D0 Top Quark Cross Section for the 1992--1995 Tevatron Run PDF Download

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Languages : en
Pages : 7

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We present a measurement of the t{bar t} cross section in p{bar p} collisions at (square root)s = 1.8 TeV using dilepton and single lepton final states. This analysis uses about 100 pb−1 of data collected with the D0 detector at Fermilab during the 1992-1995 run. Analyses in two other final states are also presented. 13 refs., 3 figs., 2 tabs.

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Languages : en
Pages : 16

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The authors present top physics results from the CDF and D0 collaborations. The data were collected at the Fermilab Tevatron over the years 1992--1995 and correspond to approximately 110 pb−1 of p{anti p} collisions. Both experiments present determination of the t{anti t} production cross section using a variety of top decay channels, and refined measurements of the top mass.

Author: Wolfgang Wagner
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Languages : en
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Run II of the Tevatron collider at Fermilab is well under way and data samples larger than those of Run I are at hand. In this contribution the author summarizes the current status of cross-section measurements for top-quark pair (t{bar t}) production at the CDF and D0 experiments.

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Languages : en
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The top quark, discovered in 1995 by the CDF and D0 collaborations at the Tevatron proton antiproton collider at Fermilab, has undergone intense studies in the last 20 years. Currently, CDF and D0 converge on their measurements of top-antitop quark production cross sections using the full Tevatron data sample. In these proceedings, the latest results on inclusive and differential measurements of top-antitop quark production cross sections at the Tevatron are reported.

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Languages : en
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The top quark pair production cross-section[sigma][sub t[bar t]] has been measured in p[bar p] collisions at center of mass energies of 1.96 TeV using Tevatron Run 2 data. In the beginning of Run 2 both CDF and D0[sigma][sub t[bar t]] measurements in the dilepton channel t[bar t][yields] WbW[bar b][yields][bar[ell]][nu][sub[ell]]b[ell][prime][bar[nu]][sub[ell][prime]][bar b] and in the lepton plus jets channel t[bar t][yields] WbW[bar b][yields] q[bar q][prime] b[ell][bar[nu]][sub[ell]][bar b]+[bar[ell]][nu][sub[ell]]bq[bar q][prime][bar b] agree with the NLO (Next-to-Leading-Order) theoretical predictions. The presence of a top signal in Tevatron data has been reestablished.

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Languages : en
Pages : 20

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We present a measurement of the t{anti t} production cross section in p{anti p} collisions at √s = 1.8 TeV and a measurement of top quark mass m{sub t} by the D0 experiment at the Fermilab Tevatron. The measurements are based on the data from the 1992- 1996 run during which the D0 detector was exposed to the integrated luminosity of approximately 125 pb−1. We observe 39 t{anti t} candidate events in the dilepton and lepton+jets decay channels with an expected background of 13.7 ± 2.2 events. We measure the top quark mass m{sub t} using a two constraint fit to m{sub t} in t{anti t} → bW {anti b}W− final states with one W decaying to q{anti q} and the other to e? or??. Events are binned in the fit mass versus a measure of probability for events to be the signal rather than a background. Likelihood fits to the data yield m{sub t} = 173.3 ± 5.6 (stat) ± 6.2 (syst) GeV/c2. For this mass we measure the t{anti t} production cross section to be 5.5 ± 1.8 pb.

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Languages : en
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Measurements of the top quark mass and the t[bar t] production cross section, obtained by CDF and D0 Collaborations at the Tevatron, are presented. The methodology of analyses and their underlying assumptions are summarized. The CDF and D0 top mass averages, based on [approx]100 pb[sup -1] of data collected by each experiment in Run-I, and obtained from a set of selected measurements in several channels are M[sub t] = 176:0 [plus-minus] 4:0(stat) [plus-minus] 5:1(syst) GeV/c[sup 2] and M[sub t] = 172:1 [plus-minus] 5:2(stat) [plus-minus] 4:9(syst) GeV/c[sup 2], respectively. The combined Tevatron top quark mass is M[sub t] = 174:3 [plus-minus]3:2(stat) [plus-minus]4:0(syst) GeV/c]sup 2], where the correlations between CDF and D0 averages were taken into account. The CDF measurement of the t[bar t] cross section (assuming M[sub t] = 175 GeV/c[sup 2]) is [sigma][sub tt] = 7.6[sup 1.8][sub 1.5] pb, and the D0 value (assuming M[sub t] = 172.1 GeV/c[sup 2]) is [sigma][sub tt] = 5:9 [plus-minus] 1:7 pb. In anticipation of the much increased statistics in Run-II, the fact that top quark physics is one of the best windows to new physics beyond the Standard Model is emphasized.

Author: E. Shabalina
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Languages : en
Pages : 4

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An overview of the preliminary results of the top quark pair production cross section measurements at a center-of-mass energy of 1.96 TeV carried out by the CDF and D0 collaborations is presented. The data samples used for the analyses are collected in the current Tevatron run and correspond to an integrated luminosity from 360 pb{sup -1} up to 760 pb{sup -1}.

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Languages : en
Pages : 4

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We present the preliminary results of the t{bar t} pair production cross-section measurements and the single top quark exclusion limits carried out by the D0 and the CDF collaborations in Run II of the Tevatron. The dataset for the various measurements ranges from 140 pb−1 to 350 pb−1.

Author: Prolay Kumar Mal
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Languages : en
Pages : 353

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Discovery of the top quark in 1995 at the Fermilab Tevatron collider concluded a long search following the 1977 discovery of bottom (b) quark [1] and represents another triumph of the Standard Model (SM) of elementary particles. Top quark is one of the fundamental fermions in the Standard Model of electroweak interactions and is the weak-isospin partner of the bottom quark. A precise measurement of top pair production cross-section would be a test of Quantum Chromodynamics (QCD) prediction. Presently, Tevatron is the world's highest energy collider where protons (p) and anti-protons ({anti p}) collide at a centre of mass energy (ps) of 1.96 TeV. At Tevatron top (t) and anti-top ({anti t}) quarks are predominantly pair produced through strong interactions--quark annihilation ({approx_equal} 85%) and gluon fusion ({approx_equal} 15%). Due to the large mass of top quark, t or {anti t} decays ({approx} 10{sup -25} sec) before hadronization and in SM framework, it decays to a W boson and a b quark with {approx} 100% branching ratio (BR). The subsequent decay of W boson determines the major signatures of t{anti t} decay. If both W bosons (coming from t and {anti t} decays) decay into leptons (viz., ev{sub e}, {mu}{nu}{sub {mu}} or {tau}{nu}{sub {tau}}) the corresponding t{bar t} decay is called dileptonic decay. Of all dileptonic decay modes of t{bar t}, the t{bar t} {yields} WWb{anti b} {yields} ev{sub e}{mu}{nu}{sub {mu}}b{anti b} (e{mu} channel) decay mode has the smallest background contamination from Z{sup 0} production or Drell-Yan process; simultaneously, it has the highest BR ({approx} 3.16%) [2] amongst all dileptonic decay modes of t{bar t}. During Run I (1992-1996) of Tevatron, three e{mu} candidate events were detected by D0 experiment, out of 80 candidate events (inclusive of all decay modes of t{bar t}). Due to the rarity of the t{bar t} events, the measured cross-section has large uncertainty in its value (viz., 5.69 {+-} 1.21(stat) {+-} 1.04(sys) pb {at} {radical}s = 1.8 TeV measured by D0 [3]). This analysis presents a cross section measurement in e{mu} channel utilizing {approx} 228 pb{sup -1} of data collected by D0 experiment during Tevatron Run II (between June 2002 and April 2004).