Search results for "fission"

showing 10 items of 421 documents

β-delayed fission of192,194At

2013

By using the recoil-fission correlation technique, the exotic process of beta-delayed fission ($\ensuremath{\beta}$DF) was unambiguously identified in the very neutron-deficient nuclei ${}^{192,194}$At in experiments at the velocity filter SHIP at Gesellschaft f\"ur Schwerionenforschung (GSI). The upper limits for the total kinetic energy release in fission of ${}^{192,194}$Po, being the daughter products of ${}^{192,194}$At after ${\ensuremath{\beta}}^{+}/EC$ decay, were estimated. The possibility of an unusually high $\ensuremath{\beta}$DF probability for ${}^{192}$At is discussed.

PhysicsNuclear and High Energy PhysicsCold fissionCluster decay010308 nuclear & particles physicsFission0103 physical sciencesBeta (velocity)Atomic physics010306 general physicsKinetic energy01 natural sciencesPhysical Review C
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Production of neutron rich isotopes in fission. A study for RNB facilities

2002

Abstract The theoretical model for calculations of the fission product yields in the light-particle induced fission is discussed. A comparison of the production cross sections in fission of 238 U by protons, thermal and fast neutrons, and photons is presented. The results of studies of the very asymmetric fission of 238 U by protons and neutron at the moderate energy are reported.

PhysicsNuclear and High Energy PhysicsCold fissionCluster decayFissionNeutron emissionIsotopes of samariumNuclear TheoryFission product yieldFast fissionNuclear physicsPhysics::Atomic and Molecular ClustersNuclear ExperimentLong-lived fission productNuclear PhysicsNuclear Physics A
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Electromagnetic fission of $^{238}$U at 600 and 1000 MeV per nucleon

1995

Electromagnetic fission of238U projectiles at E/A =600 and 1000 MeV was studied with the ALADIN spectrometer at the heavy-ion synchrotron SIS. Seven different targets (Be, C, Al, Cu, In, Au and U) were used. By considering only those fission events where the two charges added up to 92, most of the nuclear interactions were excluded. The nuclear contributions to the measured fission cross sections were determined by extrapolating from beryllium to the heavier targets with the concept of factorization. The obtained cross sections for electromagnetic fission are well reproduced by extended Weizsacker-Williams calculations which include E1 and E2 excitations. The asymmetry of the fission fragme…

PhysicsNuclear and High Energy PhysicsCold fissionCluster decayFissionNuclear Theorychemistry.chemical_elementUraniumResonance (particle physics)Nuclear physicschemistryNuclear fusionAtomic physicsBerylliumNuclear ExperimentNucleonNuclear Physics
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Mass and charge distributions in the very asymmetric mass region of the neutron induced fission of

2001

Abstract The mass-separator Lohengrin was used to measure the yields of the light fission products with A=74−85 and their nuclear charge and kinetic energy distributions from the odd- Z compound nucleus 239 Np ∗ formed by double capture of thermal neutrons. The mass yield distribution reveals an influence of the fragment shell with N=50 affecting also the nuclear charge and kinetic energy distributions. An odd–even effect for protons is found in the very asymmetric mass division, increasing from 4% to 35% with increasing fission asymmetry. This is in contrast to findings in normal asymmetric fission (region of high fission yields) where no odd–even effect for protons was observed. An odd–ev…

PhysicsNuclear and High Energy PhysicsCold fissionFission productsCluster decayPrompt neutronNeutron emissionFissionNuclear TheoryNeutronAtomic physicsNuclear ExperimentNeutron temperatureNuclear Physics A
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Measurement of fission fragments energy loss

2002

Abstract The mean energy of 252 Cf fission fragments emerging from an absorber and the determination of the capture rate in the absorber itself have been measured using two independent and complementary nuclear techniques. The results can be applied to the measurement of the energy self-absorption in a non-zero thickness source and can be used to validate simulation programs.

PhysicsNuclear and High Energy PhysicsCold fissionFissionXenon-135Isotopes of samariumFission product yieldFast fissionNuclear physicsNuclear fissionNuclear ExperimentLong-lived fission productInstrumentationComputer Science::DatabasesNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Production of neutron-rich isotopes in fission of uranium induced by neutrons of 20 MeV average energy

2000

In the context of a parameter study conducted by several laboratories for future European radioactive beam facilities based on fast-neutron induced fission, in particular for the SPIRAL-II project at GANIL, we have measured the yields of neutron-rich isotopes in the mass range of 88 to 144. These nuclei were obtained as fission products of natural uranium bombarded by neutrons of 20 MeV average energy emitted by a thick carbon target irradiated by 50 MeV deuterons. Yields have been measured using on-line mass separation with the ion-guide method. Compared with proton-induced fission at 25 MeV the magnitude of cross-sections, except for the symmetric region, is similar. Z-distributions of is…

PhysicsNuclear and High Energy PhysicsCold fissionIsotopes of uranium010308 nuclear & particles physicsNeutron emissionIsotopes of samariumNuclear TheoryFission product yield[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyFast fissionNuclear physicsUranium-2380103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsLong-lived fission product
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Production of neutron-rich nuclei in fission induced by neutrons generated by the p + 13C reaction at 55 MeV

2003

Cross-sections for the production of neutron-rich nuclei obtained by neutron-induced fission of natural uranium have been measured. The neutrons were generated by bombarding a 13C target with 55 MeV protons. The results, position of the maximum in the (Z, A)-plane, width and magnitude, are very comparable with those where the neutrons are generated by bombardment of natural 12C graphite with 50 MeV deuterons. Depending on the geometry of the converter/target assembly the isotope yields, however, are a factor of 2-3 lower due to less efficient production of neutrons per primary projectile, especially at small forward angles.

PhysicsNuclear and High Energy PhysicsCold fissionNeutron emissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryFission product yieldNeutron radiationFast fissionNeutron temperatureNuclear physicsUranium-238Nuclear ExperimentDelayed neutronThe European Physical Journal A
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Cross section limits for theCm248(Mg25,4n−5n)Hs268,269reactions

2009

We report on an attempt to produce and detect $^{268}\mathrm{Hs}$ and $^{269}\mathrm{Hs}$ in the nuclear fusion reaction $^{25}\mathrm{Mg}+^{248}\mathrm{Cm}$ using the gas phase chemistry apparatus COMPACT. No decay chains attributable to the decay of hassium isotopes were observed during the course of this experiment. From the nonobservation of $^{269}\mathrm{Hs}$ we derive a cross section limit of 0.4 pb (63% confidence limit) for the reaction $^{248}\mathrm{Cm}(^{25}\mathrm{Mg},4n)^{269}\mathrm{Hs}$ at a center-of-target beam energy of 140 MeV. The evaluated cross section limit for the $^{248}\mathrm{Cm}(^{25}\mathrm{Mg},5n)^{268}\mathrm{Hs}$ reaction depends on the assumed half-life of …

PhysicsNuclear and High Energy PhysicsCross section (physics)chemistryFissionAnalytical chemistrychemistry.chemical_elementNuclear fusionAlpha decayBeam energyHassiumGas phasePhysical Review C
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β-decay of 113Rh and the observation of 113mPd : Isomer systematics in odd-A palladium isotopes

1993

Abstract Decay of 113Rh to the levels of 113Pd was studied at the IGISOL-facility by means of β-, γ- and conversion-electron spectroscopy. The level scheme of 113Pd was constructed using 33 gamma transitions on the basis of observed γγ-coincidence relations and half-life analysis. A β-decay half-life of (2.80±0.12) s was measured for 113Rh. A new 9 − 2 isomeric state with (0.3 ± 0.1) s half-life and excitation energy 81.3 keV was discovered in 113Pd. This state and the other recently observed low-lying 9 − 2 or 11 − 2 isomeric states in 115,117Pd isotopes are directly populated in proton-induced fission. The decay of these isomers is unusually strongly hindered compared with Weisskopf estim…

PhysicsNuclear and High Energy PhysicsDecay schemeIsotope010308 nuclear & particles physicsFissionIsotopes of palladium0103 physical sciencesAtomic physics010306 general physicsSpectroscopy01 natural sciencesExcitationNuclear Physics A
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Gamow-Teller decay of 118Pd and of the new isotope 120Pd

1993

Abstract With the use of the proton-induced fission of 238 U and the ion guide-fed on-line mass separation, even- A isotopes of palladium with high neutron excess were studied by means of γ-ray and conversion-electron spectroscopy. The decay of 118 Pd was reinvestigated in detail, and evidence for the new isotope 120 Pd, with a half-life T 1 2 = 0.5 ± 0.1 s , was found. As established for 118 Pd and tentatively shown for 120 Pd, the β-decay of these two isotopes proceeds mainly through 0 + → 1 + Gamow-Teller transitions with log ft values between 4.2 and 4.7. The strength of individual transitions has been compared with the predictions of the shell-correction model with a deformed Woods-Sax…

PhysicsNuclear and High Energy PhysicsDecay schemeIsotope010308 nuclear & particles physicsFissionchemistry.chemical_element01 natural sciences7. Clean energyIonchemistryPairing0103 physical sciencesNeutronAtomic physics010306 general physicsSpectroscopyPalladiumNuclear Physics A
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