Search results for " scheme"

showing 10 items of 323 documents

High-precision mass measurement ofS31with the double Penning trap JYFLTRAP improves the mass value forCl32

2010

Nuclear physicsPhysicsNuclear and High Energy PhysicsInternal conversionDecay schemeIsotopes of germaniumDouble beta decayBeta particleAtomic physicsPenning trapMass measurementBeta-decay stable isobarsPhysical Review C
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The decay of 0.57 s114Cs

1980

Fusion reactions between58Ni projectiles and58Ni target nuclei were used to produce114Cs activity, which was studied by on-line mass separation and decay spectroscopy. The obtained half-life of 0.57±0.02 s and the probability ratio of 44±3 between betadelayed proton and beta-delayed alpha emission represent data with improved precision. The absolute branching ratios for both particle decay modes were determined to be (7 ±2)×10−2 and (1.6±0.6)×10−3, respectively. These branching ratios and the shapes of particle spectra are discussed with reference to the statistical model calculations. Groundstate alpha decay of114Cs was observed with an alpha energy of 3,226±30 keV and a branching ratio of…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle decayCluster decayDecay schemeProton decayBranching fractionNuclear fusionHigh Energy Physics::ExperimentAlpha decayAtomic physicsDecay correctZeitschrift für Physik A Atoms and Nuclei
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Neutrinoless double beta decay to excited collective 0+ states

2000

Abstract The many recently performed experiments to study the two-neutrino double beta (2 νββ ) decay to the first excited 0 + final state encourage similar experiments to be done for the neutrinoless double beta (0 νββ ) decay. Based on the accumulated theoretical and experimental information on the 2 νββ decays one could hope that the 0 νββ decay to the excited 0 + state would be very efficient in restricting the parameter space of modern particle-physics theories. In this article the 0 νββ decays of 76 Ge and 82 Se to excited collective 0 + states are studied within a realistic nuclear model. It is found that the lower limits for the half-lives of these decays are of the order of 10 27 y…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeExcited stateDouble beta decayHigh Energy Physics::ExperimentBeta (velocity)Parameter spaceBeta-decay stable isobarsPhysics Letters B
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Λ Decay Induced by Two Nucleons

1995

The decay of Λ hypernuclei induced by two nucleons is revised, along with its implications in the experimental determination of the ratio of neutron- to proton-stimulated Λ decay.

Nuclear physicsPhysicsParticle physicsDecay schemeNuclear TheoryHigh Energy Physics::ExperimentNeutronNuclear ExperimentNucleon
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Nuclear structure of (231)Ac

2008

The low-energy structure of 231Ac has been investigated by means of gamma ray spectroscopy following the beta-decay of 231Ra. Multipolarities of 28 transitions have been established by measuring conversion electrons with a mini-orange electron spectrometer. The decay scheme of 231Ra --> 231Ac has been constructed for the first time. The Advanced Time Delayed beta-gamma-gamma(t) method has been used to measure the half-lives of five levels. The moderately fast B(E1) transition rates derived suggest that the octupole effects, albeit weak, are still present in this exotic nucleus. The low-energy structure of 231 Ac has been investigated by means of γ ray spectroscopy following the β − decay of…

Nuclear reactionPhysicsNuclear and High Energy PhysicsDecay schemeNuclear structureHalf-lifeFísicaElectronNuclear physicsGamma spectroscopyNuclear Physics - ExperimentAtomic physicsSpectroscopyRadioactive decay
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Nuclear structure of 131Te studied with (n,γ) and reactions

2003

Abstract The structure of 131 Te has been investigated with the 130 Te( n , γγ ) 131 Te reaction using thermal neutrons and with the 130 Te( d , p ) 131 Te reaction using polarized deuterons with energy E d =18 MeV. About 290 levels were identified in most cases including spin, parity and γ -decay. The γ -decay scheme after neutron capture is essentially complete containing about 100% of the decay of the capture state and about 100% of the population of the 11/2 − isomer and of the ground state. The scheme includes 42 primary transitions with energies between 750 keV and 2500 keV. The experimental level scheme is compared with predictions of the Interacting Boson–Fermion model (IBFM) and of…

Nuclear reactionPhysicsNuclear and High Energy PhysicsNeutron captureDecay schemeDeuteriumAstrophysics::High Energy Astrophysical PhenomenaBinding energyNeutronAtomic physicsNuclear ExperimentGround stateNeutron temperatureNuclear Physics A
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Capturing Shock Reflections: An Improved Flux Formula

1996

Godunov type schemes, based on exact or approximate solutions to the Riemann problem, have proven to be an excellent tool to compute approximate solutions to hyperbolic systems of conservation laws. However, there are many instances in which a particular scheme produces inappropriate results. In this paper we consider several situations in which Roe's scheme gives incorrect results (or blows up all together) and we propose an alternative flux formula that produces numerical approximations in which the pathological behavior is either eliminated or reduced to computationally acceptable levels.

Numerical AnalysisConservation lawPhysics and Astronomy (miscellaneous)Applied MathematicsMathematical analysisGodunov's schemeType (model theory)Hyperbolic systemsComputer Science ApplicationsShock (mechanics)Roe solverComputational Mathematicssymbols.namesakeRiemann problemModeling and SimulationScheme (mathematics)symbolsMathematicsJournal of Computational Physics
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The MAST-edge centred lumped scheme for the flow simulation in variably saturated heterogeneous porous media

2012

A novel methodology is proposed for the solution of the flow equation in a variably saturated heterogeneous porous medium. The computational domain is descretized using triangular meshes and the governing PDEs are discretized using a lumped in the edge centres numerical technique. The dependent unknown variable of the problem is the piezometric head. A fractional time step methodology is applied for the solution of the original system, solving consecutively a prediction and a correction problem. A scalar potential of the flow field exists and in the prediction step a MArching in Space and Time (MAST) formulation is applied for the sequential solution of the Ordinary Differential Equation of…

Numerical AnalysisPhysics and Astronomy (miscellaneous)DiscretizationApplied MathematicsLinear systemScalar potentialGeometryFinite element methodSettore ICAR/01 - IdraulicaComputer Science ApplicationsComputational MathematicsHydraulic headRate of convergenceVariably saturated porous medium Numerical model Finite element Lumped scheme Mass conservation Unstructured mesh Analytical solutionModeling and SimulationOrdinary differential equationApplied mathematicsVariably saturated porous medium Numerical model Finite element Lumped scheme Mass conservation Unstructured mesh Analytical solutionConservation of massMathematicsJournal of Computational Physics
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A velocity–diffusion method for a Lotka–Volterra system with nonlinear cross and self-diffusion

2009

The aim of this paper is to introduce a deterministic particle method for the solution of two strongly coupled reaction-diffusion equations. In these equations the diffusion is nonlinear because we consider the cross and self-diffusion effects. The reaction terms on which we focus are of the Lotka-Volterra type. Our treatment of the diffusion terms is a generalization of the idea, introduced in [P. Degond, F.-J. Mustieles, A deterministic approximation of diffusion equations using particles, SIAM J. Sci. Stat. Comput. 11 (1990) 293-310] for the linear diffusion, of interpreting Fick's law in a deterministic way as a prescription on the particle velocity. Time discretization is based on the …

Numerical AnalysisSelf-diffusionDiffusion equationDiscretizationNonlinear diffusionADI schemeApplied MathematicsNumerical analysisMathematical analysisParticle methodComputational MathematicsNonlinear systemReaction–diffusion systemPattern formationParticle velocityReaction-diffusionDiffusion (business)Travelling frontsMathematicsApplied Numerical Mathematics
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Multi-party metering: An architecture for privacy-preserving profiling schemes

2013

Several privacy concerns about the massive deploy- ment of smart meters have been arisen recently. Namely, it has been shown that the fine-grained temporal traces generated by these meters can be correlated with different users behaviors. A new architecture, called multi-party metering, for enabling privacy-preserving analysis of high-frequency metering data without requiring additional complexity at the smart meter side is here proposed. The idea is to allow multiple entities to get a share of the high-frequency metering data rather than the real data, where this share does not reveal any information about the real data. By aggregating the shares provided by different users and publishing …

OptimizationInformation privacyEngineeringtatistical analysiSmart meterDistributed computingpattern clusteringC.2 COMPUTER-COMMUNICATION NETWORKSSmart gridelectricity supply industryComputer securitycomputer.software_genreCOMPUTER-COMMUNICATION NETWORKSElectricityClustering algorithmProfiling (information science)Metering modemart meterIndexeArchitectureCluster analysisgas industrydata privacybusiness.industrySettore ING-INF/03 - TelecomunicazioniComplexity theoryreal gas consumption dataVectorsA sharehigh-frequency metering datamultiparty meteringInformation sensitivityynthetic electricity consumption dataCryptographyprivacy-preserving profiling schemeprivacy-preserving analysibusinesscomputeruser profiling clustering mechanismMulti-Party Metering
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