark is not
enough heavy, such that we have not yet reached the coulombic regime.

\nin
One might
also follow \cite{YND} by including higher order $\alf$
corrections and by trying to optimize the
convergence of the QCD series, which can be
realized at a scale $\mu \approx 1.5 $ GeV. In this way,
the gluon condensate effect is almost negligible, while the perturbative series
dominated by the $\alf^2$ and $\alf^4$ terms. However, the price to pay is the
s
of the result on the $\alf$-value. One obtains in this way:
\beq
M^{nr}_b = (4.94\pm 0.10 \pm 0.03)~\mbox{GeV},
\eeq
where, we again notice the underestimate of the error in \cite{YND}.
One might expect from its derivation based on the $\overline{b}b$
potential, that $M^{nr}_b$ is likely similar to the
so-called {\it constituent mass} used in the potential model
approach for predicting the mass spectra \cite{RICH}, while it
is quite unlikely to deduce the running mass
of the $\overline{MS}$-scheme from it. It is interesting to compare this value
with the short-distance pole mass deduced from
the three-loop relation in Eq. (1),
which reads:
\beq
 M^{PT3}_b=(4.87 \pm 0.05 \pm 0.02) ~ \mbox {GeV}.
\eeq
It is important to notice that the inclusion of the three-loop terms into the
re
in Eq. (1) has boosted appreciably the value of
the pole mass $M^{PT3}_Q$, such that the next improvment of this estimate
is the inclusion of the unknown $\alf^3$-term \footnote[4]{The estimate
of this effect \`a la \cite{KATA}
cannot be used here in a straightforward way, as the running
mass has an anomalous dimension. However, if we use a guessed estimate
of the coefficient based on a geometric sum \`a la \cite{BRAT}, we
would obtain an effect of $\pm {\cal O} 100 (\alf/\pi)^3 \approx 3\%$
for the $b$, which might be an overestimate.} as well as the $\alf^2$-
term in the hadronic correlator.
%Therefore,
%a conservative estimate at the tree-loop level would be:
%\beq
% M^{PT3}_b=(4.87 \pm 0.05 \pm 0.02 \pm 0.16)~ \mbox {GeV}.
%\eeq

\nin
 One has also to notice that one should be careful in the use
of this three-loop
mass in different phenomenological applications. In particular,
for the case of different sum rule analysis
(estimate of the decay constants,...),
where the hadronic correlators are only known to two-loop accuracy,
one {\it should neither
use} $M^{PT3}_Q$, $nor$ $M^{nr}_b$ for consistency.

\nin
A comparison of $M^{PT}_b$ with $M^{NR}_b$ at the two-loop level leads to:
\beq
\Delta M_b\equiv M^{NR}_b-M^{PT2}_b = (70 ~^{-10}_{+20} )~ \mbox{MeV},
\eeq
while a comparison of $M^{nr}_b$ (which we expect from its
definition to be identical with $M^{NR}_b$)
with the value of the short-distance perturbative mass at the three-loop
level:
\beq
\Delta M_b\equiv M^{nr}_b-M^{PT3}_b =(70 \pm 100)~ \mbox{MeV},
\eeq
gives about the same small value but with a larger error.
 We might expect that
this mass difference measures
the size of the renormalon singularities, which
after a resummation of the QCD large order perturbative series is expected to
give an effect of the order of $\Lambda$
\cite{REN}\footnote[5]{ However, a precise quantitative derivation of
that value from the theoretical point of view is still lacking as one has to
wor
limit of
large number of flavours, where one loses asymptotic freedom.}.
Our analysis
indicates that the renormalon effect can be even smaller than the
present value  of $\Lambda$ given in Table 1.

\nin
For the charm quark, our results, in units of GeV, are:
\beq
\overline{m}_c(M_c	)= 1.23 ~^{+0.02}_{-0.04}~\pm 0.03 ~~~
\hat{m}_c=1.60~^{+0.18}_{-0.21}~\pm 0.04 ~~~
m^{EU}_c=1.22~^{+0.02}_{-0.04}\pm 0.03
\eeq
and:
\beq
M^{PT2}_c=1.41 \pm 0.03 ~~~~~~~~~~~~~
M^{NR}_c=1.44\pm 0.02 \pm 0.03,
\eeq
where the errors are respectively due to $\alf$
and to the gluon condensate.
At the three-loop level, we have:
\beq
M^{PT3}_c=(1.62\pm 0.07  \pm 0.04)~\mbox{GeV},
\eeq
where the last error is due to an estimate of the $\alf^3$-unknown
correction.
The same
discussions as for the $b$-quark case are valid here, when we
do the comparison with
previous estimates given in the literature.
A comparison between $M_c^{PT}$ and $M_c^{NR}$
shows that:
\beq
\Delta M_c \simeq (30 \pm 20 ) ~\mbox{MeV},
\eeq
which may indicate that the renormalon effect is smaller
for the charm than for the  bottom
quark. It may suggest that the leading-order (in $1/n_f$ and
most probably in $1/M_Q$) calculation of this contribution might be
 largely affected by the non-leading corrections.
\section{ Quark masses from the heavy-light mesons}
We re-examine in the same way, the extraction of the $b$-quark mass from
the $B$ and $B^*$ meson masses, in order to test the stability of the
result\cite{SNX}:
\beq
M_b^{PT2}= (4.56 \pm 0.05)~\mbox{GeV},
\eeq
from the ratio of relativistic
sum rules. For convenience, we introduce the variable $E_c$:
\beq
t_c= (E_c+M_b)^2.
\eeq
In order to be conservative with the different choices in the literature,
we use:
\beq
E_c = (1.3 \pm 0.3)~\mbox{GeV}.
\eeq
by multiplying by a factor 3 the error given in \cite{SNZ}. We give the
domain of predictions versus $M_b^{PT2}$ in Fig. 3,
from which we conclude:
\beq
M_b^{PT2}=(4.63 \pm 0.08)~\mbox{GeV},
\eeq
which is consistent with the previous value and with the one
from the $\Upsilon$-systems. The large error is due to the conservative
range of $E_c$, while the smaller central value in Eq. (37) is related
to the higher value of $E_c$ and to the small
value of $\alf$ used in previous
works.

\nin
We have also performed the analysis using nonrelativistic sum rules.
Though the result for $M_b^{NR}$ is consistent with the one from
the vector channel, it is quite influenced by the value of $\alf$ or
$\Lambda$ used, which renders the analysis quite inaccurate. That is
partly due to a larger value of the $\alf$ correction in this sum rule
and to the disappearance of the stability points in the analysis.
Finally, we have compared the previous results on $M_b^{NR}$
with the one from
heavy quark effective theory (HQET) sum rule \cite{BALL} in the infinite
mass limit, which gives:
\beq
\delta M^{\infty}
_b\equiv (M_B-M^{NR}_b)_{\infty} \simeq (0.5-0.6)~\mbox{GeV},
\eeq
while the
usual full-QCD relativistic sum rule for
increasing value of $M^{NR}_b~(\geq 5$ GeV) gives \cite{SNY}:
\beq
\delta M^{\infty}_b \simeq (0.6-0.8)~\mbox{GeV},
\eeq
from which, we deduce the conservative value:
\beq
\delta M^{\infty}_b \simeq (0.6^{+0.2}_{-0.1})~\mbox{GeV}.
\eeq
These results are in agreement with the previous determinations from
the $\Upsilon$-systems,
though they are less accurate. However, the agreement of the value
of $M^{NR}_b$ from the heavy-heavy and heavy-light systems may
indicate that the ambiguity due to the renormalon effects into the
definition of the pole masses entering into the two channels is
negligible, which in some sense is supported by the small value of
the mass-difference $M_b^{NR}-M_b^{PT2}$.
\section{Conclusions}
We have updated the theoretical estimate of the heavy quark masses
from QCD spectral sum rules,
by using the latest average value of $\alf$.
The best results come from the $\Upsilon$ and $\Psi$ data
and are given to two-loops in Eqs. (24), (25), (33) and (34), while the
three-loop results for the short distance pole masses
are in Eqs. (30) and (35).
The good accuracy from the vector channels is
somewhat expected as the data are known in details there.
Results from the $B$ and $B^*$ mesons are less accurate, which are
mainly due to the lesser control of the QCD continuum threshold,
which has been taken in a large range of values, in order to have
a more conservative result.


\nin
We have resolved the apparent disagreement of the results given in the
literature by a careful re-examination of each analysis. One of the
main sources of discrepancies is due to
the different values of $\alf$ used
in the literature. Our value of the Euclidian mass is in good agreement
with the direct determinations in \cite{SVZ}-\cite{BERT}. Our value
for the running mass agrees within the errors with the previous results
\cite{LEUT,SN1} deduced through the perturbative pole masses.
The small discrepancy in this determination
can be resolved if one uses the
same value of $\alf$. Our value of the short distance pole mass agrees
from the direct determination \cite{BERT} for a given value of $\alf$.
The apparent discrepancy with \cite{REINDERS} disappears once one uses
the same value of $\alf$.
Our two-loop result for the non-relativistic mass agrees with the
direct determination \cite{BERT,DOM} when one uses in these papers the
same value of $\alf$ to two-loop accuracy. However,
we do not $exceptionnally$ recover the
value 4.8 GeV of \cite{VOL} but his earlier result \cite{VOL2}.
Moreover, our two-loop result rules out the value of the pole charm quark
mass of 1.35 GeV and of the $b$-quark pole mass of 4.8 GeV,
used {\it sometimes abusively} in the literature.

\nin
The use of the three-loop relation in Eq. (1)
suggests that radiative corrections are relatively large and shifts the
two-loop pole mass by +3.8 and +14 $\%$ for the $b$ and $c$ quark masses.
This effect is, however, interesting as it restores the agreement between
the pole mass with the value of the so-called constituent mass
favoured in potential models \cite{RICH}, which is likely to be the
same as $M^{nr}_b$ appearing in the Balmer formula, with the value
given in Eq. (29).
In particular, the {\it b-c} mass difference which appears to be a safe
prediction of potential models is obtained within the errors
from our analysis. The three-loop value of the charm pole mass
is also in agreement with
the recent lattice calculations including $\alf^2$-corrections
\cite{LATTICE}, while the value of $M^{nr}_b$ including higher
order corrections, should be similar to the one obtained recently
from the lattice results in \cite{LATT}, due to the non-relativistic
way used in the lattice calculation. However, a
sharp comparison still needs
lattice results with smaller error bars and
in the $unquenched~approximation$, though one expects the probability
for creating  $\bar qq$ pairs to be small.
\nin
Finally, our results suggest that the mass difference between the
short-distance and the non-relativistic pole masses is small of
about 70 MeV, and presumably less. This is an indication that the
non-perturbative effects induced by the summation of the QCD series
at large order due to renormalon-type singularities can be relatively
negligible.

\nin
One of the immediate consequences of these $new$ two-loop results is the
prediction on the $D$ and $B$
decay constants which are very sensitive to the value
of the quark masses used in the analysis, whose explicit mass-dependence
has been studied in \cite{SNW}. With the previous values of the short
distance pole mass which are consistent with the uses of the relativistic
Laplace sum rule results, one can deduce from the table of \cite{SNW},
the updated and improved values:
\beq
f_D = (1.37\pm 0.04\pm 0.06)f_\pi~~~~~~~~~~~~~
f_B=(1.49\pm 0.06\pm 0.05)f_\pi,
\eeq
where the errors come respectively from the
pseudoscalar sum rule analysis
and from the quark masses.
 We consider this result as an improvement of
the one in \cite{SNY}, where due to the change in the quark-mass values,
the value of $f_D$ (resp. $f_B$) has slightly increased
(resp. decreased). By combining this result with the bag factor
$B_B=1\pm 0.15$ obtained to two-loops in \cite{PIVO}, one can deduce:
\beq
f_B\sqrt{B_B}=(1.49\pm 0.14)f_\pi,
\eeq
after adding the different errors quadratically. The use of this value
should improve the phenomenological constraints on the values of the
CKM-mixing parameters (see e.g. \cite{ALI}).

\vfill \eject
\section*{Figure captions}
{\bf Fig. 1:} {\bf a)}:
value of $M_\Upsilon$ from the ratio of the relativistic Laplace sum
rule ${\cal R}_\tau^b$
versus the sum rule variable $\tau$
for different values of the running mass $\overline{m}_b(M_b)$ given
$\alf(M_b)=0.217$; {\bf b)}: analogous to {\bf a)} but from the ratio of
moments; {\bf c)}: analogous to {\bf a)} but for the $\Psi$.
\vspace*{0.5cm}

\nin
{\bf Fig. 2:} {\bf a)}: non-relativistic analogue of Fig. 1a), with
$\tau_{NR}=4M_b\tau$. The dashed line is the experimental data which
tend to $M_\Upsilon$ for large $\tau_{NR}$; {\bf b)}: confrontation
of the two sides of the non-relativistic moment in Eq. (18) versus $n$
and for different values of the pole mass, given $\alf(M_b)$=0.217.
The dashed lines are the LHS from the data; {\bf c)}: analogous to
{\bf a)} but for the $\Psi$.
\vspace*{0.5cm}

\nin
{\bf Fig. 3:} Simultaneous fit of the $B$ and
$B^*$ masses from the ratios
of the relativistic moments. The horizontal
 lines correspond to the masses
from the data. The corresponding theoretical domains are for $E_c = (1.3
\pm 0.3)$ GeV for different values of the pole mass from the
$n$-stability.
\vfill \eject
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\end{document}













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%%BeginProlog
%%BeginResource: procset Adobe_level2_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Level 2 Emulation)
%%Version: 1.0
%%CreationDate: (04/10/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
userdict /Adobe_level2_AI5 21 dict dup begin
	put
	/packedarray where not
	{
		userdict begin
		/packedarray
		{
			array astore readonly
		} bind def
		/setpacking /pop load def
		/currentpacking false def
	 end
		0
	} if
	pop
	userdict /defaultpacking currentpacking put true setpacking
	/initialize
	{
		Adobe_level2_AI5 begin
	} bind def
	/terminate
	{
		currentdict Adobe_level2_AI5 eq
		{
		 end
		} if
	} bind def
	mark
	/setcustomcolor where not
	{
		/findcmykcustomcolor
		{
			5 packedarray
		} bind def
		/setcustomcolor
		{
			exch aload pop pop
			4
			{
				4 index mul 4 1 roll
			} repeat
			5 -1 roll pop
			setcmykcolor
		}
		def
	} if
	/gt38? version cvx exec 38 gt def
	userdict /deviceDPI 72 0 matrix defaultmatrix dtransform dup mul exch dup mul
a
	userdict /level2?
	systemdict /languagelevel known dup
	{
		pop systemdict /languagelevel get 2 ge
	} if
	put
	level2? not
	{
		/setcmykcolor where not
		{
			/setcmykcolor
			{
				exch .11 mul add exch .59 mul add exch .3 mul add
				1 exch sub setgray
			} def
		} if
		/currentcmykcolor where not
		{
			/currentcmykcolor
			{
				0 0 0 1 currentgray sub
			} def
		} if
		/setoverprint where not
		{
			/setoverprint /pop load def
		} if
		/selectfont where not
		{
			/selectfont
			{
				exch findfont exch
				dup type /arraytype eq
				{
					makefont
				}
				{
					scalefont
				} ifelse
				setfont
			} bind def
		} if
		/cshow where not
		{
			/cshow
			{
				[
				0 0 5 -1 roll aload pop
				] cvx bind forall
			} bind def
		} if
	} if
	cleartomark
	/anyColor?
	{
		add add add 0 ne
	} bind def
	/testColor
	{
		gsave
		setcmykcolor currentcmykcolor
		grestore
	} bind def
	/testCMYKColorThrough
	{
		testColor anyColor?
	} bind def
	userdict /composite?
	level2?
	{
		gsave 1 1 1 1 setcmykcolor currentcmykcolor grestore
		add add add 4 eq
	}
	{
		1 0 0 0 testCMYKColorThrough
		0 1 0 0 testCMYKColorThrough
		0 0 1 0 testCMYKColorThrough
		0 0 0 1 testCMYKColorThrough
		and and and
	} ifelse
	put
	composite? not
	{
		userdict begin
		gsave
		/cyan? 1 0 0 0 testCMYKColorThrough def
		/magenta? 0 1 0 0 testCMYKColorThrough def
		/yellow? 0 0 1 0 testCMYKColorThrough def
		/black? 0 0 0 1 testCMYKColorThrough def
		grestore
		/isCMYKSep? cyan? magenta? yellow? black? or or or def
		/customColor? isCMYKSep? not def
	 end
	} if
 end defaultpacking setpacking
%%EndResource
%%BeginResource: procset Adobe_typography_AI5 1.0 0
%%Title: (Typography Operators)
%%Version: 1.0
%%CreationDate:(03/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_typography_AI5 48 dict dup begin
put
/initialize
{
 begin
 begin
	Adobe_typography_AI5 begin
	Adobe_typography_AI5
	{
		dup xcheck
		{
			bind
		} if
		pop pop
	} forall
 end
 end
 end
	Adobe_typography_AI5 begin
} def
/terminate
{
	currentdict Adobe_typography_AI5 eq
	{
	 end
	} if
} def
/modifyEncoding
{
	/_tempEncode exch ddef
	/_pntr 0 ddef
	{
		counttomark -1 roll
		dup type dup /marktype eq
		{
			pop pop exit
		}
		{
			/nametype eq
			{
				_tempEncode /_pntr dup load dup 3 1 roll 1 add ddef 3 -1 roll
				put
			}
			{
				/_pntr exch ddef
			} ifelse
		} ifelse
	} loop
	_tempEncode
} def
/TE
{
	StandardEncoding 256 array copy modifyEncoding
	/_nativeEncoding exch def
} def
%
/TZ
{
	dup type /arraytype eq
	{
		/_wv exch def
	}
	{
		/_wv 0 def
	} ifelse
	/_useNativeEncoding exch def
	pop pop
	findfont _wv type /arraytype eq
	{
		_wv makeblendedfont
	} if
	dup length 2 add dict
 begin
	mark exch
	{
		1 index /FID ne
		{
			def
		} if
		cleartomark mark
	} forall
	pop
	/FontName exch def
	counttomark 0 eq
	{
		1 _useNativeEncoding eq
		{
			/Encoding _nativeEncoding def
		} if
		cleartomark
	}
	{
		/Encoding load 256 array copy
		modifyEncoding /Encoding exch def
	} ifelse
	FontName currentdict
 end
	definefont pop
} def
/tr
{
	_ax _ay 3 2 roll
} def
/trj
{
	_cx _cy _sp _ax _ay 6 5 roll
} def
/a0
{
	/Tx
	{
		dup
		currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
	} ddef
	/Tj
	{
		dup
		currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
	} ddef
} def
/a1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/e0
{
	/Tx
	{
		tr _psf
	} ddef
	/Tj
	{
		trj _pjsf
	} ddef
} def
/e1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		tr _psf
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		trj _pjsf
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/i0
{
	/Tx
	{
		tr sp
	} ddef
	/Tj
	{
		trj jsp
	} ddef
} def
/i1
{
	W N
} def
/o0
{
	/Tx
	{
		tr sw rmoveto
	} ddef
	/Tj
	{
		trj swj rmoveto
	} ddef
} def
/r0
{
	/Tx
	{
		tr _ctm _pss
	} ddef
	/Tj
	{
		trj _ctm _pjss
	} ddef
} def
/r1
{
	/Tx
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/To
{
	pop _ctm currentmatrix pop
} def
/TO
{
	iTe _ctm setmatrix newpath
} def
/Tp
{
	pop _tm astore pop _ctm setmatrix
	_tDict begin
	/W
	{
	} def
	/h
	{
	} def
} def
/TP
{
 end
	iTm 0 0 moveto
} def
/Tr
{
	_render 3 le
	{
		currentpoint newpath moveto
	} if
	dup 8 eq
	{
		pop 0
	}
	{
		dup 9 eq
		{
			pop 1
		} if
	} ifelse
	dup /_render exch ddef
	_renderStart exch get load exec
} def
/iTm
{
	_ctm setmatrix _tm concat 0 _rise translate _hs 1 scale
} def
/Tm
{
	_tm astore pop iTm 0 0 moveto
} def
/Td
{
	_mtx translate _tm _tm concatmatrix pop iTm 0 0 moveto
} def
/iTe
{
	_render -1 eq
	{
	}
	{
		_renderEnd _render get dup null ne
		{
			load exec
		}
		{
			pop
		} ifelse
	} ifelse
	/_render -1 ddef
} def
/Ta
{
	pop
} def
/Tf
{
	dup 1000 div /_fScl exch ddef
	exch findfont exch scalefont setfont
} def
/Tl
{
	pop
	0 exch _leading astore pop
} def
/Tt
{
	pop
} def
/TW
{
	3 npop
} def
/Tw
{
	/_cx exch ddef
} def
/TC
{
	3 npop
} def
/Tc
{
	/_ax exch ddef
} def
/Ts
{
	/_rise exch ddef
	currentpoint
	iTm
	moveto
} def
/Ti
{
	3 npop
} def
/Tz
{
	100 div /_hs exch ddef
	iTm
} def
/TA
{
	pop
} def
/Tq
{
	pop
} def
/Th
{
	pop pop pop pop pop
} def
/TX
{
	pop
} def
/Tk
{
	exch pop _fScl mul neg 0 rmoveto
} def
/TK
{
	2 npop
} def
/T*
{
	_leading aload pop neg Td
} def
/T*-
{
	_leading aload pop Td
} def
/T-
{
	_hyphen Tx
} def
/T+
{
} def
/TR
{
	_ctm currentmatrix pop
	_tm astore pop
	iTm 0 0 moveto
} def
/TS
{
	0 eq
	{
		Tx
	}
	{
		Tj
	} ifelse
} def
currentdict readonly pop
end
setpacking
%%EndResource
%%BeginResource: procset Adobe_IllustratorA_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Abbreviated Prolog)
%%Version: 1.0
%%CreationDate: (3/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_IllustratorA_AI5_vars 70 dict dup begin
put
/_lp /none def
/_pf
{
} def
/_ps
{
} def
/_psf
{
} def
/_pss
{
} def
/_pjsf
{
} def
/_pjss
{
} def
/_pola 0 def
/_doClip 0 def
/cf currentflat def
/_tm matrix def
/_renderStart
[
/e0 /r0 /a0 /o0 /e1 /r1 /a1 /i0
] def
/_renderEnd
[
null null null null /i1 /i1 /i1 /i1
] def
/_render -1 def
/_rise 0 def
/_ax 0 def
/_ay 0 def
/_cx 0 def
/_cy 0 def
/_leading
[
0 0
] def
/_ctm matrix def
/_mtx matrix def
/_sp 16#020 def
/_hyphen (-) def
/_fScl 0 def
/_cnt 0 def
/_hs 1 def
/_nativeEncoding 0 def
/_useNativeEncoding 0 def
/_tempEncode 0 def
/_pntr 0 def
/_tDict 2 dict def
/_wv 0 def
/Tx
{
} def
/Tj
{
} def
/CRender
{
} def
/_AI3_savepage
{
} def
/_gf null def
/_cf 4 array def
/_if null def
/_of false def
/_fc
{
} def
/_gs null def
/_cs 4 array def
/_is null def
/_os false def
/_sc
{
} def
/discardSave null def
/buffer 256 string def
/beginString null def
/endString null def
/endStringLength null def
/layerCnt 1 def
/layerCount 1 def
/perCent (%) 0 get def
/perCentSeen? false def
/newBuff null def
/newBuffButFirst null def
/newBuffLast null def
/clipForward? false def
end
userdict /Adobe_IllustratorA_AI5 74 dict dup begin
put
/initialize
{
	Adobe_IllustratorA_AI5 dup begin
	Adobe_IllustratorA_AI5_vars begin
	discardDict
	{
		bind pop pop
	} forall
	dup /nc get begin
	{
		dup xcheck 1 index type /operatortype ne and
		{
			bind
		} if
		pop pop
	} forall
 end
	newpath
} def
/terminate
{
 end
 end
} def
/_
null def
/ddef
{
	Adobe_IllustratorA_AI5_vars 3 1 roll put
} def
/xput
{
	dup load dup length exch maxlength eq
	{
		dup dup load dup
		length 2 mul dict copy def
	} if
	load begin
	def
 end
} def
/npop
{
	{
		pop
	} repeat
} def
/sw
{
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
} def
/swj
{
	dup 4 1 roll
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
	6 2 roll /_cnt 0 ddef
	{
		1 index eq
		{
			/_cnt _cnt 1 add ddef
		} if
	} forall
	pop
	exch _cnt mul exch _cnt mul 2 index add 4 1 roll 2 index add 4 1 roll pop pop
} def
/ss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put pop
		gsave
		false charpath currentpoint
		4 index setmatrix
		stroke
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	3 npop
} def
/jss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put
		gsave
		_sp eq
		{
			exch 6 index 6 index 6 index 5 -1 roll widthshow
			currentpoint
		}
		{
			false charpath currentpoint
			4 index setmatrix stroke
		} ifelse
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	6 npop
} def
/sp
{
	{
		2 npop (0) exch
		2 copy 0 exch put pop
		false charpath
		2 copy rmoveto
	} exch cshow
	2 npop
} def
/jsp
{
	{
		2 npop
		(0) exch 2 copy 0 exch put
		_sp eq
		{
			exch 5 index 5 index 5 index 5 -1 roll widthshow
		}
		{
			false charpath
		} ifelse
		2 copy rmoveto
	} exch cshow
	5 npop
} def
/pl
{
	transform
	0.25 sub round 0.25 add exch
	0.25 sub round 0.25 add exch
	itransform
} def
/setstrokeadjust where
{
	pop true setstrokeadjust
	/c
	{
		curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll curveto
	} def
	/V
	/v load def
	/y
	{
		2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		lineto
	} def
	/L
	/l load def
	/m
	{
		moveto
	} def
}
{
	/c
	{
		pl curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll pl curveto
	} def
	/V
	/v load def
	/y
	{
		pl 2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		pl lineto
	} def
	/L
	/l load def
	/m
	{
		pl moveto
	} def
} ifelse
/d
{
	setdash
} def
/cf
{
} def
/i
{
	dup 0 eq
	{
		pop cf
	} if
	setflat
} def
/j
{
	setlinejoin
} def
/J
{
	setlinecap
} def
/M
{
	setmiterlimit
} def
/w
{
	setlinewidth
} def
/H
{
} def
/h
{
	closepath
} def
/N
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			clip /_doClip 0 ddef
		} if
		newpath
	}
	{
		/CRender
		{
			N
		} ddef
	} ifelse
} def
/n
{
	N
} def
/F
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _pf grestore clip newpath /_lp /none ddef _fc
			/_doClip 0 ddef
		}
		{
			_pf
		} ifelse
	}
	{
		/CRender
		{
			F
		} ddef
	} ifelse
} def
/f
{
	closepath
	F
} def
/S
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _ps grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			_ps
		} ifelse
	}
	{
		/CRender
		{
			S
		} ddef
	} ifelse
} def
/s
{
	closepath
	S
} def
/B
{
	_pola 0 eq
	{
		_doClip 1 eq
		gsave F grestore
		{
			gsave S grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			S
		} ifelse
	}
	{
		/CRender
		{
			B
		} ddef
	} ifelse
} def
/b
{
	closepath
	B
} def
/W
{
	/_doClip 1 ddef
} def
/*
{
	count 0 ne
	{
		dup type /stringtype eq
		{
			pop
		} if
	} if
	_pola 0 eq
	{
		newpath
	} if
} def
/u
{
} def
/U
{
} def
/q
{
	_pola 0 eq
	{
		gsave
	} if
} def
/Q
{
	_pola 0 eq
	{
		grestore
	} if
} def
/*u
{
	_pola 1 add /_pola exch ddef
} def
/*U
{
	_pola 1 sub /_pola exch ddef
	_pola 0 eq
	{
		CRender
	} if
} def
/D
{
	pop
} def
/*w
{
} def
/*W
{
} def
/`
{
	/_i save ddef
	clipForward?
	{
		nulldevice
	} if
	6 1 roll 4 npop
	concat pop
	userdict begin
	/showpage
	{
	} def
	0 setgray
	0 setlinecap
	1 setlinewidth
	0 setlinejoin
	10 setmiterlimit
	[
	] 0 setdash
	newpath
	0 setgray
	false setoverprint
} def
/~
{
 end
	_i restore
} def
/O
{
	0 ne
	/_of exch ddef
	/_lp /none ddef
} def
/R
{
	0 ne
	/_os exch ddef
	/_lp /none ddef
} def
/g
{
	/_gf exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_gf setgray
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/G
{
	/_gs exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_gs setgray
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/k
{
	_cf astore pop
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_cf aload pop setcmykcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/K
{
	_cs astore pop
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_cs aload pop setcmykcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/x
{
	/_gf exch ddef
	findcmykcustomcolor
	/_if exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_if _gf 1 exch sub setcustomcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/X
{
	/_gs exch ddef
	findcmykcustomcolor
	/_is exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_is _gs 1 exch sub setcustomcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/A
{
	pop
} def
/annotatepage
{
userdict /annotatepage 2 copy known {get exec} {pop pop} ifelse
} def
/discard
{
	save /discardSave exch store
	discardDict begin
	/endString exch store
	version cvx exec 38 gt
	{
		2 add
	} if
	load
	stopped
	pop
 end
	discardSave restore
} bind def
userdict /discardDict 7 dict dup begin
put
/pre38Initialize
{
	/endStringLength endString length store
	/newBuff buffer 0 endStringLength getinterval store
	/newBuffButFirst newBuff 1 endStringLength 1 sub getinterval store
	/newBuffLast newBuff endStringLength 1 sub 1 getinterval store
} def
/shiftBuffer
{
	newBuff 0 newBuffButFirst putinterval
	newBuffLast 0
	currentfile read not
	{
	stop
	} if
	put
} def
0
{
	pre38Initialize
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff endString eq
			{
				cleartomark stop
			} if
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
1
{
	pre38Initialize
	/beginString exch store
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff beginString eq
			{
				/layerCount dup load 1 add store
			}
			{
				newBuff endString eq
				{
					/layerCount dup load 1 sub store
					layerCount 0 eq
					{
						cleartomark stop
					} if
				} if
			} ifelse
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
2
{
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		endString eq
		{
			cleartomark stop
		} if
	} loop
} def
3
{
	/beginString exch store
	/layerCnt 1 store
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		dup beginString eq
		{
			pop /layerCnt dup load 1 add store
		}
		{
			endString eq
			{
				layerCnt 1 eq
				{
					cleartomark stop
				}
				{
					/layerCnt dup load 1 sub store
				} ifelse
			} if
		} ifelse
	} loop
} def
end
userdict /clipRenderOff 15 dict dup begin
put
{
	/n /N /s /S /f /F /b /B
}
{
	{
		_doClip 1 eq
		{
			/_doClip 0 ddef clip
		} if
		newpath
	} def
} forall
/Tr /pop load def
/Bb {} def
/BB /pop load def
/Bg {12 npop} def
/Bm {6 npop} def
/Bc /Bm load def
/Bh {4 npop} def
end
/Lb
{
	4 npop
	6 1 roll
	pop
	4 1 roll
	pop pop pop
	0 eq
	{
		0 eq
		{
			(%AI5_BeginLayer) 1 (%AI5_EndLayer--) discard
		}
		{
			/clipForward? true def

			/Tx /pop load def
			/Tj /pop load def
			currentdict end clipRenderOff begin begin
		} ifelse
	}
	{
		0 eq
		{
			save /discardSave exch store
		} if
	} ifelse
} bind def
/LB
{
	discardSave dup null ne
	{
		restore
	}
	{
		pop
		clipForward?
		{
			currentdict
		 end
		 end
		 begin

			/clipForward? false ddef
		} if
	} ifelse
} bind def
/Pb
{
	pop pop
	0 (%AI5_EndPalette) discard
} bind def
/Np
{
	0 (%AI5_End_NonPrinting--) discard
} bind def
/Ln /pop load def
/Ap
/pop load def
/Ar
{
	72 exch div
	0 dtransform dup mul exch dup mul add sqrt
	dup 1 lt
	{
		pop 1
	} if
	setflat
} def
/Mb
{
	q
} def
/Md
{
} def
/MB
{
	Q
} def
/nc 3 dict def
nc begin
/setgray
{
	pop
} bind def
/setcmykcolor
{
	4 npop
} bind def
/setcustomcolor
{
	2 npop
} bind def
currentdict readonly pop
end
currentdict readonly pop
end
setpacking
%%EndResource
%%EndProlog
%%BeginSetup
%%IncludeFont: Helvetica
%%IncludeFont: Symbol
Adobe_level2_AI5 /initialize get exec
Adobe_IllustratorA_AI5_vars Adobe_IllustratorA_AI5 Adobe_typography_AI5
/initial
Adobe_IllustratorA_AI5 /initialize get exec
[
39/quotesingle 96/grave 128/Adieresis/Aring/Ccedilla/Eacute/Ntilde/Odieresis
/Udieresis/aacute/agrave/acircumflex/adieresis/atilde/aring/ccedilla/eacute
/egrave/ecircumflex/edieresis/iacute/igrave/icircumflex/idieresis/ntilde
/oacute/ograve/ocircumflex/odieresis/otilde/uacute/ugrave/ucircumflex
/udieresis/dagger/degree/cent/sterling/section/bullet/paragraph/germandbls
/registered/copyright/trademark/acute/dieresis/.notdef/AE/Oslash
/.notdef/plusminus/.notdef/.notdef/yen/mu/.notdef/.notdef
/.notdef/.notdef/.notdef/ordfeminine/ordmasculine/.notdef/ae/oslash
/questiondown/exclamdown/logicalnot/.notdef/florin/.notdef/.notdef
/guillemotleft/guillemotright/ellipsis/.notdef/Agrave/Atilde/Otilde/OE/oe
/endash/emdash/quotedblleft/quotedblright/quoteleft/quoteright/divide
/.notdef/ydieresis/Ydieresis/fraction/currency/guilsinglleft/guilsinglright
/fi/fl/daggerdbl/periodcentered/quotesinglbase/quotedblbase/perthousand
/Acircumflex/Ecircumflex/Aacute/Edieresis/Egrave/Iacute/Icircumflex
/Idieresis/Igrave/Oacute/Ocircumflex/.notdef/Ograve/Uacute/Ucircumflex
/Ugrave/dotlessi/circumflex/tilde/macron/breve/dotaccent/ring/cedilla
/hungarumlaut/ogonek/caron
TE
%AI3_BeginEncoding: _Helvetica Helvetica
[/_Helvetica/Helvetica 0 0 1 TZ
%AI3_EndEncoding AdobeType
%AI3_BeginEncoding: _Symbol Symbol
[/_Symbol/Symbol 0 0 0 TZ
%AI3_EndEncoding AdobeType
%AI5_Begin_NonPrinting
Np
%AI3_BeginPattern: (Bandes jaunes)
(Bandes jaunes) 8.4499 4.6 80.4499 76.6 [
%AI3_Tile
(0 O 0 R 0 0.4 1 0 k 0 0.4 1 0 K) @
(
800 Ar
0 J 0 j 3.6 w 4 M []0 d
%AI3_Note:
0 D
8.1999 8.1999 m
80.6999 8.1999 L
S
8.1999 22.6 m
80.6999 22.6 L
S
8.1999 37.0001 m
80.6999 37.0001 L
S
8.1999 51.3999 m
80.6999 51.3999 L
S
8.1999 65.8 m
80.6999 65.8 L
S
8.1999 15.3999 m
80.6999 15.3999 L
S
8.1999 29.8 m
80.6999 29.8 L
S
8.1999 44.1999 m
80.6999 44.1999 L
S
8.1999 58.6 m
80.6999 58.6 L
S
8.1999 73.0001 m
80.6999 73.0001 L
S
) &
] E
%AI3_EndPattern
%AI5_End_NonPrinting--
%AI5_Begin_NonPrinting
Np
3 Bn
%AI5_BeginGradient: (Jaune-bleu radial)
(Jaune-bleu radial) 1 2 Bd
[
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
000102030405060708090A0B0C0D0E031415161718191A1B1C1D1E1324252627
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
28292A2B2C2D2E233435363738393A3B3C3D3E334445464748494A4B4C4D4E4F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
505152535455565758595A5B5C5D5E536465666768696A6B6C6D6E6374757677
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
78797A7B7C7D7E738485868788898A8B8C8D8E839495969798999A9B9C9D9E9F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
A0A1A2A3A4A5A6A7A8A9AAABACADAEAFB0B1B2B3B4B5B6B7B8B9BABBBCBDBEBFC0C1C2C3C4C5C6C7
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
C8C9CACBCCCDCECFD0D1D2D3D4D5D6D7D8D9DADBDCDDDEDFE0E1E2E3E4E5E6E7E8E9EAEBECEDEEEF
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>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
5E53646465666768696A6B6C6D6E6F637475767778797A7B7B7C7D7E7F808182
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
83848586868788898A8B8C8D8E82939495969798999A9B9C9D9D9E9FA0A1A2A3A4A5A6A7
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
A8A9A9AAABACADAEAFB0B1B2B3B4B4B5B6B7B8B9BABBBCBDBEBFC0C0C1C2C3C4C5C6C7C8C9CACBCB
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
CCCDCECFD0D1D2D3D4D5D6D7D7D8D9DADBDCDDDEDFE0E1E2E2E3E4E5E6E7E8E9EAEBECEDEEEEEFF0
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>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
ABAAAAA9A8A7A7A6A5A5A4A3A3A2A1A1A09F9F9E9D9D9C9B9B9797969595949393929191
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
908F8F8E8D8D8C8B8B8787868585848383828181807F7F7E7D7D7C7B7B777776
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
7575747373727171706F6F6E6D6D6C6B6B6767666565646362626160605F5E5E5D5C5C5B
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
5A5756565554545352525150504F4E4E4D4C4C4B4A4746464544444342424140
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
403F3E3E3D3C3C3B3A3736363534343332323130302F2E2E2D2C2C2B2A272626
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
25242423222121201F1F1E1D1D1C1B1B1717161515141313121111100F0F0E0D0D0C0B0B
070706050504030302010100
>
0
1 %_Br
[
0 0.08 0.67 0 1 50 14 %_Bs
1 1 0 0 1 50 100 %_Bs
BD
%AI5_EndGradient
%AI5_BeginGradient: (Noir-blanc)
(Noir-blanc) 0 2 Bd
[
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
FFFEFDFCFBFAF9F8F7F6F5F4F3F2F1F0EFEEEDECEBEAE9E8E7E6E5E4E3E2E1E0DFDEDDDCDBDAD9D8
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
D7D6D5D4D3D2D1D0CFCECDCCCBCAC9C8C7C6C5C4C3C2C1C0BFBEBDBCBBBAB9B8B7B6B5B4B3B2B1B0
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
AFAEADACABAAA9A8A7A6A5A4A3A2A1A09F9E9D9C9B969594939291908F8E8D8C8B8A8988
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
87868584838281807F7E7D7C7B767574737271706F6E6D6C6B66656463626160
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
5F5E5D5C5B565554535251504F4E4D4C4B464544434241403F3E3D3C3B3A3938
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
37363534333231302F2E2D2C2B262524232221201F1E1D1C1B16151413121110
0F0E0D0C0B06050403020100
>
0 %_Br
[
0 0 50 100 %_Bs
1 0 50 0 %_Bs
BD
%AI5_EndGradient
%AI5_BeginGradient: (Rouge-jaune)
(Rouge-jaune) 0 2 Bd
[
0
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
000102030405060708090A0B0C0D0E031415161718191A1B1C1D1E1324252627
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
28292A2B2C2D2E233435363738393A3B3C3D3E334445464748494A4B4C4D4E4F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
505152535455565758595A5B5C5D5E536465666768696A6B6C6D6E6374757677
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
78797A7B7C7D7E738485868788898A8B8C8D8E839495969798999A9B9C9D9E9F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
A0A1A2A3A4A5A6A7A8A9AAABACADAEAFB0B1B2B3B4B5B6B7B8B9BABBBCBDBEBFC0C1C2C3C4C5C6C7
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
C8C9CACBCCCDCECFD0D1D2D3D4D5D6D7D8D9DADBDCDDDEDFE0E1E2E3E4E5E6E7E8E9EAEBECEDEEEF
F0F1F2F3F4F5F6F7F8F9FAFBFCFDFEFF
>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
FFFFFEFEFDFDFDFCFCFBFBFBFAFAF9F9F9F8F8F7F7F7F6F6F5F5F5F4F4F3F3F3F2F2F1F1F1F0F0EF
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
EFEFEEEEEDEDEDECECEBEBEBEAEAE9E9E9E8E8E7E7E7E6E6E5E5E5E4E4E3E3E3E2E2E1E1E1E0E0DF
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
DFDFDEDEDDDDDDDCDCDBDBDBDADAD9D9D9D8D8D7D7D7D6D6D5D5D5D4D4D3D3D3D2D2D1D1D1D0D0CF
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
CFCFCECECDCDCDCCCCCBCBCBCACAC9C9C9C8C8C7C7C7C6C6C5C5C5C4C4C3C3C3C2C2C1C1C1C0C0BF
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
BFBFBEBEBDBDBDBCBCBBBBBBBABAB9B9B9B8B8B7B7B7B6B6B5B5B5B4B4B3B3B3B2B2B1B1B1B0B0AF
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
AFAFAEAEADADADACACABABABAAAAA9A9A9A8A8A7A7A7A6A6A5A5A5A4A4A3A3A3A2A2A1A1A1A0A09F
9F9F9E9E9D9D9D9C9C9B9B9B9A9A9999
>
0
1 %_Br
[
0 1 0.6 0 1 50 100 %_Bs
0 0 1 0 1 50 0 %_Bs
BD
%AI5_EndGradient
%AI5_End_NonPrinting--
%AI5_BeginPalette
0 2 Pb
Pn
Pc
1 g
Pc
0 g
Pc
0 0 0 0 k
Pc
0.75 g
Pc
0.5 g
Pc
0.25 g
Pc
0 g
Pc
Bb
2 (Noir-blanc) -4111 4724.6667 0 0 1 0 0 1 0 0 Bg
0 BB
Pc
0.25 0 0 0 k
Pc
0.5 0 0 0 k
Pc
0.75 0 0 0 k
Pc
1 0 0 0 k
Pc
0.25 0.25 0 0 k
Pc
0.5 0.5 0 0 k
Pc
0.75 0.75 0 0 k
Pc
1 1 0 0 k
Pc
Bb
2 (Rouge-jaune) -4111 4724.6667 0 0 1 0 0 1 0 0 Bg
0 BB
Pc
0 0.25 0 0 k
Pc
0 0.5 0 0 k
Pc
0 0.75 0 0 k
Pc
0 1 0 0 k
Pc
0 0.25 0.25 0 k
Pc
0 0.5 0.5 0 k
Pc
0 0.75 0.75 0 k
Pc
0 1 1 0 k
Pc
Bb
0 0 0 0 Bh
2 (Jaune-bleu radial) -4111 4724.6667 0 0 1 0 0 1 0 0 Bg
0 BB
Pc
0 0 0.25 0 k
Pc
0 0 0.5 0 k
Pc
0 0 0.75 0 k
Pc
0 0 1 0 k
Pc
0.25 0 0.25 0 k
Pc
0.5 0 0.5 0 k
Pc
0.75 0 0.75 0 k
Pc
1 0 1 0 k
Pc
(Bandes jaunes) 0 0 1 1 0 0 0 0 0 [1 0 0 1 0 0] p
Pc
0.25 0.125 0 0 k
Pc
0.5 0.25 0 0 k
Pc
0.75 0.375 0 0 k
Pc
1 0.5 0 0 k
Pc
0.125 0.25 0 0 k
Pc
0.25 0.5 0 0 k
Pc
0.375 0.75 0 0 k
Pc
0.5 1 0 0 k
Pc
0 0 0 0 k
Pc
0 0.25 0.125 0 k
Pc
0 0.5 0.25 0 k
Pc
0 0.75 0.375 0 k
Pc
0 1 0.5 0 k
Pc
0 0.125 0.25 0 k
Pc
0 0.25 0.5 0 k
Pc
0 0.375 0.75 0 k
Pc
0 0.5 1 0 k
Pc
0 0 0 0 k
Pc
0.125 0 0.25 0 k
Pc
0.25 0 0.5 0 k
Pc
0.375 0 0.75 0 k
Pc
0.5 0 1 0 k
Pc
0.25 0 0.125 0 k
Pc
0.5 0 0.25 0 k
Pc
0.75 0 0.375 0 k
Pc
1 0 0.5 0 k
Pc
0 0 0 0 k
Pc
0.25 0.125 0.125 0 k
Pc
0.5 0.25 0.25 0 k
Pc
0.75 0.375 0.375 0 k
Pc
1 0.5 0.5 0 k
Pc
0.25 0.25 0.125 0 k
Pc
0.5 0.5 0.25 0 k
Pc
0.75 0.75 0.375 0 k
Pc
1 1 0.5 0 k
Pc
0 0 0 0 k
Pc
0.125 0.25 0.125 0 k
Pc
0.25 0.5 0.25 0 k
Pc
0.375 0.75 0.375 0 k
Pc
0.5 1 0.5 0 k
Pc
0.125 0.25 0.25 0 k
Pc
0.25 0.5 0.5 0 k
Pc
0.375 0.75 0.75 0 k
Pc
0.5 1 1 0 k
Pc
0 0 0 0 k
Pc
0.125 0.125 0.25 0 k
Pc
0.25 0.25 0.5 0 k
Pc
0.375 0.375 0.75 0 k
Pc
0.5 0.5 1 0 k
Pc
0.25 0.125 0.25 0 k
Pc
0.5 0.25 0.5 0 k
Pc
0.75 0.375 0.75 0 k
Pc
1 0.5 1 0 k
Pc
PB
%AI5_EndPalette
%%EndSetup
%AI5_BeginLayer
1 1 1 1 0 0 0 79 128 255 Lb
(Calque 1) Ln
0 A
0 R
0 G
800 Ar
0 J 0 j 0.5 w 4 M []0 d
%AI3_Note:
0 D
380.25 581.6667 m
380.25 790.9167 L
41.5 790.9167 L
41.5 581.6667 L
380.25 581.6667 L
s
1 w
4530 595.6667 m
(N) *
-4110 595.6667 m
(N) *
4530 610.6667 m
(N) *
-4110 610.6667 m
(N) *
4530 625.1667 m
(N) *
-4110 625.1667 m
(N) *
4530 582.1667 m
(N) *
-4110 582.1667 m
(N) *
0 R
0 G
0.5 w
49.6459 595.6667 m
41.3125 595.6667 l
S
97 590.1667 m
97 581.8333 l
S
153.6667 590.1667 m
153.6667 581.8333 l
S
210.3333 590.1667 m
210.3333 581.8333 l
S
267 590.1667 m
267 581.8333 l
S
323.6667 590.1667 m
323.6667 581.8333 l
S
380.3334 590.1667 m
380.3334 581.8333 l
S
49.6459 610.6667 m
41.3125 610.6667 l
S
53.6667 625.6667 m
41.3125 625.6667 l
S
49.6459 640.6667 m
41.3125 640.6667 l
S
53.6667 655.6667 m
41.3125 655.6667 l
S
49.6459 670.6667 m
41.3125 670.6667 l
S
49.6459 685.6667 m
41.3125 685.6667 l
S
49.6459 700.6667 m
41.3125 700.6667 l
S
49.6459 715.6667 m
41.3125 715.6667 l
S
53.6667 730.6667 m
41.3125 730.6667 l
S
49.6459 745.6667 m
41.3125 745.6667 l
S
49.6459 760.6667 m
41.3125 760.6667 l
S
49.6459 775.6667 m
41.3125 775.6667 l
S
1 w
95 -3915.3333 m
(N) *
95 4724.6667 m
(N) *
151.6667 -3915.3333 m
(N) *
151.6667 4724.6667 m
(N) *
325 -3915.3333 m
(N) *
325 4724.6667 m
(N) *
0 To
1 0 0 1 15.8889 582 0 Tp
TP
0 Tr
0 O
0 g
/_Helvetica 14 Tf
0 Ts
100 Tz
0 Tt
0 TA
0 0 5 TC
100 100 200 TW
0 0 0 Ti
0 Ta
0 0 2 2 3 Th
0 Tq
0 0 Tl
0 Tc
0 Tw
(9.4) Tx
(\r) TX
TO
0 To
1 0 0 1 31 565.4167 0 Tp
TP
0 Tr
(0.1) Tx
(\r) TX
TO
0 To
1 0 0 1 143.5 565.4167 0 Tp
TP
0 Tr
(0.3) Tx
(\r) TX
TO
0 To
1 0 0 1 258.5 565.4167 0 Tp
TP
0 Tr
(0.5) Tx
(\r) TX
TO
0 To
1 0 0 1 15.8889 650.6667 0 Tp
TP
0 Tr
(9.5) Tx
(\r) TX
TO
0 To
1 0 0 1 15.8889 724 0 Tp
TP
0 Tr
(9.6) Tx
(\r) TX
TO
0 To
1 0 0 1 0 773 0 Tp
TP
0 Tr
([GeV]) Tx
(\r) TX
TO
0 To
1 0 0 1 334 565.4167 0 Tp
TP
0 Tr
/_Symbol 14 Tf
(t) Tx
/_Helvetica 14 Tf
( [GeV) Tx
/_Helvetica 3 Tf
( ) Tx
/_Helvetica 10 Tf
6 Ts
(\320\62) Tx
/_Helvetica 14 Tf
0 Ts
(]) Tx
(\r) TX
TO
0 To
1 0 0 1 323.75 70.2813 0 Tp
TP
0 Tr
/_Symbol 14 Tf
(t) Tx
/_Helvetica 14 Tf
( [GeV) Tx
/_Helvetica 3 Tf
( ) Tx
/_Helvetica 10 Tf
6 Ts
(\320\62) Tx
/_Helvetica 14 Tf
0 Ts
(]) Tx
(\r) TX
TO
0 R
0 G
0.5 w
380.6667 342.0833 m
380.6667 536.1458 L
41.9167 536.1458 L
41.9167 342.0833 L
380.6667 342.0833 L
s
50.0625 356.0833 m
41.7292 356.0833 l
S
97.4167 350.5833 m
97.4167 342.25 l
S
154.0833 350.5833 m
154.0833 342.25 l
S
210.75 350.5833 m
210.75 342.25 l
S
267.4167 350.5833 m
267.4167 342.25 l
S
380.75 350.5833 m
380.75 342.25 l
S
50.0625 371.0833 m
41.7292 371.0833 l
S
50.0625 386.0833 m
41.7292 386.0833 l
S
50.0625 401.0833 m
41.7292 401.0833 l
S
50.0625 431.0833 m
41.7292 431.0833 l
S
50.0625 416.1458 m
41.7292 416.1458 l
S
50.0625 446.0833 m
41.7292 446.0833 l
S
50.0625 461.0833 m
41.7292 461.0833 l
S
50.0625 476.0833 m
41.7292 476.0833 l
S
54.0833 491.0833 m
41.7292 491.0833 l
S
50.0625 506.0833 m
41.7292 506.0833 l
S
50.0625 521.0833 m
41.7292 521.0833 l
S
50.0625 536.0833 m
41.7292 536.0833 l
S
0 To
1 0 0 1 16.3056 341.4167 0 Tp
TP
0 Tr
0 O
0 g
1 w
(9.4) Tx
(\r) TX
TO
0 To
1 0 0 1 33.4167 326.1042 0 Tp
TP
0 Tr
(23) Tx
(\r) TX
TO
0 To
1 0 0 1 145.9167 326.1042 0 Tp
TP
0 Tr
(25) Tx
(\r) TX
TO
0 To
1 0 0 1 260.9167 326.1042 0 Tp
TP
0 Tr
(27) Tx
(\r) TX
TO
0 To
1 0 0 1 16.3056 484.4167 0 Tp
TP
0 Tr
(9.5) Tx
(\r) TX
TO
0 To
1 0 0 1 0.4167 525.4167 0 Tp
TP
0 Tr
([GeV]) Tx
(\r) TX
TO
0 R
0 G
322.5 694.1667 m
S
41 745.1667 m
S
41.6667 730.3333 m
90.714 596.6459 191.5427 615.0084 280.6452 655.9865 c
S
42 744.4375 m
90.8885 611.1829 191.2237 628.9952 280.1127 669.6934 c
S
41.9583 715.25 m
90.9445 581.729 191.5836 599.8795 280.6042 640.7503 c
S
0 O
0 g
0.6 w 10 M
51.5 628.9077 m
60.7161 625.9119 l
51.5 622.9167 l
54.0344 625.9119 l
51.5 628.9077 l
b
0.5 w 4 M
53.6667 431.4167 m
41.3125 431.4167 l
S
0 O
0 g
0.6 w 10 M
51.5 434.6577 m
60.7161 431.6619 l
51.5 428.6667 l
54.0344 431.6619 l
51.5 434.6577 l
b
u
0 To
1 0 0 1 343.5 766.3333 0 Tp
TP
0 Tr
1 w 4 M
(R) Tx
/_Helvetica 10 Tf
6 Ts
(b) Tx
(\r) TX
TO
0 To
1 0 0 1 354.5 755.1667 0 Tp
TP
0 Tr
/_Symbol 12 Tf
7 0 Tl
(t) Tx
(\r) TX
TO
U
u
0 To
1 0 0 1 343 513.6667 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
0 Ts
0 0 Tl
(R) Tx
/_Helvetica 10 Tf
6 Ts
(b) Tx
(\r) TX
TO
0 To
1 0 0 1 354 502.5 0 Tp
TP
0 Tr
/_Helvetica 12 Tf
7 0 Tl
(n) Tx
( ) Tx
(\r) TX
TO
U
u
0 To
1 0 0 1 280.3333 686.7084 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
(m) Tx
/_Helvetica 10 Tf
2 Ts
(b) Tx
/_Helvetica 14 Tf
6 Ts
( \(M) Tx
/_Helvetica 10 Tf
2 Ts
(b) Tx
/_Helvetica 14 Tf
6 Ts
(\) [GeV]) Tx
(\r) TX
TO
0 R
0 G
0.3 w
281.3333 702.7084 m
290.3333 702.7084 l
B
U
1 w
322.5 472.8334 m
S
u
0 To
1 0 0 1 280.3333 465.375 0 Tp
TP
0 Tr
0 O
0 g
(m) Tx
/_Helvetica 10 Tf
2 Ts
(b) Tx
/_Helvetica 14 Tf
6 Ts
( \(M) Tx
/_Helvetica 10 Tf
2 Ts
(b) Tx
/_Helvetica 14 Tf
6 Ts
(\) [GeV]) Tx
(\r) TX
TO
0 R
0 G
0.3 w
281.3333 481.375 m
290.3333 481.375 l
B
U
1 w
325.1667 208.7917 m
S
u
0 To
1 0 0 1 283 201.3334 0 Tp
TP
0 Tr
0 O
0 g
(m) Tx
/_Helvetica 10 Tf
2 Ts
(c) Tx
/_Helvetica 14 Tf
6 Ts
( \(M) Tx
/_Helvetica 10 Tf
2 Ts
(c) Tx
/_Helvetica 14 Tf
6 Ts
(\) [GeV]) Tx
(\r) TX
TO
0 R
0 G
0.3 w
284 217.3334 m
293 217.3334 l
B
U
0 To
1 0 0 1 298.3333 663.1667 0 Tp
TP
0 Tr
1 w
(4.24) Tx
(\r) TX
TO
0 To
1 0 0 1 298.3333 646.1667 0 Tp
TP
0 Tr
(4.23) Tx
(\r) TX
TO
0 To
1 0 0 1 298.3333 628.6667 0 Tp
TP
0 Tr
(4.22) Tx
(\r) TX
TO
0 To
1 0 0 1 284.6666 437.3333 0 Tp
TP
0 Tr
(4.23) Tx
(\r) TX
TO
0 To
1 0 0 1 284.6666 407.3333 0 Tp
TP
0 Tr
(4.22) Tx
(\r) TX
TO
0 To
1 0 0 1 15.5 616.6667 0 Tp
TP
0 Tr
(M) Tx
/_Symbol 10 Tf
2 Ts
(U) Tx
(\r) TX
TO
0 To
1 0 0 1 15.5 422.6667 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
6 Ts
(M) Tx
/_Symbol 10 Tf
2 Ts
(U) Tx
(\r) TX
TO
0 To
1 0 0 1 308.5 326.1042 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
0 Ts
0 0 Tl
(n) Tx
(\r) TX
TO
0 R
0 G
41.5 450.6875 m
70 448.3333 262 448 268 449 c
S
41.8542 419.8958 m
81.3333 414.3333 247.8031 414.7832 268.3542 418.2083 c
S
0.5 w
380.1667 86.5833 m
380.1667 280.6458 L
41.4167 280.6458 L
41.4167 86.5833 L
380.1667 86.5833 L
s
49.5625 100.5833 m
41.2292 100.5833 l
S
96.9167 95.0833 m
96.9167 86.75 l
S
153.5833 95.0833 m
153.5833 86.75 l
S
210.25 95.0833 m
210.25 86.75 l
S
266.9167 95.0833 m
266.9167 86.75 l
S
380.25 95.0833 m
380.25 86.75 l
S
49.5625 115.5833 m
41.2292 115.5833 l
S
49.5625 130.5833 m
41.2292 130.5833 l
S
49.5625 145.5833 m
41.2292 145.5833 l
S
49.5625 160.6458 m
41.2292 160.6458 l
S
49.5625 190.5833 m
41.2292 190.5833 l
S
49.0625 175.9375 m
40.7292 175.9375 l
S
49.5625 205.5833 m
41.2292 205.5833 l
S
49.5625 220.5833 m
41.2292 220.5833 l
S
53.5833 235.5833 m
41.2292 235.5833 l
S
49.5625 250.5833 m
41.2292 250.5833 l
S
49.5625 265.5833 m
41.2292 265.5833 l
S
49.5625 280.5833 m
41.2292 280.5833 l
S
0 To
1 0 0 1 15.8056 85.9167 0 Tp
TP
0 Tr
0 O
0 g
1 w
(3.0) Tx
(\r) TX
TO
0 To
1 0 0 1 30.9167 70.2813 0 Tp
TP
0 Tr
(0.3) Tx
(\r) TX
TO
0 To
1 0 0 1 143.4167 70.2813 0 Tp
TP
0 Tr
(0.5) Tx
(\r) TX
TO
0 To
1 0 0 1 258.4167 70.2813 0 Tp
TP
0 Tr
(0.7) Tx
(\r) TX
TO
0 To
1 0 0 1 15.8056 228.9167 0 Tp
TP
0 Tr
(3.2) Tx
(\r) TX
TO
0 To
1 0 0 1 -0.0833 269.9167 0 Tp
TP
0 Tr
([GeV]) Tx
(\r) TX
TO
u
0 R
0 G
0.5 w
53.875 155.0209 m
41.5208 155.0209 l
S
0 O
0 g
0.6 w 10 M
52.3333 158.3244 m
61.5494 155.3286 l
52.3333 152.3333 l
54.8678 155.3286 l
52.3333 158.3244 l
b
U
u
0 To
1 0 0 1 342.5 258.1667 0 Tp
TP
0 Tr
1 w 4 M
(R) Tx
/_Helvetica 10 Tf
6 Ts
(c) Tx
(\r) TX
TO
0 To
1 0 0 1 353.5 247 0 Tp
TP
0 Tr
/_Symbol 12 Tf
7 0 Tl
(t ) Tx
/_Helvetica 12 Tf
( ) Tx
(\r) TX
TO
U
0 To
1 0 0 1 284.6666 166 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
(1.23) Tx
(\r) TX
TO
0 To
1 0 0 1 284.6666 150.6667 0 Tp
TP
0 Tr
(1.22) Tx
(\r) TX
TO
0 To
1 0 0 1 15 146.1667 0 Tp
TP
0 Tr
(M) Tx
/_Symbol 10 Tf
2 Ts
(y) Tx
(\r) TX
TO
0 R
0 G
43 181.3333 m
101.5258 139.6515 191.3498 141.7382 279.645 161.4287 c
S
41.5 199.3542 m
101.6103 151.6305 207.0904 159.2117 280.4034 174.3267 c
S
0 To
1 0 0 1 210 762.7083 0 Tp
TP
0 Tr
0 O
0 g
/_Helvetica 14 Tf
0 Ts
0 0 Tl
(a\)) Tx
(\r) TX
TO
0 To
1 0 0 1 210 504.7083 0 Tp
TP
0 Tr
(b\)) Tx
(\r) TX
TO
0 To
1 0 0 1 210 246.7083 0 Tp
TP
0 Tr
(c\)) Tx
/_Helvetica 16 Tf
( ) Tx
(\r) TX
TO
0 To
1 0 0 1 172.6667 36.6667 0 Tp
TP
0 Tr
/_Helvetica 14 Tf
(Fig. 1) Tx
(\r) TX
TO
295.6667 4724.6667 m
295.6667 -3915.3333 L
(N) *
280.3333 4724.6667 m
280.3333 -3915.3333 L
(N) *
LB
%AI5_EndLayer--
%%PageTrailer
gsave annotatepage grestore showpage
%%Trailer
Adobe_IllustratorA_AI5 /terminate get exec
Adobe_typography_AI5 /terminate get exec
Adobe_level2_AI5 /terminate get exec
%%EOF
%!PS-Adobe-3.0 EPSF-3.0
%%Creator: Adobe Illustrator(TM) 5.0
%%For: (Marinette) (CERN)
%%Title: (Narison Fig.2 -3 eps)
%%CreationDate: (8/23/94) (4:45 PM)
%%BoundingBox: -475 -258 -119 475
%%HiResBoundingBox: -474.4115 -258.4747 -119.6719 475.4729
%%DocumentProcessColors: Black
%%DocumentFonts: Helvetica
%%+ Symbol
%%DocumentSuppliedResources: procset Adobe_level2_AI5 1.0 0
%%+ procset Adobe_typography_AI5 1.0 0
%%+ procset Adobe_IllustratorA_AI5 1.0 0
%AI5_FileFormat 1.1
%AI3_ColorUsage: Black&White
%AI3_TemplateBox: -298 116.5 -298 116.5
%AI3_TileBox: -580 -271.5 -42 509.5
%AI3_DocumentPreview: Header
%AI5_ArtSize: 1296 1296
%AI5_RulerUnits: 1
%AI5_ArtFlags: 0 0 0 1 0 0
%AI5_TargetResolution: 800
%AI5_NumLayers: 1
%AI5_OpenToView: -562 -115.5 3 1146 827 18 1 1 3 40
%AI5_OpenViewLayers: 7
%%EndComments
%%BeginProlog
%%BeginResource: procset Adobe_level2_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Level 2 Emulation)
%%Version: 1.0
%%CreationDate: (04/10/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
userdict /Adobe_level2_AI5 21 dict dup begin
	put
	/packedarray where not
	{
		userdict begin
		/packedarray
		{
			array astore readonly
		} bind def
		/setpacking /pop load def
		/currentpacking false def
	 end
		0
	} if
	pop
	userdict /defaultpacking currentpacking put true setpacking
	/initialize
	{
		Adobe_level2_AI5 begin
	} bind def
	/terminate
	{
		currentdict Adobe_level2_AI5 eq
		{
		 end
		} if
	} bind def
	mark
	/setcustomcolor where not
	{
		/findcmykcustomcolor
		{
			5 packedarray
		} bind def
		/setcustomcolor
		{
			exch aload pop pop
			4
			{
				4 index mul 4 1 roll
			} repeat
			5 -1 roll pop
			setcmykcolor
		}
		def
	} if
	/gt38? version cvx exec 38 gt def
	userdict /deviceDPI 72 0 matrix defaultmatrix dtransform dup mul exch dup mul
a
	userdict /level2?
	systemdict /languagelevel known dup
	{
		pop systemdict /languagelevel get 2 ge
	} if
	put
	level2? not
	{
		/setcmykcolor where not
		{
			/setcmykcolor
			{
				exch .11 mul add exch .59 mul add exch .3 mul add
				1 exch sub setgray
			} def
		} if
		/currentcmykcolor where not
		{
			/currentcmykcolor
			{
				0 0 0 1 currentgray sub
			} def
		} if
		/setoverprint where not
		{
			/setoverprint /pop load def
		} if
		/selectfont where not
		{
			/selectfont
			{
				exch findfont exch
				dup type /arraytype eq
				{
					makefont
				}
				{
					scalefont
				} ifelse
				setfont
			} bind def
		} if
		/cshow where not
		{
			/cshow
			{
				[
				0 0 5 -1 roll aload pop
				] cvx bind forall
			} bind def
		} if
	} if
	cleartomark
	/anyColor?
	{
		add add add 0 ne
	} bind def
	/testColor
	{
		gsave
		setcmykcolor currentcmykcolor
		grestore
	} bind def
	/testCMYKColorThrough
	{
		testColor anyColor?
	} bind def
	userdict /composite?
	level2?
	{
		gsave 1 1 1 1 setcmykcolor currentcmykcolor grestore
		add add add 4 eq
	}
	{
		1 0 0 0 testCMYKColorThrough
		0 1 0 0 testCMYKColorThrough
		0 0 1 0 testCMYKColorThrough
		0 0 0 1 testCMYKColorThrough
		and and and
	} ifelse
	put
	composite? not
	{
		userdict begin
		gsave
		/cyan? 1 0 0 0 testCMYKColorThrough def
		/magenta? 0 1 0 0 testCMYKColorThrough def
		/yellow? 0 0 1 0 testCMYKColorThrough def
		/black? 0 0 0 1 testCMYKColorThrough def
		grestore
		/isCMYKSep? cyan? magenta? yellow? black? or or or def
		/customColor? isCMYKSep? not def
	 end
	} if
 end defaultpacking setpacking
%%EndResource
%%BeginResource: procset Adobe_typography_AI5 1.0 0
%%Title: (Typography Operators)
%%Version: 1.0
%%CreationDate:(03/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_typography_AI5 48 dict dup begin
put
/initialize
{
 begin
 begin
	Adobe_typography_AI5 begin
	Adobe_typography_AI5
	{
		dup xcheck
		{
			bind
		} if
		pop pop
	} forall
 end
 end
 end
	Adobe_typography_AI5 begin
} def
/terminate
{
	currentdict Adobe_typography_AI5 eq
	{
	 end
	} if
} def
/modifyEncoding
{
	/_tempEncode exch ddef
	/_pntr 0 ddef
	{
		counttomark -1 roll
		dup type dup /marktype eq
		{
			pop pop exit
		}
		{
			/nametype eq
			{
				_tempEncode /_pntr dup load dup 3 1 roll 1 add ddef 3 -1 roll
				put
			}
			{
				/_pntr exch ddef
			} ifelse
		} ifelse
	} loop
	_tempEncode
} def
/TE
{
	StandardEncoding 256 array copy modifyEncoding
	/_nativeEncoding exch def
} def
%
/TZ
{
	dup type /arraytype eq
	{
		/_wv exch def
	}
	{
		/_wv 0 def
	} ifelse
	/_useNativeEncoding exch def
	pop pop
	findfont _wv type /arraytype eq
	{
		_wv makeblendedfont
	} if
	dup length 2 add dict
 begin
	mark exch
	{
		1 index /FID ne
		{
			def
		} if
		cleartomark mark
	} forall
	pop
	/FontName exch def
	counttomark 0 eq
	{
		1 _useNativeEncoding eq
		{
			/Encoding _nativeEncoding def
		} if
		cleartomark
	}
	{
		/Encoding load 256 array copy
		modifyEncoding /Encoding exch def
	} ifelse
	FontName currentdict
 end
	definefont pop
} def
/tr
{
	_ax _ay 3 2 roll
} def
/trj
{
	_cx _cy _sp _ax _ay 6 5 roll
} def
/a0
{
	/Tx
	{
		dup
		currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
	} ddef
	/Tj
	{
		dup
		currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
	} ddef
} def
/a1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/e0
{
	/Tx
	{
		tr _psf
	} ddef
	/Tj
	{
		trj _pjsf
	} ddef
} def
/e1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		tr _psf
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		trj _pjsf
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/i0
{
	/Tx
	{
		tr sp
	} ddef
	/Tj
	{
		trj jsp
	} ddef
} def
/i1
{
	W N
} def
/o0
{
	/Tx
	{
		tr sw rmoveto
	} ddef
	/Tj
	{
		trj swj rmoveto
	} ddef
} def
/r0
{
	/Tx
	{
		tr _ctm _pss
	} ddef
	/Tj
	{
		trj _ctm _pjss
	} ddef
} def
/r1
{
	/Tx
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/To
{
	pop _ctm currentmatrix pop
} def
/TO
{
	iTe _ctm setmatrix newpath
} def
/Tp
{
	pop _tm astore pop _ctm setmatrix
	_tDict begin
	/W
	{
	} def
	/h
	{
	} def
} def
/TP
{
 end
	iTm 0 0 moveto
} def
/Tr
{
	_render 3 le
	{
		currentpoint newpath moveto
	} if
	dup 8 eq
	{
		pop 0
	}
	{
		dup 9 eq
		{
			pop 1
		} if
	} ifelse
	dup /_render exch ddef
	_renderStart exch get load exec
} def
/iTm
{
	_ctm setmatrix _tm concat 0 _rise translate _hs 1 scale
} def
/Tm
{
	_tm astore pop iTm 0 0 moveto
} def
/Td
{
	_mtx translate _tm _tm concatmatrix pop iTm 0 0 moveto
} def
/iTe
{
	_render -1 eq
	{
	}
	{
		_renderEnd _render get dup null ne
		{
			load exec
		}
		{
			pop
		} ifelse
	} ifelse
	/_render -1 ddef
} def
/Ta
{
	pop
} def
/Tf
{
	dup 1000 div /_fScl exch ddef
	exch findfont exch scalefont setfont
} def
/Tl
{
	pop
	0 exch _leading astore pop
} def
/Tt
{
	pop
} def
/TW
{
	3 npop
} def
/Tw
{
	/_cx exch ddef
} def
/TC
{
	3 npop
} def
/Tc
{
	/_ax exch ddef
} def
/Ts
{
	/_rise exch ddef
	currentpoint
	iTm
	moveto
} def
/Ti
{
	3 npop
} def
/Tz
{
	100 div /_hs exch ddef
	iTm
} def
/TA
{
	pop
} def
/Tq
{
	pop
} def
/Th
{
	pop pop pop pop pop
} def
/TX
{
	pop
} def
/Tk
{
	exch pop _fScl mul neg 0 rmoveto
} def
/TK
{
	2 npop
} def
/T*
{
	_leading aload pop neg Td
} def
/T*-
{
	_leading aload pop Td
} def
/T-
{
	_hyphen Tx
} def
/T+
{
} def
/TR
{
	_ctm currentmatrix pop
	_tm astore pop
	iTm 0 0 moveto
} def
/TS
{
	0 eq
	{
		Tx
	}
	{
		Tj
	} ifelse
} def
currentdict readonly pop
end
setpacking
%%EndResource
%%BeginResource: procset Adobe_IllustratorA_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Abbreviated Prolog)
%%Version: 1.0
%%CreationDate: (3/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_IllustratorA_AI5_vars 70 dict dup begin
put
/_lp /none def
/_pf
{
} def
/_ps
{
} def
/_psf
{
} def
/_pss
{
} def
/_pjsf
{
} def
/_pjss
{
} def
/_pola 0 def
/_doClip 0 def
/cf currentflat def
/_tm matrix def
/_renderStart
[
/e0 /r0 /a0 /o0 /e1 /r1 /a1 /i0
] def
/_renderEnd
[
null null null null /i1 /i1 /i1 /i1
] def
/_render -1 def
/_rise 0 def
/_ax 0 def
/_ay 0 def
/_cx 0 def
/_cy 0 def
/_leading
[
0 0
] def
/_ctm matrix def
/_mtx matrix def
/_sp 16#020 def
/_hyphen (-) def
/_fScl 0 def
/_cnt 0 def
/_hs 1 def
/_nativeEncoding 0 def
/_useNativeEncoding 0 def
/_tempEncode 0 def
/_pntr 0 def
/_tDict 2 dict def
/_wv 0 def
/Tx
{
} def
/Tj
{
} def
/CRender
{
} def
/_AI3_savepage
{
} def
/_gf null def
/_cf 4 array def
/_if null def
/_of false def
/_fc
{
} def
/_gs null def
/_cs 4 array def
/_is null def
/_os false def
/_sc
{
} def
/discardSave null def
/buffer 256 string def
/beginString null def
/endString null def
/endStringLength null def
/layerCnt 1 def
/layerCount 1 def
/perCent (%) 0 get def
/perCentSeen? false def
/newBuff null def
/newBuffButFirst null def
/newBuffLast null def
/clipForward? false def
end
userdict /Adobe_IllustratorA_AI5 74 dict dup begin
put
/initialize
{
	Adobe_IllustratorA_AI5 dup begin
	Adobe_IllustratorA_AI5_vars begin
	discardDict
	{
		bind pop pop
	} forall
	dup /nc get begin
	{
		dup xcheck 1 index type /operatortype ne and
		{
			bind
		} if
		pop pop
	} forall
 end
	newpath
} def
/terminate
{
 end
 end
} def
/_
null def
/ddef
{
	Adobe_IllustratorA_AI5_vars 3 1 roll put
} def
/xput
{
	dup load dup length exch maxlength eq
	{
		dup dup load dup
		length 2 mul dict copy def
	} if
	load begin
	def
 end
} def
/npop
{
	{
		pop
	} repeat
} def
/sw
{
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
} def
/swj
{
	dup 4 1 roll
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
	6 2 roll /_cnt 0 ddef
	{
		1 index eq
		{
			/_cnt _cnt 1 add ddef
		} if
	} forall
	pop
	exch _cnt mul exch _cnt mul 2 index add 4 1 roll 2 index add 4 1 roll pop pop
} def
/ss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put pop
		gsave
		false charpath currentpoint
		4 index setmatrix
		stroke
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	3 npop
} def
/jss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put
		gsave
		_sp eq
		{
			exch 6 index 6 index 6 index 5 -1 roll widthshow
			currentpoint
		}
		{
			false charpath currentpoint
			4 index setmatrix stroke
		} ifelse
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	6 npop
} def
/sp
{
	{
		2 npop (0) exch
		2 copy 0 exch put pop
		false charpath
		2 copy rmoveto
	} exch cshow
	2 npop
} def
/jsp
{
	{
		2 npop
		(0) exch 2 copy 0 exch put
		_sp eq
		{
			exch 5 index 5 index 5 index 5 -1 roll widthshow
		}
		{
			false charpath
		} ifelse
		2 copy rmoveto
	} exch cshow
	5 npop
} def
/pl
{
	transform
	0.25 sub round 0.25 add exch
	0.25 sub round 0.25 add exch
	itransform
} def
/setstrokeadjust where
{
	pop true setstrokeadjust
	/c
	{
		curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll curveto
	} def
	/V
	/v load def
	/y
	{
		2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		lineto
	} def
	/L
	/l load def
	/m
	{
		moveto
	} def
}
{
	/c
	{
		pl curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll pl curveto
	} def
	/V
	/v load def
	/y
	{
		pl 2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		pl lineto
	} def
	/L
	/l load def
	/m
	{
		pl moveto
	} def
} ifelse
/d
{
	setdash
} def
/cf
{
} def
/i
{
	dup 0 eq
	{
		pop cf
	} if
	setflat
} def
/j
{
	setlinejoin
} def
/J
{
	setlinecap
} def
/M
{
	setmiterlimit
} def
/w
{
	setlinewidth
} def
/H
{
} def
/h
{
	closepath
} def
/N
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			clip /_doClip 0 ddef
		} if
		newpath
	}
	{
		/CRender
		{
			N
		} ddef
	} ifelse
} def
/n
{
	N
} def
/F
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _pf grestore clip newpath /_lp /none ddef _fc
			/_doClip 0 ddef
		}
		{
			_pf
		} ifelse
	}
	{
		/CRender
		{
			F
		} ddef
	} ifelse
} def
/f
{
	closepath
	F
} def
/S
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _ps grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			_ps
		} ifelse
	}
	{
		/CRender
		{
			S
		} ddef
	} ifelse
} def
/s
{
	closepath
	S
} def
/B
{
	_pola 0 eq
	{
		_doClip 1 eq
		gsave F grestore
		{
			gsave S grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			S
		} ifelse
	}
	{
		/CRender
		{
			B
		} ddef
	} ifelse
} def
/b
{
	closepath
	B
} def
/W
{
	/_doClip 1 ddef
} def
/*
{
	count 0 ne
	{
		dup type /stringtype eq
		{
			pop
		} if
	} if
	_pola 0 eq
	{
		newpath
	} if
} def
/u
{
} def
/U
{
} def
/q
{
	_pola 0 eq
	{
		gsave
	} if
} def
/Q
{
	_pola 0 eq
	{
		grestore
	} if
} def
/*u
{
	_pola 1 add /_pola exch ddef
} def
/*U
{
	_pola 1 sub /_pola exch ddef
	_pola 0 eq
	{
		CRender
	} if
} def
/D
{
	pop
} def
/*w
{
} def
/*W
{
} def
/`
{
	/_i save ddef
	clipForward?
	{
		nulldevice
	} if
	6 1 roll 4 npop
	concat pop
	userdict begin
	/showpage
	{
	} def
	0 setgray
	0 setlinecap
	1 setlinewidth
	0 setlinejoin
	10 setmiterlimit
	[
	] 0 setdash
	newpath
	0 setgray
	false setoverprint
} def
/~
{
 end
	_i restore
} def
/O
{
	0 ne
	/_of exch ddef
	/_lp /none ddef
} def
/R
{
	0 ne
	/_os exch ddef
	/_lp /none ddef
} def
/g
{
	/_gf exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_gf setgray
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/G
{
	/_gs exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_gs setgray
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/k
{
	_cf astore pop
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_cf aload pop setcmykcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/K
{
	_cs astore pop
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_cs aload pop setcmykcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/x
{
	/_gf exch ddef
	findcmykcustomcolor
	/_if exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_if _gf 1 exch sub setcustomcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/X
{
	/_gs exch ddef
	findcmykcustomcolor
	/_is exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_is _gs 1 exch sub setcustomcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/A
{
	pop
} def
/annotatepage
{
userdict /annotatepage 2 copy known {get exec} {pop pop} ifelse
} def
/discard
{
	save /discardSave exch store
	discardDict begin
	/endString exch store
	version cvx exec 38 gt
	{
		2 add
	} if
	load
	stopped
	pop
 end
	discardSave restore
} bind def
userdict /discardDict 7 dict dup begin
put
/pre38Initialize
{
	/endStringLength endString length store
	/newBuff buffer 0 endStringLength getinterval store
	/newBuffButFirst newBuff 1 endStringLength 1 sub getinterval store
	/newBuffLast newBuff endStringLength 1 sub 1 getinterval store
} def
/shiftBuffer
{
	newBuff 0 newBuffButFirst putinterval
	newBuffLast 0
	currentfile read not
	{
	stop
	} if
	put
} def
0
{
	pre38Initialize
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff endString eq
			{
				cleartomark stop
			} if
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
1
{
	pre38Initialize
	/beginString exch store
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff beginString eq
			{
				/layerCount dup load 1 add store
			}
			{
				newBuff endString eq
				{
					/layerCount dup load 1 sub store
					layerCount 0 eq
					{
						cleartomark stop
					} if
				} if
			} ifelse
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
2
{
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		endString eq
		{
			cleartomark stop
		} if
	} loop
} def
3
{
	/beginString exch store
	/layerCnt 1 store
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		dup beginString eq
		{
			pop /layerCnt dup load 1 add store
		}
		{
			endString eq
			{
				layerCnt 1 eq
				{
					cleartomark stop
				}
				{
					/layerCnt dup load 1 sub store
				} ifelse
			} if
		} ifelse
	} loop
} def
end
userdict /clipRenderOff 15 dict dup begin
put
{
	/n /N /s /S /f /F /b /B
}
{
	{
		_doClip 1 eq
		{
			/_doClip 0 ddef clip
		} if
		newpath
	} def
} forall
/Tr /pop load def
/Bb {} def
/BB /pop load def
/Bg {12 npop} def
/Bm {6 npop} def
/Bc /Bm load def
/Bh {4 npop} def
end
/Lb
{
	4 npop
	6 1 roll
	pop
	4 1 roll
	pop pop pop
	0 eq
	{
		0 eq
		{
			(%AI5_BeginLayer) 1 (%AI5_EndLayer--) discard
		}
		{
			/clipForward? true def

			/Tx /pop load def
			/Tj /pop load def
			currentdict end clipRenderOff begin begin
		} ifelse
	}
	{
		0 eq
		{
			save /discardSave exch store
		} if
	} ifelse
} bind def
/LB
{
	discardSave dup null ne
	{
		restore
	}
	{
		pop
		clipForward?
		{
			currentdict
		 end
		 end
		 begin

			/clipForward? false ddef
		} if
	} ifelse
} bind def
/Pb
{
	pop pop
	0 (%AI5_EndPalette) discard
} bind def
/Np
{
	0 (%AI5_End_NonPrinting--) discard
} bind def
/Ln /pop load def
/Ap
/pop load def
/Ar
{
	72 exch div
	0 dtransform dup mul exch dup mul add sqrt
	dup 1 lt
	{
		pop 1
	} if
	setflat
} def
/Mb
{
	q
} def
/Md
{
} def
/MB
{
	Q
} def
/nc 3 dict def
nc begin
/setgray
{
	pop
} bind def
/setcmykcolor
{
	4 npop
} bind def
/setcustomcolor
{
	2 npop
} bind def
currentdict readonly pop
end
currentdict readonly pop
end
setpacking
%%EndResource
%%EndProlog
%%BeginSetup
%%IncludeFont: Helvetica
%%IncludeFont: Symbol
Adobe_level2_AI5 /initialize get exec
Adobe_IllustratorA_AI5_vars Adobe_IllustratorA_AI5 Adobe_typography_AI5
/initial
Adobe_IllustratorA_AI5 /initialize get exec
[
39/quotesingle 96/grave 128/Adieresis/Aring/Ccedilla/Eacute/Ntilde/Odieresis
/Udieresis/aacute/agrave/acircumflex/adieresis/atilde/aring/ccedilla/eacute
/egrave/ecircumflex/edieresis/iacute/igrave/icircumflex/idieresis/ntilde
/oacute/ograve/ocircumflex/odieresis/otilde/uacute/ugrave/ucircumflex
/udieresis/dagger/degree/cent/sterling/section/bullet/paragraph/germandbls
/registered/copyright/trademark/acute/dieresis/.notdef/AE/Oslash
/.notdef/plusminus/.notdef/.notdef/yen/mu/.notdef/.notdef
/.notdef/.notdef/.notdef/ordfeminine/ordmasculine/.notdef/ae/oslash
/questiondown/exclamdown/logicalnot/.notdef/florin/.notdef/.notdef
/guillemotleft/guillemotright/ellipsis/.notdef/Agrave/Atilde/Otilde/OE/oe
/endash/emdash/quotedblleft/quotedblright/quoteleft/quoteright/divide
/.notdef/ydieresis/Ydieresis/fraction/currency/guilsinglleft/guilsinglright
/fi/fl/daggerdbl/periodcentered/quotesinglbase/quotedblbase/perthousand
/Acircumflex/Ecircumflex/Aacute/Edieresis/Egrave/Iacute/Icircumflex
/Idieresis/Igrave/Oacute/Ocircumflex/.notdef/Ograve/Uacute/Ucircumflex
/Ugrave/dotlessi/circumflex/tilde/macron/breve/dotaccent/ring/cedilla
/hungarumlaut/ogonek/caron
TE
%AI3_BeginEncoding: _Helvetica Helvetica
[/_Helvetica/Helvetica 0 0 1 TZ
%AI3_EndEncoding AdobeType
%AI3_BeginEncoding: _Symbol Symbol
[/_Symbol/Symbol 0 0 0 TZ
%AI3_EndEncoding AdobeType
%AI5_Begin_NonPrinting
Np
%AI3_BeginPattern: (Bandes jaunes)
(Bandes jaunes) 8.4499 4.6 80.4499 76.6 [
%AI3_Tile
(0 O 0 R 0 0.4 1 0 k 0 0.4 1 0 K) @
(
800 Ar
0 J 0 j 3.6 w 4 M []0 d
%AI3_Note:
0 D
8.1999 8.1999 m
80.6999 8.1999 L
S
8.1999 22.6 m
80.6999 22.6 L
S
8.1999 37.0001 m
80.6999 37.0001 L
S
8.1999 51.3999 m
80.6999 51.3999 L
S
8.1999 65.8 m
80.6999 65.8 L
S
8.1999 15.3999 m
80.6999 15.3999 L
S
8.1999 29.8 m
80.6999 29.8 L
S
8.1999 44.1999 m
80.6999 44.1999 L
S
8.1999 58.6 m
80.6999 58.6 L
S
8.1999 73.0001 m
80.6999 73.0001 L
S
) &
] E
%AI3_EndPattern
%AI5_End_NonPrinting--
%AI5_Begin_NonPrinting
Np
3 Bn
%AI5_BeginGradient: (Jaune-bleu radial)
(Jaune-bleu radial) 1 2 Bd
[
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
000102030405060708090A0B0C0D0E031415161718191A1B1C1D1E1324252627
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
28292A2B2C2D2E233435363738393A3B3C3D3E334445464748494A4B4C4D4E4F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
505152535455565758595A5B5C5D5E536465666768696A6B6C6D6E6374757677
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
78797A7B7C7D7E738485868788898A8B8C8D8E839495969798999A9B9C9D9E9F
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
A0A1A2A3A4A5A6A7A8A9AAABACADAEAFB0B1B2B3B4B5B6B7B8B9BABBBCBDBEBFC0C1C2C3C4C5C6C7
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
C8C9CACBCCCDCECFD0D1D2D3D4D5D6D7D8D9DADBDCDDDEDFE0E1E2E3E4E5E6E7E8E9EAEBECEDEEEF
F0F1F2F3F4F5F6F7F8F9FAFBFCFDFEFF
>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
1415161718191A1B1C1D1E1F132425262728292A2A2B2C2D2E23343536363738
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
393A3B3C3D3E32434445464748494A4B4C4D4D4E43545556575858595A5B5C5D
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
5E53646465666768696A6B6C6D6E6F637475767778797A7B7B7C7D7E7F808182
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
83848586868788898A8B8C8D8E82939495969798999A9B9C9D9D9E9FA0A1A2A3A4A5A6A7
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
A8A9A9AAABACADAEAFB0B1B2B3B4B4B5B6B7B8B9BABBBCBDBEBFC0C0C1C2C3C4C5C6C7C8C9CACBCB
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
CCCDCECFD0D1D2D3D4D5D6D7D7D8D9DADBDCDDDEDFE0E1E2E2E3E4E5E6E7E8E9EAEBECEDEEEEEFF0
F1F2F3F4F5F6F7F8F9F9FAFBFCFDFEFF
>
<
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-414.9338 102.3462 -298.1333 53.8128 -282.1333 48.4794 C
-268.2665 45.2794 -244.7998 35.6793 -237.8664 31.4127 c
S
0 To
1 0 0 1 -318.9334 -248.3883 0 Tp
TP
0 Tr
0 O
0 g
0 J 1 w []0 d
/_Helvetica 14 Tf
(Fig. 2) Tx
(\r) TX
TO
-4618 -39.5 m
4022 -39.5 L
(N) *
-430 4436.5 m
-430 -4203.5 L
(N) *
0 To
1 0 0 1 -206.999 -214.7878 0 Tp
TP
0 Tr
0 O
0 g
/_Symbol 12.8 Tf
(t) Tx
/_Helvetica 8 Tf
-3.2 Ts
(NR) Tx
/_Helvetica 11.2 Tf
0 Ts
( [GeV) Tx
/_Helvetica 2.4 Tf
( ) Tx
/_Helvetica 8 Tf
4.8 Ts
(\320\61) Tx
/_Helvetica 11.2 Tf
0 Ts
(]) Tx
(\r) TX
TO
0 R
0 G
0.4 w
-419.2748 -144.5784 m
-429.1582 -144.5784 l
S
0 O
0 g
0.48 w 10 M
-421.0081 -141.9856 m
-413.6352 -144.3823 l
-421.0081 -146.7784 l
-418.9806 -144.3823 l
-421.0081 -141.9856 l
b
0 To
1 0 0 1 -449.8082 -151.7785 0 Tp
TP
0 Tr
1 w 4 M
4.8 Ts
5.6 0 Tl
(M) Tx
/_Symbol 8 Tf
1.6 Ts
(y) Tx
(\r) TX
TO
1 Ap
0 R
0 G
0.4 w
-157.9328 -201.5 m
-157.9328 -40.2681 L
-429 -40.2681 L
-429 -201.5 L
-157.9328 -201.5 L
s
0 Ap
-422.4832 -190.321 m
-429.15 -190.321 l
S
-422.3332 -178.7877 m
-429 -178.7877 l
S
-422.1832 -167.2543 m
-428.85 -167.2543 l
S
-422.0332 -155.721 m
-428.7 -155.721 l
S
-418.3332 -144.1877 m
-428.55 -144.1877 l
S
-422.5332 -132.6544 m
-429.2 -132.6544 l
S
-422.3832 -121.121 m
-429.05 -121.121 l
S
-422.2332 -109.5877 m
-428.9 -109.5877 l
S
-422.0832 -98.0544 m
-428.75 -98.0544 l
S
-418.3332 -86.521 m
-428.6 -86.521 l
S
-422.1332 -74.9873 m
-428.8 -74.9873 l
S
-421.9832 -63.4539 m
-428.65 -63.4539 l
S
-421.8332 -51.9206 m
-428.5 -51.9206 l
S
-421.6832 -40.3873 m
-428.35 -40.3873 l
S
-384.5998 -194.721 m
-384.5998 -201.3878 l
S
-339.2663 -194.721 m
-339.2663 -201.3878 l
S
-293.9328 -194.721 m
-293.9328 -201.3878 l
S
-248.5993 -194.721 m
-248.5993 -201.3878 l
S
-203.6657 -194.7044 m
-203.6657 -201.3711 l
S
-157.9322 -194.721 m
-157.9322 -201.3878 l
S
0 To
1 0 0 1 -450.3647 -204.4544 0 Tp
TP
0 Tr
0 O
0 g
1 w
/_Helvetica 11.2 Tf
0 Ts
0 0 Tl
(3.0    ) Tx
(\r) TX
TO
0 To
1 0 0 1 -437.4 -214.7878 0 Tp
TP
0 Tr
(0.4) Tx
(\r) TX
TO
0 To
1 0 0 1 -347.7996 -214.7878 0 Tp
TP
0 Tr
(0.6) Tx
(\r) TX
TO
0 To
1 0 0 1 -255.2659 -214.7878 0 Tp
TP
0 Tr
(0.8) Tx
(\r) TX
TO
0 To
1 0 0 1 -450.3647 -90.054 0 Tp
TP
0 Tr
(3.2) Tx
(\r) TX
TO
0 To
1 0 0 1 -463 -50.9872 0 Tp
TP
0 Tr
([GeV]) Tx
(\r) TX
TO
0 To
1 0 0 1 -190.9991 -214.7878 0 Tp
TP
0 Tr
/_Symbol 12.8 Tf
(   ) Tx
(\r) TX
TO
0 R
0 G
0.8 w
-429.4 -70.7205 m
S
u
0 To
1 0 0 1 -192.3324 -62.9872 0 Tp
TP
0 Tr
0 O
0 g
1 w
/_Helvetica 11.2 Tf
(R) Tx
/_Helvetica 8 Tf
4.8 Ts
(c) Tx
(\r) TX
TO
0 To
1 0 0 1 -184.0656 -68.854 0 Tp
TP
0 Tr
/_Symbol 9.6 Tf
1.6 Ts
5.6 0 Tl
(t) Tx
/_Helvetica 8 Tf
-1.6 Ts
(NR) Tx
(\r) TX
TO
U
u
0 To
1 0 0 1 -215.7991 -107.2541 0 Tp
TP
0 Tr
/_Helvetica 11.2 Tf
4.8 Ts
(M) Tx
/_Helvetica 8 Tf
1.6 Ts
(c) Tx
/_Helvetica 11.2 Tf
4.8 Ts
( [GeV]) Tx
(\r) TX
TO
U
0 To
1 0 0 1 -198.2879 -133.9208 0 Tp
TP
0 Tr
(1.45) Tx
(\r) TX
TO
0 To
1 0 0 1 -198.2879 -145.3876 0 Tp
TP
0 Tr
(1.44) Tx
(\r) TX
TO
0 To
1 0 0 1 -198.2879 -156.8543 0 Tp
TP
0 Tr
(1.43) Tx
(\r) TX
TO
0 To
1 0 0 1 -271.266 -68.5873 0 Tp
TP
0 Tr
0 Ts
0 0 Tl
(c\)) Tx
(\r) TX
TO
0 R
0 G
0.8 w
-429.3999 -56.5872 m
-356.5996 -160.1876 -263.5326 -133.7709 -203.5324 -126.9708 c
S
-428.5999 -64.5872 m
-384.5997 -115.7708 -357.933 -162.721 -204.0657 -136.3209 c
S
-429.3999 -73.6373 m
-407.2665 -88.8374 -395.2664 -176.321 -204.3324 -148.5876 c
S
[5.6 4.8 5.6 4.8 ]0 d
-430.0665 -99.5207 m
-391.3998 -112.5874 -327.9356 -152.8075 -212.4713 -143.7163 c
S
0 To
1 0 0 1 -318.7328 -249.388 0 Tp
TP
0 Tr
0 O
0 g
1 w []0 d
(\r) Tx
TO
LB
%AI5_EndLayer--
%%PageTrailer
gsave annotatepage grestore showpage
%%Trailer
Adobe_IllustratorA_AI5 /terminate get exec
Adobe_typography_AI5 /terminate get exec
Adobe_level2_AI5 /terminate get exec
%%EOF
%!PS-Adobe-3.0 EPSF-3.0
%%Creator: Adobe Illustrator(TM) 5.0
%%For: (Marinette) (CERN)
%%Title: (Narison Fig. 3 -eps)
%%CreationDate: (8/23/94) (4:59 PM)
%%BoundingBox: -16 -68 458 346
%%HiResBoundingBox: -14.5137 -68.1667 457.2466 345.571
%%DocumentProcessColors: Black
%%DocumentFonts: Helvetica
%%DocumentSuppliedResources: procset Adobe_level2_AI5 1.0 0
%%+ procset Adobe_typography_AI5 1.0 0
%%+ procset Adobe_IllustratorA_AI5 1.0 0
%AI5_FileFormat 1.1
%AI3_ColorUsage: Black&White
%AI3_IncludePlacedImages
%AI3_TemplateBox: -5.5 -67.5 510.5 344.5
%AI3_TemplateFile: Marinnette::25325:F3
%AI3_TileBox: -29.5 -249.5 508.5 531.5
%AI3_DocumentPreview: Header
%AI5_ArtSize: 1296 1296
%AI5_RulerUnits: 1
%AI5_ArtFlags: 0 0 0 1 0 0
%AI5_TargetResolution: 800
%AI5_NumLayers: 1
%AI5_OpenToView: 0.5 342.5 2 1146 827 18 0 1 3 40
%AI5_OpenViewLayers: 7
%%EndComments
%%BeginProlog
%%BeginResource: procset Adobe_level2_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Level 2 Emulation)
%%Version: 1.0
%%CreationDate: (04/10/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
userdict /Adobe_level2_AI5 21 dict dup begin
	put
	/packedarray where not
	{
		userdict begin
		/packedarray
		{
			array astore readonly
		} bind def
		/setpacking /pop load def
		/currentpacking false def
	 end
		0
	} if
	pop
	userdict /defaultpacking currentpacking put true setpacking
	/initialize
	{
		Adobe_level2_AI5 begin
	} bind def
	/terminate
	{
		currentdict Adobe_level2_AI5 eq
		{
		 end
		} if
	} bind def
	mark
	/setcustomcolor where not
	{
		/findcmykcustomcolor
		{
			5 packedarray
		} bind def
		/setcustomcolor
		{
			exch aload pop pop
			4
			{
				4 index mul 4 1 roll
			} repeat
			5 -1 roll pop
			setcmykcolor
		}
		def
	} if
	/gt38? version cvx exec 38 gt def
	userdict /deviceDPI 72 0 matrix defaultmatrix dtransform dup mul exch dup mul
a
	userdict /level2?
	systemdict /languagelevel known dup
	{
		pop systemdict /languagelevel get 2 ge
	} if
	put
	level2? not
	{
		/setcmykcolor where not
		{
			/setcmykcolor
			{
				exch .11 mul add exch .59 mul add exch .3 mul add
				1 exch sub setgray
			} def
		} if
		/currentcmykcolor where not
		{
			/currentcmykcolor
			{
				0 0 0 1 currentgray sub
			} def
		} if
		/setoverprint where not
		{
			/setoverprint /pop load def
		} if
		/selectfont where not
		{
			/selectfont
			{
				exch findfont exch
				dup type /arraytype eq
				{
					makefont
				}
				{
					scalefont
				} ifelse
				setfont
			} bind def
		} if
		/cshow where not
		{
			/cshow
			{
				[
				0 0 5 -1 roll aload pop
				] cvx bind forall
			} bind def
		} if
	} if
	cleartomark
	/anyColor?
	{
		add add add 0 ne
	} bind def
	/testColor
	{
		gsave
		setcmykcolor currentcmykcolor
		grestore
	} bind def
	/testCMYKColorThrough
	{
		testColor anyColor?
	} bind def
	userdict /composite?
	level2?
	{
		gsave 1 1 1 1 setcmykcolor currentcmykcolor grestore
		add add add 4 eq
	}
	{
		1 0 0 0 testCMYKColorThrough
		0 1 0 0 testCMYKColorThrough
		0 0 1 0 testCMYKColorThrough
		0 0 0 1 testCMYKColorThrough
		and and and
	} ifelse
	put
	composite? not
	{
		userdict begin
		gsave
		/cyan? 1 0 0 0 testCMYKColorThrough def
		/magenta? 0 1 0 0 testCMYKColorThrough def
		/yellow? 0 0 1 0 testCMYKColorThrough def
		/black? 0 0 0 1 testCMYKColorThrough def
		grestore
		/isCMYKSep? cyan? magenta? yellow? black? or or or def
		/customColor? isCMYKSep? not def
	 end
	} if
 end defaultpacking setpacking
%%EndResource
%%BeginResource: procset Adobe_typography_AI5 1.0 0
%%Title: (Typography Operators)
%%Version: 1.0
%%CreationDate:(03/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_typography_AI5 48 dict dup begin
put
/initialize
{
 begin
 begin
	Adobe_typography_AI5 begin
	Adobe_typography_AI5
	{
		dup xcheck
		{
			bind
		} if
		pop pop
	} forall
 end
 end
 end
	Adobe_typography_AI5 begin
} def
/terminate
{
	currentdict Adobe_typography_AI5 eq
	{
	 end
	} if
} def
/modifyEncoding
{
	/_tempEncode exch ddef
	/_pntr 0 ddef
	{
		counttomark -1 roll
		dup type dup /marktype eq
		{
			pop pop exit
		}
		{
			/nametype eq
			{
				_tempEncode /_pntr dup load dup 3 1 roll 1 add ddef 3 -1 roll
				put
			}
			{
				/_pntr exch ddef
			} ifelse
		} ifelse
	} loop
	_tempEncode
} def
/TE
{
	StandardEncoding 256 array copy modifyEncoding
	/_nativeEncoding exch def
} def
%
/TZ
{
	dup type /arraytype eq
	{
		/_wv exch def
	}
	{
		/_wv 0 def
	} ifelse
	/_useNativeEncoding exch def
	pop pop
	findfont _wv type /arraytype eq
	{
		_wv makeblendedfont
	} if
	dup length 2 add dict
 begin
	mark exch
	{
		1 index /FID ne
		{
			def
		} if
		cleartomark mark
	} forall
	pop
	/FontName exch def
	counttomark 0 eq
	{
		1 _useNativeEncoding eq
		{
			/Encoding _nativeEncoding def
		} if
		cleartomark
	}
	{
		/Encoding load 256 array copy
		modifyEncoding /Encoding exch def
	} ifelse
	FontName currentdict
 end
	definefont pop
} def
/tr
{
	_ax _ay 3 2 roll
} def
/trj
{
	_cx _cy _sp _ax _ay 6 5 roll
} def
/a0
{
	/Tx
	{
		dup
		currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
	} ddef
	/Tj
	{
		dup
		currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
	} ddef
} def
/a1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		tr _psf
		newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		dup currentpoint 3 2 roll
		trj _pjsf
		newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/e0
{
	/Tx
	{
		tr _psf
	} ddef
	/Tj
	{
		trj _pjsf
	} ddef
} def
/e1
{
	/Tx
	{
		dup currentpoint 4 2 roll gsave
		tr _psf
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll gsave
		trj _pjsf
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/i0
{
	/Tx
	{
		tr sp
	} ddef
	/Tj
	{
		trj jsp
	} ddef
} def
/i1
{
	W N
} def
/o0
{
	/Tx
	{
		tr sw rmoveto
	} ddef
	/Tj
	{
		trj swj rmoveto
	} ddef
} def
/r0
{
	/Tx
	{
		tr _ctm _pss
	} ddef
	/Tj
	{
		trj _ctm _pjss
	} ddef
} def
/r1
{
	/Tx
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		tr _ctm _pss
		grestore 3 1 roll moveto tr sp
	} ddef
	/Tj
	{
		dup currentpoint 4 2 roll currentpoint gsave newpath moveto
		trj _ctm _pjss
		grestore 3 1 roll moveto tr jsp
	} ddef
} def
/To
{
	pop _ctm currentmatrix pop
} def
/TO
{
	iTe _ctm setmatrix newpath
} def
/Tp
{
	pop _tm astore pop _ctm setmatrix
	_tDict begin
	/W
	{
	} def
	/h
	{
	} def
} def
/TP
{
 end
	iTm 0 0 moveto
} def
/Tr
{
	_render 3 le
	{
		currentpoint newpath moveto
	} if
	dup 8 eq
	{
		pop 0
	}
	{
		dup 9 eq
		{
			pop 1
		} if
	} ifelse
	dup /_render exch ddef
	_renderStart exch get load exec
} def
/iTm
{
	_ctm setmatrix _tm concat 0 _rise translate _hs 1 scale
} def
/Tm
{
	_tm astore pop iTm 0 0 moveto
} def
/Td
{
	_mtx translate _tm _tm concatmatrix pop iTm 0 0 moveto
} def
/iTe
{
	_render -1 eq
	{
	}
	{
		_renderEnd _render get dup null ne
		{
			load exec
		}
		{
			pop
		} ifelse
	} ifelse
	/_render -1 ddef
} def
/Ta
{
	pop
} def
/Tf
{
	dup 1000 div /_fScl exch ddef
	exch findfont exch scalefont setfont
} def
/Tl
{
	pop
	0 exch _leading astore pop
} def
/Tt
{
	pop
} def
/TW
{
	3 npop
} def
/Tw
{
	/_cx exch ddef
} def
/TC
{
	3 npop
} def
/Tc
{
	/_ax exch ddef
} def
/Ts
{
	/_rise exch ddef
	currentpoint
	iTm
	moveto
} def
/Ti
{
	3 npop
} def
/Tz
{
	100 div /_hs exch ddef
	iTm
} def
/TA
{
	pop
} def
/Tq
{
	pop
} def
/Th
{
	pop pop pop pop pop
} def
/TX
{
	pop
} def
/Tk
{
	exch pop _fScl mul neg 0 rmoveto
} def
/TK
{
	2 npop
} def
/T*
{
	_leading aload pop neg Td
} def
/T*-
{
	_leading aload pop Td
} def
/T-
{
	_hyphen Tx
} def
/T+
{
} def
/TR
{
	_ctm currentmatrix pop
	_tm astore pop
	iTm 0 0 moveto
} def
/TS
{
	0 eq
	{
		Tx
	}
	{
		Tj
	} ifelse
} def
currentdict readonly pop
end
setpacking
%%EndResource
%%BeginResource: procset Adobe_IllustratorA_AI5 1.0 0
%%Title: (Adobe Illustrator (R) Version 5.0 Abbreviated Prolog)
%%Version: 1.0
%%CreationDate: (3/26/93) ()
%%Copyright: ((C) 1987-1993 Adobe Systems Incorporated All Rights Reserved)
currentpacking true setpacking
userdict /Adobe_IllustratorA_AI5_vars 70 dict dup begin
put
/_lp /none def
/_pf
{
} def
/_ps
{
} def
/_psf
{
} def
/_pss
{
} def
/_pjsf
{
} def
/_pjss
{
} def
/_pola 0 def
/_doClip 0 def
/cf currentflat def
/_tm matrix def
/_renderStart
[
/e0 /r0 /a0 /o0 /e1 /r1 /a1 /i0
] def
/_renderEnd
[
null null null null /i1 /i1 /i1 /i1
] def
/_render -1 def
/_rise 0 def
/_ax 0 def
/_ay 0 def
/_cx 0 def
/_cy 0 def
/_leading
[
0 0
] def
/_ctm matrix def
/_mtx matrix def
/_sp 16#020 def
/_hyphen (-) def
/_fScl 0 def
/_cnt 0 def
/_hs 1 def
/_nativeEncoding 0 def
/_useNativeEncoding 0 def
/_tempEncode 0 def
/_pntr 0 def
/_tDict 2 dict def
/_wv 0 def
/Tx
{
} def
/Tj
{
} def
/CRender
{
} def
/_AI3_savepage
{
} def
/_gf null def
/_cf 4 array def
/_if null def
/_of false def
/_fc
{
} def
/_gs null def
/_cs 4 array def
/_is null def
/_os false def
/_sc
{
} def
/discardSave null def
/buffer 256 string def
/beginString null def
/endString null def
/endStringLength null def
/layerCnt 1 def
/layerCount 1 def
/perCent (%) 0 get def
/perCentSeen? false def
/newBuff null def
/newBuffButFirst null def
/newBuffLast null def
/clipForward? false def
end
userdict /Adobe_IllustratorA_AI5 74 dict dup begin
put
/initialize
{
	Adobe_IllustratorA_AI5 dup begin
	Adobe_IllustratorA_AI5_vars begin
	discardDict
	{
		bind pop pop
	} forall
	dup /nc get begin
	{
		dup xcheck 1 index type /operatortype ne and
		{
			bind
		} if
		pop pop
	} forall
 end
	newpath
} def
/terminate
{
 end
 end
} def
/_
null def
/ddef
{
	Adobe_IllustratorA_AI5_vars 3 1 roll put
} def
/xput
{
	dup load dup length exch maxlength eq
	{
		dup dup load dup
		length 2 mul dict copy def
	} if
	load begin
	def
 end
} def
/npop
{
	{
		pop
	} repeat
} def
/sw
{
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
} def
/swj
{
	dup 4 1 roll
	dup length exch stringwidth
	exch 5 -1 roll 3 index mul add
	4 1 roll 3 1 roll mul add
	6 2 roll /_cnt 0 ddef
	{
		1 index eq
		{
			/_cnt _cnt 1 add ddef
		} if
	} forall
	pop
	exch _cnt mul exch _cnt mul 2 index add 4 1 roll 2 index add 4 1 roll pop pop
} def
/ss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put pop
		gsave
		false charpath currentpoint
		4 index setmatrix
		stroke
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	3 npop
} def
/jss
{
	4 1 roll
	{
		2 npop
		(0) exch 2 copy 0 exch put
		gsave
		_sp eq
		{
			exch 6 index 6 index 6 index 5 -1 roll widthshow
			currentpoint
		}
		{
			false charpath currentpoint
			4 index setmatrix stroke
		} ifelse
		grestore
		moveto
		2 copy rmoveto
	} exch cshow
	6 npop
} def
/sp
{
	{
		2 npop (0) exch
		2 copy 0 exch put pop
		false charpath
		2 copy rmoveto
	} exch cshow
	2 npop
} def
/jsp
{
	{
		2 npop
		(0) exch 2 copy 0 exch put
		_sp eq
		{
			exch 5 index 5 index 5 index 5 -1 roll widthshow
		}
		{
			false charpath
		} ifelse
		2 copy rmoveto
	} exch cshow
	5 npop
} def
/pl
{
	transform
	0.25 sub round 0.25 add exch
	0.25 sub round 0.25 add exch
	itransform
} def
/setstrokeadjust where
{
	pop true setstrokeadjust
	/c
	{
		curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll curveto
	} def
	/V
	/v load def
	/y
	{
		2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		lineto
	} def
	/L
	/l load def
	/m
	{
		moveto
	} def
}
{
	/c
	{
		pl curveto
	} def
	/C
	/c load def
	/v
	{
		currentpoint 6 2 roll pl curveto
	} def
	/V
	/v load def
	/y
	{
		pl 2 copy curveto
	} def
	/Y
	/y load def
	/l
	{
		pl lineto
	} def
	/L
	/l load def
	/m
	{
		pl moveto
	} def
} ifelse
/d
{
	setdash
} def
/cf
{
} def
/i
{
	dup 0 eq
	{
		pop cf
	} if
	setflat
} def
/j
{
	setlinejoin
} def
/J
{
	setlinecap
} def
/M
{
	setmiterlimit
} def
/w
{
	setlinewidth
} def
/H
{
} def
/h
{
	closepath
} def
/N
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			clip /_doClip 0 ddef
		} if
		newpath
	}
	{
		/CRender
		{
			N
		} ddef
	} ifelse
} def
/n
{
	N
} def
/F
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _pf grestore clip newpath /_lp /none ddef _fc
			/_doClip 0 ddef
		}
		{
			_pf
		} ifelse
	}
	{
		/CRender
		{
			F
		} ddef
	} ifelse
} def
/f
{
	closepath
	F
} def
/S
{
	_pola 0 eq
	{
		_doClip 1 eq
		{
			gsave _ps grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			_ps
		} ifelse
	}
	{
		/CRender
		{
			S
		} ddef
	} ifelse
} def
/s
{
	closepath
	S
} def
/B
{
	_pola 0 eq
	{
		_doClip 1 eq
		gsave F grestore
		{
			gsave S grestore clip newpath /_lp /none ddef _sc
			/_doClip 0 ddef
		}
		{
			S
		} ifelse
	}
	{
		/CRender
		{
			B
		} ddef
	} ifelse
} def
/b
{
	closepath
	B
} def
/W
{
	/_doClip 1 ddef
} def
/*
{
	count 0 ne
	{
		dup type /stringtype eq
		{
			pop
		} if
	} if
	_pola 0 eq
	{
		newpath
	} if
} def
/u
{
} def
/U
{
} def
/q
{
	_pola 0 eq
	{
		gsave
	} if
} def
/Q
{
	_pola 0 eq
	{
		grestore
	} if
} def
/*u
{
	_pola 1 add /_pola exch ddef
} def
/*U
{
	_pola 1 sub /_pola exch ddef
	_pola 0 eq
	{
		CRender
	} if
} def
/D
{
	pop
} def
/*w
{
} def
/*W
{
} def
/`
{
	/_i save ddef
	clipForward?
	{
		nulldevice
	} if
	6 1 roll 4 npop
	concat pop
	userdict begin
	/showpage
	{
	} def
	0 setgray
	0 setlinecap
	1 setlinewidth
	0 setlinejoin
	10 setmiterlimit
	[
	] 0 setdash
	newpath
	0 setgray
	false setoverprint
} def
/~
{
 end
	_i restore
} def
/O
{
	0 ne
	/_of exch ddef
	/_lp /none ddef
} def
/R
{
	0 ne
	/_os exch ddef
	/_lp /none ddef
} def
/g
{
	/_gf exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_gf setgray
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/G
{
	/_gs exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_gs setgray
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/k
{
	_cf astore pop
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_cf aload pop setcmykcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/K
{
	_cs astore pop
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_cs aload pop setcmykcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/x
{
	/_gf exch ddef
	findcmykcustomcolor
	/_if exch ddef
	/_fc
	{
		_lp /fill ne
		{
			_of setoverprint
			_if _gf 1 exch sub setcustomcolor
			/_lp /fill ddef
		} if
	} ddef
	/_pf
	{
		_fc
		fill
	} ddef
	/_psf
	{
		_fc
		ashow
	} ddef
	/_pjsf
	{
		_fc
		awidthshow
	} ddef
	/_lp /none ddef
} def
/X
{
	/_gs exch ddef
	findcmykcustomcolor
	/_is exch ddef
	/_sc
	{
		_lp /stroke ne
		{
			_os setoverprint
			_is _gs 1 exch sub setcustomcolor
			/_lp /stroke ddef
		} if
	} ddef
	/_ps
	{
		_sc
		stroke
	} ddef
	/_pss
	{
		_sc
		ss
	} ddef
	/_pjss
	{
		_sc
		jss
	} ddef
	/_lp /none ddef
} def
/A
{
	pop
} def
/annotatepage
{
userdict /annotatepage 2 copy known {get exec} {pop pop} ifelse
} def
/discard
{
	save /discardSave exch store
	discardDict begin
	/endString exch store
	version cvx exec 38 gt
	{
		2 add
	} if
	load
	stopped
	pop
 end
	discardSave restore
} bind def
userdict /discardDict 7 dict dup begin
put
/pre38Initialize
{
	/endStringLength endString length store
	/newBuff buffer 0 endStringLength getinterval store
	/newBuffButFirst newBuff 1 endStringLength 1 sub getinterval store
	/newBuffLast newBuff endStringLength 1 sub 1 getinterval store
} def
/shiftBuffer
{
	newBuff 0 newBuffButFirst putinterval
	newBuffLast 0
	currentfile read not
	{
	stop
	} if
	put
} def
0
{
	pre38Initialize
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff endString eq
			{
				cleartomark stop
			} if
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
1
{
	pre38Initialize
	/beginString exch store
	mark
	currentfile newBuff readstring exch pop
	{
		{
			newBuff beginString eq
			{
				/layerCount dup load 1 add store
			}
			{
				newBuff endString eq
				{
					/layerCount dup load 1 sub store
					layerCount 0 eq
					{
						cleartomark stop
					} if
				} if
			} ifelse
			shiftBuffer
		} loop
	}
	{
	stop
	} ifelse
} def
2
{
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		endString eq
		{
			cleartomark stop
		} if
	} loop
} def
3
{
	/beginString exch store
	/layerCnt 1 store
	mark
	{
		currentfile buffer readline not
		{
		stop
		} if
		dup beginString eq
		{
			pop /layerCnt dup load 1 add store
		}
		{
			endString eq
			{
				layerCnt 1 eq
				{
					cleartomark stop
				}
				{
					/layerCnt dup load 1 sub store
				} ifelse
			} if
		} ifelse
	} loop
} def
end
userdict /clipRenderOff 15 dict dup begin
put
{
	/n /N /s /S /f /F /b /B
}
{
	{
		_doClip 1 eq
		{
			/_doClip 0 ddef clip
		} if
		newpath
	} def
} forall
/Tr /pop load def
/Bb {} def
/BB /pop load def
/Bg {12 npop} def
/Bm {6 npop} def
/Bc /Bm load def
/Bh {4 npop} def
end
/Lb
{
	4 npop
	6 1 roll
	pop
	4 1 roll
	pop pop pop
	0 eq
	{
		0 eq
		{
			(%AI5_BeginLayer) 1 (%AI5_EndLayer--) discard
		}
		{
			/clipForward? true def

			/Tx /pop load def
			/Tj /pop load def
			currentdict end clipRenderOff begin begin
		} ifelse
	}
	{
		0 eq
		{
			save /discardSave exch store
		} if
	} ifelse
} bind def
/LB
{
	discardSave dup null ne
	{
		restore
	}
	{
		pop
		clipForward?
		{
			currentdict
		 end
		 end
		 begin

			/clipForward? false ddef
		} if
	} ifelse
} bind def
/Pb
{
	pop pop
	0 (%AI5_EndPalette) discard
} bind def
/Np
{
	0 (%AI5_End_NonPrinting--) discard
} bind def
/Ln /pop load def
/Ap
/pop load def
/Ar
{
	72 exch div
	0 dtransform dup mul exch dup mul add sqrt
	dup 1 lt
	{
		pop 1
	} if
	setflat
} def
/Mb
{
	q
} def
/Md
{
} def
/MB
{
	Q
} def
/nc 3 dict def
nc begin
/setgray
{
	pop
} bind def
/setcmykcolor
{
	4 npop
} bind def
/setcustomcolor
{
	2 npop
} bind def
currentdict readonly pop
end
currentdict readonly pop
end
setpacking
%%EndResource
%%EndProlog
%%BeginSetup
%%IncludeFont: Helvetica
Adobe_level2_AI5 /initialize get exec
Adobe_IllustratorA_AI5_vars Adobe_IllustratorA_AI5 Adobe_typography_AI5
/initial
Adobe_IllustratorA_AI5 /initialize get exec
[
39/quotesingle 96/grave 128/Adieresis/Aring/Ccedilla/Eacute/Ntilde/Odieresis
/Udieresis/aacute/agrave/acircumflex/adieresis/atilde/aring/ccedilla/eacute
/egrave/ecircumflex/edieresis/iacute/igrave/icircumflex/idieresis/ntilde
/oacute/ograve/ocircumflex/odieresis/otilde/uacute/ugrave/ucircumflex
/udieresis/dagger/degree/cent/sterling/section/bullet/paragraph/germandbls
/registered/copyright/trademark/acute/dieresis/.notdef/AE/Oslash
/.notdef/plusminus/.notdef/.notdef/yen/mu/.notdef/.notdef
/.notdef/.notdef/.notdef/ordfeminine/ordmasculine/.notdef/ae/oslash
/questiondown/exclamdown/logicalnot/.notdef/florin/.notdef/.notdef
/guillemotleft/guillemotright/ellipsis/.notdef/Agrave/Atilde/Otilde/OE/oe
/endash/emdash/quotedblleft/quotedblright/quoteleft/quoteright/divide
/.notdef/ydieresis/Ydieresis/fraction/currency/guilsinglleft/guilsinglright
/fi/fl/daggerdbl/periodcentered/quotesinglbase/quotedblbase/perthousand
/Acircumflex/Ecircumflex/Aacute/Edieresis/Egrave/Iacute/Icircumflex
/Idieresis/Igrave/Oacute/Ocircumflex/.notdef/Ograve/Uacute/Ucircumflex
/Ugrave/dotlessi/circumflex/tilde/macron/breve/dotaccent/ring/cedilla
/hungarumlaut/ogonek/caron
TE
%AI3_BeginEncoding: _Helvetica Helvetica
[/_Helvetica/Helvetica 0 0 1 TZ
%AI3_EndEncoding AdobeType
%AI5_Begin_NonPrinting
Np
%AI3_BeginPattern: (Bandes jaunes)
(Bandes jaunes) 8.4499 4.6 80.4499 76.6 [
%AI3_Tile
(0 O 0 R 0 0.4 1 0 k 0 0.4 1 0 K) @
(
800 Ar
0 J 0 j 3.6 w 4 M []0 d
%AI3_Note:
0 D
8.1999 8.1999 m
80.6999 8.1999 L
S
8.1999 22.6 m
80.6999 22.6 L
S
8.1999 37.0001 m
80.6999 37.0001 L
S
8.1999 51.3999 m
80.6999 51.3999 L
S
8.1999 65.8 m
80.6999 65.8 L
S
8.1999 15.3999 m
80.6999 15.3999 L
S
8.1999 29.8 m
80.6999 29.8 L
S
8.1999 44.1999 m
80.6999 44.1999 L
S
8.1999 58.6 m
80.6999 58.6 L
S
8.1999 73.0001 m
80.6999 73.0001 L
S
) &
] E
%AI3_EndPattern
%AI5_End_NonPrinting--
%AI5_Begin_NonPrinting
Np
3 Bn
%AI5_BeginGradient: (Jaune-bleu radial)
(Jaune-bleu radial) 1 2 Bd
[
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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>
0
1 %_Br
[
0 0.08 0.67 0 1 50 14 %_Bs
1 1 0 0 1 50 100 %_Bs
BD
%AI5_EndGradient
%AI5_BeginGradient: (Noir-blanc)
(Noir-blanc) 0 2 Bd
[
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
AFAEADACABAAA9A8A7A6A5A4A3A2A1A09F9E9D9C9B969594939291908F8E8D8C8B8A8988
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
5F5E5D5C5B565554535251504F4E4D4C4B464544434241403F3E3D3C3B3A3938
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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>
0 %_Br
[
0 0 50 100 %_Bs
1 0 50 0 %_Bs
BD
%AI5_EndGradient
%AI5_BeginGradient: (Rouge-jaune)
(Rouge-jaune) 0 2 Bd
[
0
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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>
<
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
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68.1458 199.4162 l
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68.0833 228.2499 l
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76.6042 242.6665 m
68.2708 242.6665 l
S
76.7917 257.0832 m
68.4583 257.0832 l
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(Fig. 3) Tx
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%AI5_EndLayer--
%%PageTrailer
gsave annotatepage grestore showpage
%%Trailer
Adobe_IllustratorA_AI5 /terminate get exec
Adobe_typography_AI5 /terminate get exec
Adobe_level2_AI5 /terminate get exec
%%EOF

