Minutes of the muon software meeting, 27 Oct 04 ================================================ 1. Track chisq cut for MC. ============================ Else and Victoria see a different distribution for track chisq, when using the same zewk3m data sample. This is under continued investigation. 2. Cosmic tagger cuts. ======================= Summary of our discussion. Comments from Pasha, Slava, Anyes, Chris. Two problems have become apparent in the past few weeks: (1) The cut on the chisq of the di-cosmic (helix) fit is too loose for the tracking resolution in 5.3. (2) The cosmic tagger is not tagging events a low-pt. This is best illustrated by a sample from Angela Wyatt, who is looking for diffractive J/psi events. The signal is typified by 2.5 GeV muons plus photons. From a sample of 27 events she sent us, 26 were cosmics, but none were tagged as such. We have already changed the cut on the chisq of the di-cosmic fit from 300 to 1000. We discussed what other changes to make. We decided to change the cuts to identify a seed track to >=5 hits on >=2 axial and >=2 stereo tracks (same as defTracks in 5.3). We also decided to put the minimum pt required to identify the seed track in the tcl file so users who want/need to change change it for their analysis. Reducing the pt required to identify the seed track to 1.4GeV may increase the over-efficiency of the tagger, so it is something we don't want to do by default. Users of low-pt analysis where the cosmic background is large will have to tune the cosmic rejection themselves. Two other issues, that we should be addressed in the long term: i. At low-pt enemy loss effects become important in the tracking: this should be taken into account in the di-cosmic fit. ii. At low-pt the road width to find the cosmic ray is not wide enough. 3. Pasha: Simulation of the energy associated with the muon ============================================================== Pasha showed that the simulation of the hadronic energy associated to CMX muons is not well described at |x_ces|>23 cm. This why the distributions of energy for CMX muons is not well described in the MC. There is no such problem with CMUP muons. 4. Victoria: Updates to the standard muon cuts ================================================= We agreed to remove the cut on minimum energy for CMUP and CMX muons. The spike at Eem+Ehad=0 tends to come from CMX muons that are not fiducial in the CEM. For stubless muons (CMIO) a cut at Eem+Ehad>0 reduces the fake rate significantly and is still a good cut. Pasha and Chris disagreed what to do about stubless muons that go through a calorimeter crack (eg fidEle=0), where the energy cannot be reconstructed. Pasha said they should be rejected, Chris would like to keep them for more acceptance. We still don't understand the |dxCMU|>3cm muons. So we've decided to keep the cut a |dxCMU|<3cm. If the problem is easily fixed then we could run it when we remake our ntuples. [After the meeting we looked at these muons, and we are still trying to work out exactly what the problem is.]