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    If there  will be significant events in the side peaks, then they
    have to be subtracted?<br>
    <br>
    <div class="moz-cite-prefix">On 20.02.23 11:59, Richard Jones wrote:<br>
    </div>
    <blockquote type="cite"
cite="mid:CABfxa3QSFcJUvoFmMyj+cSiZUrxTFSdYmdJmz5=6jvnMsfELUA@mail.gmail.com">
      <meta http-equiv="content-type" content="text/html; charset=UTF-8">
      <div dir="ltr">Hi,
        <div><br>
        </div>
        <blockquote class="gmail_quote" style="margin:0px 0px 0px
          0.8ex;border-left:1px solid rgb(204,204,204);padding-left:1ex">one
          thing that can be done is to drag along events gated on RF
          side peaks. Then you can see whether significant amounts of
          accidentals are left after full analysis.<br>
        </blockquote>
        <div><br>
        </div>
        <div>This would mean opening up the primary coincidence peak
          window to include side peaks, and then looking at the time
          spectrum for the final sample after all cuts, right? No
          question, there will be significant events in the side peaks
          from this investigation for any final state extracted from
          GlueX phase II running. This is the reality for tagged
          experiments, otherwise we could do event-by-event tagging. But
          the argument is that it doesn't matter because the mistake you
          are making by selecting the wrong tag "doesn't get it wrong by
          much". The challenge here is what to use for the flux that
          goes with this analysis, because the flux is only defined for
          an accidentals-subtracted yield.</div>
        <div><br>
        </div>
        <div>-Richard Jones</div>
        <br class="gmail-Apple-interchange-newline">
      </div>
      <br>
      <div class="gmail_quote">
        <div dir="ltr" class="gmail_attr">On Mon, Feb 20, 2023 at 5:44
          AM Susan Schadmand via Halld-tagger <<a
            href="mailto:halld-tagger@jlab.org" moz-do-not-send="true"
            class="moz-txt-link-freetext">halld-tagger@jlab.org</a>>
          wrote:<br>
        </div>
        <blockquote class="gmail_quote" style="margin:0px 0px 0px
          0.8ex;border-left:1px solid rgb(204,204,204);padding-left:1ex">
          <div>
            <div
style="background-color:rgb(255,235,156);width:100%;border-style:none;border-color:rgb(250,235,204);border-width:1pt;padding:10pt;font-size:11pt;line-height:12pt;font-family:Calibri;color:rgb(0,0,0);text-align:left"><span
                style="color:rgb(156,101,0)"></span>*Message sent from a
              system outside of UConn.*</div>
            <br>
            <div>Hi,<br>
              <br>
              one thing that can be done is to drag along events gated
              on RF side peaks. Then you can see whether significant
              amounts of accidentals are left after full analysis.<br>
              <br>
              Su.<br>
              <br>
              <div>On 20.02.23 11:33, Richard Jones via Halld-tagger
                wrote:<br>
              </div>
              <blockquote type="cite">
                <div dir="ltr">
                  <div class="gmail_quote">
                    <div dir="ltr">Hello Peter,
                      <div><br>
                      </div>
                      <div>Thanks for asking, I noticed this as well,
                        but I thought it was only being used for PWA
                        where the primary focus is on the angular
                        distributions. I agree that it is a concern for
                        differential cross sections. You are right that
                        this is not properly taking into account the
                        accidentals that are present. Essentially it
                        amounts to a hybrid between a fully tagged and a
                        fully untagged experiment. Here are those two
                        extremes:</div>
                      <div>
                        <ol>
                          <li>A(untagged) -- the photon energy is
                            inferred from the reconstructed final state,
                            and used to compute all of the beam
                            properties associated with the event: the
                            flux, the polarization, etc.</li>
                          <li>B(fully tagged) -- the photon energy is
                            inferred from the unambiguously associated
                            hit in the tagger, which is used as input to
                            the kinematic fit and to lookup beam
                            properties for the event</li>
                        </ol>
                        <div>At the rates of GlueX phase 2, we do not
                          have the luxury of option 2 on an
                          event-by-event basis, but we can achieve it by
                          accidentals subtraction. Short of full
                          accidentals subtraction there are several
                          short-cuts you can use. All of these have
                          uncontrolled systematics.</div>
                      </div>
                      <div>
                        <ol>
                          <li>best chi square - put them all in a ring
                            and take the last man standing as the winner
                            with weight 1</li>
                          <li>weighted average - count them all above
                            some chi-square acceptance cut and weight
                            each event by 1/n where n is the number of
                            surviving tags</li>
                        </ol>
                        <div>Both of these methods reduce to tagging
                          strategy A(tagged) at low rate, while they
                          reduce to strategy B(untagged) at high rate.
                          At GlueX Phase II intensities we are some
                          intermediate hybrid of the two with these
                          shortcuts, certainly not approximating B(fully
                          tagged).</div>
                        <div><br>
                        </div>
                        <div>To see what these short-cuts entail,
                          consider the high-rate limit in the tagger. At
                          high rate, the extracted cross section goes to
                          infinity for a realistic tagger and an ideal
                          GlueX detector. In reality, the asymptote
                          would be something greater than one, channel
                          and final state dependent, and probably run
                          period dependent as well. The reason for this
                          is that the tagger detection efficiency per
                          beam photon goes down at high rate, while the
                          accidentals continue to grow and generate a
                          valid result for any reconstructed final
                          state, tagged or untagged. So the flux that
                          you need to put into the denominator under the
                          yield for extracting a cross section will be
                          different depending on the final state. Using
                          the same flux regardless of final state could
                          be a leading cause for why we are seeing
                          different cross sections for the charged and
                          neutral decays of eta.</div>
                        <div><br>
                        </div>
                        <div>Beyond that, the shape of the flux spectrum
                          (and the polarization spectrum for polar
                          observables) is different from the shape of
                          the energy dependence of the reconstructed
                          yield. Take for example the energy-dependent
                          cross section around the coherent edge. The
                          tagged flux has a sharp edge, whereas the
                          reconstructed yield washes out the edge with a
                          resolution that depends on everything in
                          sight: the kinematic fit cut, conditions in
                          the detector, the particular final state, etc.
                          One way to reduce our dependence on the
                          different beam photon energy resolutions in
                          the flux and yields is to average over a wide
                          range in beam energy. As long as we are not
                          interested in the s-dependence of the cross
                          section, this might be justified and would
                          reduce the systematics from these short-cut
                          approaches.</div>
                      </div>
                      <div><br>
                      </div>
                      <div>In PWA, i understand that this avoids the
                        pain of negative weights and so improves the
                        statistical error from the fits (or at least it
                        gives that feeling). In fact, it introduces a
                        set of new systematic errors of its own that
                        will probably drive us back to the more rigorous
                        approach before we are done. For the moment I am
                        not speaking up about this because we just need
                        to get our first results out. But eventually
                        this needs to be given a critical review. I hope
                        to be part of that at some level, as soon as my
                        work on photon beam systematics reaches a level
                        where it can be used for publications.</div>
                      <div><br>
                      </div>
                      <div>-Richard Jones</div>
                    </div>
                    <br>
                    <div class="gmail_quote">
                      <div dir="ltr" class="gmail_attr">On Sun, Feb 19,
                        2023 at 11:13 AM Peter Hurck <<a
                          href="mailto:Peter.Hurck@glasgow.ac.uk"
                          target="_blank" moz-do-not-send="true"
                          class="moz-txt-link-freetext">Peter.Hurck@glasgow.ac.uk</a>>
                        wrote:<br>
                      </div>
                      <blockquote class="gmail_quote" style="margin:0px
                        0px 0px 0.8ex;border-left:1px solid
                        rgb(204,204,204);padding-left:1ex">
                        <div>
                          <div
style="background-color:rgb(255,235,156);width:100%;border-style:none;border-color:rgb(250,235,204);border-width:1pt;padding:10pt;font-size:11pt;line-height:12pt;font-family:Calibri;color:rgb(0,0,0);text-align:left"><span
                              style="color:rgb(156,101,0)"></span>*Message
                            sent from a system outside of UConn.*</div>
                          <br>
                          <div>
                            <div>Hi Richard,</div>
                            <div><br>
                            </div>
                            <div>During the collaboration meeting a few
                              people presented analyses which used a
                              chi^2 ranking with a +-2ns cut around the
                              RF peak instead of tagger accidental
                              subtraction.</div>
                            <div><br>
                            </div>
                            <div>My initial thought was that this is
                              wrong and not recommended. Did the
                              guidance by the beam line group change
                              regarding this issue? Given that the
                              current a2 cross-section analysis is using
                              this method and there is a big push to
                              publish it asap I am concerned that this
                              might not be resolved properly and might
                              set a bad precedent going forward.</div>
                            <div><br>
                            </div>
                            <div>Given that you are the expert on this
                              topic, what are your thoughts on this
                              issue? Is that a legitimate way to perform
                              analyses?</div>
                            <div><br>
                            </div>
                            <div>Cheers,</div>
                            <div>Peter</div>
                            <div><br>
                            </div>
                            <br>
                            <div>
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                                            <div><font color="#7b7b7b">----------------------------------------------------<br>
                                                Dr Peter Hurck (né
                                                Pauli)<br>
                                                <br>
                                                My new email address is</font></div>
                                            <div><font color="#7b7b7b"><a
href="mailto:Peter.Hurck@glasgow.ac.uk" target="_blank"
                                                  moz-do-not-send="true"
class="moz-txt-link-freetext">Peter.Hurck@glasgow.ac.uk</a></font></div>
                                            <div><font color="#7b7b7b"><br>
                                                Research Associate<br>
                                                Nuclear and Hadron
                                                Physics Research<br>
                                                School of Physics and
                                                Astronomy<br>
                                                University of Glasgow</font></div>
                                          </div>
                                        </div>
                                      </div>
                                    </div>
                                  </div>
                                </div>
                              </div>
                            </div>
                            <br>
                          </div>
                        </div>
                      </blockquote>
                    </div>
                  </div>
                </div>
                <br>
                <fieldset></fieldset>
                <pre>_______________________________________________
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