Search results for "Fission"

showing 10 items of 421 documents

Simulations of the stopping efficiencies of fission ion guides

2017

With the Ion Guide Isotope Separator On-Line (IGISOL) facility, located at the University of Jyväskylä, products of nuclear reactions are separated by mass. The high resolving power of the JYFLTRAP Penning trap, with full separation of individual nuclides, capacitates the study of nuclides far from the line of stability. For the production of neutron-rich medium-heavy nuclides, fissioning of actinides is a feasible reaction. This can be achieved with protons from an in-house accelerator or, alternatively, with neutrons through the addition of a newly developed Be(p,xn)-converter. The hereby-obtained fission products are used in nuclear data measurements, for example fission yields, nuclear …

Nuclear reactionCold fissionFissionQC1-999Nuclear TheoryFission product yield01 natural sciencesmethodsSubatomär fysikNuclear physicsmenetelmätSubatomic Physics0103 physical sciencesNeutronNuclideNuclear Experiment010306 general physicsFission productsexperimental facilitiesta114010308 nuclear & particles physicsChemistryPhysicsRadiochemistryvarusteettekniikattechniquesLong-lived fission productequipmentEPJ Web of Conferences
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Estimates of the Nuclear Time Delay in Dissipative U + U and U + Cm Collisions Derived from the Shape of Positron andδ-Ray Spectra

1983

Positron and delta-ray spectra have been measured in coincidence with quasielastic scattered particles and fission fragments from the bombardment of Pd, U, and Cm targets with U beams of energies between 5.9 and 8.4 MeV/u. For collisions leading to a fission reaction, the atomic positron and delta-ray spectra fall off more steeply at high energies than expected from calculations based on pure Rutherford trajectories. A quantitative analysis of this effect is in accord with a nuclear contact time of about 10/sup -21/ s.

Nuclear reactionElastic scatteringPhysicsAntiparticleFissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and AstronomyNuclear physicssymbols.namesakePositronNuclear fissionAntimattersymbolsPhysics::Accelerator PhysicsRutherford scatteringAtomic physicsNuclear ExperimentPhysical Review Letters
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Beta decay of neutron-rich cobalt and nickel isotopes

1998

We report on the first β-γ spectroscopy measurements of the neutron-rich 68–70Co and 70–74Ni nuclei, produced in proton-induced fission of 238U and ionized in a laser ion guide coupled to an on-line mass separator. Several γ lines from the decay of these nuclei have been identified, half-lives determined and production cross sections deduced. The derived level schemes for the copper and nickel isotopes show that the occupation of the ν(1g9/2) state has a strong influence on the structure of these neutron-rich nuclei. This may have a clear impact on the predicted structure and decay properties of doubly-magic 78Ni.

Nuclear reactionIsotopeChemistryFissionNuclear Theorychemistry.chemical_elementBeta decayNuclear physicsNickelNeutronAtomic physicsNuclear ExperimentIsotopes of cobaltRadioactive decayExotic nuclei and atomic masses (ENAM 98)
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Fission fragment anisotropy for the 242mAm fission isomer by spin exchange pumping with polarized rubidium vapour

1992

Abstract The foundations of an experiment have been worked out with which, in principle, the spin, hyperfine constants and the isomer shift of the 14 ms fission isomer 242mAm can be measured. Such an experiment would be based on the fission fragment anisotropy signal which has actually been observed in this work after spin exchange pumping with polarized rubidium vapour in an optical buffer gas cell. A decrease of the count rate of (12±4)% has been measured at 90% with respect to the quantization axis. From this result it is concluded that the nuclear spin of the 242mAm fission isomer must be larger than 1. The low-energy fission isomers originating from the 242Pu(d, 2n)242mAm reaction have…

Nuclear reactionNuclear and High Energy PhysicsCluster decayFissionChemistrychemistry.chemical_elementAmericiumRubidiumNuclear physicsPlutonium-242Physics::Atomic and Molecular ClustersAtomic physicsNuclear ExperimentSpin (physics)InstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Fast and nonselective on-line mass separation of neutron-rich isotopes produced in proton-induced fission

1989

Abstract On-line mass separation of short-lived radionuclides, based on the use of thermalized primary ions from nuclear reactions, termed as an ion guide method, has recently been widely applied in the spectroscopy of both proton-rich and neutron-rich exotic nuclei. The technique has been found to be applicable to all elements and it has allowed the detection of the mass-analyzed activities with half-lives as short as 0.1 ms. The ion guide isotope separator on-line, IGISOL, has recently been used to discover over ten new short-lived isotopes or isomers produced in the nearly symmetric fission of uranium induced by 20 MeV protons. In addition to applications in nuclear-structure physics and…

Nuclear reactionNuclear and High Energy PhysicsIsotopeProtonFissionChemistryNuclear Theorychemistry.chemical_elementUraniumIonNuclear physicsIonizationNeutronNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Fission yield measurements at IGISOL

2016

The fission product yields are an important characteristic of the fission process. In fundamental physics, knowledge of the yield distributions is needed to better understand the fission process. For nuclear energy applications good knowledge of neutroninduced fission-product yields is important for the safe and efficient operation of nuclear power plants. With the Ion Guide Isotope Separator On-Line (IGISOL) technique, products of nuclear reactions are stopped in a buffer gas and then extracted and separated by mass. Thanks to the high resolving power of the JYFLTRAP Penning trap, at University of Jyväskylä, fission products can be isobarically separated, making it possible to measure rela…

Nuclear reactionNuclear fission productFission productsIsotopeta114010308 nuclear & particles physicsChemistryFissionPhysicsQC1-999Nuclear TheoryFission product yieldPenning trap01 natural sciencesNuclear physicsSubatomär fysik0103 physical sciencesSubatomic PhysicsPhysics::Atomic and Molecular ClustersNeutronfission product yieldIGISOL010306 general physicsNuclear Experiment
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Attempts to chemically investigate element 112

2006

Summary Two experiments aiming at the chemical investigation of element 112 produced in the heavy ion induced nuclear fusion reaction of 48Ca with 238U were performed at the Gesellschaft für Schwerionenforschung (GSI), Darmstadt, Germany. Both experiments were designed to determine the adsorption enthalpy of element 112 on a gold surface using a thermochromatography setup. The temperature range covered in the thermochromatography experiments allowed the adsorption of Hg at about 35 °C and of Rn at about -180 °C. Reports from the Flerov Laboratory for Nuclear Reactions (FLNR), Dubna, Russia claim production of a 5-min spontaneous fission (SF) activity assigned to 283112 for the 238U(48Ca,3n)…

Nuclear reactionNuclear physicsAdsorptionIsotopeChemistryEnthalpyRadiochemistryNuclear fusionTransactinide elementPhysical and Theoretical ChemistryAtmospheric temperature rangeSpontaneous fissionRadiochimica Acta
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Production and Decay of Element 114: High Cross Sections and the New NucleusHs277

2010

The fusion-evaporation reaction Pu-244(Ca-48, 3-4n)(288,289)114 was studied at the new gas-filled recoil separator TASCA. Thirteen correlated decay chains were observed and assigned to the production and decay of (288, 289)114. At a compound nucleus excitation energy of E* = 39.8-43.9 MeV, the 4n evaporation channel cross section was 9.8(-3.1)(+3.9) pb. At E* = 36.1-39.5 MeV, that of the 3n evaporation channel was 8.0-(+7.4)(4.5) pb. In one of the 3n evaporation channel decay chains, a previously unobserved alpha branch in (281)Ds was observed ( probability to be of random origin from background: 0.1%). This alpha decay populated the new nucleus (277)Hs, which decayed by spontaneous fission…

Nuclear reactionNuclear physicsCluster decayIsotopeFissionGeneral Physics and AstronomyDecay chainAlpha decayAtomic physicsRadioactive decaySpontaneous fissionPhysical Review Letters
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Multipole strength distributions and form factors forE1,E2/E0, andE3 fromU238(e,e’f) coincidence experiments

1987

A model-independent multipole analysis of $^{238}\mathrm{U}$(e,e'f) coincidence data, taken at four momentum transfers (0.2\ensuremath{\le}${q}_{\mathrm{eff}\mathrm{\ensuremath{\le}}0.7}$ ${\mathrm{fm}}^{\mathrm{\ensuremath{-}}1}$; \ensuremath{\omega}=4--22 MeV) yields both E1, E2/E0, and E3 form factors and strength distributions. The E2/E0 strength distribution in the fission channel shows two distinct bumps centered at \ensuremath{\omega}\ensuremath{\simeq}10 and 14 MeV, exhausting up to 12 MeV (19\ifmmode\pm\else\textpm\fi{}2)% of the isoscalar E2 sum rule. The extracted form factors can be described within a hydrodynamical model by use of parameters ${c}_{\mathrm{tr}/{c}_{0}=1.2}$ and …

Nuclear reactionPhysicsDistribution (mathematics)IsoscalarPhotofissionGeneral Physics and AstronomySum rule in quantum mechanicsInelastic scatteringAtomic physicsMultipole expansionOmegaPhysical Review Letters
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2020

The novel technology of calorimetric low-temperature detectors (CLTDs) was applied to determine isotopic yields of fission fragments using the passive absorber method for thermal-neutron-induced fission reactions at the LOHENGRIN mass spectrometer at the Institut Laue-Langevin in Grenoble, France. Precise yields were determined for $^{92}\mathrm{Rb}$ and $^{96}\mathrm{Y}$. These fission products are the dominant contributors to the high-energy portion of the reactor antineutrino spectra. Our new measurements resolve inconsistencies between previous yield measurements and fission data libraries and reduce the nuclear data uncertainties in the computation of reactor antineutrino spectra by th…

Nuclear reactionPhysicsFission products010308 nuclear & particles physicsFissionNuclear dataMass spectrometry01 natural sciences7. Clean energyNeutron temperatureSpectral linePhysics::GeophysicsNuclear physicsYield (chemistry)0103 physical sciencesNuclear Experiment010306 general physicsPhysical Review C
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