%Paper: 
%From: HAIM@amy.phys.vt.edu
%Date: 11 Feb 93 14:25:00 EST

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% Instructions for Figures:
% The 3 figures are attached at the bottom (search for the word
% "TopDrawer". From that point on there are 3 PostScript files that contains
% the 3 figures, each starts with "PostScript file for Figure i" (i=1,2,3).
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% From here till that point it's a TEX file of the whole
% paper, assuming you have PHYZZX.TEX .
% problems? please contact HAIM@VTCC1.BITNET, HAIM@AMY.PHYS.VT.EDU
% (Internet),  47309::HAIM (Decnet); (Dan Haim, for the AMY Collaboration)
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%
%   AMY Paper on TRISTAN Energy Scan for the Ting object
%
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\input phyzzx
\def\etal{{\it et al.}}
\def\qbar{\rm {\bar q}}
\def\twog{\gamma\gamma}
\def\threeg{\gamma\gamma\gamma}
\def\ll{\ell^+\ell^-}
\def\to{\rightarrow}
\def\sigmaX{\sigma_{\lower 2pt\hbox{$\scriptstyle X$}}}
\def\sigmaE{\sigma_{\lower 2pt\hbox{$\scriptstyle E$}}}
\def\Gee{\Gamma_{\rm ee}}
\def\Ggg{\Gamma_{\twog}}
\def\BRgg{{\rm BR}_{\twog}}
\def\keV{\,{\rm keV}}
\def\MeV{\,{\rm MeV}}
\def\GeV{\,{\rm GeV}}
\def\roots{\sqrt{s}}
\def\chsq{\chi^2}
\def\eeeex{\rm {ee\rightarrow eeX}}
\def\egex{\rm {e\gamma ^*\rightarrow eX}}
\def\lms{\Lambda_{\overline{MS}}}
\def\Qbar{\rm {\bar Q}}
\def\ee{{\rm e^+e^-}}
\def\eQ{\rm e_Q}
\def\eq{\rm e_q}
\def\qq{\rm overline{q}}
\def\Z0{\rm Z^{\circ}}
\def\mm{\rm \mu ^+\mu ^-}
\def\mumu{\rm \mu ^+\mu ^-}
\def\smm{\sigma _{\mu\mu}}
\def\tata{\tau ^+\tau ^-}
\def\MSB{\rm \overline{MS}}
\def\alphas{\rm {\alpha_s}}
\def\betaq{\rm {\beta_q}}
\def\rt{\rightarrow}
%\voffset=-1cm
\hsize=6in
%\vsize=8.9in
\hsize=6.0in
%
%   References for "Ting Resonance" paper
%%%% KG %%%%
\REF{\rfLTHREE}{O.~Adriani \etal\  (L3 Collaboration), Phys.~Lett.~{\bf 295B}
(1992) 337.}
%
\REF{\rfLEP}{S.~Komamiya, K.W.~Bell and S.~Holmgven, private communications.}
%%%%CERN, Dec.~1992.}
%
\REF{\rfTRIUMF}{R.~Garisto and J.N.~Ng, Preprint TRI-PP-92-124, 16
Dec.~1992.}
%
\REF{\rfKEK}{K.~Hagiwara and S.~Matsumoto, private communications.}
%%%%{To appear in a KEK Report.}
%
\REF{\rfVENUS}{K.~Abe \etal, Z.~Phys.~C {\bf 45} (1989) 175.}
%
\REF{\rfTOPAZ}{K.~Shimozawa \etal, Phys.~Lett.~{\bf B284} (1992) 144.}
%
\REF{\rfAMY}{AMY Collaboration, T.~Kumita \etal, Phys.~Rev.~D24 (1990) 1339.}
%
\REF{\rfSHC}{A.~Abashian \etal, to be published in Nucl.~Instr.~and Meth.~A.}
%
\REF{\rfFUIG}{J.~Fujimoto and M.~Igarashi, Prog.~Theor.~Phys.~{\bf 74} (1985)
791.}
%
\REF{\rfFUIGSH}{J.~Fujimoto, M.~Igarashi, Y.~Shimizu, Prog.~Theor.~Phys.
 ~{\bf 77} (1987) 118.}
%
\REF{\rfSKAW}{S.~Kawabata, Comp.~Phys.~Comm.~{\bf 41} (1986) 127.}
%
\REF{\rfJACKSON}{J.D.~Jackson and D.L.~Scharre, Nucl.~Instr.~and
 Meth.~{\bf 128} (1975) 13.}
%
\REF{\rfHELENE}{O.~Helene, Nucl.~Instr.~and Meth.~{\bf 212} (1983) 319.}
%
\REF{\rfKURIHARA}{Y.~Kurihara (unpublished).}
%
\REF{\rfGRACE}{H.~Tanaka, Comp.~Phys.~Comm.~{\bf 58} (1990) 153, H.~Tanaka,
T.~Kaneko, and Y.~Shimizu, Comp.~Phys.~Comm.~{\bf 64} (1991) 149, T.~Kaneko,
in ``New Computing Techniques in Physics Research,'' ed.~Perret-Gallix
and W.~Wojcik, (Edition du CRNS, Paris: 1990) 555.}
%
\REF{\rfOPAL}{M.Z.~Akrawy \etal\ (OPAL Collaboration), Phys.~Lett.~{\bf 257B}
 (1991) 531.}
%
\REF{\rfAGUIL}{F.~del \'Aguila, A.~M\'endez and R.~Pascual,
 Phys.~Lett.~{\bf 140B} (1984) 431.}
%
\REF{\rfKINOSH}{T.~Kinoshita and W.B.~Linquist, Phys.~Rev.~Lett.~{\bf 47}
 (1981) 1573.}
%
% \REF{\rfPIEE}{L.~Bergstr\"om, E.~Mass\'o, L.~Ametller and A.~Bramon,
% Phys.~Lett.~{\bf 126B},  (1983) 117.}
%\input references
\vskip 0.2in
\centerline{\bf Search for Anomalous $\twog$ Production at TRISTAN}
\vskip 0.2in
% 07-JAN_1993,K.Gotow; Updated for the Ting resonance paper from
% Master Author list of the AMY Collaboration; November 1, 1989
% Further updating,15-Jan-1993,to include U. of Hawaii, SSC
% and correct the ordering of the institution names.
%
% Further updating, 9-Feb-1993 to remove OSU, Kass, and Kagan
%
%Rule: Institutions in alphabetical order of their city except
%      for 1st author, whose institution is listed 1st.
%
\singlespace \twelvepoint
\newbox\smallstrutbox
\setbox\smallstrutbox=\hbox{\vrule height10.5pt depth3.5pt width0pt}
\def\smallstrut{\relax\ifmmode\copy\smallstrutbox\else\unhcopy
  \smallstrutbox\fi}
{\tenrm\offinterlineskip}
\singlespace \tenpoint
\centerline{\bf The AMY Collaboration}
\tolerance=10000
%%%%%%%%%%%%%%%%%%%%%%%%%%
\def\vpi{a}	%Blacksburg
\def\lsu{b}	%Baton Rouge
\def\beij{c}	%Beijing
\def\usc{d}	%Columbia
%\def\osu{e}	%Columbus    <-- Dropped 9-Feb-1993 SLO
\def\ssc{e}     %Dallas
\def\ucd{f}	%Davis
\def\uh{g}      %Hawaii
\def\kek{h}	%Ibaraki
%\def\utsuk{i}	%Ibaraki
\def\konan{i}	%Kobe
\def\mines{j}	%Mineapolis
\def\niig{k}	%Niigata
\def\niden{l}	%Niigata
\def\rutg{m}	%Piscataway
%\def\phil{o}	%Quezon City
\def\ur{n}	%Rochester
\def\saga{o}	%Saga
\def\kore{p}	%Seoul
\def\seoul{q}	%Seoul
\def\knu{r}	%Taegu
\def\chuo{s}	%Tokyo
%%%%%%%%%%%%%%%%%%%%%%%%%% sept 10 1990 %%%%%%%%%%%%%%
%%%%\def\tit{s}	%Tokyo
\def\sait{t}	%Urawa
%
\noindent
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%
K.L.~Sterner,\attach{\rm \vpi}
%A.Z.~Lai,\attach{\rm \vpi} <-- Should he be in ? KG
A.~Abashian,\attach{\rm \vpi}
K.~Gotow,\attach{\rm \vpi}
D.~Haim,\attach{\rm \vpi}
%K.P.~Hu,\attach{\rm \vpi}  <-- KG
%E.H.~Low,\attach{\rm \vpi}<-- KG
M.E.~Mattson,\attach{\rm \vpi}
N.~Morgan,\attach{\rm \vpi}
%F.~Naito,\attach{\rm \vpi} <--removed 7/12/89 K.Gotow
L.~Piilonen,\attach{\rm \vpi}
%
%R.~Imlay,\attach{\rm \lsu} <- proposed to drop Imlay 9/11/90
P.~Kirk,\attach{\rm \lsu}
%J.~Lim,\attach{\rm \lsu}   <- dropped (Abe 27-jan-93)
%W.~Marterer,\attach{\rm \lsu}
%R.R.~McNeil,\attach{\rm \lsu} <_ dropped (Abe 27-jan-93)
%W.~Metcalf,\attach{\rm \lsu} <- removed by SLO 2/7/91
%S.S.~Myung,\attach{\rm \lsu} <- dropped (Abe 27-jan-93)
%
C.P.~Cheng,\attach{\rm \beij}
W.X.~Gao,\attach{\rm \beij}
%P.~Gu,\attach{\rm \beij}   <- dropped (Abe 27-jan-93)
%J.~Li,\attach{\rm \beij}   <---Propose to remove SLO 9/11/90
%Z.P.~Mao,\attach{\rm \beij} <---removed 10/27/89 M. Ye
%Y.~Yan,\attach{\rm \beij}
W.G~Yan,\attach{\rm \beij}
%Y.T.~Xu,\attach{\rm \beij}  <-- removed 10/27/89 M. Ye
M.H.~Ye,\attach{\rm \beij}
%H.S.~Zhou,\attach{\rm \beij}
%Y.C.~Zhu,\attach{\rm \beij} <--- Propose to remove Nozaki 1/14/91
%
%F.~Avignone,\attach{\rm \usc}
%R.~Childers,\attach{\rm \usc}
%C.~Darden,\attach{\rm \usc}
%Y.K.~Li,\attach{\rm \usc}
S.~Lusin,\attach{\rm \usc}
C.~Rosenfeld,\attach{\rm \usc}
A.T.M.~Wang,\attach{\rm \usc}
S.~Wilson,\attach{\rm \usc}
L.Y.~Zheng,\attach{\rm \usc}
%
%D.~Johnson,\attach{\rm \osu}
%M.~Frautschi,\attach{\rm \osu} <- dropped (Abe 27-jan-93)
%H.~Kagan,\attach{\rm \osu}    <-- Dropped 9-Feb-1993 SLO
%R.~Kass,\attach{\rm \osu}    <-- Dropped 9-Feb-1993 SLO
%C.G.~Trahern,\attach{\rm \osu}  <---Propose to remove SLO 9/11/90
%
C.A.~Fry,\attach{\rm \ssc}
R.~Tanaka,\attach{\rm \ssc}      % moved from Chuo (LEP 04-feb-93)
%
R.E.~Breedon,\attach{\rm \ucd ,\kek}
L.M.~Chinitz,\attach{\rm \ucd}
%H.Y.~Lee,\attach{\rm \ucd}
%G.N.~Kim,\attach{\rm \ucd ,\kek}  <--- Propose to remove Nozaki 1/14/91
Winston~Ko,\attach{\rm \ucd}
R.L.~Lander,\attach{\rm \ucd}
%K.~Maeshima,\attach{\rm \ucd} <- dropped (Abe 27-jan-93)
%R.L.~Malchow,\attach{\rm \ucd} <- dropped (Abe 27-jan-93)
J.~Rowe,\attach{\rm \ucd}
%D.~Saroff,\attach{\rm \ucd}
J.R.~Smith,\attach{\rm \ucd}
%K.~Sparks,\attach{\rm \ucd} <-- removed 7/13/89 K.Sparks (via Thorndike)
D.~Stuart,\attach{\rm \ucd}
%M.C.S.~Williams,\attach{\rm \ucd} <--removed 10/27/89 as per W. Ko
%
S.~Kanda,\attach{\rm \uh}
S.L.~Olsen,\attach{\rm \uh}
K.~Ueno,\attach{\rm \uh}
%
K.~Abe,\attach{\rm \kek}
%S.~Chakrabarti,\attach{\rm \kek}
Y.~Fujii,\attach{\rm \kek}
%Y.~Higashi,\attach{\rm \kek}    <--- removed (LEP 04-feb-93)
%S.~Ishimoto,\attach{\rm \kek}
%S.K.~Kim,\attach{\rm \kek} <---  moved to Rutgers 3/19/91 S.Schnetzer
Y.~Kurihara,\attach{\rm \kek}
F.~Liu,\attach{\rm \kek}
A.~Maki,\attach{\rm \kek}
%P.~Mani,\attach{\rm \kek}
T.~Nozaki, \attach{\rm \kek}
T.~Omori,\attach{\rm \kek}
%P.~Perez,\attach{\rm \kek}
H.~Sagawa,\attach{\rm \kek}
Y.~Sakai,\attach{\rm \kek}
T.~Sasaki,\attach{\rm \kek}
Y.~Sugimoto,\attach{\rm \kek}
Y.~Takaiwa,\attach{\rm \kek}
S.~Terada,\attach{\rm \kek}
%K.~Tsuchiya,\attach{\rm \kek}<--removed 7/12/89 K.Abe
R.~Walker,\attach{\rm \kek ,\ur}
%
F.~Kajino,\attach{\rm \konan}
%
%D.~Perticone,\attach{\rm \mines}   <---Propose to remove SLO 9/11/90
R.~Poling,\attach{\rm \mines}
T.~Thomas,\attach{\rm \mines}
%
T.~Aso,\attach{\rm \niig}
%Y.~Ishi,\attach{\rm \niig}     <--- removed (LEP 04-feb-93)
%M.~Ishizuka,\attach{\rm \niig}  <--- removed (LEP 04-feb-93)
K.~Miyano,\attach{\rm \niig}
H.~Miyata,\attach{\rm \niig}
%M.~Ogawa,\attach{\rm \niig}<--propose to drop  SLO 7/12/89
M.~Oyoshi,\attach{\rm \niig}
%
%A.~Aldritch,\attach{\rm \rutg}
%S.K.~Kim,\attach{\rm \rutg} <- dropped (Abe 27-jan-93)
%A.~Bacala,\attach{\rm \rutg ,\phil} <- dropped (Abe 27-jan-93)
%J.~Green,\attach{\rm \rutg}<--removed 7/12/89 as per S.Schnetzer
M.H.~Lee,\attach{\rm \rutg}      % moved from Korea (LEP 04-feb-93)
%J.~Liu,\attach{\rm \rutg}  <---Propose to remove SLO 9/11/90
%I.H.~Park,\attach{\rm \rutg}  <---Propose to remove SLO 9/11/90
%S.~Sakamoto,\attach{\rm \rutg}<--removed 7/12/89 as per S.Schnetzer
F.~Sannes,\attach{\rm \rutg}
S.~Schnetzer,\attach{\rm \rutg}
R.~Stone,\attach{\rm \rutg}
%S.~Trentalange,\attach{\rm \rutg}<--removed 7/12/89 as per S.Schnetzer
J.~Vinson,\attach{\rm \rutg}
%D.~Zimmerman,\attach{\rm \rutg}
%
Y.~Yamashita,\attach{\rm \niden}
%
%P.~Auchincloss,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
%D.~Blanis,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
A.~Bodek,\attach{\rm \ur}
%H.~Budd,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
%R.~Coombes,\attach{\rm \ur}<--removed 7/12/89 S.Olsen
%S.~Eno,\attach{\rm \ur}    Propose to remove 1/14/91  Nozaki
%H.~Harada,\attach{\rm \ur}   <--- removed (LEP 04-feb-93)
%Y.H.~Ho,\attach{\rm \ur}   <- dropped (Abe 27-jan-93)
B.J.~Kim,\attach{\rm \ur}
%Y.K.~Kim,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
T.~Kumita,\attach{\rm \ur}
Y.K.~Li,\attach{\rm \ur}
%T.~Mori,\attach{\rm \ur}   <---Propose to remove SLO 9/11/90
%N.M.~Shaw,\attach{\rm \ur}   <---  Propose to remove Nozaki 1/14/91
%A.~Sill,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
%E.H.~Thorndike,\attach{\rm \ur} <--removed by SLO 2/7/91
C.~Velisarris,\attach{\rm \ur}
%H.W.~Zheng,\attach{\rm \ur} <- dropped (Abe 27-jan-93)
%
%H.~Asakura,\attach{\rm \saga}
%K.~Eguchi,\attach{\rm \saga}
%H.~Ichinose,\attach{\rm \saga}
%H.~Itoh,\attach{\rm \saga} <-removed 10/30/89 A.Maki/A.Murakami
S.~Kobayashi,\attach{\rm \saga}
A.~Murakami,\attach{\rm \saga}
S.K.~Sahu,\attach{\rm \saga}
%K.~Toyoshima,\attach{\rm \saga} <--removed 10/28/89 A Maki
%
Y.S.~Chung,\attach{\rm \kore}
J.S.~Kang,\attach{\rm \kore}
%H.J.~Kim,\attach{\rm \kore}   <--- Propose to remove 1/14/91  Nozkai
K.B.~Lee,\attach{\rm \kore}
%M.H.~Lee,\attach{\rm \kore}   <--- moved to Rutgers (LEP 04-feb-93)
K.W.~Park,\attach{\rm \kore}
%
S.K.~Kim,\attach{\rm \seoul}
S.S.~Myung,\attach{\rm \seoul}
%
S.K.~Choi,\attach{\rm \knu}
%D.H.~Han,\attach{\rm \knu} <- dropped (Abe 27-jan-93)
%E.J.~Kim,\attach{\rm \knu} <- dropped (Abe 27-jan-93)
D.~Son,\attach{\rm \knu}
%
S.~Ebara,\attach{\rm \chuo}
%H.~Kozuka,\attach{\rm \chuo}
S.~Matsumoto,\attach{\rm \chuo}
%H.~Otsuki,\attach{\rm \chuo}
N.~Takashimizu,\attach{\rm \chuo}
%T.~Takeda,\attach{\rm \chuo}
%R.~Tanaka,\attach{\rm \chuo}   <--- moved to SSC (LEP 04-feb-93)
%K.~Tomioka,\attach{\rm \chuo} <- dropped (Abe 27-jan-93)
%T.~Yasuda,\attach{\rm \chuo}
%Y.~Yamagishi,\attach{\rm \chuo}
%
%R.~Chiba,\attach{\rm \tit}<--removed 7/12/89 as per A.Maki
%K.~Hanaoka,\attach{\rm \tit}
%S.~Igarashi,\attach{\rm \tit}<--removed 7/12/89 as per A.Maki
%M.~Miyashita,\attach{\rm \tit}
%H.~Murata,\attach{\rm \tit}
%H.~Yokota,\attach{\rm \tit}<--removed 10/28/89 as per A.Maki
%
 and
T.~Ishizuka\attach{\rm \sait}
%T.~Maruta,\attach{\rm \sait}
%K.~Ohta\attach{\rm \sait} Propose to remove 1/14/91 Nozaki
%% FOLLOWING LINE CANNOT BE BROKEN BEFORE 80 CHAR
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Standard list of AMY  Institutions, in alphabetical order by city
% except for first institution.
%
\vskip .10in
\newbox\smallstrutbox
\setbox\smallstrutbox=\hbox{\vrule height10.5pt depth3.5pt width0pt}
\def\smallstrut{\relax\ifmmode\copy\smallstrutbox\else\unhcopy
  \smallstrutbox\fi}
{\tensl\offinterlineskip
%
\centerline{\smallstrut
\attach{\rm \vpi}Virginia Polytechnic Institute and State University,
	Blacksburg, VA 24061, USA}
%
\centerline{\smallstrut
\attach{\rm \lsu}Louisiana State University, Baton Rouge, LA 70803, USA}
%
\centerline{\smallstrut
\attach{\rm \beij}Institute of High Energy Physics, Beijing 100039, China}
%
\centerline{\smallstrut
\attach{\rm \usc}University of South Carolina, Columbia, SC 29208, USA}
%
%\centerline{\smallstrut
%\attach{\rm \osu}Ohio State University, Columbus, OH 43210, USA}
%
%\attach{\rm \ucd}Chungnam National University, Daejeon 300-31,~
%
\centerline{\smallstrut
\attach{\rm \ssc}SSC Laboratory, Dallas, TX 75237, USA}
%
\centerline{\smallstrut
\attach{\rm \ucd}University of California, Davis, CA 95616, USA}
%
\centerline{\smallstrut
\attach{\rm \uh}University of Hawaii, Honolulu, HI 96822, USA}
%
\centerline{\smallstrut
\attach{\rm \kek}KEK, National Laboratory for High Energy Physics,
 Ibaraki 305, Japan}
%
%\centerline{\smallstrut
%\attach{\rm \utsuk}Tsukuba University, Ibaraki 305}
%
%\centerline{\smallstrut
%\attach{\rm \utsuk}Tsukuba University, Ibaraki 305,~~~
\centerline{\smallstrut
\attach{\rm \konan}Konan University, Kobe 658, Japan}
%
\centerline{\smallstrut
\attach{\rm \mines}University of Minnesota, Minneapolis, MN 55455, USA}
%
\centerline{\smallstrut
\attach{\rm \niig}Niigata University, Niigata 950-21, Japan}
%
\centerline{\smallstrut
\attach{\rm \niden}Nihon Dental College, Niigata 951, Japan}
%
\centerline{\smallstrut
\attach{\rm \rutg}Rutgers University, Piscataway, NJ 08854, USA}
%
%\centerline{\smallstrut
%\attach{\rm \phil}University of the Philippines, Quezon City, 3004,
%Philippines}
%
\centerline{\smallstrut
\attach{\rm \ur}University of Rochester, Rochester, NY 14627, USA}
%
\centerline{\smallstrut
\attach{\rm \saga}Saga University, Saga 840, Japan}
%
\centerline{\smallstrut
\attach{\rm \kore}Korea University, Seoul 136-701, South Korea}
%
\centerline{\smallstrut
\attach{\rm \seoul}Seoul National University, Seoul 151-742, South Korea}
%
\centerline{\smallstrut
\attach{\rm \knu}Kyungpook National University, Taegu 702-701,
South Korea}
%
\centerline{\smallstrut
\attach{\rm \chuo}Chuo University, Tokyo 112, Japan}
%\smallstrut
%\attach{\rm \tit}Tokyo Institute of Technology, Tokyo 152
%
\centerline{\smallstrut
\attach{\rm \sait}Saitama University, Urawa 338, Japan}
%
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
%\input author
\Twelvepoint
\endpage
\centerline{\bf Abstract}
\singlespace

\noindent
We report on measurements of the total cross section for $\ee \to \twog$
for center-of-mass energies between 57.4 and 59.5 GeV, using the AMY
detector at the TRISTAN collider.  We set new limits on the production of
a possible new $s$-channel resonance decaying into photon pairs.
%
\vskip 1.0in
\rm
\doublespace
\Twelvepoint

\chapter{\bf Introduction}

Recently, the L3 Collaboration at LEP reported on an apparent excess of
$\ee \to \ll\twog$ events ($\ell = \mu\ {\rm or}\ e$) in which the invariant
mass of the photon pair was clustered around $59\GeV$.\refmark{\rfLTHREE}
The L3 Collaboration
did not speculate on the origin of their events beyond noting that the
probability of observing such clustering in any $5\GeV$ wide mass
bin above $40\GeV$ was ${\cal O}(10^{-3})$, if the events were due purely
to QED\null. The three other experiments at LEP have also reported on such
events.\refmark{\rfLEP} Out of fifteen $\ee \to \ll\twog$ events found at LEP
with $M_{\twog} > 40\GeV$, five
events were found with a $\twog$ invariant mass in a 1 GeV range near
59 GeV\null.

A few speculative models have been advanced\refmark{\rfTRIUMF,\rfKEK} on
the origin of the clustered events of L3 assuming that they are not due to
QED\null.  The models are based on the decay of the $Z^{\circ}$ into a massive
object $X$ and another boson, where $X$ may be a scalar-pseudoscalar mixture
or a spin-2 particle with a mass of approximately $60\GeV$ that
decays predominantly into two photons.  Regardless of the details of such
models, if the particle $X$ can couple with electrons, then the direct
$s$-channel production may be observable in the TRISTAN energy range.
If there is no coupling of $X$ to fermions, it can still be produced via
an $s$-channel photon that results in $X \to \twog$ plus a soft monochromatic
photon. Previous studies of $\ee \to \twog,\threeg$ at
TRISTAN\refmark{\rfVENUS,\rfTOPAZ} were consistent with the QED prediction,
however, no direct search for a narrow resonance was conducted.

%% LEO -- I added that last sentence 1/29/93 a KG's request.
%%        Move it or improve it as you will.  -- KLS

We have searched for the direct production of a new state $X$ via the
reaction $\ee \to X \to \twog$,
% and $\ee \to X\gamma \to \threeg$,
using the
AMY detector at the TRISTAN $\ee$ collider, for center-of-mass energies
$\sqrt{s}$ between 57.4 and 59.5 GeV in
250 MeV steps, with 1 to 2 $\rm pb^{-1}$ of integrated luminosity per point
(19 $\rm pb^{-1}$ at 57.8 GeV)\null.

\chapter{\bf The AMY Detector}

The AMY detector is a general purpose solenoidal-type instrument employing
two inner tracking chambers (VTX and ITC), a central drift chamber (CDC),
and an electromagnetic calorimeter (SHC), all contained within a 3 Tesla
magnetic field, and a barrel muon detector (MUO) outside the magnet return
yoke.  The end cap regions are instrumented with calorimeters (ESC) and
small-angle luminosity monitors (SAC)\null.  The AMY detector has been
described in detail elsewhere.\refmark{\rfAMY}

Final states with two or more photons are detected primarily by the
SHC\null.
This is a 14.4 radiation length gas-sampling calorimeter, consisting of
twenty alternating layers of lead and resistive plastic proportional
tubes.\refmark{\rfSHC}  Each tube layer is sandwiched between
%pickup
cathode strips in the $\phi$ and $\theta$ directions.
The SHC is constructed in six sextants, each covering
an azimuthal range of $60^{\circ}$ and a polar angle range of
$|\cos\theta| < 0.73$.
%%%%$45^{\circ} < \theta < 135^{\circ}$.
%It is operated with a 50\% argon--50\% ethane gas mixture at a voltage of
%2100 V\null.

Measurement of electromagnetic shower locations and energies in the SHC is
determined by the signals from the cathode strips.  The strips are arranged
in projective towers that subtend an angle of 14.2 mr from the interaction
point, and are ganged internally into five longitudinal divisions.
%Signals from the ganged strips are sent to LeCroy Fastbus 1885 ADC units that
%measure the induced charge.
%Corrections for gain drifts due to changes in pressure
%and gas composition are made using monitor tubes (fitted with radioactive
%sources) mounted within each sextant.  Energy calibration is done using
%Bhabha events and QED events with final-state low-energy electrons.
The empirical energy resolution is found to be $\Delta E/E = 0.23 / \sqrt{E} +
0.06$, with $E$ in GeV\null.  The large constant term is thought to be
due to the
effects of operating in the 3 T magnetic field.  Shower centroids are typically
located in $\phi$ and $\theta$ to less than one strip width.

\noindent\underbar{Triggering}

Within a given layer of the SHC, anode signals are ganged into 48 azimuthal
sections; the ganged signals are summed externally over multiple layers to
form trigger signals for 48 towers with either no segmentation or four
longitudinal divisions.  Three redundant combinations of these
signals provide triggering for $\ee \to \twog$ events:  (1) total
energy trigger---the analog sum of all 48 trigger signals exceeding 8 GeV,
(2) two-cluster trigger---two separate towers in coincidence with energies
exceeding 5 GeV for one and 3 GeV for the other, and (3) shower shape
trigger---coincidence between any two successive longitudinal divisions in
a given tower, or in neighboring towers, with total energy exceeding
3 GeV\null.

%%  Clause for trigger (3) modified for clarity 1/29/93 by KLS


Bhabha electrons are used to check the triggering efficiency independently,
since they behave similarly to $\twog$ events in the SHC\null.  Bhabha events
are triggered
% additionally by
independently by the SHC triggers and by charged-track triggers derived from
signals in the CDC and ITC\null.  By examining the frequency of Bhabha
events with a track trigger but no SHC trigger, we found the SHC trigger
efficiency for Bhabha events to be essentially 100\%.  We assume,
therefore, that the SHC triggering efficiency for $\twog$ events exceeded
99\% for all of the data of this study.

\noindent\underbar{Luminosity} \underbar{Determination}

To search for an anomaly in the production of $\twog$ events, the most critical
parameter aside from event statistics is the reliable determination of the
integrated luminosity.  This is accomplished in the AMY experiment by recording
small-angle Bhabha events in the
ESC, a sampling calorimeter constructed of alternating layers of lead and
scintillator, with proportional tubes at the depth of electromagnetic shower
maximum for position determination.  The ESC covers the polar angle range
$0.799 < |\cos\theta| < 0.982$.
%%%%% KG 1/15/93
The systematic error in ESC luminosity is estimated to be $\sim 2$\%, and is
dominated by the precision on alignment and fiducial definition.

\chapter{\bf Event Selection and Monte Carlo}

The selection of $\ee \to n\gamma$ events $(n \ge 2)$ was
performed according to the following criteria:
(1) at least two SHC clusters with energies greater than $E_{beam}/3$ each,
(2) the polar angle for each such cluster in the range $45^{\circ} < \theta <
135^{\circ}$,
(3) the acollinearity angle between the two most energetic clusters of
at most $10^{\circ}$, and
(4) no charged tracks in the event.
The resulting sample of 1054 events was visually scanned, resulting in the
rejection of 19 background events from cosmic
rays, misidentified Bhabhas, and SHC noise.

The cross section for $\ee \to \twog$,
including radiative corrections to ${\cal O}(\alpha^3)$,
was calculated by Monte Carlo integration using a program by
Fujimoto, Igarashi, and Shimizu.\refmark{\rfFUIG,\rfFUIGSH}
This program is an implementation of the
BASES/SPRING Monte Carlo package by Kawabata.\refmark{\rfSKAW}
The cross section of $(34.81 \pm 0.18)\,\rm pb$ is
based on a fully simulated sample of $1.06\,\rm fb^{-1}$ at 58 GeV that was
subjected to the same selection criteria as the experimental data. This
value includes an event selection efficiency of
$\varepsilon_{\twog} = 0.933 \pm 0.011$.

We estimate the error in normalization for this analysis to be 2.3\%, taking
into account the uncertainty in the luminosity measurement and including
the error in the $\twog$ event selection efficiency.

\chapter{\bf Results}
%%%% KG 10am 01-14-93, Mod. 01-15-93
Table~1 summarizes the results of the energy scan. The center-of-mass energies
$\sqrt{s}$
represent their actual values at the AMY interaction point rather than the
nominal accelerator energies. The quantity $\sigmaE$ represents the rms width
of the center-of-mass energy distribution.
The luminosities $L$ are those obtained with the ESC\null.
The quantity $N_{\twog}$ [$N_{QED}$] represents the number of observed
[simulated] $n\gamma$ $(n \ge 2)$ events that pass the event selection
criteria; $N_{QED}$ is
derived from the Monte Carlo simulation at 58 GeV discussed earlier, scaled by
$s$ and adjusted to the tabulated luminosity.
The ratio of the observed $\twog$ events to that expected from the Standard
Model is also shown for each center-of-mass energy.

Barrel Bhabha events obtained concurrently with $\twog$ events are used to
test the internal consistency of the runs and to provide an additional
check for systematic errors. For each center-of-mass energy, the ratio of
observed barrel Bhabha events to ESC luminosity is scaled by $s$.  These
quantities are given in the last column of Table~1, and indicate the
constancy in the operation of the SHC during the scan runs.

\chapter{\bf Analysis}

The ratio of observed $n\gamma$ events $(n \ge 2)$ to the QED expectation
is plotted as a function of center-of-mass
energy in Figure~1.  The vertical error bars on the ratios are statistical
only; the horizontal error bars indicate the rms spread in $\sqrt{s}$ rather
than the error on the central values.  A comparison of the data to QED alone,
allowing the normalization to float without constraint, gives a fully
consistent fit with
$\chi^2 / {\rm dof} = 0.68$ for 8 degrees of freedom and a normalization
value of $0.961 \pm 0.029$.  This fit is shown as the solid curve in Figure~1.
% If we constrain the normalization $(1 + \alpha)$ by adding a term of the form
% $\alpha^2/\sigma_alpha^2$ to the calculation of $\chi^2$, then the best fit
% gives $\chi^2 /  {\rm dof} = 0.72$ for 9 degrees of freedom with a
% normalization value of $0.972 \pm 0.024$.
The deviation of the normalization from unity is consistent, given the 2.9\%
statistical uncertainty from the fit on this parameter as well as the 2.3\%
normalization uncertainty mentioned above.
% An independent estimate of this deviation can be made
% using the large-angle Bhabha events from the $19\,\rm pb^{-1}$ data sample at
% 58 GeV.  From these data, we find a normalization of $0.964 \pm 0.014$, in
% agreement with the $\twog$ normalizations.

To examine the effect of a new state $X$, we again allow the
normalization of the $\twog$ data to float without constraint, and then
compare these data to a
model in which the $\twog$ events are produced
by an $s$-channel resonance $X$ of mass $M$ and total width $\Gamma$ that
sums incoherently with the conventional QED processes.

The effective cross section for production of $X$ at center-of-mass energy
$\sqrt{s}$,
integrated over the solid angle of the SHC, is parameterized by a Breit-Wigner
form:
$$\sigmaX(s) = (2J+1) \Gee \BRgg f(s,M,\Gamma)\,,
\eqno(1)$$
where
$$f(s,M,\Gamma) = (\Omega\varepsilon)_{\rm eff}\,
                  {\pi \over s}\,
                  {\Gamma \over (M - \sqrt{s})^2 + \Gamma^2 / 4}\,\cdot
\eqno(2)$$
$\Gee$ is the partial width for $X \to \ee$, $\BRgg \equiv
\Ggg / \Gamma$ is the branching ratio for $X \to \twog$, and
$(\Omega\varepsilon)_{\rm eff}$ is the effective acceptance for detecting
$\ee \to \twog$.  We use $(\Omega\varepsilon)_{\rm eff} =
\Omega_{\rm SHC}\cdot\varepsilon_{\twog} = 0.707 \cdot 0.933 =
0.659$.  (This must be modified somewhat if the differential
cross section is not isotropic.)  The cross section $\sigmaX$ is then convolved
with the radiatively corrected beam resolution function\refmark{\rfJACKSON}
$$G_R(s,E) = \left( {2\sigmaE \over \sqrt{s} } \right)^t
             {t \over \sqrt{2\pi}\sigmaE}
             \int_0^{\,\,\infty} x^{t-1}\,\exp\left[ -(z-x)^2/2 \right]\,dx\,,
\eqno(3)$$
where $z = (\sqrt{s} - E) / \sigmaE$,\ \ $t = 2(\alpha/\pi)[\ln(s/m_e^2) -1]$,
and $\sigmaE$ is the width of the center-of-mass energy distribution from
Table~1, to give the observed effective cross section
$$\tilde\sigmaX(s) = (2J + 1)\Gee\BRgg
                      \int_{0}^{\,\,\infty}
f(E^2,M,\Gamma)\,G_R(s,E)\,dE\,\cdot
\eqno(4)$$

The number of events expected from this process
at center-of-mass energy $\sqrt{s}$ for an integrated luminosity $L$
is given by $N_X(s) = \tilde\sigmaX(s) \cdot L$, and adds to the number
expected from QED alone, $N_{QED}(s)$, listed in Table~1.

For a normalization $A_{\circ}$, the likelihood of observing
$N_X(s_i)$ events from $s$-channel production of $X$
at center-of-mass energy $\sqrt{s_i}$ is a rescaled Poisson
distribution:\refmark{\rfHELENE}
$$\eqalign{{\cal L}(s_i) &= A_{\circ}\,
   \exp\left\{ N_{QED}(s_i) - A_{\circ}[N_X(s_i) + N_{QED}(s_i)]\right\}\cr
&\qquad {}\times \left\{{A_{\circ}[N_X(s_i) +N_{QED}(s_i)] \over N_{QED}(s_i)}
                             \right\}^{\textstyle N_{\twog}(s_i)}\cr}
\eqno(5)$$
and the overall likelihood is ${\cal L} = \prod_{i} {\cal L}(s_i)\,.$

This likelihood function peaks at $M = (58.35^{+0.24}_{-0.08})\GeV$,
$\Gamma = (16\pm 13)\MeV$ and
$(2J+1)\Gee\BRgg = (4.2^{+3.4}_{-3.1})\keV$, with a normalization of
$A_{\circ} = 0.955 \pm 0.040$.
The best-fit curve of $A_{\circ}(N_X + N_{QED}) / N_{QED}$ is shown as the
dashed curve in Figure~1.
A comparison of this curve to the data has $\chi^2 / {dof} = 0.47$
with 5 degrees of freedom. Compared to $\chi^2 / {dof} = 0.68$ with 8
degrees of freedom for QED alone, we conclude that this peak is not
statistically significant.

We extract 90\% confidence level upper limits on $(2J+1)\Gee\BRgg$, for
the normalization of 0.955 and particular choices of $M$ and $\Gamma$,
by numerical integration of the likelihood function.
\footnote{\dag} {Since the data are consistent with pure QED, the
confidence {\it interval} includes the point \hbox{$(2J+1)\Gee\BRgg=0$.}}
%it is not reasonable to
%evaluate a confidence {\it interval} that excludes $(2J+1)\Gee\BRgg = 0$.}
These limits are shown in Figure~2.  It is apparent
that the limits are insensitive to the total width $\Gamma$ when it is
comparable to or smaller than the center-of-mass energy spread $\sigmaE$\null.
Furthermore, the limits shift only slightly if the normalization is varied
from its maximum likelihood value.

% Since we do
% not have the statistical precision to place a non-zero lower bound on
% $(2J+1)\Gee\BRgg$, we are not able to place any upper limit on the total
%%width
% $\Gamma$.  On the other hand, it is clear from Figure~3 that
% the limits on $(2J+1)\Gee\BRgg$ are very insensitive to $\Gamma$
% as long as it is not much larger than $\sigmaE \sim 100\MeV$.  For the
% remainder of this section, therefore, we will arbitrarily restrict the
% discussion to cases where the total width satisfies $\Gamma < 100\MeV$.

Upper limits on $(2J+1)\Gee\BRgg$ at the 90\% confidence level range from
0.5 keV to 8 keV, for an $X$ mass between 57 and 59.6 GeV and a total width
$\Gamma$ below 100 MeV\null.  Our limits can
be compared directly with the expectation from the L3 observation of
$\ee \to \ll\twog$ under the assumption that their clustered events arose from
the production of a new state $X$\null.  For example,  if we assume
that $X$ is a
scalar that couples only to photon and lepton pairs with a total
width of $\Gamma \equiv \Ggg + 3\Gee$, then an
upper limit on $(2J+1)\Gee\BRgg$
can be converted into an exclusion region in the plane of
$\Ggg$ vs.\ $\Gee$. Our 90\% C.L. upper limit is
shown in Figure~3
%The exclusion boundary corresponds to
%the limit on $(2J+1)\Gee\BRgg$ that is found
for a scalar $X$ of mass 59 GeV\null.
%and total width $\Gamma$=10 MeV\null.
%(Similar plots are obtained for different masses.)
%In Figure~3, the expected region from the clustered
%$\ll\twog$ events of L3 are shown also.  The region
%corresponds to the 90\% C.L. limit for three observed events in L3.
%The cross section for $\ee \to X\mu^+\mu^-$ ($X \to \twog$) is
%calculated\refmark{\rfKURIHARA}
%using the automatic amplitude generator GRACE\refmark{\rfGRACE} including
%all possible diagrams.  Our limit excludes most of the expected region except
%when either $\Ggg$ or $\Gee$ is small.  However, $\Ggg > 10.6\MeV$ is
%excluded by the non-observation of an excess of $\threeg$ events with
%$M_{\twog} = 59\GeV$ by the OPAL collaboration,\refmark{\rfOPAL} while
%$\Gee > 120\MeV$ is excluded by the absence of a peak for the $\ll$ invariant
%mass near 59 GeV in the L3 $\ll\twog$ data.\refmark{\rfLTHREE}  These limits
%are also derived from cross sections calculated using the GRACE program.

Our limits may be incorporated with 90\% C.L. limits of other
experiments such as the L3 measurement\refmark{\rfLTHREE} of
$\ee\to\ll\twog$ and the OPAL measurement\refmark{\rfOPAL} of
$\ee\to\threeg$. For the former case, we calculate\refmark{\rfKURIHARA}
the cross section
using the automatic amplitude generator GRACE\refmark{\rfGRACE}
including all possible diagrams. The limits from the three events with
$M_{\twog}$ clustered near 59 GeV observed by the L3 collaboration are
shown as the dashed curve in Figure~3, while the limits imposed by the
absence of a $\ll$ invariant mass near 59 GeV are given by the
dash-dotted curve. The limits set by the non-observation of an excess
of events with $M_{\twog}=59$ GeV in the OPAL $\threeg$ measurement are
shown as the dotted curve of Figure~3. The limits of our measurement are
thereby restricted to satisfying the condition that
$\Gamma_{\twog}<10.6$ MeV and $\Gamma_{ee}<120$ MeV\null. To summarize, the
four {\it inclusion} regions overlap in the lower left of Figure~3.

For a (pseudo-)scalar that couples directly to pairs of fermions as well
as photons, the exact forms of the decay widths for $X \to \ee$ and
$X \to \twog$ are
$$\Gee = {g_{\rm ee}^{2}\over {8\pi}} M
\eqno(6)$$
and
$$\Ggg = {\alpha^{2}\over{64\pi^{3}}} {M^{3}\over F_{X}^2}
\eqno(7)$$
respectively, where $g_{\rm ee}$ is the coupling constant of $X$ to electrons,
$\alpha$ is the fine structure constant, and $F_X$ is a mass parameter
analogous to $f_{\pi}$ in $\pi^{\circ}$ decay. We use
$\alpha / (\pi F_X)$ as the coupling constant of $X$ to $\twog$.
Assuming that $\BRgg \sim 1$, we can convert the 90\% C.L. upper limit on
$\Gee\BRgg$ from our likelihood analysis into an upper limit on $g_{\rm ee}$
of $1.78\times 10^{-3}$.  We also place a 90\% C.L. lower limit
on $F_X$ of 730 MeV that comes from the OPAL upper limit on $\Gamma_{\twog}$
of 10.6 MeV.\refmark{\rfOPAL}
%%% **** Actually, the above "limit" on g_ee is the    ****
%%% **** maximum likelihood value. Fix it.             **** Fixed! (Dan)
%%% **** where did the 544 MeV limit really come from? **** From Gamma<18 MeV.
We examine the effect of these limits upon the $ee\gamma$
vertex correction value, $(g - 2)_e$, which will have an additional
contribution
from this model of the form\refmark{\rfAGUIL}
$${\cal A}_X \simeq {m_e\over F_X}{\alpha g_{\rm ee}\over 4\pi^3}
\ln {\Lambda\over M}
\eqno(8)$$
where $\Lambda$ is the ultraviolet cutoff (fixed at 1 TeV)\null.  Our limits
on $F_X$ and $g_{\rm ee}$ imply an upper bound of
${\cal A}_X < 2.0 \times 10^{-10}$,
which is within the maximum allowed
contribution\refmark{\rfKINOSH} to $(g - 2)_e$ of $2.7 \times 10^{-10}$.

%To conclude this section, we also examine the model in which $X$ does not
%couple directly to fermions. The possible detection channels at TRISTAN
%are then either through an $s$-channel resonance in which the $\ee$ fuse via
%two photons in a loop similar to $\pi^{\circ} \to \ee$, or through an
%$s$-channel photon that couples non-resonantly to $X$ to produce a
%three-photon final state with two energetic photons having
%$M_{\twog}\simeq M$ plus a third soft monochromatic photon. The latter
%process is currently under investigation.%\refmark{\rfAMYGGG}

%As in the case of $\pi^{\circ}\to\ee$,\refmark{\rfPIEE} we can get a
%new limit on $F_X$ of $15\keV$ by assuming that $B_{ee}$ is at its unitarity
%limit, $B_{ee}/B_{\twog}=2.66\times 10^{-13}$.
%There is no dependence of $B_{ee}$ on $g_{ee}$ in this case. This limit
%has a large
%uncertainty due the fact that in $\pi^{\circ}\to\ee$ we
%have almost an order of magnitude discrepancy between the unitarity limit
%and experiment\refmark{\rfPIEE} on $B_{ee}/B_{\twog}$, and this discrepancy
%may be made more severe in extrapolating
%from $m_{\pi}$ to $M$. In any case, the more strict limit on $F_X$
%that comes from $\Gamma$ indicates that the coupling of $X$ to $\ee$ has
%contributions other than the two photon loop.

%\chapter{\bf Analysis of $\threeg$ Events}
%
%Assuming the existence of a (pseudo-)scalar state $X$ with a mass
%$M = 58.35\GeV$ and a total width $\Gamma = 150\keV$ that does
%not couple to fermions,
%the only production mechanism at TRISTAN is via an $s$-channel
%photon.
%%%% **** What about gamma-gamma fusion to s-channel X? ****
%%%% **** Need to show that resonant cross section for  ****
%%%% **** e+e-  -->  gg  -->  X  -->  gg                ****
%%%% **** is not contradicted by the conclusions of     ****
%%%% **** section -- or, otherwise, that the limit on   ****
%%%% **** it from gg events is more stringent than our  ****
%%%% **** limits here --- so why include this?          ****
%The final state will then consist of two energetic photons with
%$M_{\twog}\simeq M$ plus a third soft monochromatic photon.
%
%The cross section for $\ee \to X\gamma \to \threeg$ is, in this case,
%$$\sigma_{3\gamma}(s) = ??? \cdot \Ggg
%\eqno(10)$$
%for $s > M$, where the partial width of $X \to \twog$ is given
%in Equation~(8).
%Since we observed no $\threeg$ events beyond the QED prediction at any
%center-of-mass energy between 57.4 and 59.5 GeV, we can set an upper limit
%on $\sigma_{3\gamma}$ of 2.4 fb at the 90\% confidence level, which translates
%into a 90\% C.L. lower limit on $F_X$ of $2.2\MeV$.
%This model is still consistent with the LEP $\threeg$ data.\refmark{\rfLEP}
%%%%%%% **** this last statement needs clarification ****
%In any case, this model is in contradiction
%with Technicolor, which predicts the mass parameter to be ${\cal O}(10^2\GeV)$
%for a composite (pseudo-)scalar.

\chapter{\bf Conclusion}

We have searched for resonant production of a new state $X$ in $\ee$
collisions that couples to photon pairs at center-of-mass energies between
57.4 and 59.5 GeV\null.  We find that the observed data are consistent with the
QED prediction for $\ee \to \twog$ ($\chi^2/{dof} = 0.68$ for 8 degrees of
freedom). Furthermore, we have extracted
90\% C.L. upper limits on $(2J+1)\Gee\BRgg$ of 0.5---$8.0\keV$
for the process $\ee \to X \to \twog$, should a state $X$ exist with a mass
between 57 and $59.6\GeV$\null.

\chapter{\bf Acknowledgement}

We thank the TRISTAN staff for the excellent operation of the storage
ring. In addition we acknowledge the strong support provided by the
staffs of our home institutions.  We are particularly indebted to
Professor Lay Nam Chang for fruitful discussions on the theoretical
aspects of this paper.  This work has been supported by the Japan
Ministry of Education, Science and Culture (Monbusho), the Japan Society
for the Promotion of Science, the U.S.\ Department of Energy, the U.S.
National Science Foundation, the Korean Science and Engineering
Foundation, the Ministry of Education of Korea and the Academia Sinica
of the People's Republic of China.
\vfill\endpage
\refout
\vfill\eject
\nopagenumbers
\centerline {{\bf TABLE CAPTIONS}}
\vskip 0.5 cm

\noindent{\bf Table 1.}  Results of the energy scan. $\sqrt{s}$ is the
center-of-mass energy, $\sigmaE$ is the width of the center-of-mass energy
distribution,
$L$ is the integrated luminosity from the ESC, $N_{QED}$ is the number
of events expected from QED alone, $N_{\twog}$ is the number of $\ee \to \twog$
seen, and $N_{BB}^{\ast}/L$ is the number of barrel Bhabha events seen per
$\rm pb^{-1}$ of luminosity, scaled by $s$.
\endpage
%\input tblcaptions
\vfill\eject
\noindent\kern-20truept\vbox{\tabskip=0pt \offinterlineskip
\def\tablerule{\noalign{\hrule}}
\setbox0=\hbox{$88.88$}           % for luminosities
\setbox1=\hbox{$888.8 \pm 8.8$}   % for N_QED
\setbox2=\hbox{$888$}             % for N_gg
\setbox3=\hbox{$260.9 \pm 18$}    % for N_bb / L
\setbox4=\hbox{18}                % for N_bb / L
\setbox5=\hbox{260.9}             % for N_bb / L
\def\LUM#1{\hbox to \wd0{\hfil $#1$}}
\def\NQED#1{\hbox to \wd1{\hfil $#1$}}
\def\NGG#1{\hbox to \wd2{\hfil $#1$}}
\def\NBB#1#2{\hbox to \wd3{\hfil $\hbox to \wd5{#1\hfil} \pm
\hbox to \wd4{\hfil #2}$}}
\halign{%
\vrule\enskip\hfil$\mathstrut #$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip&%
\vrule\enskip\hfil$#$\hfil\enskip\vrule\cr
\tablerule
\omit\vrule height 4pt&&&&&&\cr
\sqrt{s}\ \rm (GeV) & \sigmaE\ \rm(GeV) & L\ (\rm pb^{-1}) &
N_{QED} & N_{\twog} & N_{\twog}/N_{QED} & N_{BB}^{\ast}/L \cr
\omit\vrule height 4pt&&&&&&\cr
\tablerule
\omit\vrule height 4pt&&&&&&\cr
57.374 & 0.095 &  \LUM{2.05} &  \NQED{72.9 \pm 0.4} &  \NGG{69} &
                                0.95 \pm 0.11  &   \NBB{265}{11}  \cr
\omit\vrule height 4pt&&&&&&\cr
57.772 & 0.096 & \LUM{19.55} & \NQED{680.5 \pm 3.4} & \NGG{636} &
                               0.935 \pm 0.037 &
                               \NBB{276.0}{\rlap{3.8}\hfill} \cr
\omit\vrule height 4pt&&&&&&\cr
57.972 & 0.096 &  \LUM{1.39} &  \NQED{48.4 \pm 0.2} &  \NGG{49} &
                                1.01 \pm 0.15  &   \NBB{272}{14}  \cr
\omit\vrule height 4pt&&&&&&\cr
58.220 & 0.098 &  \LUM{1.33} &  \NQED{45.8 \pm 0.2} &  \NGG{50} &
                                1.09 \pm 0.15  &   \NBB{259}{14}  \cr
\omit\vrule height 4pt&&&&&&\cr
58.470 & 0.098 &  \LUM{1.33} &  \NQED{45.6 \pm 0.2} &  \NGG{54} &
                                1.18 \pm 0.16  &   \NBB{308}{15}  \cr
\omit\vrule height 4pt&&&&&&\cr
58.718 & 0.099 &  \LUM{1.73} &  \NQED{58.7 \pm 0.3} &  \NGG{61} &
                                1.04 \pm 0.13  &   \NBB{278}{13}  \cr
\omit\vrule height 4pt&&&&&&\cr
58.968 & 0.100 &  \LUM{1.36} &  \NQED{45.9 \pm 0.2} &  \NGG{45} &
                                0.98 \pm 0.15  &   \NBB{284}{15}  \cr
\omit\vrule height 4pt&&&&&&\cr
59.216 & 0.100 &  \LUM{1.21} &  \NQED{40.5 \pm 0.2} &  \NGG{45} &
                                1.11 \pm 0.17  &   \NBB{294}{16}  \cr
\omit\vrule height 4pt&&&&&&\cr
59.466 & 0.102 &  \LUM{0.97} &  \NQED{32.3 \pm 0.2} &  \NGG{26} &
                                0.81 \pm 0.16  &   \NBB{236}{16}  \cr
\omit\vrule height 4pt&&&&&&\cr
\tablerule}  % end of table
}  % end of \vbox
%\input table_1
\vfill\eject
\nopagenumbers
\Twelvepoint
\centerline {{\bf FIGURE CAPTIONS}}
\vskip 0.5 cm

\noindent{\bf Figure 1.}  Ratio of observed $\twog$ events to the QED
prediction.  The solid curve is the
QED prediction, with $\chi^2 / dof = 0.68$ for 8 degrees of freedom
and a normalization of 0.961.  The dashed curve is the maximum likelihood
prediction, with $\chi^2 / {dof} = 0.47$ for 5 degrees of freedom and a
normalization of 0.955.

\noindent{\bf Figure 2.} 90\% C.L. upper limits on $(2J+1)\Gee\BRgg$
as a function of mass $M$ of the state $X$, for widths of 1 MeV (solid curve),
100 MeV (dashed curve), 1 GeV (dotted curve) and 3 GeV (dash-dotted curve),
with a normalization of 0.955.  The region above a given curve is excluded.

\noindent{\bf Figure 3.} Exclusion regions (90\% C.L.) on $\Gamma_{\twog}$
{\it vs.} $\Gamma_{\rm ee}$ for a scalar $X$ with $M \sim 59\GeV$,
assuming $\Gamma \equiv \Gamma_{\twog} + 3\Gamma_{\rm ee}$.  The region above
and to the right of a given curve is excluded.  The solid curve is from this
experiment.  The other curves are from the observation of up to three
$\ll\twog$ events with $M_{\twog} \sim 59\GeV$ (dashed) and the absence
of $\ll\twog$ events with $M_{\ll} \sim 59\GeV$ (dash-dotted) (Ref.~\rfLTHREE),
and from the lack of a signal at $M_{\twog} \sim 59\GeV$ in $\threeg$ events
(dotted) (Ref.~\rfOPAL).
%The four \underbar{inclusion} regions overlap in the
%lower left of the figure.

\endpage
%\input figcaptions
% Figures go here
\end

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 6740 7201 vl
 6983 6961 il
 6983 7201 vl
 7226 7121 il
 7226 7201 vl
 7468 7121 il
 7468 7201 vl
 7711 7121 il
 7711 7201 vl
 7954 7121 il
 7954 7201 vl
 8197 6961 il
 8197 7201 vl
 8439 7121 il
 8439 7201 vl
 8682 7121 il
 8682 7201 vl
 8925 7121 il
 8925 7201 vl
 9167 7121 il
 9167 7201 vl
 9410 6961 il
 9410 7201 vl
 4 SLW
 2129 1824 il
 2209 1824 vl
 2129 2048 il
 2209 2048 vl
 2129 2272 il
 2209 2272 vl
 2129 2496 il
 2209 2496 vl
 2129 2720 il
 2369 2720 vl
 2129 2944 il
 2209 2944 vl
 2129 3168 il
 2209 3168 vl
 2129 3392 il
 2209 3392 vl
 2129 3616 il
 2209 3616 vl
 2129 3840 il
 2369 3840 vl
 2129 4064 il
 2209 4064 vl
 2129 4288 il
 2209 4288 vl
 2129 4513 il
 2209 4513 vl
 2129 4737 il
 2209 4737 vl
 2129 4961 il
 2369 4961 vl
 2129 5185 il
 2209 5185 vl
 2129 5409 il
 2209 5409 vl
 2129 5633 il
 2209 5633 vl
 2129 5857 il
 2209 5857 vl
 2129 6081 il
 2369 6081 vl
 2129 6305 il
 2209 6305 vl
 2129 6529 il
 2209 6529 vl
 2129 6753 il
 2209 6753 vl
 2129 6977 il
 2209 6977 vl
 2129 7201 il
 2369 7201 vl
 4 SLW
 1534 1661 il
 1514 1654 vl
 1501 1634 vl
 1494 1601 vl
 1494 1581 vl
 1501 1547 vl
 1514 1527 vl
 1534 1521 vl
 1547 1521 vl
 1567 1527 vl
 1581 1547 vl
 1587 1581 vl
 1587 1601 vl
 1581 1634 vl
 1567 1654 vl
 1547 1661 vl
 1534 1661 vl
 1534 1661 il
 1521 1654 vl
 1514 1647 vl
 1507 1634 vl
 1501 1601 vl
 1501 1581 vl
 1507 1547 vl
 1514 1534 vl
 1521 1527 vl
 1534 1521 vl
 1547 1521 il
 1561 1527 vl
 1567 1534 vl
 1574 1547 vl
 1581 1581 vl
 1581 1601 vl
 1574 1634 vl
 1567 1647 vl
 1561 1654 vl
 1547 1661 vl
 1641 1534 il
 1634 1527 vl
 1641 1521 vl
 1647 1527 vl
 1641 1534 vl
 1707 1661 il
 1694 1594 vl
 1694 1594 il
 1707 1607 vl
 1727 1614 vl
 1747 1614 vl
 1767 1607 vl
 1780 1594 vl
 1787 1574 vl
 1787 1561 vl
 1780 1541 vl
 1767 1527 vl
 1747 1521 vl
 1727 1521 vl
 1707 1527 vl
 1701 1534 vl
 1694 1547 vl
 1694 1554 vl
 1701 1561 vl
 1707 1554 vl
 1701 1547 vl
 1747 1614 il
 1760 1607 vl
 1774 1594 vl
 1780 1574 vl
 1780 1561 vl
 1774 1541 vl
 1760 1527 vl
 1747 1521 vl
 1707 1661 il
 1774 1661 vl
 1707 1654 il
 1740 1654 vl
 1774 1661 vl
 1867 1661 il
 1847 1654 vl
 1834 1634 vl
 1827 1601 vl
 1827 1581 vl
 1834 1547 vl
 1847 1527 vl
 1867 1521 vl
 1880 1521 vl
 1900 1527 vl
 1914 1547 vl
 1920 1581 vl
 1920 1601 vl
 1914 1634 vl
 1900 1654 vl
 1880 1661 vl
 1867 1661 vl
 1867 1661 il
 1854 1654 vl
 1847 1647 vl
 1840 1634 vl
 1834 1601 vl
 1834 1581 vl
 1840 1547 vl
 1847 1534 vl
 1854 1527 vl
 1867 1521 vl
 1880 1521 il
 1894 1527 vl
 1900 1534 vl
 1907 1547 vl
 1914 1581 vl
 1914 1601 vl
 1907 1634 vl
 1900 1647 vl
 1894 1654 vl
 1880 1661 vl
 1534 2781 il
 1514 2774 vl
 1501 2754 vl
 1494 2721 vl
 1494 2701 vl
 1501 2667 vl
 1514 2647 vl
 1534 2641 vl
 1547 2641 vl
 1567 2647 vl
 1581 2667 vl
 1587 2701 vl
 1587 2721 vl
 1581 2754 vl
 1567 2774 vl
 1547 2781 vl
 1534 2781 vl
 1534 2781 il
 1521 2774 vl
 1514 2767 vl
 1507 2754 vl
 1501 2721 vl
 1501 2701 vl
 1507 2667 vl
 1514 2654 vl
 1521 2647 vl
 1534 2641 vl
 1547 2641 il
 1561 2647 vl
 1567 2654 vl
 1574 2667 vl
 1581 2701 vl
 1581 2721 vl
 1574 2754 vl
 1567 2767 vl
 1561 2774 vl
 1547 2781 vl
 1641 2654 il
 1634 2647 vl
 1641 2641 vl
 1647 2647 vl
 1641 2654 vl
 1694 2781 il
 1694 2741 vl
 1694 2754 il
 1701 2767 vl
 1714 2781 vl
 1727 2781 vl
 1760 2761 vl
 1774 2761 vl
 1780 2767 vl
 1787 2781 vl
 1701 2767 il
 1714 2774 vl
 1727 2774 vl
 1760 2761 vl
 1787 2781 il
 1787 2761 vl
 1780 2741 vl
 1754 2707 vl
 1747 2694 vl
 1740 2674 vl
 1740 2641 vl
 1780 2741 il
 1747 2707 vl
 1740 2694 vl
 1734 2674 vl
 1734 2641 vl
 1840 2781 il
 1827 2714 vl
 1827 2714 il
 1840 2727 vl
 1860 2734 vl
 1880 2734 vl
 1900 2727 vl
 1914 2714 vl
 1920 2694 vl
 1920 2681 vl
 1914 2661 vl
 1900 2647 vl
 1880 2641 vl
 1860 2641 vl
 1840 2647 vl
 1834 2654 vl
 1827 2667 vl
 1827 2674 vl
 1834 2681 vl
 1840 2674 vl
 1834 2667 vl
 1880 2734 il
 1894 2727 vl
 1907 2714 vl
 1914 2694 vl
 1914 2681 vl
 1907 2661 vl
 1894 2647 vl
 1880 2641 vl
 1840 2781 il
 1907 2781 vl
 1840 2774 il
 1874 2774 vl
 1907 2781 vl
 1514 3874 il
 1527 3881 vl
 1547 3901 vl
 1547 3761 vl
 1541 3894 il
 1541 3761 vl
 1514 3761 il
 1574 3761 vl
 1641 3774 il
 1634 3767 vl
 1641 3761 vl
 1647 3767 vl
 1641 3774 vl
 1734 3901 il
 1714 3894 vl
 1701 3874 vl
 1694 3841 vl
 1694 3821 vl
 1701 3787 vl
 1714 3767 vl
 1734 3761 vl
 1747 3761 vl
 1767 3767 vl
 1780 3787 vl
 1787 3821 vl
 1787 3841 vl
 1780 3874 vl
 1767 3894 vl
 1747 3901 vl
 1734 3901 vl
 1734 3901 il
 1720 3894 vl
 1714 3887 vl
 1707 3874 vl
 1701 3841 vl
 1701 3821 vl
 1707 3787 vl
 1714 3774 vl
 1720 3767 vl
 1734 3761 vl
 1747 3761 il
 1760 3767 vl
 1767 3774 vl
 1774 3787 vl
 1780 3821 vl
 1780 3841 vl
 1774 3874 vl
 1767 3887 vl
 1760 3894 vl
 1747 3901 vl
 1867 3901 il
 1847 3894 vl
 1834 3874 vl
 1827 3841 vl
 1827 3821 vl
 1834 3787 vl
 1847 3767 vl
 1867 3761 vl
 1880 3761 vl
 1900 3767 vl
 1914 3787 vl
 1920 3821 vl
 1920 3841 vl
 1914 3874 vl
 1900 3894 vl
 1880 3901 vl
 1867 3901 vl
 1867 3901 il
 1854 3894 vl
 1847 3887 vl
 1840 3874 vl
 1834 3841 vl
 1834 3821 vl
 1840 3787 vl
 1847 3774 vl
 1854 3767 vl
 1867 3761 vl
 1880 3761 il
 1894 3767 vl
 1900 3774 vl
 1907 3787 vl
 1914 3821 vl
 1914 3841 vl
 1907 3874 vl
 1900 3887 vl
 1894 3894 vl
 1880 3901 vl
 1514 4994 il
 1527 5000 vl
 1547 5020 vl
 1547 4880 vl
 1541 5014 il
 1541 4880 vl
 1514 4880 il
 1574 4880 vl
 1641 4894 il
 1634 4887 vl
 1641 4880 vl
 1647 4887 vl
 1641 4894 vl
 1701 4994 il
 1707 4987 vl
 1701 4980 vl
 1694 4987 vl
 1694 4994 vl
 1701 5007 vl
 1707 5014 vl
 1727 5020 vl
 1754 5020 vl
 1774 5014 vl
 1780 5007 vl
 1787 4994 vl
 1787 4980 vl
 1780 4967 vl
 1760 4954 vl
 1727 4940 vl
 1714 4934 vl
 1701 4920 vl
 1694 4900 vl
 1694 4880 vl
 1754 5020 il
 1767 5014 vl
 1774 5007 vl
 1780 4994 vl
 1780 4980 vl
 1774 4967 vl
 1754 4954 vl
 1727 4940 vl
 1694 4894 il
 1701 4900 vl
 1714 4900 vl
 1747 4887 vl
 1767 4887 vl
 1780 4894 vl
 1787 4900 vl
 1714 4900 il
 1747 4880 vl
 1774 4880 vl
 1780 4887 vl
 1787 4900 vl
 1787 4914 vl
 1840 5020 il
 1827 4954 vl
 1827 4954 il
 1840 4967 vl
 1860 4974 vl
 1880 4974 vl
 1900 4967 vl
 1914 4954 vl
 1920 4934 vl
 1920 4920 vl
 1914 4900 vl
 1900 4887 vl
 1880 4880 vl
 1860 4880 vl
 1840 4887 vl
 1834 4894 vl
 1827 4907 vl
 1827 4914 vl
 1834 4920 vl
 1840 4914 vl
 1834 4907 vl
 1880 4974 il
 1894 4967 vl
 1907 4954 vl
 1914 4934 vl
 1914 4920 vl
 1907 4900 vl
 1894 4887 vl
 1880 4880 vl
 1840 5020 il
 1907 5020 vl
 1840 5014 il
 1874 5014 vl
 1907 5020 vl
 1514 6114 il
 1527 6120 vl
 1547 6140 vl
 1547 6000 vl
 1541 6134 il
 1541 6000 vl
 1514 6000 il
 1574 6000 vl
 1641 6014 il
 1634 6007 vl
 1641 6000 vl
 1647 6007 vl
 1641 6014 vl
 1707 6140 il
 1694 6074 vl
 1694 6074 il
 1707 6087 vl
 1727 6094 vl
 1747 6094 vl
 1767 6087 vl
 1780 6074 vl
 1787 6054 vl
 1787 6040 vl
 1780 6020 vl
 1767 6007 vl
 1747 6000 vl
 1727 6000 vl
 1707 6007 vl
 1701 6014 vl
 1694 6027 vl
 1694 6034 vl
 1701 6040 vl
 1707 6034 vl
 1701 6027 vl
 1747 6094 il
 1760 6087 vl
 1774 6074 vl
 1780 6054 vl
 1780 6040 vl
 1774 6020 vl
 1760 6007 vl
 1747 6000 vl
 1707 6140 il
 1774 6140 vl
 1707 6134 il
 1740 6134 vl
 1774 6140 vl
 1867 6140 il
 1847 6134 vl
 1834 6114 vl
 1827 6080 vl
 1827 6060 vl
 1834 6027 vl
 1847 6007 vl
 1867 6000 vl
 1880 6000 vl
 1900 6007 vl
 1914 6027 vl
 1920 6060 vl
 1920 6080 vl
 1914 6114 vl
 1900 6134 vl
 1880 6140 vl
 1867 6140 vl
 1867 6140 il
 1854 6134 vl
 1847 6127 vl
 1840 6114 vl
 1834 6080 vl
 1834 6060 vl
 1840 6027 vl
 1847 6014 vl
 1854 6007 vl
 1867 6000 vl
 1880 6000 il
 1894 6007 vl
 1900 6014 vl
 1907 6027 vl
 1914 6060 vl
 1914 6080 vl
 1907 6114 vl
 1900 6127 vl
 1894 6134 vl
 1880 6140 vl
 1514 7233 il
 1527 7240 vl
 1547 7260 vl
 1547 7120 vl
 1541 7253 il
 1541 7120 vl
 1514 7120 il
 1574 7120 vl
 1641 7133 il
 1634 7127 vl
 1641 7120 vl
 1647 7127 vl
 1641 7133 vl
 1694 7260 il
 1694 7220 vl
 1694 7233 il
 1701 7247 vl
 1714 7260 vl
 1727 7260 vl
 1760 7240 vl
 1774 7240 vl
 1780 7247 vl
 1787 7260 vl
 1701 7247 il
 1714 7253 vl
 1727 7253 vl
 1760 7240 vl
 1787 7260 il
 1787 7240 vl
 1780 7220 vl
 1754 7187 vl
 1747 7173 vl
 1740 7153 vl
 1740 7120 vl
 1780 7220 il
 1747 7187 vl
 1740 7173 vl
 1734 7153 vl
 1734 7120 vl
 1840 7260 il
 1827 7193 vl
 1827 7193 il
 1840 7207 vl
 1860 7213 vl
 1880 7213 vl
 1900 7207 vl
 1914 7193 vl
 1920 7173 vl
 1920 7160 vl
 1914 7140 vl
 1900 7127 vl
 1880 7120 vl
 1860 7120 vl
 1840 7127 vl
 1834 7133 vl
 1827 7147 vl
 1827 7153 vl
 1834 7160 vl
 1840 7153 vl
 1834 7147 vl
 1880 7213 il
 1894 7207 vl
 1907 7193 vl
 1914 7173 vl
 1914 7160 vl
 1907 7140 vl
 1894 7127 vl
 1880 7120 vl
 1840 7260 il
 1907 7260 vl
 1840 7253 il
 1874 7253 vl
 1907 7260 vl
 4 SLW
 9330 1824 il
 9410 1824 vl
 9330 2048 il
 9410 2048 vl
 9330 2272 il
 9410 2272 vl
 9330 2496 il
 9410 2496 vl
 9170 2720 il
 9410 2720 vl
 9330 2944 il
 9410 2944 vl
 9330 3168 il
 9410 3168 vl
 9330 3392 il
 9410 3392 vl
 9330 3616 il
 9410 3616 vl
 9170 3840 il
 9410 3840 vl
 9330 4064 il
 9410 4064 vl
 9330 4288 il
 9410 4288 vl
 9330 4513 il
 9410 4513 vl
 9330 4737 il
 9410 4737 vl
 9170 4961 il
 9410 4961 vl
 9330 5185 il
 9410 5185 vl
 9330 5409 il
 9410 5409 vl
 9330 5633 il
 9410 5633 vl
 9330 5857 il
 9410 5857 vl
 9170 6081 il
 9410 6081 vl
 9330 6305 il
 9410 6305 vl
 9330 6529 il
 9410 6529 vl
 9330 6753 il
 9410 6753 vl
 9330 6977 il
 9410 6977 vl
 9170 7201 il
 9410 7201 vl
 4 SLW
 4840 1061 il
 4880 1061 vl
 4940  941 vl
 4870 1061 il
 4940  921 vl
 5030 1191 vl
 5160 1041 il
 5170 1061 vl
 5170 1021 vl
 5160 1041 vl
 5150 1051 vl
 5130 1061 vl
 5090 1061 vl
 5070 1051 vl
 5060 1041 vl
 5060 1021 vl
 5070 1011 vl
 5090 1001 vl
 5140  981 vl
 5160  971 vl
 5170  961 vl
 5060 1031 il
 5070 1021 vl
 5090 1011 vl
 5140  991 vl
 5160  981 vl
 5170  971 vl
 5170  941 vl
 5160  931 vl
 5140  921 vl
 5100  921 vl
 5080  931 vl
 5070  941 vl
 5060  961 vl
 5060  921 vl
 5070  941 vl
 5469 1171 il
 5449 1151 vl
 5429 1121 vl
 5409 1081 vl
 5399 1031 vl
 5399  991 vl
 5409  941 vl
 5429  901 vl
 5449  871 vl
 5469  851 vl
 5449 1151 il
 5429 1111 vl
 5419 1081 vl
 5409 1031 vl
 5409  991 vl
 5419  941 vl
 5429  911 vl
 5449  871 vl
 5669 1101 il
 5679 1071 vl
 5679 1131 vl
 5669 1101 vl
 5649 1121 vl
 5619 1131 vl
 5599 1131 vl
 5569 1121 vl
 5549 1101 vl
 5539 1081 vl
 5529 1051 vl
 5529 1001 vl
 5539  971 vl
 5549  951 vl
 5569  931 vl
 5599  921 vl
 5619  921 vl
 5649  931 vl
 5669  951 vl
 5599 1131 il
 5579 1121 vl
 5559 1101 vl
 5549 1081 vl
 5539 1051 vl
 5539 1001 vl
 5549  971 vl
 5559  951 vl
 5579  931 vl
 5599  921 vl
 5669 1001 il
 5669  921 vl
 5679 1001 il
 5679  921 vl
 5639 1001 il
 5709 1001 vl
 5769 1001 il
 5889 1001 vl
 5889 1021 vl
 5879 1041 vl
 5869 1051 vl
 5849 1061 vl
 5819 1061 vl
 5789 1051 vl
 5769 1031 vl
 5759 1001 vl
 5759  981 vl
 5769  951 vl
 5789  931 vl
 5819  921 vl
 5839  921 vl
 5869  931 vl
 5889  951 vl
 5879 1001 il
 5879 1031 vl
 5869 1051 vl
 5819 1061 il
 5799 1051 vl
 5779 1031 vl
 5769 1001 vl
 5769  981 vl
 5779  951 vl
 5799  931 vl
 5819  921 vl
 5949 1131 il
 6019  921 vl
 5959 1131 il
 6019  951 vl
 6089 1131 il
 6019  921 vl
 5929 1131 il
 5989 1131 vl
 6049 1131 il
 6109 1131 vl
 6149 1171 il
 6169 1151 vl
 6189 1121 vl
 6209 1081 vl
 6219 1031 vl
 6219  991 vl
 6209  941 vl
 6189  901 vl
 6169  871 vl
 6149  851 vl
 6169 1151 il
 6189 1111 vl
 6199 1081 vl
 6209 1031 vl
 6209  991 vl
 6199  941 vl
 6189  911 vl
 6169  871 vl
 4 SLW
 4 SLW
 1040 3811 il
 1250 3811 vl
 1040 3821 il
 1230 3940 vl
 1060 3821 il
 1250 3940 vl
 1040 3940 il
 1250 3940 vl
 1040 3781 il
 1040 3821 vl
 1040 3911 il
 1040 3970 vl
 1250 3781 il
 1250 3841 vl
 1256 4010 il
 1243 4024 vl
 1236 4037 vl
 1236 4050 vl
 1243 4064 vl
 1250 4070 vl
 1270 4077 vl
 1296 4077 vl
 1323 4070 vl
 1376 4050 vl
 1250 4017 il
 1243 4030 vl
 1243 4057 vl
 1250 4070 vl
 1236 4124 il
 1256 4117 vl
 1270 4110 vl
 1316 4077 vl
 1350 4057 vl
 1376 4044 vl
 1236 4117 il
 1256 4110 vl
 1270 4104 vl
 1316 4077 vl
 1256 4144 il
 1243 4157 vl
 1236 4170 vl
 1236 4184 vl
 1243 4197 vl
 1250 4204 vl
 1270 4210 vl
 1296 4210 vl
 1323 4204 vl
 1376 4184 vl
 1250 4150 il
 1243 4164 vl
 1243 4190 vl
 1250 4204 vl
 1236 4257 il
 1256 4250 vl
 1270 4244 vl
 1316 4210 vl
 1350 4190 vl
 1376 4177 vl
 1236 4250 il
 1256 4244 vl
 1270 4237 vl
 1316 4210 vl
 1000 4457 il
 1320 4277 vl
 1040 4527 il
 1250 4527 vl
 1040 4537 il
 1230 4657 vl
 1060 4537 il
 1250 4657 vl
 1040 4657 il
 1250 4657 vl
 1040 4497 il
 1040 4537 vl
 1040 4627 il
 1040 4687 vl
 1250 4497 il
 1250 4557 vl
 1190 4787 il
 1196 4767 vl
 1210 4754 vl
 1223 4747 vl
 1250 4740 vl
 1270 4740 vl
 1296 4747 vl
 1310 4754 vl
 1323 4767 vl
 1330 4787 vl
 1330 4800 vl
 1323 4820 vl
 1310 4834 vl
 1296 4840 vl
 1270 4847 vl
 1250 4847 vl
 1223 4840 vl
 1210 4834 vl
 1196 4820 vl
 1190 4800 vl
 1190 4787 vl
 1190 4787 il
 1196 4774 vl
 1210 4760 vl
 1223 4754 vl
 1250 4747 vl
 1270 4747 vl
 1296 4754 vl
 1310 4760 vl
 1323 4774 vl
 1330 4787 vl
 1330 4800 il
 1323 4814 vl
 1310 4827 vl
 1296 4834 vl
 1270 4840 vl
 1250 4840 vl
 1223 4834 vl
 1210 4827 vl
 1196 4814 vl
 1190 4800 vl
 1316 4767 il
 1310 4767 vl
 1296 4774 vl
 1290 4787 vl
 1290 4794 vl
 1296 4807 vl
 1310 4814 vl
 1356 4820 vl
 1363 4827 vl
 1363 4840 vl
 1350 4847 vl
 1343 4847 vl
 1310 4814 il
 1336 4820 vl
 1350 4827 vl
 1356 4834 vl
 1356 4840 vl
 1350 4847 vl
 1190 4900 il
 1330 4900 vl
 1190 4907 il
 1330 4907 vl
 1230 4947 il
 1283 4947 vl
 1190 4880 il
 1190 4987 vl
 1230 4987 vl
 1190 4980 vl
 1256 4907 il
 1256 4947 vl
 1330 4880 il
 1330 4987 vl
 1290 4987 vl
 1330 4980 vl
 1190 5040 il
 1330 5040 vl
 1190 5047 il
 1330 5047 vl
 1190 5020 il
 1190 5087 vl
 1196 5107 vl
 1210 5120 vl
 1223 5127 vl
 1243 5134 vl
 1276 5134 vl
 1296 5127 vl
 1310 5120 vl
 1323 5107 vl
 1330 5087 vl
 1330 5020 vl
 1190 5087 il
 1196 5100 vl
 1210 5114 vl
 1223 5120 vl
 1243 5127 vl
 1276 5127 vl
 1296 5120 vl
 1310 5114 vl
 1323 5100 vl
 1330 5087 vl
 4 SLW
 5409 6800 il
 6289 6800 vl
 5409 6400 il
 5489 6400 vl
 5569 6400 il
 5649 6400 vl
 5729 6400 il
 5809 6400 vl
 5889 6400 il
 5969 6400 vl
 6049 6400 il
 6129 6400 vl
 6209 6400 il
 6289 6400 vl
 4 SLW
 6433 6875 il
 6408 6867 vl
 6391 6850 vl
 6383 6833 vl
 6374 6800 vl
 6374 6775 vl
 6383 6742 vl
 6391 6725 vl
 6408 6708 vl
 6433 6700 vl
 6449 6700 vl
 6474 6708 vl
 6491 6725 vl
 6499 6742 vl
 6508 6775 vl
 6508 6800 vl
 6499 6833 vl
 6491 6850 vl
 6474 6867 vl
 6449 6875 vl
 6433 6875 vl
 6433 6875 il
 6416 6867 vl
 6399 6850 vl
 6391 6833 vl
 6383 6800 vl
 6383 6775 vl
 6391 6742 vl
 6399 6725 vl
 6416 6708 vl
 6433 6700 vl
 6449 6700 il
 6466 6708 vl
 6483 6725 vl
 6491 6742 vl
 6499 6775 vl
 6499 6800 vl
 6491 6833 vl
 6483 6850 vl
 6466 6867 vl
 6449 6875 vl
 6408 6717 il
 6408 6725 vl
 6416 6742 vl
 6433 6750 vl
 6441 6750 vl
 6458 6742 vl
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 6313 1081 vl
 6323 1031 vl
 6323  991 vl
 6313  941 vl
 6293  901 vl
 6273  871 vl
 6253  851 vl
 6273 1151 il
 6293 1111 vl
 6303 1081 vl
 6313 1031 vl
 6313  991 vl
 6303  941 vl
 6293  911 vl
 6273  871 vl
 4 SLW
  840 2511 il
  860 2491 vl
  890 2471 vl
  930 2451 vl
  980 2441 vl
 1020 2441 vl
 1070 2451 vl
 1110 2471 vl
 1140 2491 vl
 1160 2511 vl
  860 2491 il
  900 2471 vl
  930 2461 vl
  980 2451 vl
 1020 2451 vl
 1070 2461 vl
 1100 2471 vl
 1140 2491 vl
  920 2581 il
  930 2591 vl
  940 2581 vl
  930 2571 vl
  920 2571 vl
  900 2581 vl
  890 2591 vl
  880 2621 vl
  880 2661 vl
  890 2691 vl
  900 2701 vl
  920 2711 vl
  940 2711 vl
  960 2701 vl
  980 2671 vl
 1000 2621 vl
 1010 2601 vl
 1030 2581 vl
 1060 2571 vl
 1090 2571 vl
  880 2661 il
  890 2681 vl
  900 2691 vl
  920 2701 vl
  940 2701 vl
  960 2691 vl
  980 2661 vl
 1000 2621 vl
 1070 2571 il
 1060 2581 vl
 1060 2601 vl
 1080 2651 vl
 1080 2681 vl
 1070 2701 vl
 1060 2711 vl
 1060 2601 il
 1090 2651 vl
 1090 2691 vl
 1080 2701 vl
 1060 2711 vl
 1040 2711 vl
  880 2841 il
 1050 2841 vl
 1080 2831 vl
 1090 2811 vl
 1090 2791 vl
 1080 2771 vl
 1060 2761 vl
 1040 2761 vl
 1030 2771 vl
 1040 2781 vl
 1050 2771 vl
  880 2831 il
 1050 2831 vl
 1080 2821 vl
 1090 2811 vl
  880 2801 il
  880 2871 vl
  910 3021 il
 1090 3021 vl
 1000 2931 il
 1000 3111 vl
  920 3211 il
  910 3231 vl
  880 3261 vl
 1090 3261 vl
  890 3251 il
 1090 3251 vl
 1090 3211 il
 1090 3301 vl
  840 3381 il
  860 3401 vl
  890 3421 vl
  930 3441 vl
  980 3451 vl
 1020 3451 vl
 1070 3441 vl
 1110 3421 vl
 1140 3401 vl
 1160 3381 vl
  860 3401 il
  900 3421 vl
  930 3431 vl
  980 3441 vl
 1020 3441 vl
 1070 3431 vl
 1100 3421 vl
 1140 3401 vl
  880 3701 il
 1090 3701 vl
  880 3711 il
 1090 3711 vl
  880 3671 il
  880 3821 vl
  940 3821 vl
  880 3811 vl
 1090 3671 il
 1090 3741 vl
 1116 3871 il
 1116 3950 vl
 1103 3950 vl
 1090 3944 vl
 1083 3937 vl
 1076 3924 vl
 1076 3904 vl
 1083 3884 vl
 1096 3871 vl
 1116 3864 vl
 1130 3864 vl
 1150 3871 vl
 1163 3884 vl
 1170 3904 vl
 1170 3917 vl
 1163 3937 vl
 1150 3950 vl
 1116 3944 il
 1096 3944 vl
 1083 3937 vl
 1076 3904 il
 1083 3891 vl
 1096 3877 vl
 1116 3871 vl
 1130 3871 vl
 1150 3877 vl
 1163 3891 vl
 1170 3904 vl
 1116 3997 il
 1116 4077 vl
 1103 4077 vl
 1090 4070 vl
 1083 4064 vl
 1076 4050 vl
 1076 4030 vl
 1083 4010 vl
 1096 3997 vl
 1116 3990 vl
 1130 3990 vl
 1150 3997 vl
 1163 4010 vl
 1170 4030 vl
 1170 4044 vl
 1163 4064 vl
 1150 4077 vl
 1116 4070 il
 1096 4070 vl
 1083 4064 vl
 1076 4030 il
 1083 4017 vl
 1096 4004 vl
 1116 3997 vl
 1130 3997 vl
 1150 4004 vl
 1163 4017 vl
 1170 4030 vl
  880 4294 il
 1090 4294 vl
  880 4304 il
 1090 4304 vl
  880 4264 il
  880 4384 vl
  890 4414 vl
  900 4424 vl
  920 4434 vl
  940 4434 vl
  960 4424 vl
  970 4414 vl
  980 4384 vl
  880 4384 il
  890 4404 vl
  900 4414 vl
  920 4424 vl
  940 4424 vl
  960 4414 vl
  970 4404 vl
  980 4384 vl
  980 4304 il
  980 4384 vl
  990 4414 vl
 1000 4424 vl
 1020 4434 vl
 1050 4434 vl
 1070 4424 vl
 1080 4414 vl
 1090 4384 vl
 1090 4264 vl
  980 4384 il
  990 4404 vl
 1000 4414 vl
 1020 4424 vl
 1050 4424 vl
 1070 4414 vl
 1080 4404 vl
 1090 4384 vl
  880 4514 il
 1090 4514 vl
  880 4524 il
 1090 4524 vl
  880 4484 il
  880 4604 vl
  890 4634 vl
  900 4644 vl
  920 4654 vl
  940 4654 vl
  960 4644 vl
  970 4634 vl
  980 4604 vl
  980 4524 vl
  880 4604 il
  890 4624 vl
  900 4634 vl
  920 4644 vl
  940 4644 vl
  960 4634 vl
  970 4624 vl
  980 4604 vl
 1090 4484 il
 1090 4554 vl
  980 4574 il
  990 4594 vl
 1000 4604 vl
 1070 4634 vl
 1080 4644 vl
 1080 4654 vl
 1070 4664 vl
  990 4594 il
 1010 4604 vl
 1080 4624 vl
 1090 4634 vl
 1090 4654 vl
 1070 4664 vl
 1060 4664 vl
 1096 4704 il
 1083 4717 vl
 1076 4730 vl
 1076 4744 vl
 1083 4757 vl
 1090 4764 vl
 1110 4770 vl
 1136 4770 vl
 1163 4764 vl
 1216 4744 vl
 1090 4710 il
 1083 4724 vl
 1083 4750 vl
 1090 4764 vl
 1076 4817 il
 1096 4810 vl
 1110 4804 vl
 1156 4770 vl
 1190 4750 vl
 1216 4737 vl
 1076 4810 il
 1096 4804 vl
 1110 4797 vl
 1156 4770 vl
 1096 4837 il
 1083 4850 vl
 1076 4864 vl
 1076 4877 vl
 1083 4890 vl
 1090 4897 vl
 1110 4904 vl
 1136 4904 vl
 1163 4897 vl
 1216 4877 vl
 1090 4844 il
 1083 4857 vl
 1083 4884 vl
 1090 4897 vl
 1076 4950 il
 1096 4944 vl
 1110 4937 vl
 1156 4904 vl
 1190 4884 vl
 1216 4870 vl
 1076 4944 il
 1096 4937 vl
 1110 4930 vl
 1156 4904 vl
  840 5220 il
  860 5200 vl
  890 5180 vl
  930 5160 vl
  980 5150 vl
 1020 5150 vl
 1070 5160 vl
 1110 5180 vl
 1140 5200 vl
 1160 5220 vl
  860 5200 il
  900 5180 vl
  930 5170 vl
  980 5160 vl
 1020 5160 vl
 1070 5170 vl
 1100 5180 vl
 1140 5200 vl
  880 5300 il
 1090 5300 vl
  880 5310 il
 1090 5310 vl
  950 5410 il
 1050 5310 vl
 1010 5360 il
 1090 5420 vl
 1010 5350 il
 1090 5410 vl
  880 5270 il
  880 5310 vl
  950 5380 il
  950 5440 vl
 1090 5270 il
 1090 5340 vl
 1090 5380 il
 1090 5440 vl
 1010 5500 il
 1010 5620 vl
  990 5620 vl
  970 5610 vl
  960 5600 vl
  950 5580 vl
  950 5550 vl
  960 5520 vl
  980 5500 vl
 1010 5490 vl
 1030 5490 vl
 1060 5500 vl
 1080 5520 vl
 1090 5550 vl
 1090 5570 vl
 1080 5600 vl
 1060 5620 vl
 1010 5610 il
  980 5610 vl
  960 5600 vl
  950 5550 il
  960 5530 vl
  980 5510 vl
 1010 5500 vl
 1030 5500 vl
 1060 5510 vl
 1080 5530 vl
 1090 5550 vl
  880 5680 il
 1090 5750 vl
  880 5690 il
 1060 5750 vl
  880 5820 il
 1090 5750 vl
  880 5660 il
  880 5720 vl
  880 5780 il
  880 5840 vl
  840 5880 il
  860 5900 vl
  890 5920 vl
  930 5940 vl
  980 5950 vl
 1020 5950 vl
 1070 5940 vl
 1110 5920 vl
 1140 5900 vl
 1160 5880 vl
  860 5900 il
  900 5920 vl
  930 5930 vl
  980 5940 vl
 1020 5940 vl
 1070 5930 vl
 1100 5920 vl
 1140 5900 vl
 4 SLW
 3831 3436 il
 3831 3261 vl
 3840 3436 il
 3840 3261 vl
 3806 3436 il
 3931 3436 vl
 3931 3386 vl
 3923 3436 vl
 3806 3261 il
 3865 3261 vl
 4106 3361 il
 4256 3361 vl
 4106 3311 il
 4256 3311 vl
 4473 3402 il
 4490 3411 vl
 4515 3436 vl
 4515 3261 vl
 4506 3427 il
 4506 3261 vl
 4473 3261 il
 4548 3261 vl
 4765 3436 il
 4765 3261 vl
 4773 3436 il
 4823 3286 vl
 4765 3436 il
 4823 3261 vl
 4881 3436 il
 4823 3261 vl
 4881 3436 il
 4881 3261 vl
 4890 3436 il
 4890 3261 vl
 4740 3436 il
 4773 3436 vl
 4881 3436 il
 4915 3436 vl
 4740 3261 il
 4790 3261 vl
 4856 3261 il
 4915 3261 vl
 4965 3327 il
 5065 3327 vl
 5065 3344 vl
 5056 3361 vl
 5048 3369 vl
 5031 3377 vl
 5006 3377 vl
 4981 3369 vl
 4965 3352 vl
 4956 3327 vl
 4956 3311 vl
 4965 3286 vl
 4981 3269 vl
 5006 3261 vl
 5023 3261 vl
 5048 3269 vl
 5065 3286 vl
 5056 3327 il
 5056 3352 vl
 5048 3369 vl
 5006 3377 il
 4990 3369 vl
 4973 3352 vl
 4965 3327 vl
 4965 3311 vl
 4973 3286 vl
 4990 3269 vl
 5006 3261 vl
 5115 3436 il
 5173 3261 vl
 5123 3436 il
 5173 3286 vl
 5231 3436 il
 5173 3261 vl
 5098 3436 il
 5148 3436 vl
 5198 3436 il
 5248 3436 vl
 4 SLW
 3831 3036 il
 3831 2861 vl
 3840 3036 il
 3840 2861 vl
 3806 3036 il
 3931 3036 vl
 3931 2986 vl
 3923 3036 vl
 3806 2861 il
 3865 2861 vl
 4106 2961 il
 4256 2961 vl
 4106 2911 il
 4256 2911 vl
 4473 3002 il
 4490 3011 vl
 4515 3036 vl
 4515 2861 vl
 4506 3027 il
 4506 2861 vl
 4473 2861 il
 4548 2861 vl
 4665 3036 il
 4640 3027 vl
 4623 3002 vl
 4615 2961 vl
 4615 2936 vl
 4623 2894 vl
 4640 2869 vl
 4665 2861 vl
 4681 2861 vl
 4706 2869 vl
 4723 2894 vl
 4731 2936 vl
 4731 2961 vl
 4723 3002 vl
 4706 3027 vl
 4681 3036 vl
 4665 3036 vl
 4665 3036 il
 4648 3027 vl
 4640 3019 vl
 4631 3002 vl
 4623 2961 vl
 4623 2936 vl
 4631 2894 vl
 4640 2877 vl
 4648 2869 vl
 4665 2861 vl
 4681 2861 il
 4698 2869 vl
 4706 2877 vl
 4715 2894 vl
 4723 2936 vl
 4723 2961 vl
 4715 3002 vl
 4706 3019 vl
 4698 3027 vl
 4681 3036 vl
 4831 3036 il
 4806 3027 vl
 4790 3002 vl
 4781 2961 vl
 4781 2936 vl
 4790 2894 vl
 4806 2869 vl
 4831 2861 vl
 4848 2861 vl
 4873 2869 vl
 4890 2894 vl
 4898 2936 vl
 4898 2961 vl
 4890 3002 vl
 4873 3027 vl
 4848 3036 vl
 4831 3036 vl
 4831 3036 il
 4815 3027 vl
 4806 3019 vl
 4798 3002 vl
 4790 2961 vl
 4790 2936 vl
 4798 2894 vl
 4806 2877 vl
 4815 2869 vl
 4831 2861 vl
 4848 2861 il
 4865 2869 vl
 4873 2877 vl
 4881 2894 vl
 4890 2936 vl
 4890 2961 vl
 4881 3002 vl
 4873 3019 vl
 4865 3027 vl
 4848 3036 vl
 5098 3036 il
 5098 2861 vl
 5106 3036 il
 5156 2886 vl
 5098 3036 il
 5156 2861 vl
 5215 3036 il
 5156 2861 vl
 5215 3036 il
 5215 2861 vl
 5223 3036 il
 5223 2861 vl
 5073 3036 il
 5106 3036 vl
 5215 3036 il
 5248 3036 vl
 5073 2861 il
 5123 2861 vl
 5190 2861 il
 5248 2861 vl
 5298 2927 il
 5398 2927 vl
 5398 2944 vl
 5389 2961 vl
 5381 2969 vl
 5364 2977 vl
 5339 2977 vl
 5314 2969 vl
 5298 2952 vl
 5289 2927 vl
 5289 2911 vl
 5298 2886 vl
 5314 2869 vl
 5339 2861 vl
 5356 2861 vl
 5381 2869 vl
 5398 2886 vl
 5389 2927 il
 5389 2952 vl
 5381 2969 vl
 5339 2977 il
 5323 2969 vl
 5306 2952 vl
 5298 2927 vl
 5298 2911 vl
 5306 2886 vl
 5323 2869 vl
 5339 2861 vl
 5448 3036 il
 5506 2861 vl
 5456 3036 il
 5506 2886 vl
 5564 3036 il
 5506 2861 vl
 5431 3036 il
 5481 3036 vl
 5531 3036 il
 5581 3036 vl
 4 SLW
 3831 2636 il
 3831 2461 vl
 3840 2636 il
 3840 2461 vl
 3806 2636 il
 3931 2636 vl
 3931 2586 vl
 3923 2636 vl
 3806 2461 il
 3865 2461 vl
 4106 2561 il
 4256 2561 vl
 4106 2511 il
 4256 2511 vl
 4473 2602 il
 4490 2611 vl
 4515 2636 vl
 4515 2461 vl
 4506 2627 il
 4506 2461 vl
 4473 2461 il
 4548 2461 vl
 4865 2611 il
 4873 2586 vl
 4873 2636 vl
 4865 2611 vl
 4848 2627 vl
 4823 2636 vl
 4806 2636 vl
 4781 2627 vl
 4765 2611 vl
 4756 2594 vl
 4748 2569 vl
 4748 2527 vl
 4756 2502 vl
 4765 2486 vl
 4781 2469 vl
 4806 2461 vl
 4823 2461 vl
 4848 2469 vl
 4865 2486 vl
 4806 2636 il
 4790 2627 vl
 4773 2611 vl
 4765 2594 vl
 4756 2569 vl
 4756 2527 vl
 4765 2502 vl
 4773 2486 vl
 4790 2469 vl
 4806 2461 vl
 4865 2527 il
 4865 2461 vl
 4873 2527 il
 4873 2461 vl
 4840 2527 il
 4898 2527 vl
 4948 2527 il
 5048 2527 vl
 5048 2544 vl
 5040 2561 vl
 5031 2569 vl
 5015 2577 vl
 4990 2577 vl
 4965 2569 vl
 4948 2552 vl
 4940 2527 vl
 4940 2511 vl
 4948 2486 vl
 4965 2469 vl
 4990 2461 vl
 5006 2461 vl
 5031 2469 vl
 5048 2486 vl
 5040 2527 il
 5040 2552 vl
 5031 2569 vl
 4990 2577 il
 4973 2569 vl
 4956 2552 vl
 4948 2527 vl
 4948 2511 vl
 4956 2486 vl
 4973 2469 vl
 4990 2461 vl
 5098 2636 il
 5156 2461 vl
 5106 2636 il
 5156 2486 vl
 5215 2636 il
 5156 2461 vl
 5081 2636 il
 5131 2636 vl
 5181 2636 il
 5231 2636 vl
 4 SLW
 3831 2236 il
 3831 2061 vl
 3840 2236 il
 3840 2061 vl
 3806 2236 il
 3931 2236 vl
 3931 2186 vl
 3923 2236 vl
 3806 2061 il
 3865 2061 vl
 4106 2161 il
 4256 2161 vl
 4106 2111 il
 4256 2111 vl
 4456 2202 il
 4465 2194 vl
 4456 2186 vl
 4448 2194 vl
 4448 2202 vl
 4456 2219 vl
 4465 2227 vl
 4490 2236 vl
 4523 2236 vl
 4548 2227 vl
 4556 2211 vl
 4556 2186 vl
 4548 2169 vl
 4523 2161 vl
 4498 2161 vl
 4523 2236 il
 4540 2227 vl
 4548 2211 vl
 4548 2186 vl
 4540 2169 vl
 4523 2161 vl
 4523 2161 il
 4540 2152 vl
 4556 2136 vl
 4565 2119 vl
 4565 2094 vl
 4556 2077 vl
 4548 2069 vl
 4523 2061 vl
 4490 2061 vl
 4465 2069 vl
 4456 2077 vl
 4448 2094 vl
 4448 2102 vl
 4456 2111 vl
 4465 2102 vl
 4456 2094 vl
 4548 2144 il
 4556 2119 vl
 4556 2094 vl
 4548 2077 vl
 4540 2069 vl
 4523 2061 vl
 4865 2211 il
 4873 2186 vl
 4873 2236 vl
 4865 2211 vl
 4848 2227 vl
 4823 2236 vl
 4806 2236 vl
 4781 2227 vl
 4765 2211 vl
 4756 2194 vl
 4748 2169 vl
 4748 2127 vl
 4756 2102 vl
 4765 2086 vl
 4781 2069 vl
 4806 2061 vl
 4823 2061 vl
 4848 2069 vl
 4865 2086 vl
 4806 2236 il
 4790 2227 vl
 4773 2211 vl
 4765 2194 vl
 4756 2169 vl
 4756 2127 vl
 4765 2102 vl
 4773 2086 vl
 4790 2069 vl
 4806 2061 vl
 4865 2127 il
 4865 2061 vl
 4873 2127 il
 4873 2061 vl
 4840 2127 il
 4898 2127 vl
 4948 2127 il
 5048 2127 vl
 5048 2144 vl
 5040 2161 vl
 5031 2169 vl
 5015 2177 vl
 4990 2177 vl
 4965 2169 vl
 4948 2152 vl
 4940 2127 vl
 4940 2111 vl
 4948 2086 vl
 4965 2069 vl
 4990 2061 vl
 5006 2061 vl
 5031 2069 vl
 5048 2086 vl
 5040 2127 il
 5040 2152 vl
 5031 2169 vl
 4990 2177 il
 4973 2169 vl
 4956 2152 vl
 4948 2127 vl
 4948 2111 vl
 4956 2086 vl
 4973 2069 vl
 4990 2061 vl
 5098 2236 il
 5156 2061 vl
 5106 2236 il
 5156 2086 vl
 5215 2236 il
 5156 2061 vl
 5081 2236 il
 5131 2236 vl
 5181 2236 il
 5231 2236 vl
 4 SLW
 2610 3361 il
 3730 3361 vl
 2610 2961 il
 2690 2961 vl
 2770 2961 il
 2850 2961 vl
 2930 2961 il
 3010 2961 vl
 3090 2961 il
 3170 2961 vl
 3250 2961 il
 3330 2961 vl
 3410 2961 il
 3490 2961 vl
 3570 2961 il
 3650 2961 vl
 4 SLW
 2610 2561 pt
 2708 2561 pt
 2807 2561 pt
 2905 2561 pt
 3003 2561 pt
 3102 2561 pt
 3200 2561 pt
 3299 2561 pt
 3397 2561 pt
 3495 2561 pt
 3594 2561 pt
 3692 2561 pt
 4 SLW
 2610 2161 il
 2708 2161 vl
 2807 2161 pt
 2905 2161 il
 3003 2161 vl
 3102 2161 pt
 3200 2161 il
 3299 2161 vl
 3397 2161 pt
 3495 2161 il
 3594 2161 vl
 3692 2161 pt
 4 SLW
 2130 7200 il
 2130 1601 vl
 9409 1601 vl
 9409 7200 vl
 2130 7200 vl
 4 SLW
 2129 6516 il
 2165 6503 vl
 2202 6491 vl
 2238 6482 vl
 2275 6476 vl
 2275 6476 il
 2311 6473 vl
 2347 6473 vl
 2384 6472 vl
 2420 6468 vl
 2420 6468 il
 2457 6459 vl
 2493 6447 vl
 2529 6435 vl
 2566 6426 vl
 2566 6426 il
 2602 6423 vl
 2639 6422 vl
 2675 6422 vl
 2711 6419 vl
 2711 6419 il
 2748 6413 vl
 2784 6403 vl
 2821 6390 vl
 2857 6376 vl
 2857 6376 il
 2893 6362 vl
 2930 6349 vl
 2966 6338 vl
 3003 6331 vl
 3003 6331 il
 3039 6329 vl
 3076 6328 vl
 3112 6328 vl
 3148 6325 vl
 3148 6325 il
 3185 6318 vl
 3221 6307 vl
 3258 6294 vl
 3294 6278 vl
 3294 6278 il
 3330 6263 vl
 3367 6249 vl
 3403 6237 vl
 3440 6229 vl
 3440 6229 il
 3476 6227 vl
 3512 6228 vl
 3549 6228 vl
 3585 6225 vl
 3585 6225 il
 3622 6216 vl
 3658 6203 vl
 3694 6188 vl
 3731 6173 vl
 3731 6173 il
 3767 6161 vl
 3804 6150 vl
 3840 6141 vl
 3876 6134 vl
 3876 6134 il
 3913 6126 vl
 3949 6118 vl
 3986 6106 vl
 4022 6089 vl
 4022 6089 il
 4058 6067 vl
 4095 6041 vl
 4131 6014 vl
 4168 5991 vl
 4168 5991 il
 4204 5974 vl
 4240 5962 vl
 4277 5952 vl
 4313 5941 vl
 4313 5941 il
 4350 5928 vl
 4386 5914 vl
 4423 5901 vl
 4459 5889 vl
 4459 5889 il
 4495 5879 vl
 4532 5870 vl
 4568 5856 vl
 4605 5836 vl
 4605 5836 il
 4641 5806 vl
 4677 5771 vl
 4714 5737 vl
 4750 5709 vl
 4750 5709 il
 4787 5691 vl
 4823 5678 vl
 4859 5667 vl
 4896 5650 vl
 4896 5650 il
 4932 5624 vl
 4969 5590 vl
 5005 5549 vl
 5041 5504 vl
 5041 5504 il
 5078 5456 vl
 5114 5403 vl
 5151 5340 vl
 5187 5264 vl
 5187 5264 il
 5223 5172 vl
 5260 5063 vl
 5296 4934 vl
 5333 4785 vl
 5333 4785 il
 5369 4617 vl
 5405 4443 vl
 5442 4275 vl
 5478 4129 vl
 5478 4129 il
 5515 4017 vl
 5551 3952 vl
 5587 3942 vl
 5624 3998 vl
 5624 3998 il
 5660 4121 vl
 5697 4268 vl
 5733 4390 vl
 5769 4435 vl
 5769 4435 il
 5806 4366 vl
 5842 4207 vl
 5879 3993 vl
 5915 3762 vl
 5915 3762 il
 5952 3545 vl
 5988 3355 vl
 6024 3195 vl
 6061 3071 vl
 6061 3071 il
 6097 2989 vl
 6134 2952 vl
 6170 2965 vl
 6206 3031 vl
 6206 3031 il
 6243 3151 vl
 6279 3313 vl
 6316 3505 vl
 6352 3711 vl
 6352 3711 il
 6388 3918 vl
 6425 4121 vl
 6461 4313 vl
 6498 4489 vl
 6498 4489 il
 6534 4641 vl
 6570 4760 vl
 6607 4834 vl
 6643 4852 vl
 6643 4852 il
 6680 4810 vl
 6716 4738 vl
 6752 4672 vl
 6789 4651 vl
 6789 4651 il
 6825 4698 vl
 6862 4792 vl
 6898 4899 vl
 6934 4983 vl
 6934 4983 il
 6971 5019 vl
 7007 5011 vl
 7044 4973 vl
 7080 4918 vl
 7080 4918 il
 7116 4858 vl
 7153 4805 vl
 7189 4770 vl
 7226 4764 vl
 7226 4764 il
 7262 4792 vl
 7299 4831 vl
 7335 4851 vl
 7371 4823 vl
 7371 4823 il
 7408 4728 vl
 7444 4598 vl
 7481 4473 vl
 7517 4396 vl
 7517 4396 il
 7553 4395 vl
 7590 4448 vl
 7626 4519 vl
 7663 4573 vl
 7663 4573 il
 7699 4582 vl
 7735 4555 vl
 7772 4510 vl
 7808 4465 vl
 7808 4465 il
 7845 4435 vl
 7881 4428 vl
 7917 4447 vl
 7954 4498 vl
 7954 4498 il
 7990 4579 vl
 8027 4670 vl
 8063 4746 vl
 8099 4779 vl
 8099 4779 il
 8136 4753 vl
 8172 4692 vl
 8209 4627 vl
 8245 4591 vl
 8245 4591 il
 8281 4604 vl
 8318 4647 vl
 8354 4687 vl
 8391 4693 vl
 8391 4693 il
 8427 4642 vl
 8463 4549 vl
 8500 4437 vl
 8536 4329 vl
 8536 4329 il
 8573 4246 vl
 8609 4196 vl
 8645 4188 vl
 8682 4229 vl
 8682 4229 il
 8718 4324 vl
 8755 4477 vl
 8791 4692 vl
 8828 4971 vl
 8828 4971 il
 8864 5312 vl
 8900 5694 vl
 8937 6091 vl
 8973 6477 vl
 8973 6477 il
 9010 6831 vl
 9046 7158 vl
 9051 7201 vl
 4 SLW
 2420 1600 il
 2420 1680 vl
 2711 1600 il
 2711 1680 vl
 3003 1600 il
 3003 1680 vl
 3294 1600 il
 3294 1680 vl
 3585 1600 il
 3585 1840 vl
 3876 1600 il
 3876 1680 vl
 4168 1600 il
 4168 1680 vl
 4459 1600 il
 4459 1680 vl
 4750 1600 il
 4750 1680 vl
 5041 1600 il
 5041 1840 vl
 5333 1600 il
 5333 1680 vl
 5624 1600 il
 5624 1680 vl
 5915 1600 il
 5915 1680 vl
 6206 1600 il
 6206 1680 vl
 6498 1600 il
 6498 1840 vl
 6789 1600 il
 6789 1680 vl
 7080 1600 il
 7080 1680 vl
 7371 1600 il
 7371 1680 vl
 7663 1600 il
 7663 1680 vl
 7954 1600 il
 7954 1840 vl
 8245 1600 il
 8245 1680 vl
 8536 1600 il
 8536 1680 vl
 8828 1600 il
 8828 1680 vl
 9119 1600 il
 9119 1680 vl
 9410 1600 il
 9410 1840 vl
 4 SLW
 2011 1469 il
 1998 1402 vl
 1998 1402 il
 2011 1415 vl
 2031 1422 vl
 2051 1422 vl
 2071 1415 vl
 2084 1402 vl
 2091 1382 vl
 2091 1369 vl
 2084 1349 vl
 2071 1336 vl
 2051 1329 vl
 2031 1329 vl
 2011 1336 vl
 2004 1342 vl
 1998 1355 vl
 1998 1362 vl
 2004 1369 vl
 2011 1362 vl
 2004 1355 vl
 2051 1422 il
 2064 1415 vl
 2078 1402 vl
 2084 1382 vl
 2084 1369 vl
 2078 1349 vl
 2064 1336 vl
 2051 1329 vl
 2011 1469 il
 2078 1469 vl
 2011 1462 il
 2044 1462 vl
 2078 1469 vl
 2144 1469 il
 2131 1402 vl
 2131 1402 il
 2144 1415 vl
 2164 1422 vl
 2184 1422 vl
 2204 1415 vl
 2218 1402 vl
 2224 1382 vl
 2224 1369 vl
 2218 1349 vl
 2204 1336 vl
 2184 1329 vl
 2164 1329 vl
 2144 1336 vl
 2138 1342 vl
 2131 1355 vl
 2131 1362 vl
 2138 1369 vl
 2144 1362 vl
 2138 1355 vl
 2184 1422 il
 2198 1415 vl
 2211 1402 vl
 2218 1382 vl
 2218 1369 vl
 2211 1349 vl
 2198 1336 vl
 2184 1329 vl
 2144 1469 il
 2211 1469 vl
 2144 1462 il
 2178 1462 vl
 2211 1469 vl
 3467 1469 il
 3454 1402 vl
 3454 1402 il
 3467 1415 vl
 3487 1422 vl
 3507 1422 vl
 3527 1415 vl
 3540 1402 vl
 3547 1382 vl
 3547 1369 vl
 3540 1349 vl
 3527 1336 vl
 3507 1329 vl
 3487 1329 vl
 3467 1336 vl
 3460 1342 vl
 3454 1355 vl
 3454 1362 vl
 3460 1369 vl
 3467 1362 vl
 3460 1355 vl
 3507 1422 il
 3520 1415 vl
 3534 1402 vl
 3540 1382 vl
 3540 1369 vl
 3534 1349 vl
 3520 1336 vl
 3507 1329 vl
 3467 1469 il
 3534 1469 vl
 3467 1462 il
 3500 1462 vl
 3534 1469 vl
 3667 1449 il
 3660 1442 vl
 3667 1435 vl
 3674 1442 vl
 3674 1449 vl
 3667 1462 vl
 3654 1469 vl
 3634 1469 vl
 3614 1462 vl
 3600 1449 vl
 3594 1435 vl
 3587 1409 vl
 3587 1369 vl
 3594 1349 vl
 3607 1336 vl
 3627 1329 vl
 3640 1329 vl
 3660 1336 vl
 3674 1349 vl
 3680 1369 vl
 3680 1375 vl
 3674 1395 vl
 3660 1409 vl
 3640 1415 vl
 3634 1415 vl
 3614 1409 vl
 3600 1395 vl
 3594 1375 vl
 3634 1469 il
 3620 1462 vl
 3607 1449 vl
 3600 1435 vl
 3594 1409 vl
 3594 1369 vl
 3600 1349 vl
 3614 1336 vl
 3627 1329 vl
 3640 1329 il
 3654 1336 vl
 3667 1349 vl
 3674 1369 vl
 3674 1375 vl
 3667 1395 vl
 3654 1409 vl
 3640 1415 vl
 4923 1469 il
 4910 1402 vl
 4910 1402 il
 4923 1415 vl
 4943 1422 vl
 4963 1422 vl
 4983 1415 vl
 4996 1402 vl
 5003 1382 vl
 5003 1369 vl
 4996 1349 vl
 4983 1336 vl
 4963 1329 vl
 4943 1329 vl
 4923 1336 vl
 4916 1342 vl
 4910 1355 vl
 4910 1362 vl
 4916 1369 vl
 4923 1362 vl
 4916 1355 vl
 4963 1422 il
 4976 1415 vl
 4990 1402 vl
 4996 1382 vl
 4996 1369 vl
 4990 1349 vl
 4976 1336 vl
 4963 1329 vl
 4923 1469 il
 4990 1469 vl
 4923 1462 il
 4956 1462 vl
 4990 1469 vl
 5043 1469 il
 5043 1429 vl
 5043 1442 il
 5050 1455 vl
 5063 1469 vl
 5076 1469 vl
 5110 1449 vl
 5123 1449 vl
 5130 1455 vl
 5136 1469 vl
 5050 1455 il
 5063 1462 vl
 5076 1462 vl
 5110 1449 vl
 5136 1469 il
 5136 1449 vl
 5130 1429 vl
 5103 1395 vl
 5096 1382 vl
 5090 1362 vl
 5090 1329 vl
 5130 1429 il
 5096 1395 vl
 5090 1382 vl
 5083 1362 vl
 5083 1329 vl
 6379 1469 il
 6365 1402 vl
 6365 1402 il
 6379 1415 vl
 6399 1422 vl
 6419 1422 vl
 6439 1415 vl
 6452 1402 vl
 6459 1382 vl
 6459 1369 vl
 6452 1349 vl
 6439 1336 vl
 6419 1329 vl
 6399 1329 vl
 6379 1336 vl
 6372 1342 vl
 6365 1355 vl
 6365 1362 vl
 6372 1369 vl
 6379 1362 vl
 6372 1355 vl
 6419 1422 il
 6432 1415 vl
 6445 1402 vl
 6452 1382 vl
 6452 1369 vl
 6445 1349 vl
 6432 1336 vl
 6419 1329 vl
 6379 1469 il
 6445 1469 vl
 6379 1462 il
 6412 1462 vl
 6445 1469 vl
 6532 1469 il
 6512 1462 vl
 6505 1449 vl
 6505 1429 vl
 6512 1415 vl
 6532 1409 vl
 6559 1409 vl
 6579 1415 vl
 6585 1429 vl
 6585 1449 vl
 6579 1462 vl
 6559 1469 vl
 6532 1469 vl
 6532 1469 il
 6519 1462 vl
 6512 1449 vl
 6512 1429 vl
 6519 1415 vl
 6532 1409 vl
 6559 1409 il
 6572 1415 vl
 6579 1429 vl
 6579 1449 vl
 6572 1462 vl
 6559 1469 vl
 6532 1409 il
 6512 1402 vl
 6505 1395 vl
 6499 1382 vl
 6499 1355 vl
 6505 1342 vl
 6512 1336 vl
 6532 1329 vl
 6559 1329 vl
 6579 1336 vl
 6585 1342 vl
 6592 1355 vl
 6592 1382 vl
 6585 1395 vl
 6579 1402 vl
 6559 1409 vl
 6532 1409 il
 6519 1402 vl
 6512 1395 vl
 6505 1382 vl
 6505 1355 vl
 6512 1342 vl
 6519 1336 vl
 6532 1329 vl
 6559 1329 il
 6572 1336 vl
 6579 1342 vl
 6585 1355 vl
 6585 1382 vl
 6579 1395 vl
 6572 1402 vl
 6559 1409 vl
 7835 1469 il
 7821 1402 vl
 7821 1402 il
 7835 1415 vl
 7855 1422 vl
 7875 1422 vl
 7895 1415 vl
 7908 1402 vl
 7915 1382 vl
 7915 1369 vl
 7908 1349 vl
 7895 1336 vl
 7875 1329 vl
 7855 1329 vl
 7835 1336 vl
 7828 1342 vl
 7821 1355 vl
 7821 1362 vl
 7828 1369 vl
 7835 1362 vl
 7828 1355 vl
 7875 1422 il
 7888 1415 vl
 7901 1402 vl
 7908 1382 vl
 7908 1369 vl
 7901 1349 vl
 7888 1336 vl
 7875 1329 vl
 7835 1469 il
 7901 1469 vl
 7835 1462 il
 7868 1462 vl
 7901 1469 vl
 8041 1422 il
 8035 1402 vl
 8021 1389 vl
 8001 1382 vl
 7995 1382 vl
 7975 1389 vl
 7961 1402 vl
 7955 1422 vl
 7955 1429 vl
 7961 1449 vl
 7975 1462 vl
 7995 1469 vl
 8008 1469 vl
 8028 1462 vl
 8041 1449 vl
 8048 1429 vl
 8048 1389 vl
 8041 1362 vl
 8035 1349 vl
 8021 1336 vl
 8001 1329 vl
 7981 1329 vl
 7968 1336 vl
 7961 1349 vl
 7961 1355 vl
 7968 1362 vl
 7975 1355 vl
 7968 1349 vl
 7995 1382 il
 7981 1389 vl
 7968 1402 vl
 7961 1422 vl
 7961 1429 vl
 7968 1449 vl
 7981 1462 vl
 7995 1469 vl
 8008 1469 il
 8021 1462 vl
 8035 1449 vl
 8041 1429 vl
 8041 1389 vl
 8035 1362 vl
 8028 1349 vl
 8015 1336 vl
 8001 1329 vl
 9357 1449 il
 9350 1442 vl
 9357 1435 vl
 9364 1442 vl
 9364 1449 vl
 9357 1462 vl
 9344 1469 vl
 9324 1469 vl
 9304 1462 vl
 9290 1449 vl
 9284 1435 vl
 9277 1409 vl
 9277 1369 vl
 9284 1349 vl
 9297 1336 vl
 9317 1329 vl
 9330 1329 vl
 9350 1336 vl
 9364 1349 vl
 9370 1369 vl
 9370 1375 vl
 9364 1395 vl
 9350 1409 vl
 9330 1415 vl
 9324 1415 vl
 9304 1409 vl
 9290 1395 vl
 9284 1375 vl
 9324 1469 il
 9310 1462 vl
 9297 1449 vl
 9290 1435 vl
 9284 1409 vl
 9284 1369 vl
 9290 1349 vl
 9304 1336 vl
 9317 1329 vl
 9330 1329 il
 9344 1336 vl
 9357 1349 vl
 9364 1369 vl
 9364 1375 vl
 9357 1395 vl
 9344 1409 vl
 9330 1415 vl
 9450 1469 il
 9430 1462 vl
 9417 1442 vl
 9410 1409 vl
 9410 1389 vl
 9417 1355 vl
 9430 1336 vl
 9450 1329 vl
 9464 1329 vl
 9484 1336 vl
 9497 1355 vl
 9504 1389 vl
 9504 1409 vl
 9497 1442 vl
 9484 1462 vl
 9464 1469 vl
 9450 1469 vl
 9450 1469 il
 9437 1462 vl
 9430 1455 vl
 9424 1442 vl
 9417 1409 vl
 9417 1389 vl
 9424 1355 vl
 9430 1342 vl
 9437 1336 vl
 9450 1329 vl
 9464 1329 il
 9477 1336 vl
 9484 1342 vl
 9490 1355 vl
 9497 1389 vl
 9497 1409 vl
 9490 1442 vl
 9484 1455 vl
 9477 1462 vl
 9464 1469 vl
 4 SLW
 2420 7121 il
 2420 7201 vl
 2711 7121 il
 2711 7201 vl
 3003 7121 il
 3003 7201 vl
 3294 7121 il
 3294 7201 vl
 3585 6961 il
 3585 7201 vl
 3876 7121 il
 3876 7201 vl
 4168 7121 il
 4168 7201 vl
 4459 7121 il
 4459 7201 vl
 4750 7121 il
 4750 7201 vl
 5041 6961 il
 5041 7201 vl
 5333 7121 il
 5333 7201 vl
 5624 7121 il
 5624 7201 vl
 5915 7121 il
 5915 7201 vl
 6206 7121 il
 6206 7201 vl
 6498 6961 il
 6498 7201 vl
 6789 7121 il
 6789 7201 vl
 7080 7121 il
 7080 7201 vl
 7371 7121 il
 7371 7201 vl
 7663 7121 il
 7663 7201 vl
 7954 6961 il
 7954 7201 vl
 8245 7121 il
 8245 7201 vl
 8536 7121 il
 8536 7201 vl
 8828 7121 il
 8828 7201 vl
 9119 7121 il
 9119 7201 vl
 9410 6961 il
 9410 7201 vl
 4 SLW
 2129 1600 il
 2369 1600 vl
 2129 2162 il
 2209 2162 vl
 2129 2491 il
 2209 2491 vl
 2129 2724 il
 2209 2724 vl
 2129 2905 il
 2209 2905 vl
 2129 3053 il
 2209 3053 vl
 2129 3178 il
 2209 3178 vl
 2129 3286 il
 2209 3286 vl
 2129 3382 il
 2209 3382 vl
 2129 3467 il
 2369 3467 vl
 2129 4029 il
 2209 4029 vl
 2129 4358 il
 2209 4358 vl
 2129 4591 il
 2209 4591 vl
 2129 4772 il
 2209 4772 vl
 2129 4920 il
 2209 4920 vl
 2129 5045 il
 2209 5045 vl
 2129 5153 il
 2209 5153 vl
 2129 5249 il
 2209 5249 vl
 2129 5334 il
 2369 5334 vl
 2129 5896 il
 2209 5896 vl
 2129 6225 il
 2209 6225 vl
 2129 6458 il
 2209 6458 vl
 2129 6639 il
 2209 6639 vl
 2129 6787 il
 2209 6787 vl
 2129 6912 il
 2209 6912 vl
 2129 7020 il
 2209 7020 vl
 2129 7116 il
 2209 7116 vl
 2129 7201 il
 2369 7201 vl
 4 SLW
 1370 1634 il
 1383 1641 vl
 1403 1661 vl
 1403 1521 vl
 1397 1654 il
 1397 1521 vl
 1370 1521 il
 1430 1521 vl
 1523 1661 il
 1503 1654 vl
 1490 1634 vl
 1483 1601 vl
 1483 1581 vl
 1490 1547 vl
 1503 1527 vl
 1523 1521 vl
 1537 1521 vl
 1557 1527 vl
 1570 1547 vl
 1577 1581 vl
 1577 1601 vl
 1570 1634 vl
 1557 1654 vl
 1537 1661 vl
 1523 1661 vl
 1523 1661 il
 1510 1654 vl
 1503 1647 vl
 1497 1634 vl
 1490 1601 vl
 1490 1581 vl
 1497 1547 vl
 1503 1534 vl
 1510 1527 vl
 1523 1521 vl
 1537 1521 il
 1550 1527 vl
 1557 1534 vl
 1563 1547 vl
 1570 1581 vl
 1570 1601 vl
 1563 1634 vl
 1557 1647 vl
 1550 1654 vl
 1537 1661 vl
 1623 1661 il
 1743 1661 vl
 1810 1714 il
 1823 1721 vl
 1843 1741 vl
 1843 1601 vl
 1836 1734 il
 1836 1601 vl
 1810 1601 il
 1870 1601 vl
 1514 3501 il
 1527 3507 vl
 1547 3527 vl
 1547 3387 vl
 1541 3521 il
 1541 3387 vl
 1514 3387 il
 1574 3387 vl
 1667 3527 il
 1647 3521 vl
 1634 3501 vl
 1627 3467 vl
 1627 3447 vl
 1634 3414 vl
 1647 3394 vl
 1667 3387 vl
 1681 3387 vl
 1701 3394 vl
 1714 3414 vl
 1720 3447 vl
 1720 3467 vl
 1714 3501 vl
 1701 3521 vl
 1681 3527 vl
 1667 3527 vl
 1667 3527 il
 1654 3521 vl
 1647 3514 vl
 1641 3501 vl
 1634 3467 vl
 1634 3447 vl
 1641 3414 vl
 1647 3401 vl
 1654 3394 vl
 1667 3387 vl
 1681 3387 il
 1694 3394 vl
 1701 3401 vl
 1707 3414 vl
 1714 3447 vl
 1714 3467 vl
 1707 3501 vl
 1701 3514 vl
 1694 3521 vl
 1681 3527 vl
 1800 3607 il
 1780 3601 vl
 1767 3581 vl
 1760 3547 vl
 1760 3527 vl
 1767 3494 vl
 1780 3474 vl
 1800 3467 vl
 1814 3467 vl
 1834 3474 vl
 1847 3494 vl
 1854 3527 vl
 1854 3547 vl
 1847 3581 vl
 1834 3601 vl
 1814 3607 vl
 1800 3607 vl
 1800 3607 il
 1787 3601 vl
 1780 3594 vl
 1774 3581 vl
 1767 3547 vl
 1767 3527 vl
 1774 3494 vl
 1780 3481 vl
 1787 3474 vl
 1800 3467 vl
 1814 3467 il
 1827 3474 vl
 1834 3481 vl
 1840 3494 vl
 1847 3527 vl
 1847 3547 vl
 1840 3581 vl
 1834 3594 vl
 1827 3601 vl
 1814 3607 vl
 1514 5367 il
 1527 5374 vl
 1547 5394 vl
 1547 5254 vl
 1541 5387 il
 1541 5254 vl
 1514 5254 il
 1574 5254 vl
 1667 5394 il
 1647 5387 vl
 1634 5367 vl
 1627 5334 vl
 1627 5314 vl
 1634 5280 vl
 1647 5260 vl
 1667 5254 vl
 1681 5254 vl
 1701 5260 vl
 1714 5280 vl
 1720 5314 vl
 1720 5334 vl
 1714 5367 vl
 1701 5387 vl
 1681 5394 vl
 1667 5394 vl
 1667 5394 il
 1654 5387 vl
 1647 5380 vl
 1641 5367 vl
 1634 5334 vl
 1634 5314 vl
 1641 5280 vl
 1647 5267 vl
 1654 5260 vl
 1667 5254 vl
 1681 5254 il
 1694 5260 vl
 1701 5267 vl
 1707 5280 vl
 1714 5314 vl
 1714 5334 vl
 1707 5367 vl
 1701 5380 vl
 1694 5387 vl
 1681 5394 vl
 1780 5447 il
 1794 5454 vl
 1814 5474 vl
 1814 5334 vl
 1807 5467 il
 1807 5334 vl
 1780 5334 il
 1840 5334 vl
 1514 7233 il
 1527 7240 vl
 1547 7260 vl
 1547 7120 vl
 1541 7253 il
 1541 7120 vl
 1514 7120 il
 1574 7120 vl
 1667 7260 il
 1647 7253 vl
 1634 7233 vl
 1627 7200 vl
 1627 7180 vl
 1634 7147 vl
 1647 7127 vl
 1667 7120 vl
 1681 7120 vl
 1701 7127 vl
 1714 7147 vl
 1720 7180 vl
 1720 7200 vl
 1714 7233 vl
 1701 7253 vl
 1681 7260 vl
 1667 7260 vl
 1667 7260 il
 1654 7253 vl
 1647 7247 vl
 1641 7233 vl
 1634 7200 vl
 1634 7180 vl
 1641 7147 vl
 1647 7133 vl
 1654 7127 vl
 1667 7120 vl
 1681 7120 il
 1694 7127 vl
 1701 7133 vl
 1707 7147 vl
 1714 7180 vl
 1714 7200 vl
 1707 7233 vl
 1701 7247 vl
 1694 7253 vl
 1681 7260 vl
 1767 7313 il
 1774 7307 vl
 1767 7300 vl
 1760 7307 vl
 1760 7313 vl
 1767 7327 vl
 1774 7333 vl
 1794 7340 vl
 1820 7340 vl
 1840 7333 vl
 1847 7327 vl
 1854 7313 vl
 1854 7300 vl
 1847 7287 vl
 1827 7273 vl
 1794 7260 vl
 1780 7253 vl
 1767 7240 vl
 1760 7220 vl
 1760 7200 vl
 1820 7340 il
 1834 7333 vl
 1840 7327 vl
 1847 7313 vl
 1847 7300 vl
 1840 7287 vl
 1820 7273 vl
 1794 7260 vl
 1760 7213 il
 1767 7220 vl
 1780 7220 vl
 1814 7207 vl
 1834 7207 vl
 1847 7213 vl
 1854 7220 vl
 1780 7220 il
 1814 7200 vl
 1840 7200 vl
 1847 7207 vl
 1854 7220 vl
 1854 7233 vl
 4 SLW
 9170 1600 il
 9410 1600 vl
 9330 2162 il
 9410 2162 vl
 9330 2491 il
 9410 2491 vl
 9330 2724 il
 9410 2724 vl
 9330 2905 il
 9410 2905 vl
 9330 3053 il
 9410 3053 vl
 9330 3178 il
 9410 3178 vl
 9330 3286 il
 9410 3286 vl
 9330 3382 il
 9410 3382 vl
 9170 3467 il
 9410 3467 vl
 9330 4029 il
 9410 4029 vl
 9330 4358 il
 9410 4358 vl
 9330 4591 il
 9410 4591 vl
 9330 4772 il
 9410 4772 vl
 9330 4920 il
 9410 4920 vl
 9330 5045 il
 9410 5045 vl
 9330 5153 il
 9410 5153 vl
 9330 5249 il
 9410 5249 vl
 9170 5334 il
 9410 5334 vl
 9330 5896 il
 9410 5896 vl
 9330 6225 il
 9410 6225 vl
 9330 6458 il
 9410 6458 vl
 9330 6639 il
 9410 6639 vl
 9330 6787 il
 9410 6787 vl
 9330 6912 il
 9410 6912 vl
 9330 7020 il
 9410 7020 vl
 9330 7116 il
 9410 7116 vl
 9170 7201 il
 9410 7201 vl
 4 SLW
 2129 6451 il
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 4 SLW
 4791 5515 il
 4791 5340 vl
 4800 5515 il
 4800 5340 vl
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 4825 5515 vl
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 4 SLW
 4833 5115 il
 4808 5107 vl
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 4 SLW
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 4 SLW
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 4 SLW
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 3849 2324 vl
 3853 2324 vl
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 4 SLW
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 4 SLW
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 4859 1600 il
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 6680 1600 il
 6680 1840 vl
 7590 1600 il
 7590 1840 vl
 8500 1600 il
 8500 1840 vl
 9410 1600 il
 9410 1840 vl
 4 SLW
 1874 1442 il
 1887 1449 vl
 1907 1469 vl
 1907 1329 vl
 1900 1462 il
 1900 1329 vl
 1874 1329 il
 1934 1329 vl
 2027 1469 il
 2007 1462 vl
 1994 1442 vl
 1987 1409 vl
 1987 1389 vl
 1994 1355 vl
 2007 1335 vl
 2027 1329 vl
 2040 1329 vl
 2060 1335 vl
 2074 1355 vl
 2080 1389 vl
 2080 1409 vl
 2074 1442 vl
 2060 1462 vl
 2040 1469 vl
 2027 1469 vl
 2027 1469 il
 2014 1462 vl
 2007 1455 vl
 2000 1442 vl
 1994 1409 vl
 1994 1389 vl
 2000 1355 vl
 2007 1342 vl
 2014 1335 vl
 2027 1329 vl
 2040 1329 il
 2054 1335 vl
 2060 1342 vl
 2067 1355 vl
 2074 1389 vl
 2074 1409 vl
 2067 1442 vl
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 2040 1469 vl
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 2784 1442 il
 2797 1449 vl
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 2810 1329 vl
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 2844 1329 vl
 2937 1469 il
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 3110 1409 vl
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 3707 1449 vl
 3727 1469 vl
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 3894 1355 vl
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 4 SLW
 2129 6961 il
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 4 SLW
 2129 2300 il
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 4 SLW
 1514 1634 il
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 1807 5940 il
 1794 5934 vl
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 1767 5880 vl
 1767 5840 vl
 1774 5820 vl
 1787 5807 vl
 1800 5800 vl
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 1827 5807 vl
 1840 5820 vl
 1847 5840 vl
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 1827 5880 vl
 1814 5887 vl
 1514 6534 il
 1527 6540 vl
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 1541 6420 vl
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 1574 6420 vl
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 1714 6447 vl
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 1667 6560 vl
 1667 6560 il
 1654 6554 vl
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 1647 6434 vl
 1654 6427 vl
 1667 6420 vl
 1681 6420 il
 1694 6427 vl
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 1707 6447 vl
 1714 6480 vl
 1714 6500 vl
 1707 6534 vl
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 1694 6554 vl
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 1854 6640 vl
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 1854 6640 il
 1854 6620 vl
 1847 6600 vl
 1820 6567 vl
 1814 6554 vl
 1807 6534 vl
 1807 6500 vl
 1847 6600 il
 1814 6567 vl
 1807 6554 vl
 1800 6534 vl
 1800 6500 vl
 1514 7233 il
 1527 7240 vl
 1547 7260 vl
 1547 7120 vl
 1541 7253 il
 1541 7120 vl
 1514 7120 il
 1574 7120 vl
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 1647 7253 vl
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 1667 7120 vl
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 1714 7147 vl
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 1701 7253 vl
 1681 7260 vl
 1667 7260 vl
 1667 7260 il
 1654 7253 vl
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 1641 7233 vl
 1634 7200 vl
 1634 7180 vl
 1641 7147 vl
 1647 7133 vl
 1654 7127 vl
 1667 7120 vl
 1681 7120 il
 1694 7127 vl
 1701 7133 vl
 1707 7147 vl
 1714 7180 vl
 1714 7200 vl
 1707 7233 vl
 1701 7247 vl
 1694 7253 vl
 1681 7260 vl
 1794 7340 il
 1774 7333 vl
 1767 7320 vl
 1767 7300 vl
 1774 7287 vl
 1794 7280 vl
 1820 7280 vl
 1840 7287 vl
 1847 7300 vl
 1847 7320 vl
 1840 7333 vl
 1820 7340 vl
 1794 7340 vl
 1794 7340 il
 1781 7333 vl
 1774 7320 vl
 1774 7300 vl
 1781 7287 vl
 1794 7280 vl
 1820 7280 il
 1834 7287 vl
 1840 7300 vl
 1840 7320 vl
 1834 7333 vl
 1820 7340 vl
 1794 7280 il
 1774 7273 vl
 1767 7267 vl
 1761 7253 vl
 1761 7227 vl
 1767 7213 vl
 1774 7207 vl
 1794 7200 vl
 1820 7200 vl
 1840 7207 vl
 1847 7213 vl
 1854 7227 vl
 1854 7253 vl
 1847 7267 vl
 1840 7273 vl
 1820 7280 vl
 1794 7280 il
 1781 7273 vl
 1774 7267 vl
 1767 7253 vl
 1767 7227 vl
 1774 7213 vl
 1781 7207 vl
 1794 7200 vl
 1820 7200 il
 1834 7207 vl
 1840 7213 vl
 1847 7227 vl
 1847 7253 vl
 1840 7267 vl
 1834 7273 vl
 1820 7280 vl
 4 SLW
 9170 2300 il
 9410 2300 vl
 9170 3000 il
 9410 3000 vl
 9170 3700 il
 9410 3700 vl
 9170 4400 il
 9410 4400 vl
 9170 5101 il
 9410 5101 vl
 9170 5801 il
 9410 5801 vl
 9170 6501 il
 9410 6501 vl
 9170 7201 il
 9410 7201 vl
 4 SLW
 8378 1600 il
 8378 1601 vl
 8378 1620 vl
 8378 1700 il
 8378 1776 vl
 8378 1780 vl
 8378 1860 il
 8378 1940 vl
 8378 2020 il
 8378 2100 vl
 8378 2180 il
 8378 2260 vl
 8378 2340 il
 8378 2420 vl
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 8378 2580 vl
 8378 2660 il
 8378 2740 vl
 8378 2820 il
 8378 2827 vl
 8378 2900 vl
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 8378 3002 vl
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 8378 3177 vl
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 8378 3528 vl
 8378 3540 vl
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 8378 3860 vl
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 8376 4180 vl
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 8376 4340 vl
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 8375 4430 vl
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 8374 4794 vl
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 8364 5220 il
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 8361 5300 vl
 8361 5300 vl
 8355 5380 il
 8355 5381 vl
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 8353 5407 vl
 8352 5414 vl
 8351 5421 vl
 8351 5428 vl
 8350 5434 vl
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 8339 5539 il
 8339 5542 vl
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 8333 5569 vl
 8333 5576 vl
 8332 5583 vl
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 8330 5596 vl
 8329 5603 vl
 8327 5610 vl
 8326 5616 vl
 8326 5618 vl
 8310 5696 il
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 8300 5731 vl
 8299 5738 vl
 8298 5744 vl
 8296 5751 vl
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 8288 5771 vl
 8287 5773 vl
 8258 5847 il
 8256 5852 vl
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 8242 5879 vl
 8239 5886 vl
 8235 5893 vl
 8232 5899 vl
 8229 5906 vl
 8225 5913 vl
 8222 5918 vl
 8173 5982 il
 8168 5987 vl
 8162 5994 vl
 8156 6000 vl
 8150 6007 vl
 8144 6014 vl
 8138 6021 vl
 8131 6028 vl
 8123 6035 vl
 8118 6039 vl
 4 SLW
 8055 6089 il
 8046 6095 vl
 8037 6101 vl
 8027 6108 vl
 8016 6115 vl
 8006 6122 vl
 7996 6128 vl
 7988 6133 vl
 7919 6173 il
 7915 6176 vl
 7903 6182 vl
 7891 6189 vl
 7878 6196 vl
 7866 6203 vl
 7854 6209 vl
 7849 6212 vl
 4 SLW
 2179 6657 il
 2259 6657 vl
 2339 6657 il
 2419 6657 vl
 2499 6657 il
 2579 6657 vl
 2659 6657 il
 2737 6657 vl
 2739 6657 vl
 2819 6657 il
 2899 6657 vl
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 3041 6657 vl
 3059 6657 vl
 3139 6657 il
 3219 6657 vl
 3299 6657 il
 3344 6657 vl
 3379 6657 vl
 3459 6657 il
 3539 6657 vl
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 3648 6657 vl
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 3859 6657 vl
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 3952 6657 vl
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 4339 6657 vl
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 4819 6657 vl
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 5073 6657 vl
 5139 6657 vl
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 5283 6656 vl
 5299 6656 vl
 5379 6656 il
 5459 6655 vl
 5539 6654 il
 5587 6654 vl
 5619 6654 vl
 5699 6653 il
 5773 6653 vl
 5779 6653 vl
 5859 6653 il
 5867 6653 vl
 5879 6653 vl
 5890 6653 vl
 5902 6653 vl
 5914 6653 vl
 5925 6653 vl
 5937 6653 vl
 5940 6653 vl
 6019 6651 il
 6030 6651 vl
 6042 6651 vl
 6054 6651 vl
 6065 6651 vl
 6077 6651 vl
 6089 6651 vl
 6099 6650 vl
 6179 6647 il
 6182 6647 vl
 6194 6647 vl
 6206 6647 vl
 6217 6647 vl
 6229 6647 vl
 6241 6647 vl
 6252 6647 vl
 6259 6647 vl
 6339 6644 il
 6346 6644 vl
 6357 6643 vl
 6369 6642 vl
 6381 6642 vl
 6392 6641 vl
 6404 6640 vl
 6416 6640 vl
 6419 6640 vl
 6499 6637 il
 6509 6636 vl
 6521 6635 vl
 6533 6635 vl
 6544 6634 vl
 6556 6633 vl
 6568 6632 vl
 6579 6632 vl
 6659 6627 il
 6661 6627 vl
 6673 6626 vl
 6684 6625 vl
 6696 6624 vl
 6708 6623 vl
 6719 6621 vl
 6731 6621 vl
 6738 6620 vl
 6818 6612 il
 6824 6611 vl
 6836 6609 vl
 6848 6608 vl
 6860 6607 vl
 6871 6605 vl
 6883 6604 vl
 6895 6602 vl
 6897 6602 vl
 6976 6588 il
 6976 6588 vl
 6988 6586 vl
 7000 6583 vl
 7011 6581 vl
 7023 6579 vl
 7035 6577 vl
 7046 6575 vl
 7055 6574 vl
 7133 6556 il
 7140 6554 vl
 7152 6551 vl
 7163 6547 vl
 7175 6544 vl
 7187 6540 vl
 7198 6537 vl
 7210 6533 vl
 7285 6508 il
 7292 6505 vl
 7303 6500 vl
 7315 6495 vl
 7327 6490 vl
 7338 6485 vl
 7350 6481 vl
 7359 6477 vl
 7432 6443 il
 7443 6438 vl
 7455 6432 vl
 7467 6426 vl
 4 SLW
 7467 6426 il
 7479 6420 vl
 7490 6413 vl
 7502 6407 vl
 7503 6407 vl
 7573 6368 il
 7584 6362 vl
 7595 6355 vl
 7607 6348 vl
 7619 6342 vl
 7630 6336 vl
 7642 6329 vl
 7642 6328 vl
 7711 6287 il
 7712 6287 vl
 7724 6281 vl
 7735 6275 vl
 7747 6268 vl
 7759 6262 vl
 7770 6256 vl
 7782 6250 vl
 4 SLW
 6752 1600 il
 6752 1614 vl
 6752 1635 vl
 6752 1656 vl
 6752 1677 vl
 6752 1698 vl
 6752 1698 vl
 6752 1797 pt
 6752 1895 il
 6752 1908 vl
 6752 1929 vl
 6752 1950 vl
 6752 1971 vl
 6752 1992 vl
 6752 1994 vl
 6752 2092 pt
 6752 2191 il
 6752 2202 vl
 6752 2223 vl
 6752 2244 vl
 6752 2265 vl
 6752 2286 vl
 6752 2289 vl
 6752 2388 pt
 6752 2486 il
 6752 2496 vl
 6752 2517 vl
 6752 2538 vl
 6752 2559 vl
 6752 2580 vl
 6752 2584 vl
 6752 2683 pt
 6752 2781 il
 6752 2790 vl
 6752 2811 vl
 6752 2832 vl
 6752 2853 vl
 6752 2874 vl
 6752 2880 vl
 6752 2978 pt
 6752 3077 il
 6752 3084 vl
 6752 3105 vl
 6752 3126 vl
 6752 3147 vl
 6752 3168 vl
 6752 3175 vl
 6752 3274 pt
 6752 3372 il
 6752 3378 vl
 6752 3399 vl
 6752 3420 vl
 6752 3441 vl
 6752 3462 vl
 6752 3470 vl
 6752 3569 pt
 6752 3667 il
 6752 3672 vl
 6752 3693 vl
 6752 3714 vl
 6752 3735 vl
 6752 3756 vl
 6752 3766 vl
 6754 3864 pt
 6754 3963 il
 6754 3966 vl
 6754 3987 vl
 6754 4008 vl
 6754 4029 vl
 6754 4050 vl
 6754 4061 vl
 6756 4159 pt
 6757 4258 il
 6757 4260 vl
 6757 4281 vl
 6757 4302 vl
 6758 4323 vl
 6759 4344 vl
 6759 4356 vl
 6761 4455 pt
 6765 4553 il
 6765 4555 vl
 6766 4576 vl
 6767 4597 vl
 6768 4618 vl
 6769 4639 vl
 6769 4651 vl
 6776 4749 pt
 6782 4848 il
 6782 4849 vl
 6784 4870 vl
 6787 4891 vl
 6790 4912 vl
 6792 4933 vl
 6794 4945 vl
 6804 5043 pt
 6820 5141 il
 6820 5143 vl
 6822 5164 vl
 6825 5185 vl
 6829 5206 vl
 6833 5227 vl
 6834 5238 vl
 6851 5335 pt
 6868 5432 il
 6869 5437 vl
 6873 5458 vl
 6876 5479 vl
 6880 5500 vl
 6883 5521 vl
 6884 5529 vl
 6894 5627 pt
 6897 5725 il
 6897 5731 vl
 6896 5752 vl
 6895 5773 vl
 6892 5794 vl
 6888 5815 vl
 6886 5823 vl
 6862 5918 pt
 4 SLW
 6820 6004 il
 6806 6025 vl
 6792 6046 vl
 6776 6067 vl
 6762 6084 vl
 6697 6157 pt
 6626 6226 il
 6616 6235 vl
 6593 6256 vl
 6570 6277 vl
 6553 6292 vl
 6479 6356 pt
 6403 6418 il
 6396 6424 vl
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 6326 6480 vl
 6250 6542 pt
 6172 6603 il
 6159 6613 vl
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 6017 6724 pt
 5939 6785 il
 5918 6802 vl
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 5864 6844 vl
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 5784 6906 pt
 5706 6966 il
 5700 6970 vl
 5673 6991 vl
 5646 7012 vl
 5628 7026 vl
 5550 7086 pt
 5472 7146 il
 5456 7159 vl
 5429 7180 vl
 5403 7201 vl
 4 SLW
 2129 4419 pt
 2227 4419 pt
 2326 4419 pt
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 2523 4417 pt
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 3409 4409 pt
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 4193 4354 pt
 4291 4339 pt
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 5249 4121 pt
 5347 4111 pt
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 5544 4097 pt
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 5740 4089 pt
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 7118 4077 pt
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 7709 4077 pt
 7807 4077 pt
 4 SLW
 7854 4077 pt
 7952 4077 pt
 8051 4077 pt
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 8247 4077 pt
 8346 4077 pt
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 8543 4077 pt
 8641 4077 pt
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