The CIDF II eXtremely Fast Tracker (XFT) is a trigger processor which reconstructs charged particle tracks in the transverse plane of the central tracking chamber. The XFT tracks are also extrapolated to the electromagnetic calorimeter and muon chambers to generate trigger electron and muon candidates. The XFT is crucial for the entire CDF II physics program: it detects high P(t) lepton from WIZ and heavy flavors decay and, in conjunction with the level 2 processor, it identifies secondary vertices from beauty decay. The XFT has thus been crucial for the recent measurement of the B(5)(0) oscillation and Sigma(b). The increase of the Tevatron instantaneous luminosity demanded an upgrade of the system to cope with the higher occupancy of the chamber. In the upgraded XFT three-dimensional tracking reduces the level of fake tracks and measures the longitudinal track parameters, which strongly reinforce the trigger selection. This allows to maintain the trigger perfectly efficient at the record luminosities 2-3 x 10(32) cm(-2) s(-1) and to maintain intact the CDF II high luminosity physics program, which includes the Higgs search. In this paper we review the architecture, the used technology, the performance and the impact of the upgraded XFT on the entire CDF II trigger strategy. (C) 2008 Elsevier B.V. All rights reserved.

eXtremely Fast Tracker trigger upgrade at CDF

DONATI, SIMONE;
2009-01-01

Abstract

The CIDF II eXtremely Fast Tracker (XFT) is a trigger processor which reconstructs charged particle tracks in the transverse plane of the central tracking chamber. The XFT tracks are also extrapolated to the electromagnetic calorimeter and muon chambers to generate trigger electron and muon candidates. The XFT is crucial for the entire CDF II physics program: it detects high P(t) lepton from WIZ and heavy flavors decay and, in conjunction with the level 2 processor, it identifies secondary vertices from beauty decay. The XFT has thus been crucial for the recent measurement of the B(5)(0) oscillation and Sigma(b). The increase of the Tevatron instantaneous luminosity demanded an upgrade of the system to cope with the higher occupancy of the chamber. In the upgraded XFT three-dimensional tracking reduces the level of fake tracks and measures the longitudinal track parameters, which strongly reinforce the trigger selection. This allows to maintain the trigger perfectly efficient at the record luminosities 2-3 x 10(32) cm(-2) s(-1) and to maintain intact the CDF II high luminosity physics program, which includes the Higgs search. In this paper we review the architecture, the used technology, the performance and the impact of the upgraded XFT on the entire CDF II trigger strategy. (C) 2008 Elsevier B.V. All rights reserved.
2009
Abulencia, A.; Azzurri, P.; Cochran, E.; Cox, C.; Cox, D.; Dittmann, J.; Donati, Simone; Efron, J.; Erbacher, R.; Errede, D.; Fedorko, I.; Flanagan, G.; Forrest, R.; Gerberich, H.; Gartner, J.; Hewamanage, S.; Holm, S.; Hughes, R.; Ivanov, A.; Jones, T.; Johnson, M.; Junk, T.; Kasten, M.; Kilminster, B.; Klein, R.; Krumnack, N.; Lannon, K.; Levine, S.; Lister, A.; Mckim, J.; Mokos, R.; Olivito, D.; Parks, B.; Pitts, K.; Rogers, E.; Sartori, L.; Schmidt, E.; Scott, L.; Shaw, T.; Slaunwhite, J.; Soha, A.; Veramendi, G.; Wilson, P. J.; Wilson, J. S.; Winer, B.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/134941
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