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  <front>
    <journal-meta>
      <journal-title-group>
        <journal-title>Phys. Rev. Lett.</journal-title>
      </journal-title-group>
    </journal-meta>
    <article-meta>
      <title-group>
        <article-title>NEW PARTICLE POSITION DETERMINATION MODULES FOR DOUBLE SIDED SILICON STRIP DETECTOR AT DGFRS</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>L. Schlattauer</string-name>
          <email>leo.schlattauer@upol.cz</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>V.G. Subbotin</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>A.M. Zubareva</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Y. S. Tsyganov</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>A.A. Voinov</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Experimental Physics, Faculty of Science, Palacký University</institution>
          ,
          <addr-line>17. listopadu 1192/12, 771 46 Olomouc</addr-line>
          ,
          <country country="CZ">Czech Republic</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research</institution>
          ,
          <addr-line>6 Joliot-Curie, Dubna, Moscow region, 141980</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2017</year>
      </pub-date>
      <volume>104</volume>
      <issue>142502</issue>
      <fpage>265</fpage>
      <lpage>270</lpage>
      <abstract>
        <p>New particle position determination modules for double-sided silicon strip detector (DSSD) were designed that allow to simplify existing multi-channel measurement system in search for the rare events of super heavy elements formation at DGFRS. The main principle is to search position correlated sequences of implanted SHE and followed by alpha-particles/or SF events above predefined threshold energy level in real-time for all 128 back strips. The resulting information is about providing the address of active strip and the coincidence sign. The newly developed system trigger passed the prototyping stage and is about to use in next experiment. This system will reduce the overall system dead time. This article is about describe in deep of the CD32-5M coder units and the PKK-05 preregister which are together the main part of the developed position determination subsystem.</p>
      </abstract>
      <kwd-group>
        <kwd>DGFRS</kwd>
        <kwd>DSSD</kwd>
        <kwd>SHE</kwd>
        <kwd>Triggering</kwd>
        <kwd>Data Acquisition</kwd>
        <kwd>Nuclear electronics</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        The pioneering research of the predicted domain of enhanced stability of the super heavy
nuclei around Z 114 and N=184 was performed in the FLNR JINR (Dubna, Russia) during last 15
years [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. Six new super heavy elements with Z = 113-118 and more than 50 new isotopes with
Z = 104-118 were observed for the first time at the Dubna Gas-Filled Recoil Separator (DGFRS) in
irradiations of the targets of 233,238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 249Bk and 249Cf with
accelerated 48Ca ions beam delivered by U-400 cyclotron.
      </p>
      <p>
        These new nuclei were detected using arrays of position-sensitive Si strip detectors
(manufactured by Canberra NV, Belgium) in the focal plane of the DGFRS of two kinds, with 12
strips and 32 ones. Appropriate registering systems were designed and applied for the measurement
of energy, position and time information from reaction products implanted into the detector and from
their subsequent alpha-decay or spontaneous fission [
        <xref ref-type="bibr" rid="ref2 ref3">2, 3</xref>
        ]. Recently the array of detectors at the
DGFRS has been modified to improve the position resolution of recorded signals and to reduce
accordingly the probability of observing sequences of random events that imitate decay chains of
implanted nuclei (fig. 1).
      </p>
      <p>New detection system includes 0.3mm thick double-sided silicon strip detector (DSSD)
manufactured by Micron Semiconductor Ltd. This large DSSD has 1-mm wide strips, 48 at the front
side and 128 at the back side, equal to 6144 pixels of 1 mm2 in one Silicon wafer (to compare with
240 and 960 individual cells of formerly used 12-strip and 32-strip detectors, respectively). Such a
high pixilation enables to achieve superior position resolution for registering recoil-correlated decay
sequences and thus reducing number of potential random events. This detector of implanted recoils
was surrounded by six side Si-detectors (MICRON), each 500 microns thick with an active area of
65 mm by 120 mm without position sensitivity. This new Si-detector array has been designed,
assembled, commissioned off-line and provided by the Oak Ridge National Laboratory.</p>
      <p>
        Signals from all the detectors are processed using MESYTEC linear preamplifiers [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ].
Further, analog signals from preamplifiers were split into two independent measurement branches.
Special analog splitter-amplifier PA32-64 was designed by DGFRS group as 4M CAMAC module to
provide sharing of every spectroscopic channel between two measuring branches. Transfer factor
from input to output is 1.1. For better precision and stability, precision resistors with tolerance of
0.1% and low temperature coefficient of 25 ppm/°C were used in gain circuits. Every module splits
32 input signals into two separate output 32-channel streams. First 32 outputs go to analog registering
system of the DGFRS, like what was used in previous experiments [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ]; the other 32 outputs go to
50Ω digitizer inputs based on XIA PIXIE-16 modules provided by ORNL [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ]. To split the all
spectroscopic signals from 183 individual measuring cells of the focal plane detectors (48 plus 128
from DSSD,
plus 6 from side SSSD and one from backplane detector used in “VETO-mode”) six modules of the
splitters PA32-64 were produced. Thus, all the spectroscopic signals together with signals from
“START” and “STOP” multi-wire proportional chambers were processed by two different (“analog”
CAMAC based and “digital” PIXIE-16 based) registering systems simultaneously, providing
additional confidence in validity of performed data analysis.
      </p>
    </sec>
    <sec id="sec-2">
      <title>2. Development of coordinate determination units</title>
      <p>Another development of the operating “analog” registering system is associated with
attempts to reduce the total system dead-time of data recording and to optimize the method
(activecorrelation method) of the on-line search for “recoil – alpha-particle” or “recoil – SF” correlations
when detecting nuclei of the SHE and their decays.</p>
      <p>
        Application of this method developed in DGFRS research group [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ] allows to stop the 48Ca
ion beam from the cyclotron after detecting of candidate correlation sequence within energy and time
intervals corresponding to decays of parent and/or daughter nuclei in the same position on detector.
Thus, the background event rate in the separator’s focal plane associated with ions beam, target-like
nuclei and transfer-reactions products is strongly reduced. As an example, total energy spectra of
beam-on -like signals and beam-off  particles and total fission-fragment energy spectra, both
beam-on and beam-off are shown in fig. 2, a) and b) correspondently. The arrows point the energies
of events observed in the correlated decay chains.
      </p>
      <p>
        Amplitude of the signals of the detected events in the “analog” CAMAC-based registering
system are recorded after spectroscopic signals from 48 front strips and 128 rear strips of the DSSD
are processed by measuring SAR ADCs. Every ADC works in combination with a 16-channel analog
multiplexer (MUX) that reduces the total number of the measuring channels and gives the code
number of the working strip [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ]. Thus, we can measure the particle energy and its position in focal
plane detector’s area using three couples of MUX-ADC for serving the 48 front strips of DSSD and
eight MUX-ADC couples for serving the 128 rear strips. In fact, we measure the energy of the
detected particle in the DSSD twice (using separate ADCs for signals from front and rear detectors
simultaneously). In CAMAC-based registering system the total “dead-time” can be reduced if the
conversion time of each ADC is short enough and the number of ADCs to be read in CAMAC is
minimum with this aim in view, a new fast analog multiplexer and a new 12-bit SAR ADC were
designed (0.8 μs conversion time, compare with 40 μs in [9]).
      </p>
      <p>On the other hand, new system for determining coordinate of detected particles from 128 rear
strips was proposed and constructed. It consists of four individual modules CD32-5 that produce
binary code “1 strip of 32” each and primary register PKK-05 producing final code “1 of 128 strips”.
Every coder CD32-5 has 32 spectroscopic inputs with adjustable amplitude threshold from 5 mV to
300 mV with its viewing in front panel display (fig. 3).</p>
      <p>The common threshold level can be adjusted for all 32 channels in the module. The AD8564
quad 7 ns comparator [10] works as fast trigger with signals after additional amplification by factor 8
(eight vertical PCBs in fig. 3) and produce logical signal to priority coder if amplitude of input signal
exceeds the preset threshold level of the comparator. At the output, each module gives the logical
TTL-compatible 5-bit binary code corresponding to the channel. CD32-5 produces also additional
output bit for “majority marker” if there were any two neighboring channels worked at the same
time. The logical scheme for output code formation based on EPM7128SLC-15N chip application for
32 input channels is shown in fig. 4.
advantage of CAMAC-crate power supply. So, instead of reading data words of 4 coders, one should
read just one data word from KP-005 to obtain data about the strip number among 128 rear strips of
focal plane detector. Reading just two data words from one MUX-ADC couple and from register
KP005 one can obtain full info about energy and two-dimensional position of registered charged particle
in DSSSD. It helps to minimize the number of modules to be read in CAMAC cycle from eight to
one and to get the digital address of the strip with the detected event when serving the rear 128 strips
of the DSSSD.
3. Conclusion
 The subsystem prototype consisting of four 32-inputs modules for coding the strip number
for 128 rear strips of DSSD is manufactured. Maximum event rate is 100KHz.
 Just one CAMAC 1M station is needed to be read for launched rear strip determination in
“analog” registering system. Now the coordinate determination system is under testing in
real experiment conditions with usage of DSSD array.
 Subsystem provides also event sign, coincidence sign based on 25ns time window plus
inter-block coincidence.
</p>
      <p>Using this created subsystem prototype will improve the total system “dead-time”
by ~15 μs.
 System is software configurable in digital logic sections thanks to Altera MAX7000s
series PLDs. So, the new features can be added by new chip software based on request.
 The convenient code debug testing tool was designed during development for easy tuning
the individual coders CD32-5 and the system in general.</p>
    </sec>
    <sec id="sec-3">
      <title>4. Acknowledgments</title>
      <p>The present work was carried out with the support of the Russian Foundation for Basic
Research by grants No. 13-02-12052 and No. 16-52-55002; and by Moscow Region Government
through Grant No. 736/36-16.09.2014. Also, this work was partially supported by the internal student
grant IGA of Palacký University in Olomouc, Czech Republic, No. IGA_PrF_2015_017.</p>
      <p>Logarithmic Preamplifier, http://www.mesytec.com.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          [1]
          <string-name>
            <given-names>Yu. Ts.</given-names>
            <surname>Oganessian</surname>
          </string-name>
          and
          <string-name>
            <given-names>V. K.</given-names>
            <surname>Utyonkov</surname>
          </string-name>
          Super-heavy element research. // Rep. Prog. Phys.
          <volume>78</volume>
          ,
          <issue>036301</issue>
          (
          <year>2015</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          [2]
          <string-name>
            <given-names>Yu. S.</given-names>
            <surname>Tsyganov Yu</surname>
          </string-name>
          <string-name>
            <surname>S</surname>
          </string-name>
          ,
          <string-name>
            <given-names>V. G.</given-names>
            <surname>Subbotin</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A. N.</given-names>
            <surname>Polyakov</surname>
          </string-name>
          , et al.,
          <source>Nucl. Instrum. Methods Phys. Res</source>
          .,
          <source>Sec. A 392</source>
          ,
          <issue>197</issue>
          (
          <year>1997</year>
          ). Yu.
          <string-name>
            <given-names>S.</given-names>
            <surname>Tsyganov Yu</surname>
          </string-name>
          <string-name>
            <surname>S</surname>
          </string-name>
          ,
          <string-name>
            <given-names>V. G.</given-names>
            <surname>Subbotin</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A. N.</given-names>
            <surname>Polyakov</surname>
          </string-name>
          , et al.,
          <source>Nucl. Instrum. Methods Phys. Res</source>
          .,
          <source>Sec. A 525</source>
          , pp.
          <fpage>213</fpage>
          -
          <lpage>216</lpage>
          (
          <year>2004</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          [3]
          <string-name>
            <given-names>Yu. S.</given-names>
            <surname>Tsyganov</surname>
          </string-name>
          . et al. /
          <source>/ Proceedings of the XXIV International Symposium on Nuclear Electronics and Computing “NEC'</source>
          <year>2013</year>
          ”, Varna, Bulgaria, September 9-
          <issue>16</issue>
          ,
          <year>2013</year>
          , pp.
          <fpage>250</fpage>
          -
          <lpage>256</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          [4]
          <string-name>
            <surname>M. M. Rajabali</surname>
          </string-name>
          et al. // Phys. Rev. C
          <volume>85</volume>
          ,
          <issue>034326</issue>
          (
          <year>2012</year>
          )
          <article-title>: Mesytec GmbH &amp; Co</article-title>
          . KG, Multichannel
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          [5]
          <string-name>
            <surname>Yu</surname>
          </string-name>
          . Ts. Oganessian et al // Phys. Rev. C
          <volume>87</volume>
          ,
          <issue>054621</issue>
          (
          <year>2013</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          [6]
          <string-name>
            <given-names>R.</given-names>
            <surname>Grzywacz</surname>
          </string-name>
          et al.,
          <source>Nucl. Instrum. Methods. Phys. Res., Sect B 261</source>
          ,
          <issue>1103</issue>
          (
          <year>2007</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          [7]
          <string-name>
            <given-names>Yu. S.</given-names>
            <surname>Tsyganov Yu</surname>
          </string-name>
          <string-name>
            <surname>S</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A. N.</given-names>
            <surname>Polyakov</surname>
          </string-name>
          , Nucl. Instr. and Meth.
          <source>in Phys. Res. A 513</source>
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>