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Data/MC discrepancy in FCal Matching around Beam Hole #196

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aaust opened this issue Sep 14, 2021 · 14 comments
Open

Data/MC discrepancy in FCal Matching around Beam Hole #196

aaust opened this issue Sep 14, 2021 · 14 comments

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@aaust
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aaust commented Sep 14, 2021

Comparing the monitoring plots for a recent bggen sample with the real data reconstruction, I noticed a striking difference in the track matching rate for small radii around the beam hole.

For real data (e.g. 2017), we see an accumulation of tracks matched to showers for R<20cm (bottom row, right plot). The extra showers are mostly located in the 1st quadrant, which corresponds to the region where some of the inner FCal blocks were not masked in the trigger (bottom row, left plot), but there is a second cluster below the hole.
recon_ver03

In the MC sample, this is effect is not simulated. Could there be a background component that is beam-correlated, which is not taken into account properly by the random trigger background?

mc_bggen_ver36

@rjones30
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rjones30 commented Sep 14, 2021 via email

@aaust
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aaust commented Sep 17, 2021

The trigger simulation seems to have the correct mask with the hole in the first quadrant:
image
I assume there is just no EM background to trigger any events. I will try the BeamPhotons background or directly some BH signal.

@aaust
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aaust commented Sep 21, 2021

When the trigger mask was fixed in 2018, the peak in the match rate for real data disappeared:
run 042514

@igjaegle
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For the 2017 data set, the first 3 rings are not calibrated (R < 20 cm), this is clearly seen on slide 8 of https://halldweb.jlab.org/primexd/gluex-201701/gluex_201701_method0_period_0.pdf. The pi0 peak position and width are off and much larger, respectively. Furthermore if in standard analysis, there is a fiducial cut that excludes the first 3 inner rings and the last three outer rings for photons, it must also be applied for tracks.

@igjaegle
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Related to the behavior below 1 GeV.

The current MC simulation FCAL non-linear energy correction corresponds to this https://logbooks.jlab.org/entry/3810677 but the parametrization below 1GeV is wrong as reported in https://halldweb.jlab.org/wiki-private/images/7/7c/Glue-primexd-igal-jaegle-28052020.pdf slide-6.

@sdobbs
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sdobbs commented Dec 15, 2021

Thinking a little bit more about the modeling of beam backgrounds in the FCAL, I selected the first couple inner rings and looked at a few distributions in the random and PS triggers, which should just be due to backgrounds.

For reference, here's the energy distribution for the FCAL hits:
fcal_random_energy

But one main thing to look at is the distribution of hit times:
fcal_random_time

and hit time - RF time:
fcal_random_rf_time

Note that in these events, we don't have enough information to pick out the "correct" beam bunch, but we at least see that there is a some structure correlated with the beam timing, and nothing else besides that - basically what one would expect from the random trigger.

We can look at the PS triggered events:

FCAL hit time:
fcal_ps_time

FCAL hit time - RF time:
fcal_ps_rf_time

And there is a peaking structure - this is maybe correlated to the PS event?

@rjones30
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rjones30 commented Dec 15, 2021 via email

@markito3
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The e+e- pair from a legitimate PS trigger is depositing multi-GeVs into the Hall. Are we sure that the shielding behind the PS detectors will absorb all of that energy? If not you would expect a prompt peak in the FCAL and elsewhere as well.

@sdobbs
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sdobbs commented Dec 15, 2021

Richard, Mark - interesting point. Here are timing plots where I've rejected events that have a PS coincidence within 0.5 GeV of a tagger hit, and the peak does go away. I don't quite understand the timing, though - there's about a 20 ns difference between this peak and the prompt PS time peak, which corresponds to about 6 m. I think there's a larger difference between the PS and FCAL than this...

FCAL hit time (reject PS/tagger coincidences):

fcal_ps_time-cut

FCAL hit time - RF time (reject PS/tagger coincidences):

fcal_ps_rf_time-cut

@rjones30
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rjones30 commented Dec 15, 2021 via email

@sdobbs
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sdobbs commented Dec 15, 2021

Sure, here is a zoomed in version of the above timing peak in the FCAL for PS triggered events, and also attached is the PS timing peak. The FCAL times peak at about -8 ns, while the PS times peak at about -28 ns (very roughly).

I think this should be a consistent comparison, since the PS timing is aligned to the tagger, which is aligned to the main spectrometer, but maybe there are some offsets I don't quite understand.

fcal_t_peak
ps_t_peak

@rjones30
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rjones30 commented Dec 15, 2021 via email

@rjones30
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rjones30 commented Dec 15, 2021 via email

@sdobbs
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sdobbs commented Dec 15, 2021

Richard, that is certainly possible, though we would probably want to do some more studies (and perhaps simulations?) to be convinced that this signal is really due to radiative photons and not some splash of energy from some other interaction upstream of the FCAL (there is a lot of upstream). It's a very cool possibility.

Regarding the timing, I think you're right - the tagger counters are aligned to have t=0 at z=65, so the PS should be this way as well since the PS is aligned against the tagger.

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