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    <p>Folks,</p>
    <p>Please find the minutes <a moz-do-not-send="true"
href="https://halldweb.jlab.org/wiki/index.php/HDGeant4_Meeting,_March_26,_2019#Minutes">here</a>
      and below.</p>
    <p>  -- Mark</p>
    <p>_____________________________________</p>
    <p> </p>
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          <h1 id="firstHeading" class="firstHeading" lang="en"><span
              dir="auto">Minutes, HDGeant4 Meeting, March 26, 2019</span></h1>
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              <p>Present: </p>
              <ul>
                <li> <b> JLab: </b> Alex Austregesilo, Thomas Britton,
                  Sean Dobbs, Mark Ito (chair),Richard Jones, Simon
                  Taylor</li>
              </ul>
              <p>There is a <a rel="nofollow" class="external text"
                  href="https://bluejeans.com/s/96_2v"
                  moz-do-not-send="true">recording of this meeting</a>
                on the BlueJeans site. Use your JLab credentials to
                access it. </p>
              <h3><span class="mw-headline"
                  id="Review_of_minutes_from_the_last_meeting">Review of
                  minutes from the last meeting</span></h3>
              <p>We went over <a
href="https://halldweb.jlab.org/wiki/index.php/HDGeant4_Meeting,_March_12,_2019#Minutes"
                  title="HDGeant4 Meeting, March 12, 2019"
                  moz-do-not-send="true">the minutes</a> without
                significant comment. </p>
              <h3><span class="mw-headline"
                  id="Do-over_on_comparison_studies">Do-over on
                  comparison studies</span></h3>
              <p>Simon has run some single-particle gun simulations for
                both HDG3 and HDG4 on the OSG. He has not had a chance
                to look at them in detail yet. His initial impression is
                that differences are seen in calorimetry. </p>
              <h3><span class="mw-headline"
                  id="Further_comparative_studies_of_calorimeter_response">Further
                  comparative studies of calorimeter response</span></h3>
              <p>Richard showed <a rel="nofollow" class="external text"
href="https://docs.google.com/presentation/d/1IDw4LD2GhBpzam9E1V8LRBcb49Kb1V3GMTWR2Inw2V8/edit?usp=sharing"
                  moz-do-not-send="true">some slides</a> describing
                extensions of his work on low-level comparisons of HDG3
                and HDG4 for calorimetry. </p>
              <ul>
                <li> He looked at the residual non-linearity, albeit up
                  to 8 GeV, for reconstructed shower energy in the FCAL.
                  Agreement between HDG3 and HDG4 is very good now, at
                  all energies.</li>
                <li> He has examined cluster time, relative to "RF".
                  Both HDG3 and 4 show the same linear systematic
                  dependence in relative time as a function of energy.</li>
                <li> For BCAL energy response, he showed the same
                  residual non-linearity study as shown earlier for the
                  FCAL. Here the qualitative agreement is good, with
                  perhaps an 8 MeV upward shift of HDG4 relative to
                  HDG3. The effect of energy leakage out the back of
                  BCAL dominates the changes in the trends as polar
                  angle moves from far forward to 90 degrees.</li>
                <li> For BCAL timing, he noted a difference in the
                  algorithm used to get cluster timing between HDG3 and
                  HDG4
                  <ul>
                    <li> HDG3 uses energy-weighted average shower times</li>
                    <li> HDG4 uses the earliest hit per sector for times</li>
                  </ul>
                </li>
                <li> We noted that mcsmear smears the BCAL timing by 55
                  ps, not a lot. Richard sees this in his study.</li>
                <li> The difference in the BCAL algorithms does not make
                  much apparent difference. He suggests we use energy
                  weighted for both to be consistent.</li>
                <li> Richard is planning to deprecate the bcalSiPMUpHit
                  and bcalSiPMDownHit elements in HDDM in favor of a
                  single bcalTruthCell element that can serve
                  information from both upsteam and downstream ends of
                  the BCAL,</li>
                <li> There is still an issue that Alex sees with the ρ's
                  albeit with charged tracks and not electromagnetic
                  showers. Hopefully Simon's single-track studies will
                  address it.</li>
              </ul>
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          <li id="lastmod"> This page was last modified on 29 March
            2019, at 13:25.</li>
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