Search results for "Fermi"

showing 10 items of 1388 documents

Measurement of thepp¯→tt¯production cross section and the top quark mass ats=1.96  TeVin the all-hadronic decay mode

2007

We report the measurements of the t{bar t} production cross section and of the top quark mass using 1.02 fb{sup -1} of p{bar p} data collected with the CDF II detector at the Fermilab Tevatron. We select events with six or more jets on which a number of kinematical requirements are imposed by means of a neural network algorithm. At least one of these jets must be identified as initiated by a b-quark candidate by the reconstruction of a secondary vertex. The cross section is measured to be {sigma}{sub t{bar t}} = 8.3 {+-} 1.0(stat. ){sup +2.0}{sub -1.5}(syst.) {+-} 0.5(lumi.) pb, which is consistent with the standard model prediction. The top quark mass of 174.0 {+-} 2.2(stat.){+-}4.8(syst.)…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMass distribution010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyTevatron01 natural sciencesParticle identificationStandard ModelNuclear physicsPair productionAntiproton0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Invariant massFermilabNuclear Experiment010306 general physicsPhysical Review D
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Measurement of the top quark pair production cross section in thelepton+jetschannel in proton-antiproton collisions ats=1.96  TeV

2011

We present a measurement of the inclusive top quark pair production cross section in \ppbar collisions at (\sqrt{s}=1.96) TeV utilizing data corresponding to an integrated luminosity of \lumi\ collected with the D0 detector at the Fermilab Tevatron Collider. We consider final states containing one high-$p_{T}$ isolated electron or muon and at least two jets, and we perform three analyses: one exploiting specific kinematic features of \ttbar events, the second using $b$-jet identification, and the third using both techniques to separate \ttbar\ signal from background. In the third case, we determine simultaneously the $t\bar{t}$ cross section and the ratio of the production rates of $W$+heav…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatron01 natural sciences7. Clean energyNuclear physicsPair productionAntiproton0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Fermilab010306 general physicsLeptonPhysical Review D
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Measurement of B(t→Wb)/B(t→Wq) at s=1.96TeV

2006

We present the measurement of R = B(t -> Wb)/B(t -> Wq) in pp collisions at root s = 1.96 TeV, using 230 pb(-1) of data collected by the DO experiment at the Fermilab Tevatron Collider. We fit simultaneously R and the number (N-tt) of selected top quark pairs (tt), to the number of identified b-quark jets in events with one electron or one muon, three or more jets, and high transverse energy imbalance. To improve sensitivity, kinematical properties of events with no identified b-quark jets are included in the fit. We measure R = 1.03(-0.17)(0.19) (stat + syst), in good agreement with the standard model. We set lower limits of R > 0.61 and vertical bar V-tb vertical bar > 0.78 at 95% confide…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronElectron7. Clean energy01 natural sciencesLower limitStandard Modellaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysics Letters B
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Measurement of Leptonic Asymmetries and Top Quark Polarization in ttbar Production

2013

We present measurements of lepton (l) angular distributions in ttbar -> W+ b W- b -> l+ nu b l- nubar bbar decays produced in ppbar collisions at a center-of-mass energy of sqrt(s)=1.96TeV, where l is an electron or muon. Using data corresponding to an integrated luminosity of 5.4fb^-1, collected with the D0 detector at the Fermilab Collider, we find that the angular distributions of l- relative to anti-protons and l+ relative to protons are in agreement with each other. Combining the two distributions and correcting for detector acceptance we obtain the forward-backward asymmetry A^l_FB = (5.8 +- 5.1(stat) +- 1.3(syst))%, compared to the standard model prediction of A^l_FB (predicted…

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMuon010308 nuclear & particles physicsmedia_common.quotation_subjectDetectorFOS: Physical sciencesElectronPolarization (waves)01 natural sciences7. Clean energyAsymmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFermilab010306 general physicsLeptonmedia_common
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The decay η → π0h0 in two-higgs-doublet models

1991

The possibility of a light scalar in the framework of two-Higgs-doublet models is studied. The range of masses 100 MeV < mh0 < 2mπ is already excluded by present experiment bounds on the transition η → π0h0 in the model where the neutral component of one doublet couples to fermions with weak isospin T3 = −12 and the neutral component of the second doublet to fermions with T3 = +12. These bounds also constrain tightly the structure of the Yukawa couplings in two-Higgs-doublet models.

PhysicsNuclear and High Energy PhysicsParticle physicsWeak isospinHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyScalar (mathematics)Yukawa potentialElementary particleFermionAtomic and Molecular Physics and OpticsNuclear physicsHiggs fieldsymbols.namesakeHiggs bosonsymbolsHiggs mechanismNuclear Physics B - Proceedings Supplements
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Absolute Lower Limits on the Masses of Selectrons and Sneutrinos in the MSSM

2002

The results of searches for selectrons, charginos and neutralinos performed with the data collected by the ALEPH detector at LEP at centre-of-mass energies up to 209 GeV are interpreted in the framework of the Minimal Supersymmetric extension of the Standard Model with R-parity conservation. Under the assumptions of gaugino and sfermion mass unification and no sfermion mixing, an absolute lower limit of 73 GeV/c2 is set on the mass of the lighter selectron at the 95% confidence level. Similarly, limits on the masses of the heavier selectron and of the sneutrino are set at 107 and 84 GeV/c2, respectively. Additional constraints are derived from the results of the searches for Higgs bosons. T…

PhysicsNuclear and High Energy PhysicsParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGauginoFOS: Physical sciencesSupersymmetry7. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear physicsSelectron tubeHigh Energy Physics - Experiment (hep-ex)CharginoSfermion0103 physical sciencesNeutralinoHiggs boson[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsParticle Physics - Experiment
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Collective and broken pair states of65,67Ga

1999

Excited states of 65Ga and 67Ga nuclei were populated through the 12C(58Ni,αp) and 12C(58Ni,3p) reactions, respectively, and investigated by in-beam γ-ray spectroscopic methods. The NORDBALL array equipped with a charged particle ball and 11 neutron detectors was used to detect the evaporated particles and γ rays. The level schemes of 65,67Ga were constructed on the basis of γγ-coincidence relations up to 8.6 and 10 MeV excitation energy, and Iπ=27/2 and 33/2+ spin and parity, respectively. The structure of 65,67Ga nuclei was described in the interacting boson-fermion plus broken pair model, including quasiproton, quasiproton-two-quasineutron, and three-quasiproton fermion configurations in…

PhysicsNuclear and High Energy PhysicsPhononExcited stateNuclear structureQuasiparticleNeutronFermionAtomic physicsInteracting boson modelCharged particlePhysical Review C
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Extended Thomas - Fermi expansion from nuclear linear response

1996

The coefficients of the successive orders of the extended Thomas - Fermi expansion of the kinetic energy density are obtained to the leading order in the density inhomogeneities. This is done by comparing the corresponding static polarizability with the exact value in two cases: a non-interacting nuclear infinite system and symmetric nuclear matter with a Skyrme interaction.

PhysicsNuclear and High Energy PhysicsPolarizabilityQuantum electrodynamicsQuantum mechanicsNuclear TheoryOrder (group theory)Kinetic energyFermi gasNuclear matterFermi Gamma-ray Space TelescopeJournal of Physics G: Nuclear and Particle Physics
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Multiparticle emission in the decay ofAr31

2014

A multihit capacity setup was used to study the decay of the dripline nucleus Ar-31, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the beta-delayed three-proton decay of Ar-31 is presented for the first time together with a quantitative analysis of the beta-delayed 2p gamma decay. A new method for determination of the spin of low-lying levels in the beta p daughter 30S using proton-proton angular correlations is presented and used to determine that the spin of the 5.2-MeV level is most likely 3(+) with 4(+) also possible. The half-life of Ar-31 is found to be 15.1(3) ms. An improved analysis of the Fermi beta strength including the beta 3p-decay mode gives a total mea…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsBranching fractionGamma ray7. Clean energy01 natural sciencesNuclear physicsmedicine.anatomical_structure0103 physical sciencesmedicineIsobaric processBeta (velocity)Atomic physics010306 general physicsNucleusSpin-½Fermi Gamma-ray Space TelescopePhysical Review C
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Recoil-beta tagging: A novel technique for studying proton-drip-line nuclei

2006

Abstract Tagging with charged particles and γ -rays at the focal plane of recoil separators has proven, over the last two decades, to be a very powerful tool for the identification of excited states in exotic nuclei produced with very low cross-sections. One of the key areas so far unexplored in terms of the tagging methodology has been performing correlations with β -particles at the focal plane of a recoil separator. A new technique entitled Recoil-Beta Tagging (RBT) has been developed, this technique exploits the unusual properties of Fermi super-allowed β emitters, which have both a short half-life ( ∼ 100 ms ) and high β + -endpoint energy. Correlating with such β -particles using a do…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsDetector[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCharged particleSemiconductor detectorNuclear physicsRecoilPositronExcited state27.50.þe; 29.30.Kv; 29.40.Wk0103 physical sciencesAtomic physics010306 general physicsNuclear ExperimentInstrumentationFermi Gamma-ray Space Telescope
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