ў7#SёДLЅp№Є№Є№Є:№о,ё ёёёё ё$ ё. ё8ё8ё8ё8ё8 ёёXёXёXё–ёё˜ёœёX'ё ёЂёІёЊёЌёА4.C.7. - Prototype and Test Beam Program A Small Prototype EMC (SPEMC) was constructed to optimize the construction techniques and study the performance of the stack and several SMD prototypes in test beams appropriate for the RHIC environment. These efforts are described in this section. Detailed results on the construction the spliced optical fibers that are part of the SPEMC's optical read-out chain will be discussed. An automated device with seven independent settings to control was used to perform the splices. Considerable care was take to optimize these settings to produce splices that are mechanically strong, optically efficient, and consistent. Results on the performance of the SPEMC stack and the several SMD prototypes obtained in two comprehensive test beam runs are then described. It is important to note that the design of this SPEMC is based on the design of the BEMC as described in the original STAR EMC CDR. Since then, several revisions to the design of the stack were made, and each of these revisions improves the performance of the stack. Therefore the test beam results for the energy resolution of the stack (shown in 4.C.7 Figure 4 below) are a somewhat poorer than that one would expect from the BEMC as presently designed. Also, the e/h discrimination and efficiency numbers presented in section 4.C.7.3 should also be considered as lower limits for at momenta below ~2 GeV/c, where the so-called дE/pе cuts are the most important. However the remainder of the test beam results, i.e. all of the SMD analyses should be taken at face value. 4.C.7.1 - Optical Fiber Splicing Due to space limitations and the relatively high cost of magnetic field-insensitive PMTs, the scintillation light is to be shifted and carried outside of the magnet coils to externally mounted PMTs. Round 1 mm diameter plastic optical fibers will be circuitously routed over a path that's ~3 m long, which is large compared to the typical attenuation length of WSFs. We have therefore adopted a design similar to that used in the CDF calorimeters which involves the thermal splicing of 20-35 cm long WSFs to ~3 m long CFs. If this method is to work, one must simultaneously maximize the optical transmission efficiency at each splice, minimize the splice-to-splice variation in this transmission, and maximize the mechanical strength of the splice joint. The fibers used in this study and in the SPEMC are Bicron BCF-91A. The thermal splicing was done using an automated device developed by the Michigan State University - High Energy Physics group for use in the construction of CDF calorimeters. As the optical fibers for the STAR-EMC differ from those used in the CDF calorimeters, it is important to re-explore the parameter space of this fiber splicer for the present application. The mechanical strength and optical transmission efficiency of the splices can depend strongly (and often inversely) on the various splicer settings.  4.C.7 Figure 1 - The dimensions of a typical splice. The various diameters are held to ~1 mil by the splicer over a wide ranges of the splicer settings, while the splice length depends strongly on the heating time (see below). The operation of the MSU-HEP fiber splicer is highly automated, which results in very consistent splices. Four time intervals and two pressures are adjustable, but in general the most important parameter is the heating time. This is the time interval over which a modified projector lamp melts the two fibers where they meet. The fibers are held inside a short section of preshrunk FEP tubing (the вjacketг), which is enclosed by a pair of precision milled glass half tubes. A side view of a typical splice is shown in 4.C.7 Figure 1. The splices obtained from this device look similar to those obtained from other optical fiber splicers. The jacket increases the splice width, but it also adds a considerable amount of strain relief to the joint.  4.C.7 Figure 2 -The splice length (upper frame) and the break radius (lower frame) versus the heating time. The mechanical strength of the splices were studied versus the heating time and the other splicer parameters in two different ways. The strength longitudinally was studied using a machine provided by the MSU-HEP group which held the fiber on both sides of the splice and pulled by increasing amounts. Undeformed splices typically had longitudinal strengths within ~20% of that for lengths of the same fiber without a splice, supporting more than 10 lbs. of force along the fiber. The вtransverseг strength is a somewhat more critical attribute, as the fibers may be bent over radii of curvature ~3.0 cm near the splice. This bending strength depends more strongly on the splicer parameters than the longitudinal strength. It was evaluated by bending spliced fibers in a circle at the splice and measuring the radius of this circle that results in the breaking of the splice joint. The strongest splices have minimal break radii, while Liouville's theorem demands light losses of an amount increasing with the splice length. The best heating time thus results in a minimal break radius and a minimal splice length. The break radius and the splice length are shown versus the heating time in 4.C.7 Figure 2. The splice length increases linearly with the heating time in the range from 5 to 15 s. As the heating time is increased, however, the break radius of the splice decreases, i.e. the splices become mechanically stronger. For heating times in the range from 10 to 14 seconds, the splice joints do not break for radii of curvature that are larger than ~0.5 cm. Here the splice joint is stronger than the fiber itself, as for radii larger than ~1.5 cm, the fibers themselves more often break where they enter the jacket. We therefore set the heating time at 11 s for the SPEMC fibers. This results in the shortest possible splice lengths for essentially unbreakable splices. The focus was then directed onto maximizing the optical transmission efficiency of the splices over the more limited range of splicer parameters leading to unbreakable splices. However, unlike the mechanical properties, the optical transmission efficiency can be significantly affected by the quality of the fiber preparation before the splicing. A linear scanner including a collimated UV light source and reference measurements was used to measure the shifted light transmission as a function of the position along unspliced WSF fibers and spliced WSF+WSF fibers. These measurements were used to extract the optical transmission efficiency for shifted light across each splice, which was tabulated versus different splicer settings following different methods used to prepare the fibers before splicing.   4.C.7 Figure 3 -The light output at the end of unspliced (left frame) and spliced fibers of various qualities (right frame). Besides the optical transmission from the linear scanner, there are two splice properties that can be evaluated visually with a hand-held UV light source. The first is splice deformation (either along the splice or azimuthally), which results from the occasional uneven heating of the joint producing a mechanically weak and optically inefficient splice. The second is by far the most important contributor of optical transmission inefficiencies. If the cladding on one or both fibers is damaged during the cutting of these fibers, a break in the cladding exists where the (spliced) fibers meet, which allows a significant amount of light to escape. The splices were therefore classified into three categories (вgoldг, вsilverг, and вbronzeг) on the basis of the visual inspection with a hand-held UV source. The best splices (вgoldг) were undeformed and showed no cladding breaks. The next best class of splices (вsilverг) were either slightly deformed, or showed small cladding breaks (typically less than ~1/3 of the circumference of the splice). The apparently worst splices (вbronzeг) were either very deformed or had large cladding breaks, or both. The typical results from the linear scanning is shown in 4.C.7 Figure 3. The left frame shows the dependence of the shifted light output on the linear distance between the collimated UV source and a PMT which are ``connected" by a straight unspliced WSF fiber. The core attenuation length was consistently measured to be 1.8 m. Exponential fits to the transmission curves for spliced fibers were employed with fixed attenuation lengths to extract the transmission efficiency of shifted light across each WSF to WSF splice. Examples of these fits for typical gold, silver, and bronze splices are shown in the right frame of 4.C.7 Figure 3. The attributes of the splices evaluated by the visual inspection under a UV light source (i.e. splice deformation and/or cladding breaks) were strongly correlated with the transmission efficiencies measured by the linear scanner. This is because the splice dimensions are fixed at the constant values appropriate for the final set of splicer parameters. Thus, Liouville's theorem contributes much less to the splice-to-splice variations in the transmission as compared to sloppy fiber preparation, which results in visually apparent cladding breaks, and rarely, splice deformation. The optical efficiencies obtained were (92Б4)%, (80Б10)%, and (65Б20)% for the gold, silver, and bronze splices, respectively. The average optical efficiency of our gold splices is consistent with that obtained by the CDF group for their best splices, although our fibers have a larger diameter and different manufacturer, and our set of splicer parameters are different. The 240 spliced fibers needed for the SPEMC were then produced. As the fiber preparation is by far the most important aspect of the production of consistently high quality splices, considerable care was taken to cut the WSFs and CFs using a jig that minimized damage to the fiber cladding. During the final production, approximately 14/15 of the splices were visually classified as golden. Loading the fibers in the preshrunk jacket, inserting these into the splicer, and running the splicer takes about 90 seconds per splice. Cladding breaks are essentially eliminated altogether by polishing the two ends to be spliced using another automated device (also developed for the construction of the CDF calorimeters). This polishing takes about 60 s/splice, but it leads to gold splices essentially every time. The SPEMC was then assembled using a scintillator wrapping and scintillator/WSF coupling technique involving Tyvek paper and Aluminized mylar that results in an average of 1.75 photoelectrons per minimum ionizing particle for WSFs(CFs) that were 18(200) cm long. In the SPEMC, the scintillator was Kurrary SCSN38 and the Lead was unclad and unalloyed. The scintillators were arranged in six towers, four(two) of which were the same size as the BEMC towers at h ~ 0(1). An aluminum box was placed in the stack after 5 lead/scintillator layers (~4.5 X0) to allow the insertion of different prototype SMDs. Selected results from the in-beam tests of the SPEMC and the prototypical SMDs are described in the next section. 4.C.7.2 - SPEMC and SMD Performance The SPEMC was studied in beam at the Brookhaven AGS B2 line in two runs in May 1994 and July 1995. Five different configurations of the SPEMC were studied systematically for eБ, hБ (p and p), and mБ at 5-7 momenta in the range from 0.3 to 8 GeV/c and at 12-20 positions on the face of the stack. The configurations differ in the depth segmentation (none, 5/15, or 10/10 in layers) and the angle of incidence (zero or 15А). Three different prototype SMDs were inserted into the SPEMC stack to study their performance as well. A high speed transputer data acquisition system was used, which allowed event rates to tape approaching 15 kHz, and resulted in over 1.4 billion events on tape in total.  4.C.7 Figure 4 -The energy resolution (left frame) and the linearity (right frame) of the total signal from the SPEMC stack for electrons. The linearity is shown before (solid points) and after (open points) the correction for the electron energy loss in the beam-line. The SPEMC energy resolution and linearity for electrons is shown in 4.C.7 Figure 4. This resolution is consistent with that from similarly designed EMCs in other experiments, and better than the ~20%/жE design goal for the STAR-EMC. The SPEMC is linear to better than 1% for electron energies below ~6 GeV/c after the correction for the electron energy loss in the beam line. Of the three SMDs that were studied in beam, one was a scintillator/-fiber/PMT design (вSciFiг) and the other two were wire/strip chambers. The SciFi SMD consists of two layers, each of which consists of a 2 mm thick Lead plate and 5 mm thick by 1.4 cm wide scintillator strips. It is just under one X0 in thickness, which is considerably thicker in radiation lengths than either of the prototype wire/strip chamber SMDs. This will be apparent in the results shown below. Due to significant differences in the cost, wire/strip chambers will be the SMD technology used in the STAR-EMC. The design of the two different wire/strip SMD prototypes that were studied in the SPEMC is similar to that for the SMDs in CDF. The following will concentrate on the results obtained from one of these chambers, called вASMDг; the data from the other SMD is being analyzed independently. The wire(strip) pitch in the ASMD was (0.725)1.56 cm, and the wires were ganged in two per read-out channel. The gas was 5% CO2 and 95% Argon, while the Voltage was ~1400 V. There were transresistance amplifiers on the chamber itself, all of which where within ~2 cm of the wires or strips. The ASMD gas volume was inside an aluminum foil EM shield which was isolated from both the ASMD ground and the SPEMC ground. This ground was connected to the cable shield. On the basis of SPICE simulations (see below), the twisted-pair signal cables were shielded with aluminum foil and an outside insulator. On the other end of these ~20 meter signal cables, there were MAX436 differential receiver chips before the ADCs. The cable shield was connected to ground only at the receiver end.  4.C.7 Figure 5 - The SMD summed pulse height response (upper frame) and pulse height resolution (lower frame) versus the energy of electrons incident on the SPEMC for the SciFi SMD (down triangles) and the ASMD (up triangles). The inset depicts the linearity of the SMD total pulse heights without any constraint on the depth of the shower maximum (see text.) The average values of the total pulse height distributions from the SciFi SMD and the ASMD are shown versus the electron energy in 4.C.7 Figure 5. Without any constraint on the depth of the shower maximum via a cut on the front/back energy sharing in the depth segmented SPEMC, the average total pulse heights from both SMDs is linear to ~15%. Employing such a gate to select showers with maxima near the SMD layer, the SMD signal linearity can be improved by a factor of two. The lower frames of Figure 4.C.7 Figure 5 depict the energy weighted SMD pulse height resolution, (DSжE)/S, where S and D are the average and standard deviation of the pulse height distribution for electrons of an energy E. The ratio D/S for the SciFi SMD thus behaves like ~0.6/жE, while the ASMD resolution goes like ~1/жE. The considerably better pulse height resolution obtained from the SciFi SMD is the natural result of its much larger thickness in radiation lengths.  4.C.7 Figure 6 -The total pulse height distributions obtained from a prototype wire/strip SMD in the SPEMC for 0.5 GeV/c and 1.0 GeV/c electrons, as labelled, with the simulated magnet noise signal off (solid lines) and on (dashed lines). Like the optical fibers for the stack, the signal cables for the (wire/strip chamber) SMDs in STAR are routed out radially through the magnet coils. The STAR magnet coils could potentially have a voltage ripple of a few hundred Volts, but this could be reduced to ~20 V with some filtering of the magnet power. A test was therefore performed to evaluate the performance of the SMD with and without the presence of a (simulated) capacitively coupled noise signal from a magnet coil. To simulate the magnet noise, a 20 V square wave (1 kHz rate, 1 ms rise time) was added though ~500 pF to the ASMD cable shield. The summed pulse height distributions obtained from the ASMD when low energy electrons are directed at the SPEMC are shown in 4.C.7 Figure 6. The solid and dashed histograms show what is obtained with the fake magnet off and on, respectively. No modification of the summed pulse heights, or the signals from individual ASMD channels (not shown), is apparent. The shielding of the ASMD and its cables that was described above thus provides the necessary protection from ~20 V magnet noise that is coupled through ~500 pF. 4.C.7.3 - Electron/hadron discrimination  4.C.7 Figure 7 - Three stack observables (upper frames) and three SMD observables (lower frames) that support cuts leading to e/h discrimination, shown for 8.0 GeV/c electrons (shaded histograms) and hadrons (open histograms). The direct identification of electrons with momenta above a few GeV/c in STAR is possible only with the information provided by the EMC. As the SPEMC and all three prototype SMDs worked well in the test beam, it is relevant to explore the electron/hadron discrimination that is possible using a variety of cuts on both stack and SMD observables.  4.C.7 Figure 8 - The e/h discrimination (squares, left axes) and electron efficiency (triangles, right axes) versus the particle momentum for the particular sets of cuts (depending on the momentum) described in the text.. Only simple дaddsе of one-dimensional cuts on the variables shown in 4.C.7 Figure 7 were used to make this plot. For SMD-equipped EMCs that are segmented into two depth sections, the six observables shown in 4.C.7 Figure 7 support cuts that provide e/h discrimination for hits of known momentum. The stack observables are the total energy (вSPEMC SPHг), the front, F, to back, B, energy sharing quantified by Z=(B-F)/(B+F) (вCal-Zг), and the ratio of the struck tower energy to the total (вisolationг). The SMD observables are the total pulse height (вSMD SPHг), the pulse-height weighted shower width in both the X and Y directions (вSMD DXХDY"), and the difference between the expected location of the shower centroid and the measured shower centroid (в|Xsmd-Xpred|г). The geometry of the actual STAR-EMC is somewhat different from the SPEMC geometry, while the test beam data cannot include the tower and SMD channel occupancy expected in RHIC events. We have thus concentrated only on simple and approximately located cuts to get a feel for the general trends. At momenta below ~1.5 GeV/c, the most effective cuts are the E/p cut and the front/back energy cut. For larger momenta, the front/back energy cut becomes less effective, while the E/p cut and all of the SMD-based cuts become more effective. Using reasonable but unoptimized cuts on these two combinations of observables above, the discrimination is roughly 6:1 at electron efficiency of ~80% for momenta below ~1 GeV/c. In this range of momenta, however, other detectors in STAR, primarily the STAR TOF, also provide a significant e/h discrimination. At momenta above ~2 GeV/c, the discrimination is ~100:1 and the electron efficiency is between 60 and 80%.  W.J. Llope, to be published in the proceedings, вVIth International Conference on Calorimetry in High Energy Physicsг, Frascati (Roma), Italy, June 8-14, 1996 (Plenum Publishing, in press).  Preliminary bench tests the a-groove coupling increases the light yield from ~1.75 p.e./m.i.p. (see text below) to ~3 p.e./m.i.p. Also, the scintillators are now 5 mm instead of 4 mm thick, which increases the sampling fraction by ~20%.  http://www-cdf.fnal.gov/  R. Richards, private communication; B. Tannenbaum, Masters Thesis, Michigan State University, unpublished (1994); J.P. Mansour et al., /CDF/DOC/PLUG_UPGR/PUBLIC/2562.  G. Apollinari et al., Nucl. Inst. and Methods A311, 520 (1992).  K.G. Steffen, High Energy Beam Optics, pgs. 161-172 (Interscience Publishers, New York, N.Y.).  Increasing the splice diameter relative to the fibers also increases light loss at the splice according to this theorem, but the splice diameter is held constant to ~1 mil by the splicer.  D.G. Underwood, published in the Proceedings from the IV International Conference on Calorimetry in High Energy Physics, La Biodola, Elba (1993).  A. Patwa et al., PHENIX Technical Note 181 (1995). 4.C.7 Prototype and Test Beam Program (WJL, 20-Nov-96) €‚hй3€Zјй%Zјй]Ьџ џўHH]ЬЁђ8BIM]ЬGr‰phЏbj ]Ьšџ0]ЬHH 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џџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџ.џџџџџџџџџџџџџџџџџџџџџџџџbin5555452r LabУ?€љљУ1љљ77џ џџџџ77 77# ОЁРcurrentpoint  П"77 ОЁР$/picTop exch def /picLeft exch def ЁР4currentpoint /picBottom exch def /picRight exch def ЁР[ 0 0 567 567] ЁРл1 dict begin /s exch def picLeft picTop translate picRight picLeft sub s 2 get s 0 get sub div picBottom picTop sub s 1 get s 3 get sub div scale s 0 get neg s 3 get neg translate end /showpage {} def /copypage {} def ЁР %!PS-Adobe-2.0 EPSF-2.0 %%BoundingBox: 0 0 567 567 %%Title: splice_heat.eps %%Creator: HIGZ Version 1.22/09 %%CreationDate: 96/05/11 12.23 %%EndComments 80 dict begin /s {stroke} def /l {lineto} def /m {moveto} def /t {translate} def /sw {stringwidth} def /r {rotate} def /rl {roll} def /R {repeat} def /d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def /c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def /cl {closepath} def /sf {scalefont setfont} def /black {0 setgray} def /box {m dup 0 exch d exch 0 d 0 exch neg d cl} def /NC{systemdict begin initclip end}def/C{NC box clip newpath}def /bl {box s} def /bf {box f} def /Y { 0 exch d} def /X { 0 d} def /mp {newpath /y exch def /x exch def} def /side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def /mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def /mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def /mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def /m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def /m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def /m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def /m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def /m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl fill gr} def /m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 5 {side} repeat s gr} def /m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d x w2 sub y w2 add m w w neg d x w2 sub y w2 sub m w w d s} def /m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def /m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def /DP {/PT exch def gsave 47.2 47.2 scale PT 1 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 > } image } if PT 2 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE > } image } if PT 3 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE > } image } if PT 4 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < DF DF BF BF 7F 7F FE FE FD FD FB FB F7 F7 EF EF DF DF BF BF 7F 7F FE FE FD FD FB FB F7 F7 EF EF > } image } if PT 5 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 7F 7F BF B F DF DF EF EF F7 F7 FB FB FD FD FE FE 7F 7F BF BF DF DF EF EF F7 F7 FB FB FD FD FE FE > } image } if PT 6 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB > } image } if PT 7 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 > } image } if PT 8 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EE EE 47 47 83 83 C5 C5 EE EE 5C 5C 38 38 74 74 EE EE 47 47 83 83 C5 C5 EE EE 5C 5C 38 38 74 74 > } image } if PT 9 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EF EF EF EF D7 D7 38 38 FE FE FE FE 7D 7D 83 83 EF EF EF EF D7 D7 38 38 FE FE FE FE 7D 7D 83 83 > } image } if PT 10 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EF EF EF EF EF EF 00 00 FE FE FE FE FE FE 00 00 EF EF EF EF EF EF 00 00 FE FE FE FE FE FE 00 00 > } image } if PT 11 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < F7 F7 B6 B6 D5 D5 E3 E3 D5 D5 B6 B6 F7 F7 FF FF 7F 7F 6B 6B 5D 5D 3E 3E 5D 5D 6B 6B 7F 7F FF FF > } image } if PT 12 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < E3 E3 DD DD BE BE BE BE BE BE DD DD E3 E3 FF FF 3E 3E DD DD EB EB EB EB EB EB DD DD 3E 3E FF FF > } image } if PT 13 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FE FE 7D 7D BB BB D7 D7 EF EF D7 D7 BB BB 7D 7D FE FE 7D 7D BB BB D7 D7 EF EF D7 D7 BB BB 7D 7D > } image } if PT 14 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 00 00 EE EF EE EF EE EF 0E E0 EE EE EE EE EE EE 00 EE FE EE FE EE FE EE 00 00 FE EF FE EF FE EF > } image } if PT 15 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < DD DD AA AA DD DD FF FF 77 77 AA AA 77 77 FF FF DD DD AA AA DD DD FF FF 77 77 AA AA 77 77 FF FF > } image } if PT 16 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < F1 F1 EE EE 1F 1F FF FF F1 F1 EE EE 1F 1F FF FF F1 F1 EE EE 1F 1F FF FF F1 F1 EE EE 1F 1F FF FF > } image } if PT 17 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EE EE DD DD BB BB FF FF EE EE DD DD BB BB FF FF EE EE DD DD BB BB FF FF EE EE DD DD BB BB FF FF > } image } if PT 18 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < BB BB DD DD EE EE FF FF BB BB DD DD EE EE FF FF BB BB DD DD EE EE FF FF BB BB DD DD EE EE FF FF > } image } if PT 19 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 1F FC 67 F3 7B EF BD DE BD DE DE BD E6 B3 F8 0F E6 B3 DE BD BD DE BD DE 7B EF 67 F3 1F FC 7F FF > } image } if PT 20 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < DD DD EE EE EE EE EE EE DD DD BB BB BB BB BB BB DD DD EE EE EE EE EE EE DD DD BB BB BB BB BB BB > } image } if PT 21 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 0E 0E EF EF EF EF EF EF E0 E0 FE FE FE FE FE FE 0E 0E EF EF EF EF EF EF E0 E0 FE FE FE FE FE FE > } image } if PT 22 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 70 70 F7 F7 F7 F7 F7 F7 07 07 7F 7F 7F 7F 7F 7F 70 70 F7 F7 F7 F7 F7 F7 07 07 7F 7F 7F 7F 7F 7F > } image } if PT 23 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < AA AA 55 55 A9 A9 D1 D1 E1 E1 D1 D1 A9 A9 55 55 AA AA 55 55 A9 A9 D1 D1 E1 E1 D1 D1 A9 A9 55 55 > } image } if PT 24 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FE FF FC EA A8 D5 54 EA A8 D5 54 E8 28 D4 54 E8 E8 D4 D4 E8 EA 54 D5 A8 EA 54 D5 00 C0 00 80 > } image } if PT 25 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FE FF FC FF F8 FF F0 F0 00 F0 00 F0 20 F0 60 F0 E0 F1 E0 F3 E0 F0 00 E0 00 C0 00 80 00 00 00 > } image } if gr } def /FA { /PT exch def gsave clip 0 0 translate 1 1 54 { 1 sub 47.2 mul /Xcurr exch def 1 1 74 { 1 sub 47.2 mul /Ycurr exch def gsave Xcurr Ycurr translate PT DP gr } for } for gr } def /reencdict 24 dict def /ReEncode {reencdict begin /nco&na exch def /nfnam exch def /basefontname exch def /basefontdict basefontname findfont def /newfont basefontdict maxlength dict def basefontdict {exch dup /FID ne {dup /Encoding eq {exch dup length array copy newfont 3 1 roll put} {exch newfont 3 1 roll put} ifelse} {pop pop} ifelse } forall newfont /FontName nfnam put nco&na aload pop nco&na length 2 idiv {newfont /Encoding get 3 1 roll put} repeat nfnam newfont definefont pop end } def /accvec [ 176 /agrave 181 /Agrave 190 /acircumflex 192 /Acircumflex 201 /adieresis 204 /Adieresis 209 /ccedilla 210 /Ccedilla 211 /eacute 212 /Eacute 213 /egrave 214 /Egrave 215 /ecircumflex 216 /Ecircumflex 217 /edieresis 218 /Edieresis 219 /icircumflex 220 /Icircumflex 221 /idieresis 222 /Idieresis 223 /ntilde 224 /Ntilde 226 /ocircumflex 228 /Ocircumflex 229 /odieresis 230 /Odieresis 231 /ucircumflex 236 /Ucircumflex 237 /udieresis 238 /Udieresis 239 /aring 242 /Aring 243 /ydieresis 244 /Ydieresis 246 /aacute 247 /Aacute 252 /ugrave 253 /Ugrave] def /Times-Roman /Times-Roman accvec ReEncode /Times-Italic /Times-Italic accvec ReEncode /Times-Bold /Times-Bold accvec ReEncode /Times-BoldItalic /Times-BoldItalic accvec ReEncode /Helvetica /Helvetica accvec ReEncode /Helvetica-Oblique /Helvetica-Oblique accvec ReEncode /Helvetica-Bold /Helvetica-Bold accvec ReEncode /Helvetica-BoldOblique /Helvetica-BoldOblique accvec ReEncode /Courier /Courier accvec ReEncode /Courier-Oblique /Courier-Oblique accvec ReEncode /Courier-Bold /Courier-Bold accvec ReEncode /Courier-BoldOblique /Courier-BoldOblique accvec ReEncode /oshow {gsave [] 0 sd true charpath stroke gr} def /stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf text sw pop xs add /xs exch def} def /stwb { /fs exch def /fn exch def /nbas exch def /textf exch def textf length /tlen exch def nbas tlen gt {/nbas tlen def} if fn findfont fs sf textf dup length nbas sub nbas getinterval sw pop neg xs add /xs exch def} def /accspe [ 65 /plusminus 66 /bar 67 /existential 68 /universal 69 /exclam 70 /numbersign 71 /greater 72 /question 73 /integral 74 /colon 75 /semicolon 76 /less 77 /bracketleft 78 /bracketright 79 /greaterequal 80 /braceleft 81 /braceright 82 /radical 83 /spade 84 /heart 85 /diamond 86 /club 87 /lessequal 88 /multiply 89 /ЁР percent 90 /infinity 48 /circlemultiply 49 /circleplus 50 /emptyset 51 /lozenge 52 /bullet 53 /arrowright 54 /arrowup 55 /arrowleft 56 /arrowdown 57 /arrowboth 48 /degree 44 /comma 43 /plus 45 /angle 42 /angleleft 47 /divide 61 /notequal 40 /equivalence 41 /second 97 /approxequal 98 /congruent 99 /perpendicular 100 /partialdiff 101 /florin 102 /intersection 103 /union 104 /propersuperset 105 /reflexsuperset 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110 /notelement 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright 118 /arrowdbldown 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def /Symbol /Special accspe ReEncode gsave .25 .25 scale %%EndProlog gsave 0 0 t black [] 0 sd 1 lw 1588 942 340 1213 bl 1588 942 340 1213 C 473 1327 m 8 Y s 473 1366 m 8 Y s /w 32 def /w2 {w 2 div} def /w3 {w 3 div} def 473 1351 m21 737 1469 m 8 Y s 737 1508 m 8 Y s 737 1492 m21 1002 1540 m 8 Y s 1002 1579 m 8 Y s 1002 1563 m21 1266 1682 m 7 Y s 1266 1721 m 8 Y s 1266 1705 m21 1531 1847 m 8 Y s 1531 1887 m 7 Y s 1531 1871 m21 1796 1918 m 32 Y s 1796 1981 m 32 Y s 1796 1965 m21 340 1284 m 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 9 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 9 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 9 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 9 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 4 d 8 3 d 8 4 d 8 4 d 8 4 d 8 3 d s NC 340 1213 m 942 Y s 374 1445 m -34 X s 374 1682 m -34 X s 374 1918 m -34 X s 374 2155 m -34 X s 374 1445 m -34 X s /xs 0 def (0.5) /Times-Roman 111 stwn gsave 323 1408 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (0.5) show gr /xs 0 def (1) /Times-Roman 111 stwn gsave 323 1645 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (1) show gr /xs 0 def (1.5) /Times-Roman 111 stwn gsave 323 1881 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (1.5) show gr /xs 0 def (2) /Times-Roman 111 stwn gsave 323 2118 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (2) show gr 340 1213 m 1588 X s 340 1247 m -34 Y s 605 1247 m -34 Y s 869 1247 m -34 Y s 1134 1247 m -34 Y s 1399 1247 m -34 Y s 1663 1247 m -34 Y s 1928 1247 m -34 Y s /xs 0 def (4) /Times-Roman 111 stwn gsave 340 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (4) show gr /xs 0 def (6) /Times-Roman 111 stwn gsave 605 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (6) show gr /xs 0 def (8) /Times-Roman 111 stwn gsave 869 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (8) show gr /xs 0 def (10) /Times-Roman 111 stwn gsave 1134 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (10) show gr /xs 0 def (12) /Times-Roman 111 stwn gsave 1399 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (12) show gr /xs 0 def (14) /Times-Roman 111 stwn gsave 1663 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (14) show gr /xs 0 def (16) /Times-Roman 111 stwn gsave 1928 -10200 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (16) show gr 1588 942 340 1213 C 2268 2268 0 0 C /xs 0 def (Splice length \(cm\)) /Times-Roman 111 stwn gsave 147 2155 t 90 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (Splice length \(cm\)) show gr 1588 942 340 1213 C NC 1588 941 340 261 bl 1588 941 340 261 C NC 340 261 m 941 Y s 374 449 m -34 X s 374 637 m -34 X s 374 826 m -34 X s 374 1014 m -34 X s 374 1202 m -34 X s 374 449 m -34 X s /xs 0 def (1) /Times-Roman 111 stwn gsave 323 412 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (1) show gr /xs 0 def (2) /Times-Roman 111 stwn gsave 323 600 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (2) show gr /xs 0 def (3) /Times-Roman 111 stwn gsave 323 789 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (3) show gr /xs 0 def (4) /Times-Roman 111 stwn gsave 323 977 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (4) show gr /xs 0 def (5) /Times-Roman 111 stwn gsave 323 1165 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (5) show gr 340 261 m 1588 X s 340 295 m -34 Y s 605 295 m -34 Y s 869 295 m -34 Y s 1134 295 m -34 Y s 1399 295 m -34 Y s 1663 295 m -34 Y s 1928 295 m -34 Y s /xs 0 def (4) /Times-Roman 111 stwn gsave 340 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (4) show gr /xs 0 def (6) /Times-Roman 111 stwn gsave 605 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (6) show gr /xs 0 def (8) /Times-Roman 111 stwn gsave 869 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (8) show gr /xs 0 def (10) /Times-Roman 111 stwn gsave 1134 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (10) show gr /xs 0 def (12) /Times-Roman 111 stwn gsave 1399 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (12) show gr /xs 0 def (14) /Times-Roman 111 stwn gsave 1663 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (14) show gr /xs 0 def (16) /Times-Roman 111 stwn gsave 1928 170 t 0 r xs 2 div neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (16) show gr 1588 941 340 261 C 1 1 0 c 420 731 m 595 -188 d 93 -254 d 423 X 331 141 d 104 Y -331 -188 d -423 X -93 417 d -595 241 d f black /w 31 def /w2 {w 2 div} def /w3 {w 3 div} def 1838 435 1833 477 452 724 452 797 4 { m21} R 1281 331 1283 318 1277 313 1287 319 1277 315 1289 325 1285 323 1561 318 1551 326 1555 311 1549 317 1555 311 1564 326 1561 328 1003 564 1010 566 1013 589 1008 613 1009 625 1006 638 735 670 730 679 734 671 720 720 720 724 1008 712 725 732 452 761 450 783 456 786 732 785 457 840 458 869 455 934 459 957 35 { m21} R 1144 321 1144 328 1142 331 1135 324 1146 327 1145 330 1281 311 1277 308 1277 323 1274 326 1274 316 1287 313 1839 440 1839 437 1825 439 1827 444 1830 438 1829 441 1007 622 1007 619 997 637 1012 621 858 647 999 642 866 676 1000 672 867 716 868 709 861 764 875 795 30 { m25} R 2268 2268 0 0 C /w 2 def /w2 {w 2 div} def /w3 {w 3 div} def 347 355 m20 347 355 m20 355 355 m 17 X s 381 355 m20 381 355 m20 389 355 m 17 X s 415 355 m20 415 355 m20 423 355 m 17 X s 449 355 m20 449 355 m20 457 355 m 17 X s 483 355 m20 483 355 m20 491 355 m 17 X s 517 355 m20 517 355 m20 525 355 m 17 X s 551 355 m20 551 355 m20 559 355 m 17 X s 585 355 m20 585 355 m20 593 355 m 17 X s 619 355 m20 619 355 m20 627 355 m 17 X s 653 355 m20 653 355 m20 661 355 m 18 X s 687 355 m20 687 355 m20 696 355 m 17 X s 721 355 m20 721 355 m20 730 355 m 17 X s 755 355 m20 755 355 m20 764 355 m 17 X s 789 355 m20 789 355 m20 798 355 m 17 X s 823 355 m20 823 355 m20 832 355 m 17 X s 857 355 m20 857 355 m20 866 355 m 17 X s 891 355 ЁР Gm20 891 355 m20 900 355 m 17 X s 925 355 m20 925 355 m20 934 355 m 17 X s 959 355 m20 959 355 m20 968 355 m 17 X s 993 355 m20 993 355 m20 1002 355 m 17 X s 1027 355 m20 1027 355 m20 1036 355 m 17 X s 1061 355 m20 1061 355 m20 1070 355 m 17 X s 1095 355 m20 1095 355 m20 1104 355 m 17 X s 1129 355 m20 1129 355 m20 1138 355 m 17 X s 1163 355 m20 1163 355 m20 1172 355 m 17 X s 1197 355 m20 1197 355 m20 1206 355 m 17 X s 1231 355 m20 1231 355 m20 1240 355 m 17 X s 1265 355 m20 1265 355 m20 1274 355 m 17 X s 1299 355 m20 1299 355 m20 1308 355 m 17 X s 1333 355 m20 1333 355 m20 1342 355 m 17 X s 1367 355 m20 1367 355 m20 1376 355 m 17 X s 1401 355 m20 1401 355 m20 1410 355 m 17 X s 1435 355 m20 1435 355 m20 1444 355 m 17 X s 1469 355 m20 1469 355 m20 1478 355 m 17 X s 1503 355 m20 1503 355 m20 1512 355 m 17 X s 1538 355 m20 1538 355 m20 1546 355 m 17 X s 1572 355 m20 1572 355 m20 1580 355 m 17 X s 1606 355 m20 1606 355 m20 1614 355 m 17 X s 1640 355 m20 1640 355 m20 1648 355 m 17 X s 1674 355 m20 1674 355 m20 1682 355 m 17 X s 1708 355 m20 1708 355 m20 1716 355 m 17 X s 1742 355 m20 1742 355 m20 1750 355 m 17 X s 1776 355 m20 1776 355 m20 1784 355 m 17 X s 1810 355 m20 1810 355 m20 1818 355 m 17 X s 1844 355 m20 1844 355 m20 1852 355 m 17 X s 1878 355 m20 1878 355 m20 1886 355 m 17 X s 1912 355 m20 1912 355 m20 1920 355 m 8 X s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1919 355 m20 1919 355 m20 1928 355 m cl s 1927 355 m20 1927 355 m20 1588 941 340 261 C 2268 2268 0 0 C /xs 0 def (Heating time \(sec\)) /Times-Roman 111 stwn gsave 1928 68 t 0 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (Heating time \(sec\)) show gr /xs 0 def (Break Radius \(cm\)) /Times-Roman 111 stwn gsave 147 1202 t 90 r xs neg 0 t 0 0 m /Times-Roman findfont 111 sf 0 0 m (Break Radius \(cm\)) show gr 1588 941 340 261 C 2268 2268 0 0 C 1588 941 340 261 C 2268 2268 0 0 C /w 32 def /w2 {w 2 div} def /w3 {w 3 div} def 1007 1117 m21 gsave 1070 1089 t 0 r 0 0 m /Times-Roman findfont 86 sf 0 0 m (WSF-WSF Splices) show gr 1588 941 340 261 C 2268 2268 0 0 C 1588 941 340 261 C 2268 2268 0 0 C 1007 1033 m25 gsave 1070 1004 t 0 r 0 0 m /Times-Roman findfont 86 sf 0 0 m (CF-CF Splices) show gr 1588 941 340 261 C gr gr showpage end %%EOF 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џџџџ77 77# ОЁРcurrentpoint  П"77 ОЁР$/picTop exch def /picLeft exch def ЁР4currentpoint /picBottom exch def /picRight exch def ЁР[ 0 0 567 567] ЁРл1 dict begin /s exch def picLeft picTop translate picRight picLeft sub s 2 get s 0 get sub div picBottom picTop sub s 1 get s 3 get sub div scale s 0 get neg s 3 get neg translate end /showpage {} def /copypage {} def ЁР %!PS-Adobe-2.0 EPSF-2.0 %%BoundingBox: 0 0 567 567 %%Title: trans_unspliced.eps %%Creator: HIGZ Version 1.22/09 %%CreationDate: 96/05/31 13.05 %%EndComments 80 dict begin /s {stroke} def /l {lineto} def /m {moveto} def /t {translate} def /sw {stringwidth} def /r {rotate} def /rl {roll} def /R {repeat} def /d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def /c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def /cl {closepath} def /sf {scalefont setfont} def /black {0 setgray} def /box {m dup 0 exch d exch 0 d 0 exch neg d cl} def /NC{systemdict begin initclip end}def/C{NC box clip newpath}def /bl {box s} def /bf {box f} def /Y { 0 exch d} def /X { 0 d} def /mp {newpath /y exch def /x exch def} def /side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def /mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def /mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def /mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def /m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def /m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def /m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def /m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def /m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl fill gr} def /m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 5 {side} repeat s gr} def /m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d x w2 sub y w2 add m w w neg d x w2 sub y w2 sub m w w d s} def /m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def /m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def /DP {/PT exch def gsave 47.2 47.2 scale PT 1 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 AA AA 55 55 > } image } if PT 2 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE BB BB EE EE > } image } if PT 3 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE FF FF BB BB FF FF EE EE > } image } if PT 4 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < DF DF BF BF 7F 7F FE FE FD FD FB FB F7 F7 EF EF DF DF BF BF 7F 7F FE FE FD FD FB FB F7 F7 EF EF > } image } if PT 5 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < 7F 7F BF B F DF DF EF EF F7 F7 FB FB FD FD FE FE 7F 7F BF BF DF DF EF EF F7 F7 FB FB FD FD FE FE > } image } if PT 6 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB BB > } image } if PT 7 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 FF FF FF FF FF FF 00 00 > } image } if PT 8 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EE EE 47 47 83 83 C5 C5 EE EE 5C 5C 38 38 74 74 EE EE 47 47 83 83 C5 C5 EE EE 5C 5C 38 38 74 74 > } image } if PT 9 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EF EF EF EF D7 D7 38 38 FE FE FE FE 7D 7D 83 83 EF EF EF EF D7 D7 38 38 FE FE FE FE 7D 7D 83 83 > } image } if PT 10 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < EF EF EF EF EF EF 00 00 FE FE FE FE FE FE 00 00 EF EF EF EF EF EF 00 00 FE FE FE FE FE FE 00 00 > } image } if PT 11 eq { 16 16 1 [ 16 0 0 16 neg 0 16 ] { < F7 F7 B6 B6 D5 D5 E3 E3 D5 D5 B6 B6 F7 F7 FF FF 7F 7F 6B