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1
Measurement of the average time-integrated mixing probability of b-flavored hadrons produced at the Fermilab Tevatron
Published 2004“…The observed ratio of LS to OS dileptons leads to a measurement of the average time-integrated mixing probability of all produced b-flavored hadrons which decay weakly, χ̄=0.152±0.007 (stat)±0.011 (syst), that is significantly larger than the world average χ̄=0.118±0.005. © 2004 The American Physical Society.…”
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2
Search for resonant production of tt̄ pairs in 4.8fb-1 of integrated luminosity of pp̄ collisions at √s=1.96TeV
Published 2011“…We search for resonant production of tt̄ pairs in 4.8fb-1 integrated luminosity of pp̄ collision data at √s=1.96TeV in the lepton+jets decay channel, where one top quark decays leptonically and the other hadronically. …”
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3
Search for the standard model Higgs boson produced in association with a W-+/- boson with 7.5 fb(-1) integrated luminosity at CDF
Published 2012“…This search uses data corresponding to an integrated luminosity of 7.5fb -1 collected by the CDF detector at the Tevatron. …”
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4
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5
Measurement of CP-violation asymmetries in D0 to Ks pi+ pi-
Published 2012“…We report a measurement of time-integrated CP-violation asymmetries in the resonant substructure of the three-body decay D0 to Ks pi+ pi- using CDF II data corresponding to 6.0 invfb of integrated luminosity from Tevatron ppbar collisions at sqrt(s) = 1.96 TeV. …”
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6
Measurement of the B+ production cross section in pp̄ collisions at s=1960GeV
Published 2007“…The data correspond to an integrated luminosity of 739pb-1 collected with the upgraded CDF detector (CDF II) at the Fermilab Tevatron collider. …”
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7
Measurement of the difference in CP-violating asymmetries in D(0)→K(+)K(-) and D(0)→π(+)π(-) decays at CDF.
Published 2012“…We report a measurement of the difference (ΔA(CP)) between time-integrated CP-violating asymmetries in D(0)→K(+)K(-) and D(0)→π(+)π(-) decays reconstructed in the full data set of proton-antiproton collisions collected by the Collider Detector at Fermilab, corresponding to 9.7 fb(-1) of integrated luminosity. …”
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8
Production of ψ(2S) mesons in pp̄ collisions at 1.96 TeV
Published 2009“…These measurements have been made using a data set from an integrated luminosity of 1.1fb-1 collected by the CDF II detector at Fermilab. …”
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9
Top quark mass measurement in the lepton + jets channel using a matrix element method and in situ jet energy calibration.
Published 2010“…Using a total of 1087 events in 5.6 fb(-1) of integrated luminosity, a value of m(t)=173.0 ± 1.2 GeV/c(2) is measured.…”
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10
Combination of CDF and D0 W-Boson Mass Measurements
Published 2013“…Earlier measurements from CDF and D0 are combined with the two latest, more precise measurements: a CDF measurement in the electron and muon channels using data corresponding to $2.2 \mathrm{fb}^{-1}$ of integrated luminosity, and a D0 measurement in the electron channel using data corresponding to $4.3 \mathrm{fb}^{-1}$ of integrated luminosity. …”
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11
Measurement of the top pair production cross section in the lepton+jets channel using a jet flavor discriminant
Published 2011“…We present a new method to measure the top quark pair production cross section and the background rates with data corresponding to an integrated luminosity of 2.7fb-1 from pp̄ collisions at √s=1.96TeV collected with the CDF II Detector. …”
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12
Combination of measurements of the top-quark pair production cross section from the Tevatron Collider
Published 2014“…The data correspond to integrated luminosities of up to 8.8fb-1. We obtain a value of σtt̄=7.60±0.41pb for a top-quark mass of mt=172.5GeV. …”
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13
Top quark mass measurement in the lepton+jets channel using a matrix element method and in situ jet energy calibration
Published 2010“…A likelihood is calculated using a matrix element method with quasi-Monte Carlo integration taking into account finite detector resolution and jet mass effects. …”
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14
Measurement of the J/ψ meson and b-hadron production cross sections in pp̄ collisions at √s = 1960 GeV
Published 2005“…The data correspond to an integrated luminosity of 39.7 pb-1 collected by the CDF run II detector. …”
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15
Search for the Higgs boson in the all-hadronic final state using the CDF II detector
Published 2011“…The data sample used corresponds to an integrated luminosity of approximately 4fb-1 of pp̄ collisions at √s=1.96TeV recorded by the CDF II experiment. …”
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16
Measurement of cross sections for b jet production in events with a Z boson in p(p)over-bar collisions at root s=1.96 TeV
Published 2009“…A measurement of the b jet production cross section is presented for events containing a Z boson produced in pp̄ collisions at s=1.96TeV, using data corresponding to an integrated luminosity of 2fb-1 collected by the CDF II detector at the Tevatron. …”
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17
Measurement of the inclusive jet cross section using the kT algorithm in pp collisions at (square root s)=1.96 TeV.
Published 2006“…We report on a measurement of the inclusive jet production cross section as a function of the jet transverse momentum in pp collisions at (square root s)=1.96 TeV using data collected with the upgraded Collider Detector at Fermilab in run II, corresponding to an integrated luminosity of 385 pb-1. The measurement is carried out for jets with rapidity 0.1…”
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18
Study of jet shapes in inclusive jet production in pp̄ collisions at s=1.96 TeV
Published 2005“…We report on a study of jet shapes in inclusive jet production in pp̄ collisions at s=1.96 TeV using the upgraded collider detector at Fermilab in Run II (CDF II) and based on an integrated luminosity of 170 pb-1. Measurements are carried out on jets with rapidity 0.1<|Yjet|<0.7 and transverse momentum 37GeV/c…”
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19
Measurement of the inclusive jet cross section using the kT algorithm in pp̄ collisions at s=1.96TeV
Published 2006“…We report on a measurement of the inclusive jet production cross section as a function of the jet transverse momentum in pp̄ collisions at s=1.96TeV using data collected with the upgraded Collider Detector at Fermilab in run II, corresponding to an integrated luminosity of 385pb-1. The measurement is carried out for jets with rapidity 0.1<|yjet|<0.7 and transverse momentum in the range 54…”
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20
Top quark mass measurement in the lepton plus jets channel using a modified matrix element method
Published 2009“…We calculate a signal likelihood using a matrix element integration method, where the matrix element is modified by using effective propagators to take into account assumptions on event kinematics. …”
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