SoLID Ecal Weekly 20230727
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Revision as of 16:16, 27 July 2023 by Xiaochao (Talk | contribs) (Created page with "==SPD Timing discussion== *Carter showed his slides from previous week. SC_C - SC_D seems reasonable. See comparison table at [https://hallaweb.jlab.org/experiment/PVDIS/SoLI...")
Contents
SPD Timing discussion
- Carter showed his slides from previous week. SC_C - SC_D seems reasonable. See comparison table at SPD page, 2nd table from top. Note that HRS S2 was 50mm thick and had ~300ps resolution. Scale by 1/sqrt(Npe) or 1/sqrt(thickness) we expect 474ps for the 2-cm thick scintillators we are using. (This also means our PMT might have better "Transient Time Spread(TTS)" than the S2 PMTs.
- For LASPD timing, should plot (T+B)/2 minus another scintillator.
- Mike will post PMT information soon
Rate data/sim discussion
- from previous week, it was obvious that MIP for Shower shifted to higher values for high rate runs. Pulse deconvolution might help
- Mike will check with Jixie on the code and technical note availability. The note should contains the 2 simpler options (fixed vs. dynamic pedestal subtraction, no deconvolution). Perhaps co-writing the note?
- Ye showed 10uA run comparison throughout the 18-deg run period and the MIPs remained stable
- Jixie's pedestal study (on redmine) is without beam. Did we have one with beam?
- Ye showed SC-B pulses and it had significant higher rates and baseline shift than front scintillators. (SC-B had no beam-side shielding.) THis is okay if we want to cut on half-MIP, just need to shift the MIP position accordingly.
- For longer term we need to simulate pulse shape in SoLID full sim. This will give us: baseline shift, timing, etc.
PID classical method by Spencer
- Spencer's slide
PID ML method by Darren
- Darren's slide