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Status of test beam analysis. Aleksei Pavlinov WSU. Used provided MTEST DAQ incl. scintillator to define the beam, muon veto scintillator after beam dump + 3 stations with a total of 14 MWPC layers with 1mm wire spacing. [numbers below are all in inches].
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Status of test beam analysis Aleksei Pavlinov WSU Aleksei Pavlinov
Used provided MTEST DAQ incl. scintillator to define the beam, muon veto scintillator after beam dump + 3 stations with a total of 14 MWPC layers with 1mm wire spacing. [numbers below are all in inches] FNAL meson test beam line Muon veto, Scint. Cherenkov Aleksei Pavlinov
Key improvements of Test Beam analysis • Calibration procedure itself. • We had two problems: • a) Led measurements • b) Big difference in resolution for one run and for groups of runs Answer: Dependence of APD gain from APD bias -> we can not set the same APD bias after bias scan => gain changes. We have to recalibrate our detector after each bias scan. Aleksei Pavlinov
Tracking of PWC. The satellite peak problem has been solved and the mean of residuals are properly around zero for all planes. Noisy MWPC-plane6 was removed from tracking. We can do now coordinate business with EMCAL. a) we have to do alignment between MPWC and EMCAL (can use all statistics in this case) => spatial resolution in vertical(horizontal) directions; => profile measurement (0 reconstruction – separation of overlapping showers) Tracking of PWC (Akitomo Enokizono). Aleksei Pavlinov
Resolution – 3GeV All patch - 6.78%; N(el) = 1902+/-55 RP - 6.09%; N(el) = 362+/-23 LP - 6.92%; N (el) = 1321 +/- 45 Aleksei Pavlinov
Resolution – 8 GeV All patch - 4.32%; N(el) = 206700; RP - 4.30%; N(el) = 68800; LP - 4.56%; N(el) = 76900; Aleksei Pavlinov
Resolution – 16 GeV All patch - 3.70%; N(el) = 109200; RP - 3.48%; N(el) = 30200; LP - 3.86%; N(el) = 60600; Aleksei Pavlinov
Resolution – 33 GeV All patch - 2.76%; N(el) = 4096; RP - 2.55%; N(el) = 1021; LP - 2.97%; N(el) = 2165; Aleksei Pavlinov
Resolution – final picture( = 0.0) • We understand our device, accepted statistics and • the calibration procedure enough good. • EMCAL resolution result is reasonable relatively • MC and similar detector (PHENIX) Aleksei Pavlinov
EMCAL spatial resolution • Exponential shape of shower (GAMS) • Log weight method Aleksei Pavlinov
Shower coordinate – I (sh) Exponential shower model (Akopdjanov et al., NIM (1977) 441-445, GAMS coll.) Aleksei Pavlinov
YCoG vs. YPWC b~0.54 cm(0.13 cell unit) b~0.85 cm => Phenix Aleksei Pavlinov
Ysh vs. YPWC Aleksei Pavlinov
Shower coordinate – II(log) (T.C.Awes et al., NIM A311, 130-138,1992 ) Typical value of w0 is 4-5. I am using 4.4. Aleksei Pavlinov
Ylog vs. YPWC Aleksei Pavlinov
8GeV – spatial resolution summary • Both methods give approximately the same value • of resolution (~4 mm at 8GeV/C) • Y (vertical) direction has a little bit better resolution than • X (horizontal) direction. Aleksei Pavlinov
Spatial resolution vs. beam momentum po+p1/sqrt(p) 0.155+0.57/sqrt(E) - PHENIX Aleksei Pavlinov
Dependence of spatial resolution from parameters:b and w0 Best values: b ~ 0.13 in cell unit, 0.55 cm w0 ~ 4.4-4.5 Aleksei Pavlinov
Shower profile – I Aleksei Pavlinov
Shower profile – II Aleksei Pavlinov
One dimensional vertical shower profile Aleksei Pavlinov
Conclusion • We understand our device, accepted statistics and • calibration procedure enough good. • EMCAL result is reasonable relatively • MC and similar detector (PHENIX.GAMS) • EMCAL resolution as for short shaper time as for long shaper time fulfills the requirement – 12/E+2. • Shower shape business is not so understandable now Aleksei Pavlinov
Backup slide Aleksei Pavlinov
Dependence resolution vs. entry point (8GeV/c) Aleksei Pavlinov
Dependence MIP(MOP) vs. entry point (16GeV/c) Aleksei Pavlinov
MIP , all statistics, 16 GeV, =0 Aleksei Pavlinov
MIP, 8GeV, tilt 100, ncell=1 Aleksei Pavlinov
MIP, 8GeV, tilt 100, ncell=2 Aleksei Pavlinov
MIP calibration table Aleksei Pavlinov