Search results for "Tevatron"

showing 10 items of 358 documents

Search forCPviolation inBs0→μ+Ds−Xdecays inpp¯collisions ats=1.96  TeV

2010

We have performed a search for CP violation in a sample of B-s(0) -> mu+Ds-X decays corresponding to 5 fb(-1) of proton-antiproton collisions collected by the D0 detector in Run II at the Fermilab Tevatron Collider. New physics in B-s(0) mixing could contribute a significant CP violating weak phase, which would be observed as a difference in the decay-time distribution for B-s(0) -> (B) over bar (0)(s) oscillated states versus that for (B) over bar (0)(s) -> B-s(0). A fit to the decay-time distributions of the B-s(0)/(B) over bar (0)(s) candidates yields the flavor-specific asymmetry as a(fs)(s) = [-1.7 +/- 9.1(stat)(-1.5)(+1.4)(syst) x 10(-3), which excludes CP violation due to new physics…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonMeson010308 nuclear & particles physicsPhysics beyond the Standard ModelHadronTevatron01 natural sciencesNuclear physicsParticle decay0103 physical sciencesCP violationHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Study ofCP-violating charge asymmetries of single muons and like-sign dimuons inpp¯collisions

2014

We measure the inclusive single muon charge asymmetry and the like-sign dimuon charge asymmetry in $p \bar{p}$ collisions using the full data set of 10.4 fb$^{-1}$ collected with the D0 detector at the Fermilab Tevatron. The standard model predictions of the charge asymmetries induced by CP violation are small in magnitude compared to the current experimental precision, so non-zero measurements could indicate new sources of CP violation. The measurements differ from the standard model predictions of CP violation in these asymmetries with a significance of 3.6 standard deviations. These results are interpreted in a framework of $B$ meson mixing within the CKM formalism to measure the relativ…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonMeson010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatron01 natural sciencesAsymmetryStandard deviationNuclear physicsBaryon asymmetry0103 physical sciencesCP violationHigh Energy Physics::ExperimentFermilab010306 general physicsmedia_commonPhysical Review D
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Measurement of σ(pp¯→Z+X)Br(Z→τ+τ−) at s=1.96 TeV

2009

We present a measurement of the cross section for Z boson production times the branching fraction to tau lepton pairs sigma(p (p) over bar -> Z + X)Br(Z -> tau(+)tau(-)) in p (p) over bar collisions at root s = 1.96 TeV. The measurement is performed in the channel in which one tau lepton decays into a muon and neutrinos. and the other tau lepton decays hadronically or into an electron and neutrinos. The data sample corresponds to an integrated luminosity of 1.0 fb(-1) collected with the DO detector at the Fermilab Tevatron Collider. The sample contains 1511 candidate events with an estimated 20% background from jets or muons misidentified as tau leptons. We obtain sigma . Br = 240 +/- 8 (st…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyTevatron01 natural sciences7. Clean energyStandard Modellaw.inventionLuminosityNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsColliderLeptonPhysics Letters B
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Search for excited muons inpp¯collisions ats=1.96  TeV

2006

We present the results of a search for the production of an excited state of the muon, mu(*), in proton antiproton collisions at root s =1.96 TeV. The data have been collected with the D0 experiment at the Fermilab Tevatron Collider and correspond to an integrated luminosity of approximately 380 pb(-1). We search for mu(*) in the process p (p) over bar ->mu(*)mu, with the mu(*) subsequently decaying to a muon plus photon. No excess above the standard model expectation is observed in data. Interpreting our data in the context of a model that describes mu(*) production by four-fermion contact interactions and mu(*) decay via electroweak processes, we set a 95% confidence level production cros…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsTevatronContext (language use)D0 experiment7. Clean energy01 natural sciencesNuclear physicsParticle decayAntiproton0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilab010306 general physicsLeptonPhysical Review D
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Search for the rare decayBs0→ϕμ+μ−with the D0 detector

2006

We present a search for the flavor-changing neutral current decay B-s(0)->phi mu(+)mu(-) using about 0.45 fb(-1) of data collected in p (p) over bar collisions at root s=1.96 TeV with the D0 detector at the Fermilab Tevatron Collider. We find an upper limit on the branching ratio of this decay normalized to B-s(0)-> J/psi phi of B(B-s(0)->phi mu(+)mu(-))/B(B-s(0)-> J/psi phi) J/psi phi, the limit corresponds to B(B-s(0)->phi mu(+)mu(-))< 4.1x10(-6) at the 95% C.L., the most stringent upper bound to date.

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral current010308 nuclear & particles physicsBranching fractionDetectorTevatron01 natural sciencesUpper and lower boundslaw.inventionlaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderBar (unit)Physical Review D
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Probing neutrino mass with multilepton production at the Tevatron in the simplest R-parity violation model

2003

We analyze the production of multileptons in the simplest supergravity model with bilinear violation of R parity at the Fermilab Tevatron. Despite the small R-parity violating couplings needed to generate the neutrino masses indicated by current atmospheric neutrino data, the lightest supersymmetric particle is unstable and can decay inside the detector. This leads to a phenomenology quite distinct from that of the R-parity conserving scenario. We quantify by how much the supersymmetric multilepton signals differ from the R-parity conserving expectations, displaying our results in the $m_0 \otimes m_{1/2}$ plane. We show that the presence of bilinear R-parity violating interactions enhances…

PhysicsNuclear and High Energy PhysicsParticle physicsParidad RSupergravityHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesFísicaParameter spaceLightest Supersymmetric ParticleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SupersimetríaR-parityModelo estándarMultileptonHigh Energy Physics::ExperimentFermilabNeutrinosNeutrinoPhenomenology (particle physics)
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Measurement of direct photon pair production cross sections in pp¯ collisions at s=1.96 TeV

2010

We present a measurement of direct photon pair production cross sections using 4.2 fb(-1) of data collected with the DO detector at the Fermilab Tevatron p (p) over bar Collider. We measure single differential cross sections as a function of the diphoton mass, the transverse momentum of the diphoton system, the azimuthal angle between the photons, and the polar scattering angle of the photons. In addition, we measure double differential cross sections considering the last three kinematic variables in three diphoton mass bins. The results are compared with different perturbative QCD predictions and event generators. (C) 2010 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsScatteringTevatronPerturbative QCD01 natural scienceslaw.inventionNuclear physicsCross section (physics)Pair productionlaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysics Letters B
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Measurement of the isolated photon cross section in pp¯ collisions at s=1.96 TeV

2006

The cross section for the inclusive production of isolated photons has been measured in p anti-p collisions at sqrt{s}=1.96 TeV with the D0 detector at the Fermilab Tevatron Collider. The photons span transverse momenta 23 to 300 GeV and have pseudorapidity |eta|<0.9. The cross section is compared with the results from two next-to-leading order perturbative QCD calculations. The theoretical predictions agree with the measurement within uncertainties.

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsTevatronPerturbative QCD7. Clean energy01 natural sciencesNuclear physicsTransverse planePseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentFermilabNuclear Experiment010306 general physicsPhysics Letters B
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Search for a Higgs boson in diphoton final states with the D0 detector in9.6  fb−1ofpp¯collisions ats=1.96  TeV

2013

We present a search for a Higgs boson decaying into a pair of photons based on 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques to discriminate signal from the non-resonant background and is separately optimized for a standard model and a fermiophobic Higgs boson. No significant excess of data above the background prediction is observed and upper limits on the product of the cross section and branching fraction are derived at the 95% confidence level as a function of Higgs boson mass. For a standard model Higgs boson with mass of 125 GeV, the observed (expected) upper limits are a f…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyTevatron01 natural sciencesStandard Modellaw.inventionNuclear physicslaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysical Review D
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Search for a scalar or vector particle decaying into Zγ in pp¯ collisions at s=1.96 TeV

2009

We present a search for a narrow scalar or vector resonance decaying into Z gamma with a subsequent Z boson decay into a pair of electrons or moons. The data for this search were collected with the D circle divide detecror at the Fermilab Tevatron p (p) over bar collider at a center of mass energy root s = 1.96 TeV. Using 1.1 (1.0) fb(-1) of data, we observe 49 (50) candidate events in the electron (muon) channel, in good agreement with the standard model prediction. From the combination of both channels, we derive 95% C.L. upper limits on the cross section times branching fraction (sigma x B) into Z gamma. These limits range from 0.19 (0.20) pb for a scalar (vector) resonance mass of 600 G…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMuon010308 nuclear & particles physicsBranching fractionScalar (mathematics)TevatronElectron01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsBosonPhysics Letters B
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