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Results of the Analysis of 2004 DT Test Beam

Results of the Analysis of 2004 DT Test Beam. C. Battilana and S. Marcellini – INFN Bologna. Trigger Performance : Single Muons Di-Muons Absorber and Energy Dependance. A Sketch of the Experimental Set-Up. ~ 1 m. 10 x 10 cm² Trigger scintillator. µ beam. Iron slabs 5 cm thick.

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Results of the Analysis of 2004 DT Test Beam

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  1. Results of the Analysis of 2004 DT Test Beam C. Battilana and S. Marcellini – INFN Bologna • Trigger Performance: • Single Muons • Di-Muons • Absorber and Energy Dependance CMS week mar 05

  2. A Sketch of the Experimental Set-Up ~1 m 10 x 10 cm² Trigger scintillator µ beam Iron slabs 5 cm thick MB3 configured as MB2 MB1 CMS week mar 05

  3. Single Muon Analysis • Event selection similar to TB2003 analysis. • Muon candidates are selected in MB1 and the • output of the local trigger is studied in MB3 (or the • other way around) • Some problems to deal with: • Few Front-End problems • - Bad TDCs configuration in MB3 relevant in some cases • Some Theta BTIs were masked by mistake, which turned into a • wrong treatment of the uncorrelated Low quality triggers • (as Theta Triggers validate uncorr. Low quality Triggers in the • Phi view) CMS week mar 05

  4. Trigger Efficiency at Correct BX vs Angle F.E. problems Wrong TDC config. Higher efficiency for the emulation due to the uncorrelated Low trigger problem mentioned before. CMS week mar 05

  5. Ghost Rate at Correct BX vs angle Higher noise rate in the emulation, still due to the Low trigger problem mentioned before (most of the ghosts are uncorrelated Low triggers) CMS week mar 05

  6. Effect of the Iron Absorber vs Beam Energy ~ 1-2 % CMS week mar 05

  7. Actually when the Track Finder tries to match trigger segments from different stations, it opens a time window of ± 1 BX around the centered BX. This means that also triggers at BX=±1 with respect to the correct BX can in principle contribute to make a muon Trigger track, if they can be matched with other segments in the rest of the muon detector. This happens if they have the correct positionand bending angle, even if they occur at the wrong BX. Therefore a fraction of the triggers at wrong BX can be recovered to enhance the effective trigger efficiency. CMS week mar 05

  8. Among the triggers at BX=Correct±1 let’s assume as good (i.e which contribute to the efficiency) only the triggers which occur in the range indidated by the arrows, No iron With iron CMS week mar 05 Trigger position (trig. Units)

  9. The same also for the bending angle of the trigger segment No iron With iron CMS week mar 05 Trigger position (trig. Units)

  10. The effective efficiency can be increased only by about 0.5 % if also triggers at BX=±1 with respect to the correct BX (and with correct position and bending) are also included CMS week mar 05

  11. Efficiency gain as a function of beam energy, with and without iron, when triggers occurring at BX next to the correct one are also included. ~ 0.5 % with iron ~ 0.3 % without iron CMS week mar 05

  12. Di-Muon Analysis As the two stations were often shifted and rotated during the data taking,it is not trivial to select di-muons in one station and check the trigger performace in the other one Therefore for the moment the muon pair selection was performed as for 2003 test beam, i.e. each station was treated independently. We are developing a more accurate di-muon selection MB1 MB3 CMS week mar 05

  13. All events Di-Muon Selection Di-muons Two fitted tracks (TDC hits) in the Phi view with at least 4 hits and average Mean Timer in the espected time range (to reject off time di-muons) AND Two fitted tracks (TDC hits) n the Theta view N hits in a station (Phi) After di-muon selection CMS week mar 05 N hits in a station (Phi)

  14. Di-Muon Efficiency 1 Trig at BX=OK Most of the data usable for di-muon analysis are at 0 deg. for which effic. is lower than for other track incident angle. Good agreeement with 2003 test beam results. Good matching with emulation, also in view of the wrong uncorr. Low trigger treatment, which occurs only on Data and not in the Emulation No cases with no triggers at all (at least 1 track is always triggered) 2 Trig at BX=OK 2 Trig at BX=OK±1 Efficiency Data Emulation CMS week mar 05 ∆x between tracks (cm)

  15. Di-Muons: are the two triggers the correct ones ? Correlation between track distance and trigger distance: Ghost triggers lay out of the diagonal band ∆x between triggers(trig. units) Very few ghosts CMS week mar 05 ∆x between tracks (cm)

  16. Data Emulator Quality of the Trigger Segments 1st Trigger Server Track at correct BX Discrepancy with emulator due to wrong uncorr. Low Trigger treatment and bad TDC configuration in MB3 Li Lo Hi Ho LL HL HH 2nd Trigger Server Track at correct BX CMS week mar 05 Li Lo Hi Ho LL HL HH

  17. No absorber – 0 deg Data Emulation Small drop of efficiency when the iron absorber is placed in front of MB3, expecially when tracks are very close in space Efficiency Data With absorber – 0 deg Emulation CMS week mar 05 ∆x between tracks (cm)

  18. Incident angles different from zero 1 Trig at BX=OK 2 Trig at BX=OK 2 Trig at BX=OK±1 Efficiency Data Efficiency Data 0 deg no 0 deg Emulation Emulation CMS week mar 05 ∆x between tracks (cm) ∆x between tracks (cm)

  19. Conclusions • Trigger performances in good agreement with 2003 results. • New results from energy dependence and the effect of the iron absorber. • Some refinements of the analysis is the two-muon selection will come soon. • A written note is in preparation. • Updated results from Track Finder performaces are expected also expected (Jorge) CMS week mar 05

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