Search results for "Interaction"

showing 10 items of 5710 documents

The Two-Nucleon System beyond the Pion Threshold

2003

A model is developed for the hadronic and electromagnetic interaction in the two-nucleon system above pion threshold in the framework of meson, nucleon and Δ degrees of freedom. It is based on time-ordered perturbation theory and includes full meson retardation in potentials and exchange currents as well as loop contributions to the nucleonic one-body current. Results for some selected processes are discussed.

PhysicsParticle physicsMesonNuclear TheoryHadronDegrees of freedom (physics and chemistry)Loop (topology)Nuclear physicsElectromagnetic interactionPionHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Nuclear ExperimentNucleon
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Weak Decays of ExcitedBMesons

2015

We investigate the decays of the excited (bq[over ¯]) mesons as probes of the short-distance structure of the weak ΔB=1 transitions. These states are unstable under the electromagnetic or strong interactions, although their widths are typically suppressed by phase space. Compared to the pseudoscalar B meson, the purely leptonic decays of the vector B^{*} are not chirally suppressed and are sensitive to different combinations of the underlying weak effective operators. An interesting example is B_{s}^{*}→ℓ^{+}ℓ^{-}, which has a rate that can be accurately predicted in the standard model. The branching fraction is B∼10^{-11}, irrespective of the lepton flavor and where the main uncertainty st…

PhysicsParticle physicsMesonsMeson010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyStrong interactionGeneral Physics and AstronomyModels Theoretical01 natural sciencesResonance (particle physics)Standard ModelNuclear physicsPseudoscalar0103 physical sciencesHigh Energy Physics::ExperimentB meson010306 general physicsNuclear PhysicsLeptonPhysical Review Letters
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Search for the Standard Model Higgs Boson in theH→WW→lνq′q¯Decay Channel

2011

We present a search for the standard model Higgs boson (H) in ppbar collisions at sqrt{s}=1.96 TeV in events containing a charged lepton (ell), missing transverse energy, and at least two jets, using 5.4 fb^-1 of integrated luminosity recorded with the D0 detector at the Fermilab Tevatron Collider. This analysis is sensitive primarily to Higgs bosons produced through the fusion of two gluons or two electroweak bosons, with subsequent decay H->WW->ell+nu+q'qbar, where ell is an electron or muon. The search is also sensitive to contributions from other production channels, such as WH->ell+nu+bbbar In the absence of signal, we set limits at the 95% C.L. on the cross section for H production si…

PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionTevatronGeneral Physics and AstronomyElementary particle7. Clean energy01 natural sciencesStandard ModelNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonLeptonPhysical Review Letters
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Neutrinos in Nuclear Physics: RPA, MEC, 2p2h (Pionic Modes of Excitation in Nuclei)

2016

This chapter is devoted to the study of weak interactions on nucleons and nuclei. I pay a special attention to the study of neutrino and antineutrino quasi-elastic reactions in nuclei , which are of the greatest importance for neutrino oscillation experiments, and crucial to achieve the precision goals required to make new discoveries, like the CP violation in the leptonic sector, possible. In particular, I discuss RPA correlations and 2p2h (multi-nucleon) effects on charged-current neutrino-nucleus reactions, and the influence of these nuclear effects on the recently measured MiniBooNE flux folded differential cross sections, and on the so-called nucleon axial mass puzzle. The modification…

PhysicsParticle physicsMuon010308 nuclear & particles physicsNuclear TheoryWeak interactionNuclear matter01 natural sciencesNuclear physicsMiniBooNE0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrinoNuclear Experiment010306 general physicsNeutrino oscillationNucleon
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Tau leptonic branching ratios

1996

A sample of 62249 tau-pair events is selected from data taken with the ALEPH detector in 1991, 1992 and 1993. The measurement of the branching fractions for tau decays into electrons and muons is presented with emphasis on the study of systematic effects from selection, particle identification and decay classification. The results obtained are: B-e=17.79+/-0.12(stat)+/-0.06(syst)(%) and B-mu=17.31+/-0.11(stat)+/-0.05(syst)(%). Combined with the most recent ALEPH determination of the tau lifetime, these results provide a relative measurement of the leptonic couplings in the weak charged current for transverse W bosons: g(mu)/g(e)=1.0002+/-0.0051 and g(tau)/g(mu)=0.9943+/-0.0065. RI ANTONELLI…

PhysicsParticle physicsMuonPhysics and Astronomy (miscellaneous)[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsElectron–positron annihilationPhysicsElectroweak interaction01 natural sciencesParticle identificationNuclear physicsPositron0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsCharged currentParticle Physics - ExperimentBhabha scatteringBoson
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Measurement of the single π0 production rate in neutral current neutrino interactions on water

2018

The single π0 production rate in neutral current neutrino interactions on water in a neutrino beam with a peak neutrino energy of 0.6 GeV has been measured using the POD, one of the subdetectors of the T2K near detector. The production rate was measured for data taking periods when the POD contained water (2.64×1020 protons-on-target) and also periods without water (3.49×1020 protons-on-target). A measurement of the neutral current single π0 production rate on water is made using appropriate subtraction of the production rate with water in from the rate with water out of the target region. The subtraction analysis yields 106±41±69 signal events where the uncertainties are statistical (stat.…

PhysicsParticle physicsNeutral currentPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorFluxInteraction energy01 natural sciences7. Clean energyNuclear physicsCross section (physics)0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentNeutrinoNuclear Experiment010306 general physicsNucleonPhysical Review D
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Maximal isospin few-body systems of nucleons and $\Xi$ hyperons

2016

By using local central Yukawa-type interactions that reproduce the low-energy parameters of the latest updates of the Nijmegen ESC08c potentials we show that the $N\Xi$, $NN\Xi$, $N\Xi\Xi$ and $NN\Xi\Xi$ systems with maximal isospin are bound. Since in these states the strong decay $N\Xi\to\Lambda\Lambda$ is forbidden by isospin conservation, these strange few-body systems will be stable under the strong interaction. These results may suggest that other states with different number of $N$'s and $\Xi$'s in the maximal isospin channel could also be bound.

PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsStrong interactionNuclear TheoryHyperonFew-body systemsLambda01 natural sciencesHigh Energy Physics - PhenomenologyIsospin0103 physical sciencesNucleon010303 astronomy & astrophysicsNuclear theory
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The coannihilation codex

2015

We present a general classification of simplified models that lead to dark matter (DM) coannihilation processes of the form DM + X $\rightarrow$ SM$_1$ + SM$_2$, where X is a coannihilation partner for the DM particle and SM$_1$, SM$_2$ are Standard Model fields. Our classification also encompasses regular DM pair annihilation scenarios if DM and X are identical. Each coannhilation scenario motivates the introduction of a mediating particle M that can either belong to the Standard Model or be a new field, whereby the resulting interactions between the dark sector and the Standard Model are realized as tree-level and dimension-four couplings. We construct a basis of coannihilation models, cl…

PhysicsParticle physicsNuclear and High Energy PhysicsAnnihilationLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionDark matterFOS: Physical sciencesFermionQuantum number01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Hadronic CollidersSymmetry breaking010306 general physicsPhenomenological ModelsJournal of High Energy Physics
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Prediction for the lightest Higgs boson mass in the CMSSM using indirect experimental constraints

2007

Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the preferred value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with …

PhysicsParticle physicsNuclear and High Energy PhysicsCold dark matterHigh Energy Physics::LatticeDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentMinimal Supersymmetric Standard ModelFree parameterParticle Physics - Phenomenology
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Strong phase transition, dark matter and vacuum stability from simple hidden sectors

2014

Motivated by the possibility to explain dark matter abundance and strong electroweak phase transition, we consider simple extensions of the Standard Model containing singlet fields coupled with the Standard Model via a scalar portal. Concretely, we consider a basic portal model consisting of a singlet scalar with $Z_2$ symmetry and a model containing a singlet fermion connected with the Standard Model fields via a singlet scalar portal. We perform a Monte Carlo analysis of the parameter space of each model, and we find that in both cases the dark matter abundance can be produced either via freeze-out or freeze-in mechanisms, but only in the latter model one can obtain also a strong electrow…

PhysicsParticle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)ta114Physics beyond the Standard ModelScalar (mathematics)Electroweak interactionDark matterHigh Energy Physics::PhenomenologyeducationFOS: Physical sciences114 Physical sciencesSymmetry (physics)Standard ModelHidden sectorBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityAstrophysics - Cosmology and Nongalactic AstrophysicsNuclear Physics B
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