[Halld-offline] HDGeant4 Meeting Minutes, March 9, 2021
Mark Ito
marki at jlab.org
Mon Mar 15 15:14:37 EDT 2021
Folks,
Please find the minutes here
<https://halldweb.jlab.org/wiki/index.php/HDGeant4_Meeting,_March_9,_2021#Minutes>
and below.
-- Mark
__________________________________________
HDGeant4 Meeting, March 9, 2021, Minutes
Present: Tegan Beattie, Mark Ito (chair), Richard Jones, Zisis
Papandreou, Churamani Paudel, Lubomir Pentchev, Justin Stevens, Simon
Taylor, Nilanga Wickramaarachchi
There is a recording of this meeting
<https://bluejeans.com/s/wKdTln_kEz3/> on the BlueJeans site. Log into
the BlueJeans site first to gain access (use your JLab credentials).
Review of minutes from the last meeting
We went over the minutes from February 23rd
<https://halldweb.jlab.org/wiki/index.php/HDGeant4_Meeting,_February_23,_2021#Minutes>.
Richard has already made the proposed changes to the
tagger-hit-to-energy conversion
<https://mailman.jlab.org/pipermail/halld-offline/2021-February/008475.html>.
Pull requests await merging in the halld_recon and halld_sim repositories.
New wiki page: Particle Gun Collection
Richard described an upcoming historical catalog of single particle gun
simulations. See his new wiki page
<https://halldweb.jlab.org/wiki/index.php/Particle_Gun_Collection> for
the complete description.
Issues on GitHub
We went over the issues <https://github.com/JeffersonLab/HDGeant4/issues>.
Hits in both CALs from the same track
Lubomir led us through a discussion of Issues on GitHub
<https://github.com/JeffersonLab/HDGeant4/issues/185>. Two ideas that
came up:
* There might be an effect where a charged particle's trajectory is
extrapolated beyond what is reasonable, allowing it to hit the FCAL
and create a spurious match there.
* Particles that clip the corner of the BCAL and send parts of the
shower into the FCAL could explain some of the double matching. This
behavior could be different between G3 and G4.
For all the details, see the Issue itself, linked above.
Proton timing in the BCAL
Again, Issue #179 <https://github.com/JeffersonLab/HDGeant4/issues/179>
has mainly to do with late hits in the BCAL from charged hadrons. Tegan
presented results from a study to determine the physical mechanism for
the late hits, as usual,comparing the effects among G4, G3/HADR1, and
G3/HADR4. It turns out identifying parent particles for the particles
creating late hits was not possible in an unambiguous manner. He was
able to plot the timing distributions for the various physical
interaction mechanisms separately, again comparing the different Geant
engines. In fact, some of these interactions happen quite late, tens of
nanoseconds after the event.
For all of the details see Tegan's plots on the DocDB
<https://halldweb.jlab.org/doc-private/DocDB/ShowDocument?docid=4878>.
They are the ones with "MAR04" in the name.
G3/G4 Difference in FDC wire efficiency at the cell boundary
Richard reported on the root cause of Issue #181
<https://github.com/JeffersonLab/HDGeant4/issues/181>. Interestingly,
the G3 simulation agrees better with the data because of the requirement
that only one cell in a layer is hit. This artificially eliminates hits
from tracks that spend a small amount of time in a cell, but happily
since those trajectory have lower detection efficiency, their
elimination mimics what is seen in data. The G4 simulation has no such
mechanism for eliminating corner-clipping tracks and so hits with long
drift times are produced at a rate higher than seen in the data.
See the Issue, linked above, for a more detailed explanation, with
diagrams.
We seemed to be forming a consensus that Richard should allow multiple
hits per layer, but implement an efficiency function that reduced the
number of large DOCA hits.
[Added in press: in the issue itself you will see Richard's description
of adding actual wires to the FDC simulation geometry.]
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