Attendees: Guang Yang (GY), Ciro Riccio (CR), Shih-Kai Lin (SKL), Wilf Shorrock (WS), Abraham Teklu (AT), Eric Chong (EC), Dana Douqa (DD), Perri Zilberman (PZ), Chang Kee Jung (CKJ), David Last (DL), Etam Noah (EN), Clark McGrew (CMG), David Martinez Caicedo (DMC), Rick Van Berg (RVB), Andriaseta Sitraka (AS)
CERN test beam data analysis:
LANL neutron test beam:
-
- GY: Action items all covered by the various groups included in this analysis.
-
GY: slide 4: MC spread as observed in CAPTAIN.
-
CKJ: CAPTAIN see this in data or MC? CMG: In MC as Guang sees. CKJ: Is this caused by elastics scattering? CMG: Secondary inelastic scattering but still to be understood. CKJ: We need to investigate this further.
-
CKJ: How CAPTAIN dealt with this? CMG: This was a systematics for the CAPTAIN analysis.
-
CR: comparison with models is important. CMG: True, but this mis-modelling in G4 make harder the systematics error estimation
-
- DL: Probably we have to extend it 1.8 microseconds. We can look at the raw files.
-
SKL: Is everyone going to use the same data structure? GY: Yes, we will use this structure for data and MC. CR: We are developing a software framework and you can start to use it for your studies. Email me and I’ll add you to the gitlab group where this code is stored.
-
DL: Some people refer to macropulse [Ciro: I didn’t get if it was micro or macro] as proton bunch. We can call macropulse “spill”.
-
DL: Slide 11: our trigger does not start until our second proton trigger arrives. Things you are seeing before are "mid-neutron". GY: You are not seeing the real first neutron. CKJ: This means the first MP is actually the second. GY: Yes. CKJ: If you plot the MP data you should see MP-1. Somebody should check this.
-
SKL: Slide 12: I used the wrong variable for the PE so I will redo these plots.
-
DL: Shin-Kai, can you investigate what is the actual difference in power between the MP? SKL: Yes, will do.
-
- GY: What energy corresponds to the red line on slide 5? WS: I don’t remember.
-
Important information from Wilf:
- 20 PE cut applied to CERN data to remove cross-talk. We should understand if this is still valid for LANL data analysis.
-
Cut on Dt to be used for LANL data analysis for remove gammas: -326 ns (90 m data) -278 ns (20 m data).
-
CKJ: Can you calculate the energy vs time difference?I mean the actual number. It could be useful for the future. GY: Yes we can. We already have the plot and we can translate it into a table.
-
- CKJ: What do you mean by no time delay between MPPC hits? GY: We correct for the time delay due to the fiber length.
-
CKJ: [Ciro: missed the last question]
-
GY: In the MC Eric I did not include cross-talk, but I’ve processed some MC with this information included and we will make the study Eric showed using also such MC.
-
- DD: My suggestion is to cut on the cross-talk after the voxelization and not before. For the CERN test beam data analysis we cut on the minimum charge of the three fiber and the cut is at 10 PE. Also, the time tick cut using which you get rid of the ghost voxels is too strict. You should avoid to use that and just use the cut on the energy as I suggest in the last slide. In this way, you get a better purity in terms of cross-talk and ghost hits.