Search results for "nuclear physics"

showing 10 items of 5307 documents

Calculation of the neutrinoless ββ decay of 76Ge using a quark model with harmonic confinement

1991

Abstract The half-life of the neutrinoless double beta decay of 76Ge into the ground state of 76Se is calculated in a relativistic quark confinement model. The proton-neutron quasi-particle random-phase approximation is used to evaluate the s- and p-wave nuclear matrix elements contained in the decay amplitude. We avoid the closure approximation and calculate the effective vector and axial-vector coupling constants of the hadronic currents using our quark model. In our formulation the recoil matrix element arises from the quark recoil in the decaying neutrons. The recoil and the p-wave effect are discussed and compared with other calculations. From the experimental lower bound for the decay…

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::PhenomenologyNuclear TheoryNuclear physicsMAJORANARecoilDouble beta decayHigh Energy Physics::ExperimentNeutronColor confinementNeutrinoNuclear ExperimentNuclear Physics A
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Search for pair production of heavy top-like quarks decaying to a high-pT W boson and a b quark in the lepton plus jets final state at s=7 TeV with t…

2013

A search is presented for production of a heavy up-type quark (t') together with its antiparticle, assuming a significant branching ratio for subsequent decay into a W boson and a b quark. The search is based on 4.7 fb(-1) of pp collisions root s = 7 TeV recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Data are analyzed in the lepton + jets final state, characterized by a high-transverse-momentum isolated electron or muon, large missing transverse momentum and at least three jets. The analysis strategy relies on the substantial boost of the W bosons in the t'(t') over bar signal when m(t') greater than or similar to 400 GeV. No significant excess of events above t…

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicsW and Z bosons0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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Measurement of the top quark mass in the dilepton channel using mT2 at CDF

2010

We present measurements of the top quark mass using mT2, a variable related to the transverse mass in events with two missing particles. We use the template method applied to tt̅ dilepton events produced in pp̅ collisions at Fermilab’s Tevatron Collider and collected by the CDF detector. From a data sample corresponding to an integrated luminosity of 3.4  fb-1, we select 236 tt̅ candidate events. Using the mT2 distribution, we measure the top quark mass to be Mtop=168.0-4.0+4.8(stat)±2.9(syst)  GeV/c2. By combining mT2 with the reconstructed top quark mass distributions based on a neutrino weighting method, we measure Mtop=169.3±2.7(stat)±3.2(syst)  GeV/c2. This is the first application of …

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsMass distribution010308 nuclear & particles physicshep-exHadronHigh Energy Physics::PhenomenologyTevatronddc:500.201 natural sciences114 Physical scienceslaw.inventionNuclear physicslaw0103 physical sciencesTransverse massHigh Energy Physics::ExperimentFermilab010306 general physicsColliderNuclear Experiment
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Search for admixture of scalar top quarks in the tt¯ lepton + jets final state at s=1.96 TeV

2009

A search for pair production of the lightest supersymmetric partner of the top quark is performed in the lepton+jets channel using 0.9 fb-1 of data collected by the D0 experiment. Kinematic differences between scalar top quark pair production and the dominant top quark pair production background are used to separate the two processes. First limits from Run II of the Fermilab Tevatron Collider for the scalar top quark decaying to a chargino and a b quark are obtained for scalar top quark masses of 130-190 GeV and chargino masses of 90-150 GeV.

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsStop squark010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyTevatronTop quark condensate7. Clean energy01 natural sciencesBottom quarkNuclear physicsNonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentB meson010306 general physicsMinimal Supersymmetric Standard ModelPhysics Letters B
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Transverse spin asymmetries in p ↑ p → π± + X and lp ↑ → l′ + π± + X

2000

Abstract While transverse spin effects have been studied in hadronic interactions since a few decades, investigations with leptonic probes have started very recently. Azimuthal distributions of hadrons (mainly π + and π − ) produced in DIS off transversely polarized targets (proton and deuteron) are studied for the first time in SMC. According to Collins (‘Collins effect’), the azimuthal distribution of the leading hadron might exhibit an asymmetry which originates from the transverse polarization of the final quark.

PhysicsQuarkNuclear and High Energy Physicsmedia_common.quotation_subjectNuclear TheoryHigh Energy Physics::PhenomenologyHadronPolarization (waves)AsymmetryNuclear physicsTransverse planeAngular distributionDeuteriumHigh Energy Physics::ExperimentNuclear Experimentmedia_commonNuclear Physics A
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Study ofππcorrelations at LHC and RHIC energies inppcollisions within the quark-gluon string model

2011

The quark-gluon string model reproduces well the global characteristics of the $pp$ collisions at energies of $\sqrt{s}=200\text{ }\text{ }\mathrm{GeV}$ (RHIC) and $\sqrt{s}=900\text{ }\text{ }\mathrm{GeV}$ (LHC). In present paper the quark-gluon string model is employed for the description of femtoscopic characteristics of identical pions produced in the aforementioned reactions. The study is concentrated on the low multiplicity and multiplicity averaged events, where no collective effects are expected. The different procedures for fitting the one-dimensional correlation functions of pions are studied and compared with the space-time distributions extracted directly from the model. Particu…

PhysicsQuarkNuclear physicsNuclear and High Energy PhysicsParticle physicsPionLarge Hadron ColliderMonte Carlo methodHigh Energy Physics::ExperimentMultiplicity (chemistry)Nuclear ExperimentNuclear theoryGluonPhysical Review D
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Search for Single Vectorlike Quarks inpp¯Collisions ats=1.96  TeV

2011

We present a search for hypothetical vector-like quarks in ppbar collisions at sqrt(s) = 1.96 TeV. The data were collected by the D0 detector at the Fermilab Tevatron Collider and correspond to an integrated luminosity of 5.4 fb^(-1). We select events with a final state composed of a W or Z boson and a jet consistent with a heavy object decay. We observe no significant excess in comparison to the background prediction and set limits on production cross sections for vector-like quarks decaying to W+jet and Z+jet. These are the most stringent mass limits for electroweak single vector-like quark production at hadron colliders.

PhysicsQuarkParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHadronElectroweak interactionTevatronGeneral Physics and AstronomyElementary particleJet (particle physics)7. Clean energy01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysical Review Letters
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Measurement of the Branching Fractions ofB¯→D**ℓ−ν¯ℓDecays in Events Tagged by a Fully ReconstructedBMeson

2008

We report a measurement of the branching fractions of D**- decays based on 417 fb-1 of data collected at the (4S) resonance with the BABAR detector at the PEP-II e+e- storage rings. Events are selected by fully reconstructing one of the B mesons in a hadronic decay mode. A fit to the invariant mass differences m(D(*))-m(D(*)) is performed to extract the signal yields of the different D** states. We observe the D**- decay modes corresponding to the four D** states predicted by heavy quark symmetry with a significance greater than 5 standard deviations including systematic uncertainties.

PhysicsQuarkParticle physics010308 nuclear & particles physicsBranching fractionGeneral Physics and AstronomyResonanceBranching (polymer chemistry)01 natural sciencesSymmetry (physics)Nuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massB meson010306 general physicsBar (unit)Physical Review Letters
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Search for Neutral Higgs Bosons at Hightanβin theb(h/H/A)→bτ+τ−Channel

2009

The first search in p (p) over bar collisions at root s = 1.96 TeV for the production of neutral Higgs bosons in association with bottom quarks and decaying in two tau leptons is presented. The cross section for this process is enhanced in many extensions of the standard model, such as its minimal supersymmetric extension (MSSM) at large tan beta. The data, corresponding to an integrated luminosity of 328 pb(-1), were collected with the D0 detector at the Fermilab Tevatron Collider. An upper limit is set on the production cross section of neutral Higgs bosons in the mass range of 90 to 150 GeV, and this limit is used to exclude part of the MSSM parameter space.

PhysicsQuarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomySupersymmetry7. Clean energy01 natural sciencesStandard ModelNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonMinimal Supersymmetric Standard ModelLeptonPhysical Review Letters
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X(3872) and its charmonium content in Heavy Quark limit

2016

X (3872) still presents many puzzles more than a decade after its discovery. Some of its properties, like the isospin violating decays, can easily be accommodated in a molecular model, whereas its other properties, such as radiative decays can be more naturally explained in the quarkonium picture. The best of these schemes can be combined in a picture of X (3872) where it is dominantly a molecular state with some charmonium components. In this work, we present a model based on heavy quark symmetry which describes X (3872) as a superposition of molecular and charmonium components.

PhysicsQuarkParticle physics010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuarkonium01 natural sciencesSymmetry (physics)Nuclear physicsSuperposition principleIsospin0103 physical sciencesRadiative transferHigh Energy Physics::ExperimentLimit (mathematics)010306 general physicsComputer Science::DatabasesX(3872)EPJ Web of Conferences
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