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The CDF II eXtremely Fast Tracker Upgrade

The CDF II eXtremely Fast Tracker (XFT) is the 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 candida...

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Detalles Bibliográficos
Autores principales: Fedorko, I, Abulencia, A, Errede, D, Gerberich, H, Junk, T, Kasten, M, Levine, S, Mokos, R, Pitts, K, Rogers, E, Veramendi, G, Azzurri, P, Donati, S, Staveris-Polykalas, A, Cochran, E, Efron, J, Gartner, J, Hughes, R, Johnson, M, Kilminster, B, Lannon, K, McKim, J, Olivito, D, Parks, B, Slaunwhite, J, Winer, B, Dittmann, J, Hewamanage, S, Krumnack, N, Wilson, J S, Erbacher, R, Forrest, R, Ivanov, A, Soha, A, Flanagan, G, Jones, T, Holm, S, Klein, R, Schmidt, E E, Scott, L, Shaw, T, Wilson, P J
Lenguaje:eng
Publicado: 2008
Materias:
Acceso en línea:https://dx.doi.org/10.1142/9789812819093_0159
http://cds.cern.ch/record/2119584
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author Fedorko, I
Abulencia, A
Errede, D
Gerberich, H
Junk, T
Kasten, M
Levine, S
Mokos, R
Pitts, K
Rogers, E
Veramendi, G
Azzurri, P
Donati, S
Staveris-Polykalas, A
Cochran, E
Efron, J
Gartner, J
Hughes, R
Johnson, M
Kilminster, B
Lannon, K
McKim, J
Olivito, D
Parks, B
Slaunwhite, J
Winer, B
Dittmann, J
Hewamanage, S
Krumnack, N
Wilson, J S
Erbacher, R
Forrest, R
Ivanov, A
Soha, A
Flanagan, G
Jones, T
Holm, S
Klein, R
Schmidt, E E
Scott, L
Shaw, T
Wilson, P J
author_facet Fedorko, I
Abulencia, A
Errede, D
Gerberich, H
Junk, T
Kasten, M
Levine, S
Mokos, R
Pitts, K
Rogers, E
Veramendi, G
Azzurri, P
Donati, S
Staveris-Polykalas, A
Cochran, E
Efron, J
Gartner, J
Hughes, R
Johnson, M
Kilminster, B
Lannon, K
McKim, J
Olivito, D
Parks, B
Slaunwhite, J
Winer, B
Dittmann, J
Hewamanage, S
Krumnack, N
Wilson, J S
Erbacher, R
Forrest, R
Ivanov, A
Soha, A
Flanagan, G
Jones, T
Holm, S
Klein, R
Schmidt, E E
Scott, L
Shaw, T
Wilson, P J
author_sort Fedorko, I
collection CERN
description The CDF II eXtremely Fast Tracker (XFT) is the 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 pT leptons from W/Z and heavy flavor decays and, in conjunction with the Level 2 processors, it identifies secondary vertices from beauty decays. The XFT has thus been crucial for the recent measurement of the oscilation and Σb discovery. 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 selections. This allows to mantain the trigger perfectly efficient at the record luminosities 2–3·1032 cm-2 s-1 and to mantain intact the CDF II high luminosity physics program, which includes the Higgs search. The architecture, the used technology, the performance and the impact of the upgraded XFT on the entire CDF II trigger strategy are reviewed.
id oai-inspirehep.net-1308769
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2008
record_format invenio
spelling oai-inspirehep.net-13087692019-09-30T06:29:59Zdoi:10.1142/9789812819093_0159http://cds.cern.ch/record/2119584engFedorko, IAbulencia, AErrede, DGerberich, HJunk, TKasten, MLevine, SMokos, RPitts, KRogers, EVeramendi, GAzzurri, PDonati, SStaveris-Polykalas, ACochran, EEfron, JGartner, JHughes, RJohnson, MKilminster, BLannon, KMcKim, JOlivito, DParks, BSlaunwhite, JWiner, BDittmann, JHewamanage, SKrumnack, NWilson, J SErbacher, RForrest, RIvanov, ASoha, AFlanagan, GJones, THolm, SKlein, RSchmidt, E EScott, LShaw, TWilson, P JThe CDF II eXtremely Fast Tracker UpgradeDetectors and Experimental TechniquesThe CDF II eXtremely Fast Tracker (XFT) is the 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 pT leptons from W/Z and heavy flavor decays and, in conjunction with the Level 2 processors, it identifies secondary vertices from beauty decays. The XFT has thus been crucial for the recent measurement of the oscilation and Σb discovery. 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 selections. This allows to mantain the trigger perfectly efficient at the record luminosities 2–3·1032 cm-2 s-1 and to mantain intact the CDF II high luminosity physics program, which includes the Higgs search. The architecture, the used technology, the performance and the impact of the upgraded XFT on the entire CDF II trigger strategy are reviewed.The CDF II eXtremely Fast Tracker (XFT) is the 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 pT leptons from W/Z and heavy flavor decays and, in conjunction with the Level 2 processors, it identifies secondary vertices from beauty decays. The XFT has thus been crucial for the recent measurement of the oscilation and Σb discovery. 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 selections. This allows to mantain the trigger perfectly efficient at the record luminosities 2–3·1032 cm-2 s-1 and to mantain intact the CDF II high luminosity physics program, which includes the Higgs search. The architecture, the used technology, the performance and the impact of the upgraded XFT on the entire CDF II trigger strategy are reviewed.oai:inspirehep.net:13087692008
spellingShingle Detectors and Experimental Techniques
Fedorko, I
Abulencia, A
Errede, D
Gerberich, H
Junk, T
Kasten, M
Levine, S
Mokos, R
Pitts, K
Rogers, E
Veramendi, G
Azzurri, P
Donati, S
Staveris-Polykalas, A
Cochran, E
Efron, J
Gartner, J
Hughes, R
Johnson, M
Kilminster, B
Lannon, K
McKim, J
Olivito, D
Parks, B
Slaunwhite, J
Winer, B
Dittmann, J
Hewamanage, S
Krumnack, N
Wilson, J S
Erbacher, R
Forrest, R
Ivanov, A
Soha, A
Flanagan, G
Jones, T
Holm, S
Klein, R
Schmidt, E E
Scott, L
Shaw, T
Wilson, P J
The CDF II eXtremely Fast Tracker Upgrade
title The CDF II eXtremely Fast Tracker Upgrade
title_full The CDF II eXtremely Fast Tracker Upgrade
title_fullStr The CDF II eXtremely Fast Tracker Upgrade
title_full_unstemmed The CDF II eXtremely Fast Tracker Upgrade
title_short The CDF II eXtremely Fast Tracker Upgrade
title_sort cdf ii extremely fast tracker upgrade
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1142/9789812819093_0159
http://cds.cern.ch/record/2119584
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