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<p class="MsoNormal"><b>From:</b> Raffaella De Vita <devita@jlab.org> <br>
<b>Sent:</b> Tuesday, February 26, 2019 12:29<br>
<b>To:</b> Nathan Baltzell <baltzell@jlab.org>; Stepan Stepanyan <stepanya@jlab.org>; Annalisa D'Angelo <annalisa.dangelo@roma2.infn.it>; Lucilla Lanza <lucilla.lanza@roma2.infn.it>; William Phelps <wphelps@jlab.org>; Eugene Pasyuk <pasyuk@jlab.org>; Derek
Glazier <Derek.Glazier@glasgow.ac.uk>; Marco Battaglieri <battaglieri@ge.infn.it><br>
<b>Subject:</b> Re: FT-based PID<o:p></o:p></p>
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<p class="MsoNormal">Now with the attachment.<o:p></o:p></p>
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<br>
> On 26 Feb 2019, at 18:28, Raffaella De Vita <<a href="mailto:devita@jlab.org">devita@jlab.org</a>> wrote:<br>
> <br>
> Dear All,<br>
> I have continued working on testing different PID schemes for events with no electrons in the FD but in the FT.<br>
> I have included in attachment a set of slides summarizing the results. Basically, I compared the results obtained by using simply the most energetic electron in the FT with what obtained by looking for the best time coincidence between FT electrons and tracks
in the FD. The latter is quite similar to what was done in CLAS for photon runs.<br>
> My preference, based on the results, would be for the second algorithm but, to conclude, it would be good to test it on some exclusive final state to see what the performance are.<br>
> Let me know if you have comments or suggestions.<br>
> Best regards,<br>
> Raffaella<o:p></o:p></p>
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