A non-perturbative study of gauge theory on a non-commutative plane
Wolfgang Bietenholz and Frank Hofheinz
Institut f\"{u}r Physik
Humboldt Universit\"{a}t zu Berlin
Invalidenstr. 110
D-10115 Berlin
Germany
We perform a non-perturbative study of pure gauge theory in a two dimensional non-commutative (NC) space. On the lattice, it is equivalent to the twisted Eguchi-Kawai model, which we simulated at $N$ ranging from 25 to 515. We observe a clear large-$N$ scaling for the 1- and 2-point function of Wilson loops, as well as the 2-point function of Polyakov lines. The 2-point functions agree with a universal wave function renormalization. Based on a Morita equivalence, the large-$N$ double scaling limit corresponds to the continuum limit of NC gauge theory, so the observed large-$N$ scaling demonstrates the non-perturbative renormalizability of this NC field theory. The area law for the Wilson loops holds at small physical area as in commutative 2d planar gauge theory, but at large areas we find an oscillating behavior instead. In that regime the phase of the Wilson loop grows linearly with the area. This agrees with the Aharonov-Bohm effect in the presence of a constant magnetic field, identified with the inverse non-commutativity parameter.
jhep092002009.tex
\documentclass[published]{JHEP3}
\JHEP{09(2002)009}

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\title{A non-perturbative study of gauge theory on a non-commutative
plane}



\author{Wolfgang Bietenholz and Frank Hofheinz\\
Institut f\"{u}r Physik, Humboldt Universit\"{a}t zu Berlin\\
Invalidenstr. 110, D-10115 Berlin, Germany\\
E-mail: \email{bietenho@physik.hu-berlin.de}, \email{hofheinz@physik.hu-berlin.de}}

\author{Jun Nishimura\\
Dept.\ of Physics, Nagoya University\\
Nagoya 464-8602, Japan\\
E-mail: \email{nisimura@eken.phys.nagoya-u.ac.jp}}



\abstract{We perform a non-perturbative study of pure gauge theory in
a two dimensional non-commutative (NC) space.  On the lattice, it is
equivalent to the twisted Eguchi-Kawai model, which we simulated at
$N$ ranging from 25 to 515.  We observe a clear large-$N$ scaling for
the 1- and 2-point function of Wilson loops, as well as the 2-point
function of Polyakov lines.  The 2-point functions agree with a
universal wave function renormalization.  Based on a Morita
equivalence, the large-$N$ double scaling limit corresponds to the
continuum limit of NC gauge theory, so the observed large-$N$ scaling
demonstrates the non-perturbative renormalizability of this NC field
theory.  The area law for the Wilson loops holds at small physical
area as in commutative 2d planar gauge theory, but at large areas we
find an oscillating behavior instead. In that regime the phase of the
Wilson loop grows linearly with the area.  This agrees with the
Aharonov-Bohm effect in the presence of a constant magnetic field,
identified with the inverse non-commutativity parameter.}

\accepted{September 3, 2002}
\keywords{Non-Commutative Geometry, Matrix Models, Lattice Gauge Field Theories, Field Theories in Lower Dimensions}
\received{June 19, 2002}
\revised{August 30, 2002}


\begin{document}

\section{Introduction}

The concept of spaces with NC coordinates has been known
for a number of decades (see, e.g.~\cite{Sny}), before the
mathematicians worked out a precise formulation of field theory
on such geometries~\cite{Con}. In the recent years, these
NC field theories experienced a tremendous boom, which reflects
a wide-spread belief that this variation of standard (commutative)
field theory is well motivated. The main reason for this popularity
is that they are obtained as low energy limits from string theories
and M-theory with antisymmetric tensor fields~\cite{CDS,DH,SW}.
Moreover, there may be practical applications to the quantum Hall 
effect~\cite{QHall}. For recent reviews we refer to refs.~\cite{DN}.

As an important deviation from standard field theory, the 
non-commutativity tensor
\begin{eqnarray}
\Theta_{\mu \nu} &=& i \, [\hat x_{\nu},\hat x_{\mu}] 
\qquad 
(  \hat x_{\mu}:  \hbox{ hermitean~operators}) 
\nonumber \\ 
                &=& \theta \, \epsilon_{\mu \nu} 
\qquad 
(  \hbox{in } d=2  ) 
\label{non-comm}
\end{eqnarray}
introduces some \emph{non-locality} inside a short range, which is
characterized by the scale of the parameter $\theta$.  This
non-locality implies deep conceptual problems, but on the other hand
it is considered a virtue which could be crucial for the link to
quantum gravity as well as string and M-theory.  Moreover, there was
originally some hope that this property could help to weaken or even
remove the UV divergences~\cite{Sny}.

However, it is exactly the question of renormalizability where NC
field theory runs into problems which are even worse than in standard
field theory. UV singularities are still present, and in addition new
IR singularities are mixed in (this is discussed for instance in
ref.~\cite{Filk}). In perturbation theory, this notorious UV/IR mixing
affects certain non-planar diagrams~\cite{Min}.  Intuitively one may
grasp from eq.~(\ref{non-comm}) that short distance effects in one
direction translate into long range effects in the other directions
and vice versa, which causes this kind of mixed singularities in
non-planar diagrams, which do not occur in standard field
theory. This property poses severe difficulties for the
renormalization of perturbation theory, which are not overcome yet.
For instance, scalar fields can become unstable (tachyons) due to IR
effects as the non-commutativity is switched on~\cite{Min}.  The
attempts to renormalize perturbation theory include the methods known
from standard field theory (see e.g.\ ref.~\cite{Che}), the
application of Wilson's renormalization group technique~\cite{RG},
controlling IR divergences in the framework of
supersymmetry~\cite{GGRS} and the Hartree method~\cite{GS}.  In spite
of some plausibility arguments in favor of perturbative
renormalizability, it is an open question if NC quantum field theories
do really have finite UV and IR limits. There are even claims that
basic NC field theories, like NC QED, are not
renormalizable~\cite{NCQED}.

Our approach is the non-perturbative study of NC field theory by means
of Monte Carlo simulations. In this paper we present --- as a pilot
project --- numeric results for 2d NC gauge theory.\footnote{While our
simulations were running, a related project was suggested by S.\
Profumo~\cite{SP}.}  In this particular model, the UV/IR mixing does
not occur \emph{perturbatively} since there are no UV divergent
diagrams in the commutative case.  However, such mixing effects are
still possible on the non-perturbative level, and indeed our study is
going to reveal their existence.  For interesting analytical work in
this field, see refs.~\cite{Mafia}. In particular, Paniak and Szabo
worked out an explicit form for the corresponding partition
function. Due to Morita equivalence, 2d NC $\U(n)$ gauge theory can be
identified with the twisted Eguchi-Kawai model (TEK)~\cite{GAO} in the
large-$N$ limit \cite{AIIKKT}. The TEK at finite $N$ corresponds to
lattice NC gauge theory~\cite{AMNS}, as we briefly review in
section~\ref{sec2}.  In section~\ref{sec3} we present our simulation
results for the TEK, which do reveal that 2d NC gauge theory is
renormalizable. We also observe the similarities and differences from
commutative gauge theory and discuss their interpretation.  Our
conclusions are given in section~\ref{sec4}.


\section{The twisted Eguchi-Kawai model as a formulation of 
NC gauge theory}\label{sec2}

Back in 1982, Eguchi and Kawai conjectured that standard $\U(N)$ and
$\SU(N)$ lattice gauge theories may be equivalent to their dimensional
reductions to $d=0$ (one point) in the large-$N$ limit~\cite{EK}. Then
all link variables are replaced by $U_{x,\mu} \to U_{\mu}$, and the
plaquette action simplifies to
\begin{equation}
S_{EK}[U] = - N \beta \sum_{\mu \ne \nu} \Tr  \Bigl(
U_{\mu}U_{\nu}U_{\mu}^{\dagger} U_{\nu}^{\dagger} \Bigr) \,,
\end{equation}
where $\mu,\nu = 1, \dots, d$.  Eguchi and Kawai proved that the
Schwinger-Dyson equations --- and therefore the Wilson loops --- are
unaltered under dimensional reduction, assuming that the $\U(1)^{d}$
symmetry of the phases (or center symmetry) is not spontaneously
broken. This is correct in $d=2$ of course, but in $d>2$ it only holds
at strong coupling~\cite{BHN}, so the proof for the equivalence to the
reduced model (EK equivalence) has only a limited
application. However, it was shown recently that a variant of the 4d
Eguchi-Kawai model (EK model) surprisingly obeys the area law in a
significant range of scale, so EK equivalence may still be in business
in some finite regime~\cite{ABN}.

In order to avoid the problem with the limited viability of the proof
for EK equivalence, the EK model was soon modified such that the phase
symmetries are preserved. This was achieved by the ``quenched EK
model''~\cite{BHN}, and in even dimensions also by the TEK~\cite{GAO},
\begin{equation}
\label{TEK}
S_{\rm TEK} [U] = - N \beta \sum_{\mu \ne \nu} {\cal Z}_{\mu \nu} \,
\Tr \Bigl( U_{\mu}U_{\nu}U_{\mu}^{\dagger} U_{\nu}^{\dagger} \Bigr) \,.
\end{equation}
The factor ${\cal Z}_{\mu \nu}$ represents the \emph{twist},
\begin{equation}
{\cal Z}_{\mu \nu} = {\cal Z}_{\nu \mu}^{*} = \exp \left( \frac{2 \pi
i k }{L}\right), 
\qquad 
(\mu < \nu ) \,,
\end{equation}
where $k$ is an integer and $L = N^{2/d}$ is the size of the system.
The usual formulation sets $k=1$.  Further variants of the TEK have
been invented~\cite{GA-KA,Fab1}.  For numerical studies in $d>2$, see
refs.~\cite{GAO,Fab2} ($d=4$) and ref.~\cite{JN} ($d=6$).

Here we are concerned with the 2d TEK. It seemed for a long time that
adding a twist is not highly motivated in $d=2$, since there even the
ordinary EK model coincides with lattice gauge theory in the planar
limit, which was solved analytically by Gross and Witten~\cite{GW}.
This agreement was shown already in the famous ref.~\cite{EK}, and it
seemed likely to hold also with twist at $N \to \infty$.  Still the 2d
model was simulated with the $k=1$ twist first in ref.~\cite{Fab3} and
later in ref.~\cite{NN}, where the finite $N$ effects were studied;
but they did still not provide much motivation for including the
twist.\footnote{A very recent reconsideration of the corresponding EK
equivalence is presented in ref.~\cite{ProfVic}.}

However the situation changed suddenly due to a new interpretation of
the TEK as an equivalent description of NC gauge theory.  The latter
can be formulated if we multiply the fields by star products,
\begin{eqnarray}
S &=& \frac{1}{4} \int d^{2}x \Tr  \left( F_{\mu \nu}(x)
\star F_{\mu \nu}(x) \right), 
\nonumber \\
F_{\mu \nu} &=& \partial_{\mu} A_{\nu} - \partial_{\nu}A_{\mu}
+ig (A_{\mu} \star A_{\nu} - A_{\nu} \star A_{\mu} ) \,. 
\label{actNC}
\end{eqnarray}
For completeness we mention that the star product is defined as
\begin{equation}
f(x) \star g(x) = \left. \exp \left( \frac{i}{2} \Theta_{\mu \nu}
\frac{\partial}{\partial x_{\mu}} \frac{\partial}{\partial y_{\nu}} \right)
f(x) g(y) \right|_{x=y} ,
\end{equation}
and that under a star gauge transformation
\begin{eqnarray}
A_{\mu}(x) & \to & V(x) \star A_{\mu}(x) \star V(x)^{\dagger}
- \frac{i}{g} V(x) \star \frac{\partial}{\partial x_{\mu}} 
V(x)^{\dagger} \,, 
\nonumber \\
&& V(x) \star V(x)^{\dagger} = 1 \,,
\label{star-gauge}
\end{eqnarray}
the lagrangian $\Tr F_{\mu \nu} \star F_{\mu \nu}$ is not invariant,
but the action in eq.~(\ref{actNC}) is star gauge invariant.

This new interpretation of twisted reduced models holds in the
stringent sense of \emph{``Morita equivalence''}.  Roughly speaking,
this means that the algebras involved in two models can be mapped onto
each other one-to-one, in a way which maps each module and its
structure properly from one algebra to the other.\footnote{As an even
stronger relation, ``gauge Morita equivalence'' implies that also the
connections between two modules are mapped onto each
other~\cite{Schwarz98}.}

This kind of equivalence was found between NC gauge theory and twisted
large-$N$ reduced models~\cite{AIIKKT}.  That relation was established
by embedding the (dynamically generated) coordinates and momenta of
the reduced model into matrices.  These matrices can be mapped on
functions, where the trace turns into an integral and the star
products arise, so that one arrives at action~(\ref{actNC}).  The
construction of NC $\U(n)$ gauge theories (for certain $n \in \{ 1,2,
\dots \}$) works out in this way at $N = \infty$.\footnote{On the
other hand, there are severe problems in formulating $\SU(n)$ gauge
theory on a NC space.}  Ref.~\cite{HI} pointed out that this
transition corresponds to a Morita equivalence. At finite $N$ the
conditions cannot be matched at the boundaries.

However, in refs.~\cite{AMNS} this mapping was refined and it turned
out that certain reduced twisted $\U(N)$ models at finite $N$
correspond to NC Yang-Mills theories on the lattice.  The
corresponding lattice formulation itself was also elaborated in
refs.~\cite{AMNS}.\footnote{For earlier work on a lattice formulation
of NC gauge theory, see e.g.\ ref.~\cite{Bars}.}  From the UV/IR
mixing it can be understood that such a formulation appears
necessarily on a periodic lattice, so that the singularities are
consistently regularized, and also the non-commutativity parameter
$\theta$ takes discrete values.  The continuum limit of lattice NC
gauge theory coincides precisely with the large-$N$ limit of the
reduced (twisted, commutative) model. This observation completes the
explicit non-perturbative (``constructive'') formulation of NC gauge
theory, in a form which can be studied by numerical simulations.  This
would be very difficult in the direct lattice formulation, due to the
problems related to the star pro\-duct: first it is complicated to
introduce star unitary link variables and a measure for them, then one
would still have to find a way to compute a discrete version of the
star products in action~(\ref{actNC}).

The $\U(N)$ symmetry of the twisted reduced models corresponds to the
gauge invariance~(\ref{star-gauge}) in the NC gauge theories.  In the
twisted reduced model the formulation of $\U(N)$ invariant observables
(Wilson loops, in particular) is straightforward, and the mapping on
NC gauge theories led also to the formulation of NC Wilson
loops~\cite{IIKK}.  This formulation works perfectly on the lattice as
well~\cite{AMNS}.  Various aspects of gauge invariant observables have
been investigated in refs.~\cite{NCloops}.

In order to remain in the framework of the \emph{discrete Morita
equivalence} of refs.~\cite{AMNS} one has to take the large-$N$ limit
from specific finite $N$ TEK formulations.  For the 2d TEK this
prescription is different from ref.~\cite{NN}, which used $k=1$ and
$N$ even. For the equivalence to lattice NC gauge theory with rank-one
gauge group, the twist in eq.~(\ref{TEK}) has to be taken as
\begin{equation}
\label{twist2}
{\cal Z}_{12} = {\cal Z}_{21}^{*} = \exp \left(\pi i
\frac{(L+1)}{L}\right),
\end{equation}
which implies $2k = L+1$, hence $L$ must be \emph{odd} (and $L=N$ in
two dimensions).  Then there exists an explicit map from matrices onto
NC fields~\cite{Nishimura:2001dq}.  Corresponding to $N \times N$
matrices, one obtains fields on a NC torus, which is discretized into
a $N \times N$ periodic lattice.  The number of degrees of freedom
matches exactly.  The non-commutativity is encoded in the discretized
version of the star product, which is used to define products of
fields in the action.  If we introduce a lattice spacing $a$, the
(dimensionful) non-commutativity parameter takes the form
\begin{equation}
\label{theta_lat}
\theta = \frac{1}{\pi} N a^2 \,.
\end{equation}

In the context of EK equivalence, one takes the limit $N \rightarrow
\infty$ at fixed $\beta$, which ensures the equivalence of the TEK
model to $\U(\infty )$ commutative lattice gauge theory.  This is
called the \emph{planar} large-$N$ limit, since only planar diagrams
survive.  Then the continuum limit should be taken by sending $a
\rightarrow 0 $ along with $\beta \rightarrow \infty$ in a particular
way dictated by the coupling constant renormalization.  In the present
$d=2$ case, the coupling constant scaling is purely canonical (see
below)
\begin{equation}
\label{cont_lim}
\beta \propto a^{-2} \,.
\end{equation}
Now interpreting the TEK as a lattice NC gauge theory, the planar
limit corresponds to $\theta = \infty$ due to eq.~(\ref{theta_lat}).
This is a non-perturbative account of the well-known equivalence
between $\theta = \infty$ NC field theory and the corresponding
(commutative) planar field theory.

In this paper, we are interested in a continuum limit of the lattice
NC gauge theory at \emph{finite} $\theta$.  According to
eq.~(\ref{theta_lat}), this requires the large-$N$ limit to be taken
simultaneously with the continuum limit $a \rightarrow
0$.\footnote{The physical extent of the NC torus $Na$ goes to infinity
in this limit.  In order to obtain a finite torus in the continuum
limit, one would have to use a different formulation of lattice NC
gauge theory~\cite{AMNS}.}  This also implies that non-planar diagrams
are included, but in this specific model they do not involve
perturbative UV/IR mixing, as we mentioned in the introduction.  As we
are going to explain in the next section, $\beta$ has to be scaled as
a function of the lattice spacing $a$ in exactly the same way as in
the planar theory.  Hence in $d=2$ we are going to search for a
\emph{double scaling limit} keeping the ratio $N / \beta $ constant.
The question of renormalizability of 2d NC gauge theory at finite
$\theta$ can be answered by studying this large-$N$ limit of the TEK.
If the observables converge to finite values, we can conclude that 2d
lattice NC gauge theory does have a finite continuum limit. Our
results will also be presented in the next section.

A double scaling limit of the \emph{untwisted} EK model was searched
for in ref.~\cite{NN}.  Large-$N$ scaling of observables was indeed
observed at a fixed ratio $N/ \beta$, but this combination of
parameters was identified empirically.  The TEK, on the other hand,
was studied only at fixed $\beta$ in ref.~\cite{NN} and did not reveal
systematic finite $N$ effects.  However, we repeat that the TEK was
studied there with twist parameter $k=1$ and even values for $N$.


\section{Numeric results}\label{sec3}

In this section we present our numeric simulation results for the 2d
TEK at odd $N$, with the twist specified in eq.\ (\ref{twist2}). In
the form of eq.~(\ref{TEK}), the action cannot be simulated with a
heat bath algorithm because it is not linear in the matrices
$U_{\mu}$. Following ref.~\cite{Fab4} we introduce an auxiliary matrix
field $Q$, which enters in a gaussian form and which linearizes the
action in the $U_{\mu}$,
\begin{eqnarray}
S_{\rm TEK}[U,Q] &=& 
N \beta \sum_{\mu < \nu} \Tr   \Bigl[ Q_{\mu \nu}^{\dagger}
Q_{\mu \nu} - Q_{\mu \nu}^{\dagger} \left(t_{\mu \nu} U_{\mu}
U_{\nu} + t_{\nu \mu} U_{\nu} U_{\mu} \right) -\qquad
\nonumber \\&& 
            \hphantom{N \beta \sum_{\mu < \nu} \Tr   \Bigl[}\!
- \left(t_{\mu \nu}^{*} U_{\mu}^{\dagger} U_{\nu}^{\dagger} + t_{\nu
\mu}^{*} U_{\nu}^{\dagger} U_{\mu}^{\dagger} \right) Q_{\mu \nu} \Bigr] \,.
\end{eqnarray}
The auxiliary field $Q$ consists of general complex $N\times N$
matrices, and their integration reproduces the TEK as given in
eq.~(\ref{TEK}), if $t_{\mu \nu} = \sqrt{{\cal Z}_{\mu \nu}}$.  In
this respect, and in all other technical points of the simulation, we
follow the methods which were used and described in ref.~\cite{NN}.
For instance, we also update $\SU(2)$ subgroups of the $U_{\mu}$
matrices, in the spirit of Cabbibo and Marinari~\cite{CM}.

\TABLE[t]{\begin{tabular}{|c|c|c|c|c|c|c|c|c|}\hline
$N$ & 25 & 35 & 55 & 85 & 125 & 195 & 255 & 515 
\\\hline
\# of configurations & 9000 & 8400 & 20000 & 8000 & 3400 & 260 & 120 & 18 
\\\hline
\end{tabular}%
\caption{Overview of the statistics in our simulation of the
TEK.\label{tab1}}}

Table~\ref{tab1} displays the number of configurations that we
generated at various $N$. Note that the few configurations at our
largest values of $N$ provide conclusive signals only for part of the
observables that we evaluated, see below.  In most of our study we
fixed
\begin{equation}
\frac{N}{\beta} = 32 \,,
\end{equation}
which corresponds to 
\begin{equation}
\theta= \frac{1}{4\pi} \frac{N}{\beta} = \frac{8}{\pi} \approx 2.55
\end{equation}
in the continuum limit.

As a point of orientation for the interpretation of our data, we
consider the exact solution of planar $\U(\infty )$ and $\SU(\infty )$
lattice gauge theory in $d=2$~\cite{GW}.  There the Wilson loop of a
rectangle $I \times J$ follows the area law
\begin{equation}
\label{arealaw}
w(I\times J) = \exp ( - \kappa (\beta ) I J ) \,,
\end{equation}
where the (dimensionless) string tension $\kappa(\beta)$ is given by
\begin{equation}
\kappa (\beta ) = \left\{
\begin{array}{ll}
- \ln \beta & \beta \leq \frac{1}{2} \\
- \ln \Bigl( 1 - \frac{1}{4 \beta} \Bigr)\qquad & 
\beta \geq \frac{1}{2}\,.
\end{array} \right. 
\end{equation}
In particular, the internal energy amounts to
\begin{equation}
E (\beta ) =  w(1\times 1) = \left\{
\begin{array}{ll}
\beta & \beta \leq \frac{1}{2} 
\\
1 - \frac{1}{4 \beta}\qquad & 
\beta \geq \frac{1}{2}
\end{array} \right. \,,
\end{equation}
which reveals a third order phase transition.\footnote{Note that we
are always in the $\beta \geq 1/2$ regime for the values of $N$ that
we are going to consider.}  Eq.~(\ref{arealaw}) shows how one should
tune the bare coupling constant $\beta$ as a function of $a$ when one
takes the continuum limit $a\rightarrow 0$.  In fact in this case the
scaling is exact if one takes the lattice spacing $a$ to be
\begin{equation}
\label{a_beta}
a = \sqrt{\kappa (\beta)} \,.
\end{equation}
Then the Wilson loop becomes an $a$-independent function of the
physical area $a^{2}IJ$.  From eq.~(\ref{a_beta}) we see that $\beta$
should be sent to infinity in the continuum limit as in
relation~(\ref{cont_lim}).

The EK equivalence implies that the exact result~(\ref{arealaw}) is
reproduced by considering the corresponding Wilson loops in the TEK in
the large-$N$ limit at fixed $\beta$.  More specifically, we define
`Wilson loops' in the TEK model as \cite{GAO}
\begin{equation}
\label{wilson-loop}
W_{\mu \nu}(I \times J) = \left({\cal Z}_{\mu \nu}\right)^{I\cdot J}
\Tr \Bigl( U_{\mu}^{I} U_{\nu}^{J} U_{\mu}^{\dagger \, I}
U_{\nu}^{\dagger \, J} \Bigr) \,,
\end{equation}
where $I,J=1,2, \dots$.  For $I=J=1$ it reduces to the plaquette,
which appears in the action~(\ref{TEK}).  Then the EK equivalence
states that
\begin{equation}
\lim _{N\rightarrow \infty} \frac{1}{N} \langle W_{12}(I \times J)
\rangle = w(I\times J) \,,
\end{equation}
at fixed $\beta$.  Here the term $w(I\times J)$ is the expectation
value of Wilson loop in the $\U(\infty )$ lattice gauge theory, given
by eq.~(\ref{arealaw}).

Let us now consider Wilson loops in NC gauge theory.  Since the Wilson
loop~(\ref{wilson-loop}) in the TEK model is $\U(N)$ invariant, it
defines a star gauge invariant observable upon mapping the matrices
onto NC fields~\cite{IIKK}.  This is precisely what we consider as the
Wilson loop in NC gauge theory on the lattice~\cite{AMNS}.  Now we
take the large-$N$ limit together with the continuum limit $a \to 0$
in order to obtain a finite non-commutativity parameter $\theta$ in
eq.~(\ref{theta_lat}).  We define a ``lattice spacing'' as in the
planar theory, i.e.\ as in eq.~(\ref{a_beta}).  Then the Wilson loop
still agrees with the planar result~(\ref{arealaw}) when the physical
extent of the Wilson loop is much smaller than the non-commutativity
scale $\sqrt{\theta}$.  (In the limit $\theta \to \infty$ it agrees
with the planar result for arbitrarily large area, as we mentioned
before.)  Therefore, the scaling in the small area regime requires the
lattice spacing to be chosen in the same way as in the planar
theory. The first interesting question is now whether the scaling of
the Wilson loop extends also to larger areas.

In the EK model it was observed that square shaped Wilson loops
converge faster to the known exact results in the planar limit than
other rectangles with the same area~\cite{NN}.  Hence we also focus on
square shaped Wilson loops here, which corresponds to the $I=J$ case
in definition~(\ref{wilson-loop}).  We define the normalized Wilson
loop
\begin{equation}
W(I) = \frac{1}{N} \langle W_{12}(I \times I) \rangle \,,
\end{equation}
which should agree with $w(I \times I)$ in 
eq.~(\ref{arealaw}) when $aI \ll \sqrt{\theta}$.
Due to the presence of the twist, there is no invariance
under the parity transformation $U_{1} \to U_{2}$, $U_{2} \to U_{1}$.
As a consequence, $W_{\mu \nu}$ is complex in general, and $W_{12}
= W_{21}^{*}$, hence the Wilson loop depends on its orientation.
The real part represents an average over both orientations.
Figure~\ref{fig:Wil1a} shows the real part $\mbox{Re}[W(I)]$
as a function of the physical loop area.


\FIGURE[t]{\input{wilsonloop1}
\input{wilsonloop2}%
\caption{The real part of the normalized Wilson loop $W(I)$ against
the physical area for various values of $N$.  At small areas
$\mbox{Re}[W(I)]$ follows the Gross-Witten area law, but at larger
areas it oscillates around zero.  The dashed lines are plotted to
guide the eye.\label{fig:Wil1a}}}


\FIGURE[t]{\input{wilsonloop3s}
\input{wilsonloop4s}%
\caption{The polar coordinates of the complex Wilson loop $W(I)$
plotted against the physical area $A = a^2 I^2$.  At small areas it is
approximately real and follows the Gross-Witten area law (solid line),
c.f.\ figure~\ref{fig:Wil1a}.  At larger areas the absolute value does
not seem to decay any more, and the phase agrees with the formula
$\Phi = A/\theta$, c.f. figure~\ref{fig:wl-phase4}.\label{fig:Wil1b}}}

Large-$N$ scaling is clearly confirmed. At small up to moderate areas,
the Wilson loop follows the area law of planar lattice gauge theory
given in eq.~(\ref{arealaw}), but at large areas it deviates and the
real part oscillates around zero instead.  This observation is
consistent over a wide range of $N$.  Remarkably, not even the
absolute value decays monotonously; at large areas it seems to
fluctuate around an approximately constant value. This is illustrated
in figure~\ref{fig:Wil1b} (on top).

Figure~\ref{fig:Wil1b} (below) shows that beyond the Gross-Witten
regime, the phase increases \emph{linearly} (in the physical area) in
the large-$N$ limit.  Additional measurements at $N/\beta =16$, 24 and
48, corresponding to different values of $\theta$, reveal that the
phase $\Phi$ of the Wilson loop $W(I)$ (beyond the Gross-Witten
regime) is, in fact, given to a very high precision by the simple
relation
\begin{equation}
\Phi = \frac{A}{\theta} \,,
\label{formula}
\end{equation}
\looseness=1where $A$ is the physical loop area, see figure~\ref{fig:wl-phase4}.
This has been confirmed also for other (non-square) rectangular Wilson
loops, which shows that the effect does not depend on the shape of the
Wilson loop.\footnote{Note, however, that the expectation values of
Wilson loops with the same area but with different shapes have in
general different absolute values in the double scaling limit.}
Indeed the formula~(\ref{formula}) agrees with the Aharonov-Bohm
effect in the presence of a constant magnetic field $B=1/ \theta$
across the plane.  This is reminiscent of the description of NC gauge
theory by Seiberg and Witten~\cite{SW}. Our numeric results seem to
support a picture of that kind, which is also known in solid state
physics~\cite{QHall}.

\FIGURE[t]{\input{nbeta2.tex}%
\caption{The phase of the Wilson loop $W(I)$ is plotted as a function
of the physical area $A=a^2 I^2$ for $N=125$ and various values of
$N/\beta$, corresponding to $\theta = 1.27, 1.91, 2.55, 3.82$.  For
large areas ($A \gtrsim O(\theta )$), the phase $\Phi$ agrees with the
formula $\Phi = A/\theta$, represented by the straight
lines.\label{fig:wl-phase4}}}

The observed large area behavior of the Wilson loop confirms that the
continuum limit of NC gauge theory is different from any
\emph{ordinary} (commutative) gauge theory, hence we have found a new
universality class.  Naively one might think that in the large area
regime $A \gg \sqrt{\theta}$, the effect of non-commutativity is
invisible.  The fact that we do observe the contrary can be understood
as a manifestation of non-perturbative UV/IR mixing.  This observation
also implies that the limit $\theta \rightarrow 0$ does not commute
with the continuum limit.

In the double scaling limit of the untwisted EK model, the expectation
value of the Wilson loop is real, and it remains positive even at
large physical areas~\cite{NN}.  This means that the two models,
twisted and untwisted, yield qualitatively \emph{different double
scaling limits}, although they become identical in the planar
large-$N$ limit.

\FIGURE[t]{\input{wilsontwo1}
\input{wilsontwo2}%
\caption{The 2-point function $G_{2}^{(W)}(I)$, defined in
eq.~(\ref{G2W}), with the renormalization factor given in
eq.~(\ref{wave1}) (bottom) and without (top), plotted against the
physical area, for $I=1 ,\dots ,N$.  The solid line connects the
results for $N=195$.\label{fig:Wil2}}}

Figure~\ref{fig:Wil2} shows the connected Wilson loop 2-point function
\begin{equation}
\label{G2W}
G_{2}^{(W)}(I) = \langle W_{12}(I \times I ) W_{21}(I \times I )
\rangle - \langle W_{12}(I \times I ) \rangle \langle W_{21}(I \times
I ) \rangle \in \R \,,
\end{equation}
again plotted against the physical area, for $I=1 ,\dots ,N$.  Here we
include a wave function renormalization factor
\begin{equation}
\label{wave1}
G_{2}^{(W)} \to \beta^{-0.6} G_{2}^{(W)} \,.
\end{equation}
The exponent $-0.6$ was found to be optimal for $G_{2}^{(W)}$ to
scale.  Indeed it leads to a neat large-$N$ scaling in some regime.

Next we consider the Polyakov line
\begin{equation}
P_{\mu}(I) = \Tr  \Bigl( U_{\mu}^{I} \Bigr) \,,
\end{equation}
which is also $\U(N)$ invariant and therefore has an interpretation as
a star gauge invariant observable in NC gauge theory.  In fact
\pagebreak[3]Polyakov lines are mapped to \emph{open} Wilson lines which carry
non-zero total momentum~\cite{IIKK}.  Their momentum $\vec{p}$ is
related to the separation vector $\vec{v}$ between the two ends of the
line.  In general the relation is given by $v_\mu = \Theta_{\mu\nu}
p_{\nu}$ modulo the periodicity of the torus.  In the present case,
the Polyakov line $P_{\mu}(I)$ corresponds to a momentum mode with
$p_{\nu} = 2 \pi \ell / (Na)$, where the integer $\ell$ is given by
$I/2$ and by $(I+N)/2$ for even and odd $I$, respectively.  In what
follows, we plot the results against $a I$ for even $I = 2 ,\dots
,N-1$.


\FIGURE[t]{\input{poltwo1}\\ \\
\input{poltwo2}
\caption{The 2-point function $G_{2}^{(P)}(I)$, defined in
eq.~(\ref{G2P}), with the renormalization factor given in
eq.~(\ref{wave1}) (bottom) and without (top), plotted against the
physical distance, for $I=2 ,\dots, N-1$.\label{fig:pol2}}}

The phase symmetry\footnote{In the terminology of NC gauge theory,
this corresponds to momentum conservation.}  makes $\langle P_{\mu}(I)
\rangle$ vanish, but the connected $n$-point functions \mbox{($n>1$)}
of Polyakov lines are sensible observables.  In figure~\ref{fig:pol2}
we show the 2-point function\footnote{The choice of the direction
$\mu$ is irrelevant. In practice we average over both possibilities in
order to enhance the statistics.}
\begin{equation}
\label{G2P}
G_{2}^{(P)}(I) = \langle P_{\mu}(I) P_{-\mu}(I) \rangle \,,
\end{equation}
where $P_{-\mu}(I) = \Tr (U_{\mu}^{\dagger \, I})$.  Note that there
is no disconnected part in $G_{2}^{(P)}$.  Again we insert the wave
function renormalization which was optimal for the Wilson 2-point
function,
\begin{equation} 
\label{renorm}
G_{2}^{(P)} \to \beta^{-0.6 } \, G_{2}^{(P)} \,.
\end{equation}
As a function of the physical length $aI$, the result is consistent
with large-$N$ scaling, as well as a \emph{universal} wave function
renormalization.  A similar wave function renormalization was also
observed in the EK model~\cite{NN}, where the optimal factor in
relation~(\ref{renorm}) is modified to $\beta^{-0.65}$.

\FIGURE[t]{\input{polthree2}%
\caption{The 3-point function $G_{3}^{(P)}(I)$, defined in
eq.~(\ref{G3P}) and rescaled by a universal renormalization factor,
plotted against the physical distance.\label{fig:pol3}}}

Our statistics was not sufficient to extract conclusive signals for
the connected parts of 3-point functions or even 4-point functions.
For completeness we present nevertheless our result for
\begin{equation} \label{G3P}
G_{3}^{(P)}(I) = \langle P_{\mu}(I)  P_{\mu}(I) P_{-\mu}(2I) \rangle
\end{equation}
(there is still no disconnected part).  In figure~\ref{fig:pol3} we
show our data after re-scaling, if we assume a universal wave function
renormalization, which is not ruled out.  This means that any
$n$-point function is renormalized as $G_{n} \to \beta^{-0.6n/2}G_{n}$
(for $n \geq 2$).


\section{Conclusions}\label{sec4}

We have investigated the 2d TEK in the form which allows for a mapping
onto 2d NC gauge theory on the lattice, by discrete Morita
equivalence. In this representation as a twisted reduced model, NC
gauge theory takes a form which can be simulated numerically. It
requires the specific twist given in eq.~(\ref{twist2}) and odd values
of $N$.

\pagebreak[3]

The first conclusion from our simulation results is that we do observe
a double scaling limit as $N, \, \beta \to \infty$. This corresponds
to the continuum limit of the NC rank-one gauge theory, which has
therefore also finite observables. This observation demonstrates the
non-perturbative renormalizability of 2d NC rank-one gauge theory.

The Wilson loop follows an area law at small physical areas, and in
this regime NC gauge theory agrees with planar standard gauge
theory. However, at larger areas the Wilson loop becomes complex and
the real part (the mean values over both loop orientations) begins to
oscillate around zero.  The phase is proportional to the physical area
enclosed by the Wilson loop, irrespectively of its shape, and the
coefficient of proportionality is given by the inverse of the
non-commutativity parameter $\theta$.  This agrees with the
Aharonov-Bohm effect in the presence of a constant magnetic background
field
\begin{equation}
B = \frac{1}{\theta} \,.
\end{equation}
Our results support this law, which is also a key element of the
Seiberg and Witten description of NC gauge theory~\cite{SW}. Moreover,
the same law also occurs in condensed matter physics: if one assumes a
plane crossed by a constant magnetic flux, then the electrons in this
plane can be projected to the lowest Landau level in a NC space, where
$\theta = \hbar c/eB $~\cite{QHall}.

The behavior of the Wilson loop at large areas implies that we have
found a qualitatively new universality class.  At first sight, it may
look surprising that the non-commutativity --- which introduces a
short-ranged non-locality in the action --- changes the IR behavior of
the gauge theory completely.  However, this effect does not appear
unnatural in the presence of UV/IR mixing. It is remarkable that this
mixing effect does not occur in the perturbative expansion of this
model, hence our results for large Wilson loops reveal a purely
non-perturbative UV/IR mixing.

For the connected Wilson loop 2-point function, as well as the 2-point
function of the Polyakov line, we can confirm the large-$N$
scaling. These observables are in agreement with a universal wave
function renormalization, which yields a factor $\beta^{-0.6}$ for a
connected $2$-point function.  This is similar to --- but not
identical with --- the universal renormalization factor which was
found for the (untwisted) EK model.\footnote{On the other hand, in the
hermitean matrix version of the (untwisted) reduced model, the
universal wave function renormalization holds only in the presence of
supersymmetry~\cite{4dSUSY}.}

Finally we should mention that in $d>2$, NC field theories are often
formulated such that the time coordinate is \emph{not} included in the
non-commutativity.  Including it causes especially severe conceptual
problems regarding causality etc. Therefore it would be important to
confirm non-perturbative renormalizability also in higher dimensions,
where non-commutativity is introduced only between spatial
coordinates.  We are currently simulating the 3d NC $\phi^{4}$
model~\cite{prep}, which can also be mapped onto a twisted reduced
matrix model~\cite{IIKK}.  A self consistent one-loop analysis in
$d=4$ suggests the appearance of an interesting phase
diagram~\cite{GS}.


\acknowledgments

It is a pleasure to thank Harald Dorn, Philippe de Forcrand and
Richard Szabo for inspiring remarks.


\begin{thebibliography}{50}

\bibitem{Sny}
H.S. Snyder, \emph{Quantized space-time}, \pr{71}{1947}{38}.

\bibitem{Con}
A. Connes and M. Rieffel, \emph{Yang-Mills for noncommutative two-tori},
\emph{Contempt.\ Math.\ Oper.\ Algebra Math.\ Phys.} {\bf 62} (1987) 237;\\
A. Connes, \emph{Noncommutative geometry}, Academic Press, San Diego 1994.

\bibitem{CDS}
A. Connes, M.R. Douglas and A. Schwarz, \emph{Noncommutative geometry
and Matrix theory: compactification on tori}, \jhep{02}{1998}{003}
[\hepth{9711162}];\\
R.~Kallosh, \emph{Bound states of branes with minimal energy},
\prd{55}{1997}{3241} [\hepth{9611162}].

\bibitem{DH}
M.R. Douglas and C.M. Hull, \emph{D-branes and the noncommutative
  torus}, \jhep{02}{1998}{008} [\hepth{9711165}].

\bibitem{SW}
N.~Seiberg and E.~Witten, \emph{String theory and noncommutative
  geometry}, \jhep{09}{1999}{032} [\hepth{9908142}].

\bibitem{QHall}
S.M. Girvin, A.H. MacDonald and P.M. Platzman,
\emph{Magneto-roton theory of collective excitations in the fractional 
quantum Hall effect}, \prb{33}{1986}{2481};\\
J. Bellissard, A. van Elst and H. Schulz-Baldes,
\emph{The non-commutative geometry of the quantum Hall effect},
\condmat{9411052};\\
S. Girvin, \emph{The quantum Hall effect: novel excitations and
broken symmetries}, in \emph{Proceedings of
Ecole d'Et\'{e}}, Les Houches 1998 [\condmat{9907002}].

\bibitem{DN}
M.R. Douglas and N.A. Nekrasov, \emph{Noncommutative field theory},
\rmp{73}{2001}{977} [\hepth{0106048}];\\
R.J. Szabo, \emph{Quantum field theory on noncommutative spaces},
  \hepth{0109162}.

\bibitem{Filk}
T.~Filk, \emph{Divergencies in a field theory on quantum space},
\plb{376}{1996}{53}.

\bibitem{Min}
S.~Minwalla, M.~Van~Raamsdonk and N.~Seiberg, \emph{Noncommutative
  perturbative dynamics}, \jhep{02}{2000}{020} [\hepth{9912072}].

\bibitem{Che}
I.~Chepelev and R.~Roiban, \emph{Renormalization of quantum field
  theories on noncommutative $R^d$, 1. Scalars}, \jhep{05}{2000}{037}
  [\hepth{9911098}].

\bibitem{RG}
L.~Griguolo and M.~Pietroni, \emph{Hard non-commutative loops
  resummation}, \prl{88}{2002}{071601} [\hepth{0102070}];\\
\emph{Wilsonian renormalization group and the non-commutative IR/UV
  connection}, \jhep{05}{2001}{032} [\hepth{0104217}];\\
S.~Sarkar, \emph{On the UV renormalizability of noncommutative field
  theories}, \jhep{06}{2002}{003} [\hepth{0202171}].

\bibitem{GGRS}
H.O. Girotti, M.~Gomes, V.O. Rivelles and A.J. da~Silva, \emph{A
  consistent noncommutative field theory: the Wess-Zumino model},
  \npb{587}{2000}{299} [\hepth{0005272}];\\
H.O. Girotti, M.~Gomes, A.Y. Petrov, V.O. Rivelles and A.J. da~Silva,
  \emph{The three-dimensional noncommutative nonlinear sigma model in
  superspace}, \plb{521}{2001}{119} [\hepth{0109222}].

\bibitem{GS}
S.S. Gubser and S.L. Sondhi, \emph{Phase structure of non-commutative
  scalar field theories}, \npb{605}{2001}{395} [\hepth{0006119}].

\bibitem{NCQED}
R.~Wulkenhaar, \emph{Non-renormalizability of theta-expanded
  noncommutative QED}, \jhep{03}{2002}{024} [\hepth{0112248}].

\bibitem{SP}
S. Profumo, \emph{Noncommutative principle chiral modes},
\hepth{0111285}.

\bibitem{Mafia}
L.~Griguolo, D.~Seminara and P.~Valtancoli, \emph{Towards the solution
  of noncommutative $YM_2$: Morita equivalence and large-$N$-limit},
  \jhep{12}{2001}{024} [\hepth{0110293}];\\
A.~Bassetto, G.~Nardelli and A.~Torrielli, \emph{Perturbative Wilson
  loop in two-dimensional non-commutative Yang-Mills theory},
  \npb{617}{2001}{308} [\hepth{0107147}];
\emph{Scaling properties of the perturbative Wilson loop in
two-dimensional non-commutative Yang-Mills theory}, \hepth{0205210};\\
L.D. Paniak and R.J. Szabo, \emph{Instanton expansion of
  noncommutative gauge theory in two dimensions}, \hepth{0203166}.

\bibitem{GAO}
A. Gonz\'{a}lez-Arroyo and M. Okawa, \emph{A twisted
model for large-$N$ lattice gauge theory}, \plb{120}{1983}{174};
\emph{The twisted Eguchi-Kawai model: a reduced model for
large-$N$ lattice gauge theory}, \prd{27}{1983}{2397}.

\bibitem{AIIKKT}
H.~Aoki, N. Ishibashi, S. Iso, H. Kawai, Y. Kitazawa and T. Tada,
\emph{Noncommutative Yang-Mills in IIB matrix model},
\npb{565}{2000}{176} [\hepth{9908141}].

\bibitem{AMNS}
J.~Ambj{\o}rn, Y.M. Makeenko, J.~Nishimura and R.J. Szabo,
  \emph{Finite N matrix models of noncommutative gauge theory},
  \jhep{11}{1999}{029} [\hepth{9911041}];
\emph{Nonperturbative dynamics of noncommutative gauge theory},
  \plb{480}{2000}{399} [\hepth{0002158}];\\
\emph{Lattice gauge fields and discrete noncommutative Yang-Mills
  theory}, \jhep{05}{2000}{023} [\hepth{0004147}].

\bibitem{EK}
T.~Eguchi and H.~Kawai, \emph{Reduction of dynamical degrees of
  freedom in the large-$N$ gauge theory}, \prl{48}{1982}{1063}.

\bibitem{BHN}
G.~Bhanot, U.M. Heller and H.~Neuberger, \emph{The quenched
  Eguchi-Kawai model}, \plb{113}{1982}{47};\\
U.M. Heller and H.~Neuberger, \emph{The role of gauge theories in
  constructing reduced models at infinite N}, \npb{207}{1982}{399}.

\bibitem{ABN}
K.N. Anagnostopoulos, W.~Bietenholz and J.~Nishimura, \emph{The area
  law in matrix models for large-$N$ QCD strings},
  \ijmpc{13}{2002}{555}  [\heplat{0112035}].

\bibitem{GA-KA}
A. Gonz\'{a}lez-Arroyo and C.P. Korthals Altes, \emph{Reduced model
for large-$N$ continuum field theories}, \plb{131}{1983}{2397}.

\bibitem{Fab1}
K.~Fabricius, O.~Haan and T.~Filk, \emph{Generalized twisted
  Eguchi-Kawai models}, \plb{144}{1984}{240}.

\bibitem{Fab2}
K.~Fabricius and O.~Haan, \emph{Numerical analysis of the twisted
  Eguchi-Kawai model in four-dimensions}, \plb{139}{1984}{293}.

\bibitem{JN}
J.~Nishimura, \emph{On existence of nontrivial fixed points in
  large-$N$ gauge theory in more than four dimensions},
  \mpla{11}{1996}{3049} [\heplat{9608119}].

\bibitem{GW}
D.J. Gross and E.~Witten, \emph{Possible third order phase transition
  in the large-$N$ lattice gauge theory}, \prd{21}{1980}{446}.

\bibitem{Fab3}
K.~Fabricius and O.~Haan, \emph{Numerical analysis of the twisted
  Eguchi-Kawai model in two-dimensions}, \plb{131}{1983}{399}.

\bibitem{NN}
T.~Nakajima and J.~Nishimura, \emph{Numerical study of the double
  scaling limit in two-dimensional large-$N$ reduced model},
  \npb{528}{1998}{355} [\hepth{9802082}].

\bibitem{ProfVic}
S.~Profumo and E.~Vicari, \emph{Twisted Eguchi-Kawai reduced chiral
  models}, \jhep{05}{2002}{014} [\hepth{0203155}].

\bibitem{Schwarz98}
A.~Schwarz, \emph{Morita equivalence and duality},
\npb{534}{1998}{720} [\hepth{9805034}].

\bibitem{IIKK}
N.~Ishibashi, S.~Iso, H.~Kawai and Y.~Kitazawa, \emph{Wilson loops in
  noncommutative Yang-Mills}, \npb{573}{2000}{573} [\hepth{9910004}].

\bibitem{HI}
A.~Hashimoto and N.~Itzhaki, \emph{On the hierarchy between
  non-commutative and ordinary supersymmetric Yang-Mills},
  \jhep{12}{1999}{007} [\hepth{9911057}].

\bibitem{Bars}
I.~Bars and D.~Minic, \emph{Non-commutative geometry on a discrete
  periodic lattice and gauge theory}, \prd{62}{2000}{105018}
  [\hepth{9910091}].

\bibitem{NCloops}
L.~Alvarez-Gaum\'e and S.R. Wadia, \emph{Gauge theory on a quantum
  phase space}, \plb{501}{2001}{319} [\hepth{0006219}];\\
S.R. Das and S.-J. Rey, \emph{Open Wilson lines in noncommutative
  gauge theory and tomography of holographic dual supergravity},
  \npb{590}{2000}{453} [\hepth{0008042}];\\
D.J. Gross, A.~Hashimoto and N.~Itzhaki, \emph{Observables of
  non-commutative gauge theories}, \atmp{4}{2000}{893}
  [\hepth{0008075}];\\
A.~Dhar and Y.~Kitazawa, \emph{Loop equation and Wilson line
  correlators in non-commutative gauge theories},
  \npb{613}{2001}{105} [\hepth{0104021}].

\bibitem{Nishimura:2001dq}
J.~Nishimura and M.A. V\'azquez-Mozo, \emph{Noncommutative chiral gauge
  theories on the lattice with manifest star-gauge invariance},
  \jhep{08}{2001}{033} [\hepth{0107110}].

\bibitem{Fab4}
K.~Fabricius and O.~Haan, \emph{Heat bath method for the twisted
  Eguchi-Kawai model}, \plb{143}{1984}{459}.

\bibitem{CM}
N. Cabbibo and E. Marinari, \emph{A new method for updating 
${\rm SU}(N)$ matrices in computer simulations of gauge theories},
\plb{119}{1982}{387}.

\bibitem{4dSUSY}
J.~Ambj{\o}rn, K.N. Anagnostopoulos, W.~Bietenholz, T.~Hotta and
  J.~Nishimura, \emph{Large-$N$ dynamics of dimensionally reduced 4d
  ${\rm SU}(N)$ super Yang-Mills theory}, \jhep{07}{2000}{013}
  [\hepth{0003208}].

\bibitem{prep}
W. Bietenholz, F. Hofheinz and J. Nishimura, in preparation.

\end{thebibliography}

\end{document}

nbeta2.tex
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/C2 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 90 180 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C3 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 180 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C4 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 180 270 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C5 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 90 arc
       2 copy moveto
       2 copy  vpt 180 270 arc closepath fill
               vpt 0 360 arc } bind def
/C6 { BL [] 0 setdash 2 copy moveto
      2 copy  vpt 90 270 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C7 { BL [] 0 setdash 2 copy moveto
      2 copy  vpt 0 270 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C8 { BL [] 0 setdash 2 copy moveto
      2 copy vpt 270 360 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C9 { BL [] 0 setdash 2 copy moveto
      2 copy  vpt 270 450 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C10 { BL [] 0 setdash 2 copy 2 copy moveto vpt 270 360 arc closepath fill
       2 copy moveto
       2 copy vpt 90 180 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C11 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 180 arc closepath fill
       2 copy moveto
       2 copy  vpt 270 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C12 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 180 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C13 { BL [] 0 setdash  2 copy moveto
       2 copy  vpt 0 90 arc closepath fill
       2 copy moveto
       2 copy  vpt 180 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C14 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 90 360 arc closepath fill
               vpt 0 360 arc } bind def
/C15 { BL [] 0 setdash 2 copy vpt 0 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/Rec   { newpath 4 2 roll moveto 1 index 0 rlineto 0 exch rlineto
       neg 0 rlineto closepath } bind def
/Square { dup Rec } bind def
/Bsquare { vpt sub exch vpt sub exch vpt2 Square } bind def
/S0 { BL [] 0 setdash 2 copy moveto 0 vpt rlineto BL Bsquare } bind def
/S1 { BL [] 0 setdash 2 copy vpt Square fill Bsquare } bind def
/S2 { BL [] 0 setdash 2 copy exch vpt sub exch vpt Square fill Bsquare } bind def
/S3 { BL [] 0 setdash 2 copy exch vpt sub exch vpt2 vpt Rec fill Bsquare } bind def
/S4 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt Square fill Bsquare } bind def
/S5 { BL [] 0 setdash 2 copy 2 copy vpt Square fill
       exch vpt sub exch vpt sub vpt Square fill Bsquare } bind def
/S6 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt vpt2 Rec fill Bsquare } bind def
/S7 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt vpt2 Rec fill
       2 copy vpt Square fill
       Bsquare } bind def
/S8 { BL [] 0 setdash 2 copy vpt sub vpt Square fill Bsquare } bind def
/S9 { BL [] 0 setdash 2 copy vpt sub vpt vpt2 Rec fill Bsquare } bind def
/S10 { BL [] 0 setdash 2 copy vpt sub vpt Square fill 2 copy exch vpt sub exch vpt Square fill
       Bsquare } bind def
/S11 { BL [] 0 setdash 2 copy vpt sub vpt Square fill 2 copy exch vpt sub exch vpt2 vpt Rec fill
       Bsquare } bind def
/S12 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill Bsquare } bind def
/S13 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill
       2 copy vpt Square fill Bsquare } bind def
/S14 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill
       2 copy exch vpt sub exch vpt Square fill Bsquare } bind def
/S15 { BL [] 0 setdash 2 copy Bsquare fill Bsquare } bind def
/D0 { gsave translate 45 rotate 0 0 S0 stroke grestore } bind def
/D1 { gsave translate 45 rotate 0 0 S1 stroke grestore } bind def
/D2 { gsave translate 45 rotate 0 0 S2 stroke grestore } bind def
/D3 { gsave translate 45 rotate 0 0 S3 stroke grestore } bind def
/D4 { gsave translate 45 rotate 0 0 S4 stroke grestore } bind def
/D5 { gsave translate 45 rotate 0 0 S5 stroke grestore } bind def
/D6 { gsave translate 45 rotate 0 0 S6 stroke grestore } bind def
/D7 { gsave translate 45 rotate 0 0 S7 stroke grestore } bind def
/D8 { gsave translate 45 rotate 0 0 S8 stroke grestore } bind def
/D9 { gsave translate 45 rotate 0 0 S9 stroke grestore } bind def
/D10 { gsave translate 45 rotate 0 0 S10 stroke grestore } bind def
/D11 { gsave translate 45 rotate 0 0 S11 stroke grestore } bind def
/D12 { gsave translate 45 rotate 0 0 S12 stroke grestore } bind def
/D13 { gsave translate 45 rotate 0 0 S13 stroke grestore } bind def
/D14 { gsave translate 45 rotate 0 0 S14 stroke grestore } bind def
/D15 { gsave translate 45 rotate 0 0 S15 stroke grestore } bind def
/DiaE { stroke [] 0 setdash vpt add M
  hpt neg vpt neg V hpt vpt neg V
  hpt vpt V hpt neg vpt V closepath stroke } def
/BoxE { stroke [] 0 setdash exch hpt sub exch vpt add M
  0 vpt2 neg V hpt2 0 V 0 vpt2 V
  hpt2 neg 0 V closepath stroke } def
/TriUE { stroke [] 0 setdash vpt 1.12 mul add M
  hpt neg vpt -1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt 1.62 mul V closepath stroke } def
/TriDE { stroke [] 0 setdash vpt 1.12 mul sub M
  hpt neg vpt 1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt -1.62 mul V closepath stroke } def
/PentE { stroke [] 0 setdash gsave
  translate 0 hpt M 4 {72 rotate 0 hpt L} repeat
  closepath stroke grestore } def
/CircE { stroke [] 0 setdash 
  hpt 0 360 arc stroke } def
/Opaque { gsave closepath 1 setgray fill grestore 0 setgray closepath } def
/DiaW { stroke [] 0 setdash vpt add M
  hpt neg vpt neg V hpt vpt neg V
  hpt vpt V hpt neg vpt V Opaque stroke } def
/BoxW { stroke [] 0 setdash exch hpt sub exch vpt add M
  0 vpt2 neg V hpt2 0 V 0 vpt2 V
  hpt2 neg 0 V Opaque stroke } def
/TriUW { stroke [] 0 setdash vpt 1.12 mul add M
  hpt neg vpt -1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt 1.62 mul V Opaque stroke } def
/TriDW { stroke [] 0 setdash vpt 1.12 mul sub M
  hpt neg vpt 1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt -1.62 mul V Opaque stroke } def
/PentW { stroke [] 0 setdash gsave
  translate 0 hpt M 4 {72 rotate 0 hpt L} repeat
  Opaque stroke grestore } def
/CircW { stroke [] 0 setdash 
  hpt 0 360 arc Opaque stroke } def
/BoxFill { gsave Rec 1 setgray fill grestore } def
end
%%EndProlog
}}%
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LTb
300 417 M
63 0 V
3087 0 R
-63 0 V
300 652 M
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3119 0 R
-31 0 V
300 887 M
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3087 0 R
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1875 300 M
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2190 300 M
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2505 300 M
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2820 300 M
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3135 300 M
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3450 300 M
0 63 V
0 1697 R
0 -63 V
1.000 UL
LTa
300 417 M
3150 0 V
1.000 UL
LTa
300 300 M
0 1760 V
1.000 UL
LTb
300 300 M
3150 0 V
0 1760 V
-3150 0 V
300 300 L
0.800 UP
1.000 UL
LT8
1056 1825 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
304 417 M
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30 3 R
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39 -1 R
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47 227 R
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55 60 R
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72 33 R
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79 33 R
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104 58 R
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113 76 R
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120 78 R
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129 66 R
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137 77 R
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145 84 R
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154 83 R
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304 417 Box
316 417 Box
337 417 Box
366 418 Box
402 418 Box
448 419 Box
501 420 Box
562 423 Box
632 422 Box
710 651 Box
796 713 Box
890 722 Box
993 756 Box
1103 789 Box
1222 831 Box
1349 883 Box
1484 942 Box
1628 1020 Box
1779 1099 Box
1939 1165 Box
2107 1242 Box
2283 1328 Box
2468 1411 Box
2660 1493 Box
2861 1582 Box
3070 1681 Box
3287 1783 Box
1181 1825 Box
0.800 UP
1.000 UL
LT1
1056 1725 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
306 417 M
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37 2 R
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50 4 R
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62 17 R
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-31 -1 R
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62 0 V
74 41 R
0 3 V
-31 -3 R
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87 130 R
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-31 -2 R
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99 48 R
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-31 -1 R
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-62 1 R
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112 31 R
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62 0 V
123 40 R
0 1 V
-31 -1 R
62 0 V
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62 0 V
137 44 R
0 1 V
-31 -1 R
62 0 V
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149 47 R
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-31 -3 R
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161 59 R
0 1 V
-31 -1 R
62 0 V
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62 0 V
173 65 R
0 1 V
-31 -1 R
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-62 1 R
62 0 V
186 65 R
0 1 V
-31 -1 R
62 0 V
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62 0 V
198 74 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
211 66 R
0 1 V
-31 -1 R
62 0 V
-62 1 R
62 0 V
223 80 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
236 74 R
0 1 V
-31 -1 R
62 0 V
-62 1 R
62 0 V
306 417 TriU
325 417 TriU
356 417 TriU
399 418 TriU
455 418 TriU
523 420 TriU
604 424 TriU
697 441 TriU
802 485 TriU
920 617 TriU
1050 666 TriU
1193 698 TriU
1347 739 TriU
1515 784 TriU
1695 833 TriU
1887 893 TriU
2091 960 TriU
2308 1025 TriU
2537 1101 TriU
2779 1168 TriU
3033 1250 TriU
3300 1326 TriU
1181 1725 TriU
0.800 UP
1.000 UL
LT1
1056 1625 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
308 417 M
-31 0 R
62 0 V
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27 1 R
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44 1 R
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61 4 R
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77 8 R
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-31 -1 R
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94 40 R
0 1 V
-31 -1 R
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111 78 R
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-31 -2 R
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-62 2 R
62 0 V
127 64 R
0 2 V
-31 -2 R
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-62 2 R
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144 37 R
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-31 -3 R
62 0 V
-62 3 R
62 0 V
161 31 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
177 44 R
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-31 -1 R
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194 50 R
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211 55 R
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-31 -3 R
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-62 3 R
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227 54 R
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-31 -2 R
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244 50 R
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-31 -1 R
62 0 V
-62 1 R
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261 74 R
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-31 -1 R
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-62 1 R
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277 60 R
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308 417 Circle
333 417 Circle
375 417 Circle
433 418 Circle
508 419 Circle
600 423 Circle
708 431 Circle
833 473 Circle
975 552 Circle
1133 618 Circle
1308 658 Circle
1500 691 Circle
1708 736 Circle
1933 787 Circle
2175 844 Circle
2433 901 Circle
2708 953 Circle
3000 1027 Circle
3308 1090 Circle
1181 1625 Circle
1.000 UL
LT0
300 417 M
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
32 15 V
32 15 V
31 14 V
32 15 V
32 15 V
32 14 V
32 15 V
32 14 V
31 15 V
32 15 V
32 14 V
1.000 UL
LT0
300 417 M
32 10 V
32 10 V
31 9 V
32 10 V
32 9 V
32 10 V
32 10 V
32 9 V
31 10 V
32 9 V
32 10 V
32 10 V
32 9 V
31 10 V
32 9 V
32 10 V
32 10 V
32 9 V
32 10 V
31 9 V
32 10 V
32 10 V
32 9 V
32 10 V
31 9 V
32 10 V
32 10 V
32 9 V
32 10 V
32 9 V
31 10 V
32 10 V
32 9 V
32 10 V
32 9 V
31 10 V
32 10 V
32 9 V
32 10 V
32 9 V
32 10 V
31 10 V
32 9 V
32 10 V
32 9 V
32 10 V
31 10 V
32 9 V
32 10 V
32 9 V
32 10 V
32 10 V
31 9 V
32 10 V
32 9 V
32 10 V
32 10 V
31 9 V
32 10 V
32 9 V
32 10 V
32 10 V
32 9 V
31 10 V
32 9 V
32 10 V
32 10 V
32 9 V
31 10 V
32 9 V
32 10 V
32 10 V
32 9 V
32 10 V
31 9 V
32 10 V
32 10 V
32 9 V
32 10 V
31 9 V
32 10 V
32 10 V
32 9 V
32 10 V
32 9 V
31 10 V
32 10 V
32 9 V
32 10 V
32 9 V
31 10 V
32 10 V
32 9 V
32 10 V
32 9 V
32 10 V
31 10 V
32 9 V
32 10 V
1.000 UL
LT0
300 417 M
32 7 V
32 7 V
31 7 V
32 8 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 8 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 8 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 8 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 8 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
32 7 V
32 7 V
32 7 V
31 7 V
32 7 V
32 7 V
1.000 UL
LT0
300 417 M
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
32 5 V
31 5 V
32 5 V
32 4 V
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
31 4 V
32 5 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
31 5 V
32 5 V
32 5 V
32 4 V
32 5 V
32 5 V
31 5 V
32 4 V
32 5 V
32 5 V
32 5 V
31 4 V
32 5 V
32 5 V
32 5 V
32 5 V
32 4 V
31 5 V
32 5 V
32 5 V
0.800 UP
1.000 UL
LT3
1056 1525 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
313 417 M
-31 0 R
62 0 V
-62 0 R
62 0 V
7 0 R
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62 0 V
-62 0 R
62 0 V
32 0 R
-31 0 R
62 0 V
-62 0 R
62 0 V
58 1 R
-31 0 R
62 0 V
-62 0 R
62 0 V
84 2 R
-31 0 R
62 0 V
-62 0 R
62 0 V
109 10 R
0 1 V
-31 -1 R
62 0 V
-62 1 R
62 0 V
134 19 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
160 64 R
0 4 V
-31 -4 R
62 0 V
-62 4 R
62 0 V
185 41 R
0 3 V
-31 -3 R
62 0 V
-62 3 R
62 0 V
211 40 R
0 1 V
-31 -1 R
62 0 V
-62 1 R
62 0 V
236 32 R
0 5 V
-31 -5 R
62 0 V
-62 5 R
62 0 V
261 46 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
287 49 R
0 7 V
-31 -7 R
62 0 V
-62 7 R
62 0 V
312 38 R
0 2 V
-31 -2 R
62 0 V
-62 2 R
62 0 V
338 52 R
0 11 V
-31 -11 R
62 0 V
-62 11 R
62 0 V
313 417 TriD
351 417 TriD
414 417 TriD
503 418 TriD
618 420 TriD
758 430 TriD
923 451 TriD
1114 518 TriD
1330 563 TriD
1572 605 TriD
1839 639 TriD
2131 689 TriD
2449 742 TriD
2792 785 TriD
3161 844 TriD
1181 1525 TriD
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polthree2.tex
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poltwo1.tex
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poltwo2.tex
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wilsonloop1.tex
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wilsonloop2.tex
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%%Title: wilson-loop2.tex
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%%CreationDate: Wed Mar 13 14:38:42 2002
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/UP { dup vpt_ mul /vpt exch def hpt_ mul /hpt exch def
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/LT6 { PL [2 dl 2 dl 2 dl 4 dl] 0 0 0 DL } def
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/TriD { stroke [] 0 setdash 2 copy vpt 1.12 mul sub M
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/Circle { stroke [] 0 setdash 2 copy
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/CircleF { stroke [] 0 setdash hpt 0 360 arc fill } def
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/C3 { BL [] 0 setdash 2 copy moveto
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/C8 { BL [] 0 setdash 2 copy moveto
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/C15 { BL [] 0 setdash 2 copy vpt 0 360 arc closepath fill
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/Rec   { newpath 4 2 roll moveto 1 index 0 rlineto 0 exch rlineto
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/Square { dup Rec } bind def
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/S4 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt Square fill Bsquare } bind def
/S5 { BL [] 0 setdash 2 copy 2 copy vpt Square fill
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/S7 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt vpt2 Rec fill
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/S8 { BL [] 0 setdash 2 copy vpt sub vpt Square fill Bsquare } bind def
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/S10 { BL [] 0 setdash 2 copy vpt sub vpt Square fill 2 copy exch vpt sub exch vpt Square fill
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/S12 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill Bsquare } bind def
/S13 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill
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/S15 { BL [] 0 setdash 2 copy Bsquare fill Bsquare } bind def
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/D7 { gsave translate 45 rotate 0 0 S7 stroke grestore } bind def
/D8 { gsave translate 45 rotate 0 0 S8 stroke grestore } bind def
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/Opaque { gsave closepath 1 setgray fill grestore 0 setgray closepath } def
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wilsonloop3s.tex
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%%Title: wilson-loop3.tex
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%%CreationDate: Fri Apr  5 12:56:45 2002
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482 1460 Box
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736 1058 Box
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2236 519 Box
2482 667 Box
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1.000 UL
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1.000 UL
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913 770 TriU
1001 658 TriU
1096 606 TriU
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1311 640 TriU
1429 680 TriU
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1.000 UL
LT0
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602 1268 TriD
638 1212 TriD
677 1150 TriD
721 1083 TriD
768 1008 TriD
818 928 TriD
873 837 TriD
931 742 TriD
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1059 598 TriD
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1201 618 TriD
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1359 656 TriD
1444 641 TriD
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1720 641 TriD
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2622 593 TriD
2751 549 TriD
2885 578 TriD
3022 507 TriD
3163 561 TriD
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LT2
454 1505 M
11 -19 V
19 -31 V
27 -43 V
35 -55 V
42 -67 V
49 -79 V
58 -90 V
65 -105 V
833 901 L
913 770 L
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104 56 V
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142 -65 V
149 42 V
157 -83 V
164 59 V
172 -95 V
180 69 V
188 -98 V
195 84 V
3238 461 L
211 116 V
1 -1 V
1.000 UL
LT2
458 1498 M
24 -38 V
39 -64 V
56 -89 V
71 -114 V
88 -135 V
839 890 L
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1093 539 L
151 134 V
166 -57 V
183 71 V
1791 576 L
215 81 V
2236 519 L
246 148 V
2744 460 L
278 179 V
3315 393 L
135 103 V
1.000 UL
LT2
452 1508 M
6 -9 V
9 -15 V
13 -22 V
17 -27 V
21 -33 V
24 -39 V
28 -45 V
32 -50 V
36 -56 V
39 -62 V
44 -67 V
47 -75 V
50 -80 V
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100 -38 V
103 22 V
107 -54 V
111 38 V
114 -36 V
119 27 V
122 -44 V
126 37 V
129 -44 V
134 29 V
137 -71 V
141 54 V
145 -64 V
142 60 V
1.000 UL
LT2
455 1503 M
15 -25 V
25 -40 V
35 -57 V
46 -72 V
55 -87 V
65 -103 V
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953 731 L
1058 612 L
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146 -67 V
156 43 V
166 -79 V
176 63 V
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3109 440 L
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104 -81 V
1.000 UL
LT0
450 1511 M
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wilsonloop4s.tex
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%%Title: wilson-loop4.tex
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%%CreationDate: Fri Apr  5 12:56:45 2002
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gnudict begin
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/Cshow { currentpoint stroke M
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/C2 { BL [] 0 setdash 2 copy moveto
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/C3 { BL [] 0 setdash 2 copy moveto
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/C4 { BL [] 0 setdash 2 copy moveto
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/C5 { BL [] 0 setdash 2 copy moveto
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       2 copy moveto
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               vpt 0 360 arc } bind def
/C6 { BL [] 0 setdash 2 copy moveto
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/C7 { BL [] 0 setdash 2 copy moveto
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/C8 { BL [] 0 setdash 2 copy moveto
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/C9 { BL [] 0 setdash 2 copy moveto
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/C10 { BL [] 0 setdash 2 copy 2 copy moveto vpt 270 360 arc closepath fill
       2 copy moveto
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/C11 { BL [] 0 setdash 2 copy moveto
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       2 copy moveto
       2 copy  vpt 270 360 arc closepath fill
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/C12 { BL [] 0 setdash 2 copy moveto
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/C13 { BL [] 0 setdash  2 copy moveto
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       2 copy moveto
       2 copy  vpt 180 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C14 { BL [] 0 setdash 2 copy moveto
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               vpt 0 360 arc } bind def
/C15 { BL [] 0 setdash 2 copy vpt 0 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/Rec   { newpath 4 2 roll moveto 1 index 0 rlineto 0 exch rlineto
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/Square { dup Rec } bind def
/Bsquare { vpt sub exch vpt sub exch vpt2 Square } bind def
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/S1 { BL [] 0 setdash 2 copy vpt Square fill Bsquare } bind def
/S2 { BL [] 0 setdash 2 copy exch vpt sub exch vpt Square fill Bsquare } bind def
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wilsontwo1.tex
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/DL { Color {setrgbcolor Solid {pop []} if 0 setdash }
 {pop pop pop Solid {pop []} if 0 setdash} ifelse } def
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/LT3 { PL [1 dl 1.5 dl] 1 0 1 DL } def
/LT4 { PL [5 dl 2 dl 1 dl 2 dl] 0 1 1 DL } def
/LT5 { PL [4 dl 3 dl 1 dl 3 dl] 1 1 0 DL } def
/LT6 { PL [2 dl 2 dl 2 dl 4 dl] 0 0 0 DL } def
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  hpt vpt V hpt neg vpt V closepath stroke
  Pnt } def
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  currentpoint stroke M
  hpt neg vpt neg R hpt2 0 V stroke
  } def
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  hpt2 neg 0 V closepath stroke
  Pnt } def
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  hpt 2 mul 0 V
  hpt neg vpt 1.62 mul V closepath stroke
  Pnt  } def
/Star { 2 copy Pls Crs } def
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/TriD { stroke [] 0 setdash 2 copy vpt 1.12 mul sub M
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  hpt 2 mul 0 V
  hpt neg vpt -1.62 mul V closepath stroke
  Pnt  } def
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  hpt 2 mul 0 V
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  hpt vpt V hpt neg vpt V closepath fill } def
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  closepath stroke grestore Pnt } def
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  translate 0 hpt M 4 {72 rotate 0 hpt L} repeat
  closepath fill grestore } def
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  hpt 0 360 arc stroke Pnt } def
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               vpt 0 360 arc closepath } bind def
/C2 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 90 180 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C3 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 180 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C4 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 180 270 arc closepath fill
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/C5 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 90 arc
       2 copy moveto
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               vpt 0 360 arc } bind def
/C6 { BL [] 0 setdash 2 copy moveto
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/C7 { BL [] 0 setdash 2 copy moveto
      2 copy  vpt 0 270 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C8 { BL [] 0 setdash 2 copy moveto
      2 copy vpt 270 360 arc closepath fill
              vpt 0 360 arc closepath } bind def
/C9 { BL [] 0 setdash 2 copy moveto
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/C10 { BL [] 0 setdash 2 copy 2 copy moveto vpt 270 360 arc closepath fill
       2 copy moveto
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               vpt 0 360 arc closepath } bind def
/C11 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 0 180 arc closepath fill
       2 copy moveto
       2 copy  vpt 270 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C12 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 180 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C13 { BL [] 0 setdash  2 copy moveto
       2 copy  vpt 0 90 arc closepath fill
       2 copy moveto
       2 copy  vpt 180 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/C14 { BL [] 0 setdash 2 copy moveto
       2 copy  vpt 90 360 arc closepath fill
               vpt 0 360 arc } bind def
/C15 { BL [] 0 setdash 2 copy vpt 0 360 arc closepath fill
               vpt 0 360 arc closepath } bind def
/Rec   { newpath 4 2 roll moveto 1 index 0 rlineto 0 exch rlineto
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/Square { dup Rec } bind def
/Bsquare { vpt sub exch vpt sub exch vpt2 Square } bind def
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/S1 { BL [] 0 setdash 2 copy vpt Square fill Bsquare } bind def
/S2 { BL [] 0 setdash 2 copy exch vpt sub exch vpt Square fill Bsquare } bind def
/S3 { BL [] 0 setdash 2 copy exch vpt sub exch vpt2 vpt Rec fill Bsquare } bind def
/S4 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt Square fill Bsquare } bind def
/S5 { BL [] 0 setdash 2 copy 2 copy vpt Square fill
       exch vpt sub exch vpt sub vpt Square fill Bsquare } bind def
/S6 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt vpt2 Rec fill Bsquare } bind def
/S7 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt vpt2 Rec fill
       2 copy vpt Square fill
       Bsquare } bind def
/S8 { BL [] 0 setdash 2 copy vpt sub vpt Square fill Bsquare } bind def
/S9 { BL [] 0 setdash 2 copy vpt sub vpt vpt2 Rec fill Bsquare } bind def
/S10 { BL [] 0 setdash 2 copy vpt sub vpt Square fill 2 copy exch vpt sub exch vpt Square fill
       Bsquare } bind def
/S11 { BL [] 0 setdash 2 copy vpt sub vpt Square fill 2 copy exch vpt sub exch vpt2 vpt Rec fill
       Bsquare } bind def
/S12 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill Bsquare } bind def
/S13 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill
       2 copy vpt Square fill Bsquare } bind def
/S14 { BL [] 0 setdash 2 copy exch vpt sub exch vpt sub vpt2 vpt Rec fill
       2 copy exch vpt sub exch vpt Square fill Bsquare } bind def
/S15 { BL [] 0 setdash 2 copy Bsquare fill Bsquare } bind def
/D0 { gsave translate 45 rotate 0 0 S0 stroke grestore } bind def
/D1 { gsave translate 45 rotate 0 0 S1 stroke grestore } bind def
/D2 { gsave translate 45 rotate 0 0 S2 stroke grestore } bind def
/D3 { gsave translate 45 rotate 0 0 S3 stroke grestore } bind def
/D4 { gsave translate 45 rotate 0 0 S4 stroke grestore } bind def
/D5 { gsave translate 45 rotate 0 0 S5 stroke grestore } bind def
/D6 { gsave translate 45 rotate 0 0 S6 stroke grestore } bind def
/D7 { gsave translate 45 rotate 0 0 S7 stroke grestore } bind def
/D8 { gsave translate 45 rotate 0 0 S8 stroke grestore } bind def
/D9 { gsave translate 45 rotate 0 0 S9 stroke grestore } bind def
/D10 { gsave translate 45 rotate 0 0 S10 stroke grestore } bind def
/D11 { gsave translate 45 rotate 0 0 S11 stroke grestore } bind def
/D12 { gsave translate 45 rotate 0 0 S12 stroke grestore } bind def
/D13 { gsave translate 45 rotate 0 0 S13 stroke grestore } bind def
/D14 { gsave translate 45 rotate 0 0 S14 stroke grestore } bind def
/D15 { gsave translate 45 rotate 0 0 S15 stroke grestore } bind def
/DiaE { stroke [] 0 setdash vpt add M
  hpt neg vpt neg V hpt vpt neg V
  hpt vpt V hpt neg vpt V closepath stroke } def
/BoxE { stroke [] 0 setdash exch hpt sub exch vpt add M
  0 vpt2 neg V hpt2 0 V 0 vpt2 V
  hpt2 neg 0 V closepath stroke } def
/TriUE { stroke [] 0 setdash vpt 1.12 mul add M
  hpt neg vpt -1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt 1.62 mul V closepath stroke } def
/TriDE { stroke [] 0 setdash vpt 1.12 mul sub M
  hpt neg vpt 1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt -1.62 mul V closepath stroke } def
/PentE { stroke [] 0 setdash gsave
  translate 0 hpt M 4 {72 rotate 0 hpt L} repeat
  closepath stroke grestore } def
/CircE { stroke [] 0 setdash 
  hpt 0 360 arc stroke } def
/Opaque { gsave closepath 1 setgray fill grestore 0 setgray closepath } def
/DiaW { stroke [] 0 setdash vpt add M
  hpt neg vpt neg V hpt vpt neg V
  hpt vpt V hpt neg vpt V Opaque stroke } def
/BoxW { stroke [] 0 setdash exch hpt sub exch vpt add M
  0 vpt2 neg V hpt2 0 V 0 vpt2 V
  hpt2 neg 0 V Opaque stroke } def
/TriUW { stroke [] 0 setdash vpt 1.12 mul add M
  hpt neg vpt -1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt 1.62 mul V Opaque stroke } def
/TriDW { stroke [] 0 setdash vpt 1.12 mul sub M
  hpt neg vpt 1.62 mul V
  hpt 2 mul 0 V
  hpt neg vpt -1.62 mul V Opaque stroke } def
/PentW { stroke [] 0 setdash gsave
  translate 0 hpt M 4 {72 rotate 0 hpt L} repeat
  Opaque stroke grestore } def
/CircW { stroke [] 0 setdash 
  hpt 0 360 arc Opaque stroke } def
/BoxFill { gsave Rec 1 setgray fill grestore } def
end
%%EndProlog
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-31 -7 R
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977 933 TriU
1331 1586 TriU
1539 1840 TriU
1686 1896 TriU
1800 1855 TriU
1893 1808 TriU
1972 1766 TriU
2040 1747 TriU
2100 1697 TriU
2154 1704 TriU
2203 1702 TriU
2247 1691 TriU
2288 1663 TriU
2326 1690 TriU
2361 1679 TriU
2394 1683 TriU
2425 1675 TriU
2455 1716 TriU
2482 1701 TriU
2509 1714 TriU
2534 1692 TriU
2557 1705 TriU
2580 1732 TriU
2602 1723 TriU
2623 1707 TriU
2643 1725 TriU
2662 1723 TriU
2681 1747 TriU
2699 1758 TriU
2716 1759 TriU
2733 1755 TriU
2749 1756 TriU
2765 1786 TriU
2780 1781 TriU
2795 1783 TriU
2809 1784 TriU
2823 1804 TriU
2837 1771 TriU
2850 1818 TriU
2863 1799 TriU
2876 1814 TriU
2888 1818 TriU
2900 1845 TriU
2912 1846 TriU
2923 1879 TriU
2934 1821 TriU
2945 1864 TriU
2956 1805 TriU
2967 1858 TriU
2977 1849 TriU
2987 1869 TriU
2997 1849 TriU
3007 1897 TriU
3016 1858 TriU
3026 1921 TriU
2575 1074 TriU
0.800 UP
1.000 UL
LT0
2450 974 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
858 710 M
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-31 -6 R
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324 729 R
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176 334 R
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116 143 R
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83 30 R
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62 -30 R
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48 -46 R
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38 -64 R
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29 -55 R
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23 -17 R
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17 -58 R
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10 -44 R
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-31 -14 R
62 0 V
currentpoint stroke M
-62 14 R
62 0 V
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62 0 V
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62 0 V
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-31 -13 R
62 0 V
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62 0 V
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62 0 V
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0 6 V
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62 0 V
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62 0 V
-24 -9 R
0 10 V
-31 -10 R
62 0 V
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62 0 V
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0 10 V
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62 0 V
-62 10 R
62 0 V
-24 -49 R
0 13 V
-31 -13 R
62 0 V
-62 13 R
62 0 V
-25 49 R
0 16 V
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62 0 V
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62 0 V
-24 -65 R
0 16 V
-31 -16 R
62 0 V
-62 16 R
62 0 V
-25 44 R
0 9 V
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62 0 V
-62 9 R
62 0 V
-24 -62 R
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62 0 V
-62 9 R
62 0 V
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62 0 V
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62 0 V
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62 0 V
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62 0 V
-25 52 R
0 8 V
-31 -8 R
62 0 V
-62 8 R
62 0 V
858 713 TriD
1213 1448 TriD
1420 1788 TriD
1567 1938 TriD
1681 1977 TriD
1774 1955 TriD
1853 1917 TriD
1922 1864 TriD
1982 1817 TriD
2036 1807 TriD
2084 1759 TriD
2129 1772 TriD
2170 1733 TriD
2208 1754 TriD
2243 1719 TriD
2276 1727 TriD
2307 1676 TriD
2336 1721 TriD
2364 1705 TriD
2390 1710 TriD
2415 1686 TriD
2439 1702 TriD
2461 1702 TriD
2483 1683 TriD
2504 1661 TriD
2524 1704 TriD
2543 1710 TriD
2562 1721 TriD
2580 1694 TriD
2597 1706 TriD
2614 1697 TriD
2630 1698 TriD
2646 1699 TriD
2661 1725 TriD
2676 1705 TriD
2690 1727 TriD
2705 1745 TriD
2718 1725 TriD
2731 1729 TriD
2744 1737 TriD
2757 1753 TriD
2769 1738 TriD
2781 1755 TriD
2793 1759 TriD
2805 1762 TriD
2816 1764 TriD
2827 1777 TriD
2838 1749 TriD
2848 1751 TriD
2858 1760 TriD
2869 1784 TriD
2878 1768 TriD
2888 1799 TriD
2898 1797 TriD
2907 1797 TriD
2916 1789 TriD
2925 1814 TriD
2934 1783 TriD
2943 1803 TriD
2952 1808 TriD
2960 1847 TriD
2968 1801 TriD
2977 1862 TriD
2985 1823 TriD
2993 1840 TriD
3000 1817 TriD
3008 1850 TriD
3016 1817 TriD
3023 1854 TriD
3030 1831 TriD
3038 1882 TriD
3045 1850 TriD
3052 1850 TriD
3059 1849 TriD
3066 1873 TriD
3073 1836 TriD
3079 1899 TriD
3086 1850 TriD
3092 1907 TriD
3099 1853 TriD
3105 1891 TriD
3111 1848 TriD
3118 1893 TriD
3124 1856 TriD
3130 1916 TriD
2575 974 TriD
0.800 UP
1.000 UL
LT0
2450 874 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
756 505 M
0 6 V
-31 -6 R
62 0 V
-62 6 R
62 0 V
323 792 R
0 11 V
-31 -11 R
62 0 V
-62 11 R
62 0 V
176 395 R
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-31 -10 R
62 0 V
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62 0 V
116 192 R
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62 0 V
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62 0 V
84 87 R
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62 0 V
-62 5 R
62 0 V
62 29 R
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48 -34 R
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62 0 V
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37 -30 R
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29 -45 R
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23 -40 R
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62 0 V
18 -39 R
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13 -21 R
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10 -57 R
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7 -26 R
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4 -58 R
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2 31 R
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0 -56 R
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0 12 V
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62 0 V
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62 0 V
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0 5 V
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62 0 V
currentpoint stroke M
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62 0 V
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0 12 V
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62 0 V
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62 0 V
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62 0 V
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0 11 V
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62 0 V
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62 0 V
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0 5 V
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62 0 V
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62 0 V
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0 11 V
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62 0 V
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62 0 V
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0 23 V
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62 0 V
-62 23 R
62 0 V
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0 6 V
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62 0 V
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62 0 V
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0 16 V
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62 0 V
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62 0 V
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0 8 V
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62 0 V
-62 8 R
62 0 V
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0 1 V
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62 0 V
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62 0 V
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0 13 V
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62 0 V
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62 0 V
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0 16 V
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62 0 V
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62 0 V
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0 17 V
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62 0 V
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62 0 V
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0 8 V
-31 -8 R
62 0 V
-62 8 R
62 0 V
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0 14 V
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62 0 V
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62 0 V
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0 23 V
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-62 23 R
62 0 V
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0 11 V
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62 0 V
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62 0 V
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62 0 V
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62 0 V
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62 0 V
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62 0 V
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0 11 V
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62 0 V
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62 0 V
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0 17 V
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62 0 V
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0 18 V
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62 0 V
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62 0 V
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62 0 V
-62 17 R
62 0 V
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0 6 V
-31 -6 R
62 0 V
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62 0 V
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0 14 V
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62 0 V
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62 0 V
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0 10 V
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62 0 V
-62 10 R
62 0 V
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wilsontwo2.tex
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%%Title: wilson-two2.tex
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0 -31 V
2006 300 M
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2062 300 M
0 63 V
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2236 300 M
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2411 300 M
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2512 300 M
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2585 300 M
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2641 300 M
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2815 300 M
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2989 300 M
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3091 300 M
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3164 300 M
0 31 V
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3220 300 M
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3394 300 M
0 31 V
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0 -31 V
1.000 UL
LTb
500 300 M
2950 0 V
0 1976 V
-2950 0 V
500 300 L
1.000 UL
LTb
1967 639 M
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0 -600 V
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0.800 UP
1.000 UL
LT0
2467 1189 M
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1244 1561 M
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81 -43 R
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1244 1563 Box
1592 1980 Box
1796 1995 Box
1941 1963 Box
2053 1924 Box
2145 1933 Box
2222 1947 Box
2289 1933 Box
2348 1954 Box
2401 1952 Box
2449 1973 Box
2493 1967 Box
2533 2004 Box
2571 1993 Box
2605 2006 Box
2638 2007 Box
2668 2022 Box
2697 2058 Box
2724 2077 Box
2750 2023 Box
2774 2087 Box
2798 2093 Box
2820 2094 Box
2842 2090 Box
2862 2150 Box
2592 1189 Box
0.800 UP
1.000 UL
LT0
2467 1089 M
250 0 V
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1144 1369 Circle
1493 1894 Circle
1697 2019 Circle
1841 1995 Circle
1953 1948 Circle
2045 1920 Circle
2123 1882 Circle
2190 1905 Circle
2249 1893 Circle
2302 1911 Circle
2350 1895 Circle
2393 1900 Circle
2434 1922 Circle
2471 1930 Circle
2506 1930 Circle
2538 1916 Circle
2569 1929 Circle
2597 1961 Circle
2624 1936 Circle
2650 1952 Circle
2675 1961 Circle
2698 1969 Circle
2721 1975 Circle
2742 1968 Circle
2762 2028 Circle
2782 2016 Circle
2801 2025 Circle
2819 1998 Circle
2837 2074 Circle
2854 2048 Circle
2871 2068 Circle
2887 2059 Circle
2902 2113 Circle
2917 2058 Circle
2932 2108 Circle
2592 1089 Circle
0.800 UP
1.000 UL
LT0
2467 989 M
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250 62 R
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1018 1092 M
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1018 1095 TriU
1367 1735 TriU
1571 1983 TriU
1715 2038 TriU
1827 1998 TriU
1919 1953 TriU
1996 1911 TriU
2064 1892 TriU
2123 1844 TriU
2176 1851 TriU
2224 1848 TriU
2267 1838 TriU
2308 1810 TriU
2345 1836 TriU
2380 1825 TriU
2412 1830 TriU
2443 1822 TriU
2471 1862 TriU
2498 1847 TriU
2524 1860 TriU
2549 1839 TriU
2572 1851 TriU
2595 1878 TriU
2616 1869 TriU
2636 1853 TriU
2656 1871 TriU
2675 1869 TriU
2693 1892 TriU
2711 1903 TriU
2728 1905 TriU
2745 1901 TriU
2761 1901 TriU
2776 1930 TriU
2791 1926 TriU
2806 1928 TriU
2820 1929 TriU
2834 1948 TriU
2847 1916 TriU
2860 1962 TriU
2873 1943 TriU
2885 1958 TriU
2897 1962 TriU
2909 1989 TriU
2921 1989 TriU
2932 2021 TriU
2943 1965 TriU
2954 2007 TriU
2964 1950 TriU
2975 2001 TriU
2985 1992 TriU
2995 2012 TriU
3005 1992 TriU
3014 2040 TriU
3024 2002 TriU
3033 2063 TriU
2592 989 TriU
0.800 UP
1.000 UL
LT0
2467 889 M
250 0 V
-250 31 R
0 -62 V
250 62 R
0 -62 V
902 819 M
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currentpoint stroke M
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2756 1824 TriD
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2804 1845 TriD
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1034 1099 Pent
1238 1540 Pent
1383 1814 Pent
1495 1976 Pent
1587 2057 Pent
1664 2100 Pent
1731 2112 Pent
1790 2084 Pent
1843 2059 Pent
1891 2026 Pent
1935 2013 Pent
1975 1965 Pent
2013 1949 Pent
2047 1915 Pent
2080 1923 Pent
2110 1858 Pent
2139 1860 Pent
2166 1834 Pent
2192 1823 Pent
2216 1789 Pent
2240 1789 Pent
2262 1771 Pent
2284 1762 Pent
2304 1729 Pent
2324 1771 Pent
2343 1736 Pent
2361 1742 Pent
2379 1714 Pent
2396 1746 Pent
2412 1686 Pent
2428 1719 Pent
2444 1680 Pent
2459 1732 Pent
2473 1684 Pent
2487 1697 Pent
2501 1670 Pent
2515 1696 Pent
2528 1665 Pent
2540 1696 Pent
2553 1654 Pent
2565 1715 Pent
2577 1660 Pent
2588 1688 Pent
2600 1664 Pent
2611 1671 Pent
2621 1648 Pent
2632 1726 Pent
2642 1656 Pent
2653 1683 Pent
2662 1680 Pent
2672 1700 Pent
2682 1663 Pent
2691 1683 Pent
2700 1654 Pent
2709 1698 Pent
2718 1659 Pent
2727 1686 Pent
2736 1668 Pent
2744 1654 Pent
2752 1680 Pent
2761 1672 Pent
2769 1671 Pent
2777 1685 Pent
2784 1672 Pent
2792 1672 Pent
2800 1671 Pent
2807 1698 Pent
2814 1679 Pent
2822 1704 Pent
2829 1671 Pent
2836 1683 Pent
2843 1700 Pent
2850 1697 Pent
2856 1667 Pent
2863 1718 Pent
2870 1698 Pent
2876 1687 Pent
2882 1679 Pent
2889 1700 Pent
2895 1694 Pent
2901 1669 Pent
2907 1692 Pent
2913 1698 Pent
2919 1713 Pent
2925 1712 Pent
2931 1711 Pent
2937 1691 Pent
2942 1707 Pent
2948 1716 Pent
2954 1727 Pent
2959 1718 Pent
2964 1715 Pent
2970 1726 Pent
2975 1716 Pent
2980 1697 Pent
2986 1735 Pent
2991 1717 Pent
2996 1732 Pent
3001 1705 Pent
3006 1741 Pent
3011 1708 Pent
3016 1749 Pent
3021 1707 Pent
3025 1778 Pent
3030 1704 Pent
3035 1732 Pent
3040 1738 Pent
3044 1759 Pent
3049 1766 Pent
3053 1743 Pent
3058 1738 Pent
3062 1746 Pent
3067 1750 Pent
3071 1765 Pent
3076 1741 Pent
3080 1768 Pent
3084 1739 Pent
3088 1751 Pent
3093 1718 Pent
3097 1763 Pent
3101 1749 Pent
3105 1761 Pent
3109 1763 Pent
3113 1764 Pent
3117 1756 Pent
3121 1773 Pent
3125 1753 Pent
3129 1801 Pent
3133 1768 Pent
3137 1808 Pent
3141 1803 Pent
3144 1785 Pent
3148 1787 Pent
3152 1797 Pent
3156 1796 Pent
3159 1816 Pent
3163 1779 Pent
3167 1782 Pent
3170 1778 Pent
3174 1808 Pent
3177 1771 Pent
3181 1833 Pent
3184 1792 Pent
3188 1821 Pent
3191 1789 Pent
3195 1814 Pent
3198 1766 Pent
3201 1809 Pent
3205 1773 Pent
3208 1816 Pent
3211 1786 Pent
3215 1816 Pent
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3221 1845 Pent
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3231 1765 Pent
3234 1839 Pent
3237 1826 Pent
3240 1828 Pent
3243 1851 Pent
3247 1824 Pent
3250 1820 Pent
3253 1820 Pent
3256 1802 Pent
3259 1863 Pent
3262 1823 Pent
3265 1866 Pent
3268 1860 Pent
3271 1817 Pent
3274 1825 Pent
3277 1852 Pent
3279 1799 Pent
3282 1851 Pent
3285 1815 Pent
3288 1892 Pent
3291 1814 Pent
3294 1875 Pent
3296 1852 Pent
3299 1858 Pent
3302 1818 Pent
3305 1839 Pent
3308 1814 Pent
3310 1873 Pent
3313 1833 Pent
3316 1892 Pent
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3321 1856 Pent
3324 1800 Pent
3326 1872 Pent
3329 1889 Pent
3332 1888 Pent
3334 1824 Pent
3337 1846 Pent
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686 347 M
348 752 V
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145 274 V
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67 12 V
59 -28 V
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48 -33 V
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hep-th0203151.extracted_bib
\begin{thebibliography}{50}

\bibitem{Sny}
H.S. Snyder, \emph{Quantized space-time}, \pr{71}{1947}{38}.

\bibitem{Con}
A. Connes and M. Rieffel, \emph{Yang-Mills for noncommutative two-tori},
\emph{Contempt.\ Math.\ Oper.\ Algebra Math.\ Phys.} {\bf 62} (1987) 237;\\
A. Connes, \emph{Noncommutative geometry}, Academic Press, San Diego 1994.

\bibitem{CDS}
A. Connes, M.R. Douglas and A. Schwarz, \emph{Noncommutative geometry
and Matrix theory: compactification on tori}, \jhep{02}{1998}{003}
[\hepth{9711162}];\\
R.~Kallosh, \emph{Bound states of branes with minimal energy},
\prd{55}{1997}{3241} [\hepth{9611162}].

\bibitem{DH}
M.R. Douglas and C.M. Hull, \emph{D-branes and the noncommutative
  torus}, \jhep{02}{1998}{008} [\hepth{9711165}].

\bibitem{SW}
N.~Seiberg and E.~Witten, \emph{String theory and noncommutative
  geometry}, \jhep{09}{1999}{032} [\hepth{9908142}].

\bibitem{QHall}
S.M. Girvin, A.H. MacDonald and P.M. Platzman,
\emph{Magneto-roton theory of collective excitations in the fractional 
quantum Hall effect}, \prb{33}{1986}{2481};\\
J. Bellissard, A. van Elst and H. Schulz-Baldes,
\emph{The non-commutative geometry of the quantum Hall effect},
\condmat{9411052};\\
S. Girvin, \emph{The quantum Hall effect: novel excitations and
broken symmetries}, in \emph{Proceedings of
Ecole d'Et\'{e}}, Les Houches 1998 [\condmat{9907002}].

\bibitem{DN}
M.R. Douglas and N.A. Nekrasov, \emph{Noncommutative field theory},
\rmp{73}{2001}{977} [\hepth{0106048}];\\
R.J. Szabo, \emph{Quantum field theory on noncommutative spaces},
  \hepth{0109162}.

\bibitem{Filk}
T.~Filk, \emph{Divergencies in a field theory on quantum space},
\plb{376}{1996}{53}.

\bibitem{Min}
S.~Minwalla, M.~Van~Raamsdonk and N.~Seiberg, \emph{Noncommutative
  perturbative dynamics}, \jhep{02}{2000}{020} [\hepth{9912072}].

\bibitem{Che}
I.~Chepelev and R.~Roiban, \emph{Renormalization of quantum field
  theories on noncommutative $R^d$, 1. Scalars}, \jhep{05}{2000}{037}
  [\hepth{9911098}].

\bibitem{RG}
L.~Griguolo and M.~Pietroni, \emph{Hard non-commutative loops
  resummation}, \prl{88}{2002}{071601} [\hepth{0102070}];\\
\emph{Wilsonian renormalization group and the non-commutative IR/UV
  connection}, \jhep{05}{2001}{032} [\hepth{0104217}];\\
S.~Sarkar, \emph{On the UV renormalizability of noncommutative field
  theories}, \jhep{06}{2002}{003} [\hepth{0202171}].

\bibitem{GGRS}
H.O. Girotti, M.~Gomes, V.O. Rivelles and A.J. da~Silva, \emph{A
  consistent noncommutative field theory: the Wess-Zumino model},
  \npb{587}{2000}{299} [\hepth{0005272}];\\
H.O. Girotti, M.~Gomes, A.Y. Petrov, V.O. Rivelles and A.J. da~Silva,
  \emph{The three-dimensional noncommutative nonlinear sigma model in
  superspace}, \plb{521}{2001}{119} [\hepth{0109222}].

\bibitem{GS}
S.S. Gubser and S.L. Sondhi, \emph{Phase structure of non-commutative
  scalar field theories}, \npb{605}{2001}{395} [\hepth{0006119}].

\bibitem{NCQED}
R.~Wulkenhaar, \emph{Non-renormalizability of theta-expanded
  noncommutative QED}, \jhep{03}{2002}{024} [\hepth{0112248}].

\bibitem{SP}
S. Profumo, \emph{Noncommutative principle chiral modes},
\hepth{0111285}.

\bibitem{Mafia}
L.~Griguolo, D.~Seminara and P.~Valtancoli, \emph{Towards the solution
  of noncommutative $YM_2$: Morita equivalence and large-$N$-limit},
  \jhep{12}{2001}{024} [\hepth{0110293}];\\
A.~Bassetto, G.~Nardelli and A.~Torrielli, \emph{Perturbative Wilson
  loop in two-dimensional non-commutative Yang-Mills theory},
  \npb{617}{2001}{308} [\hepth{0107147}];
\emph{Scaling properties of the perturbative Wilson loop in
two-dimensional non-commutative Yang-Mills theory}, \hepth{0205210};\\
L.D. Paniak and R.J. Szabo, \emph{Instanton expansion of
  noncommutative gauge theory in two dimensions}, \hepth{0203166}.

\bibitem{GAO}
A. Gonz\'{a}lez-Arroyo and M. Okawa, \emph{A twisted
model for large-$N$ lattice gauge theory}, \plb{120}{1983}{174};
\emph{The twisted Eguchi-Kawai model: a reduced model for
large-$N$ lattice gauge theory}, \prd{27}{1983}{2397}.

\bibitem{AIIKKT}
H.~Aoki, N. Ishibashi, S. Iso, H. Kawai, Y. Kitazawa and T. Tada,
\emph{Noncommutative Yang-Mills in IIB matrix model},
\npb{565}{2000}{176} [\hepth{9908141}].

\bibitem{AMNS}
J.~Ambj{\o}rn, Y.M. Makeenko, J.~Nishimura and R.J. Szabo,
  \emph{Finite N matrix models of noncommutative gauge theory},
  \jhep{11}{1999}{029} [\hepth{9911041}];
\emph{Nonperturbative dynamics of noncommutative gauge theory},
  \plb{480}{2000}{399} [\hepth{0002158}];\\
\emph{Lattice gauge fields and discrete noncommutative Yang-Mills
  theory}, \jhep{05}{2000}{023} [\hepth{0004147}].

\bibitem{EK}
T.~Eguchi and H.~Kawai, \emph{Reduction of dynamical degrees of
  freedom in the large-$N$ gauge theory}, \prl{48}{1982}{1063}.

\bibitem{BHN}
G.~Bhanot, U.M. Heller and H.~Neuberger, \emph{The quenched
  Eguchi-Kawai model}, \plb{113}{1982}{47};\\
U.M. Heller and H.~Neuberger, \emph{The role of gauge theories in
  constructing reduced models at infinite N}, \npb{207}{1982}{399}.

\bibitem{ABN}
K.N. Anagnostopoulos, W.~Bietenholz and J.~Nishimura, \emph{The area
  law in matrix models for large-$N$ QCD strings},
  \ijmpc{13}{2002}{555}  [\heplat{0112035}].

\bibitem{GA-KA}
A. Gonz\'{a}lez-Arroyo and C.P. Korthals Altes, \emph{Reduced model
for large-$N$ continuum field theories}, \plb{131}{1983}{2397}.

\bibitem{Fab1}
K.~Fabricius, O.~Haan and T.~Filk, \emph{Generalized twisted
  Eguchi-Kawai models}, \plb{144}{1984}{240}.

\bibitem{Fab2}
K.~Fabricius and O.~Haan, \emph{Numerical analysis of the twisted
  Eguchi-Kawai model in four-dimensions}, \plb{139}{1984}{293}.

\bibitem{JN}
J.~Nishimura, \emph{On existence of nontrivial fixed points in
  large-$N$ gauge theory in more than four dimensions},
  \mpla{11}{1996}{3049} [\heplat{9608119}].

\bibitem{GW}
D.J. Gross and E.~Witten, \emph{Possible third order phase transition
  in the large-$N$ lattice gauge theory}, \prd{21}{1980}{446}.

\bibitem{Fab3}
K.~Fabricius and O.~Haan, \emph{Numerical analysis of the twisted
  Eguchi-Kawai model in two-dimensions}, \plb{131}{1983}{399}.

\bibitem{NN}
T.~Nakajima and J.~Nishimura, \emph{Numerical study of the double
  scaling limit in two-dimensional large-$N$ reduced model},
  \npb{528}{1998}{355} [\hepth{9802082}].

\bibitem{ProfVic}
S.~Profumo and E.~Vicari, \emph{Twisted Eguchi-Kawai reduced chiral
  models}, \jhep{05}{2002}{014} [\hepth{0203155}].

\bibitem{Schwarz98}
A.~Schwarz, \emph{Morita equivalence and duality},
\npb{534}{1998}{720} [\hepth{9805034}].

\bibitem{IIKK}
N.~Ishibashi, S.~Iso, H.~Kawai and Y.~Kitazawa, \emph{Wilson loops in
  noncommutative Yang-Mills}, \npb{573}{2000}{573} [\hepth{9910004}].

\bibitem{HI}
A.~Hashimoto and N.~Itzhaki, \emph{On the hierarchy between
  non-commutative and ordinary supersymmetric Yang-Mills},
  \jhep{12}{1999}{007} [\hepth{9911057}].

\bibitem{Bars}
I.~Bars and D.~Minic, \emph{Non-commutative geometry on a discrete
  periodic lattice and gauge theory}, \prd{62}{2000}{105018}
  [\hepth{9910091}].

\bibitem{NCloops}
L.~Alvarez-Gaum\'e and S.R. Wadia, \emph{Gauge theory on a quantum
  phase space}, \plb{501}{2001}{319} [\hepth{0006219}];\\
S.R. Das and S.-J. Rey, \emph{Open Wilson lines in noncommutative
  gauge theory and tomography of holographic dual supergravity},
  \npb{590}{2000}{453} [\hepth{0008042}];\\
D.J. Gross, A.~Hashimoto and N.~Itzhaki, \emph{Observables of
  non-commutative gauge theories}, \atmp{4}{2000}{893}
  [\hepth{0008075}];\\
A.~Dhar and Y.~Kitazawa, \emph{Loop equation and Wilson line
  correlators in non-commutative gauge theories},
  \npb{613}{2001}{105} [\hepth{0104021}].

\bibitem{Nishimura:2001dq}
J.~Nishimura and M.A. V\'azquez-Mozo, \emph{Noncommutative chiral gauge
  theories on the lattice with manifest star-gauge invariance},
  \jhep{08}{2001}{033} [\hepth{0107110}].

\bibitem{Fab4}
K.~Fabricius and O.~Haan, \emph{Heat bath method for the twisted
  Eguchi-Kawai model}, \plb{143}{1984}{459}.

\bibitem{CM}
N. Cabbibo and E. Marinari, \emph{A new method for updating 
${\rm SU}(N)$ matrices in computer simulations of gauge theories},
\plb{119}{1982}{387}.

\bibitem{4dSUSY}
J.~Ambj{\o}rn, K.N. Anagnostopoulos, W.~Bietenholz, T.~Hotta and
  J.~Nishimura, \emph{Large-$N$ dynamics of dimensionally reduced 4d
  ${\rm SU}(N)$ super Yang-Mills theory}, \jhep{07}{2000}{013}
  [\hepth{0003208}].

\bibitem{prep}
W. Bietenholz, F. Hofheinz and J. Nishimura, in preparation.

\end{thebibliography}