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%Date: Tue, 21 Jul 1992 15:00:05 EDT

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\begin{document}

\hfill {MIT-CTP-2108}

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\hfill {UMS/HEP 92-021}


\begin{title}
I=3/2 $K \pi $ Scattering in the\\
Nonrelativistic Quark Potential Model\\
\end{title}

\author{T. Barnes}

\begin{instit}
Physics Division and Center for Computationally Intensive Physics\\
Oak Ridge National Laboratory, Oak Ridge, TN 37831-6373\\
and\\
Department of Physics\\
University of Tennessee, Knoxville, TN 37996-1200\\
\end{instit}

\author{E.S. Swanson}

\begin{instit}
Center for Theoretical Physics\\
Laboratory of Nuclear Science and Department of Physics\\
Massachusetts Institute of Technology, Cambridge, MA 02139\\
\end{instit}

\author {J. Weinstein}

\begin{instit}
Department of Physics and Astronomy\\
University of Mississippi\\
University, MS 38677\\
\end{instit}


%\vspace{0.5cm}
\begin{abstract}
We study $I=3/2$ elastic $K\pi $  scattering to Born order
using nonrelativistic quark wavefunctions in a constituent-exchange model.
This channel is ideal for the study of nonresonant meson-meson scattering
amplitudes
since s-channel resonances do not contribute significantly.
Standard
quark model parameters yield good agreement with the measured S- and P-wave
phase shifts and with PCAC calculations of the scattering length.
The P-wave phase shift is especially interesting because it is nonzero
solely due to
$SU(3)_f$ symmetry breaking effects, and is found to be in good agreement
with experiment given conventional values for the strange and nonstrange
constituent quark masses.
\end{abstract}

%\receipt{}
%\pacs{}
%\vfill
\centerline{Submitted to {\sl Phys. Rev.} {\bf D}}
%\vfill
\centerline{June 1992}
\newpage

\section{Introduction}

The derivation of hadronic interactions from QCD has been a goal of nuclear
physics for many years. At present this appears to be a very difficult problem;
even the
more modest goal of deriving hadronic interactions from the nonrelativistic
quark model is difficult, due in part
to the variety of mechanisms which contribute to
scattering.
In a typical hadronic scattering process these mechanisms include
s-channel resonance production, t-channel
resonance exchange, and nonresonant scattering.
Despite the apparent complexity, there is considerable evidence
that some scattering amplitudes
are dominated by relatively simple
perturbative QCD processes.
One well known example is the
short-range part of the
NN interaction; many
groups have concluded that the NN repulsive core is due to the combined
effects of
the Pauli principle and the color magnetic spin-spin component of one gluon
exchange.
Similarly, the
intermediate-range
attractive interaction may be due to a relatively simple effect at the
quark level, specifically a color-dipole interaction induced by the spatial
distortion of the three-quark clusters \cite{NIcart}.
Of course one pion exchange dominates at sufficiently large
separations, and in a more complete description one should adjoin this to
the short-range quark interaction.

In this paper we discuss $I = 3/2$ $K\pi $ elastic scattering in the
nonrelativistic quark model. This process resembles $NN$
scattering in that s-channel resonances are not expected to give important
contributions, assuming that multiquark resonances are not in evidence.
The Born-order QCD scattering amplitude for this process involves
one gluon exchange followed by quark exchange.
In a previous paper \cite{BS} it was shown that this simple
description of hadron-hadron scattering leads to
good agreement with the nonperturbative variational results
of Weinstein and Isgur
\cite{WI} near threshold,
and with the measured $I=2$ $\pi\pi$ S-wave phase shift throughout the
full range of $M_{\pi\pi}$ for which data exists. A
similar method was used in Ref.\ \cite{Swan}
to extract effective potentials for many
low-lying
meson-meson channels.  These
potentials have recently been applied to several
problems in low-energy meson
physics. In particular, Dooley {\it et al.} \cite{DSB} used the results
of Ref.\ \cite{Swan} to suggest that the $IJ^{PC} = 0 0^{++}$ $\theta
(1720)$ may be a  $(K^*\bar K^*)$-$(\omega\phi)$ vector-vector molecular
bound state. Simple estimates of
branching ratios in this model find
good agreement with Particle Data Group values
and predict new decay modes. In another application it has been
argued that the $f_1(1420)$ ``E" effect may be a threshold enhancement which is
due to an attractive $(K^* \bar K)$-$(\omega \phi)$ interaction
in the $01^{++}$ channel \cite{Swan}.

The $I= 3/2$ $K\pi $ channel is an ideal one for testing our model
of Born scattering amplitudes,
since we expect it to be largely unaffected by s-channel resonances.
%Thus we expect pure quark
%effects to dominate the reaction.
The success of the
previous application of the model to $I = 2$ $\pi\pi$ scattering
and the assumption of flavor symmetry suggest
that we may also find reasonable agreement with the experimental
S-wave $K\pi $ phase shift. The P-wave, however, is driven entirely by
flavor symmetry {\it breaking}, and hence the interplay of these two waves
provides an interesting and nontrivial test of the model.

\section{Method}

The calculation is based on a standard quark model Hamiltonian of the
form

\begin{equation}
H = \sum_{i=1}^4 \left( {p_i^2 \over 2 m_i} + m_i \right) + \sum_{i<j}
\left[ V_{conf}(r_{ij}) + V_{cont}(r_{ij})\; \vec S_i \cdot \vec S_j +
V_{orb} \; \right] \vec F_i \cdot \vec F_j
\end {equation}
where
\begin{equation}
V_{cont} = {-8 \pi \alpha_s\over 3 m_i m_j}\; \delta(\vec r_{ij})
\end {equation}
is the contact color-hyperfine interaction, $V_{conf}$ is a
confinement potential, and $V_{orb}$ represents spin-orbit and tensor
interactions.
We
neglect $V_{orb}$ in this paper since its effects are generally found to
be numerically small
in meson spectroscopy \cite{GI}, and are expected to be unimportant in
the scattering of two $\ell=0$ mesons as well.
We shall also ignore the contribution of $V_{conf}$ to the scattering
interaction.
This may appear to be a questionable approximation; however,
resonating group calculations have found that the exchange (scattering)
kernel due to $V_{conf}$ is much smaller than the corresponding
kernel for the
hyperfine term \cite{Shim}. This result was also found in the
variational
calculation of Ref.\ \cite{WI} and the perturbative calculation of Ref.\
\cite{Swan}. The latter reference noted that the small $V_{conf}$
contribution to scattering is due to a color-factor
cancellation in the matrix element of $V_{conf}$.
However, this result only applies to certain channels;
one should {\it not} neglect the
effects of the confinement term in scattering involving
vector mesons.

Although we calculate the scattering amplitude only
to Born order, there is
evidence that this is a useful and even accurate approximation
in systems which are not dominated by s-channel resonances or t-channel
meson exchange.
First, as there is
little evidence for flavor mixing
in meson spectroscopy outside the $\eta-\eta'$ system,
one anticipates that neglecting higher terms in
the Born series (such as $q \bar q \rightarrow gg \rightarrow q \bar q$)
is not a bad approximation. In addition, the Born-approximation
$I=2$ $\pi\pi$ effective
potentials
derived in Refs.\ \cite{BS} and \cite{Swan} are numerically very similar
to the
nonperturbative potentials derived by Weinstein and Isgur.
Finally, comparison of perturbative phase shifts to those found in a
variational resonating group calculation shows good numerical
agreement \cite{Swan}.

For simplicity we use single Gaussians for the asymptotic pion and kaon
wavefunctions,
\begin{equation}
\psi_{\pi(K)}(r) = \left({\beta_{\pi(K)}^2 \over \pi}\right)^{3/4}
{\rm e}^{-\beta_{\pi(K)}^2\, r^2/2} \ ,
\end {equation}
where $r = |\vec r_q - \vec r_{\bar q}|$.
The corresponding momentum-space wavefunction $\phi(k_{rel})$ is
a function of the magnitude of the relative momentum vector
$\vec k_{rel}=(m_{\bar q}\vec k_q - m_q\vec k_{\bar q})/(m_q + m_{\bar q})$.

Flavor symmetry breaking is incorporated through unequal strange
and nonstrange quark masses (we introduce a mass ratio
$\rho = m_u/m_s$) and a meson width parameter $\xi$
(defined by $\xi = \beta_\pi^2/\beta_K^2$;
$\xi < 1$ corresponds to a smaller kaon than
pion).
Of course these parameters are related.
For instance if
we take $V_{conf}(r_{ij}) = C + \kappa r_{ij}^2 /2$  then
$\xi = \sqrt{(1 + \rho)/2}$.
Standard quark model values for the constituent masses,
$m_u = 0.33$ GeV and $m_s =
0.55$ GeV, give $\rho = 0.6$, and from the SHO relation above
we might anticipate
$\xi \approx 0.9$.
A fit to light meson spectroscopy in a
Coulomb plus linear potential model with a contact hyperfine term
finds a similar $\rho $ value of $\rho = 0.58$.  With this $\rho$
a single-Gaussian variational calculation
\cite{Swan} actually finds a value for $\xi$ slightly above unity,
$\xi = 1.05$, because the stronger pion hyperfine attraction leads to a smaller
pion than kaon despite the heavier strange quark mass. In any case we expect
$\xi$ to be near unity.

There are four Born-order quark exchange graphs for $K\pi $ scattering,
which
we previously classified as two
``transfer"  or ``capture" processes in our discussion of $\pi\pi$
scattering \cite{BS}.
The transfer diagrams represent scattering due to a
spin-spin hyperfine interaction between a
quark pair ($T_1$) or an antiquark pair ($T_2$).
In the capture
diagrams the interaction is between a quark-antiquark pair in different mesons,
$u\bar s$ for $C_1$ and $u \bar d$ for $C_2$. We apply the
methods of Ref. \cite{BS} (Appendix C)
to obtain the Born-order Hamiltonian matrix element
$h_{fi}$ for these diagrams, which is

\begin{equation}
h_{fi} = {1\over (2\pi)^3}
{4 \pi \alpha_s \over 9 m_u^2} \Big( T_1 + T_2 + C_1 + C_2 \Big) \ ,
\end {equation}
where the term contributed by each diagram is

\begin{mathletters}
\begin{eqnarray}
T_1 &=& \exp\bigg\{
- (1 + \xi(1+\zeta)^2 )\;
\bigg[ {1- \mu\over 2} \bigg] \;
{k^2 \over 4 \beta_\pi^2}\;
\bigg\} \\
T_2 &=& \rho \left({2\sqrt{\xi} \over 1 + \xi } \right)^{3}
\exp\bigg\{ -
{\xi \over 1+\xi} \; \bigg[ 1 + (1-\zeta)^2 + 2(1-\zeta)\mu \, \bigg] \;
{k^2 \over 4\beta_\pi^2} \; \bigg\} \\
C_1 &=& \rho \left({4 \over 2 + \xi}\right)^{3/2} \exp \bigg\{
-{ 1 \over 2+\xi} \; \bigg[ 1+ 3\xi - \xi \zeta (1-\zeta)
+ ( \xi - 1- 3 \xi \zeta) \mu \,
\bigg]  \; {k^2 \over 4\beta_\pi^2}\; \bigg\} \\
C_2 &=& \left({4\xi \over 1 +2\xi}\right)^{3/2} \exp \bigg\{
-{ \xi \over 1+2\xi} \;
\bigg[ 3 - \zeta + \zeta^2 + \xi (1+\zeta)^2 \nonumber \\
&& + (1 - 3\zeta -\xi (1+\zeta)^2 ) \mu \, \bigg]
{k^2 \over 4\beta_\pi^2} \; \bigg\} \ .\\
\nonumber
\end{eqnarray}
\end{mathletters}
In these matrix elements $\mu = \cos(\theta_{CM})$, where $\theta_{CM}$ is
the center of mass
scattering angle, the quark mass parameter $\zeta$ is $
(m_s-m_u)/(m_s+m_u) = (1-\rho)/(1+\rho)$, and $k$ is the magnitude of
the asymptotic three-momentum of each meson in the CM frame.
The matrix element $h_{fi}$ is related to the $\ell$th partial-wave
phase shift by \cite{BS}
\begin{equation}
\delta^{(\ell)} = {- 2\pi^2 k E_\pi E_K \over ( E_\pi + E_K)} \int_{-1}^{1}
h_{fi}(\mu)\, P_\ell (\mu)\,d\mu \ ,
\end{equation}
with the meson energies related to $k$ by relativistic kinematics.
This result involves $\delta^{(\ell )} $ rather than
$\sin \delta^{(\ell)} $ because we choose to
equate our Born amplitude to the leading
term in the
elastic scattering amplitude $(\exp\{2i\delta^{(\ell)}\}-1)/2i$
rather than to the full real part. The phase shifts for all partial waves
follow
from this result
through application of the integral $\int_{-1}^1 e^{a\mu} P_\ell (\mu)
d\mu = 2 i_\ell (a)$ where $i_\ell$ is the modified spherical Bessel function
of the first kind.

\section{Results and Discussion}

On evaluating the angular integrals (6) we find
$I=3/2$ $K\pi $ phase shifts for all $\ell$ in Born
approximation given SHO wavefunctions; these are functions of the
four free parameters
$\beta_\pi$, $\alpha_s/m_u^2$, $\rho=m_u/m_s$, and $\xi=\beta_\pi^2/\beta_K^2$,
and require the physical meson masses as input.
In the following discussion we shall fix the nonstrange
quark mass to be
$m_u=0.33$ GeV since the phase shifts actually involve the ratios given
above rather than the absolute scale of $m_u$.

We proceed by fitting the predicted phase shifts to the S- and P-wave phase
shift data of Estabrooks {\it et al.} \cite{Esta}.
Note however that there may be a discrepancy between this
data and earlier $I=3/2$ $K\pi$ results \cite{Jong,LP} near threshold;
two S-wave data sets are shown in Fig.\ \ref{fig1}.

As an initial ``benchmark" prediction we first
neglect flavor-symmetry violation (except for the use of
physical meson masses in kinematics and phase space)
and employ the same
parameters we previously used to describe
$I=2$ $\pi\pi$ scattering in Ref.\ \cite{BS};
$\alpha_s = 0.6$, $m_u = 0.33$ GeV and $\beta_\pi($fitted to $\pi\pi)
= 0.337$ GeV,
and we
set $m_s=m_u$ and $\beta_K=\beta_{\pi}$ so that $\rho = 1$ and $\xi = 1$.
The resulting S-wave phase shift is shown as
a dotted line in Fig.\ \ref{fig1}. Although the shape of the predicted phase
shift is qualitatively correct, evidently the predicted magnitude is
somewhat larger
than the data at invariant masses above 0.9 GeV.

Of course this flavor-symmetric
parameter set is unrealistic because it does not assume a
heavier strange quark; allowing $m_s$ to vary
yields the value $\rho = 0.677$ in a fit to the S-wave data
of Estabrooks {\it et al.}; this is
close to the $\rho \approx 0.33 \ \hbox{GeV} / 0.55 \ \hbox{GeV}$ $= 0.6$
expected
from $q\bar q$ quark model spectroscopy. The resulting phase shift is shown as
a dashed line in Fig.\ \ref{fig1}, and the agreement is impressive. The same
parameter set gives a P-wave phase shift which is shown as a dashed line in
Fig.\ \ref{fig2}. Evidently the agreement with experiment
is again quite good. Note that
the predicted P-wave phase shift is zero for $\rho = 1$, so the S-wave data
are consistent with approximate flavor symmetry (which implies
$\pi\pi$ S-wave $\approx$ $K\pi $ S-wave) and the P-wave data are consistent
with the expected amount of
flavor symmetry breaking (seen in the nonzero $K\pi $ P-wave).

Although we have found a satisfactory description of the data simply by using
$\pi\pi$ parameters and physical meson masses
and fitting $m_s$, it is of interest to investigate the
sensitivity of our results to changes in the other parameters and to
determine their global optimum values.
Fixing $\xi = 1$ and $\beta_\pi = 0.337$ GeV and fitting $\alpha_s$ and
$\rho$ to the Estabrooks {\it et al.} S-wave data
gives $\alpha_s = 0.634$ and $\rho = 0.604$,
again consistent with standard quark model values.
A global fit to the 33 S- and P-wave data points of Estabrooks
{\it et al.}
with all four parameters free
gives $\rho = 0.789$, $\alpha_s = 0.577$, $\beta_\pi = 0.293$
GeV and $\xi = 0.568$. The rather large $m_u/m_s$ in this fit
is partially compensated by a spatially small kaon wavefunction, but as the
phase shifts are rather insensitive to $\xi$, and we expect a value
closer to unity, this best fit probably gives less realistic
parameter values than the
single-parameter fit which found $\rho=0.677$.
The phase shifts
predicted by the
the global four-parameter set are shown as
solid lines
in Figs.\
\ref{fig1} and \ref{fig2}.
Note that the four-parameter
S-wave phase shift is essentially indistinguishable
from the one-parameter $(m_s)$ fit (dashed line);
the most important difference in the predictions of the two parameter sets
is in the P-wave, which is not yet very well determined
experimentally.

Estabrooks {\it et al.} also reported measurements of the $I=3/2$ $K\pi $
D-wave phase shift. We predict a
small negative D-wave phase shift in accord with the data, although
the magnitude of our D-wave is somewhat smaller than is observed.
A similar discrepancy in the $I=2$ $\pi\pi$ D-wave was previously noted
\ \cite{BS,Swan}.
It should be stressed that the
D-wave is qualitatively different from the P-wave;
it is not driven by flavor symmetry breaking and is an intrinsically
small effect at these energies, so that other contributions which we have
neglected may be important here. Possible contributions to this higher
partial wave include
the confinement, spin-orbit and tensor interactions.
The departure of the actual $q\bar q$ wavefunction from the assumed single
Gaussian may also be important, although
this effect was investigated in Ref.\ \cite{Swan} for
$I=2$ $\pi\pi$ scattering
and was found to be small.

Weinberg \cite{Wein} used PCAC to predict an
$I=3/2$ $K\pi $ scattering length of
\begin{equation}
a_S^{(3)}  = -{m_K m_\pi \over m_K + m_\pi} \ {1 \over 8 \pi f^2}
\end{equation}
in his original PCAC paper.
Here, $f$ is the pseudoscalar decay constant which may be identified with
$f_\pi$ in the flavor symmetric limit.
The quark Born approximation for the
scattering length may be extracted from our expression for the S-wave phase
shift, and is

\begin{equation}
a_S^{(3)} = -{m_K m_\pi \over m_K + m_\pi}\;
{2 \alpha_s \over 9 m_u^2} \left[ 1 +
  \left( {4 \xi \over 1 + 2\xi}\right)^{3/2} +  \rho \left( {4 \over 2 +\xi}
\right)^{3/2} +  \rho \left( {2 \sqrt{\xi} \over 1 +\xi}\right)^3 \right] \ .
\end{equation}
With our various parameter sets we find the following values for
the scattering length $a_S^{(3)}$:
$-0.092/m_\pi$ ($\rho = 1, \xi = 1$); $-0.077/m_\pi$
($\rho = 0.677, \alpha_s = 0.6$); $-0.078/m_\pi$ ($\rho = 0.604,
\alpha_s = 0.634$); $-0.076/m_\pi$ (global fit). These are compared to the
PCAC prediction, one-loop chiral perturbation
theory and various model calculations in Table\ \ref{table1}.
Experimental values for the scattering length range from
$-0.07/m_\pi$  to $-0.14/m_\pi$, and are also summarized
in Table\ \ref{table1}. Note that
we may also interpret our scattering length as
a quark Born formula for $f_\pi $
if we assume the PCAC relation (7).
With the flavor-symmetric parameter set we find $f_\pi = 80$ MeV,
in reasonable agreement with the experimental value of 93 MeV.

Our theoretical values for the scattering length
are consistent with most
experimental results, but not with the most recent,
which is that of Estabrooks {\it et al}.
Lang and Porod \cite{LP} note that the
Estabrooks {\it et al.} S-wave phase shift agrees with previous data for
$m_{K\pi } \agt 1$ GeV, but is
somewhat larger in magnitude than previous measurements
for $m_{K\pi } \alt 1$ GeV. Presumably this leads to their rather
large scattering length. It would clearly
be useful to resolve this experimental
discrepancy, since only in this mass region is there any indication
of a possible disagreement between the S-wave phase shift and our predictions.
It would also be very useful to improve the accuracy of the P-wave
measurement, which is a sensitive test of flavor symmetry breaking,
and to extend the S-wave phase shift measurements to higher invariant masses
as a test of the extremum predicted and perhaps observed near 1.4 GeV.

\section{Conclusions}

We have calculated
$I = 3/2$ $K\pi $ elastic scattering phase shifts
using a Born-order constituent-exchange description
in the framework of
the nonrelativistic quark
potential model.

Extensive
previous work leads us to believe that
one gluon exchange combined with quark exchange
may accurately describe nonresonant
hadron scattering in certain channels including $I=3/2$ $K\pi$,
and that the Born
approximation to the scattering amplitude is an acceptable one. This
reaction
is appropriate
for testing this model of scattering because
t-channel pion exchange is forbidden by $G$-parity and the experimental phase
shift shows no evidence for s-channel resonance formation.

Since this model was previously found to describe
the related $I=2$ $\pi\pi$ S-wave phase shift accurately \cite{BS},
approximate flavor
symmetry leads us to expect
that the predicted $I = 3/2$ $K\pi $
S-wave phase shift should at least be
in qualitative agreement with the data. This is
indeed found to be the case. The agreement is considerably improved
when flavor symmetry is broken by assigning the strange quark
a mass consistent with standard quark model values.
The P-wave $K\pi $ phase shift however
is generated entirely by flavor symmetry breaking effects
(primarily by the strange-nonstrange quark mass difference in our model), and
is not present in $I=2$ $\pi\pi$ scattering.
The very reasonable result we find for the P-wave phase shift using
fitted S-wave parameters is therefore a nontrivial and successful test
of the model.
Finally, the model predicts an
S-wave scattering length of about $-0.077/m_\pi$, which is in the range of
reported experimental values and is commensurate with the predictions of chiral
perturbation theory.

Although we find a small negative D-wave phase shift as has been reported
experimentally, the magnitude and energy dependence are
not well reproduced. This, however, is a
small contribution to the scattering amplitude, and the various other
scattering mechanisms which have been neglected in this calculation
may be significant in this case, and should be investigated in future.

Weinstein and Isgur have also studied S-wave
$I=3/2$ $K\pi $ scattering in the nonrelativistic quark model, using a
nonperturbative variational technique \cite{WI2}.
(Their method does not allow extraction of higher partial waves
at present.)
They find good agreement
with the S-wave data, although they must first
scale the range and strength of their
effective $K\pi $ potentials.
We perform no such scaling
but do employ relativistic phase space; the fact that both methods agree
well with experiment suggests that their scaling may
actually be compensating for kinematic effects above threshold. This conclusion
is supported by a recent reanalysis of the Weinstein-Isgur variational
calculations \cite{JW}.

The obvious extension of this work is to meson-baryon and baryon-baryon
scattering, with the caveat that one should specialize to channels such as
K$^+$-nucleon and baryon-baryon in which $q\bar q$ pair creation and
annihilation is unimportant. These topics are currently under investigation.

\acknowledgements

This research was sponsored by the Natural Sciences and Engineering
Research Council of Canada; the United States Department of Energy under
contracts DE-AC05-840R21400 with Martin Marietta Energy Systems Inc.,
DE-FG05-91ER40627 with the Physics Department of the University of
Tennessee, DE-AC02-76ER03069 with the Center for Theoretical Physics at
the Massachusetts Institute of Technology; and by the State of
Tennessee Science Alliance Center under contract R01-1062-32.


\newpage

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Rev. {\bf D3}, 1233 (1971).

\bibitem[20]{lang} C.B. Lang, Nuovo Cim. {\bf 41A}, 73 (1972).

\bibitem[21]{WI2} J. Weinstein and N. Isgur,
Phys. Rev. {\bf D43}, 95 (1991).

\bibitem[22]{JW} J. Weinstein, {\sl Comments on Low Mass
Pseudoscalar-Pseudoscalar Dynamics Including the S-wave $I=1$ KK System},
University of Mississippi report UMS/HEP 92-018 (1992).

\end{references}


\figure{S-wave $K\pi $ Phase Shift. The filled squares are data from
\cite{Esta}; the open squares are from \cite{Jong} (second solution). The
dotted
line corresponds to $\rho = 1$, the dashed line to $\rho = 0.677$, and the
solid line corresponds to the global fit (see text). \label{fig1}}

\figure{P-wave $K\pi $ Phase Shift. The data are from \cite{Esta}. The dashed
line corresponds to $\rho = 0.677$ and the solid line to the global fit (see
text). \label{fig2}}


\bigskip
\narrowtext
\begin{table}
\caption{Experimental and Theoretical Values for the S-wave Scattering Length.}
\begin{tabular}{lll}
$a_S^{(3)} \cdot m_\pi$ & Ref. & comments\\
\tableline
$-0.071(10)$ & \cite{Jong} & experimental \\
$-0.076(10)$ & \cite{ant} & experimental \\
$-0.084(11)$ & \cite{bak} & experimental \\
$-0.086(24)$ & \cite{kir} & experimental \\
$-0.091(9)$ & \cite{cho} & experimental \\
$-0.110(16)$ & \cite{ling} & experimental \\
$-0.138(7)$ & \cite{Esta} & experimental \\
       &            &           \\
$-0.05$ & \cite{BKM} & 1-loop chiral pert. theory \\
$-0.05$ & \cite{Pond} & pointlike meson model \\
$-0.06$ & \cite{Curry} & crossing-symmetric Regge model \\
$-0.07$ & \cite{Wein} & PCAC \\
$-0.074$ & \cite{lang} & coupled channel model \\
$-0.077$ & --- & this work (central value)\\
\end{tabular}
\label{table1}
\end{table}


\end{document}



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4 Sw
N
1397 1464 M
1397 1450 D
1411 1450 D
1411 1464 D
1397 1464 D
S
N
1400 1461 M
1400 1453 D
1408 1453 D
1408 1461 D
1400 1461 D
S
2 Sw
N
1473 1406 M
1473 1429 D
S
N
1473 1418 M
1419 1418 D
S
N
1419 1406 M
1419 1429 D
S
N
1448 1416 M
1448 1419 D
1444 1419 D
1444 1416 D
1448 1416 D
1446 1418 D
S
4 Sw
N
1439 1425 M
1439 1411 D
1453 1411 D
1453 1425 D
1439 1425 D
S
N
1442 1422 M
1442 1414 D
1450 1414 D
1450 1422 D
1442 1422 D
S
2 Sw
N
1392 1347 M
1392 1370 D
S
N
1392 1359 M
1356 1359 D
S
N
1356 1347 M
1356 1370 D
S
N
1376 1357 M
1376 1361 D
1372 1361 D
1372 1357 D
1376 1357 D
1374 1359 D
S
4 Sw
N
1367 1366 M
1367 1352 D
1381 1352 D
1381 1366 D
1367 1366 D
S
N
1370 1363 M
1370 1355 D
1378 1355 D
1378 1363 D
1370 1363 D
S
2 Sw
N
1416 1269 M
1416 1292 D
S
N
1416 1280 M
1374 1280 D
S
N
1374 1269 M
1374 1292 D
S
N
1397 1279 M
1397 1282 D
1393 1282 D
S
N
1393 1282 M
1393 1279 D
1397 1279 D
1395 1280 D
S
4 Sw
N
1388 1287 M
1388 1273 D
1402 1273 D
1402 1287 D
1388 1287 D
S
N
1391 1284 M
1391 1276 D
1399 1276 D
1399 1284 D
1391 1284 D
S
2 Sw
N
1458 1191 M
1458 1213 D
S
N
1458 1202 M
1398 1202 D
S
N
1398 1191 M
1398 1213 D
S
N
1430 1200 M
1430 1204 D
1426 1204 D
1426 1200 D
1430 1200 D
1428 1202 D
S
4 Sw
N
1421 1209 M
1421 1195 D
1435 1195 D
1435 1209 D
1421 1209 D
S
N
1424 1206 M
1424 1198 D
1432 1198 D
1432 1206 D
1424 1206 D
S
2 Sw
N
1542 1073 M
1542 1096 D
S
N
1542 1084 M
1482 1084 D
S
N
1482 1073 M
1482 1096 D
S
N
1514 1083 M
1514 1086 D
1510 1086 D
1510 1083 D
1514 1083 D
1512 1084 D
S
4 Sw
N
1505 1091 M
1505 1077 D
1519 1077 D
1519 1091 D
1505 1091 D
S
N
1508 1088 M
1508 1080 D
1516 1080 D
1516 1088 D
1508 1088 D
S
2 Sw
N
1218 2280 M
1146 2280 D
S
N
1170 2231 M
1146 2231 D
S
N
1170 2182 M
1146 2182 D
S
N
1170 2133 M
1146 2133 D
S
N
1170 2084 M
1146 2084 D
S
N
1218 2035 M
1146 2035 D
S
N
1170 1986 M
1146 1986 D
S
N
1170 1937 M
1146 1937 D
S
N
1170 1888 M
1146 1888 D
S
N
1170 1839 M
1146 1839 D
S
N
1218 1790 M
1146 1790 D
S
N
1170 1741 M
1146 1741 D
S
N
1170 1692 M
1146 1692 D
S
N
1170 1643 M
1146 1643 D
S
N
1170 1594 M
1146 1594 D
S
N
1218 1545 M
1146 1545 D
S
N
1170 1496 M
1146 1496 D
S
N
1170 1447 M
1146 1447 D
S
N
1170 1398 M
1146 1398 D
S
N
1170 1349 M
1146 1349 D
S
N
1218 1300 M
1146 1300 D
S
N
1170 1251 M
1146 1251 D
S
N
1170 1202 M
1146 1202 D
S
N
1170 1153 M
1146 1153 D
S
N
1170 1104 M
1146 1104 D
S
N
1218 1055 M
1146 1055 D
S
N
1170 1006 M
1146 1006 D
S
N
1170 957 M
1146 957 D
S
N
1170 908 M
1146 908 D
S
N
1170 859 M
1146 859 D
S
N
1218 810 M
1146 810 D
S
N
1106 2329 M
1104 2335 D
1098 2339 D
1088 2341 D
1082 2341 D
1072 2339 D
1066 2335 D
1064 2329 D
1064 2325 D
1066 2319 D
1072 2315 D
1082 2313 D
1088 2313 D
1098 2315 D
1104 2319 D
1106 2325 D
1106 2329 D
S
N
1106 2329 M
1104 2333 D
1102 2335 D
1098 2337 D
1088 2339 D
1082 2339 D
1072 2337 D
1068 2335 D
1066 2333 D
1064 2329 D
S
N
1064 2325 M
1066 2321 D
1068 2319 D
1072 2317 D
1082 2315 D
1088 2315 D
1098 2317 D
1102 2319 D
1104 2321 D
1106 2325 D
S
N
1068 2297 M
1066 2299 D
1064 2297 D
1066 2295 D
1068 2297 D
S
N
1106 2277 M
1086 2281 D
S
N
1086 2281 M
1090 2277 D
1092 2271 D
1092 2265 D
1090 2259 D
1086 2255 D
1080 2253 D
1076 2253 D
1070 2255 D
1066 2259 D
1064 2265 D
1064 2271 D
1066 2277 D
1068 2279 D
1072 2281 D
1074 2281 D
1076 2279 D
1074 2277 D
1072 2279 D
S
N
1092 2265 M
1090 2261 D
1086 2257 D
1080 2255 D
1076 2255 D
1070 2257 D
1066 2261 D
1064 2265 D
S
N
1106 2277 M
1106 2257 D
S
N
1104 2277 M
1104 2267 D
1106 2257 D
S
N
1106 2106 M
1104 2112 D
1098 2116 D
1088 2118 D
1082 2118 D
1072 2116 D
1066 2112 D
1064 2106 D
1064 2102 D
1066 2096 D
1072 2092 D
1082 2090 D
1088 2090 D
1098 2092 D
1104 2096 D
1106 2102 D
1106 2106 D
S
N
1106 2106 M
1104 2110 D
1102 2112 D
1098 2114 D
1088 2116 D
1082 2116 D
1072 2114 D
1068 2112 D
1066 2110 D
1064 2106 D
S
N
1064 2102 M
1066 2098 D
1068 2096 D
1072 2094 D
1082 2092 D
1088 2092 D
1098 2094 D
1102 2096 D
1104 2098 D
1106 2102 D
S
N
1068 2074 M
1066 2076 D
1064 2074 D
1066 2072 D
1068 2074 D
S
N
1106 2058 M
1094 2058 D
S
N
1098 2058 M
1102 2056 D
1106 2052 D
1106 2048 D
1100 2038 D
1100 2034 D
1102 2032 D
1106 2030 D
S
N
1102 2056 M
1104 2052 D
1104 2048 D
1100 2038 D
S
N
1106 2030 M
1100 2030 D
1094 2032 D
1084 2040 D
1080 2042 D
1074 2044 D
1064 2044 D
S
N
1094 2032 M
1084 2042 D
1080 2044 D
1074 2046 D
1064 2046 D
S
N
1106 2014 M
1086 2018 D
S
N
1086 2018 M
1090 2014 D
1092 2008 D
1092 2002 D
1090 1996 D
1086 1992 D
1080 1990 D
1076 1990 D
1070 1992 D
1066 1996 D
1064 2002 D
1064 2008 D
1066 2014 D
1068 2016 D
1072 2018 D
1074 2018 D
1076 2016 D
1074 2014 D
1072 2016 D
S
N
1092 2002 M
1090 1998 D
1086 1994 D
1080 1992 D
1076 1992 D
1070 1994 D
1066 1998 D
1064 2002 D
S
N
1106 2014 M
1106 1994 D
S
N
1104 2014 M
1104 2004 D
1106 1994 D
S
N
1098 1802 M
1100 1798 D
1106 1792 D
1064 1792 D
S
N
1104 1794 M
1064 1794 D
S
N
1064 1802 M
1064 1784 D
S
N
1098 1622 M
1100 1618 D
1106 1612 D
1064 1612 D
S
N
1104 1614 M
1064 1614 D
S
N
1064 1622 M
1064 1604 D
S
N
1068 1584 M
1066 1586 D
1064 1584 D
1066 1582 D
1068 1584 D
S
N
1098 1566 M
1096 1564 D
1094 1566 D
1096 1568 D
1098 1568 D
1102 1566 D
1104 1564 D
1106 1558 D
1106 1550 D
1104 1544 D
1102 1542 D
1098 1540 D
1094 1540 D
1090 1542 D
1086 1548 D
1082 1558 D
1080 1562 D
1076 1566 D
1070 1568 D
1064 1568 D
S
N
1106 1550 M
1104 1546 D
1102 1544 D
1098 1542 D
1094 1542 D
1090 1544 D
1086 1550 D
1082 1558 D
S
N
1068 1568 M
1070 1566 D
1070 1562 D
1066 1552 D
1066 1546 D
1068 1542 D
1070 1540 D
S
N
1070 1562 M
1064 1552 D
1064 1544 D
1066 1542 D
1070 1540 D
1074 1540 D
S
N
1106 1524 M
1086 1528 D
S
N
1086 1528 M
1090 1524 D
1092 1518 D
1092 1512 D
1090 1506 D
1086 1502 D
1080 1500 D
1076 1500 D
1070 1502 D
1066 1506 D
1064 1512 D
1064 1518 D
1066 1524 D
1068 1526 D
1072 1528 D
1074 1528 D
1076 1526 D
1074 1524 D
1072 1526 D
S
N
1092 1512 M
1090 1508 D
1086 1504 D
1080 1502 D
1076 1502 D
1070 1504 D
1066 1508 D
1064 1512 D
S
N
1106 1524 M
1106 1504 D
S
N
1104 1524 M
1104 1514 D
1106 1504 D
S
N
1098 1355 M
1100 1351 D
1106 1345 D
1064 1345 D
S
N
1104 1347 M
1064 1347 D
S
N
1064 1355 M
1064 1337 D
S
N
1068 1317 M
1066 1319 D
1064 1317 D
1066 1315 D
1068 1317 D
S
N
1106 1297 M
1086 1301 D
S
N
1086 1301 M
1090 1297 D
1092 1291 D
1092 1285 D
1090 1279 D
1086 1275 D
1080 1273 D
1076 1273 D
1070 1275 D
1066 1279 D
1064 1285 D
1064 1291 D
1066 1297 D
1068 1299 D
1072 1301 D
1074 1301 D
1076 1299 D
1074 1297 D
1072 1299 D
S
N
1092 1285 M
1090 1281 D
1086 1277 D
1080 1275 D
1076 1275 D
1070 1277 D
1066 1281 D
1064 1285 D
S
N
1106 1297 M
1106 1277 D
S
N
1104 1297 M
1104 1287 D
1106 1277 D
S
N
1098 1132 M
1100 1128 D
1106 1122 D
1064 1122 D
S
N
1104 1124 M
1064 1124 D
S
N
1064 1132 M
1064 1114 D
S
N
1068 1094 M
1066 1096 D
1064 1094 D
1066 1092 D
1068 1094 D
S
N
1106 1078 M
1094 1078 D
S
N
1098 1078 M
1102 1076 D
1106 1072 D
1106 1068 D
1100 1058 D
1100 1054 D
1102 1052 D
1106 1050 D
S
N
1102 1076 M
1104 1072 D
1104 1068 D
1100 1058 D
S
N
1106 1050 M
1100 1050 D
1094 1052 D
1084 1060 D
1080 1062 D
1074 1064 D
1064 1064 D
S
N
1094 1052 M
1084 1062 D
1080 1064 D
1074 1066 D
1064 1066 D
S
N
1106 1034 M
1086 1038 D
S
N
1086 1038 M
1090 1034 D
1092 1028 D
1092 1022 D
1090 1016 D
1086 1012 D
1080 1010 D
1076 1010 D
1070 1012 D
1066 1016 D
1064 1022 D
1064 1028 D
1066 1034 D
1068 1036 D
1072 1038 D
1074 1038 D
1076 1036 D
1074 1034 D
1072 1036 D
S
N
1092 1022 M
1090 1018 D
1086 1014 D
1080 1012 D
1076 1012 D
1070 1014 D
1066 1018 D
1064 1022 D
S
N
1106 1034 M
1106 1014 D
S
N
1104 1034 M
1104 1024 D
1106 1014 D
S
N
1098 826 M
1096 824 D
1094 826 D
1096 828 D
1098 828 D
1102 826 D
1104 824 D
1106 818 D
1106 810 D
1104 804 D
1102 802 D
1098 800 D
1094 800 D
1090 802 D
1086 808 D
1082 818 D
1080 822 D
1076 826 D
1070 828 D
1064 828 D
S
N
1106 810 M
1104 806 D
1102 804 D
1098 802 D
1094 802 D
1090 804 D
1086 810 D
1082 818 D
S
N
1068 828 M
1070 826 D
1070 822 D
1066 812 D
1066 806 D
1068 802 D
1070 800 D
S
N
1070 822 M
1064 812 D
1064 804 D
1066 802 D
1070 800 D
1074 800 D
S
N
2196 2280 M
2124 2280 D
S
N
2196 2231 M
2172 2231 D
S
N
2196 2182 M
2172 2182 D
S
N
2196 2133 M
2172 2133 D
S
N
2196 2084 M
2172 2084 D
S
N
2196 2035 M
2124 2035 D
S
N
2196 1986 M
2172 1986 D
S
N
2196 1937 M
2172 1937 D
S
N
2196 1888 M
2172 1888 D
S
N
2196 1839 M
2172 1839 D
S
N
2196 1790 M
2124 1790 D
S
N
2196 1741 M
2172 1741 D
S
N
2196 1692 M
2172 1692 D
S
N
2196 1643 M
2172 1643 D
S
N
2196 1594 M
2172 1594 D
S
N
2196 1545 M
2124 1545 D
S
N
2196 1496 M
2172 1496 D
S
N
2196 1447 M
2172 1447 D
S
N
2196 1398 M
2172 1398 D
S
N
2196 1349 M
2172 1349 D
S
N
2196 1300 M
2124 1300 D
S
N
2196 1251 M
2172 1251 D
S
N
2196 1202 M
2172 1202 D
S
N
2196 1153 M
2172 1153 D
S
N
2196 1104 M
2172 1104 D
S
N
2196 1055 M
2124 1055 D
S
N
2196 1006 M
2172 1006 D
S
N
2196 957 M
2172 957 D
S
N
2196 908 M
2172 908 D
S
N
2196 859 M
2172 859 D
S
N
2196 810 M
2124 810 D
S
N
1176 2256 M
1176 2280 D
S
N
1236 2256 M
1236 2280 D
S
N
1296 2208 M
1296 2280 D
S
N
1356 2256 M
1356 2280 D
S
N
1416 2256 M
1416 2280 D
S
N
1476 2256 M
1476 2280 D
S
N
1536 2256 M
1536 2280 D
S
N
1596 2208 M
1596 2280 D
S
N
1656 2256 M
1656 2280 D
S
N
1716 2256 M
1716 2280 D
S
N
1776 2256 M
1776 2280 D
S
N
1836 2256 M
1836 2280 D
S
N
1896 2208 M
1896 2280 D
S
N
1956 2256 M
1956 2280 D
S
N
2016 2256 M
2016 2280 D
S
N
2076 2256 M
2076 2280 D
S
N
2136 2256 M
2136 2280 D
S
N
2196 2208 M
2196 2280 D
S
N
1290 2426 M
1290 2390 D
S
N
1306 2374 M
1304 2372 D
1302 2374 D
1304 2376 D
1306 2376 D
1310 2374 D
1312 2372 D
1314 2366 D
1314 2358 D
1312 2352 D
1308 2350 D
1302 2350 D
1298 2352 D
1296 2358 D
1296 2364 D
S
N
1314 2358 M
1312 2354 D
1308 2352 D
1302 2352 D
1298 2354 D
1296 2358 D
S
N
1296 2358 M
1294 2354 D
1290 2350 D
1286 2348 D
1280 2348 D
1276 2350 D
1274 2352 D
1272 2358 D
1272 2366 D
1274 2372 D
1276 2374 D
1280 2376 D
1282 2376 D
1284 2374 D
1282 2372 D
1280 2374 D
S
N
1292 2352 M
1286 2350 D
1280 2350 D
1276 2352 D
1274 2354 D
1272 2358 D
S
N
1314 2324 M
1312 2330 D
1306 2334 D
1296 2336 D
1290 2336 D
1280 2334 D
1274 2330 D
1272 2324 D
1272 2320 D
1274 2314 D
1280 2310 D
1290 2308 D
1296 2308 D
1306 2310 D
1312 2314 D
1314 2320 D
1314 2324 D
S
N
1314 2324 M
1312 2328 D
1310 2330 D
1306 2332 D
1296 2334 D
1290 2334 D
1280 2332 D
1276 2330 D
1274 2328 D
1272 2324 D
S
N
1272 2320 M
1274 2316 D
1276 2314 D
1280 2312 D
1290 2310 D
1296 2310 D
1306 2312 D
1310 2314 D
1312 2316 D
1314 2320 D
S
N
1590 2426 M
1590 2390 D
S
N
1606 2374 M
1604 2372 D
1602 2374 D
1604 2376 D
1606 2376 D
1610 2374 D
1612 2372 D
1614 2366 D
1614 2358 D
1612 2352 D
1610 2350 D
1606 2348 D
1602 2348 D
1598 2350 D
1594 2356 D
1590 2366 D
1588 2370 D
1584 2374 D
1578 2376 D
1572 2376 D
S
N
1614 2358 M
1612 2354 D
1610 2352 D
1606 2350 D
1602 2350 D
1598 2352 D
1594 2358 D
1590 2366 D
S
N
1576 2376 M
1578 2374 D
1578 2370 D
1574 2360 D
1574 2354 D
1576 2350 D
1578 2348 D
S
N
1578 2370 M
1572 2360 D
1572 2352 D
1574 2350 D
1578 2348 D
1582 2348 D
S
N
1614 2324 M
1612 2330 D
1606 2334 D
1596 2336 D
1590 2336 D
1580 2334 D
1574 2330 D
1572 2324 D
1572 2320 D
1574 2314 D
1580 2310 D
1590 2308 D
1596 2308 D
1606 2310 D
1612 2314 D
1614 2320 D
1614 2324 D
S
N
1614 2324 M
1612 2328 D
1610 2330 D
1606 2332 D
1596 2334 D
1590 2334 D
1580 2332 D
1576 2330 D
1574 2328 D
1572 2324 D
S
N
1572 2320 M
1574 2316 D
1576 2314 D
1580 2312 D
1590 2310 D
1596 2310 D
1606 2312 D
1610 2314 D
1612 2316 D
1614 2320 D
S
N
1890 2426 M
1890 2390 D
S
N
1906 2370 M
1908 2366 D
1914 2360 D
1872 2360 D
S
N
1912 2362 M
1872 2362 D
S
N
1872 2370 M
1872 2352 D
S
N
1914 2324 M
1912 2330 D
1906 2334 D
1896 2336 D
1890 2336 D
1880 2334 D
1874 2330 D
1872 2324 D
1872 2320 D
1874 2314 D
1880 2310 D
1890 2308 D
1896 2308 D
1906 2310 D
1912 2314 D
1914 2320 D
1914 2324 D
S
N
1914 2324 M
1912 2328 D
1910 2330 D
1906 2332 D
1896 2334 D
1890 2334 D
1880 2332 D
1876 2330 D
1874 2328 D
1872 2324 D
S
N
1872 2320 M
1874 2316 D
1876 2314 D
1880 2312 D
1890 2310 D
1896 2310 D
1906 2312 D
1910 2314 D
1912 2316 D
1914 2320 D
S
N
2214 2352 M
2212 2358 D
2206 2362 D
2196 2364 D
2190 2364 D
2180 2362 D
2174 2358 D
2172 2352 D
2172 2348 D
2174 2342 D
2180 2338 D
2190 2336 D
2196 2336 D
2206 2338 D
2212 2342 D
2214 2348 D
2214 2352 D
S
N
2214 2352 M
2212 2356 D
2210 2358 D
2206 2360 D
2196 2362 D
2190 2362 D
2180 2360 D
2176 2358 D
2174 2356 D
2172 2352 D
S
N
2172 2348 M
2174 2344 D
2176 2342 D
2180 2340 D
2190 2338 D
2196 2338 D
2206 2340 D
2210 2342 D
2212 2344 D
2214 2348 D
S
N
1176 810 M
1176 834 D
S
N
1236 810 M
1236 834 D
S
N
1296 810 M
1296 882 D
S
N
1356 810 M
1356 834 D
S
N
1416 810 M
1416 834 D
S
N
1476 810 M
1476 834 D
S
N
1536 810 M
1536 834 D
S
N
1596 810 M
1596 882 D
S
N
1656 810 M
1656 834 D
S
N
1716 810 M
1716 834 D
S
N
1776 810 M
1776 834 D
S
N
1836 810 M
1836 834 D
S
N
1896 810 M
1896 882 D
S
N
1956 810 M
1956 834 D
S
N
2016 810 M
2016 834 D
S
N
2076 810 M
2076 834 D
S
N
2136 810 M
2136 834 D
S
N
2196 810 M
2196 882 D
S
N
2038 1986 M
2017 1986 D
S
N
2028 1986 M
2028 2153 D
S
N
2038 2153 M
2017 2153 D
S
N
2040 2058 M
2040 2081 D
S
N
2040 2069 M
2016 2069 D
S
N
2016 2058 M
2016 2081 D
S
N
2021 2076 M
2021 2062 D
2035 2062 D
2035 2076 D
2021 2076 D
S
N
1838 1839 M
1817 1839 D
S
N
1827 1839 M
1827 1986 D
S
N
1838 1986 M
1817 1986 D
S
N
1848 1901 M
1848 1924 D
S
N
1848 1912 M
1806 1912 D
S
N
1806 1901 M
1806 1924 D
S
N
1820 1919 M
1820 1906 D
1834 1906 D
1834 1919 D
1820 1919 D
S
N
1699 1839 M
1679 1839 D
S
N
1689 1839 M
1689 1692 D
S
N
1699 1692 M
1679 1692 D
S
N
1722 1754 M
1722 1777 D
S
N
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S
N
1656 1754 M
1656 1777 D
S
N
1682 1772 M
1682 1759 D
1696 1759 D
1696 1772 D
1682 1772 D
S
N
1693 1545 M
1672 1545 D
S
N
1683 1545 M
1683 1692 D
S
N
1693 1692 M
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S
N
1743 1607 M
1743 1630 D
S
N
1743 1618 M
1623 1618 D
S
N
1623 1607 M
1623 1630 D
S
N
1676 1625 M
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1690 1612 D
1690 1625 D
1676 1625 D
S
4 Sw
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N
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2173 2148 D
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2047 2100 D
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2036 2094 D
2030 2092 D
2024 2089 D
2018 2086 D
2012 2083 D
2006 2080 D
2000 2076 D
1994 2073 D
1988 2070 D
1981 2067 D
1975 2063 D
1969 2060 D
1962 2057 D
1956 2053 D
1949 2050 D
1943 2046 D
1936 2043 D
1929 2039 D
1923 2035 D
1916 2032 D
1909 2028 D
1902 2024 D
1895 2020 D
1888 2016 D
1882 2013 D
1875 2009 D
1868 2005 D
1861 2001 D
1854 1997 D
1847 1993 D
1840 1989 D
1832 1985 D
1825 1981 D
1818 1976 D
1811 1972 D
1804 1968 D
1797 1964 D
1790 1960 D
1783 1955 D
1776 1951 D
1768 1947 D
1761 1942 D
1754 1938 D
1747 1934 D
1740 1929 D
1733 1925 D
1726 1920 D
1719 1916 D
1712 1911 D
1705 1907 D
1698 1902 D
1691 1898 D
1684 1893 D
1677 1888 D
1670 1884 D
1663 1879 D
1656 1874 D
1649 1870 D
1642 1865 D
1636 1860 D
1629 1856 D
1622 1851 D
1616 1846 D
1609 1841 D
1603 1836 D
1596 1832 D
1590 1827 D
1583 1822 D
1577 1817 D
1570 1812 D
1564 1807 D
1558 1802 D
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1522 1772 D
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1451 1706 D
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1334 1539 D
1331 1534 D
1329 1528 D
1327 1523 D
1324 1517 D
1322 1511 D
1320 1506 D
1318 1500 D
1316 1495 D
1314 1489 D
1313 1484 D
1311 1478 D
1309 1472 D
1308 1467 D
1306 1461 D
1305 1455 D
1304 1450 D
1303 1444 D
1301 1438 D
1300 1433 D
1299 1427 D
1298 1421 D
1298 1416 D
1297 1410 D
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1296 1399 D
1295 1393 D
1295 1387 D
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1294 1370 D
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1293 1359 D
1293 1353 D
1293 1347 D
1293 1341 D
1293 1335 D
1294 1330 D
1294 1324 D
1294 1318 D
S
N
1294 1318 M
1295 1312 D
1295 1307 D
1296 1301 D
1296 1295 D
1297 1289 D
1298 1283 D
1298 1277 D
1299 1272 D
1300 1266 D
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1359 1058 D
1361 1052 D
1363 1046 D
1366 1040 D
1368 1034 D
1370 1028 D
1373 1022 D
1375 1016 D
S
N
1375 1016 M
1378 1010 D
1380 1004 D
1383 998 D
1385 992 D
1388 986 D
1390 980 D
1393 974 D
1395 968 D
1398 962 D
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1418 914 D
1421 908 D
1423 902 D
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1429 889 D
1431 883 D
1434 877 D
1437 871 D
1439 865 D
1442 859 D
1444 853 D
1447 847 D
1450 841 D
1452 834 D
1455 828 D
1458 822 D
1460 816 D
1463 810 D
1463 810 D
S
2 Sw
[39] 0 Sd
N
2186 2149 M
2183 2149 D
2180 2148 D
2177 2148 D
2173 2147 D
2170 2146 D
2167 2146 D
2163 2145 D
2160 2144 D
2156 2143 D
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2142 2137 D
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2131 2132 D
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2123 2128 D
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2071 2100 D
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2062 2094 D
2057 2092 D
2052 2089 D
2047 2086 D
2042 2083 D
2037 2080 D
2032 2076 D
2027 2073 D
2022 2070 D
2016 2067 D
2011 2063 D
2006 2060 D
2000 2057 D
1995 2053 D
1990 2050 D
1984 2046 D
1979 2043 D
1973 2039 D
1967 2035 D
1962 2032 D
1956 2028 D
1950 2024 D
1945 2020 D
1939 2016 D
1933 2013 D
1928 2009 D
1922 2005 D
1916 2001 D
1910 1997 D
1904 1993 D
1898 1989 D
1893 1985 D
1887 1981 D
1881 1976 D
1875 1972 D
1869 1968 D
1863 1964 D
1857 1960 D
1851 1955 D
1845 1951 D
1839 1947 D
1834 1942 D
1828 1938 D
1822 1934 D
1816 1929 D
1810 1925 D
1804 1920 D
1798 1916 D
1793 1911 D
1787 1907 D
1781 1902 D
1775 1898 D
1769 1893 D
1764 1888 D
1758 1884 D
1752 1879 D
1747 1874 D
1741 1870 D
1736 1865 D
1730 1860 D
1724 1856 D
1719 1851 D
1714 1846 D
1708 1841 D
1703 1836 D
1697 1832 D
1692 1827 D
1687 1822 D
1682 1817 D
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1671 1807 D
1666 1802 D
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1637 1772 D
1632 1767 D
1627 1762 D
1623 1757 D
1618 1752 D
1614 1747 D
1609 1742 D
1605 1737 D
1600 1732 D
1596 1727 D
1592 1721 D
1588 1716 D
1583 1711 D
1579 1706 D
1575 1701 D
1571 1695 D
1568 1690 D
1564 1685 D
1560 1680 D
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1553 1669 D
1549 1664 D
1546 1658 D
1542 1653 D
1539 1648 D
1536 1642 D
1532 1637 D
1529 1632 D
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1523 1621 D
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1482 1528 D
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1478 1517 D
1476 1511 D
1475 1506 D
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1472 1495 D
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1469 1484 D
1468 1478 D
1466 1472 D
1465 1467 D
1464 1461 D
1463 1455 D
1462 1450 D
1461 1444 D
1460 1438 D
1460 1433 D
1459 1427 D
1458 1421 D
1458 1416 D
1457 1410 D
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1456 1399 D
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1455 1376 D
1455 1370 D
1455 1364 D
1455 1359 D
1455 1353 D
1455 1347 D
1455 1341 D
1455 1335 D
1455 1330 D
1456 1324 D
1456 1318 D
S
N
1456 1318 M
1456 1312 D
1457 1307 D
1457 1301 D
1458 1295 D
1458 1289 D
1459 1283 D
1460 1277 D
1460 1272 D
1461 1266 D
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1478 1178 D
1479 1172 D
1480 1166 D
1482 1160 D
1483 1154 D
1485 1148 D
1486 1142 D
1488 1136 D
1489 1130 D
1491 1124 D
1493 1118 D
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1498 1100 D
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1503 1082 D
1505 1076 D
1507 1070 D
1508 1064 D
1510 1058 D
1512 1052 D
1514 1046 D
1516 1040 D
1518 1034 D
1520 1028 D
1522 1022 D
1524 1016 D
S
N
1524 1016 M
1526 1010 D
1528 1004 D
1530 998 D
1532 992 D
1534 986 D
1536 980 D
1538 974 D
1540 968 D
1542 962 D
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1559 914 D
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1585 841 D
1587 834 D
1589 828 D
1591 822 D
1593 816 D
1595 810 D
1595 810 D
S
[] 0 Sd
N
2187 2149 M
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2180 2148 D
2177 2148 D
2174 2147 D
2170 2146 D
2167 2146 D
2164 2145 D
2160 2144 D
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2055 2089 D
2050 2086 D
2045 2083 D
2040 2080 D
2035 2076 D
2030 2073 D
2025 2070 D
2020 2067 D
2015 2063 D
2010 2060 D
2004 2057 D
1999 2053 D
1994 2050 D
1988 2046 D
1983 2043 D
1977 2039 D
1972 2035 D
1966 2032 D
1961 2028 D
1955 2024 D
1949 2020 D
1944 2016 D
1938 2013 D
1932 2009 D
1927 2005 D
1921 2001 D
1915 1997 D
1909 1993 D
1904 1989 D
1898 1985 D
1892 1981 D
1886 1976 D
1880 1972 D
1875 1968 D
1869 1964 D
1863 1960 D
1857 1955 D
1851 1951 D
1845 1947 D
1839 1942 D
1834 1938 D
1828 1934 D
1822 1929 D
1816 1925 D
1810 1920 D
1804 1916 D
1799 1911 D
1793 1907 D
1787 1902 D
1781 1898 D
1776 1893 D
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1764 1884 D
1759 1879 D
1753 1874 D
1747 1870 D
1742 1865 D
1736 1860 D
1731 1856 D
1725 1851 D
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1714 1841 D
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1451 1335 D
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1451 1324 D
1452 1318 D
S
N
1452 1318 M
1452 1312 D
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1452 1301 D
1453 1295 D
1453 1289 D
1454 1283 D
1454 1277 D
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1507 1040 D
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1512 1022 D
1514 1016 D
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N
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1528 974 D
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N
1241 2690 M
1237 2692 D
1233 2692 D
1227 2690 D
1223 2684 D
1221 2678 D
1221 2672 D
1223 2668 D
1225 2666 D
1229 2664 D
1233 2664 D
1239 2666 D
1243 2672 D
1245 2678 D
1245 2684 D
1243 2688 D
1235 2698 D
1233 2702 D
1233 2706 D
1235 2708 D
1239 2708 D
1243 2706 D
1247 2702 D
S
N
1233 2692 M
1229 2690 D
1225 2684 D
1223 2678 D
1223 2670 D
1225 2666 D
S
N
1233 2664 M
1237 2666 D
1241 2672 D
1243 2678 D
1243 2686 D
1241 2690 D
1237 2696 D
1235 2700 D
1235 2704 D
1237 2706 D
1241 2706 D
1247 2702 D
S
N
1262 2676 M
1262 2648 D
S
N
1264 2676 M
1264 2648 D
S
N
1258 2676 M
1274 2676 D
1278 2675 D
1280 2673 D
1281 2671 D
1281 2667 D
1280 2664 D
1278 2663 D
1274 2661 D
1264 2661 D
S
N
1274 2676 M
1277 2675 D
1278 2673 D
1280 2671 D
1280 2667 D
1278 2664 D
1277 2663 D
1274 2661 D
S
N
1258 2648 M
1268 2648 D
S
N
1300 2729 M
1297 2727 D
1294 2723 D
1292 2717 D
1290 2711 D
1290 2705 D
1292 2699 D
1294 2693 D
1297 2689 D
1300 2687 D
S
N
1297 2727 M
1294 2721 D
1293 2717 D
1292 2711 D
1292 2705 D
1293 2699 D
1294 2695 D
1297 2689 D
S
N
1309 2719 M
1310 2717 D
1309 2716 D
1308 2717 D
1308 2719 D
1309 2721 D
1310 2723 D
1314 2724 D
1320 2724 D
1324 2723 D
1325 2720 D
1325 2716 D
1324 2713 D
1320 2712 D
1316 2712 D
S
N
1320 2724 M
1322 2723 D
1324 2720 D
1324 2716 D
1322 2713 D
1320 2712 D
S
N
1320 2712 M
1322 2711 D
1325 2708 D
1326 2705 D
1326 2701 D
1325 2699 D
1324 2697 D
1320 2696 D
1314 2696 D
1310 2697 D
1309 2699 D
1308 2701 D
1308 2703 D
1309 2704 D
1310 2703 D
1309 2701 D
S
N
1324 2709 M
1325 2705 D
1325 2701 D
1324 2699 D
1322 2697 D
1320 2696 D
S
N
1334 2729 M
1337 2727 D
1340 2723 D
1342 2717 D
1344 2711 D
1344 2705 D
1342 2699 D
1340 2693 D
1337 2689 D
1334 2687 D
S
N
1337 2727 M
1340 2721 D
1341 2717 D
1342 2711 D
1342 2705 D
1341 2699 D
1340 2695 D
1337 2689 D
S
N
1400 2714 M
1396 2710 D
1392 2704 D
1388 2696 D
1386 2686 D
1386 2678 D
1388 2668 D
1392 2660 D
1396 2654 D
1400 2650 D
S
N
1396 2710 M
1392 2702 D
1390 2696 D
1388 2686 D
1388 2678 D
1390 2668 D
1392 2662 D
1396 2654 D
S
N
1436 2706 M
1436 2664 D
S
N
1438 2706 M
1438 2664 D
S
N
1436 2686 M
1432 2690 D
1428 2692 D
1424 2692 D
1418 2690 D
1414 2686 D
1412 2680 D
1412 2676 D
1414 2670 D
1418 2666 D
1424 2664 D
1428 2664 D
1432 2666 D
1436 2670 D
S
N
1424 2692 M
1420 2690 D
1416 2686 D
1414 2680 D
1414 2676 D
1416 2670 D
1420 2666 D
1424 2664 D
S
N
1430 2706 M
1438 2706 D
S
N
1436 2664 M
1444 2664 D
S
N
1456 2680 M
1480 2680 D
1480 2684 D
1478 2688 D
1476 2690 D
1472 2692 D
1466 2692 D
1460 2690 D
1456 2686 D
1454 2680 D
1454 2676 D
1456 2670 D
1460 2666 D
1466 2664 D
1470 2664 D
1476 2666 D
1480 2670 D
S
N
1478 2680 M
1478 2686 D
1476 2690 D
S
N
1466 2692 M
1462 2690 D
1458 2686 D
1456 2680 D
1456 2676 D
1458 2670 D
1462 2666 D
1466 2664 D
S
N
1502 2692 M
1498 2690 D
1496 2688 D
1494 2684 D
1494 2680 D
1496 2676 D
1498 2674 D
1502 2672 D
1506 2672 D
1510 2674 D
1512 2676 D
1514 2680 D
1514 2684 D
1512 2688 D
1510 2690 D
1506 2692 D
1502 2692 D
S
N
1498 2690 M
1496 2686 D
1496 2678 D
1498 2674 D
S
N
1510 2674 M
1512 2678 D
1512 2686 D
1510 2690 D
S
N
1512 2688 M
1514 2690 D
1518 2692 D
1518 2690 D
1514 2690 D
S
N
1496 2676 M
1494 2674 D
1492 2670 D
1492 2668 D
1494 2664 D
1500 2662 D
1510 2662 D
1516 2660 D
1518 2658 D
S
N
1492 2668 M
1494 2666 D
1500 2664 D
1510 2664 D
1516 2662 D
1518 2658 D
1518 2656 D
1516 2652 D
1510 2650 D
1498 2650 D
1492 2652 D
1490 2656 D
1490 2658 D
1492 2662 D
1498 2664 D
S
N
1534 2692 M
1534 2664 D
S
N
1536 2692 M
1536 2664 D
S
N
1536 2680 M
1538 2686 D
1542 2690 D
1546 2692 D
1552 2692 D
1554 2690 D
1554 2688 D
1552 2686 D
1550 2688 D
1552 2690 D
S
N
1528 2692 M
1536 2692 D
S
N
1528 2664 M
1542 2664 D
S
N
1566 2680 M
1590 2680 D
1590 2684 D
1588 2688 D
1586 2690 D
1582 2692 D
1576 2692 D
1570 2690 D
1566 2686 D
1564 2680 D
1564 2676 D
1566 2670 D
1570 2666 D
1576 2664 D
1580 2664 D
1586 2666 D
1590 2670 D
S
N
1588 2680 M
1588 2686 D
1586 2690 D
S
N
1576 2692 M
1572 2690 D
1568 2686 D
1566 2680 D
1566 2676 D
1568 2670 D
1572 2666 D
1576 2664 D
S
N
1604 2680 M
1628 2680 D
1628 2684 D
1626 2688 D
1624 2690 D
1620 2692 D
1614 2692 D
1608 2690 D
1604 2686 D
1602 2680 D
1602 2676 D
1604 2670 D
1608 2666 D
1614 2664 D
1618 2664 D
1624 2666 D
1628 2670 D
S
N
1626 2680 M
1626 2686 D
1624 2690 D
S
N
1614 2692 M
1610 2690 D
1606 2686 D
1604 2680 D
1604 2676 D
1606 2670 D
1610 2666 D
1614 2664 D
S
N
1660 2688 M
1662 2692 D
1662 2684 D
1660 2688 D
1658 2690 D
1654 2692 D
1646 2692 D
1642 2690 D
1640 2688 D
1640 2684 D
1642 2682 D
1646 2680 D
1656 2676 D
1660 2674 D
1662 2672 D
S
N
1640 2686 M
1642 2684 D
1646 2682 D
1656 2678 D
1660 2676 D
1662 2674 D
1662 2668 D
1660 2666 D
1656 2664 D
1648 2664 D
1644 2666 D
1642 2668 D
1640 2672 D
1640 2664 D
1642 2668 D
S
N
1674 2714 M
1678 2710 D
1682 2704 D
1686 2696 D
1688 2686 D
1688 2678 D
1686 2668 D
1682 2660 D
1678 2654 D
1674 2650 D
S
N
1678 2710 M
1682 2702 D
1684 2696 D
1686 2686 D
1686 2678 D
1684 2668 D
1682 2662 D
1678 2654 D
S
N
2196 2280 M
1146 2280 D
S
N
1146 2280 M
1146 810 D
S
N
1146 810 M
2196 810 D
S
N
2196 810 M
2196 2280 D
S
N
1776 1759 M
1776 1782 D
S
N
1776 1770 M
1671 1770 D
S
N
1671 1759 M
1671 1782 D
S
N
1725 1769 M
1725 1772 D
1722 1772 D
1722 1769 D
1725 1769 D
1724 1770 D
S
4 Sw
N
1717 1777 M
1717 1763 D
1730 1763 D
1730 1777 D
1717 1777 D
S
N
1720 1774 M
1720 1766 D
1727 1766 D
1727 1774 D
1720 1774 D
S
2 Sw
N
1960 1720 M
1960 1743 D
S
N
1960 1731 M
1802 1731 D
S
N
1802 1720 M
1802 1743 D
S
N
1883 1729 M
1883 1733 D
1879 1733 D
1879 1729 D
1883 1729 D
1881 1731 D
S
4 Sw
N
1874 1738 M
1874 1724 D
1888 1724 D
1888 1738 D
1874 1738 D
S
N
1877 1735 M
1877 1727 D
1885 1727 D
1885 1735 D
1877 1735 D
S
2 Sw
N
1776 1681 M
1776 1703 D
S
N
1776 1692 M
1618 1692 D
S
N
1618 1681 M
1618 1703 D
S
N
1699 1690 M
1699 1694 D
1695 1694 D
1695 1690 D
1699 1690 D
1697 1692 D
S
4 Sw
N
1690 1699 M
1690 1685 D
1704 1685 D
1704 1699 D
1690 1699 D
S
N
1693 1696 M
1693 1688 D
1701 1688 D
1701 1696 D
1693 1696 D
S
2 Sw
N
1724 1641 M
1724 1664 D
S
N
1724 1653 M
1566 1653 D
S
N
1566 1641 M
1566 1664 D
S
N
1647 1651 M
1647 1655 D
1643 1655 D
1643 1651 D
1647 1651 D
1645 1653 D
S
4 Sw
N
1638 1660 M
1638 1646 D
1652 1646 D
1652 1660 D
1638 1660 D
S
N
1641 1657 M
1641 1649 D
1649 1649 D
1649 1657 D
1641 1657 D
S
2 Sw
N
1855 1602 M
1855 1625 D
S
N
1855 1614 M
1697 1614 D
S
N
1697 1602 M
1697 1625 D
S
N
1778 1612 M
1778 1615 D
1774 1615 D
1774 1612 D
1778 1612 D
1776 1614 D
S
4 Sw
N
1769 1621 M
1769 1607 D
1783 1607 D
1783 1621 D
1769 1621 D
S
N
1772 1618 M
1772 1610 D
1780 1610 D
1780 1618 D
1772 1618 D
S
2 Sw
N
1855 1563 M
1855 1586 D
S
N
1855 1574 M
1697 1574 D
S
N
1697 1563 M
1697 1586 D
S
N
1778 1573 M
1778 1576 D
1774 1576 D
1774 1573 D
1778 1573 D
1776 1574 D
S
4 Sw
N
1769 1581 M
1769 1567 D
1783 1567 D
1783 1581 D
1769 1581 D
S
N
1772 1578 M
1772 1570 D
1780 1570 D
1780 1578 D
1772 1578 D
S
2 Sw
N
1855 1524 M
1855 1547 D
S
N
1855 1535 M
1697 1535 D
S
N
1697 1524 M
1697 1547 D
S
N
1778 1533 M
1778 1537 D
1774 1537 D
1774 1533 D
1778 1533 D
1776 1535 D
S
4 Sw
N
1769 1542 M
1769 1528 D
1783 1528 D
1783 1542 D
1769 1542 D
S
N
1772 1539 M
1772 1531 D
1780 1531 D
1780 1539 D
1772 1539 D
S
2 Sw
N
2012 1485 M
2012 1507 D
S
N
2012 1496 M
1802 1496 D
S
N
1802 1485 M
1802 1507 D
S
N
1909 1494 M
1909 1498 D
1905 1498 D
1905 1494 D
1909 1494 D
1907 1496 D
S
4 Sw
N
1900 1503 M
1900 1489 D
1914 1489 D
1914 1503 D
1900 1503 D
S
N
1903 1500 M
1903 1492 D
1911 1492 D
1911 1500 D
1903 1500 D
S
2 Sw
N
1855 1445 M
1855 1468 D
S
N
1855 1457 M
1645 1457 D
S
N
1645 1445 M
1645 1468 D
S
N
1752 1455 M
1752 1459 D
1748 1459 D
1748 1455 D
1752 1455 D
1750 1457 D
S
4 Sw
N
1743 1464 M
1743 1450 D
1757 1450 D
1757 1464 D
1743 1464 D
S
N
1746 1461 M
1746 1453 D
1754 1453 D
1754 1461 D
1746 1461 D
S
2 Sw
N
1960 1406 M
1960 1429 D
S
N
1960 1418 M
1750 1418 D
S
N
1750 1406 M
1750 1429 D
S
N
1857 1416 M
1857 1419 D
1853 1419 D
1853 1416 D
1857 1416 D
1855 1418 D
S
4 Sw
N
1848 1425 M
1848 1411 D
1862 1411 D
1862 1425 D
1848 1425 D
S
N
1851 1422 M
1851 1414 D
1859 1414 D
1859 1422 D
1851 1422 D
S
2 Sw
N
1697 1347 M
1697 1370 D
S
N
1697 1359 M
1540 1359 D
S
N
1540 1347 M
1540 1370 D
S
N
1620 1357 M
1620 1361 D
1617 1361 D
1617 1357 D
1620 1357 D
1618 1359 D
S
4 Sw
N
1612 1366 M
1612 1352 D
1625 1352 D
1625 1366 D
1612 1366 D
S
N
1615 1363 M
1615 1355 D
1622 1355 D
1622 1363 D
1615 1363 D
S
2 Sw
N
1382 1269 M
1382 1292 D
S
N
1382 1280 M
1225 1280 D
S
N
1225 1269 M
1225 1292 D
S
N
1305 1279 M
1305 1282 D
1302 1282 D
1302 1279 D
1305 1279 D
1303 1280 D
S
4 Sw
N
1297 1287 M
1297 1273 D
1310 1273 D
1310 1287 D
1297 1287 D
S
N
1300 1284 M
1300 1276 D
1307 1276 D
1307 1284 D
1300 1284 D
S
2 Sw
N
1487 1191 M
1487 1213 D
S
N
1487 1202 M
1277 1202 D
S
N
1277 1191 M
1277 1213 D
S
N
1384 1200 M
1384 1204 D
1380 1204 D
1380 1200 D
1384 1200 D
1382 1202 D
S
4 Sw
N
1375 1209 M
1375 1195 D
1389 1195 D
1389 1209 D
1375 1209 D
S
N
1378 1206 M
1378 1198 D
1386 1198 D
1386 1206 D
1378 1206 D
S
2 Sw
N
1408 1073 M
1408 1096 D
S
N
1408 1084 M
1198 1084 D
S
N
1198 1073 M
1198 1096 D
S
N
1305 1083 M
1305 1086 D
1302 1086 D
1302 1083 D
1305 1083 D
1303 1084 D
S
4 Sw
N
1297 1091 M
1297 1077 D
1310 1077 D
1310 1091 D
1297 1091 D
S
N
1300 1088 M
1300 1080 D
1307 1080 D
1307 1088 D
1300 1088 D
S
2 Sw
N
1218 2280 M
1146 2280 D
S
N
1170 2231 M
1146 2231 D
S
N
1170 2182 M
1146 2182 D
S
N
1170 2133 M
1146 2133 D
S
N
1170 2084 M
1146 2084 D
S
N
1218 2035 M
1146 2035 D
S
N
1170 1986 M
1146 1986 D
S
N
1170 1937 M
1146 1937 D
S
N
1170 1888 M
1146 1888 D
S
N
1170 1839 M
1146 1839 D
S
N
1218 1790 M
1146 1790 D
S
N
1170 1741 M
1146 1741 D
S
N
1170 1692 M
1146 1692 D
S
N
1170 1643 M
1146 1643 D
S
N
1170 1594 M
1146 1594 D
S
N
1218 1545 M
1146 1545 D
S
N
1170 1496 M
1146 1496 D
S
N
1170 1447 M
1146 1447 D
S
N
1170 1398 M
1146 1398 D
S
N
1170 1349 M
1146 1349 D
S
N
1218 1300 M
1146 1300 D
S
N
1170 1251 M
1146 1251 D
S
N
1170 1202 M
1146 1202 D
S
N
1170 1153 M
1146 1153 D
S
N
1170 1104 M
1146 1104 D
S
N
1218 1055 M
1146 1055 D
S
N
1170 1006 M
1146 1006 D
S
N
1170 957 M
1146 957 D
S
N
1170 908 M
1146 908 D
S
N
1170 859 M
1146 859 D
S
N
1218 810 M
1146 810 D
S
N
1106 2329 M
1104 2335 D
1098 2339 D
1088 2341 D
1082 2341 D
1072 2339 D
1066 2335 D
1064 2329 D
1064 2325 D
1066 2319 D
1072 2315 D
1082 2313 D
1088 2313 D
1098 2315 D
1104 2319 D
1106 2325 D
1106 2329 D
S
N
1106 2329 M
1104 2333 D
1102 2335 D
1098 2337 D
1088 2339 D
1082 2339 D
1072 2337 D
1068 2335 D
1066 2333 D
1064 2329 D
S
N
1064 2325 M
1066 2321 D
1068 2319 D
1072 2317 D
1082 2315 D
1088 2315 D
1098 2317 D
1102 2319 D
1104 2321 D
1106 2325 D
S
N
1068 2297 M
1066 2299 D
1064 2297 D
1066 2295 D
1068 2297 D
S
N
1106 2277 M
1086 2281 D
S
N
1086 2281 M
1090 2277 D
1092 2271 D
1092 2265 D
1090 2259 D
1086 2255 D
1080 2253 D
1076 2253 D
1070 2255 D
1066 2259 D
1064 2265 D
1064 2271 D
1066 2277 D
1068 2279 D
1072 2281 D
1074 2281 D
1076 2279 D
1074 2277 D
1072 2279 D
S
N
1092 2265 M
1090 2261 D
1086 2257 D
1080 2255 D
1076 2255 D
1070 2257 D
1066 2261 D
1064 2265 D
S
N
1106 2277 M
1106 2257 D
S
N
1104 2277 M
1104 2267 D
1106 2257 D
S
N
1106 2106 M
1104 2112 D
1098 2116 D
1088 2118 D
1082 2118 D
1072 2116 D
1066 2112 D
1064 2106 D
1064 2102 D
1066 2096 D
1072 2092 D
1082 2090 D
1088 2090 D
1098 2092 D
1104 2096 D
1106 2102 D
1106 2106 D
S
N
1106 2106 M
1104 2110 D
1102 2112 D
1098 2114 D
1088 2116 D
1082 2116 D
1072 2114 D
1068 2112 D
1066 2110 D
1064 2106 D
S
N
1064 2102 M
1066 2098 D
1068 2096 D
1072 2094 D
1082 2092 D
1088 2092 D
1098 2094 D
1102 2096 D
1104 2098 D
1106 2102 D
S
N
1068 2074 M
1066 2076 D
1064 2074 D
1066 2072 D
1068 2074 D
S
N
1106 2058 M
1094 2058 D
S
N
1098 2058 M
1102 2056 D
1106 2052 D
1106 2048 D
1100 2038 D
1100 2034 D
1102 2032 D
1106 2030 D
S
N
1102 2056 M
1104 2052 D
1104 2048 D
1100 2038 D
S
N
1106 2030 M
1100 2030 D
1094 2032 D
1084 2040 D
1080 2042 D
1074 2044 D
1064 2044 D
S
N
1094 2032 M
1084 2042 D
1080 2044 D
1074 2046 D
1064 2046 D
S
N
1106 2014 M
1086 2018 D
S
N
1086 2018 M
1090 2014 D
1092 2008 D
1092 2002 D
1090 1996 D
1086 1992 D
1080 1990 D
1076 1990 D
1070 1992 D
1066 1996 D
1064 2002 D
1064 2008 D
1066 2014 D
1068 2016 D
1072 2018 D
1074 2018 D
1076 2016 D
1074 2014 D
1072 2016 D
S
N
1092 2002 M
1090 1998 D
1086 1994 D
1080 1992 D
1076 1992 D
1070 1994 D
1066 1998 D
1064 2002 D
S
N
1106 2014 M
1106 1994 D
S
N
1104 2014 M
1104 2004 D
1106 1994 D
S
N
1098 1802 M
1100 1798 D
1106 1792 D
1064 1792 D
S
N
1104 1794 M
1064 1794 D
S
N
1064 1802 M
1064 1784 D
S
N
1098 1622 M
1100 1618 D
1106 1612 D
1064 1612 D
S
N
1104 1614 M
1064 1614 D
S
N
1064 1622 M
1064 1604 D
S
N
1068 1584 M
1066 1586 D
1064 1584 D
1066 1582 D
1068 1584 D
S
N
1098 1566 M
1096 1564 D
1094 1566 D
1096 1568 D
1098 1568 D
1102 1566 D
1104 1564 D
1106 1558 D
1106 1550 D
1104 1544 D
1102 1542 D
1098 1540 D
1094 1540 D
1090 1542 D
1086 1548 D
1082 1558 D
1080 1562 D
1076 1566 D
1070 1568 D
1064 1568 D
S
N
1106 1550 M
1104 1546 D
1102 1544 D
1098 1542 D
1094 1542 D
1090 1544 D
1086 1550 D
1082 1558 D
S
N
1068 1568 M
1070 1566 D
1070 1562 D
1066 1552 D
1066 1546 D
1068 1542 D
1070 1540 D
S
N
1070 1562 M
1064 1552 D
1064 1544 D
1066 1542 D
1070 1540 D
1074 1540 D
S
N
1106 1524 M
1086 1528 D
S
N
1086 1528 M
1090 1524 D
1092 1518 D
1092 1512 D
1090 1506 D
1086 1502 D
1080 1500 D
1076 1500 D
1070 1502 D
1066 1506 D
1064 1512 D
1064 1518 D
1066 1524 D
1068 1526 D
1072 1528 D
1074 1528 D
1076 1526 D
1074 1524 D
1072 1526 D
S
N
1092 1512 M
1090 1508 D
1086 1504 D
1080 1502 D
1076 1502 D
1070 1504 D
1066 1508 D
1064 1512 D
S
N
1106 1524 M
1106 1504 D
S
N
1104 1524 M
1104 1514 D
1106 1504 D
S
N
1098 1355 M
1100 1351 D
1106 1345 D
1064 1345 D
S
N
1104 1347 M
1064 1347 D
S
N
1064 1355 M
1064 1337 D
S
N
1068 1317 M
1066 1319 D
1064 1317 D
1066 1315 D
1068 1317 D
S
N
1106 1297 M
1086 1301 D
S
N
1086 1301 M
1090 1297 D
1092 1291 D
1092 1285 D
1090 1279 D
1086 1275 D
1080 1273 D
1076 1273 D
1070 1275 D
1066 1279 D
1064 1285 D
1064 1291 D
1066 1297 D
1068 1299 D
1072 1301 D
1074 1301 D
1076 1299 D
1074 1297 D
1072 1299 D
S
N
1092 1285 M
1090 1281 D
1086 1277 D
1080 1275 D
1076 1275 D
1070 1277 D
1066 1281 D
1064 1285 D
S
N
1106 1297 M
1106 1277 D
S
N
1104 1297 M
1104 1287 D
1106 1277 D
S
N
1098 1132 M
1100 1128 D
1106 1122 D
1064 1122 D
S
N
1104 1124 M
1064 1124 D
S
N
1064 1132 M
1064 1114 D
S
N
1068 1094 M
1066 1096 D
1064 1094 D
1066 1092 D
1068 1094 D
S
N
1106 1078 M
1094 1078 D
S
N
1098 1078 M
1102 1076 D
1106 1072 D
1106 1068 D
1100 1058 D
1100 1054 D
1102 1052 D
1106 1050 D
S
N
1102 1076 M
1104 1072 D
1104 1068 D
1100 1058 D
S
N
1106 1050 M
1100 1050 D
1094 1052 D
1084 1060 D
1080 1062 D
1074 1064 D
1064 1064 D
S
N
1094 1052 M
1084 1062 D
1080 1064 D
1074 1066 D
1064 1066 D
S
N
1106 1034 M
1086 1038 D
S
N
1086 1038 M
1090 1034 D
1092 1028 D
1092 1022 D
1090 1016 D
1086 1012 D
1080 1010 D
1076 1010 D
1070 1012 D
1066 1016 D
1064 1022 D
1064 1028 D
1066 1034 D
1068 1036 D
1072 1038 D
1074 1038 D
1076 1036 D
1074 1034 D
1072 1036 D
S
N
1092 1022 M
1090 1018 D
1086 1014 D
1080 1012 D
1076 1012 D
1070 1014 D
1066 1018 D
1064 1022 D
S
N
1106 1034 M
1106 1014 D
S
N
1104 1034 M
1104 1024 D
1106 1014 D
S
N
1098 826 M
1096 824 D
1094 826 D
1096 828 D
1098 828 D
1102 826 D
1104 824 D
1106 818 D
1106 810 D
1104 804 D
1102 802 D
1098 800 D
1094 800 D
1090 802 D
1086 808 D
1082 818 D
1080 822 D
1076 826 D
1070 828 D
1064 828 D
S
N
1106 810 M
1104 806 D
1102 804 D
1098 802 D
1094 802 D
1090 804 D
1086 810 D
1082 818 D
S
N
1068 828 M
1070 826 D
1070 822 D
1066 812 D
1066 806 D
1068 802 D
1070 800 D
S
N
1070 822 M
1064 812 D
1064 804 D
1066 802 D
1070 800 D
1074 800 D
S
N
2196 2280 M
2124 2280 D
S
N
2196 2231 M
2172 2231 D
S
N
2196 2182 M
2172 2182 D
S
N
2196 2133 M
2172 2133 D
S
N
2196 2084 M
2172 2084 D
S
N
2196 2035 M
2124 2035 D
S
N
2196 1986 M
2172 1986 D
S
N
2196 1937 M
2172 1937 D
S
N
2196 1888 M
2172 1888 D
S
N
2196 1839 M
2172 1839 D
S
N
2196 1790 M
2124 1790 D
S
N
2196 1741 M
2172 1741 D
S
N
2196 1692 M
2172 1692 D
S
N
2196 1643 M
2172 1643 D
S
N
2196 1594 M
2172 1594 D
S
N
2196 1545 M
2124 1545 D
S
N
2196 1496 M
2172 1496 D
S
N
2196 1447 M
2172 1447 D
S
N
2196 1398 M
2172 1398 D
S
N
2196 1349 M
2172 1349 D
S
N
2196 1300 M
2124 1300 D
S
N
2196 1251 M
2172 1251 D
S
N
2196 1202 M
2172 1202 D
S
N
2196 1153 M
2172 1153 D
S
N
2196 1104 M
2172 1104 D
S
N
2196 1055 M
2124 1055 D
S
N
2196 1006 M
2172 1006 D
S
N
2196 957 M
2172 957 D
S
N
2196 908 M
2172 908 D
S
N
2196 859 M
2172 859 D
S
N
2196 810 M
2124 810 D
S
N
1146 2208 M
1146 2280 D
S
N
1198 2256 M
1198 2280 D
S
N
1251 2256 M
1251 2280 D
S
N
1303 2256 M
1303 2280 D
S
N
1356 2256 M
1356 2280 D
S
N
1408 2208 M
1408 2280 D
S
N
1461 2256 M
1461 2280 D
S
N
1513 2256 M
1513 2280 D
S
N
1566 2256 M
1566 2280 D
S
N
1619 2256 M
1619 2280 D
S
N
1671 2208 M
1671 2280 D
S
N
1724 2256 M
1724 2280 D
S
N
1776 2256 M
1776 2280 D
S
N
1829 2256 M
1829 2280 D
S
N
1881 2256 M
1881 2280 D
S
N
1933 2208 M
1933 2280 D
S
N
1986 2256 M
1986 2280 D
S
N
2038 2256 M
2038 2280 D
S
N
2091 2256 M
2091 2280 D
S
N
2143 2256 M
2143 2280 D
S
N
2196 2208 M
2196 2280 D
S
N
1140 2382 M
1140 2346 D
S
N
1156 2330 M
1154 2328 D
1152 2330 D
1154 2332 D
1156 2332 D
1160 2330 D
1162 2328 D
1164 2322 D
1164 2314 D
1162 2308 D
1158 2306 D
1152 2306 D
1148 2308 D
1146 2314 D
1146 2320 D
S
N
1164 2314 M
1162 2310 D
1158 2308 D
1152 2308 D
1148 2310 D
1146 2314 D
S
N
1146 2314 M
1144 2310 D
1140 2306 D
1136 2304 D
1130 2304 D
1126 2306 D
1124 2308 D
1122 2314 D
1122 2322 D
1124 2328 D
1126 2330 D
1130 2332 D
1132 2332 D
1134 2330 D
1132 2328 D
1130 2330 D
S
N
1142 2308 M
1136 2306 D
1130 2306 D
1126 2308 D
1124 2310 D
1122 2314 D
S
N
1403 2382 M
1403 2346 D
S
N
1418 2330 M
1416 2328 D
1414 2330 D
1416 2332 D
1418 2332 D
1422 2330 D
1424 2328 D
1426 2322 D
1426 2314 D
1424 2308 D
1422 2306 D
1418 2304 D
1414 2304 D
1410 2306 D
1407 2312 D
1403 2322 D
1401 2326 D
1397 2330 D
1391 2332 D
1385 2332 D
S
N
1426 2314 M
1424 2310 D
1422 2308 D
1418 2306 D
1414 2306 D
1410 2308 D
1407 2314 D
1403 2322 D
S
N
1389 2332 M
1391 2330 D
1391 2326 D
1387 2316 D
1387 2310 D
1389 2306 D
1391 2304 D
S
N
1391 2326 M
1385 2316 D
1385 2308 D
1387 2306 D
1391 2304 D
1395 2304 D
S
N
1665 2382 M
1665 2346 D
S
N
1681 2326 M
1683 2322 D
1689 2316 D
1647 2316 D
S
N
1687 2318 M
1647 2318 D
S
N
1647 2326 M
1647 2308 D
S
N
1951 2340 M
1949 2346 D
1943 2350 D
1934 2352 D
1928 2352 D
1918 2350 D
1912 2346 D
1910 2340 D
1910 2336 D
1912 2330 D
1918 2326 D
1928 2324 D
1934 2324 D
1943 2326 D
1949 2330 D
1951 2336 D
1951 2340 D
S
N
1951 2340 M
1949 2344 D
1947 2346 D
1943 2348 D
1934 2350 D
1928 2350 D
1918 2348 D
1914 2346 D
1912 2344 D
1910 2340 D
S
N
1910 2336 M
1912 2332 D
1914 2330 D
1918 2328 D
1928 2326 D
1934 2326 D
1943 2328 D
1947 2330 D
1949 2332 D
1951 2336 D
S
N
2206 2346 M
2208 2342 D
2214 2336 D
2172 2336 D
S
N
2212 2338 M
2172 2338 D
S
N
2172 2346 M
2172 2328 D
S
N
1146 810 M
1146 882 D
S
N
1198 810 M
1198 834 D
S
N
1251 810 M
1251 834 D
S
N
1303 810 M
1303 834 D
S
N
1356 810 M
1356 834 D
S
N
1408 810 M
1408 882 D
S
N
1461 810 M
1461 834 D
S
N
1513 810 M
1513 834 D
S
N
1566 810 M
1566 834 D
S
N
1619 810 M
1619 834 D
S
N
1671 810 M
1671 882 D
S
N
1724 810 M
1724 834 D
S
N
1776 810 M
1776 834 D
S
N
1829 810 M
1829 834 D
S
N
1881 810 M
1881 834 D
S
N
1933 810 M
1933 882 D
S
N
1986 810 M
1986 834 D
S
N
2038 810 M
2038 834 D
S
N
2091 810 M
2091 834 D
S
N
2143 810 M
2143 834 D
S
N
2196 810 M
2196 882 D
S
[39] 0 Sd
N
1933 2149 M
1933 2149 D
1933 2148 D
1933 2148 D
1933 2147 D
1933 2146 D
1933 2146 D
1933 2145 D
1933 2144 D
1933 2143 D
1933 2141 D
1933 2140 D
1933 2139 D
1933 2137 D
1933 2135 D
1933 2134 D
1933 2132 D
1933 2130 D
1933 2128 D
1933 2126 D
1933 2124 D
1932 2122 D
1932 2120 D
1932 2118 D
1932 2115 D
1932 2113 D
1931 2111 D
1931 2108 D
1931 2105 D
1931 2103 D
1930 2100 D
1930 2097 D
1930 2094 D
1929 2092 D
1929 2089 D
1929 2086 D
1928 2083 D
1928 2080 D
1927 2076 D
1927 2073 D
1926 2070 D
1926 2067 D
1925 2063 D
1924 2060 D
1924 2057 D
1923 2053 D
1922 2050 D
1921 2046 D
1921 2043 D
1920 2039 D
1919 2035 D
1918 2032 D
1917 2028 D
1916 2024 D
1915 2020 D
1914 2016 D
1913 2013 D
1912 2009 D
1910 2005 D
1909 2001 D
1908 1997 D
1906 1993 D
1905 1989 D
1904 1985 D
1902 1980 D
1901 1976 D
1899 1972 D
1897 1968 D
1896 1964 D
1894 1960 D
1892 1955 D
1890 1951 D
1888 1947 D
1887 1942 D
1885 1938 D
1883 1934 D
1880 1929 D
1878 1925 D
1876 1920 D
1874 1916 D
1872 1911 D
1869 1907 D
1867 1902 D
1864 1898 D
1862 1893 D
1859 1888 D
1857 1884 D
1854 1879 D
1851 1874 D
1848 1870 D
1846 1865 D
1843 1860 D
1840 1856 D
1837 1851 D
1834 1846 D
1831 1841 D
1827 1836 D
1824 1832 D
1821 1827 D
1818 1822 D
1814 1817 D
1811 1812 D
1807 1807 D
1804 1802 D
1800 1797 D
1797 1792 D
1793 1787 D
1790 1782 D
1786 1777 D
1782 1772 D
1778 1767 D
1774 1762 D
1770 1757 D
1766 1752 D
1763 1747 D
1758 1742 D
1754 1737 D
1750 1732 D
1746 1726 D
1742 1721 D
1738 1716 D
1734 1711 D
1729 1706 D
1725 1701 D
1721 1695 D
1716 1690 D
1712 1685 D
1707 1680 D
1703 1674 D
1698 1669 D
1694 1664 D
1689 1658 D
1685 1653 D
1680 1648 D
1676 1642 D
1671 1637 D
1667 1632 D
1662 1626 D
1657 1621 D
1653 1616 D
1648 1610 D
1643 1605 D
1639 1599 D
1634 1594 D
1629 1589 D
1624 1583 D
1620 1578 D
1615 1572 D
1610 1567 D
1606 1561 D
1601 1556 D
1596 1550 D
1591 1545 D
1587 1539 D
1582 1534 D
1577 1528 D
1573 1523 D
1568 1517 D
1563 1511 D
1559 1506 D
1554 1500 D
1549 1495 D
1545 1489 D
1540 1484 D
1536 1478 D
1531 1472 D
1527 1467 D
1522 1461 D
1518 1455 D
1513 1450 D
1509 1444 D
1505 1438 D
1500 1433 D
1496 1427 D
1492 1421 D
1487 1416 D
1483 1410 D
1479 1404 D
1475 1399 D
1471 1393 D
1467 1387 D
1463 1382 D
1459 1376 D
1455 1370 D
1451 1364 D
1447 1359 D
1443 1353 D
1440 1347 D
1436 1341 D
1432 1335 D
1429 1330 D
1425 1324 D
1422 1318 D
S
N
1422 1318 M
1418 1312 D
1415 1307 D
1412 1301 D
1408 1295 D
1405 1289 D
1402 1283 D
1399 1277 D
1396 1272 D
1393 1266 D
1390 1260 D
1387 1254 D
1384 1248 D
1381 1242 D
1379 1236 D
1376 1231 D
1374 1225 D
1371 1219 D
1369 1213 D
1366 1207 D
1364 1201 D
1362 1195 D
1359 1189 D
1357 1183 D
1355 1178 D
1353 1172 D
1351 1166 D
1349 1160 D
1348 1154 D
1346 1148 D
1344 1142 D
1343 1136 D
1341 1130 D
1339 1124 D
1338 1118 D
1337 1112 D
1335 1106 D
1334 1100 D
1333 1094 D
1332 1088 D
1331 1082 D
1330 1076 D
1329 1070 D
1328 1064 D
1327 1058 D
1327 1052 D
1326 1046 D
1325 1040 D
1325 1034 D
1324 1028 D
1324 1022 D
1324 1016 D
S
N
1324 1016 M
1323 1010 D
1323 1004 D
1323 998 D
1323 992 D
1323 986 D
1323 980 D
1323 974 D
1323 968 D
1323 962 D
1324 956 D
1324 950 D
1324 944 D
1325 938 D
1325 932 D
1326 926 D
1326 920 D
1327 914 D
1328 908 D
1328 902 D
1329 895 D
1330 889 D
1331 883 D
1332 877 D
1333 871 D
1334 865 D
1335 859 D
1336 853 D
1337 847 D
1338 841 D
1340 834 D
1341 828 D
1342 822 D
1344 816 D
1345 810 D
1345 810 D
S
[] 0 Sd
N
1933 2149 M
1933 2149 D
1933 2148 D
1933 2148 D
1933 2147 D
1933 2146 D
1933 2146 D
1933 2145 D
1933 2144 D
1933 2143 D
1933 2141 D
1933 2140 D
1933 2139 D
1933 2137 D
1933 2135 D
1933 2134 D
1933 2132 D
1933 2130 D
1933 2128 D
1933 2126 D
1933 2124 D
1933 2122 D
1933 2120 D
1932 2118 D
1932 2115 D
1932 2113 D
1932 2111 D
1932 2108 D
1932 2105 D
1931 2103 D
1931 2100 D
1931 2097 D
1931 2094 D
1930 2092 D
1930 2089 D
1930 2086 D
1930 2083 D
1929 2080 D
1929 2076 D
1928 2073 D
1928 2070 D
1928 2067 D
1927 2063 D
1927 2060 D
1926 2057 D
1926 2053 D
1925 2050 D
1925 2046 D
1924 2043 D
1923 2039 D
1923 2035 D
1922 2032 D
1921 2028 D
1920 2024 D
1920 2020 D
1919 2016 D
1918 2013 D
1917 2009 D
1916 2005 D
1915 2001 D
1914 1997 D
1913 1993 D
1912 1989 D
1911 1985 D
1910 1980 D
1909 1976 D
1908 1972 D
1907 1968 D
1905 1964 D
1904 1960 D
1903 1955 D
1901 1951 D
1900 1947 D
1898 1942 D
1897 1938 D
1895 1934 D
1894 1929 D
1892 1925 D
1891 1920 D
1889 1916 D
1887 1911 D
1885 1907 D
1884 1902 D
1882 1898 D
1880 1893 D
1878 1888 D
1876 1884 D
1874 1879 D
1872 1874 D
1870 1870 D
1868 1865 D
1865 1860 D
1863 1856 D
1861 1851 D
1859 1846 D
1856 1841 D
1854 1836 D
1851 1832 D
1849 1827 D
1847 1822 D
1844 1817 D
1841 1812 D
1839 1807 D
1836 1802 D
1833 1797 D
1831 1792 D
1828 1787 D
1825 1782 D
1822 1777 D
1819 1772 D
1816 1767 D
1814 1762 D
1811 1757 D
1808 1752 D
1805 1747 D
1801 1742 D
1798 1737 D
1795 1732 D
1792 1726 D
1789 1721 D
1786 1716 D
1782 1711 D
1779 1706 D
1776 1701 D
1772 1695 D
1769 1690 D
1766 1685 D
1762 1680 D
1759 1674 D
1755 1669 D
1752 1664 D
1748 1658 D
1745 1653 D
1741 1648 D
1738 1642 D
1734 1637 D
1731 1632 D
1727 1626 D
1723 1621 D
1720 1616 D
1716 1610 D
1712 1605 D
1709 1599 D
1705 1594 D
1701 1589 D
1698 1583 D
1694 1578 D
1690 1572 D
1687 1567 D
1683 1561 D
1679 1556 D
1676 1550 D
1672 1545 D
1668 1539 D
1664 1534 D
1661 1528 D
1657 1523 D
1653 1517 D
1650 1511 D
1646 1506 D
1642 1500 D
1639 1495 D
1635 1489 D
1631 1484 D
1628 1478 D
1624 1472 D
1620 1467 D
1617 1461 D
1613 1455 D
1610 1450 D
1606 1444 D
1603 1438 D
1599 1433 D
1596 1427 D
1592 1421 D
1589 1416 D
1585 1410 D
1582 1404 D
1579 1399 D
1575 1393 D
1572 1387 D
1569 1382 D
1565 1376 D
1562 1370 D
1559 1364 D
1556 1359 D
1553 1353 D
1550 1347 D
1547 1341 D
1544 1335 D
1541 1330 D
1538 1324 D
1535 1318 D
S
N
1535 1318 M
1532 1312 D
1529 1307 D
1526 1301 D
1523 1295 D
1520 1289 D
1518 1283 D
1515 1277 D
1512 1272 D
1510 1266 D
1507 1260 D
1505 1254 D
1502 1248 D
1500 1242 D
1498 1236 D
1495 1231 D
1493 1225 D
1491 1219 D
1489 1213 D
1486 1207 D
1484 1201 D
1482 1195 D
1480 1189 D
1478 1183 D
1476 1178 D
1474 1172 D
1473 1166 D
1471 1160 D
1469 1154 D
1467 1148 D
1466 1142 D
1464 1136 D
1463 1130 D
1461 1124 D
1460 1118 D
1458 1112 D
1457 1106 D
1456 1100 D
1454 1094 D
1453 1088 D
1452 1082 D
1451 1076 D
1450 1070 D
1449 1064 D
1448 1058 D
1447 1052 D
1446 1046 D
1445 1040 D
1445 1034 D
1444 1028 D
1443 1022 D
1442 1016 D
S
N
1442 1016 M
1442 1010 D
1441 1004 D
1441 998 D
1440 992 D
1440 986 D
1440 980 D
1439 974 D
1439 968 D
1439 962 D
1439 956 D
1438 950 D
1438 944 D
1438 938 D
1438 932 D
1438 926 D
1438 920 D
1439 914 D
1439 908 D
1439 902 D
1439 895 D
1439 889 D
1440 883 D
1440 877 D
1440 871 D
1441 865 D
1441 859 D
1442 853 D
1442 847 D
1443 841 D
1443 834 D
1444 828 D
1445 822 D
1445 816 D
1446 810 D
1446 810 D
S
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