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221
SEARCH FOR CHARGED BOSONS HEAVIER THAN THE W-BOSON IN P(P)OVER-BAR COLLISIONS AT ROOT-S=1800 GEV
Published 1995“…The data used in the search represent 19.7 pb-1 collected by the Collider Detector at Fermilab. Limits are placed on σB(pp̄→W′→eν) as a function of MW′. …”
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222
Jet pseudorapidity distribution in direct photon events in p(p)over-bar collisions at root s=1.8 TeV
Published 1998“…We present the first measurement of the jet pseudorapidity distribution in direct photon events from a sample of pp̄ collisions at √s= 1.8 TeV, recorded with the Collider Detector at Fermilab. Quantum chromodynamics (QCD) predicts that these events are primarily from hard quark-gluon Compton scattering, qg→qγ, with the final state quark producing the jet of hadrons. …”
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223
Search for the decay Bs→μ+μ-φ in pp̄ collisions at √s = 1.8 TeV
Published 2002“…We present a search for the flavor-changing neutral current decay Bs→μ+μ-φ in pp̄ collisions at √s = 1.8 TeV, using 91 pb-1 of data collected at the Collider Detector at Fermilab (CDF). We find two candidate events for this decay, which are consistent with the background estimate of one event, and set an upper limit on the branching fraction of B(Bs→ μ+μ-φ)<6.7×10-5 at a 95% confidence level. …”
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224
Measurement of the cross section for prompt diphoton production in pp collisions at square root of s=1.96 TeV.
Published 2005“…We report a measurement of the rate of prompt diphoton production in pp collisions at square root of s=1.96 TeV using a data sample of 207 pb(-1) collected with the upgraded Collider Detector at Fermilab. The background from nonprompt sources is determined using a statistical method based on differences in the electromagnetic showers. …”
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225
Quasi-model-independent search for new high p(T) physics at D0.
Published 2001“…We apply a quasi-model-independent strategy ("Sleuth") to search for new high p(T) physics in approximately 100 pb(-1) of pp collisions at square root of (s) = 1.8 TeV collected by the D0 experiment during 1992-1996 at the Fermilab Tevatron. We systematically analyze many exclusive final states and demonstrate sensitivity to a variety of models predicting new phenomena at the electroweak scale. …”
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226
Direct measurement of the W Boson width in ppover collisions at square roots = 1.96 TeV.
Published 2008“…A direct measurement of the total decay width of the W boson Gamma(W) is presented using 350 pb(-1) of data from pp[over ] collisions at square root s = 1.96 TeV collected with the CDF II detector at the Fermilab Tevatron. The width is determined by normalizing predicted signal and background distributions to 230 185 W candidates decaying to enu and micronu in the transverse-mass region 50…”
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227
Measurement of the isolated photon cross section in p over(p, ̄) collisions at sqrt(s) = 1.96 TeV
Published 2006“…The cross section for the inclusive production of isolated photons has been measured in p over(p, ̄) collisions at sqrt(s) = 1.96 TeV with the DØ detector at the Fermilab Tevatron Collider. The photons span transverse momenta 23 to 300 GeV and have pseudorapidity | η | < 0.9. …”
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228
Quasi-model-independent search for new high p(T) physics at D0.
Published 2001“…We apply a quasi-model-independent strategy ("Sleuth") to search for new high p(T) physics in approximately 100 pb(-1) of pp collisions at square root of (s) = 1.8 TeV collected by the D0 experiment during 1992-1996 at the Fermilab Tevatron. We systematically analyze many exclusive final states and demonstrate sensitivity to a variety of models predicting new phenomena at the electroweak scale. …”
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229
Observation of the Bc meson in the exclusive decay Bc-->J/psipi.
Published 2008“…A fully reconstructed Bc-->J/psipi signal is observed with the D0 detector at the Fermilab Tevatron pp[over] collider using 1.3 fb(-1) of integrated luminosity. …”
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230
Model uncertainties at MicroBooNE
Published 2017“…The MicroBooNE experiment is a 170 ton Liquid Argon Time Projection Chamber (LArTPC) experiment designed for short-baseline neutrino physics, located at surface level in the Booster Neutrino Beam (BNB) at Fermilab. A muon neutrino-argon charged current (CC) cross section measurement in the energy range of ~200 MeV - 2 GeV has recently been started. …”
Conference item -
231
First measurement of the W-boson mass in run II of the Tevatron.
Published 2007“…We present a measurement of the W-boson mass using 200 pb{-1} of data collected in pp[over ] collisions at sqrt[s]=1.96 TeV by the CDF II detector at run II of the Fermilab Tevatron. With a sample of 63 964 W-->enu candidates and 51 128 W-->munu candidates, we measure M_{W}=80 413+/-34{stat}+/-34{syst}=80,413+/-48 MeV/c;{2}. …”
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232
Measurement of the top quark mass in the dilepton channel
Published 1999“…We report a measurement of the top quark mass using six candidate events for the process pp̄→tt̄+X →l+vbl-v̄b̄+X, observed in the D0 experiment at the Fermilab pp̄ collider. Using maximum likelihood fits to the dynamics of the decays, we measure a mass for the top quark of mt=168.4±12.3(stat) ±3.6(syst) Gev. …”
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233
Measurement of the forward-backward charge asymmetry from W→ev production in pp̄ collisions at √s=1.96 TeV
Published 2005“…We report a measurement of the forward-backward charge asymmetry of electrons from W boson decays in pp̄ collisions at √s=1.96 TeV using a data sample of 170 pb-1 collected by the Collider Detector at Fermilab. The asymmetry is measured as a function of electron rapidity and transverse energy and provides new input on the momentum fraction dependence of the u and d quark parton distribution functions within the proton. © 2005 The American Physical Society.…”
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234
Search for Randall-Sundrum gravitons with 1 fb(-1) of data from pp collisions at sqrt(s)=1.96 TeV.
Published 2008“…We search for decays of Kaluza-Klein excitations of the graviton in the Randall-Sundrum model of extra dimensions to e+ e(-) and gamma gamma in 1 fb(-1) of pp collisions at sqrt(s)=1.96 TeV collected by the D0 detector at the Fermilab Tevatron. We set 95% confidence level upper limits on the production cross section times branching fraction, which translate into lower limits on the mass of the lightest excitation between 300 and 900 GeV for values of the coupling k/MPl between 0.01 and 0.1.…”
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235
PRODUCTION OF CHARGED HADRONS BY POSITIVE MUONS ON DEUTERIUM AND XENON AT 490 GEV
Published 1994“…The data were taken with the E665 spectrometer, which was exposed to the 490 GeV muon beam of the Tevatron at Fermilab. The use of a streamer chamber as vertex detector provides nearly 4π acceptance for charged particles. …”
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236
Electromagnetic shower properties in a lead-scintillator sampling calorimeter
Published 2013“…The Collider Detector at Fermilab (CDF) is a general-purpose experimental apparatus with an inner tracking detector for measuring charged particles, surrounded by a calorimeter for measurements of electromagnetic and hadronic showers. …”
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237
Second generation leptoquark earch in pp̄ collisions at √s = 1.8 TeV
Published 1995“…We report on a search for second generation scalar leptoquarks with the D0 detector at the Fermilab Tevatron pp̄ collider at √s = 1.8 TeV. This search is based on 12.7 pb-1 of data. …”
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238
Small angle J/ψ production in pp̄ collisions at √s = 1.8 TeV
Published 1999“…The results are based on 9.8 pb-1 of data collected using the D0 detector at the Fermilab Tevatron Collider. The inclusive J/ψ cross section for transverse momenta between 1 and 16 GeV/c is compared with theoretical models of charmonium production.…”
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239
Search for Higgs bosons decaying to tau pairs in p(p)over-bar collisions with the D0 detector
Published 2008“…The data, corresponding to an integrated luminosity of approximately 1fb-1, were collected by the D0 experiment at the Fermilab Tevatron Collider. Limits on the production cross section times branching ratio are set. …”
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240
MHz gravitational wave constraints with decameter Michelson interferometers
Published 2017“…A new detector, the Fermilab Holometer, consists of separate yet identical 39-meter Michelson interferometers. …”
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