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[Sphenix-physics-l] [minutes] Heavy Flavor/Quarkonium TG meeting Wed Nov 15 at 1:30PM ET
- From: "Huang, Jin" <jhuang AT bnl.gov>
- To: "Sphenix-upsilons-l AT lists.bnl.gov" <Sphenix-upsilons-l AT lists.bnl.gov>, "sphenix-hf-Jets-l AT lists.bnl.gov" <sphenix-hf-jets-l AT lists.bnl.gov>
- Cc: "sphenix-physics-l AT lists.bnl.gov" <sphenix-physics-l AT lists.bnl.gov>
- Subject: [Sphenix-physics-l] [minutes] Heavy Flavor/Quarkonium TG meeting Wed Nov 15 at 1:30PM ET
- Date: Wed, 15 Nov 2023 20:11:38 +0000
D0 reco: Thomas Marshall
Cameron/Thomas: primary_vertex_z is a reconstructed vertex value that is different Tony: curious about the truth vertex distribution. The reco histogram has a hard cut in the misalignment simulation. We can simulate a flat vertex distribution for a test too
Slide 3, D0 mass vs pT: Thomas: uncertainty produced is from TProfile Jin: invariant mass has a large tail, and a slice-by-slice Gaussian fit would be a better approach
Sdlie 17+: Tony: MVTX is an important anchor of the track at the inner radius. Just the misalignment is not critical for that. Tony/Jin: silicon misalignment will matter a lot on DCA and impact the D0 efficiency via decay topological cuts
Lambda-c reconstruction with TPC PID
Joe: truth reco map not existing?
Marzia: pT matching may be too tight
Marzia: a deeper look into the chi2 cut Joe/Jin: The matched track appears to have much better Chi2, which is a survival bias Tony: Chi2/ndof < 2 leads to a strange subset of tracks, suggesting relaxing to a higher value of 5-10
Jin: the peak at Chi2/ndof<1 is strange. Cameron: no-matched track leads to Chi2/ndof ->0 Charles: these are reconstructed tracks. Need some investigation.
Peak shape: Jin: The right side needs to be zoomed into the peak region to conclude the invariant mass resolution. On the left side, the pT-matched plot has a survival bias that rejects the tail. But the main resolution could be similar after zoom-in around the peak region.
Wei/Cameron: PID-mass is used in the resonance reconstruction Jin: Proton-assumption in Kalman filter fit would be useful to get the best resolution, especially for low momentum proton (p<2 GeV)
Slide 21+ Charles: proton-track only is used in these efficiency studies
Zhaozhong: b-bar is included in the simulation sample so both prompt and non-prompt Lc are included in this study
Tony: efficiency has a strong vertex dependence.
______________________________
Jin HUANG
Physicist, Ph.D. Brookhaven National Laboratory Physics Department, Bldg 510 C Upton, NY 11973-5000
Office: 631-344-5898 Cell: 757-604-9946 ______________________________
From: Huang, Jin
Dear all
Reminder of our joint Heavy Flavor/Quarkonium TG meeting
Wed Nov 15 at 1:30PM ET.
______________________________
Jin HUANG
Physicist, Ph.D. Brookhaven National Laboratory Physics Department, Bldg 510 C Upton, NY 11973-5000
Office: 631-344-5898 Cell: 757-604-9946 ______________________________
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[Sphenix-physics-l] [reminder] Heavy Flavor/Quarkonium TG meeting Wed Nov 15 at 1:30PM ET,
Huang, Jin, 11/14/2023
- [Sphenix-physics-l] [minutes] Heavy Flavor/Quarkonium TG meeting Wed Nov 15 at 1:30PM ET, Huang, Jin, 11/15/2023
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