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Pedestal Stability Plots
Updated on Mon, 2008-06-09 12:57. Originally created by mattheww on 2008-06-09 10:52.These plots compare the pedestals in each of the 4 barrel detectors for runs 9047017 and 9064017. These are from the first and last fills that had the BSMD in the run.
Cuts on the data
Updated on Mon, 2009-11-30 14:05. Originally created by gdwebb on 2008-06-09 10:41.
SMD Sector Edge Effects
Updated on Sun, 2008-06-08 15:15. Originally created by jwebb on 2008-06-08 15:15.0.0 Data Sample and Cuts
Geometry for 2007 simulation
Updated on Mon, 2008-06-09 14:16. Originally created by bouchet on 2008-06-08 09:06.root4star -q -b bfc.C\(1,10,\"trs,srs,ssd,fss,y2005f,Idst,IAna,l0,tpcI,fcf,Tree,logger,ITTF,Sti,genvtx,SvtIt,SsdIt,geant,-evout,IdTruth,tags,bbcSim,tofsim,emcY2,EEfs,-GeantOut,big,-dstout,fzin
Underlying Event
Updated on Thu, 2011-12-15 19:17. Originally created by gdwebb on 2008-06-06 09:48.Slides for Spectra Meeting 06/05/2008
Updated on Thu, 2008-06-05 09:18. Originally created by chajecki on 2008-06-05 09:18.Few slides I wanna show at Spectra Meeting.
MC pT spectra after various cuts
Updated on Tue, 2008-06-03 14:00. Originally created by rcorliss on 2008-06-03 14:00.There was some concern about the effectiveness of the proposed cuts at different cluster energies, so here are plots showing exactly that.
Lorentz effect on charged tracks
Updated on Tue, 2008-07-15 08:29. Originally created by bouchet on 2008-06-02 17:23.For this study, I generated 1000 pions +/- per event with :
Statistical Errors for data and simulation for 2006 dijet cross section
Updated on Wed, 2008-05-28 16:45. Originally created by mattheww on 2008-05-28 16:45.For both data and simulation, I calculated the distribution of cos(theta*), 1/2(eta3 + eta4), and invariant mass. The simulation jets were appropriately weighted.
Silicon hits
Updated on Tue, 2008-05-27 15:47. Originally created by bouchet on 2008-05-25 10:00.We put the silicon hits information for analysis code.
cuts used :
nHitsFit >20
|eta|<1.0
dcaGlobal <1.5
nFit/nPoss >0.52